diff --git a/test/Makefile b/test/Makefile
index b5bec7d344c38893eb94c6dfe71082b04739af36..3c98a5bf6dd94947a3f6bd2d11845209b7cc15ac 100644
--- a/test/Makefile
+++ b/test/Makefile
@@ -706,6 +706,7 @@ distclean: clean
-@cd RootShower && $(MAKE) distclean
-@cd rhtml && $(MAKE) distclean
-@cd RootIDE && $(MAKE) distclean
+ -@cd periodic && $(MAKE) distclean
.SUFFIXES: .$(SrcSuf)
diff --git a/test/periodic/LoadXS.C b/test/periodic/LoadXS.C
new file mode 100644
index 0000000000000000000000000000000000000000..ebcd3a4c9435b91fd7c1401246e4c6f72d6c8e85
--- /dev/null
+++ b/test/periodic/LoadXS.C
@@ -0,0 +1,53 @@
+void LoadXS()
+{
+ gSystem->Load("libNdb");
+ NdbMTReactionXS pb(1,"Total Cross Section");
+
+ pb.LoadENDF("8200.endf");
+
+ const Int_t npoint=1000;
+
+ Double_t e=1.0E-3;
+
+ const Double_t fact = TMath::Exp(TMath::Log(2.0E7/e)/(Double_t)(npoint-1));
+
+ Float_t *x=new Float_t[npoint];
+ Float_t *y=new Float_t[npoint];
+
+
+ for (Int_t i=0; i<npoint; ++i) {
+ x[i]=e;
+ y[i]=pb.Interpolate(e);
+ e*=fact;
+ }
+
+ c1 = new TCanvas("c1","Lead Cross section",200,10,700,500);
+
+ c1->SetFillColor(42);
+ c1->SetGridx();
+ c1->SetGridy();
+ c1->GetFrame()->SetFillColor(21);
+ c1->GetFrame()->SetBorderSize(12);
+ c1->SetLogx();
+ c1->SetLogy();
+
+ TGraph *gr = new TGraph(npoint,x,y);
+ gr->SetFillColor(19);
+ gr->SetLineColor(2);
+ gr->SetLineWidth(2);
+ gr->SetMarkerColor(4);
+ gr->SetMarkerStyle(21);
+ gr->SetMarkerSize(0.2);
+ gr->SetTitle("Lead Total Cross section");
+ gr->Draw("AWLP");
+
+ //Add axis titles.
+ //A graph is drawn using the services of the TH1F histogram class.
+ //The histogram is created by TGraph::Paint.
+ //TGraph::Paint is called by TCanvas::Update. This function is called by default
+ //when typing <CR> at the keyboard. In a macro, one must force TCanvas::Update.
+
+ c1->Update();
+ gr->GetHistogram()->SetXTitle("Energy in eV");
+ gr->GetHistogram()->SetYTitle("Cross Section in Barns");
+}
diff --git a/test/periodic/Makefile b/test/periodic/Makefile
new file mode 100644
index 0000000000000000000000000000000000000000..33bf51395cb51b6012f714d92043e1fafc29738a
--- /dev/null
+++ b/test/periodic/Makefile
@@ -0,0 +1,54 @@
+############# MACROS ##############
+
+include ../Makefile.arch
+
+DICT := NdbDict.$(SrcSuf)
+DICTH := $(DICT:.$(SrcSuf)=.h)
+DICTO := $(DICT:.$(SrcSuf)=.$(ObjSuf))
+
+DBSRCS := $(wildcard Ndb*.$(SrcSuf))
+
+XSSRCS := $(wildcard XS*.$(SrcSuf))
+
+SRCS := $(XSSRCS) $(DBSRCS)
+
+HDRS := $(SRCS:.$(SrcSuf)=.h) NdbLinkDef.h
+HDRS := $(filter-out $(DICTH),$(HDRS))
+
+TARGETLIB = libNdb.$(DllSuf)
+TARGETPRG = XSGui$(ExeSuf)
+
+DBOBJS = $(DBSRCS:.$(SrcSuf)=.$(ObjSuf))
+XSOBJS = $(XSSRCS:.$(SrcSuf)=.$(ObjSuf))
+
+############# RULES ###############
+
+.$(SrcSuf).$(ObjSuf):
+ $(CXX) $(CXXFLAGS) -c $<
+
+############# TARGETS #############
+
+.SUFFIXES: .$(SrcSuf) .$(ObjSuf) $(ExeSuf) .$(DllSuf)
+
+all: $(TARGETPRG) $(TARGETLIB)
+
+$(DICT): $(HDRS)
+ @echo "Generating dictionary $@..."
+ @$(ROOTCINT) -f $@ -c $^
+
+$(TARGETPRG): $(XSOBJS) $(DBOBJS) $(DICTO)
+ $(LD) $(LDFLAGS) $^ $(GLIBS) $(OutPutOpt)$@
+ @echo "$@ done"
+
+$(TARGETLIB): $(DBOBJS) $(DICTO)
+ifeq ($(PLATFORM),macosx)
+ @$(LD) $(SOFLAGS)$@ $(LDFLAGS) $^ $(OutPutOpt) $@
+else
+ @$(LD) $(SOFLAGS) $(LDFLAGS) $^ $(OutPutOpt) $@
+endif
+
+distclean: clean
+ @rm -f $(TARGETPRG) $(TARGETLIB) $(DICT) $(DICTH)
+
+clean:
+ @rm -f $(DBOBJS) $(XSOBJS) $(DICTO)
diff --git a/test/periodic/NdbAngularDist.cxx b/test/periodic/NdbAngularDist.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..ba990a4fa387331e0052e6b24ea92af44a865b2d
--- /dev/null
+++ b/test/periodic/NdbAngularDist.cxx
@@ -0,0 +1,6 @@
+
+#include "NdbAngularDist.h"
+
+
+ClassImp(NdbAngularDist)
+
diff --git a/test/periodic/NdbAngularDist.h b/test/periodic/NdbAngularDist.h
new file mode 100644
index 0000000000000000000000000000000000000000..4b6f952f636cd520c7c73dcc1892ac92109d30a3
--- /dev/null
+++ b/test/periodic/NdbAngularDist.h
@@ -0,0 +1,20 @@
+#ifndef NDBANGULARDIST_H
+#define NDBANGULARDIST_H
+
+#include "NdbMF.h"
+
+/* ========= TMFAngularDist ============ */
+class NdbAngularDist : public NdbMF
+{
+protected:
+
+public:
+ NdbAngularDist()
+ : NdbMF(4, "Angular distributions for emitted particles") {}
+ ~NdbAngularDist() {}
+
+ ClassDef(NdbAngularDist,1)
+
+}; // NdbMfAngularDist
+
+#endif
diff --git a/test/periodic/NdbDCAngularDist.cxx b/test/periodic/NdbDCAngularDist.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..7b1e9817ba214352a3f4fe669bba1f51bd8fd9d4
--- /dev/null
+++ b/test/periodic/NdbDCAngularDist.cxx
@@ -0,0 +1,5 @@
+#include "NdbDCAngularDist.h"
+
+ClassImp(NdbDCAngularDist)
+
+
diff --git a/test/periodic/NdbDCAngularDist.h b/test/periodic/NdbDCAngularDist.h
new file mode 100644
index 0000000000000000000000000000000000000000..15172750cfe4bd69f3e60561c0ed6d28673b7ac9
--- /dev/null
+++ b/test/periodic/NdbDCAngularDist.h
@@ -0,0 +1,20 @@
+#ifndef DCANGULARDIST_H
+#define DCANGULARDIST_H
+
+#include "NdbMF.h"
+
+/* ========= NdbDCAngularDist ============ */
+class NdbDCAngularDist : public NdbMF
+{
+protected:
+
+public:
+ NdbDCAngularDist()
+ : NdbMF(34, "Data covariances for angular distributions") {}
+ ~NdbDCAngularDist() {}
+
+ ClassDef(NdbDCAngularDist,1)
+
+}; // NdbDCAngularDist
+
+#endif
diff --git a/test/periodic/NdbDCEnergyDist.cxx b/test/periodic/NdbDCEnergyDist.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..c09166ce8f250d5e0ea9f6009299a625632453be
--- /dev/null
+++ b/test/periodic/NdbDCEnergyDist.cxx
@@ -0,0 +1,3 @@
+#include "NdbDCEnergyDist.h"
+
+ClassImp(NdbDCEnergyDist)
diff --git a/test/periodic/NdbDCEnergyDist.h b/test/periodic/NdbDCEnergyDist.h
new file mode 100644
index 0000000000000000000000000000000000000000..996e8380128fc3b2596fa267bbf67fb87a6a57b0
--- /dev/null
+++ b/test/periodic/NdbDCEnergyDist.h
@@ -0,0 +1,20 @@
+#ifndef MFDCENERGYDIST_H
+#define MFDCENERGYDIST_H
+
+#include "NdbMF.h"
+
+/* ========= NdbDCEnergyDist ============ */
+class NdbDCEnergyDist : public NdbMF
+{
+protected:
+
+public:
+ NdbDCEnergyDist()
+ : NdbMF(35, "Data covariances for energy distributions") {}
+ ~NdbDCEnergyDist() {}
+
+ ClassDef(NdbDCEnergyDist,1)
+
+}; // NdbDCEnergyDist
+
+#endif
diff --git a/test/periodic/NdbDCNuBar.cxx b/test/periodic/NdbDCNuBar.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..eb224d8a179e62e18148e9bf3e5120a063abe236
--- /dev/null
+++ b/test/periodic/NdbDCNuBar.cxx
@@ -0,0 +1,3 @@
+#include "NdbDCNuBar.h"
+
+ClassImp(NdbDCNuBar)
diff --git a/test/periodic/NdbDCNuBar.h b/test/periodic/NdbDCNuBar.h
new file mode 100644
index 0000000000000000000000000000000000000000..ff7b1a20fd2a7e77b3a08e7a3f72e77199753609
--- /dev/null
+++ b/test/periodic/NdbDCNuBar.h
@@ -0,0 +1,20 @@
+#ifndef MFDCNUBAR_H
+#define MFDCNUBAR_H
+
+#include "NdbMF.h"
+
+/* ========= TMFDCNuBar ============ */
+class NdbDCNuBar : public NdbMF
+{
+protected:
+
+public:
+ NdbDCNuBar()
+ : NdbMF(31, "Data covariances for nu(bar)") {}
+ ~NdbDCNuBar() {}
+
+ ClassDef(NdbDCNuBar,1)
+
+}; // NdbDCNuBar
+
+#endif
diff --git a/test/periodic/NdbDCRadioXS.cxx b/test/periodic/NdbDCRadioXS.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..430a5b6473008f450385023742ce4bef506d9cdb
--- /dev/null
+++ b/test/periodic/NdbDCRadioXS.cxx
@@ -0,0 +1,3 @@
+#include "NdbDCRadioXS.h"
+
+ClassImp(NdbDCRadioXS)
diff --git a/test/periodic/NdbDCRadioXS.h b/test/periodic/NdbDCRadioXS.h
new file mode 100644
index 0000000000000000000000000000000000000000..0be22aee8845bb31d2e5c2c3479fc84b05fe0215
--- /dev/null
+++ b/test/periodic/NdbDCRadioXS.h
@@ -0,0 +1,21 @@
+#ifndef MFDCRADIOXS_H
+#define MFDCRADIOXS_H
+
+#include "NdbMF.h"
+
+/* ========= NdbDCRadioXS ============ */
+class NdbDCRadioXS : public NdbMF
+{
+protected:
+
+public:
+ NdbDCRadioXS()
+ : NdbMF(40, "Data covariances for radionuclide production "
+ "cross sections") {}
+ ~NdbDCRadioXS() {}
+
+ ClassDef(NdbDCRadioXS,1)
+
+}; // NdbDCRadioXS
+
+#endif
diff --git a/test/periodic/NdbDCRadioYield.cxx b/test/periodic/NdbDCRadioYield.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..6798ab2cadac5f67ae777ef2dc78d9710395235c
--- /dev/null
+++ b/test/periodic/NdbDCRadioYield.cxx
@@ -0,0 +1,3 @@
+#include "NdbDCRadioYield.h"
+
+ClassImp(NdbDCRadioYield)
diff --git a/test/periodic/NdbDCRadioYield.h b/test/periodic/NdbDCRadioYield.h
new file mode 100644
index 0000000000000000000000000000000000000000..2c66b62c683ec1da5fa7a2c733da91e19a2453d0
--- /dev/null
+++ b/test/periodic/NdbDCRadioYield.h
@@ -0,0 +1,21 @@
+#ifndef DCRADIOYIELD_H
+#define DCRADIOYIELD_H
+
+#include "NdbMF.h"
+
+/* ========= NdbDCRadioYield ============ */
+class NdbDCRadioYield : public NdbMF
+{
+protected:
+
+public:
+ NdbDCRadioYield()
+ : NdbMF(39, "Data covariances for radionuclide "
+ "production yields") {}
+ ~NdbDCRadioYield() {}
+
+ ClassDef(NdbDCRadioYield,1)
+
+}; // NdbDCRadioYield
+
+#endif
diff --git a/test/periodic/NdbDCReactionXS.cxx b/test/periodic/NdbDCReactionXS.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..318e264cf499eccc5a838dee77f52464764ea1cd
--- /dev/null
+++ b/test/periodic/NdbDCReactionXS.cxx
@@ -0,0 +1,3 @@
+#include "NdbDCReactionXS.h"
+
+ClassImp(NdbDCReactionXS)
diff --git a/test/periodic/NdbDCReactionXS.h b/test/periodic/NdbDCReactionXS.h
new file mode 100644
index 0000000000000000000000000000000000000000..9eb62bbf2976e330b82ebf68ad0bf8e7d087fc7b
--- /dev/null
+++ b/test/periodic/NdbDCReactionXS.h
@@ -0,0 +1,21 @@
+#ifndef DCREACTIONXS_H
+#define DCREACTIONXS_H
+
+#include "NdbMF.h"
+
+/* ========= NdbDCReactionXS ============ */
+class NdbDCReactionXS : public NdbMF
+{
+protected:
+
+public:
+ NdbDCReactionXS()
+ : NdbMF(33, "Data covariances for reaction cross section") {}
+
+ ~NdbDCReactionXS() {}
+
+ ClassDef(NdbDCReactionXS,1)
+
+}; // NdbDCReactionXS
+
+#endif
diff --git a/test/periodic/NdbDCResParam.cxx b/test/periodic/NdbDCResParam.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..7acda35d720466c0dd6bac00b1c8ebf3bb5cfeba
--- /dev/null
+++ b/test/periodic/NdbDCResParam.cxx
@@ -0,0 +1,3 @@
+#include "NdbDCResParam.h"
+
+ClassImp(NdbDCResParam)
diff --git a/test/periodic/NdbDCResParam.h b/test/periodic/NdbDCResParam.h
new file mode 100644
index 0000000000000000000000000000000000000000..c1640d6f47bf6104891b92d6fcf967d51b9b793a
--- /dev/null
+++ b/test/periodic/NdbDCResParam.h
@@ -0,0 +1,20 @@
+#ifndef DCRESPARAM_H
+#define DCRESPARAM_H
+
+#include "NdbMF.h"
+
+/* ========= NdbDCResParam ============ */
+class NdbDCResParam : public NdbMF
+{
+protected:
+
+public:
+ NdbDCResParam()
+ : NdbMF(32, "Data covariances for resonance parameters") {}
+ ~NdbDCResParam() {}
+
+ ClassDef(NdbDCResParam,1)
+
+}; // NdbDCResParam
+
+#endif
diff --git a/test/periodic/NdbDataCovariances.cxx b/test/periodic/NdbDataCovariances.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..db28827d9798e9ce8ea6f9958bdabd2a022a9ae6
--- /dev/null
+++ b/test/periodic/NdbDataCovariances.cxx
@@ -0,0 +1,3 @@
+#include "NdbDataCovariances.h"
+
+ClassImp(NdbDataCovariances)
diff --git a/test/periodic/NdbDataCovariances.h b/test/periodic/NdbDataCovariances.h
new file mode 100644
index 0000000000000000000000000000000000000000..f13bcfb32133ef91cb6b9d551a8350e9cc0ff13e
--- /dev/null
+++ b/test/periodic/NdbDataCovariances.h
@@ -0,0 +1,22 @@
+#ifndef DATACOVARIANCES_H
+#define DATACOVARIANCES_H
+
+#include "NdbMF.h"
+
+/* ========= NdbDataCovariances ============ */
+class NdbDataCovariances : public NdbMF
+{
+protected:
+
+public:
+ NdbDataCovariances()
+ : NdbMF(30, "Data covariances obtained from parameter "
+ "covariances and sensitivities") {}
+
+ ~NdbDataCovariances() {}
+
+ ClassDef(NdbDataCovariances,1)
+
+}; // NdbDataCovariances
+
+#endif
diff --git a/test/periodic/NdbDefs.h b/test/periodic/NdbDefs.h
new file mode 100644
index 0000000000000000000000000000000000000000..098d9b3df790bc19b389b60d29154bb2f5734885
--- /dev/null
+++ b/test/periodic/NdbDefs.h
@@ -0,0 +1,119 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#ifndef __DEFS_H
+#define __DEFS_H
+
+#ifndef TRUE
+# define FALSE 0
+# define TRUE 1
+#endif
+#ifndef OFF
+# define OFF 0
+# define ON 1
+#endif
+#ifndef NO
+# define NO 0
+# define YES 1
+#endif
+
+#define NOTFOUND -1
+
+#define THERMAL_ENERGY 0.05
+#define MAX_REAL 1e38
+#ifndef PI
+# define PI 3.14159265358979323844
+# define PI2 6.28318530717958647692
+#endif
+#define PIover2 1.57079632679489661923
+#define PIover180 1.74532925199433E-002
+#define PIunder180 5.72957795130823E+001
+#define LN10 2.30258509299405
+#define ONEoverLN10 0.43429448190325
+
+/* --- BIT definitions --- */
+#define MASK1 0x0001
+#define MASK2 0x0003
+#define MASK3 0x0007
+#define MASK4 0x000f
+#define MASK5 0x001f
+#define MASK6 0x003f
+#define MASK7 0x007f
+#define MASK8 0x00ff
+#define MASK9 0x01ff
+#define MASK10 0x03ff
+#define MASK11 0x07ff
+#define MASK12 0x0fff
+#define MASK13 0x1fff
+#define MASK14 0x3fff
+#define MASK15 0x7fff
+#define MASK16 0xffff
+
+#define BIT0 0x0001
+#define BIT1 0x0002
+#define BIT2 0x0004
+#define BIT3 0x0008
+#define BIT4 0x0010
+#define BIT5 0x0020
+#define BIT6 0x0040
+#define BIT7 0x0080
+#define BIT8 0x0100
+#define BIT9 0x0200
+#define BIT10 0x0400
+#define BIT11 0x0800
+#define BIT12 0x1000
+#define BIT13 0x2000
+#define BIT14 0x4000
+#define BIT15 0x8000
+#define BIT16 0x10000L
+
+/* ------------------ comonly used macros -------------------- */
+#define ISPRINT(c) ((c)>=' ' && (c)<='~' && (c)!='\'')
+#define ISSPACE(c) ((c==0x09) || (c==0x0D) || (c==0x20))
+#define HEXVAL(x) (((x)>='A')?((((x)>='a')?((x)&(0xdf)):(x))-'A'+10):((x)-'0'))
+#define CTL(a) (('a') & 0x1f)
+#define ESC ((char)27)
+
+#define SWAP(a,b) a ^= b ^= a ^= b;
+
+#define DIMENSION(p) (sizeof(p) / sizeof(p[0]))
+#define ABS(a) (((a)<0)?-(a):(a))
+
+#ifndef MAX
+# define MAX(a,b) (((a)>(b))?(a):(b))
+# define MIN(a,b) (((a)<(b))?(a):(b))
+#endif
+
+#define MAX3(a,b,c) MAX(MAX(a,b),c)
+#define MAX4(a,b,c,d) MAX(MAX3(a,b,c),d)
+
+#define MIN3(a,b,c) MIN(MIN(a,b),c)
+#define MIN4(a,b,c,d) MIN(MIN3(a,b,c),d)
+
+#define RANGE(a,x,b) ((x)<(a)?(a): ((x)>(b)?(b):(x)))
+#define IN_RANGE(a,x,b) (((a) <= (x)) && ((x) <= (b)))
+
+#define ODD(n) ((n)&1)
+#define EVEN(n) (!((n)&1))
+
+#define TRUNC(a) ((a)>=0? (int)(a) : (int)((a)-1))
+#define ROUND(a) ((a)>=0? (int)((a)+0.5): -(int)(0.5-(a)))
+#define CEILING(a) ((a)==(int)(a)? (int)(a): \
+ (a)>0? (int)(1+(int)(a)): -(int)(1+(int)(-(a))))
+#define FRAC(x) ((x)-(float)((int)(x)))
+#define SIGN(x) ((x)>0? 1:(((x)==0)?0:-1))
+#define SQR(x) ((x)*(x))
+
+#define RAD(a) ((a)*PIover180)
+#define DEG(a) ((a)*PIunder180)
+
+#define COSD(a) cos(RAD(a))
+#define SIND(a) sin(RAD(a))
+#define TAND(a) tan(RAD(a))
+
+#define LOG(x) (log(x)*ONEoverLN10)
+#define EXP10(x) exp((x)*LN10)
+
+#endif
diff --git a/test/periodic/NdbEndfIO.cxx b/test/periodic/NdbEndfIO.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..e24ee97b125af66cca4c3d8a83d9c328588e59fe
--- /dev/null
+++ b/test/periodic/NdbEndfIO.cxx
@@ -0,0 +1,273 @@
+#include <stdlib.h>
+
+#include "NdbEndfIO.h"
+
+#define NUMBER_SIZE 11
+
+char NdbEndfIO::_str[100]; // define static _str var
+
+ClassImp(NdbEndfIO)
+
+/* ============ NdbEndfIO ============== */
+NdbEndfIO::NdbEndfIO( char *filename, Int_t mode )
+{
+ f = fopen(filename,mode==TENDF_READ?"r":"w");
+ matStart = 0;
+ mfStart = 0;
+ mtStart = 0;
+ iMAT = 0;
+ iMF = 0;
+ iMT = 0;
+ lineNum = 0;
+ lineTxt[0] = 0;
+} // NdbEndfIO
+
+
+/* -------- FindMAT --------- */
+// Will search for the specific material
+Bool_t
+NdbEndfIO::FindMAT( Int_t mat, Bool_t rewind )
+{
+ if (rewind)
+ fseek(f, 0L, SEEK_SET);
+
+ while (ReadLine())
+ if (iMAT == mat)
+ return TRUE;
+
+ return FALSE;
+} // FindMAT
+
+/* -------- FindMATMF --------- */
+// Will search for the specific material - mf
+Bool_t
+NdbEndfIO::FindMATMF( Int_t mat, Int_t mf, Bool_t rewind )
+{
+ FindMAT(mat,rewind);
+
+ do {
+ if (iMF == mf)
+ return TRUE;
+ } while (ReadLine());
+
+ return FALSE;
+} // FindMATMF
+
+/* -------- FindMATMFMT --------- */
+// Will search for the specific material - mf - mt
+Bool_t
+NdbEndfIO::FindMATMFMT( Int_t mat, Int_t mf, Int_t mt, Bool_t rewind )
+{
+ FindMATMF(mat,mf,rewind);
+
+ do {
+ if (iMT == mt)
+ return TRUE;
+ } while (ReadLine());
+
+ return FALSE;
+} // FindMATMFMT
+
+/* ------------ FindMFMT ------------- */
+Bool_t
+NdbEndfIO::FindMFMT( Int_t mf, Int_t mt )
+{
+ // If current MFMT is higher than what we search go to the beggining
+ if (mf*1000+mt >= iMF*1000+iMT) {
+ RewindMAT();
+ if (!ReadLine())
+ return FALSE;
+ }
+
+ while (mf*1000+mt > iMF*1000+iMT)
+ if (!ReadLine())
+ return FALSE;
+ return TRUE;
+} // FindMFMT
+
+/* -------- Substr ---------- */
+char *
+NdbEndfIO::Substr(Int_t start, Int_t length)
+{
+ if (start + length > lineLen) {
+// error(ERR_INVALID_RECORD);
+ return NULL;
+ }
+ memcpy(_str, lineTxt+start, length);
+ _str[length] = 0;
+
+ return _str;
+} // Substr
+
+/* -------- NextNumber ---------- */
+/* Advance lastNumber Point to the correct number
+ * so to read 6 numbers of width 11 in each line
+ */
+Bool_t
+NdbEndfIO::NextNumber(Int_t pos)
+{
+ if (pos<0 || pos>5*NUMBER_SIZE) {
+ lastNumPos += NUMBER_SIZE;
+ if (lineTxt[0]=='\0' || lastNumPos>5*NUMBER_SIZE) {
+ Int_t mf = iMF; // Remember current MF, MT
+ Int_t mt = iMT;
+ if (!ReadLine() || (mf*1000+mt != iMF*1000+iMT))
+ return TRUE;
+ lastNumPos = 0;
+ }
+ } else {
+ lastNumPos = pos * NUMBER_SIZE;
+ }
+ return FALSE;
+} // NextNumber
+
+/* -------- SubReadInt ---------- */
+Int_t
+NdbEndfIO::SubReadInt(Int_t start, Int_t length)
+{
+ NdbEndfIO::Substr(start,length);
+ return atoi(_str);
+} // SubReadInt
+
+/* ---------- ReadInt ------------- */
+/* Read one by one the int numbers with length 11 from the current line.
+ * If the this is the last one then it prompts for an new line
+ * only if it stays inside the same MF:MT type
+ */
+Int_t
+NdbEndfIO::ReadInt(Bool_t *error, Int_t pos)
+{
+ if (NextNumber(pos)) {
+ *error = TRUE;
+ return 0;
+ }
+ *error = FALSE;
+ return SubReadInt(lastNumPos,NUMBER_SIZE);
+} // ReadInt
+
+/* -------- SubReadReal ---------- */
+Float_t
+NdbEndfIO::SubReadReal(Int_t start, Int_t length)
+{
+ char numstr[20];
+ char *dst, *src;
+
+ NdbEndfIO::Substr(start,length);
+
+ // Real numbers are in the following formats
+ // +/- N.NNNNNN+/-N
+ // +/- N.NNNNN+/-bN (b=Blank)
+ // +/- N.NNNNN+/-NN
+
+ dst = numstr;
+ src = _str;
+
+ /* skip blanks */
+ while (*src==' ') src++;
+
+ /* copy sign */
+ if (*src=='+' || *src=='-') *dst++ = *src++;
+
+ /* copy realpart */
+ while (1) {
+ if (memchr(".0123456789",*src,11))
+ *dst++ = *src++;
+ else
+ break;
+ }
+
+ /* append the exponent */
+ *dst++ = 'E';
+
+ /* copy sign */
+ if (*src=='+' || *src=='-') *dst++ = *src++;
+
+ /* skip blanks */
+ while (*src==' ') src++;
+
+ /* copy exponent */
+ while (1) {
+ if (memchr("0123456789",*src,10))
+ *dst++ = *src++;
+ else
+ break;
+ }
+
+ /* close the destination */
+ *dst = 0;
+
+ /* if something is still in source then we have an error number */
+ if (*src) {
+// error(ERR_INVALID_REAL_NUMBER);
+ return 0.0;
+ }
+
+ return atof(numstr);
+} // SubReadReal
+
+/* ---------- ReadReal ------------- */
+/* Read one by one the real numbers with length 11 from the current line.
+ * If the this is the last one then it prompts for an new line
+ * only if it stays inside the same MF:MT type
+ */
+Float_t
+NdbEndfIO::ReadReal(Bool_t *error, Int_t pos)
+{
+ if (NextNumber(pos)) {
+ *error = TRUE;
+ return 0.0;
+ }
+ *error = FALSE;
+ return SubReadReal(lastNumPos,NUMBER_SIZE);
+} // ReadReal
+
+/* -------- ReadLine -------- */
+Bool_t
+NdbEndfIO::ReadLine()
+{
+ Long_t current_pos;
+
+ // --- Force the next number reading to be from the beggining of line
+ lastNumPos = -NUMBER_SIZE;
+
+ // --- Have we reached the end of file
+ if (feof(f)) {
+ lineTxt[0] = 0;
+ return FALSE;
+ }
+
+ // --- Remember the position of start of line ---
+ current_pos = ftell(f);
+
+ // --- Read one line ---
+ fgets(lineTxt,sizeof(lineTxt),f);
+
+ lineLen = strlen(lineTxt);
+
+ // Chop the trailing newline char
+ if (lineTxt[lineLen-1] == '\n')
+ lineTxt[--lineLen] = 0;
+
+ // --- Remember previous values ---
+ Int_t oldMAT = iMAT;
+ Int_t oldMF = iMF;
+ Int_t oldMT = iMT;
+
+ // --- Read the material, mf, mt and line number ---
+ iMAT = SubReadInt(66, 4);
+ iMF = SubReadInt(70, 2);
+ iMT = SubReadInt(72, 3);
+ lineNum = SubReadInt(75, 5);
+
+ // --- Update pointers if necessary ---
+ if (iMAT && iMAT != oldMAT)
+ matStart = current_pos;
+
+ if (iMF && iMF != oldMF)
+ mfStart = current_pos;
+
+ if (iMT && iMT != oldMT)
+ mtStart = current_pos;
+
+ return TRUE;
+} // ReadLine
diff --git a/test/periodic/NdbEndfIO.h b/test/periodic/NdbEndfIO.h
new file mode 100644
index 0000000000000000000000000000000000000000..63203903e46d24129e8397247fe2e47b589b804c
--- /dev/null
+++ b/test/periodic/NdbEndfIO.h
@@ -0,0 +1,139 @@
+#ifndef __ENDFIO_H
+#define __ENDFIO_H
+
+#include <stdio.h>
+#include <string.h>
+
+#include <TObject.h>
+
+#include "NdbDefs.h"
+
+// I/O Options
+enum {
+ TENDF_READ=1,
+ TENDF_WRITE=2
+};
+
+#define TENDF_NEXT_NUMBER -1
+#define TENDF_MAXREC 100
+
+// End records
+enum {
+ SEND=1,
+ FEND=2,
+ MEND=3,
+ TEND=4
+};
+
+class NdbEndfIO : public TObject
+{
+ // ================== NdbEndfIO ===================
+ // This class is handling all the input/output
+ // to an ENDF-B/VI file
+ //
+protected:
+ FILE *f; //! Working file
+ Int_t mode; // Open mode
+ Int_t iMAT; // Material number
+ Int_t iMF; // Current file type
+ Int_t iMT; // Current section
+ Int_t lineNum; // Keep track of current line
+
+ Long_t matStart; // Pointer of the current
+ // material starting pos
+ Long_t mfStart; // Current MF starting pos
+ Long_t mtStart; // Current MT starting pos
+
+ Int_t lineLen; // Length of line
+ char lineTxt[TENDF_MAXREC]; // Complete line
+ Int_t lastNumPos; // for readReal and readInt;
+ static char _str[TENDF_MAXREC]; // Used for substrings
+
+public:
+ NdbEndfIO() { f=NULL; }
+ virtual ~NdbEndfIO()
+ { if (f) fclose(f); }
+
+ NdbEndfIO( char *filename, Int_t mode);
+
+ NdbEndfIO( NdbEndfIO *endf ) {
+ f = endf->f;
+ mode = endf->mode;
+ iMAT = endf->iMAT;
+ iMF = endf->iMF;
+ iMF = endf->iMT;
+ matStart= endf->matStart;
+ mfStart = endf->mfStart;
+ mtStart = endf->mtStart;
+ lineNum = endf->lineNum;
+ lineLen = endf->lineLen;
+ strcpy(lineTxt, endf->lineTxt);
+ }
+
+
+ // Access functions
+ inline Int_t LineNumber() const { return lineNum; }
+ inline char *Line() { return lineTxt; }
+ inline Int_t MAT() const { return iMAT; }
+ inline Int_t MF() const { return iMF; }
+ inline Int_t MT() const { return iMT; }
+
+ // Is the file open?
+ inline Bool_t IsOpen() { return (f!=NULL); }
+
+ // Have we reached End of file?
+ inline Bool_t Eof() { return feof(f); }
+
+ // End of Section
+ inline Bool_t EOMT() { return (iMT==0); }
+
+ // End of MF
+ inline Bool_t EOMF() { return (iMF==0); }
+
+ // End of MATerial
+ inline Bool_t EOMAT() { return (iMAT==0); }
+
+ // Find Material
+ Bool_t FindMAT( Int_t mat, Bool_t rewind=FALSE );
+
+ // Find File inside material
+ Bool_t FindMATMF( Int_t mat, Int_t mf, Bool_t rewind=FALSE );
+
+ // Find Section
+ Bool_t FindMATMFMT( Int_t mat, Int_t mf, Int_t mt,
+ Bool_t rewind=FALSE );
+
+ // Find the specific MF:MT file:section, for current MAT
+ Bool_t FindMFMT(Int_t mf, Int_t mt);
+
+ // Rewind to beggining of current material
+ Bool_t RewindMAT() { return fseek(f, matStart, SEEK_SET); }
+
+ // Rewind to beggining of current file (MF)
+ Bool_t RewindMF() { return fseek(f, mfStart, SEEK_SET); }
+
+ // Rewind to beggining of current section (MT)
+ Bool_t RewindMT() { return fseek(f, mtStart, SEEK_SET); }
+
+ // Read entire line
+ Bool_t ReadLine();
+
+ // Reads one by one the real numbers from the current line
+ Int_t ReadInt(Bool_t *error, Int_t pos=TENDF_NEXT_NUMBER);
+
+ Float_t ReadReal(Bool_t *error, Int_t pos=TENDF_NEXT_NUMBER);
+
+ // Return a substring of current line in a static variable
+ char* Substr(Int_t start, Int_t length);
+
+protected:
+ Bool_t NextNumber(Int_t pos=TENDF_NEXT_NUMBER);
+ Int_t SubReadInt(Int_t start, Int_t length);
+ Float_t SubReadReal(Int_t start, Int_t length);
+
+
+ ClassDef(NdbEndfIO,1)
+
+}; // NdbEndfIO
+
+#endif
diff --git a/test/periodic/NdbEnergyAngleDist.cxx b/test/periodic/NdbEnergyAngleDist.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..8e1d060deeb6f88b618dce1accb377e8a32f3c13
--- /dev/null
+++ b/test/periodic/NdbEnergyAngleDist.cxx
@@ -0,0 +1,3 @@
+#include "NdbEnergyAngleDist.h"
+
+ClassImp(NdbEnergyAngleDist)
diff --git a/test/periodic/NdbEnergyAngleDist.h b/test/periodic/NdbEnergyAngleDist.h
new file mode 100644
index 0000000000000000000000000000000000000000..e0505a1c1d3ed516d176cfadd7b78a1aeeb6aed1
--- /dev/null
+++ b/test/periodic/NdbEnergyAngleDist.h
@@ -0,0 +1,21 @@
+#ifndef ENERGYANGLEDIST_H
+#define ENERGYANGLEDIST_H
+
+#include "NdbMF.h"
+
+/* ========= NdbEnergyAngleDist ============ */
+class NdbEnergyAngleDist : public NdbMF
+{
+protected:
+
+public:
+ NdbEnergyAngleDist()
+ : NdbMF(6, "Energy-angle distributions for emitted particles") {}
+
+ ~NdbEnergyAngleDist() {}
+
+ ClassDef(NdbEnergyAngleDist,1)
+
+}; // NdbEnergyAngleDist
+
+#endif
diff --git a/test/periodic/NdbEnergyDist.cxx b/test/periodic/NdbEnergyDist.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..e3cc73efeec2a7ebdb9720a4a20ba06c6b29886b
--- /dev/null
+++ b/test/periodic/NdbEnergyDist.cxx
@@ -0,0 +1,3 @@
+#include "NdbEnergyDist.h"
+
+ClassImp(NdbEnergyDist)
diff --git a/test/periodic/NdbEnergyDist.h b/test/periodic/NdbEnergyDist.h
new file mode 100644
index 0000000000000000000000000000000000000000..f9b3f93fea6f084979260ac0f2cb322210bd563c
--- /dev/null
+++ b/test/periodic/NdbEnergyDist.h
@@ -0,0 +1,21 @@
+#ifndef ENERGYDIST_H
+#define ENERGYDIST_H
+
+#include "NdbMF.h"
+
+/* ========= NdbEnergyDist ============ */
+class NdbEnergyDist : public NdbMF
+{
+protected:
+
+public:
+ NdbEnergyDist()
+ : NdbMF(5, "Energy distributions for emitted particles") {}
+
+ ~NdbEnergyDist() {}
+
+ ClassDef(NdbEnergyDist,1)
+
+}; // NdbEnergyDist
+
+#endif
diff --git a/test/periodic/NdbFissionYield.cxx b/test/periodic/NdbFissionYield.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..7ec03f3e2dd2d31669f5387cfc5b81dfd90a0420
--- /dev/null
+++ b/test/periodic/NdbFissionYield.cxx
@@ -0,0 +1,4 @@
+#include "NdbFissionYield.h"
+
+ClassImp(NdbFissionYield)
+
diff --git a/test/periodic/NdbFissionYield.h b/test/periodic/NdbFissionYield.h
new file mode 100644
index 0000000000000000000000000000000000000000..dc4c67d461e6883a56aca3eb194b389fdc3fc0e6
--- /dev/null
+++ b/test/periodic/NdbFissionYield.h
@@ -0,0 +1,20 @@
+#ifndef FISSIONYIELD_H
+#define FISSIONYIELD_H
+
+#include "NdbMF.h"
+
+/* ========= NdbFissionYield ============ */
+class NdbFissionYield : public NdbMF
+{
+protected:
+
+public:
+ NdbFissionYield()
+ : NdbMF(8, "Radioactivity and fission-product yield data") {}
+ ~NdbFissionYield() {}
+
+ ClassDef(NdbFissionYield,1)
+
+}; // NdbFissionYield
+
+#endif
diff --git a/test/periodic/NdbFormFactors.cxx b/test/periodic/NdbFormFactors.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..29c8ba38035fbb43ccd0fa3308f14c9ae666779d
--- /dev/null
+++ b/test/periodic/NdbFormFactors.cxx
@@ -0,0 +1,3 @@
+#include "NdbFormFactors.h"
+
+ClassImp(NdbFormFactors)
diff --git a/test/periodic/NdbFormFactors.h b/test/periodic/NdbFormFactors.h
new file mode 100644
index 0000000000000000000000000000000000000000..44ad3f107185e1a6ec92ababb0e96552ce747c90
--- /dev/null
+++ b/test/periodic/NdbFormFactors.h
@@ -0,0 +1,21 @@
+#ifndef MFFORMFACTORS_H
+#define MFFORMFACTORS_H
+
+#include "NdbMF.h"
+
+/* ========= NdbFormFactors ============ */
+class NdbFormFactors : public NdbMF
+{
+protected:
+
+public:
+ NdbFormFactors()
+ : NdbMF(27, "Atomic form factors or scattering functions "
+ "for photo-atomic interactions") {}
+ ~NdbFormFactors() {}
+
+ ClassDef(NdbFormFactors,1)
+
+}; // NdbFormFactors
+
+#endif
diff --git a/test/periodic/NdbGeneralInfo.cxx b/test/periodic/NdbGeneralInfo.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..a902d75034f2fb4eabbe95655f36608e1a389361
--- /dev/null
+++ b/test/periodic/NdbGeneralInfo.cxx
@@ -0,0 +1,4 @@
+#include "NdbGeneralInfo.h"
+
+ClassImp(NdbGeneralInfo)
+
diff --git a/test/periodic/NdbGeneralInfo.h b/test/periodic/NdbGeneralInfo.h
new file mode 100644
index 0000000000000000000000000000000000000000..5769dacb3905805f7da1bb8036332cf425906c6a
--- /dev/null
+++ b/test/periodic/NdbGeneralInfo.h
@@ -0,0 +1,21 @@
+#ifndef GENERALINFO_H
+#define GENERALINFO_H
+
+#include "NdbMF.h"
+
+/* ========= NdbGeneralInfo ============ */
+class NdbGeneralInfo : public NdbMF
+{
+protected:
+
+public:
+ NdbGeneralInfo()
+ : NdbMF(1, "General Information") {}
+
+ ~NdbGeneralInfo() {}
+
+ ClassDef(NdbGeneralInfo,1)
+
+}; // NdbGeneralInfo
+
+#endif
diff --git a/test/periodic/NdbLinkDef.h b/test/periodic/NdbLinkDef.h
new file mode 100644
index 0000000000000000000000000000000000000000..fa9b65c493528d170bb539cdae19c18e14e61770
--- /dev/null
+++ b/test/periodic/NdbLinkDef.h
@@ -0,0 +1,42 @@
+#ifdef __CINT__
+
+#pragma link off all globals;
+#pragma link off all classes;
+#pragma link off all functions;
+
+#pragma link C++ class NdbAngularDist;
+#pragma link C++ class NdbDCAngularDist;
+#pragma link C++ class NdbDCEnergyDist;
+#pragma link C++ class NdbDCNuBar;
+#pragma link C++ class NdbDCRadioXS;
+#pragma link C++ class NdbDCRadioYield;
+#pragma link C++ class NdbMF;
+#pragma link C++ class NdbMT;
+#pragma link C++ class NdbEndfIO;
+#pragma link C++ class NdbDCReactionXS;
+#pragma link C++ class NdbDCResParam;
+#pragma link C++ class NdbDataCovariances;
+#pragma link C++ class NdbEnergyAngleDist;
+#pragma link C++ class NdbEnergyDist;
+#pragma link C++ class NdbFissionYield;
+#pragma link C++ class NdbFormFactors;
+#pragma link C++ class NdbGeneralInfo;
+#pragma link C++ class NdbMTDir;
+#pragma link C++ class NdbMTReactionXS;
+#pragma link C++ class NdbMTReacDesc;
+#pragma link C++ class NdbMaterial;
+#pragma link C++ class NdbParticle;
+#pragma link C++ class NdbParticleList;
+#pragma link C++ class NdbPhotonAngleDist;
+#pragma link C++ class NdbPhotonEnergyDist;
+#pragma link C++ class NdbPhotonInteractionXS;
+#pragma link C++ class NdbPhotonMult;
+#pragma link C++ class NdbPhotonProdXS;
+#pragma link C++ class NdbRadioMult;
+#pragma link C++ class NdbRadioXS;
+#pragma link C++ class NdbReaction;
+#pragma link C++ class NdbResParam;
+#pragma link C++ class NdbThermalNeutron;
+
+
+#endif
diff --git a/test/periodic/NdbMF.cxx b/test/periodic/NdbMF.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..cf9f65f956352492f280a437802fe2efdb84539c
--- /dev/null
+++ b/test/periodic/NdbMF.cxx
@@ -0,0 +1,50 @@
+#include "NdbMF.h"
+
+ClassImp(NdbMF)
+
+#include <Riostream.h>
+
+/* -------- Section -------- */
+NdbMT *
+NdbMF::Section(Int_t id)
+{
+ TObjArrayIter iter(&aSection);
+ while (iter()) {
+ NdbMT *mt = (NdbMT*)(iter.Next());
+ if (mt->MT() == id)
+ return mt;
+ }
+ return NULL;
+} // Section
+
+/* -------- Section -------- */
+NdbMT *
+NdbMF::Section(const char *name )
+{
+ TObjArrayIter iter(&aSection);
+ while (iter()) {
+ NdbMT *mt = (NdbMT*)(iter.Next());
+ if (mt->Description().CompareTo(name))
+ return mt;
+ }
+ return NULL;
+} // Section
+
+/* ---------- Add ---------- */
+void
+NdbMF::Add(NdbMT& )
+{
+ cout << "NdbMF::add(sec)" << endl;
+} // Add
+
+/* ---------- EnumerateENDFType ---------- */
+/* Enumerates all the available sections inside the ENDF file
+ * @param sec Find the next section after <B>sec</B>
+ * @return Next available section in ENDF file, -1 if EOF
+ */
+Int_t
+NdbMF::EnumerateENDFType( Int_t )
+{
+ cout << "NdbMF ::enumerateENDFSection" << endl;
+ return 0;
+} // EnumerateENDFType
diff --git a/test/periodic/NdbMF.h b/test/periodic/NdbMF.h
new file mode 100644
index 0000000000000000000000000000000000000000..2ebee4c96b066f22a61d8a9cca465125e797619b
--- /dev/null
+++ b/test/periodic/NdbMF.h
@@ -0,0 +1,57 @@
+#ifndef NDBMF_H
+#define NDBMF_H
+
+#include <TObject.h>
+#include <TString.h>
+#include <TObjArray.h>
+
+#include "NdbMT.h"
+
+/* ================== NdbMF =================== */
+/*
+ * Base class for the File Types (MF)
+ */
+class NdbMF: public TObject
+{
+protected:
+ Int_t iMF; // MF number
+ TString sDescription; // Description of the File TYPE (MF)
+ TObjArray aSection; // Array of sections (MT)
+
+public:
+ NdbMF( Int_t aMF, const char *aDesc)
+ : TObject(), sDescription(aDesc), aSection() {
+ iMF = aMF;
+ }
+
+ ~NdbMF() {}
+
+ // Virtual functions
+ virtual Int_t Compare(const TObject *o) const
+ { return ((iMF==((NdbMF*)o)->iMF)? 0 :
+ (iMF > ((NdbMF*)o)->iMF)? 1 : -1 ); }
+
+ // Access functions
+ inline Int_t MF() const { return iMF; }
+ inline TString Description() const { return sDescription; }
+
+ // Find Section, by type
+ NdbMT* Section(Int_t id);
+
+ // Find Section by name
+ NdbMT* Section(const char *name);
+
+ // Add a new section in the section list
+ void Add(NdbMT& sec);
+
+ // Enumerate sections in ENDF file
+ Int_t EnumerateENDFType( Int_t sec );
+
+ // Move File pointer to beggining of MF section in ENDF file
+ void LocateType() {}
+
+ ClassDef(NdbMF,1)
+
+}; // NdbMF
+
+#endif
diff --git a/test/periodic/NdbMT.cxx b/test/periodic/NdbMT.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..37f391c7b21d159f042b751c08cf871978c1ae1a
--- /dev/null
+++ b/test/periodic/NdbMT.cxx
@@ -0,0 +1,3 @@
+#include "NdbMT.h"
+
+ClassImp(NdbMT);
diff --git a/test/periodic/NdbMT.h b/test/periodic/NdbMT.h
new file mode 100644
index 0000000000000000000000000000000000000000..85fca543ca690d535990cf6decca2aec2eed76c4
--- /dev/null
+++ b/test/periodic/NdbMT.h
@@ -0,0 +1,58 @@
+#ifndef MT_H
+#define MT_H
+
+#ifndef ROOT_TObject
+# include <TObject.h>
+#endif
+
+#ifndef ROOT_TString
+# include <TString.h>
+#endif
+
+#include <stdio.h>
+
+/* ================== NdbMT =================== */
+/*
+ * Defines the basic object for Sections of a File Type
+ */
+class NdbMT: public TObject
+{
+protected:
+ Int_t iMT; // MT number
+ TString sDescription;
+
+public:
+ NdbMT( Int_t aMT, const char *desc)
+ : sDescription(desc) { iMT = aMT; }
+
+ ~NdbMT() {}
+
+ // Virtual functions
+ virtual Int_t Compare(const TObject *o) const
+ { return ((iMT == ((NdbMT*)o)->iMT)? 0 :
+ (iMT > ((NdbMT*)o)->iMT)? 1 : -1 ); }
+
+ // Access functions
+ inline Int_t MT() const { return iMT; }
+ inline TString Description() const { return sDescription; }
+
+ // Assign a working file
+
+ // Enumerate sections in ENDF file
+ Int_t EnumerateENDFSection( Int_t /* sec */) {return 0;}
+
+ // Move File pointer to beggining of MT section in ENDF file
+ void LocateENDFSection() {}
+
+ // END of ENDF Section reached?
+ Bool_t ENDF_EOS() {return 0;}
+
+ // Abstract functions (or Virtual?)
+ virtual void ReadENDFSectionHeader() {}
+ virtual void ReadENDFSection() {}
+
+ ClassDef(NdbMT,1)
+
+}; // NdbMT
+
+#endif
diff --git a/test/periodic/NdbMTDir.cxx b/test/periodic/NdbMTDir.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..505122839c17fd417a0fa229c9b06f5d49034eae
--- /dev/null
+++ b/test/periodic/NdbMTDir.cxx
@@ -0,0 +1,108 @@
+#include <stdlib.h>
+#include <string.h>
+
+#include "NdbDefs.h"
+#include "NdbEndfIO.h"
+#include "NdbMTDir.h"
+
+ClassImp(NdbMTDir);
+
+/* ========= NdbMTDir ======== */
+NdbMTDir::~NdbMTDir( )
+{
+ if (ZSYMAM) free(ZSYMAM);
+ if (ALAB) free(ALAB);
+ if (EDATE) free(EDATE);
+ if (AUTH) free(AUTH);
+ if (REF) free(REF);
+ if (DDATE) free(DDATE);
+ if (RDATE) free(RDATE);
+ if (ENDATE) free(ENDATE);
+} // ~NdbMTDir
+
+/* -------- LoadENDF -------- */
+Bool_t
+NdbMTDir::LoadENDF( char *filename )
+{
+ Bool_t error;
+
+ NdbEndfIO endf(filename,TENDF_READ);
+
+ if (!endf.IsOpen()) return kTRUE;
+
+ endf.FindMFMT(1,MT());
+
+ ZA = endf.ReadReal(&error);
+ AWR = endf.ReadReal(&error);
+ LRP = endf.ReadInt(&error);
+ LFI = endf.ReadInt(&error);
+ NLIB = endf.ReadInt(&error);
+ NMOD = endf.ReadInt(&error);
+
+ ELIS = endf.ReadReal(&error);
+ STA = endf.ReadInt(&error);
+ LIS = endf.ReadInt(&error);
+ LISO = endf.ReadInt(&error);
+ endf.ReadInt(&error); // Skip one number
+ NFOR = endf.ReadInt(&error);
+
+ AWI = endf.ReadReal(&error);
+ endf.ReadReal(&error); // Skip three number
+ endf.ReadInt(&error);
+ endf.ReadInt(&error);
+ NSUB = endf.ReadInt(&error);
+ NVER = endf.ReadInt(&error);
+
+ TEMP = endf.ReadReal(&error);
+ endf.ReadReal(&error);
+ LDRV = endf.ReadInt(&error);
+ endf.ReadInt(&error); // Skip one number
+ NWD = endf.ReadInt(&error);
+ NXC = endf.ReadInt(&error);
+
+//
+// Author, Dates, etc, skip 'em for the moment
+//
+ endf.ReadLine();
+ ZSYMAM = strdup(endf.Substr(0,11));
+ ALAB = strdup(endf.Substr(11,10));
+ EDATE = strdup(endf.Substr(22,10));
+ AUTH = strdup(endf.Substr(33,33));
+ endf.ReadLine();
+ REF = strdup(endf.Substr(1,20));
+ DDATE = strdup(endf.Substr(22,10));
+ RDATE = strdup(endf.Substr(33,10));
+ ENDATE = strdup(endf.Substr(55,6));
+
+// Skip comments
+ for (int i=0; i<NWD-2; i++) {
+ endf.ReadLine();
+ INFO.Append(endf.Substr(0,66));
+ INFO.Append("\n");
+ }
+//printf("ZSYMAM=\"%s\"\n",ZSYMAM);
+//printf("ALAB=\"%s\"\n",ALAB);
+//printf("EDATE=\"%s\"\n",EDATE);
+//printf("AUTH=\"%s\"\n",AUTH);
+//printf("REF=\"%s\"\n",REF);
+//printf("DDATE=\"%s\"\n",DDATE);
+//printf("RDATE=\"%s\"\n",RDATE);
+//printf("ENDATE=\"%s\"\n",ENDATE);
+//printf("INFO=\"%s\"\n",INFO.Data());
+
+ dir_mf.Set(NXC);
+ dir_mt.Set(NXC);
+ dir_mc.Set(NXC);
+ dir_mod.Set(NXC);
+
+ endf.ReadLine();
+ for (int i=0; i<NXC; i++) {
+ dir_mf.AddAt(endf.ReadInt(&error,2), i);
+ dir_mt.AddAt(endf.ReadInt(&error), i);
+ dir_mc.AddAt(endf.ReadInt(&error), i);
+ dir_mod.AddAt(endf.ReadInt(&error), i);
+ endf.ReadLine();
+//printf("MF=%d MT=%d MC=%d\n",dir_mf[i], dir_mt[i], dir_mc[i]);
+ }
+ return kFALSE;
+} // LoadENDF
diff --git a/test/periodic/NdbMTDir.h b/test/periodic/NdbMTDir.h
new file mode 100644
index 0000000000000000000000000000000000000000..be620da26fda70c10e7bbc106670d1652d6b9991
--- /dev/null
+++ b/test/periodic/NdbMTDir.h
@@ -0,0 +1,87 @@
+#ifndef MTDIRXS_H
+#define MTDIRXS_H
+
+#include <TArrayI.h>
+
+#include "NdbDefs.h"
+#include "NdbMT.h"
+#include "NdbMaterial.h"
+
+/* ========= NdbMTDir ============ */
+class NdbMTDir : public NdbMT
+{
+protected:
+ Float_t ZA;
+ Float_t AWR;
+ Int_t LRP; // Flag for resonances in MF=2
+ Int_t LFI; // Whether this material fissions
+ Int_t NLIB; // Library
+ Int_t NVER; // Version
+ Int_t NFOR; // Format
+ Float_t ELIS; // Excitation energy
+ Int_t STA; // Stability flag
+ Int_t LIS; // Ground state
+ Int_t LISO; // Isomeric state number
+ Int_t NMOD; // Modification number
+ Float_t AWI; // Mass in neutron units
+ Int_t NSUB; // Sublibrary number
+ Float_t TEMP; // Target temperature
+ Int_t LDRV; // Special Derived material flag
+ Int_t NWD; // Number of records
+ Int_t NXC; // Number of records in the dir.
+ char *ZSYMAM; //! Symbol
+ char *ALAB; //! Laboratory mnemonic
+ char *EDATE; //! Evaluation date
+ char *AUTH; //! Authors name
+ char *REF; //! Primary reference
+ char *DDATE; //! Distribution date
+ char *RDATE; //! Date&Number of last revision
+ char *ENDATE; //! Master entry date yymmdd
+ TString INFO;
+
+
+ TArrayI dir_mf; // Directory entries
+ TArrayI dir_mt;
+ TArrayI dir_mc;
+ TArrayI dir_mod;
+
+public:
+ NdbMTDir()
+ : NdbMT(451,"Descriptive Data and Directory")
+ {
+ NXC = 0;
+ ZSYMAM = NULL;
+ ALAB = NULL;
+ EDATE = NULL;
+ AUTH = NULL;
+ REF = NULL;
+ DDATE = NULL;
+ RDATE = NULL;
+ ENDATE = NULL;
+ }
+
+ ~NdbMTDir();
+
+ // --- Input/Output routines ---
+ Bool_t LoadENDF(char *filename);
+
+ inline Int_t Sections() const { return NXC; }
+ inline Int_t DIRMF(Int_t i) { return dir_mf[i]; }
+ inline Int_t DIRMT(Int_t i) { return dir_mt[i]; }
+ inline Int_t DIRMC(Int_t i) { return dir_mc[i]; }
+ inline Int_t DIRMOD(Int_t i) { return dir_mod[i]; }
+
+ inline char* SymbolName() { return ZSYMAM; }
+ inline char* Laboratory() { return ALAB; }
+ inline char* EvaluationDate() { return EDATE;}
+ inline char* Author() { return AUTH; }
+ inline char* Reference() { return REF; }
+ inline char* DistributionDate() { return DDATE; }
+ inline char* LastRevisionDate() { return RDATE; }
+ inline char* MasterEntryDate() { return ENDATE; }
+ inline TString GetInfo() { return INFO; }
+
+ ClassDef(NdbMTDir,1)
+}; // NdbMTDir
+
+#endif
diff --git a/test/periodic/NdbMTReacDesc.cxx b/test/periodic/NdbMTReacDesc.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..2218b655069c868bf96f4bc6138d3b610bd9475a
--- /dev/null
+++ b/test/periodic/NdbMTReacDesc.cxx
@@ -0,0 +1,150 @@
+#include <ctype.h>
+#include <stdio.h>
+#include <stdlib.h>
+
+#include "NdbMTReacDesc.h"
+
+ClassImp(NdbMTReacDesc)
+
+/* ================ NdbMTReacDesc ================== */
+NdbMTReacDesc::NdbMTReacDesc(const char *filename)
+{
+ Init(filename);
+} // NdbMTReacDesc
+
+/* ------- ~NdbMTReacDesc ------- */
+NdbMTReacDesc::~NdbMTReacDesc()
+{
+ if (shrt) {
+ for (int i=0; i<mt.GetSize(); i++) {
+ if (shrt[i]) free(shrt[i]);
+ if (desc[i]) free(desc[i]);
+ if (comment[i]) free(comment[i]);
+ }
+ free(shrt);
+ free(desc);
+ free(comment);
+ }
+} // ~NdbMTReacDesc
+
+/* ------ Init ------ */
+void
+NdbMTReacDesc::Init(const char *filename)
+{
+ shrt = NULL;
+ desc = NULL;
+ comment = NULL;
+
+ FILE *f;
+
+ if ((f=fopen(filename,"r"))==NULL) {
+ fprintf(stderr,"ERROR: NdbMTReacDesc::NdbMTReacDesc(%s) cannot open file.\n",filename);
+ return;
+ }
+
+ /* ----- First read total number of MT's ------ */
+ Int_t N;
+
+ fscanf(f,"%d",&N);
+ if (N<=0) {
+ fprintf(stderr,"ERROR: NdbMTReacDesc::NdbMTReacDesc(%s) error reading from file.\n",filename);
+ fclose(f);
+ }
+
+ /* ----- Allocate memory ----- */
+ mt.Set(N);
+ shrt = (char **)malloc(N * sizeof(char*));
+ desc = (char **)malloc(N * sizeof(char*));
+ comment = (char **)malloc(N * sizeof(char*));
+
+ for (int i=0; i<N; i++) {
+ /* --- read mt number and short description --- */
+ Int_t mt_num, ch;
+ char str[512], str2[256];
+
+ fscanf(f,"%d",&mt_num);
+
+ mt.AddAt(mt_num,i);
+
+ /* --- skip blanks --- */
+ do {} while (isspace(ch=fgetc(f)));
+ ungetc(ch,f);
+
+ /* get rest of line */
+ fgets(str,sizeof(str),f);
+
+ /* --- strip last newline char --- */
+ str[strlen(str)-1] = 0;
+
+ shrt[i] = strdup(str);
+
+ /* --- Read the description line until the empty line --- */
+ str[0] = 0;
+ while (1) {
+ fgets(str2,sizeof(str2),f);
+ if (str2[0] == '\n') break;
+ strcat(str,str2);
+ }
+ str[strlen(str)-1] = 0;
+ desc[i] = strdup(str);
+
+ /* --- Read the description line until the empty line --- */
+ str[0] = 0;
+ while (1) {
+ fgets(str2,sizeof(str2),f);
+ if (str2[0] == '\n') break;
+ strcat(str,str2);
+ }
+ str[strlen(str)-1] = 0;
+ comment[i] = strdup(str);
+ }
+ fclose(f);
+} // NdbMTReacDesc
+
+/* ------- FindMT -------- */
+Int_t
+NdbMTReacDesc::FindMT( Int_t MT )
+{
+ /* Make a linear search */
+ if (shrt)
+ for (int i=0; i<mt.GetSize(); i++)
+ if (mt[i] == MT)
+ return i;
+ else
+ if (mt[i] > MT)
+ break;
+ return -1;
+} // FindMT
+
+/* ------- GetShort -------- */
+char *
+NdbMTReacDesc::GetShort(Int_t MT)
+{
+ Int_t idx = FindMT(MT);
+ if (idx<0)
+ return NULL;
+
+ return shrt[idx];
+} // GetShort
+
+/* ------- GetDescription -------- */
+char *
+NdbMTReacDesc::GetDescription(Int_t MT)
+{
+ Int_t idx = FindMT(MT);
+ if (idx<0)
+ return NULL;
+
+ return desc[idx];
+} // GetDescription
+
+/* ------- GetComment -------- */
+char *
+NdbMTReacDesc::GetComment(Int_t MT)
+{
+ Int_t idx = FindMT(MT);
+ if (idx<0)
+ return NULL;
+
+ return comment[idx];
+} // GetComment
diff --git a/test/periodic/NdbMTReacDesc.h b/test/periodic/NdbMTReacDesc.h
new file mode 100644
index 0000000000000000000000000000000000000000..79d26ecf885f53dc61812886ada17351ee0b849b
--- /dev/null
+++ b/test/periodic/NdbMTReacDesc.h
@@ -0,0 +1,47 @@
+#ifndef NDB_REACDESC_H
+#define NDB_REACDESC_H
+
+#include <TArrayI.h>
+
+#include "NdbDefs.h"
+#include "NdbMF.h"
+#include "NdbMT.h"
+#include "NdbParticleList.h"
+#include "NdbMaterial.h"
+
+/* ========= NdbMTReactionXS ============ */
+// This class provides the descriptions and comments of all the reactions
+// that are available in MF=3
+class NdbMTReacDesc : public TObject
+{
+protected:
+ TArrayI mt; // MT number
+ char **shrt; //! Short description (n,f)
+ char **desc; //! Long description
+ char **comment; //! Comments on reaction
+
+public:
+ NdbMTReacDesc() {
+ shrt = NULL;
+ desc = NULL;
+ comment = NULL;
+ }
+ NdbMTReacDesc(const char *filename);
+ ~NdbMTReacDesc();
+
+ void Init(const char *filename);
+
+ // --- Access functions ---
+ inline Int_t GetSize() const { return mt.GetSize(); }
+ inline Int_t MT(Int_t i) { return mt[i]; }
+
+ Int_t FindMT(Int_t MT);
+ char* GetShort(Int_t MT);
+ char* GetDescription(Int_t MT);
+ char* GetComment(Int_t MT);
+
+ ClassDef(NdbMTReacDesc,1)
+
+}; // NdbMTReacDesc
+
+#endif
diff --git a/test/periodic/NdbMTReactionXS.cxx b/test/periodic/NdbMTReactionXS.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..76347455a7bbfc0314925994de3da8a6dab2e736
--- /dev/null
+++ b/test/periodic/NdbMTReactionXS.cxx
@@ -0,0 +1,116 @@
+#include <Riostream.h>
+
+#include "NdbDefs.h"
+#include "NdbEndfIO.h"
+#include "NdbMTReactionXS.h"
+
+ClassImp(NdbMTReactionXS);
+
+/* -------- LoadENDF -------- */
+Bool_t
+NdbMTReactionXS::LoadENDF( char *filename )
+{
+ NdbEndfIO endf(filename,TENDF_READ);
+ Int_t za;
+ Float_t awr;
+ Bool_t error;
+
+ if (!endf.IsOpen()) return kTRUE;
+
+ minxs = MAX_REAL;
+ maxxs = -MAX_REAL;
+
+ endf.FindMFMT(3,MT()); // Find total cross section
+ za = (int)endf.ReadReal(&error); // ??
+ awr = endf.ReadReal(&error);
+ endf.ReadLine();
+ QM = endf.ReadReal(&error);
+ QI = endf.ReadReal(&error);
+ endf.ReadInt(&error); // Skip number
+
+ LR = endf.ReadInt(&error); if (error) return error;
+ NR = endf.ReadInt(&error); if (error) return error;
+ NP = endf.ReadInt(&error); if (error) return error;
+ endf.ReadLine(); // Skip line
+
+ IT = endf.ReadInt(&error,2); // Interpolation type
+ endf.ReadLine(); // Skip line
+
+ ene.Set(NP);
+ xs.Set(NP);
+
+ for (int i=0; i<NP; i++) {
+ Float_t f;
+ ene.AddAt(endf.ReadReal(&error), i);
+ xs.AddAt( f = endf.ReadReal(&error), i);
+ minxs = MIN(minxs,f);
+ maxxs = MAX(maxxs,f);
+ }
+ return kFALSE;
+} // loadENDF
+
+/* -------- BinSearch -------- */
+Int_t
+NdbMTReactionXS::BinSearch( Float_t e )
+{
+ Int_t low = 0;
+ Int_t high = NP-1;
+ Int_t mid;
+
+ if (e < ene[low]) return NOTFOUND;
+ if (e > ene[high]) return NOTFOUND;
+
+ while (1) {
+ mid = (low+high)/2;
+ if (mid==low) return mid;
+ if (e > ene[mid])
+ low = mid;
+ else
+ if (e < ene[mid])
+ high = mid;
+ else
+ return mid;
+ }
+} // BinSearch
+
+/* -------- Interpolate -------- */
+Float_t
+NdbMTReactionXS::Interpolate( Float_t e )
+{
+ Int_t p = BinSearch(e);
+
+ if (p==NOTFOUND)
+ return xs[ e<ene[0]? 0 : NP-1 ];
+
+ if (p==NP-1)
+ return xs[p];
+
+ Float_t el = ene[p];
+ Float_t xl = xs[p];
+ p++;
+
+ switch (IT) {
+ case IT_LINLOG:
+ cout << "Linear-Log interpolation" << endl;
+ return 0.0;
+
+ case IT_LOGLIN:
+ cout << "Log-Linear interpolation" << endl;
+ return 0.0;
+
+ case IT_LOGLOG:
+ cout << "Log-Log interpolation" << endl;
+ return 0.0;
+
+ case IT_GAMOW:
+ cout << "GAMOW interpolation" << endl;
+ return 0.0;
+
+ case IT_LINLIN:
+ return xs[p] + (e-el) * (xs[p]-xl) / (ene[p]-el);
+
+ default:
+ break;
+ }
+ return 0.0;
+} // interpolate
diff --git a/test/periodic/NdbMTReactionXS.h b/test/periodic/NdbMTReactionXS.h
new file mode 100644
index 0000000000000000000000000000000000000000..a07d74b393bd0d41636bd430435a7b69a758ef89
--- /dev/null
+++ b/test/periodic/NdbMTReactionXS.h
@@ -0,0 +1,78 @@
+#ifndef REACTIONXS_H
+#define REACTIONXS_H
+
+#include <TArrayF.h>
+
+#include "NdbDefs.h"
+#include "NdbMF.h"
+#include "NdbMT.h"
+#include "NdbParticleList.h"
+#include "NdbMaterial.h"
+
+// --- Interpolation types ----
+#define IT_HISTOGRAM 1
+#define IT_LINLIN 2
+#define IT_LINLOG 3
+#define IT_LOGLIN 4
+#define IT_LOGLOG 5
+#define IT_GAMOW 6
+
+/* ========= NdbMTReactionXS ============ */
+class NdbMTReactionXS : public NdbMT
+{
+protected:
+ TArrayF ene; // Energy in eV
+ TArrayF xs; // Cross section in barn
+
+ Float_t minxs, // Minimum and
+ maxxs; // Maximum limits of XS
+
+ NdbParticle projectile; // Projectile particle
+ NdbParticleList daugthers; // Reaction products
+ NdbMaterial residual; // Residual nucleus
+ Double_t QM; // Mass-difference Q value (eV)
+ Double_t QI; // reaction Q for the lowest
+ // energy state
+ Int_t LR; // Complex or "breakup" flag.
+ Int_t NP; // No. Points (x,y)
+ Int_t NR; // interpolation regions
+ Int_t IT; // Interpolation type
+
+public:
+ NdbMTReactionXS(int aMt, const char *desc)
+ : NdbMT(aMt,desc) {
+ LR = -1;
+ NP = -1;
+ NR = -1;
+ minxs = maxxs = 0.0;
+ }
+ ~NdbMTReactionXS() {}
+
+ // --- Access functions ---
+ inline Float_t Energy(int i) { return ene[i]; }
+ inline Float_t XS(int i) { return xs[i]; }
+
+ inline Int_t Pairs() const { return NP; }
+ inline Int_t InterpolationType() const { return IT; }
+ inline Int_t InterpolationRegions() const { return NR; }
+ inline Float_t MassDifference() const { return QM; }
+ inline Float_t ReactionQ() const { return QI; }
+
+ // --- Input/Output routines ---
+ Bool_t LoadENDF(char *filename);
+
+ // --- Interpolation routines ---
+ Int_t BinSearch( Float_t e);
+ Float_t Interpolate(Float_t e);
+
+ // --- Limits ---
+ inline Float_t MinEnergy() { return ene[0]; }
+ inline Float_t MaxEnergy() { return ene[NP-1]; }
+ inline Float_t MinXS() const { return minxs; }
+ inline Float_t MaxXS() const { return maxxs; }
+
+ ClassDef(NdbMTReactionXS,1)
+
+}; // NdbMTReactionXS
+
+#endif
diff --git a/test/periodic/NdbMaterial.cxx b/test/periodic/NdbMaterial.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..df779adca6ee7b47ec332156bfec1c58e9f62f97
--- /dev/null
+++ b/test/periodic/NdbMaterial.cxx
@@ -0,0 +1,3 @@
+#include "NdbMaterial.h"
+
+ClassImp(NdbMaterial)
diff --git a/test/periodic/NdbMaterial.h b/test/periodic/NdbMaterial.h
new file mode 100644
index 0000000000000000000000000000000000000000..95d47436caa847b173b21a3fa74275c15cc6f99b
--- /dev/null
+++ b/test/periodic/NdbMaterial.h
@@ -0,0 +1,106 @@
+#ifndef MATERIAL_H
+#define MATERIAL_H
+
+#include <TObject.h>
+#include <TString.h>
+
+//////////////// NdbMaterial /////////////////
+class NdbMaterial : public TObject
+{
+protected:
+ TString eMnemonic; // Mnemonic of the element XX-AAAii
+ TString eName; // Name of isotope "Gold"
+ Long_t eId; // AZ code = Z*10000 + A*10 + ISO
+ Int_t eZ; // Z = number of protons
+ Int_t eA; // A = mass number
+ Int_t eIS; // Isomeric state of element
+ Float_t eMass; // Mass of the element
+ Float_t eMassExcess; // M-A
+ Float_t eHalfLife; // Half life
+ Float_t eAbundance; // Percentage of natural isotope
+ Float_t eDensity; // Density of element
+ Float_t eMeltingPoint; // Melting point in K
+ Float_t eBoilingPoint; // Boiling point in K
+
+// TDecayMode eDecayMode; // Decay mode of element
+
+ TObjArray *mf; // Array of File types
+
+public:
+ NdbMaterial() {}
+
+ NdbMaterial(
+ const char *aName,
+ const char *aMnemonic,
+ Int_t aZ,
+ Int_t anA,
+ Int_t anIso=0,
+ Float_t aMass=0.0,
+ Float_t aMassExcess=0.0,
+ Float_t aHalfLife=0.0,
+ Float_t aAbundance=0.0,
+ Float_t aDensity=0.0,
+ Float_t aMeltingPoint=0.0,
+ Float_t aBoilingPoint=0.0)
+ : TObject(), eMnemonic(aMnemonic), eName(aName) {
+ eZ = aZ;
+ eA = anA;
+ eIS = anIso;
+ eId = eZ*10000 + eA*10 + eIS;
+ if (aMass!=0.0)
+ eMass = aMass;
+ else
+ eMass = (Float_t)anA;
+ eMassExcess = aMassExcess;
+ eAbundance = aAbundance;
+ eHalfLife = aHalfLife;
+ eDensity = aDensity;
+ eMeltingPoint = aMeltingPoint;
+ eBoilingPoint = aBoilingPoint;
+ }
+
+ NdbMaterial( NdbMaterial& elem )
+ : TObject(), eName(elem.eName)
+ {
+ eZ = elem.eZ;
+ eA = elem.eA;
+ eIS = elem.eIS;
+ eId = elem.eId;
+ eMass = elem.eMass;
+ eMassExcess = elem.eMassExcess;
+ eDensity = elem.eDensity;
+ eMeltingPoint = elem.eMeltingPoint;
+ eBoilingPoint = elem.eBoilingPoint;
+ eAbundance = elem.eAbundance;
+ eHalfLife = elem.eHalfLife;
+ eMeltingPoint = elem.eMeltingPoint;
+ eBoilingPoint = elem.eBoilingPoint;
+ }
+
+ ~NdbMaterial() {}
+
+ // --- Virtual functions ---
+ Int_t Compare(const TObject *o) const
+ { return ((eId==((NdbMaterial*)o)->eId)? 0 :
+ (eId > ((NdbMaterial*)o)->eId)? 1 : -1 ); }
+
+ // --- Access functions ---
+ inline TString Name() const { return eName; }
+ inline TString Mnemonic() const { return eMnemonic; }
+ inline Long_t Id() const { return eId; }
+ inline Int_t A() const { return eA; }
+ inline Int_t Z() const { return eZ; }
+ inline Int_t ISO() const { return eIS; }
+ inline Float_t Mass() const { return eMass; }
+ inline Float_t MassExcess() const { return eMassExcess; }
+ inline Float_t HalfLife() const { return eHalfLife; }
+ inline Float_t Abundance() const { return eAbundance; }
+ inline Float_t Density() const { return eDensity; }
+ inline Float_t MeltingPoint() const { return eMeltingPoint; }
+ inline Float_t BoilingPoint() const { return eBoilingPoint; }
+
+ ClassDef(NdbMaterial,1)
+
+}; // NdbMaterial
+
+#endif
diff --git a/test/periodic/NdbParticle.cxx b/test/periodic/NdbParticle.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..e40c759ceb19dd70a866584e601f5e2b62703a3c
--- /dev/null
+++ b/test/periodic/NdbParticle.cxx
@@ -0,0 +1,3 @@
+#include "NdbParticle.h"
+
+ClassImp(NdbParticle)
diff --git a/test/periodic/NdbParticle.h b/test/periodic/NdbParticle.h
new file mode 100644
index 0000000000000000000000000000000000000000..a316196a2db3fb6d4f3a98b28157f90be4421df9
--- /dev/null
+++ b/test/periodic/NdbParticle.h
@@ -0,0 +1,70 @@
+#ifndef PARTICLE_H
+#define PARTICLE_H
+
+#include <TObject.h>
+#include <TString.h>
+
+/* ------------- Particle Types ---------------- */
+enum ParticleType {
+ PTGamma,
+ PTNeutron,
+ PTAntiNeutron,
+ PTNeutrino,
+ PTAntiNeutrino,
+ PTProton,
+ PTAntiProton,
+ PTElectron,
+ PTPositron,
+ PTPionPlus,
+ PTPionMinus,
+ PTMuonPlus,
+ PTMuonMinus,
+ PTKaonPlus,
+ PTKaonMinus,
+ PTKaonLong,
+ PTKaonShort,
+ PTKaonZero,
+ PTLambda,
+ PTAlpha
+};
+
+/* ------------ Particle Class ---------------- */
+class NdbParticle : public TObject
+{
+protected:
+ Long_t pId; // Unique id of each particle
+ TString pName; // Particle Name
+ TString pMnemonic; // Particle Mnemonic
+ ParticleType pType; // Type of particle
+ Int_t pCharge; // Particle charge
+ Float_t pMass; // mass in MeV/c^2
+ Float_t pHalfLife; // Half life in sec.
+
+public:
+ NdbParticle() { pId = -1; }
+
+ NdbParticle(
+ const char *aName,
+ ParticleType aType,
+ long anId = 0)
+ : TObject(), pName(aName)
+ {
+ pType = aType;
+ pId = anId;
+ }
+
+ ~NdbParticle() {}
+
+ // --- Access Functions ---
+ inline TString Name() const { return pName; }
+ inline TString Mnemonic() const { return pMnemonic; }
+ inline Long_t Id() const { return pId; }
+ inline Float_t Mass() const { return pMass; }
+ inline Float_t HalfLife() const { return pHalfLife; }
+ inline Int_t Charge() const { return pCharge; }
+
+ ClassDef(NdbParticle,1)
+
+}; // NdbParticle
+
+#endif
diff --git a/test/periodic/NdbParticleList.cxx b/test/periodic/NdbParticleList.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..d5c22a7448f9731e3d3710bc029d66ca5ad7165d
--- /dev/null
+++ b/test/periodic/NdbParticleList.cxx
@@ -0,0 +1,53 @@
+#include <stdlib.h>
+#include <Riostream.h>
+#include "NdbParticleList.h"
+
+ClassImp(NdbParticleList)
+
+/* -------- TotalCharge -------- */
+Int_t
+NdbParticleList::TotalCharge()
+{
+ Int_t charge = 0;
+
+ for (int i=0; i<mult.GetSize(); i++)
+ charge += ((NdbParticle*)part[i])->Charge() * mult[i];
+
+ return charge;
+} // TotalCharge
+
+/* -------- TotalMass -------- */
+Float_t
+NdbParticleList::TotalMass()
+{
+ Float_t mass = 0.0;
+
+ for (int i=0; i<mult.GetSize(); i++)
+ mass += ((NdbParticle*)part[i])->Mass() * mult[i];
+
+ return mass;
+} // TotalMass
+
+/* -------- Name -------- */
+TString
+NdbParticleList::Name()
+{
+ TString nm;
+
+ for (int i=0; i<mult.GetSize(); i++) {
+ if (mult[i]>1) {
+ char num[10];
+ sprintf(num,"%d",mult[i]);
+ nm.Append(num);
+ }
+ nm.Append(((NdbParticle*)part[i])->Name());
+ }
+ return nm;
+} // Name
+
+/* --------- Add --------- */
+void
+NdbParticleList::Add(NdbParticle *, Int_t)
+{
+ cout << "NdbParticleList::add()" << endl;
+} // Add
diff --git a/test/periodic/NdbParticleList.h b/test/periodic/NdbParticleList.h
new file mode 100644
index 0000000000000000000000000000000000000000..f4083a6e0557b14f6fca65c465045a10e7ada2d9
--- /dev/null
+++ b/test/periodic/NdbParticleList.h
@@ -0,0 +1,32 @@
+#ifndef PARTICLELIST_H
+#define PARTICLELIST_H
+
+#include <TArrayI.h>
+#include <TObjArray.h>
+
+#include "NdbParticle.h"
+
+/* ------------ Particle List ---------------- */
+class NdbParticleList : public TObject
+{
+protected:
+ TArrayI mult; // How many times each particle occurs
+ TObjArray part; // Link to particle types
+
+public:
+ NdbParticleList() : mult(), part() { }
+ ~NdbParticleList() {}
+
+ // --- Access Functions ---
+ Int_t TotalCharge(); // Total charge
+ Float_t TotalMass(); // Total mass
+ TString Name(); // string containing the name
+ // in a format like 2np
+
+ void Add(NdbParticle *p, Int_t n=1);
+
+ ClassDef(NdbParticleList,1)
+
+}; // NdbParticleList
+
+#endif
diff --git a/test/periodic/NdbPhotonAngleDist.cxx b/test/periodic/NdbPhotonAngleDist.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..5b56f1f127d499754dc72d3fd0be24e706fa843a
--- /dev/null
+++ b/test/periodic/NdbPhotonAngleDist.cxx
@@ -0,0 +1,4 @@
+#include "NdbPhotonAngleDist.h"
+
+ClassImp(NdbPhotonAngleDist)
+
diff --git a/test/periodic/NdbPhotonAngleDist.h b/test/periodic/NdbPhotonAngleDist.h
new file mode 100644
index 0000000000000000000000000000000000000000..b54e60d83237d99d42288099a234f0de51a2c827
--- /dev/null
+++ b/test/periodic/NdbPhotonAngleDist.h
@@ -0,0 +1,20 @@
+#ifndef PHOTONANGLEDIST_H
+#define PHOTONANGLEDIST_H
+
+#include "NdbMF.h"
+
+/* ========= NdbPhotonAngleDist ============ */
+class NdbPhotonAngleDist : public NdbMF
+{
+protected:
+
+public:
+ NdbPhotonAngleDist()
+ : NdbMF(14, "Angular distributions for photon production") {}
+
+ ~NdbPhotonAngleDist() {}
+
+ ClassDef(NdbPhotonAngleDist,1)
+}; // NdbPhotonAngleDist
+
+#endif
diff --git a/test/periodic/NdbPhotonEnergyDist.cxx b/test/periodic/NdbPhotonEnergyDist.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..3a3a198ab49df51b610410dac7021b84a1931d71
--- /dev/null
+++ b/test/periodic/NdbPhotonEnergyDist.cxx
@@ -0,0 +1,4 @@
+#include "NdbPhotonEnergyDist.h"
+
+ClassImp(NdbPhotonEnergyDist)
+
diff --git a/test/periodic/NdbPhotonEnergyDist.h b/test/periodic/NdbPhotonEnergyDist.h
new file mode 100644
index 0000000000000000000000000000000000000000..abe49e280571f9a0b0e87ede7a0ce18c2b0e6f90
--- /dev/null
+++ b/test/periodic/NdbPhotonEnergyDist.h
@@ -0,0 +1,19 @@
+#ifndef PHOTONENERGYDIST_H
+#define PHOTONENERGYDIST_H
+
+#include "NdbMF.h"
+
+/* ========= NdbPhotonEnergyDist ============ */
+class NdbPhotonEnergyDist : public NdbMF
+{
+protected:
+
+public:
+ NdbPhotonEnergyDist()
+ : NdbMF(15, "Energy distributions for photon production") {}
+ ~NdbPhotonEnergyDist() {}
+
+ ClassDef(NdbPhotonEnergyDist,1)
+}; // NdbPhotonEnergyDist
+
+#endif
diff --git a/test/periodic/NdbPhotonInteractionXS.cxx b/test/periodic/NdbPhotonInteractionXS.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..e4f7c0132038925712fea16389a4a36ee7cfd53e
--- /dev/null
+++ b/test/periodic/NdbPhotonInteractionXS.cxx
@@ -0,0 +1,4 @@
+#include "NdbPhotonInteractionXS.h"
+
+ClassImp(NdbPhotonInteractionXS)
+
diff --git a/test/periodic/NdbPhotonInteractionXS.h b/test/periodic/NdbPhotonInteractionXS.h
new file mode 100644
index 0000000000000000000000000000000000000000..a40bafb617468acdf403fb005bc550bbbdbbb808
--- /dev/null
+++ b/test/periodic/NdbPhotonInteractionXS.h
@@ -0,0 +1,19 @@
+#ifndef PHOTONINTERACTIONXS_H
+#define PHOTONINTERACTIONXS_H
+
+#include "NdbMF.h"
+
+/* ========= NdbPhotonInteractionXS ============ */
+class NdbPhotonInteractionXS : public NdbMF
+{
+protected:
+
+public:
+ NdbPhotonInteractionXS()
+ : NdbMF(23, "Photo-atomic interaction cross sections") {}
+ ~NdbPhotonInteractionXS() {}
+
+ ClassDef(NdbPhotonInteractionXS,1)
+}; // NdbPhotonInteractionXS
+
+#endif
diff --git a/test/periodic/NdbPhotonMult.cxx b/test/periodic/NdbPhotonMult.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..cfd94c3afea629c7ec2ca12d10d6a66aba0fafbe
--- /dev/null
+++ b/test/periodic/NdbPhotonMult.cxx
@@ -0,0 +1,4 @@
+#include "NdbPhotonMult.h"
+
+ClassImp(NdbPhotonMult)
+
diff --git a/test/periodic/NdbPhotonMult.h b/test/periodic/NdbPhotonMult.h
new file mode 100644
index 0000000000000000000000000000000000000000..2cb4f2250f83dddd3c9ae292722c192bb6ba40b9
--- /dev/null
+++ b/test/periodic/NdbPhotonMult.h
@@ -0,0 +1,19 @@
+#ifndef PHOTONMULT_H
+#define PHOTONMULT_H
+
+#include "NdbMF.h"
+
+/* ========= NdbPhotonMult ============ */
+class NdbPhotonMult : public NdbMF
+{
+protected:
+
+public:
+ NdbPhotonMult()
+ : NdbMF(12, "Multiplicities for photon production") {}
+ ~NdbPhotonMult() {}
+
+ ClassDef(NdbPhotonMult,1)
+}; // NdbPhotonMult
+
+#endif
diff --git a/test/periodic/NdbPhotonProdXS.cxx b/test/periodic/NdbPhotonProdXS.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..637fb4e300a2416f503ee6a222573c3bd4c37dc4
--- /dev/null
+++ b/test/periodic/NdbPhotonProdXS.cxx
@@ -0,0 +1,4 @@
+#include "NdbPhotonProdXS.h"
+
+ClassImp(NdbPhotonProdXS)
+
diff --git a/test/periodic/NdbPhotonProdXS.h b/test/periodic/NdbPhotonProdXS.h
new file mode 100644
index 0000000000000000000000000000000000000000..0c169d1157ed89afa7ade2e0d8d4a9fcc8d81f17
--- /dev/null
+++ b/test/periodic/NdbPhotonProdXS.h
@@ -0,0 +1,20 @@
+#ifndef PHOTONPRODXS_H
+#define PHOTONPRODXS_H
+
+#include "NdbMF.h"
+
+/* ========= NdbPhotonProdXS ============ */
+class NdbPhotonProdXS : public NdbMF
+{
+protected:
+
+public:
+ NdbPhotonProdXS()
+ : NdbMF(13, "Cross sections for photon production") {}
+
+ ~NdbPhotonProdXS() {}
+
+ ClassDef(NdbPhotonProdXS,1)
+}; // NdbPhotonProdXS
+
+#endif
diff --git a/test/periodic/NdbRadioMult.cxx b/test/periodic/NdbRadioMult.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..7431b3fbc2b31f522969bc2ce5ed3f8461367e5e
--- /dev/null
+++ b/test/periodic/NdbRadioMult.cxx
@@ -0,0 +1,3 @@
+#include "NdbRadioMult.h"
+
+ClassImp(NdbRadioMult)
diff --git a/test/periodic/NdbRadioMult.h b/test/periodic/NdbRadioMult.h
new file mode 100644
index 0000000000000000000000000000000000000000..56e0ab8fe3119c48d09e69e9f8600d9f99c46cd2
--- /dev/null
+++ b/test/periodic/NdbRadioMult.h
@@ -0,0 +1,19 @@
+#ifndef RADIOMULT_H
+#define RADIOMULT_H
+
+#include "NdbMF.h"
+
+/* ========= NdbRadioMult ============ */
+class NdbRadioMult : public NdbMF
+{
+protected:
+
+public:
+ NdbRadioMult()
+ : NdbMF(9, "Multiplicities for radioactive nuclide production") {}
+ ~NdbRadioMult() {}
+
+ ClassDef(NdbRadioMult,1)
+}; // NdbRadioMult
+
+#endif
diff --git a/test/periodic/NdbRadioXS.cxx b/test/periodic/NdbRadioXS.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..4dd51078f01fd7f513709546ce8ab05aa0409de8
--- /dev/null
+++ b/test/periodic/NdbRadioXS.cxx
@@ -0,0 +1,4 @@
+#include "NdbRadioXS.h"
+
+ClassImp(NdbRadioXS)
+
diff --git a/test/periodic/NdbRadioXS.h b/test/periodic/NdbRadioXS.h
new file mode 100644
index 0000000000000000000000000000000000000000..52b617e7e28a4cc5066308d898fd8071ba7c1b45
--- /dev/null
+++ b/test/periodic/NdbRadioXS.h
@@ -0,0 +1,20 @@
+#ifndef RADIOXS_H
+#define RADIOXS_H
+
+#include "NdbMF.h"
+
+/* ========= NdbRadioXS ============ */
+class NdbRadioXS : public NdbMF
+{
+protected:
+
+public:
+ NdbRadioXS()
+ : NdbMF(10, "Cross section for radioactive nuclide production") {}
+
+ ~NdbRadioXS() {}
+
+ ClassDef(NdbRadioXS,1)
+}; // NdbRadioXS
+
+#endif
diff --git a/test/periodic/NdbReaction.cxx b/test/periodic/NdbReaction.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..5f6b85ebfc56b8c15f69f74d540efe8877cd8b3e
--- /dev/null
+++ b/test/periodic/NdbReaction.cxx
@@ -0,0 +1,3 @@
+#include "NdbReaction.h"
+
+ClassImp(NdbReaction)
diff --git a/test/periodic/NdbReaction.h b/test/periodic/NdbReaction.h
new file mode 100644
index 0000000000000000000000000000000000000000..50251ab99d976aabaf70fb0c57092d6922e6acc6
--- /dev/null
+++ b/test/periodic/NdbReaction.h
@@ -0,0 +1,25 @@
+#ifndef REACTION_H
+#define REACTION_H
+
+#include <TObjArray.h>
+
+#include "NdbMF.h"
+#include "NdbMTReactionXS.h"
+#include "NdbParticleList.h"
+
+/* ========= NdbReaction ============ */
+class NdbReaction : public NdbMF
+{
+protected:
+ TObjArray reac; // List of reaction Cross Sections
+
+public:
+ NdbReaction()
+ : NdbMF(3, "Reaction cross sections"),
+ reac() { }
+ ~NdbReaction() {}
+
+ ClassDef(NdbReaction,1)
+}; // NdbReaction
+
+#endif
diff --git a/test/periodic/NdbResParam.cxx b/test/periodic/NdbResParam.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..2a32dbe7ecdfbeb18d49a36330f1dbeeaa95e510
--- /dev/null
+++ b/test/periodic/NdbResParam.cxx
@@ -0,0 +1,4 @@
+#include "NdbResParam.h"
+
+ClassImp(NdbResParam)
+
diff --git a/test/periodic/NdbResParam.h b/test/periodic/NdbResParam.h
new file mode 100644
index 0000000000000000000000000000000000000000..dc91fe2b59d08f77da1afde72fc7689d95ef0f44
--- /dev/null
+++ b/test/periodic/NdbResParam.h
@@ -0,0 +1,19 @@
+#ifndef RESPARAM_H
+#define RESPARAM_H
+
+#include "NdbMF.h"
+
+/* ============= NdbResParam ============== */
+class NdbResParam : public NdbMF
+{
+protected:
+
+public:
+ NdbResParam()
+ : NdbMF(2, "Resonance prameter data") {}
+ ~NdbResParam() {}
+
+ ClassDef(NdbResParam,1)
+}; // NdbResParam
+
+#endif
diff --git a/test/periodic/NdbThermalNeutron.cxx b/test/periodic/NdbThermalNeutron.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..625bd98eb24447ce05c4665c86d6da20ee65c1ea
--- /dev/null
+++ b/test/periodic/NdbThermalNeutron.cxx
@@ -0,0 +1,4 @@
+#include "NdbThermalNeutron.h"
+
+ClassImp(NdbThermalNeutron)
+
diff --git a/test/periodic/NdbThermalNeutron.h b/test/periodic/NdbThermalNeutron.h
new file mode 100644
index 0000000000000000000000000000000000000000..ac2e54e0290deab460b7f582cc35e5c61431169b
--- /dev/null
+++ b/test/periodic/NdbThermalNeutron.h
@@ -0,0 +1,20 @@
+#ifndef THERMALNEUTRON_H
+#define THERMALNEUTRON_H
+
+#include "NdbMF.h"
+
+/* ========= NdbThermalNeutron ============ */
+class NdbThermalNeutron : public NdbMF
+{
+protected:
+
+public:
+ NdbThermalNeutron()
+ : NdbMF(7, "Thermal neutron scattering law data") {}
+
+ ~NdbThermalNeutron() {}
+
+ ClassDef(NdbThermalNeutron,1)
+}; // NdbThermalNeutron
+
+#endif
diff --git a/test/periodic/README b/test/periodic/README
new file mode 100644
index 0000000000000000000000000000000000000000..7d01837afdf14c6505cf65818101ebc222c9011d
--- /dev/null
+++ b/test/periodic/README
@@ -0,0 +1,18 @@
+ROOT GUI demo showing a very nice periodic system and element selection panel
+-----------------------------------------------------------------------------
+
+Use "make" to compile the project.
+
+After make you will have a program XSGui. Execute this program and select
+from the menubar the option "Element/Reaction". To get the periodic system
+click on the little icon in the top right of the "Select Element/Reaction"
+panel.
+
+For H (isotope 1) and Pb (isotopes 208 and natural) the reactions
+can be plotted. Select a reaction and click on "Ok" or "Execute".
+
+This is a code snapshot of a project in development so not much more can
+be done, but it shows execellent use of the ROOT GUI.
+
+The author is:
+ Vasilis Vlachoudis <Vasilis.Vlachoudis@cern.ch>
diff --git a/test/periodic/XSElementDlg.cxx b/test/periodic/XSElementDlg.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..8f5c9b94edd3fc2b0488327cc498a34195bbfc00
--- /dev/null
+++ b/test/periodic/XSElementDlg.cxx
@@ -0,0 +1,231 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#include <ctype.h>
+#include <stdlib.h>
+
+#include <TGTab.h>
+#include <TGFrame.h>
+#include <TGButton.h>
+#include <TGWindow.h>
+#include <TGButton.h>
+#include <TGMsgBox.h>
+
+#include "XSElementList.h"
+#include "XSPeriodicTable.h"
+#include "XSElementDlg.h"
+
+//ClassImp(XSElementDlg)
+
+enum XSElementDlgEnum {
+ ELEM_OK=900,
+ ELEM_CANCEL
+ };
+
+static Int_t activeTab=0; // Remember last active Tab
+static Int_t LastWinX = -1;
+static Int_t LastWinY = -1;
+
+
+/* ----- XSElementDlg ----- */
+XSElementDlg::XSElementDlg( const TGWindow *p, const TGWindow *main,
+ UInt_t *retZ, UInt_t w, UInt_t h)
+ : TGTransientFrame(p,main,w,h)
+{
+ selectedZ = retZ; // Save Address
+
+ lHints = new TGLayoutHints( kLHintsTop | kLHintsLeft |
+ kLHintsExpandX | kLHintsExpandY,
+ 2, 2, 2, 2);
+
+ buttonFrame = new TGHorizontalFrame(this, 120, 20, kFixedWidth);
+ okButton = new TGTextButton(buttonFrame, "&Ok", ELEM_OK);
+ okButton->Associate(this);
+ closeButton = new TGTextButton(buttonFrame, "&Close", ELEM_CANCEL);
+ closeButton->Associate(this);
+
+ buttonLayoutHints = new TGLayoutHints(
+ kLHintsTop | kLHintsLeft | kLHintsExpandX,
+ 2, 2, 5, 1);
+ buttonFrame->AddFrame(okButton, buttonLayoutHints);
+ buttonFrame->AddFrame(closeButton, buttonLayoutHints);
+
+ frameLayoutHints = new TGLayoutHints(kLHintsBottom | kLHintsRight,
+ 2, 2, 2, 2);
+ AddFrame(buttonFrame, frameLayoutHints);
+
+ // ---------- Add Periodic table -------------
+ TGCompositeFrame *tf;
+ tabMenu = new TGTab(this, w, h);
+
+ tf = tabMenu->AddTab("Periodic Table");
+
+ pTable = new XSPeriodicTable(this,tf,w,h);
+ pTable->SelectZ(*selectedZ);
+ tf->AddFrame(pTable, lHints);
+
+ // ------------- Table Sorted by Name ------------
+ tf = tabMenu->AddTab("Name");
+
+ nameFrame = new TGCompositeFrame(tf,w,h, kVerticalFrame);
+ nameListBox = new XSElementList(nameFrame,XSEL_SORTBY_NAME);
+ nameListBox->SelectZ(*selectedZ);
+ nameFrame->AddFrame(nameListBox,lHints);
+
+ tf->AddFrame(nameFrame,lHints);
+
+ // ------------- Table Sorted by Mnemonic -------------
+ tf = tabMenu->AddTab("Mnemonic");
+
+ mnemonicFrame = new TGCompositeFrame(tf,w,h,kVerticalFrame);
+ mnemonicListBox = new XSElementList(mnemonicFrame,XSEL_SORTBY_MNEMONIC);
+ mnemonicListBox->SelectZ(*selectedZ);
+ mnemonicFrame->AddFrame(mnemonicListBox, lHints);
+
+ tf->AddFrame(mnemonicFrame, lHints);
+
+ // ------------- Table Sorted by Charge -------------
+ tf = tabMenu->AddTab("Z (Charge)");
+
+ zFrame = new TGCompositeFrame(tf,w,h,kVerticalFrame);
+ zListBox = new XSElementList(zFrame,XSEL_SORTBY_Z);
+ zListBox->SelectZ(*selectedZ);
+ zFrame->AddFrame(zListBox, lHints);
+ tf->AddFrame(zFrame, lHints);
+
+ // ------------- Finalise settings -----------------
+ lHints2 = new TGLayoutHints(
+ kLHintsBottom | kLHintsExpandX | kLHintsExpandY,
+ 2, 2, 5, 1);
+ AddFrame(tabMenu, lHints2);
+
+ tabMenu->SetTab(activeTab);
+
+ /* --------- Set Windows Position --------- */
+ int ax, ay;
+ if (LastWinX == -1) { // Go to the middle of parent window
+ Window_t wdum;
+ gVirtualX->TranslateCoordinates(main->GetId(), GetParent()->GetId(),
+ (((TGFrame *) main)->GetWidth() - fWidth) >> 1,
+ (((TGFrame *) main)->GetHeight() - fHeight) >> 1,
+ ax, ay, wdum);
+ } else {
+ ax = LastWinX;
+ ay = LastWinY;
+ }
+ Move(ax,ay);
+ SetWMPosition(ax,ay);
+
+ MapSubwindows();
+ Resize(GetDefaultSize());
+ SetWindowName("Select Element");
+ MapWindow();
+
+ fClient->WaitFor(this);
+} // XSElementDlg
+
+/* ----- ~XSElementDlg ----- */
+XSElementDlg::~XSElementDlg()
+{
+ activeTab = tabMenu->GetCurrent();
+
+ delete closeButton;
+ delete buttonFrame;
+ delete buttonLayoutHints;
+ delete frameLayoutHints;
+ delete lHints;
+ delete tabMenu;
+ delete pTable;
+ delete nameListBox;
+ delete nameFrame;
+ delete mnemonicListBox;
+ delete mnemonicFrame;
+ delete zListBox;
+ delete zFrame;
+ delete lHints2;
+} // ~XSElementDlg
+
+/* ----- CloseWindow ----- */
+void
+XSElementDlg::CloseWindow()
+{
+ // --- Remember old position ---
+ Window_t wdum;
+ gVirtualX->TranslateCoordinates(GetId(), GetParent()->GetId(),
+ 0, 0, LastWinX, LastWinY, wdum);
+
+ delete this;
+} // CloseWindow
+
+/* ----- ProcessButton ----- */
+Bool_t
+XSElementDlg::ProcessButton(Long_t param)
+{
+ Int_t activeTab;
+
+ switch (param) {
+ case ELEM_OK:
+ // Find active Tab
+ activeTab = tabMenu->GetCurrent();
+ if (activeTab==0)
+ goto LERROR;
+ else {
+ switch (activeTab) {
+ case 1:
+ *selectedZ =
+ nameListBox->CurrentZ();
+ break;
+ case 2:
+ *selectedZ =
+ mnemonicListBox->CurrentZ();
+ break;
+ case 3:
+ *selectedZ =
+ zListBox->CurrentZ();
+ break;
+ }
+ if (*selectedZ==0)
+ goto LERROR;
+ }
+ break;
+
+ case ELEM_CANCEL:
+ *selectedZ = 0;
+ break;
+ default:
+ *selectedZ = param;
+ break;
+ }
+ CloseWindow();
+ return kTRUE;
+
+LERROR:
+ // Issue a message to select an Element
+ int retval;
+ new TGMsgBox(fClient->GetRoot(), this, "Info",
+ "Please Select one Element!",
+ kMBIconAsterisk, kMBOk, &retval );
+ return kFALSE;
+} // ProcessButton
+
+/* ----- ProcessMessage ----- */
+Bool_t
+XSElementDlg::ProcessMessage(Long_t msg, Long_t param1, Long_t /*param2*/)
+{
+ switch (GET_MSG(msg)) {
+ case kC_COMMAND:
+ switch (GET_SUBMSG(msg)) {
+ case kCM_BUTTON:
+ ProcessButton(param1);
+ break;
+
+ default:
+ break;
+ }
+ default:
+ break;
+ }
+ return kTRUE;
+} // ProcessMessage
diff --git a/test/periodic/XSElementDlg.h b/test/periodic/XSElementDlg.h
new file mode 100644
index 0000000000000000000000000000000000000000..900b5340ed76707e0a73e0434a8f906d4c81b7da
--- /dev/null
+++ b/test/periodic/XSElementDlg.h
@@ -0,0 +1,52 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#ifndef __XSELEMENT_DLG_H
+#define __XSELEMENT_DLG_H
+
+#include <TGTab.h>
+#include <TGFrame.h>
+#include <TGButton.h>
+#include <TGLayout.h>
+
+#include "XSElementList.h"
+#include "XSPeriodicTable.h"
+
+/* =========== XSElementDlg ============== */
+class XSElementDlg : public TGTransientFrame
+{
+private:
+ UInt_t *selectedZ;
+
+ XSPeriodicTable *pTable;
+ TGTab *tabMenu;
+ TGButton *okButton,
+ *closeButton;
+ TGCompositeFrame *buttonFrame,
+ *nameFrame,
+ *mnemonicFrame,
+ *zFrame;
+ XSElementList *nameListBox,
+ *mnemonicListBox,
+ *zListBox;
+ TGLayoutHints *buttonLayoutHints,
+ *frameLayoutHints,
+ *lHints,
+ *lHints2;
+
+public:
+ XSElementDlg(const TGWindow *p, const TGWindow *main,
+ UInt_t *retZ, UInt_t w=600, UInt_t h=350);
+ ~XSElementDlg();
+
+ virtual void CloseWindow();
+ virtual Bool_t ProcessButton(Long_t param);
+ virtual Bool_t ProcessMessage(Long_t msg,
+ Long_t param1, Long_t param2);
+
+ //ClassDef(XSElementDlg,1)
+}; // XSElementDlg
+
+#endif
diff --git a/test/periodic/XSElementList.cxx b/test/periodic/XSElementList.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..32f0ecae267b08e25155a0957e45ae6dc591f1ff
--- /dev/null
+++ b/test/periodic/XSElementList.cxx
@@ -0,0 +1,176 @@
+/*
+ * $Header$
+ * $Log$
+ *
+ * Fills a listbox with the elements sorted, by name, mnemonic, or Z
+ */
+
+#include <ctype.h>
+#include <stdlib.h>
+#include <string.h>
+
+#include <TGFrame.h>
+#include <TGLayout.h>
+#include <TGWidget.h>
+#include <TGWindow.h>
+#include <TGPicture.h>
+
+#include "XSVarious.h"
+#include "XSElementList.h"
+
+//ClassImp(XSElementList)
+
+/* ----- XSElementList ----- */
+XSElementList::XSElementList(TGWindow* p, Int_t sortby)
+ : TGListBox(p,50,50)
+{
+ UInt_t i;
+ int *index = new int[XSelements->GetSize()];
+
+ sortBy = sortby;
+
+ for (i=0; i<XSelements->GetSize(); i++)
+ index[i] = i;
+
+ Sort(index);
+
+ for (i=0; i<XSelements->GetSize(); i++) {
+ char str[100];
+ Int_t Z = ElementString(index[i]+1, str);
+ TGString *tgstr = new TGString(str);
+ TGTextLBEntry *lbe = new TGTextLBEntry(fLbc,tgstr,Z,
+ fixedGC,fixedFontStruct);
+
+ TGLayoutHints *lhints = new TGLayoutHints(
+ kLHintsExpandX | kLHintsTop);
+
+ fItemVsize = TMath::Max(fItemVsize, lbe->GetDefaultHeight());
+
+ AddEntry((TGLBEntry*)lbe, lhints);
+ }
+
+ delete [] index;
+} // XSElementList
+
+/* ----- ~XSElementList ----- */
+XSElementList::~XSElementList()
+{
+} // ~XSElementList
+
+/* ----- Compare ----- */
+Int_t
+XSElementList::Compare(int i, int j) const
+{
+ switch (sortBy) {
+ case XSEL_SORTBY_NAME:
+ return strcmp(XSelements->Name(i+1),
+ XSelements->Name(j+1));
+
+ case XSEL_SORTBY_MNEMONIC:
+ return strcmp(XSelements->Mnemonic(i+1),
+ XSelements->Mnemonic(j+1));
+
+ case XSEL_SORTBY_Z:
+ return (i<j? -1 : i>j? 1 : 0);
+
+ default:
+ return 0;
+ }
+} // Compare
+
+/* ----- Sort ----- */
+void
+XSElementList::Sort(int *index)
+{
+ // --- Perform a bubble sort ---
+ for (UInt_t i=0; i<XSelements->GetSize(); i++) {
+ int change = 0;
+ for (UInt_t j=XSelements->GetSize()-1; j>i; j--) {
+ if (Compare(index[j],index[j-1]) < 0) {
+ int t = index[j];
+ index[j] = index[j-1];
+ index[j-1] = t;
+ change = 1;
+ }
+ }
+ if (!change)
+ return;
+ }
+} // Sort
+
+/* ----- ElementString ----- */
+Int_t
+XSElementList::ElementString(Int_t Z, char *buf)
+{
+ switch (sortBy) {
+ case XSEL_SORTBY_NAME:
+ sprintf(buf,"%-20s %-4s %d",
+ XSelements->Name(Z),
+ XSelements->Mnemonic(Z),
+ Z);
+ break;
+
+ case XSEL_SORTBY_MNEMONIC:
+ sprintf(buf,"%-4s %-20s %d",
+ XSelements->Mnemonic(Z),
+ XSelements->Name(Z),
+ Z);
+ break;
+
+ case XSEL_SORTBY_Z:
+ sprintf(buf,"%3d %-4s %-20s",
+ Z,
+ XSelements->Mnemonic(Z),
+ XSelements->Name(Z));
+ break;
+ }
+ return Z;
+} // ElementString
+
+/* ----- GetZ ------- */
+UInt_t
+XSElementList::GetZ( TGTextLBEntry *entry )
+{
+ if (entry == NULL) return 0;
+
+ const TGString *txt = entry->GetText();
+ if (txt == NULL) return 0;
+
+ const char *str = txt->GetString();
+ if (str == NULL) return 0;
+
+ // Search the string for the Z
+ while (*str && !isdigit(*str))
+ str++;
+ return atol(str);
+} // GetZ
+
+/* ----- SelectZ ----- */
+void
+XSElementList::SelectZ( UInt_t Z )
+{
+ TGTextLBEntry *f;
+ TGFrameElement *el;
+
+ if (Z<1 || Z>XSelements->GetSize()) return;
+
+ TGLBContainer *ct = (TGLBContainer *) fVport->GetContainer();
+
+ TIter next(ct->GetList());
+ while ((el = (TGFrameElement *) next())) {
+ f = (TGTextLBEntry *) el->fFrame;
+ if (GetZ(f) == Z) {
+ f->Activate(kTRUE);
+ return;
+ }
+ }
+ return;
+} // SelectZ
+
+/* ----- CurrentZ ----- */
+UInt_t
+XSElementList::CurrentZ( )
+{
+ TGTextLBEntry *entry = (TGTextLBEntry*)(GetSelectedEntry());
+ return GetZ(entry);
+} // CurrentZ
diff --git a/test/periodic/XSElementList.h b/test/periodic/XSElementList.h
new file mode 100644
index 0000000000000000000000000000000000000000..b28a7048604e4a2596ba9817c5016738649724c7
--- /dev/null
+++ b/test/periodic/XSElementList.h
@@ -0,0 +1,40 @@
+/*
+ * $Header$
+ * $Log$
+ *
+ * Array of Elements with names and mnemonics
+ */
+
+#ifndef __XSELEMENT_LIST_H
+#define __XSELEMENT_LIST_H
+
+#include <TGListBox.h>
+
+#define XSEL_SORTBY_NAME 0
+#define XSEL_SORTBY_MNEMONIC 1
+#define XSEL_SORTBY_Z 2
+
+/* =================== XSElementList ===================== */
+class XSElementList : public TGListBox
+{
+protected:
+ Int_t sortBy;
+
+public:
+ XSElementList(TGWindow *p, Int_t sortby = XSEL_SORTBY_NAME);
+ ~XSElementList();
+
+ void SelectZ(UInt_t Z);
+ UInt_t CurrentZ();
+
+protected:
+ Int_t Compare(int i, int j) const;
+ Int_t Compare(const TObject *o) const { return TObject::Compare(o); }
+ UInt_t GetZ( TGTextLBEntry *entry );
+ void Sort(int *index);
+ Int_t ElementString(Int_t idx, char *buf);
+
+ //ClassDef(XSElementList,1)
+}; // XSElementList
+
+#endif
diff --git a/test/periodic/XSElements.cxx b/test/periodic/XSElements.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..cb5abe4c93244b5cd991515c947a89c656253728
--- /dev/null
+++ b/test/periodic/XSElements.cxx
@@ -0,0 +1,161 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#include <ctype.h>
+#include <stdio.h>
+#include <stdlib.h>
+#include <string.h>
+
+#include "XSElements.h"
+
+//ClassImp(XSElement)
+
+/* =================== XSElement ===================== */
+XSElement::XSElement()
+{
+ z = 0;
+ name = NULL;
+ symbol = NULL;
+ isotope = NULL;
+ atomic_weight = NULL;
+ density = NULL;
+ melting_point = NULL;
+ boiling_point = NULL;
+ oxidation_states = NULL;
+ isotope = NULL;
+} // XSElement
+
+/* ---------- ~XSElement ----------- */
+XSElement::~XSElement()
+{
+ if (name) free(name);
+ if (symbol) free(symbol);
+ if (atomic_weight) free(atomic_weight);
+ if (density) free(density);
+ if (melting_point) free(melting_point);
+ if (boiling_point) free(boiling_point);
+ if (oxidation_states) free(oxidation_states);
+ for (int i=0; i<ni; i++) {
+ free(isotope[i]);
+ free(isotope_info[i]);
+ }
+ free(isotope);
+ free(isotope_info);
+ free(isotope_stable);
+} // ~XSElement
+
+/* ------- IsotopeInfo ------- */
+// Search for information by name
+const char*
+XSElement::IsotopeInfo( const char *isot )
+{
+ for (int i=0; i<ni; i++)
+ if (!strcmp(isotope[i],isot))
+ return isotope_info[i];
+
+ return "-";
+} // IsotopeInfo
+
+/* ------- ReadLine ------- */
+/* Reads one line and allocates a string for it */
+char *
+XSElement::ReadLine(FILE *f)
+{
+ char buf[256];
+ char *p=buf;
+ char ch;
+
+ /* skip leading spaces */
+ do {
+ ch=fgetc(f);
+ } while (isspace(ch));
+
+ do {
+ *p++ = ch;
+ ch = fgetc(f);
+ } while (ch != '\n');
+ *p = 0;
+ return strdup(buf);
+} /* ReadLine */
+
+/* ------- Read -------- */
+void
+XSElement::Read(FILE *f)
+{
+ char tmpsym[5], tmpname[30];
+ fscanf(f,"%d %s %s %d",&z,tmpsym,tmpname,&ni);
+
+ symbol = strdup(tmpsym);
+ name = strdup(tmpname);
+
+ if (ni==0) return;
+
+ atomic_weight = ReadLine(f);
+ density = ReadLine(f);
+ melting_point = ReadLine(f);
+ boiling_point = ReadLine(f);
+ oxidation_states = ReadLine(f);
+
+ isotope = (char **)malloc(ni*sizeof(char*));
+ isotope_info = (char **)malloc(ni*sizeof(char*));
+ isotope_stable = (Bool_t *)malloc(ni*sizeof(Bool_t));
+
+ for (int i=0; i<ni; i++) {
+ char ch;
+ char buf[30];
+
+ /* get first character */
+ ch = fgetc(f);
+ if (ch != '*')
+ ungetc(ch,f); // Put it back
+
+ fscanf(f,"%s",buf);
+ isotope[i] = strdup(buf);
+ isotope_info[i] = ReadLine(f);
+
+ isotope_stable[i] = (ch=='*');
+ }
+} // Read
+
+/* =================== XSElements ===================== */
+//ClassImp(XSElements)
+
+XSElements::XSElements(const char *filename)
+{
+ FILE *f;
+
+ if ((f=fopen(filename,"r"))==NULL) {
+ fprintf(stderr,"XSElements::XSElements: Error opening file %s\n",filename);
+ exit(0);
+ }
+
+ fscanf(f,"%d",&NElements);
+ elements = new TObjArray(NElements);
+
+ for (UInt_t i=0; i<NElements; i++) {
+ elements->Add(new XSElement());
+ ((XSElement*)(*elements)[i])->Read(f);
+ }
+ fclose(f);
+} // XSElements
+
+/* --------- ~XSElements ---------- */
+XSElements::~XSElements()
+{
+ delete elements;
+} // ~XSElements
+
+/* --------- Find ----------- */
+UInt_t
+XSElements::Find(const char *str)
+{
+ for (UInt_t z=1; z<=NElements; z++) {
+ if (!strcmp(str,Name(z)))
+ return z;
+ if (!strcmp(str,Mnemonic(z)))
+ return z;
+ }
+ return 0;
+} // Find
diff --git a/test/periodic/XSElements.h b/test/periodic/XSElements.h
new file mode 100644
index 0000000000000000000000000000000000000000..c6d862d461fb74f32f81467303eaeb771c8ce4c2
--- /dev/null
+++ b/test/periodic/XSElements.h
@@ -0,0 +1,91 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#ifndef __XSELEMENTS_H
+#define __XSELEMENTS_H
+
+#include <TObject.h>
+#include <TObjArray.h>
+
+enum Element_State {
+ Element_GroundState,
+ Element_Metastable,
+ Element_SecondMetastable
+};
+
+/* =================== XSElement ===================== */
+class XSElement : public TObject
+{
+protected:
+ Int_t z;
+ char *name;
+ char *symbol;
+
+ char *atomic_weight;
+ char *density;
+ char *melting_point;
+ char *boiling_point;
+ char *oxidation_states;
+
+ Int_t ni;
+ char **isotope;
+ char **isotope_info;
+ Bool_t *isotope_stable;
+
+public:
+ XSElement();
+ ~XSElement();
+
+ inline char* Name() const { return name; }
+ inline char* Mnemonic() const { return symbol; }
+ inline char* Symbol() const { return symbol; }
+ inline char* AtomicWeight() const { return atomic_weight; }
+ inline char* Density() const { return density; }
+ inline char* MeltingPt() const { return melting_point; }
+ inline char* BoilingPt() const { return boiling_point; }
+ inline char* Oxidation() const { return oxidation_states; }
+ inline Int_t Isotopes() const { return ni; }
+ inline char* Isotope(int i) const { return isotope[i]; }
+ const char* IsotopeInfo(const char *isotope);
+ inline char* IsotopeInfo(int i)
+ const { return isotope_info[i]; }
+ inline Bool_t IsStable(int i) const { return isotope_stable[i]; }
+
+ void Read(FILE *f);
+ Int_t Read(const char *name) { return TObject::Read(name); }
+protected:
+ char* ReadLine(FILE *f);
+ //ClassDef(XSElement,1)
+}; // XSElement
+
+/* =================== XSElements ===================== */
+class XSElements : public TObject
+{
+protected:
+ UInt_t NElements;
+ TObjArray *elements;
+
+public:
+ XSElements( const char *filename );
+ ~XSElements();
+
+ inline UInt_t GetSize() const { return NElements; }
+
+ inline char* Name(Int_t Z)
+ { return ((XSElement*)((*elements)[Z-1]))->Name(); }
+
+ inline char* Mnemonic(Int_t Z)
+ { return ((XSElement*)((*elements)[Z-1]))->Mnemonic(); }
+
+ inline XSElement *Elem(Int_t Z)
+ { return ((XSElement*)((*elements)[Z-1])); }
+
+ // Search for element either by name or mnemonic
+ UInt_t Find(const char *str);
+
+ //ClassDef(XSElements,1)
+}; // XSElements
+
+#endif
diff --git a/test/periodic/XSGraph.cxx b/test/periodic/XSGraph.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..099ebff372c2d2eacef3dff7cf84e200a3800b65
--- /dev/null
+++ b/test/periodic/XSGraph.cxx
@@ -0,0 +1,27 @@
+#include "XSGraph.h"
+
+/* ===================== XSGraph ================= */
+XSGraph::XSGraph( NdbMTReactionXS *reac )
+{
+ N = reac->Pairs();
+
+ X = new Float_t[N];
+ Y = new Float_t[N];
+
+ for (int i=0; i<N; i++) {
+ X[i] = reac->Energy(i);
+ Y[i] = reac->XS(i);
+ }
+
+ graph = new TGraph(N,X,Y);
+} // XSGraph
+
+/* ---------- ~XSGraph --------- */
+XSGraph::~XSGraph()
+{
+ if (N) {
+ delete [] X;
+ delete [] Y;
+ delete graph;
+ }
+} // ~XSGraph
diff --git a/test/periodic/XSGraph.h b/test/periodic/XSGraph.h
new file mode 100644
index 0000000000000000000000000000000000000000..f75fe377082788eb1691cdf6796ef4c729e40eb9
--- /dev/null
+++ b/test/periodic/XSGraph.h
@@ -0,0 +1,44 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#ifndef __XSGRAPH_H
+#define __XSGRAPH_H
+
+#include <TGraph.h>
+#include <TString.h>
+
+#include "NdbMTReactionXS.h"
+
+/* =================== XSGraph ===================== */
+class XSGraph : public TObject
+{
+protected:
+ TString desc;
+ Int_t Z;
+ Int_t A;
+
+ Int_t N;
+ Float_t *X;
+ Float_t *Y;
+
+ TGraph *graph;
+
+public:
+ XSGraph()
+ {
+ N = 0;
+ X = Y = NULL;
+ graph = NULL;
+ }
+
+ XSGraph( NdbMTReactionXS *reac );
+ ~XSGraph();
+
+ inline TGraph* GetGraph() { return graph; }
+
+ //ClassDef(XSGraph,1)
+}; // XSGraph
+
+#endif
diff --git a/test/periodic/XSGui.cxx b/test/periodic/XSGui.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..caa9e13e589347d1d0f21d88b43c5e87f172e929
--- /dev/null
+++ b/test/periodic/XSGui.cxx
@@ -0,0 +1,258 @@
+/*
+ * $Header$
+ * $Log$
+ *
+ * The graphical user interface for the Neutron Cross section database
+ */
+
+#define __XSGUI_CXX
+
+#include <stdio.h>
+#include <stdlib.h>
+
+#include <TROOT.h>
+#include <TGraph.h>
+#include <TFrame.h>
+#include <TCanvas.h>
+#include <TSystem.h>
+#include <TApplication.h>
+#include <Riostream.h>
+
+#include "XSGui.h"
+#include "XSVarious.h"
+#include "XSElementDlg.h"
+#include "XSReactionDlg.h"
+
+//ClassImp(XSGui)
+
+const char *filetypes[] = { "All files", "*",
+ "Data file", "*.dat",
+ "ENDF files", "*.endf",
+ 0, 0 };
+
+/* ----- XSGui ----- */
+XSGui::XSGui(const TGWindow *p, UInt_t w, UInt_t h)
+ : TGMainFrame(p, w, h)
+{
+ // Create the main frame. A TGMainFrame is a top level window.
+
+ // Create menubar and popup menus. The hint objects are used to place
+ // and group the different menu widgets with respect to eachother.
+ menuBarLayout = new TGLayoutHints(
+ kLHintsTop | kLHintsLeft | kLHintsExpandX,
+ 0, 0, 1, 1);
+ menuBarItemLayout = new TGLayoutHints(kLHintsTop | kLHintsLeft,
+ 0, 4, 0, 0);
+ menuBarHelpLayout = new TGLayoutHints(kLHintsTop | kLHintsRight);
+
+ // Build up the menus
+ // First the Main (FILE) menu
+ fileMenu = new TGPopupMenu(fClient->GetRoot());
+ fileMenu->AddEntry("&Open...", M_FILE_OPEN);
+ fileMenu->AddEntry("&Save", M_FILE_SAVE);
+ fileMenu->AddEntry("S&ave as...", M_FILE_SAVEAS);
+ fileMenu->AddEntry("&Close", M_FILE_CLOSE);
+ fileMenu->AddSeparator();
+ fileMenu->AddEntry("&Print", M_FILE_PRINT);
+ fileMenu->AddEntry("P&rint setup...", M_FILE_PRINT_SETUP);
+ fileMenu->AddSeparator();
+ fileMenu->AddEntry("E&xit", M_FILE_EXIT);
+
+ fileMenu->DisableEntry(M_FILE_SAVEAS);
+ fileMenu->DisableEntry(M_FILE_CLOSE);
+
+ // The database menu and the current elements in graph
+ elemMenu = new TGPopupMenu(fClient->GetRoot());
+ elemMenu->AddEntry("&Reaction", M_ELEM_REACTION);
+ elemMenu->AddEntry("&Modify", M_ELEM_MODIFY);
+ elemMenu->AddEntry("&Clear", M_ELEM_CLEAR);
+ elemMenu->AddSeparator();
+ elemMenu->AddLabel("Current Elements in Graph");
+
+ // The Currently Editing elements menu
+ optMenu = new TGPopupMenu(fClient->GetRoot());
+ optMenu->AddEntry("&Zoom", -1);
+ optMenu->AddEntry("&Options", -1);
+
+ // The Help Menu
+ helpMenu = new TGPopupMenu(fClient->GetRoot());
+ helpMenu->AddEntry("&About",M_HELP_ABOUT);
+
+ // Menu button messages are handled by the main frame (i.e. "this")
+ // ProcessMessage() method.
+ fileMenu->Associate(this);
+ elemMenu->Associate(this);
+ optMenu->Associate(this);
+ helpMenu->Associate(this);
+
+ menuBar = new TGMenuBar(this, 1, 1, kHorizontalFrame);
+ menuBar->AddPopup("&File", fileMenu, menuBarItemLayout);
+ menuBar->AddPopup("&Element", elemMenu, menuBarItemLayout);
+ menuBar->AddPopup("&Options", optMenu, menuBarItemLayout);
+ menuBar->AddPopup("&Help", helpMenu, menuBarHelpLayout);
+
+ AddFrame(menuBar, menuBarLayout);
+
+ // Create a ROOT Canvas used for drawing...
+ canvasWindow = new TRootEmbeddedCanvas("Canvas",this,
+ 600,400);
+
+ // Initialise the canvas
+ canvas = canvasWindow->GetCanvas();
+ canvas->SetFillColor(42);
+ canvas->SetGrid();
+ canvas->GetFrame()->SetFillColor(21);
+ canvas->GetFrame()->SetBorderSize(6);
+ canvas->SetLogx();
+ canvas->SetLogy();
+ canvas->Update();
+
+ AddFrame(canvasWindow,
+ new TGLayoutHints(kLHintsExpandX | kLHintsExpandY,
+ 0, 0, 2, 2));
+
+ statusBar = new TGStatusBar(this, 60, 20);
+ AddFrame(statusBar, new TGLayoutHints(kLHintsBottom | kLHintsExpandX,
+ 0, 0, 1, 0));
+ statusBar->SetText(PRGNAME);
+
+ SetWindowName(PRGNAME);
+
+ MapSubwindows();
+
+ // we need to use GetDefault...() to initialize the layout algorithm...
+ Resize(GetDefaultSize());
+
+ MapWindow();
+} // XSGui
+
+/* ----- ~XSGui ----- */
+XSGui::~XSGui()
+{
+ // Delete all created widgets.
+ delete menuBarLayout;
+ delete menuBarItemLayout;
+ delete menuBarHelpLayout;
+
+ delete fileMenu;
+ delete elemMenu;
+ delete optMenu;
+ delete helpMenu;
+
+ delete statusBar;
+ delete canvasWindow;
+} // ~XSGui
+
+/* ----- CloseWindow ----- */
+void
+XSGui::CloseWindow()
+{
+ // Got close message for this MainFrame. Calls parent CloseWindow()
+ // (which destroys the window) and terminate the application.
+ // The close message is generated by the window manager when its close
+ // window menu item is selected.
+
+ TGMainFrame::CloseWindow();
+ gApplication->Terminate(0);
+} // CloseWindow
+
+/* ----- ProcessMenuMessage ----- */
+Bool_t
+XSGui::ProcessMenuMessage( Long_t param )
+{
+ switch (param) {
+ case M_FILE_OPEN:
+ {
+ static TString dir(".");
+ TGFileInfo fi;
+ fi.fFileTypes = filetypes;
+ fi.fIniDir = StrDup(dir);
+ new TGFileDialog(fClient->GetRoot(), this, kFDOpen, &fi);
+ dir = fi.fIniDir;
+ }
+ break;
+
+ case M_FILE_SAVE:
+ printf("M_FILE_SAVE\n");
+ break;
+
+ case M_FILE_EXIT:
+ // this also terminates theApp
+ CloseWindow();
+ break;
+
+ case M_ELEM_REACTION:
+ new XSReactionDlg(fClient->GetRoot(), this, 1, 500,600);
+ break;
+
+ case M_HELP_ABOUT:
+ // About();
+ int retval;
+ new TGMsgBox(fClient->GetRoot(), this,
+ "About", "About....",
+ kMBIconAsterisk, kMBOk, &retval );
+ break;
+
+ default:
+ break;
+ }
+ return kTRUE;
+} // ProcessMenuMessage
+
+/* ----- ProcessMessage ----- */
+Bool_t
+XSGui::ProcessMessage(Long_t msg, Long_t param1, Long_t)
+{
+ // Handle messages send to the XSGui object.
+ char str[100];
+
+ switch (GET_MSG(msg)) {
+
+ case kC_COMMAND:
+ switch (GET_SUBMSG(msg)) {
+
+ case kCM_BUTTON:
+ sprintf(str,
+ "Button was pressed, id = %ld\n",
+ param1);
+ statusBar->SetText(str);
+ break;
+
+ case kCM_MENUSELECT:
+ if (param1>=0)
+ statusBar->SetText(menuTip[param1]);
+ else
+ statusBar->SetText("Undefined Menu!");
+ break;
+
+ case kCM_MENU:
+ ProcessMenuMessage(param1);
+ break;
+
+ default:
+ break;
+ }
+ default:
+ break;
+ }
+ return kTRUE;
+} // ProcessMessage
+
+//---- Main program ----------------------------------------------------------
+
+TROOT root("GUI", "GUI test environement");
+
+/* ----- main ----- */
+int main(int ac, char *av[])
+{
+ TApplication theApp("App", &ac, av);
+
+ XSGui mainWindow(gClient->GetRoot(), 400, 220);
+
+ XSinitialise();
+
+ theApp.Run();
+
+ XSfinalise();
+ return 0;
+} // main
diff --git a/test/periodic/XSGui.h b/test/periodic/XSGui.h
new file mode 100644
index 0000000000000000000000000000000000000000..d700230d98da0b564f68cd54eb0a0f7f0fe7bacf
--- /dev/null
+++ b/test/periodic/XSGui.h
@@ -0,0 +1,103 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#ifndef __XSGUI_H
+#define __XSGUI_H
+
+#include <TVirtualX.h>
+#include <TGMenu.h>
+#include <TGFrame.h>
+#include <TGLabel.h>
+#include <TGButton.h>
+#include <TGCanvas.h>
+#include <TGClient.h>
+#include <TGMsgBox.h>
+#include <TGStatusBar.h>
+#include <TGTextEntry.h>
+#include <TGFileDialog.h>
+
+#define PRGNAME "XSGui"
+#define VERSION "1.0a"
+#define AUTHOR "V.Vlachoudis"
+#define DATE "Jun-1999"
+#define EMAIL "V.Vlachoudis@cern.ch"
+
+#define ABOUT PRGNAME" "VERSION"\n" \
+ AUTHOR" "DATE \
+ EMAIL
+
+/* ---- Define all the available commands ----- */
+enum TCommandIdentifiers {
+ M_FILE_OPEN,
+ M_FILE_SAVE,
+ M_FILE_SAVEAS,
+ M_FILE_CLOSE,
+ M_FILE_PRINT,
+ M_FILE_PRINT_SETUP,
+ M_FILE_EXIT,
+
+ M_ELEM_REACTION,
+ M_ELEM_MODIFY,
+ M_ELEM_CLEAR,
+
+ M_OPTION_ZOOM,
+ M_OPTION_SETUP,
+
+ M_HELP_ABOUT,
+};
+
+/* --- Define the Help for each menu item --- */
+// WARNING!!! MUST BE IN ALIGN WITH TCommandsIdentifiers
+#ifdef __XSGUI_CXX
+static const char *menuTip[] = {
+ "Open a file",
+ "Save drawing",
+ "Save drawing as",
+ "Close current drawing",
+ "Print drawing",
+ "Printer Setup",
+ "Exit from program",
+
+ "Select a Reaction",
+ "Edit/Modify/Delete the current graphs",
+ "Clear Current Graph",
+
+ "Zoom current image",
+ "General graphic options",
+
+ "About the program"
+};
+#endif
+
+/* ================== XSGui ===================== */
+class XSGui : public TGMainFrame
+{
+private:
+ TGMenuBar *menuBar;
+
+ TGPopupMenu *fileMenu,
+ *elemMenu,
+ *optMenu,
+ *helpMenu;
+
+ TGLayoutHints *menuBarLayout,
+ *menuBarItemLayout,
+ *menuBarHelpLayout;
+
+ TGStatusBar *statusBar;
+
+public:
+ XSGui(const TGWindow *p, UInt_t w, UInt_t h);
+ virtual ~XSGui();
+
+ virtual void CloseWindow();
+ virtual Bool_t ProcessMessage(Long_t msg, Long_t param, Long_t);
+
+ Bool_t ProcessMenuMessage( Long_t param );
+
+ //ClassDef(XSGui,1)
+}; // XSGui
+
+#endif
diff --git a/test/periodic/XSPeriodicTable.cxx b/test/periodic/XSPeriodicTable.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..c133e7d0f22ee5dc58a1c6e6eb10e9885b91b8ec
--- /dev/null
+++ b/test/periodic/XSPeriodicTable.cxx
@@ -0,0 +1,313 @@
+/*
+ * $Header$
+ * $Log$
+ *
+ * Implements the periodic table of elements
+ */
+
+#include <TGFrame.h>
+#include <TGLayout.h>
+#include <TGWindow.h>
+
+#include "XSVarious.h"
+#include "XSElementList.h"
+#include "XSPeriodicTable.h"
+
+//ClassImp(XSTblElement)
+
+/* =========== XSTblElement ============== */
+XSTblElement::XSTblElement(const TGWindow *p, Int_t z, UInt_t color)
+ : TGButton(p,z)
+{
+ Z = z;
+
+ char str[5];
+ sprintf(str,"%d",Z);
+ lZ = new TGLabel(this,str);
+ lName = new TGLabel(this,XSelements->Mnemonic(Z), blueBoldGC);
+
+ ChangeBackground(color);
+
+ tpZ = NULL;
+ tpName = NULL;
+} // XSTblElement
+
+/* ----- ~XSTblElement ----- */
+XSTblElement::~XSTblElement()
+{
+ delete lZ;
+ delete lName;
+ delete tpZ;
+ delete tpName;
+} // ~XSTblElement
+
+/* ----- Layout ----- */
+void
+XSTblElement::Layout()
+{
+ int w = GetWidth() - 2*fBorderWidth;
+ int h = (GetHeight() - 2*fBorderWidth) / 2;
+
+ lZ->MoveResize(fBorderWidth, fBorderWidth, w, h);
+ lZ->MapWindow();
+
+ lName->MoveResize(fBorderWidth, fBorderWidth+h, w, h);
+ lName->MapWindow();
+
+ if (tpZ == NULL) {
+ tpZ = new TGToolTip(fClient->GetRoot(),
+ lZ, XSelements->Name(Z), 1000);
+ tpName = new TGToolTip(fClient->GetRoot(),
+ lName, XSelements->Name(Z), 1000);
+ }
+
+ TGButton::Layout();
+} // Layout
+
+/* ------ SetState ------ */
+void
+XSTblElement::SetState(EButtonState state, Bool_t emit)
+{
+ if (state != fState) {
+ if (state==kButtonDown /*|| state==kButtonEngaged*/) {
+ lZ->Move(lZ->GetX()+1, lZ->GetY()+1);
+ lName->Move(lName->GetX()+1, lName->GetY()+1);
+ } else
+ if (state == kButtonUp) {
+ lZ->Move(lZ->GetX()-1, lZ->GetY()-1);
+ lName->Move(lName->GetX()-1, lName->GetY()-1);
+ }
+ }
+
+ TGButton::SetState(state, emit);
+} // SetState
+
+/* ------ SetState ------ */
+void
+XSTblElement::ChangeBackground( ULong_t color )
+{
+ lZ->ChangeBackground(color);
+ lName->ChangeBackground(color);
+} // ChangeBackground
+
+/////////////////////////////////////////////////////////////////////
+
+//ClassImp(XSPeriodicTable)
+
+static Int_t colwidth[XSPTBL_COLS] =
+ { 8, 5, 5, 2, 5,
+ 5, 5, 5, 5, 5,
+ 5, 5, 5, 5, 5,
+ 5, 5, 5, 5, 5 };
+static Int_t colsum;
+static Int_t rowheight[XSPTBL_ROWS] =
+ { 5, 5, 10, 10, 10, 10, 10, 10, 10, 3, 10, 10 };
+static Int_t rowsum;
+
+#define A(x) (Long_t)(char *)(x)
+static Long_t ptable[XSPTBL_ROWS][XSPTBL_COLS] = {
+ { A("Group"), A("1"), A("2"), 0, A("3"), A("4"), A("5"), A("6"), A("7"),
+ A("8"), A("9"), A("10"), A("11"), A("12"), A("13"), A("14"), A("15"),
+ A("16"), A("17"), A("18") },
+ { A("Period"), 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0},
+ { A("1"), 1, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 2},
+ { A("2"), 3, 4, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 5, 6, 7, 8, 9,10},
+ { A("3"),11,12, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0, 0,13, 14,15,16,17,18},
+ { A("4"),19,20, 0,21, 22,23,24,25,26, 27,28,29,30,31, 32,33,34,35,36},
+ { A("5"),37,38, 0,39, 40,41,42,43,44, 45,46,47,48,49, 50,51,52,53,54},
+ { A("6"),55,56,A("*"),71, 72,73,74,75,76, 77,78,79,80,81, 82,83,84,85,86},
+ { A("7"),87,88,A("**"),103, 104,105,106,107,108, 109,110,111,112,113, 114,115,116,117,118},
+ { 0,0,0,0,0, 0,0,0,0,0, 0,0,0,0,0, 0,0,0,0,0 },
+ { A("* Lanthanoids"),0,0,A("*"),57, 58,59,60,61,62, 63,64,65,66,67, 68,69,70,0,0},
+ { A("** Actinoids"),0,0,A("**"),89, 90,91,92,93,94, 95,96,97,98,99, 100,101,102,0,0}
+};
+#undef A
+
+
+#define COLORS 7
+
+//#define w 0xFFFFFFL // White
+//#define A 0xCCCCCCL // Gray
+//#define B 0xCCCCFFL // Blue
+//#define Y 0xFFFFCCL // Yellow
+//#define O 0xFFCCCCL // Orange
+//#define G 0xCCFFCCL // Green
+
+#define w 0
+#define A 1
+#define B 2
+#define Y 3
+#define O 4
+#define G 5
+static const char *colorName[COLORS] = {
+ "White",
+ "#CCCCCC",
+ "#CCCCFF",
+ "#FFFFCC",
+ "#FFCCCC",
+ "#CCFFCC",
+ "yellow",
+/******
+ "White",
+ "LightGrey",
+ "LightSteelBlue1",
+ "lemon chiffon",
+ "pink",
+ "DarkSeaGreen1",
+ "yellow",
+*******/
+ };
+
+static ULong_t colorPixels[COLORS];
+
+static Byte_t ecolor[XSPTBL_ROWS][XSPTBL_COLS] = {
+ { A,A,A,w,A, A,A,A,A,A, A,A,A,A,A, A,A,A,A,A },
+ { A,w,w,w,w, w,w,w,w,w, w,w,w,w,w, w,w,w,w,w },
+ { A,B,w,w,w, w,w,w,w,w, w,w,w,w,w, w,w,w,w,Y },
+ { A,B,B,w,w, w,w,w,w,w, w,w,w,w,Y, Y,Y,Y,Y,Y },
+ { A,B,B,w,w, w,w,w,w,w, w,w,w,w,Y, Y,Y,Y,Y,Y },
+ { A,B,B,w,O, O,O,O,O,O, O,O,O,O,Y, Y,Y,Y,Y,Y },
+ { A,B,B,w,O, O,O,O,O,O, O,O,O,O,Y, Y,Y,Y,Y,Y },
+ { A,B,B,w,O, O,O,O,O,O, O,O,O,O,Y, Y,Y,Y,Y,Y },
+ { A,B,B,w,O, O,O,O,O,O, O,O,O,O,A, Y,A,Y,A,Y },
+ { w,w,w,w,w, w,w,w,w,w, w,w,w,w,w, w,w,w,w,w },
+ { A,A,A,w,G, G,G,G,G,G, G,G,G,G,G, G,G,G,w,w },
+ { A,A,A,w,G, G,G,G,G,G, G,G,G,G,G, G,G,G,w,w }
+};
+#undef w
+#undef A
+#undef B
+#undef Y
+#undef O
+#undef G
+
+/* ----- XSPeriodicTable ----- */
+XSPeriodicTable::XSPeriodicTable(const TGWindow *msgWnd, const TGWindow* p,
+ UInt_t w, UInt_t h)
+ : TGCompositeFrame(p,w,h, kFitWidth | kFitHeight | kSunkenFrame)
+{
+ int i, j;
+
+ rowsum = 0;
+ for (j=0; j<XSPTBL_ROWS; j++)
+ rowsum += rowheight[j];
+
+ colsum = 0;
+ for (j=0; j<XSPTBL_COLS; j++)
+ colsum += colwidth[j];
+
+ /** Initialise colors **/
+ for (i=0; i<COLORS; i++)
+ gClient->GetColorByName(colorName[i], colorPixels[i]);
+
+ for (j=0; j<XSPTBL_ROWS; j++)
+ for (i=0; i<XSPTBL_COLS; i++) {
+ long val = ptable[j][i];
+ int col = colorPixels[ecolor[j][i]];
+ if (val) {
+ if (val < 120) {
+ elem[j][i] = new XSTblElement(this,
+ val,col);
+ ((XSTblElement*)elem[j][i])->Associate(msgWnd);
+ } else {
+ elem[j][i] = new TGLabel(this,
+ (char*)val);
+ elem[j][i]->ChangeBackground(col);
+ }
+ } else
+ elem[j][i] = NULL;
+ }
+ ChangeBackground(colorPixels[0]);
+
+ width = w;
+ height = h;
+} // XSPeriodicTable
+
+/* ----- ~XSPeriodicTable ----- */
+XSPeriodicTable::~XSPeriodicTable()
+{
+ for (int j=0; j<XSPTBL_ROWS; j++)
+ for (int i=0; i<XSPTBL_COLS; i++)
+ if (elem[j][i])
+ delete elem[j][i];
+} // ~XSPeriodicTable
+
+/* ----- Layout ----- */
+void
+XSPeriodicTable::Layout()
+{
+ int w, h;
+ Float_t cwidth[XSPTBL_COLS];
+ Float_t rheight[XSPTBL_ROWS];
+
+ TGCompositeFrame::Layout();
+
+ w = GetWidth() - 2*fBorderWidth - 4;
+ h = GetHeight() - 2*fBorderWidth - 4;
+
+ // --- Normalise height and widths ---
+ for (int i=0; i<XSPTBL_COLS; i++) {
+ cwidth[i] = (Float_t)(colwidth[i]*w)/(Float_t)colsum;
+ }
+
+ for (int i=0; i<XSPTBL_ROWS; i++) {
+ rheight[i] = (Float_t)(rowheight[i]*h)/(Float_t)rowsum;
+ }
+
+ Float_t yt = fBorderWidth+2;
+ for (int j=0; j<XSPTBL_ROWS; j++) {
+ Float_t xl = fBorderWidth+2;
+ for (int i=0; i<XSPTBL_COLS; i++) {
+ if (j<10) {
+ if (elem[j][i]) {
+ elem[j][i]->MoveResize(
+ (int)xl,
+ (int)yt,
+ (int)cwidth[i]-1,
+ (int)rheight[j]-1);
+ elem[j][i]->MapWindow();
+ }
+ xl += cwidth[i];
+ } else {
+ if (i<3) {
+ Float_t w = cwidth[0]+cwidth[1]+
+ cwidth[2];
+ if (elem[j][0]) {
+ elem[j][0]->MoveResize(
+ (int)xl,
+ (int)yt,
+ (int)w-1,
+ (int)rheight[j]-1);
+ elem[j][0]->MapWindow();
+ }
+ xl += w;
+ i = 2;
+ } else {
+ if (elem[j][i]) {
+ elem[j][i]->MoveResize(
+ (int)xl,
+ (int)yt,
+ (int)cwidth[i]-1,
+ (int)rheight[j]-1);
+ elem[j][i]->MapWindow();
+ }
+ xl += cwidth[i];
+ }
+ }
+ }
+ yt += rheight[j];
+ }
+} // Layout
+
+/* ----- SelectZ ----- */
+void
+XSPeriodicTable::SelectZ( ULong_t Z )
+{
+ // Find the selection and change the color
+ for (int j=0; j<XSPTBL_ROWS; j++)
+ for (int i=0; i<XSPTBL_COLS; i++)
+ if ((ULong_t)ptable[j][i] == Z) {
+ // Setting the background
+ elem[j][i]->ChangeBackground(colorPixels[6]);
+ }
+} // SelectZ
diff --git a/test/periodic/XSPeriodicTable.h b/test/periodic/XSPeriodicTable.h
new file mode 100644
index 0000000000000000000000000000000000000000..683eb6e73a187a30166e0fdfeadd30973c9f1ffd
--- /dev/null
+++ b/test/periodic/XSPeriodicTable.h
@@ -0,0 +1,66 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#ifndef __XSPERIODIC_TABLE_H
+#define __XSPERIODIC_TABLE_H
+
+#include <TGLabel.h>
+#include <TGFrame.h>
+#include <TGButton.h>
+#include <TGToolTip.h>
+
+/* =========== XSTblElement ============== */
+class XSTblElement : public TGButton
+{
+friend class TGClient;
+
+private:
+ Int_t Z;
+ TGLabel *lZ;
+ TGToolTip *tpZ;
+ TGLabel *lName;
+ TGToolTip *tpName;
+
+public:
+ XSTblElement( const TGWindow *p, Int_t z, UInt_t color);
+ ~XSTblElement();
+ virtual void Layout();
+ virtual TGDimension GetDefaultSize() const
+ { return TGDimension(20,20); }
+
+ virtual void SetState(EButtonState state, Bool_t emit = kFALSE);
+
+ Int_t GetZ() const { return Z; }
+ virtual void ChangeBackground( ULong_t color );
+
+ //ClassDef(XSTblElement,1)
+}; // XSTblElement
+
+//////////////////////////////////////////////////////////////
+
+#define XSPTBL_ROWS 12
+#define XSPTBL_COLS 20
+
+/* ================== XSPeriodicTable ===================== */
+class XSPeriodicTable : public TGCompositeFrame
+{
+private:
+ Int_t width, height;
+ TGFrame *elem[XSPTBL_ROWS][XSPTBL_COLS];
+
+public:
+ XSPeriodicTable(const TGWindow *msgWnd, const TGWindow* p,
+ UInt_t w, UInt_t h);
+ virtual ~XSPeriodicTable();
+
+ virtual void SelectZ( ULong_t Z );
+ virtual void Layout();
+ virtual TGDimension GetDefaultSize() const
+ { return TGDimension(width,height); }
+
+ //ClassDef(XSPeriodicTable,1)
+}; // XSPeriodicTable
+
+#endif
diff --git a/test/periodic/XSReactionDlg.cxx b/test/periodic/XSReactionDlg.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..51d345ff3409a3f448f01a762d20e80c6db8183a
--- /dev/null
+++ b/test/periodic/XSReactionDlg.cxx
@@ -0,0 +1,1077 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#include <dirent.h>
+#include <stdlib.h>
+#include <unistd.h>
+#include <sys/stat.h>
+#include <sys/types.h>
+
+#include <Riostream.h>
+#include <TGTab.h>
+#include <TGFrame.h>
+#include <TGButton.h>
+#include <TGWindow.h>
+#include <TGButton.h>
+#include <TGMsgBox.h>
+
+#include "XSVarious.h"
+#include "XSElementDlg.h"
+#include "XSReactionDlg.h"
+
+#include "NdbMTDir.h"
+
+//ClassImp(XSReactionDlg)
+
+// Options for filling containers
+enum DirOptions {
+ DIROnlyFiles,
+ DIROnlyDirectories,
+ DIRBoth
+ };
+
+// Options for creating the path
+enum PathOptions {
+ PATHIsotope,
+ PATHProjectile,
+ PATHDatabase,
+ PATHFile
+ };
+
+enum XSReactionMessages {
+ REAC_ELEMENT_STEP,
+ REAC_TABLE,
+ REAC_OK,
+ REAC_EXEC,
+ REAC_CLOSE,
+ REAC_RESET,
+ REAC_PTABLE
+ };
+
+enum ComboIds {
+ ISOTOPE_COMBO,
+ PROJECTILE_COMBO,
+ TEMPERATURE_COMBO,
+ DATABASE_COMBO,
+ LINE_WIDTH_COMBO,
+ LINE_COLOR_COMBO,
+ MARKER_STYLE_COMBO,
+ MARKER_COLOR_COMBO,
+ MARKER_SIZE_COMBO,
+ ERRORBAR_COLOR_COMBO,
+ REACTION_LISTBOX,
+ };
+
+static Int_t LastWinX = -1;
+static Int_t LastWinY = -1;
+
+/* ----- XSReactionDlg ----- */
+XSReactionDlg::XSReactionDlg( const TGWindow *p,
+ const TGWindow *main, UInt_t initZ, UInt_t w, UInt_t h)
+ : TGTransientFrame(p,main,w,h)
+{
+ // Remember the main window
+ mainWindow = main;
+
+ /* ---------- Prepare the Layout Hints ------- */
+ lHFixed = new TGLayoutHints(kLHintsTop | kLHintsLeft,
+ 3, 3, 2, 2);
+ lHExpX = new TGLayoutHints(kLHintsTop | kLHintsLeft | kLHintsExpandX,
+ 3, 3, 2, 2);
+ lHExpY = new TGLayoutHints(kLHintsTop | kLHintsLeft | kLHintsExpandY,
+ 3, 3, 2, 2);
+ lHExpXY = new TGLayoutHints(kLHintsTop | kLHintsLeft |
+ kLHintsExpandX | kLHintsExpandY,
+ 3, 3, 2, 2);
+ lHBot = new TGLayoutHints(kLHintsBottom | kLHintsRight,
+ 3, 3, 2, 2);
+
+ lHExpXCen = new TGLayoutHints( kLHintsTop | kLHintsLeft |
+ kLHintsExpandX | kLHintsCenterY,
+ 5, 5, 2, 2);
+ lHFixedCen = new TGLayoutHints( kLHintsTop | kLHintsLeft |
+ kLHintsCenterY,
+ 5, 5, 2, 2);
+
+ /* --------- Create the Dialog -------------- */
+ buttonFrame = new TGHorizontalFrame(this, 240, 20, kFixedWidth);
+ okButton = new TGTextButton(buttonFrame, "&Ok", REAC_OK);
+ okButton->Associate(this);
+ execButton = new TGTextButton(buttonFrame, "&Execute", REAC_EXEC);
+ execButton->Associate(this);
+ resetButton = new TGTextButton(buttonFrame, "&Reset", REAC_RESET);
+ resetButton->Associate(this);
+ closeButton = new TGTextButton(buttonFrame, "&Close", REAC_CLOSE);
+ closeButton->Associate(this);
+
+ buttonFrame->AddFrame(okButton, lHExpX);
+ buttonFrame->AddFrame(execButton, lHExpX);
+ buttonFrame->AddFrame(resetButton, lHExpX);
+ buttonFrame->AddFrame(closeButton, lHExpX);
+ AddFrame(buttonFrame, lHBot);
+
+ /* ------------ Material --------------- */
+ materialGroup = new TGGroupFrame(this,"Material",kVerticalFrame);
+
+ /* ----- First Sub-Frame ---- */
+ frm1 = new TGHorizontalFrame(
+ materialGroup, w, 36,
+ kChildFrame|kFitWidth );
+frm1->ChangeBackground(0xFF00);
+
+ elementLbl = new TGLabel(frm1,"Element:");
+ elementLbl->SetTextJustify(kTextRight | kTextCenterY);
+ frm1->AddFrame(elementLbl,lHFixedCen);
+
+ elementBuf = new TGTextBuffer(20);
+ elementText = new TGTextEntry(frm1,elementBuf);
+ elementText->Resize(50, elementText->GetDefaultHeight());
+ elementText->Associate(this);
+ frm1->AddFrame(elementText,lHFixedCen);
+
+ elementStep = new XSStepButton(frm1,REAC_ELEMENT_STEP);
+ elementStep->Associate(this);
+ frm1->AddFrame(elementStep,lHFixedCen);
+
+ nameLbl = new TGLabel(frm1,"X",blueBoldGC);
+ nameLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ frm1->AddFrame(nameLbl,lHExpXCen);
+
+ ptableButton = new TGPictureButton(frm1,
+ fClient->GetPicture(PTBL_ICON),
+ REAC_PTABLE);
+ ptableButton->SetToolTipText(
+ "Choose the Element from the Periodic Table");
+ ptableButton->Associate(this);
+ frm1->AddFrame(ptableButton,lHFixedCen);
+
+ materialGroup->AddFrame(frm1,lHExpX);
+
+ /* ----- Second Sub-Frame ---- */
+ frm2 = new TGHorizontalFrame(materialGroup,w,20,
+ kChildFrame|kFitWidth);
+
+ Vfrm1 = new TGCompositeFrame(frm2, w, 70,
+ kChildFrame|kFitHeight|kFitWidth);
+ Vfrm1->SetLayoutManager(new TGMatrixLayout(Vfrm1,0,4));
+
+ chargeLbl = new TGLabel(Vfrm1,"Charge (Z):");
+ chargeLbl->SetTextJustify(kTextRight | kTextCenterY);
+ Vfrm1->AddFrame(chargeLbl);
+
+ zLbl = new TGLabel(Vfrm1,"ZZZZZZZZ",blueBoldGC);
+ zLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm1->AddFrame(zLbl);
+
+ massLbl = new TGLabel(Vfrm1,"Atomic Mass:");
+ massLbl->SetTextJustify(kTextRight | kTextCenterY);
+ Vfrm1->AddFrame(massLbl);
+
+ massValLbl = new TGLabel(Vfrm1,"ZZZZZZZZ",blueBoldGC);
+ massValLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm1->AddFrame(massValLbl);
+
+ densityLbl = new TGLabel(Vfrm1,"Density:");
+ densityLbl->SetTextJustify(kTextRight | kTextCenterY);
+ Vfrm1->AddFrame(densityLbl);
+
+ densityValLbl = new TGLabel(Vfrm1,"ZZZZZZZZ",blueBoldGC);
+ densityValLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm1->AddFrame(densityValLbl);
+
+ oxidationLbl = new TGLabel(Vfrm1,"Oxidation:");
+ oxidationLbl->SetTextJustify(kTextRight | kTextCenterY);
+ Vfrm1->AddFrame(oxidationLbl);
+
+ oxidationValLbl = new TGLabel(Vfrm1,"ZZZZZZZZ",blueBoldGC);
+ oxidationValLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm1->AddFrame(oxidationValLbl);
+
+ meltingPtLbl = new TGLabel(Vfrm1,"Melting Pt (C):");
+ meltingPtLbl->SetTextJustify(kTextRight | kTextCenterY);
+ Vfrm1->AddFrame(meltingPtLbl);
+
+ meltingValLbl = new TGLabel(Vfrm1,"ZZZZZZZZ",blueBoldGC);
+ meltingValLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm1->AddFrame(meltingValLbl);
+
+ boilingPtLbl = new TGLabel(Vfrm1,"Boiling Pt (C):");
+ boilingPtLbl->SetTextJustify(kTextRight | kTextCenterY);
+ Vfrm1->AddFrame(boilingPtLbl);
+
+ boilingValLbl = new TGLabel(Vfrm1,"ZZZZZZZZ",blueBoldGC);
+ boilingValLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm1->AddFrame(boilingValLbl);
+
+ frm2->AddFrame(Vfrm1,lHExpX);
+ materialGroup->AddFrame(frm2,lHExpX);
+
+ /* ----- Fourth Sub-Frame ---- */
+ frm3 = new TGHorizontalFrame(materialGroup,w,20,
+ kChildFrame|kFitWidth);
+
+ isotopeLbl = new TGLabel(frm3,"Isotope (A):");
+ isotopeLbl->SetTextJustify(kTextRight | kTextCenterY);
+ frm3->AddFrame(isotopeLbl,lHFixedCen);
+
+ isotopeCombo = new TGComboBox(frm3,ISOTOPE_COMBO);
+ isotopeCombo->Resize(80,20);
+ isotopeCombo->Associate(this);
+ frm3->AddFrame(isotopeCombo,lHFixedCen);
+
+ isotopeInfoLbl = new TGLabel(frm3,"Isotope Info:");
+ isotopeInfoLbl->SetTextJustify(kTextRight | kTextCenterY);
+ frm3->AddFrame(isotopeInfoLbl,lHFixedCen);
+
+ isotopeInfoValLbl = new TGLabel(frm3,"MMMM",blueBoldGC);
+ isotopeInfoValLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ frm3->AddFrame(isotopeInfoValLbl,lHExpXCen);
+
+ materialGroup->AddFrame(frm3,lHExpX);
+
+ AddFrame(materialGroup,lHExpX);
+
+ /* --------------- Reaction ------------------ */
+ reactionGroup = new TGGroupFrame(this,"Reaction",kVerticalFrame);
+
+ frm4 = new TGHorizontalFrame(reactionGroup,w,60,
+ kChildFrame|kFitWidth);
+
+ Vfrm2 = new TGCompositeFrame(frm4, 160, 70,
+ kChildFrame|kFitHeight|kFitWidth);
+
+ Vfrm2->SetLayoutManager(new TGMatrixLayout(Vfrm2,0,2));
+
+ projectileLbl = new TGLabel(Vfrm2,"Projectile:");
+ projectileLbl->SetTextJustify(kTextRight | kTextCenterY);
+ Vfrm2->AddFrame(projectileLbl);
+
+ projectileCombo = new TGComboBox(Vfrm2,PROJECTILE_COMBO);
+ projectileCombo->Resize(90,20);
+ projectileCombo->Associate(this);
+ Vfrm2->AddFrame(projectileCombo);
+
+ temperatureLbl = new TGLabel(Vfrm2,"Temperature:");
+ temperatureLbl->SetTextJustify(kTextRight | kTextCenterY);
+ Vfrm2->AddFrame(temperatureLbl);
+
+ temperatureCombo = new TGComboBox(Vfrm2,TEMPERATURE_COMBO);
+ temperatureCombo->Resize(90,20);
+ temperatureCombo->Associate(this);
+ Vfrm2->AddFrame(temperatureCombo);
+
+ databaseLbl = new TGLabel(Vfrm2,"Database:");
+ databaseLbl->SetTextJustify(kTextRight | kTextCenterY);
+ Vfrm2->AddFrame(databaseLbl);
+
+ databaseCombo = new TGComboBox(Vfrm2,DATABASE_COMBO);
+ databaseCombo->Resize(90,20);
+ databaseCombo->Associate(this);
+ Vfrm2->AddFrame(databaseCombo);
+
+ frm4->AddFrame(Vfrm2,lHExpXCen);
+
+ reactionLbl = new TGLabel(frm4,"Reaction:");
+ reactionLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ frm4->AddFrame(reactionLbl,lHFixedCen);
+
+ reactionList = new TGListBox(frm4,REACTION_LISTBOX);
+ reactionList->Resize(70,80);
+ //reactionList->SetMultipleSelections(kTRUE);
+ reactionList->Associate(this);
+ frm4->AddFrame(reactionList,lHExpXCen);
+
+ reactionGroup->AddFrame(frm4,lHExpX);
+
+ // --- Second sub frame ---
+ frm5 = new TGHorizontalFrame(reactionGroup,w,20,
+ kChildFrame|kFitWidth);
+ reactionInfoLbl = new TGLabel(frm5,"Reaction Info:");
+ reactionInfoLbl->SetTextJustify(kTextRight | kTextCenterY);
+ frm5->AddFrame(reactionInfoLbl,lHFixedCen);
+
+ reactionInfoValLbl = new TGLabel(frm5,"-",blueBoldGC);
+ reactionInfoValLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ frm5->AddFrame(reactionInfoValLbl,lHExpXCen);
+
+ reactionGroup->AddFrame(frm5,lHExpX);
+
+ AddFrame(reactionGroup,lHExpX);
+
+ /* --------------- Options ------------------ */
+ optionGroup = new TGGroupFrame(this,"Options",kVerticalFrame);
+
+ Vfrm3 = new TGCompositeFrame(optionGroup, w, 70,
+ kChildFrame|kFitHeight|kFitWidth);
+
+ Vfrm3->SetLayoutManager(new TGMatrixLayout(Vfrm3,0,4));
+
+ lineWidthLbl = new TGLabel(Vfrm3,"Line Width:");
+ lineWidthLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm3->AddFrame(lineWidthLbl);
+
+ lineWidthCombo = new TGComboBox(Vfrm3,LINE_WIDTH_COMBO);
+ lineWidthCombo->Resize(100,20);
+ lineWidthCombo->Associate(this);
+ Vfrm3->AddFrame(lineWidthCombo);
+
+ lineColorLbl = new TGLabel(Vfrm3," Line Color:");
+ lineColorLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm3->AddFrame(lineColorLbl);
+
+ lineColorCombo = new TGComboBox(Vfrm3,LINE_COLOR_COMBO);
+ lineColorCombo->Resize(100,20);
+ lineColorCombo->Associate(this);
+ Vfrm3->AddFrame(lineColorCombo);
+
+ markerStyleLbl = new TGLabel(Vfrm3,"Marker Style:");
+ markerStyleLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm3->AddFrame(markerStyleLbl);
+
+ markerStyleCombo = new TGComboBox(Vfrm3,MARKER_STYLE_COMBO);
+ markerStyleCombo->Resize(100,20);
+ markerStyleCombo->Associate(this);
+ Vfrm3->AddFrame(markerStyleCombo);
+
+ markerColorLbl = new TGLabel(Vfrm3," Marker Color:");
+ markerColorLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm3->AddFrame(markerColorLbl);
+
+ markerColorCombo = new TGComboBox(Vfrm3, MARKER_COLOR_COMBO);
+ markerColorCombo->Resize(100,20);
+ markerColorCombo->Associate(this);
+ Vfrm3->AddFrame(markerColorCombo);
+
+ markerSizeLbl = new TGLabel(Vfrm3,"Marker Size:");
+ markerSizeLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm3->AddFrame(markerSizeLbl);
+
+ markerSizeCombo = new TGComboBox(Vfrm3, MARKER_SIZE_COMBO);
+ markerSizeCombo->Resize(100,20);
+ markerSizeCombo->Associate(this);
+ Vfrm3->AddFrame(markerSizeCombo);
+
+ errorbarColorLbl = new TGLabel(Vfrm3," ErrorBar Color:");
+ errorbarColorLbl->SetTextJustify(kTextLeft | kTextCenterY);
+ Vfrm3->AddFrame(errorbarColorLbl);
+
+ errorbarColorCombo = new TGComboBox(Vfrm3,ERRORBAR_COLOR_COMBO);
+ errorbarColorCombo->Resize(100,20);
+ errorbarColorCombo->Associate(this);
+ Vfrm3->AddFrame(errorbarColorCombo);
+
+ optionGroup->AddFrame(Vfrm3,lHExpX);
+ AddFrame(optionGroup,lHExpX);
+
+ /* -------------- Information ------------------ */
+ infoGroup = new TGGroupFrame(this,"Information",kVerticalFrame);
+
+ infoView = new TGTextView(infoGroup, 200, 100,
+ kChildFrame | kSunkenFrame);
+ infoGroup->AddFrame(infoView,lHExpXY);
+
+ AddFrame(infoGroup, lHExpXY);
+
+ /* --------- Initialize layout algorithm with Resize() -------- */
+ MapSubwindows();
+ Resize(GetDefaultSize());
+
+ /* --------- Initialise with Element Z ---------- */
+ SetElement(initZ);
+ InitCombos();
+
+ /* --------- Set Windows Position --------- */
+ int ax, ay;
+
+ if (LastWinX == -1) { // Go to the middle of parent window
+ Window_t wdum;
+ gVirtualX->TranslateCoordinates(main->GetId(), GetParent()->GetId(),
+ (((TGFrame *) main)->GetWidth() - fWidth) >> 1,
+ (((TGFrame *) main)->GetHeight() - fHeight) >> 1,
+ ax, ay, wdum);
+ ax = MAX(ax,0);
+ ay = MAX(ay,0);
+ } else {
+ ax = LastWinX;
+ ay = LastWinY;
+ }
+ Move(ax,ay);
+ SetWMPosition(ax,ay);
+
+ /* --------- Map everything -------- */
+ SetWindowName("Select Element/Reaction");
+ MapWindow();
+
+} // XSReactionDlg
+
+/* ----- ~XSReactionDlg ----- */
+XSReactionDlg::~XSReactionDlg()
+{
+ // --- Delete Layout Hints ---
+ delete lHFixed;
+ delete lHExpX;
+ delete lHExpY;
+ delete lHExpXY;
+ delete lHFixedCen;
+ delete lHExpXCen;
+
+ // --- Delete Material Group ----
+ delete elementLbl;
+ delete elementText;
+ delete elementStep;
+ delete ptableButton;
+ delete chargeLbl;
+ delete zLbl;
+ delete nameLbl;
+ delete massLbl;
+ delete massValLbl;
+ delete densityLbl;
+ delete densityValLbl;
+ delete meltingPtLbl;
+ delete meltingValLbl;
+ delete boilingPtLbl;
+ delete boilingValLbl;
+ delete oxidationLbl;
+ delete oxidationValLbl;
+ delete isotopeInfoLbl;
+ delete isotopeInfoValLbl;
+ delete isotopeLbl;
+ delete isotopeCombo;
+ delete materialGroup;
+
+ // --- Delete Reaction group ---
+ delete projectileLbl;
+ delete projectileCombo;
+ delete temperatureLbl;
+ delete temperatureCombo;
+ delete databaseLbl;
+ delete databaseCombo;
+ delete reactionLbl;
+ delete reactionList;
+ delete reactionInfoLbl;
+ delete reactionInfoValLbl;
+ delete reactionGroup;
+
+ // --- Option Group ----
+ delete lineWidthLbl;
+ delete lineColorLbl;
+ delete markerStyleLbl;
+ delete markerColorLbl;
+ delete markerSizeLbl;
+ delete errorbarColorLbl;
+
+ delete lineWidthCombo;
+ delete lineColorCombo;
+ delete markerStyleCombo;
+ delete markerColorCombo;
+ delete markerSizeCombo;
+ delete errorbarColorCombo;
+
+ delete optionGroup;
+
+ // --- Info Group ----
+ delete infoView;
+ delete infoGroup;
+
+ // --- Frames ---
+ delete frm1;
+ delete frm2;
+ delete frm3;
+ delete frm4;
+ delete frm5;
+
+ delete Vfrm1;
+ delete Vfrm2;
+ delete Vfrm3;
+
+ // --- Buttons ---
+ delete okButton;
+ delete execButton;
+ delete resetButton;
+ delete closeButton;
+ delete buttonFrame;
+} // ~XSReactionDlg
+
+/* ----- InitColorCombo ----- */
+void
+XSReactionDlg::InitColorCombo(TGComboBox *cb)
+{
+ // Normaly this should be filled with color entries!!!
+
+ cb->AddEntry("Black",0);
+ cb->AddEntry("Red",1);
+ cb->AddEntry("Green",2);
+ cb->AddEntry("Blue",3);
+ cb->AddEntry("Yellow",4);
+ cb->AddEntry("Magenta",5);
+ cb->AddEntry("Cyan",6);
+ // .......
+ cb->Select(0); // <<<< Should find the correct color...
+} // InitColorCombos
+
+/* ----- InitCombos ----- */
+void
+XSReactionDlg::InitCombos()
+{
+ InitColorCombo(lineColorCombo);
+ InitColorCombo(markerColorCombo);
+ InitColorCombo(errorbarColorCombo);
+
+ /* ---- Line Widths ----- */
+ lineWidthCombo->AddEntry("None",0);
+ lineWidthCombo->AddEntry("1",1);
+ lineWidthCombo->AddEntry("2",2);
+ lineWidthCombo->AddEntry("3",3);
+ lineWidthCombo->AddEntry("4",4);
+ lineWidthCombo->AddEntry("5",5);
+ lineWidthCombo->AddEntry("6",6);
+ lineWidthCombo->AddEntry("7",7);
+ lineWidthCombo->AddEntry("8",8);
+ lineWidthCombo->AddEntry("9",9);
+ lineWidthCombo->AddEntry("10",10);
+ lineWidthCombo->Select(1);
+ // --- Select the correct one ---
+
+ /* ---- Marker Style ----- */
+ markerStyleCombo->AddEntry("None",0);
+ markerStyleCombo->AddEntry("Bullet",1);
+ markerStyleCombo->AddEntry("Triangle Up",2);
+ markerStyleCombo->AddEntry("Triangle Down",3);
+ markerStyleCombo->AddEntry("Square",4);
+ markerStyleCombo->AddEntry("Diamond",5);
+ markerStyleCombo->AddEntry("Star",6);
+ markerStyleCombo->AddEntry("Empty Bullet",7);
+ markerStyleCombo->AddEntry("Empty Tri-Up",8);
+ markerStyleCombo->AddEntry("Empty Tri-Down",9);
+ markerStyleCombo->AddEntry("Empty Square",10);
+ markerStyleCombo->Select(0);
+ // --- Select the correct one ---
+
+ /* ---- Marker Size ----- */
+ markerSizeCombo->AddEntry("None",0);
+ markerSizeCombo->AddEntry("0.1",1);
+ markerSizeCombo->AddEntry("0.2",2);
+ markerSizeCombo->AddEntry("0.3",3);
+ markerSizeCombo->AddEntry("0.4",4);
+ markerSizeCombo->AddEntry("0.5",5);
+ markerSizeCombo->AddEntry("0.6",6);
+ markerSizeCombo->AddEntry("0.7",7);
+ markerSizeCombo->AddEntry("0.8",8);
+ markerSizeCombo->AddEntry("0.9",9);
+ markerSizeCombo->AddEntry("1.0",10);
+ markerSizeCombo->Select(0);
+
+ // --- Select the correct one ---
+} // InitCombos
+
+/* ----- GetString ------- */
+const char *
+XSReactionDlg::GetString( int box )
+{
+ const TGLBEntry *entry;
+ switch (box) {
+ case ISOTOPE_COMBO:
+ entry = isotopeCombo->GetSelectedEntry();
+ break;
+
+ case PROJECTILE_COMBO:
+ entry = projectileCombo->GetSelectedEntry();
+ break;
+
+ case TEMPERATURE_COMBO:
+ entry = temperatureCombo->GetSelectedEntry();
+ break;
+
+ case DATABASE_COMBO:
+ entry = databaseCombo->GetSelectedEntry();
+ break;
+
+ case LINE_WIDTH_COMBO:
+ entry = lineWidthCombo->GetSelectedEntry();
+ break;
+
+ case LINE_COLOR_COMBO:
+ entry = lineColorCombo->GetSelectedEntry();
+ break;
+
+ case MARKER_STYLE_COMBO:
+ entry = markerStyleCombo->GetSelectedEntry();
+ break;
+
+ case MARKER_COLOR_COMBO:
+ entry = markerColorCombo->GetSelectedEntry();
+ break;
+
+ case MARKER_SIZE_COMBO:
+ entry = markerSizeCombo->GetSelectedEntry();
+ break;
+
+ case ERRORBAR_COLOR_COMBO:
+ entry = errorbarColorCombo->GetSelectedEntry();
+ break;
+
+ case REACTION_LISTBOX:
+ entry = reactionList->GetSelectedEntry();
+ break;
+
+ default:
+ entry = NULL;
+ }
+ if (entry==NULL) return NULL;
+
+ return ((TGTextLBEntry*)entry)->GetText()->GetString();
+} // GetString
+
+/* ----- CreatePath ------ */
+char*
+XSReactionDlg::CreatePath( int option )
+{
+ static char path[256];
+
+ strcpy(path, DBDIR); // Initialise directory
+ strcat(path, XSelements->Mnemonic(Z));
+ strcat(path, PATHSEP);
+
+ if (option == PATHIsotope) return path;
+
+ /* --- add the selected isotope --- */
+ strcat(path, GetString(ISOTOPE_COMBO));
+ strcat(path, PATHSEP);
+
+ if (option == PATHProjectile) return path;
+
+ /* --- add the selected projectile --- */
+ strcat(path, GetString(PROJECTILE_COMBO));
+ strcat(path, PATHSEP);
+
+ if (option == PATHDatabase) return path;
+
+ /* --- finally add the file --- */
+ strcat(path, GetString(DATABASE_COMBO));
+
+ return path;
+} // CreatePath
+
+/* ----- UpdateContainer ----- */
+int
+XSReactionDlg::UpdateContainer( TGListBox *lb, char *path, int option)
+{
+ DIR *dirp;
+ struct dirent *entry;
+ struct stat st;
+
+ // --- First Remove everything ---
+ lb->RemoveEntries(0,1000);
+
+ // Scan directory to update the combo box
+ dirp = opendir(path);
+ if (dirp==NULL) {
+ lb->AddEntry("-",0);
+ return kTRUE; // Ooops not found
+ }
+
+ int i=0;
+ while ((entry=readdir(dirp)) != NULL) {
+ // Skip the . and .* directory entries
+ if (entry->d_name[0] == '.') continue;
+
+ char fn[256];
+ strcpy(fn,path);
+ strcat(fn,entry->d_name);
+ stat(fn,&st);
+ if (((option == DIROnlyFiles) && !S_ISDIR(st.st_mode)) ||
+ ((option == DIROnlyDirectories) && S_ISDIR(st.st_mode)) ||
+ (option == DIRBoth)) {
+ lb->AddEntry(entry->d_name,i++);
+ }
+ }
+ (void) closedir(dirp);
+ if (i==0) {
+ lb->AddEntry("None",0);
+ return kTRUE; // Ooops not found
+ }
+ return kFALSE;
+} // UpdateContainer
+
+/* ----- UpdateIsotopes ------ */
+void
+XSReactionDlg::UpdateIsotopes()
+{
+ // --- Update the isotopes ---
+ UpdateContainer(
+ isotopeCombo->GetListBox(),
+ CreatePath(PATHIsotope),
+ DIROnlyDirectories);
+ isotopeCombo->Select(0);
+} // UpdateIsotopes
+
+/* ----- UpdateProjectile ------ */
+void
+XSReactionDlg::UpdateProjectile()
+{
+ // --- Update the projectiles ---
+ UpdateContainer(
+ projectileCombo->GetListBox(),
+ CreatePath(PATHProjectile),
+ DIROnlyDirectories);
+ projectileCombo->Select(0);
+} // UpdateProjectile
+
+/* ----- UpdateDatabase ------ */
+void
+XSReactionDlg::UpdateDatabase()
+{
+ // --- Update the databases ---
+ UpdateContainer(
+ databaseCombo->GetListBox(),
+ CreatePath(PATHDatabase),
+ DIRBoth);
+ databaseCombo->Select(0);
+} // UpdateDatabase
+
+/* ----- UpdateReactions ------ */
+void
+XSReactionDlg::UpdateReactions()
+{
+ NdbMTDir elemDir;
+
+ reactionList->RemoveEntries(0,1000);
+ infoView->Clear();
+
+ if (elemDir.LoadENDF(CreatePath(PATHFile)))
+ return;
+
+ int id = 0;
+ for (int i=0; i<elemDir.Sections(); i++) {
+ if (elemDir.DIRMF(i) == 3)
+ reactionList->AddEntry(
+ XSReactionDesc->GetShort(elemDir.DIRMT(i)),
+ id++);
+ }
+ reactionList->MapSubwindows();
+ reactionList->Select(0);
+
+ // ------------------------------------------
+ // Prepare a string with information
+ TString info;
+
+ info.Append("Symbol name:\t\t");
+ info.Append(elemDir.SymbolName());
+
+ info.Append("\nLaboratory:\t\t");
+ info.Append(elemDir.Laboratory());
+
+ info.Append("\nEvaluation Date:\t");
+ info.Append(elemDir.EvaluationDate());
+
+ info.Append("\nAuthor(s):\t\t");
+ info.Append(elemDir.Author());
+
+ info.Append("\nReference:\t\t");
+ info.Append(elemDir.Reference());
+
+ info.Append("\nDistribution Date:\t");
+ info.Append(elemDir.DistributionDate());
+ info.Append("\nLast Revision Date:\t");
+ info.Append(elemDir.LastRevisionDate());
+ info.Append("\nMaster Entry Date:\t");
+ info.Append(elemDir.MasterEntryDate());
+ info.Append("\n\n");
+ info.Append(elemDir.GetInfo());
+
+ infoView->LoadBuffer(info.Data());
+} // UpdateReactions
+
+/* ----- UpdateCurIsotope ----- */
+void
+XSReactionDlg::UpdateCurIsotope()
+{
+ XSElement *elem = XSelements->Elem(Z);
+
+ const char *str = GetString(ISOTOPE_COMBO);
+ if (str)
+ isotopeInfoValLbl->SetText(
+ new TGString(elem->IsotopeInfo(str)));
+ else
+ isotopeInfoValLbl->SetText(new TGString("-"));
+
+ // --- Update combos depending on isotope ---
+ UpdateProjectile();
+ UpdateDatabase();
+ UpdateReactions();
+} // UpdateCurIsotope
+
+/* ----- SetElement ----- */
+void
+XSReactionDlg::SetElement(UInt_t aZ)
+{
+ char str[5];
+
+ Z = aZ;
+ if (Z<1)
+ Z = 1;
+ else
+ if (Z>XSelements->GetSize())
+ Z = XSelements->GetSize();
+
+
+ XSElement *elem = XSelements->Elem(Z);
+
+ elementBuf->Clear();
+ elementBuf->AddText(0,elem->Symbol());
+ fClient->NeedRedraw(elementText);
+ nameLbl->SetText(new TGString(elem->Name()));
+
+ sprintf(str,"%d",Z);
+ zLbl->SetText(new TGString(str));
+
+ // --- Update several values for element ---
+ massValLbl->SetText(new TGString(elem->AtomicWeight()));
+ densityValLbl->SetText(new TGString(elem->Density()));
+ densityValLbl->SetText(new TGString(elem->Density()));
+ meltingValLbl->SetText(new TGString(elem->MeltingPt()));
+ boilingValLbl->SetText(new TGString(elem->BoilingPt()));
+ oxidationValLbl->SetText(new TGString(elem->Oxidation()));
+
+ // --------------------------------
+ UpdateIsotopes();
+ UpdateCurIsotope();
+
+ // --------------------------------
+ // ---Update the rest of combos ---
+ // --------------------------------
+ temperatureCombo->RemoveEntries(0,1000);
+ temperatureCombo->AddEntry("0",0);
+ temperatureCombo->AddEntry("293",1);
+ temperatureCombo->AddEntry("900",2);
+ temperatureCombo->AddEntry("1000",3);
+ temperatureCombo->Select(1);
+
+
+ // Redraw everything
+ fClient->NeedRedraw(this);
+ Layout();
+} // SetElement
+
+/* ----- CloseWindow ----- */
+void
+XSReactionDlg::CloseWindow()
+{
+ // --- Remember old position ---
+ Window_t wdum;
+ gVirtualX->TranslateCoordinates(GetId(), GetParent()->GetId(),
+ 0, 0, LastWinX, LastWinY, wdum);
+
+ delete this;
+} // CloseWindow
+
+/* ----- elementEntryChanged ---- */
+void
+XSReactionDlg::ElementEntryChanged()
+{
+ const char *name;
+ UInt_t newZ;
+
+ /* --- get contents --- */
+ name = elementBuf->GetString();
+
+ /* --- check if it is a number --- */
+ newZ = atoi(name);
+ if ((newZ>0) && (newZ<=XSelements->GetSize())) {
+ SetElement(newZ);
+ return;
+ }
+
+ /* Search for the specific element */
+ newZ = XSelements->Find(name);
+
+ if (newZ == 0) {
+ // --- Error Entry ---
+ // issue message and put the old one
+ char msg[256];
+ int retval;
+ sprintf(msg,"Element %s not found!", elementBuf->GetString());
+ new TGMsgBox(fClient->GetRoot(),this,"Not found",msg,
+ kMBIconAsterisk,kMBOk,&retval);
+ SetElement(Z);
+ } else
+ SetElement(newZ);
+} // ElementEntryChanged
+
+/* ----- UpdateGraph ---- */
+void
+XSReactionDlg::UpdateGraph( NdbMTReactionXS *xs )
+{
+ char title[256];
+
+ //!!! --- Only if new ---
+ //!!! --- Else update the old one ---
+ XSGraph *gr = new XSGraph(xs);
+
+ // Prepare the title
+ sprintf(title,"%s-%s %s",
+ XSelements->Mnemonic(Z),
+ GetString(ISOTOPE_COMBO),
+ xs->Description().Data()
+ );
+
+ gr->GetGraph()->SetTitle(title);
+ gr->GetGraph()->SetFillColor(19);
+ gr->GetGraph()->SetLineColor(2);
+ gr->GetGraph()->SetLineWidth(2);
+ gr->GetGraph()->Draw("ALW");
+
+// gr->GetGraph()->GetHistogram()->SetXTitle(TString("Energy (eV)"));
+// gr->GetGraph()->GetHistogram()->SetYTitle(TString("Cross Section (barn)"));
+
+ Add2GraphList(gr);
+ fClient->NeedRedraw(canvasWindow);
+ fClient->NeedRedraw(const_cast<TGWindow*>(mainWindow));
+ canvas->Update();
+} // UpdateGraph
+
+/* ----- ExecCommand ---- */
+Bool_t
+XSReactionDlg::ExecCommand()
+{
+ // --- Load the data base ---
+ NdbMTDir el;
+ if (el.LoadENDF(CreatePath(PATHFile)))
+ return kTRUE;
+
+ // --- Get the selected reaction ---
+ const char *reacstr = GetString(REACTION_LISTBOX);
+
+ // --- Search for the reaction ---
+ for (int i=0; i<el.Sections(); i++) {
+ if (el.DIRMF(i) == 3 && XSReactionDesc->GetShort(el.DIRMT(i))) {
+ if (reacstr && !strcmp(reacstr,
+ XSReactionDesc->GetShort(el.DIRMT(i)))) {
+ NdbMTReactionXS xs(el.DIRMT(i), reacstr);
+ xs.LoadENDF(CreatePath(PATHFile));
+
+ UpdateGraph(&xs);
+ }
+ }
+ }
+ return kFALSE;
+} // ExecCommand
+
+/* ----- ProcessButton ----- */
+Bool_t
+XSReactionDlg::ProcessButton(Long_t param1, Long_t param2)
+{
+ UInt_t newZ;
+ switch (param1) {
+ case REAC_ELEMENT_STEP:
+ if (param2==XSSTEPBUTTON_UP) {
+ newZ = Z+1;
+ if (newZ > XSelements->GetSize()) Z = 1;
+ } else {
+ newZ = Z-1;
+ if (newZ<1) Z = XSelements->GetSize();
+ }
+ SetElement(newZ);
+ break;
+
+ case REAC_OK:
+ // Execute the command and close the window
+ if (!ExecCommand())
+ CloseWindow();
+ break;
+
+ case REAC_EXEC:
+ // Execute the command, but don't close the window
+ ExecCommand();
+ break;
+
+ case REAC_RESET:
+ SetElement(1);
+ break;
+
+ case REAC_CLOSE:
+ CloseWindow();
+ break;
+
+ case REAC_PTABLE:
+ newZ = Z;
+ new XSElementDlg(fClient->GetRoot(), this, &newZ);
+ if (newZ>0)
+ SetElement(newZ);
+ break;
+
+ default:
+ break;
+ }
+ return kTRUE;
+} // ProcessButton
+
+/* ----- ProcessCombo ------ */
+Bool_t
+XSReactionDlg::ProcessCombo( Long_t param1, Long_t param2 )
+{
+ printf("ComboMessage %ld %ld\n",param1,param2);
+
+ switch (param1) {
+ case ISOTOPE_COMBO:
+ UpdateCurIsotope();
+ break;
+
+ case PROJECTILE_COMBO:
+ UpdateDatabase();
+ UpdateReactions();
+ break;
+
+ case DATABASE_COMBO:
+ UpdateReactions();
+ break;
+
+ case REACTION_LISTBOX:
+////// reactionInfoValLbl->SetText(
+////// new TGString(elem->IsotopeInfo(str)));
+ break;
+
+ default:
+ // Ooops an error in the code
+ break;
+ }
+
+ return kTRUE;
+} // ProcessCombo
+
+/* ----- ProcessMessage ----- */
+Bool_t
+XSReactionDlg::ProcessMessage(Long_t msg, Long_t param1, Long_t param2)
+{
+ printf("Message = %d (%d)\n", GET_MSG(msg), GET_SUBMSG(msg));
+
+ switch (GET_MSG(msg)) {
+ case kC_COMMAND:
+ switch (GET_SUBMSG(msg)) {
+ case kCM_BUTTON:
+ ProcessButton(param1,param2);
+ break;
+
+ case kCM_COMBOBOX:
+ ProcessCombo(param1,param2);
+ break;
+
+ default:
+ break;
+ }
+ case kC_TEXTENTRY:
+ switch (GET_SUBMSG(msg)) {
+ case kTE_ENTER:
+ ElementEntryChanged();
+ break;
+ default:
+ break;
+ }
+ default:
+// printf("Message = %d (%d)\n", GET_MSG(msg), GET_SUBMSG(msg));
+ break;
+ }
+ return kTRUE;
+} // ProcessMessage
diff --git a/test/periodic/XSReactionDlg.h b/test/periodic/XSReactionDlg.h
new file mode 100644
index 0000000000000000000000000000000000000000..3b061ba255c9c912f9dc6692c8a68773ab858663
--- /dev/null
+++ b/test/periodic/XSReactionDlg.h
@@ -0,0 +1,166 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#ifndef __XSREACTION_DLG_H
+#define __XSREACTION_DLG_H
+
+#include <TGTab.h>
+#include <TGFrame.h>
+#include <TGButton.h>
+#include <TGLayout.h>
+#include <TGListBox.h>
+#include <TGComboBox.h>
+#include <TGTextView.h>
+#include <TGTextEntry.h>
+
+#include "NdbMTReactionXS.h"
+
+#include "XSStepButton.h"
+#include "XSElementList.h"
+#include "XSPeriodicTable.h"
+
+/* =========== XSReactionDlg ============== */
+class XSReactionDlg : public TGTransientFrame
+{
+protected:
+
+ UInt_t Z;
+
+ const TGWindow *mainWindow;
+
+ TGHorizontalFrame *frm1,
+ *frm2,
+ *frm3,
+ *frm4,
+ *frm5;
+
+ TGCompositeFrame *Vfrm1,
+ *Vfrm2,
+ *Vfrm3;
+
+ TGLayoutHints *lHFixed,
+ *lHExpX,
+ *lHExpY,
+ *lHExpXY,
+ *lHBot,
+ *lHExpXCen,
+ *lHFixedCen;
+
+ // ---- Material Items ----
+ TGGroupFrame *materialGroup;
+
+ TGLabel *elementLbl;
+ TGTextBuffer *elementBuf; //!
+ TGTextEntry *elementText;
+ XSStepButton *elementStep;
+
+ TGLabel *nameLbl,
+ *mnemonicLbl,
+
+ *chargeLbl,
+ *zLbl,
+
+ *massLbl,
+ *massValLbl,
+
+ *isotopeLbl,
+
+ *densityLbl,
+ *densityValLbl,
+
+ *meltingPtLbl,
+ *meltingValLbl,
+ *boilingPtLbl,
+ *boilingValLbl,
+
+ *oxidationLbl,
+ *oxidationValLbl,
+
+ *isotopeInfoLbl,
+ *isotopeInfoValLbl;
+
+ TGButton *ptableButton;
+
+ TGComboBox *isotopeCombo;
+
+ // ----- Reaction ----
+ TGGroupFrame *reactionGroup;
+
+ TGLabel *projectileLbl,
+ *temperatureLbl,
+ *databaseLbl,
+ *reactionLbl,
+ *reactionInfoLbl,
+ *reactionInfoValLbl;
+
+ TGComboBox *projectileCombo,
+ *temperatureCombo,
+ *databaseCombo;
+
+ TGListBox *reactionList;
+
+ // ----- Options -----
+ TGGroupFrame *optionGroup;
+
+ TGLabel *lineWidthLbl,
+ *lineColorLbl,
+ *markerStyleLbl,
+ *markerColorLbl,
+ *markerSizeLbl,
+ *errorbarColorLbl;
+
+ TGComboBox *lineWidthCombo,
+ *lineColorCombo,
+ *markerStyleCombo,
+ *markerColorCombo,
+ *markerSizeCombo,
+ *errorbarColorCombo;
+
+ // ----- Info Group -----
+ TGGroupFrame *infoGroup;
+
+ TGTextView *infoView;
+
+
+ // ----- Execution Buttons ----
+ TGHorizontalFrame *buttonFrame;
+ TGButton *okButton,
+ *execButton,
+ *resetButton,
+ *closeButton;
+
+
+public:
+ XSReactionDlg(const TGWindow *p,
+ const TGWindow *main, UInt_t initZ, UInt_t w, UInt_t h);
+ ~XSReactionDlg();
+
+protected:
+ void InitColorCombo(TGComboBox *cb);
+ void InitCombos();
+ const char* GetString(int box);
+ char* CreatePath(int option);
+ int UpdateContainer( TGListBox *lb, char *path, int option);
+ void UpdateCurIsotope();
+ void UpdateIsotopes();
+ void UpdateProjectile();
+ void UpdateDatabase();
+ void UpdateReactions();
+
+ void SetElement(UInt_t aZ);
+ void ElementEntryChanged();
+
+ void UpdateGraph(NdbMTReactionXS *xs);
+ Bool_t ExecCommand();
+
+ virtual void CloseWindow();
+ Bool_t ProcessButton(Long_t param1, Long_t param2);
+ Bool_t ProcessCombo(Long_t param1, Long_t param2);
+ virtual Bool_t ProcessMessage(Long_t msg, Long_t param1, Long_t param2);
+
+ //ClassDef(XSReactionDlg,1)
+}; // XSReactionDlg
+
+#endif
diff --git a/test/periodic/XSStepButton.cxx b/test/periodic/XSStepButton.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..9381fdac8ef14a3663d896c3414d5ea3a316cd67
--- /dev/null
+++ b/test/periodic/XSStepButton.cxx
@@ -0,0 +1,67 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#include "XSStepButton.h"
+
+//ClassImp(XSStepButton)
+
+/* ----- XSStepButton ----- */
+XSStepButton::XSStepButton( const TGWindow *p, Int_t id )
+ : TGCompositeFrame(p, 10, 10, kFixedSize)
+{
+ buttonId = id;
+ fMsgWindow = NULL;
+
+ lHints = new TGLayoutHints(kLHintsTop | kLHintsLeft);
+ upButton = new TGPictureButton(this,
+ fClient->GetPicture("arrow_up.xpm"),XSSTEPBUTTON_UP);
+ upButton->Associate(this);
+ downButton = new TGPictureButton(this,
+ fClient->GetPicture("arrow_down.xpm"),XSSTEPBUTTON_DOWN);
+ downButton->Associate(this);
+ AddFrame(upButton, lHints);
+ AddFrame(downButton, lHints);
+
+ width = upButton->GetDefaultWidth() + 2*fBorderWidth;
+ height = 2*upButton->GetDefaultHeight() + 2*fBorderWidth;
+
+ MapSubwindows();
+ Resize(GetDefaultSize());
+ MapWindow();
+} // XSStepButton
+
+/* ----- ~XSStepButton ----- */
+XSStepButton::~XSStepButton( )
+{
+ delete lHints;
+ delete upButton;
+ delete downButton;
+} // ~XSStepButton
+
+/* ----- ProcessMessage ----- */
+Bool_t
+XSStepButton::ProcessMessage(Long_t msg, Long_t param1, Long_t /* param2 */)
+{
+ switch (GET_MSG(msg)) {
+ case kC_COMMAND:
+ switch (GET_SUBMSG(msg)) {
+ case kCM_BUTTON:
+ // Send a message
+ if (fMsgWindow)
+ SendMessage(
+ fMsgWindow,
+ MK_MSG(kC_COMMAND,
+ kCM_BUTTON),
+ buttonId,
+ param1);
+ break;
+ default:
+ break;
+ }
+ default:
+ break;
+ }
+ return kTRUE;
+} // ProcessMessage
diff --git a/test/periodic/XSStepButton.h b/test/periodic/XSStepButton.h
new file mode 100644
index 0000000000000000000000000000000000000000..6452da877e549e68c33533b8fa1c6acc343b583c
--- /dev/null
+++ b/test/periodic/XSStepButton.h
@@ -0,0 +1,49 @@
+/*
+ * $Header$
+ * $Log$
+ */
+
+#ifndef __XSSTEPBUTTON_H
+#define __XSSTEPBUTTON_H
+
+#include <TGFrame.h>
+#include <TGButton.h>
+
+/* --- Messages that generate ---- */
+
+#define XSSTEPBUTTON_UP 0
+#define XSSTEPBUTTON_DOWN 1
+
+/* =========== XSStepButton ============== */
+class XSStepButton : public TGCompositeFrame
+{
+protected:
+ const TGWindow *fMsgWindow; // window handling listbox messages
+
+ Int_t buttonId;
+
+ TGLayoutHints *lHints;
+
+ TGPictureButton *upButton,
+ *downButton;
+
+ UInt_t width,
+ height;
+
+public:
+ XSStepButton( const TGWindow *p, Int_t id );
+ ~XSStepButton();
+
+ virtual void Associate(const TGWindow *w) { fMsgWindow = w; }
+
+ virtual Bool_t ProcessMessage(Long_t msg,
+ Long_t param1, Long_t param2);
+
+ virtual TGDimension GetDefaultSize() const
+ { return TGDimension(width,height); }
+
+
+ //ClassDef(XSStepButton,1)
+}; // XSStepButton
+
+#endif
diff --git a/test/periodic/XSVarious.cxx b/test/periodic/XSVarious.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..2434ae67996c6370ec43249b673643ee2765bf03
--- /dev/null
+++ b/test/periodic/XSVarious.cxx
@@ -0,0 +1,67 @@
+/*
+ * $Header$
+ * $Log$
+ *
+ * Various routines, and global variables
+ */
+
+#define __XSVARIOUS_CXX
+
+#include <TEnv.h>
+#include <TGClient.h>
+#include <TGWindow.h>
+#include <TGWindow.h>
+
+#include "XSGraph.h"
+#include "XSVarious.h"
+
+/* --------------- XSinitialise ---------------- */
+void
+XSinitialise( )
+{
+ XSelements = new XSElements(ISOTOPES_DESC_FILE);
+ XSReactionDesc = new NdbMTReacDesc(MT_DESC_FILE);
+ graphList = new TList();
+
+ // --- Initialise GUI variables ---
+ fixedFontStruct = gClient->GetFontByName(
+ gEnv->GetValue("Gui.NormalFont","fixed"));
+
+ // Define new graphics context.
+ memset(&gval,0,sizeof(gval));
+ gval.fMask = kGCForeground | kGCBackground | kGCFont |
+ kGCFillStyle | kGCGraphicsExposures;
+ gval.fFillStyle = kFillSolid;
+ gval.fGraphicsExposures = kFALSE;
+ gval.fFont = gVirtualX->GetFontHandle(fixedFontStruct);
+ fixedGC=gVirtualX->CreateGC(gClient->GetRoot()->GetId(), &gval);
+
+ blueFontStruct = gClient->GetFontByName(
+ gEnv->GetValue("Gui.NormalFont",
+ "-adobe-helvetica-bold-r-*-*-12-*-*-*-*-*-iso8859-1"));
+ // Define new graphics context.
+ gval.fMask = kGCForeground | kGCFont;
+ gval.fFont = gVirtualX->GetFontHandle(blueFontStruct);
+ gClient->GetColorByName("blue", gval.fForeground);
+ blueBoldGC=gVirtualX->CreateGC(gClient->GetRoot()->GetId(), &gval);
+
+} // XSinitialise
+
+/* ---------------- XSfinalise ----------------- */
+void
+XSfinalise()
+{
+ delete XSelements;
+ delete XSReactionDesc;
+ delete graphList;
+} // XSfinalise
+
+/* --------------- Add2GraphList --------------- */
+void
+Add2GraphList( XSGraph *gr)
+{
+ graphList->Add(gr);
+
+ /* --- Scan all graphs and update the canvas --- */
+ // ....
+} // Add2GraphList
diff --git a/test/periodic/XSVarious.h b/test/periodic/XSVarious.h
new file mode 100644
index 0000000000000000000000000000000000000000..bd55fb3e9e42765b0a9e972339f634e6a3e91c49
--- /dev/null
+++ b/test/periodic/XSVarious.h
@@ -0,0 +1,58 @@
+/*
+ * $Header$
+ * $Log$
+ *
+ * Various routines, and global variables
+ */
+
+#ifndef __XSVARIOUS_H
+#define __XSVARIOUS_H
+
+#include <TROOT.h>
+#include <TList.h>
+#include <TCanvas.h>
+#include <TRootEmbeddedCanvas.h>
+
+#include "NdbMTReacDesc.h"
+#include "NdbMTReactionXS.h"
+
+#include "XSGraph.h"
+#include "XSElements.h"
+
+#ifdef __XSVARIOUS_CXX
+# define EXT
+#else
+# define EXT extern
+#endif
+
+/* ---------------- Global DEFINES ---------------------- */
+#define PATHSEP "/"
+#define ICONDIR "icons" PATHSEP
+#define DBDIR "db" PATHSEP
+#define PTBL_ICON ICONDIR "ptable_s.xpm"
+#define ISOTOPES_DESC_FILE DBDIR "isotopes.dat"
+#define MT_DESC_FILE DBDIR "mt.dat"
+
+/* ---------------- Global Variables -------------------- */
+EXT XSElements *XSelements;
+EXT NdbMTReacDesc *XSReactionDesc;
+EXT TList *graphList;
+
+// --- GUI vars ---
+EXT GCValues_t gval;
+EXT FontStruct_t fixedFontStruct;
+EXT FontStruct_t blueFontStruct;
+EXT GContext_t fixedGC;
+EXT GContext_t blueBoldGC;
+
+EXT TCanvas *canvas;
+EXT TRootEmbeddedCanvas *canvasWindow;
+
+/* ----------------- function prototypes ---------------- */
+void XSinitialise();
+void XSfinalise();
+
+void Add2GraphList( XSGraph *gr);
+
+#undef EXT
+#endif
diff --git a/test/periodic/db/H/1/neutron/BROND-2.2 b/test/periodic/db/H/1/neutron/BROND-2.2
new file mode 100644
index 0000000000000000000000000000000000000000..d48c6706681452e338f4182031ddd72a55fc79b2
--- /dev/null
+++ b/test/periodic/db/H/1/neutron/BROND-2.2
@@ -0,0 +1,648 @@
+H/1 1
+ 1.00100+ 3 9.99167- 1 0 0 41 1 101 1451 1
+ 0.00000+ 0 0.00000+ 0 0 0 0 6 101 1451 2
+ 1.00000+ 0 0.00000+ 0 0 0 10 2 101 1451 3
+ 0.00000+ 0 0.00000+ 0 0 0 135 10 101 1451 4
+ 1-H - 1 FEI EVAL-DEC70 DODDER, L.STEWART,G.HALE 101 1451 5
+ DIST-JAN89 REV1-DEC90 901228 101 1451 6
+----BROND-2 MATERIAL= 101 101 1451 7
+-----INCIDENT NEUTRON DATA 101 1451 8
+------CONTENT: NEUTRON TRANSPORT 101 1451 9
+-------ENDF-6 FORMAT REVISED AND CHECKED BY M.N.NIKOLAEV 101 1451 10
+****************************************************************** 101 1451 11
+ 1-H - 1 101 1451 12
+****************************************************************** 101 1451 13
+ CONTENT OF THE FILE 101 1451 14
+ 101 1451 15
+ MF = 1 GENERAL INFORMATION 101 1451 16
+ 101 1451 17
+ MT = 451 COMMENTS WERE FORMED BY M.N.NIKOLAEV AT 101 1451 18
+ 1988 REVISION. 101 1451 19
+ 101 1451 20
+ IS BASED ON EVALUATION BY L.STEWART, HALE G. 101 1451 21
+ REF.[1] (LANL) PREPARED FOR ENDF/B-5 101 1451 22
+ LIBRARY (1970). 101 1451 23
+ THE 1988 REVISION WAS IN THE FOLLOWING: 101 1451 24
+ 101 1451 25
+ 1. SCATTERING AND CAPTURE C.-S. IN THE 101 1451 26
+ ENERGY REGION BELOW 1 KEV WERE BROUGHT 101 1451 27
+ INTO ACCORD WITH DATA RECOMMENDED BY 101 1451 28
+ MUGHABGHAB ET AL. REF.[2] AND TAKEN IN 101 1451 29
+ KORT-88 LIBRARY REF.[3]. 101 1451 30
+ 101 1451 31
+ 2. THE TOTAL C.-S. IN THE ENERGY REGION 101 1451 32
+ BELOW 1 KEV IS GIVEN IN A HIGH NUMBER OF 101 1451 33
+ ENERGY POINTS TO PROVIDE AN ACCURATE 101 1451 34
+ PRESENTATION OF THE TOTAL 101 1451 35
+ C.-S..INTERPOLATION ERROR (< 0.2%) IS 101 1451 36
+ LESS THEN C.-S. IS KNOWN. 101 1451 37
+ 101 1451 38
+ 3. ELASTIC SCATTERING HIGHER THAN 1 KEV WAS 101 1451 39
+ TAKEN AS RECOMMENDED AT ENDF/B-6 REF.[5]. 101 1451 40
+ 101 1451 41
+ 4. NEUTRON ELASTIC SCATTERING ANGULAR 101 1451 42
+ DISTRIBUTIONS ARE GIVEN THROUGH C.M.S. 101 1451 43
+ LEGENDRE COEFFICIENTS AS RECOMMENDED A 101 1451 44
+ ENDF/B-6 REF.[5]. 101 1451 45
+ 101 1451 46
+ 5. DATA ON PHOTON PRODUCTION AND DEUTERIUM 101 1451 47
+ RECOIL DATA FROM NEUTRON CAPTURE ARE 101 1451 48
+ GIVEN AT MF=6 REF.[4]. THEY REPLACE MF=12 101 1451 49
+ AND MF=14 FILES. 101 1451 50
+ 101 1451 51
+ 6. DATA ON NEUTRON THERMAL SCATTERING LAW AT 101 1451 52
+ FREE PROTONS (MF=7) ARE DISCARDED FOR 101 1451 53
+ LACK OF PRACTICAL INTEREST. 101 1451 54
+ 101 1451 55
+ 7. DATA ON COVARINCES (MF=33) ARE EXCLUDED 101 1451 56
+ DUE TO THEIR INCONSISTENCY WITH THERMAL 101 1451 57
+ NEUTRON C.-S. DATA AND DEVIATIONS FROM 101 1451 58
+ ENDF-6 FORMAT REF.[4]. MF=33 FILE WILL BE 101 1451 59
+ PREPARED LATER. 101 1451 60
+ 101 1451 61
+ * NEUTRON C.S. DATA FOR HYDROGEN SATISFY * 101 1451 62
+ * THE REQUIREMENTS OF THE NUCLEAR * 101 1451 63
+ * REACTOR DESIGN * 101 1451 64
+ * * 101 1451 65
+ 101 1451 66
+ * NEUTRON ELASTIC SCATTERING C.S. AT * 101 1451 67
+ * HYDROGEN IS RECOMMENDED TO USE AS * 101 1451 68
+ * STANDARD FOR NEUTRON C.-S. * 101 1451 69
+ * MEASUREMENTS. * 101 1451 70
+ * * 101 1451 71
+ 101 1451 72
+ -------------------------------------------------- 101 1451 73
+ * C.-S. AT 0.0253 EV: * 101 1451 74
+ * ELASTIC SCATTERING (MT=2) - 20.491+- 0.0140 B * 101 1451 75
+ * RAD.CAPTURE(MT=102) - 0.3326 +- 0.0007 B * 101 1451 76
+ -------------------------------------------------- 101 1451 77
+ 101 1451 78
+ MF = 2 RESONANCE PARAMETERS: 101 1451 79
+ 101 1451 80
+ MT = 151 SCATTERING LENGTH L=1.27696E-12 CM. 101 1451 81
+ 101 1451 82
+ MF = 3 NEUTRON CROSS-SECTIONS: 101 1451 83
+ 101 1451 84
+ MT = 1 TOTAL C.-S. IS OBTAINED AS SUM OF ELASTIC 101 1451 85
+ SCATTERING AND RADIOACTIVE CAPTURE C.-S. 101 1451 86
+ 101 1451 87
+ MT = 2 ELASTIC SCATTERING C.-S. WAS EVALUATED BY 101 1451 88
+ DODDER AND HALE (LANL) THROUGH THEORETICAL 101 1451 89
+ ANALYSIS OF EXPERIMENTAL DATA. THE DATA WERE 101 1451 90
+ CORRECTED (<0.2%) BELOW 1 KEV TO PROVIDE THE 101 1451 91
+ COINSISTENCY WITH EVALUATION REF.[2] OF THE 101 1451 92
+ THERMAL NEUTRON SCATTERING C.-S. AT FREE 101 1451 93
+ HYDROGEN ATOMS. 101 1451 94
+ 101 1451 95
+ MT = 102 RADIATIVE CAPTURE C.-S. WAS TAKEN AS 101 1451 96
+ PREPARED BY A.HORSLEY [6]. THE RESULTS OF 101 1451 97
+ THIS EVALUATION WERE CORRECTED (<0.2%) BELOW 101 1451 98
+ 1 KEV FOR CONSISTENCY WITH EVALUATION REF.[2] 101 1451 99
+ OF THE THERMAL NEUTRON CAPTURE C.-S. 101 1451 100
+ 101 1451 101
+ MT = 251, 252, 253 DATA OBTAINED BY CALCULATIONS 101 1451 102
+ FROM FILE MF=4 OF ANGULAR DISTRIBUTIONS OF 101 1451 103
+ ELASTIC SCATTERING (MT=2). 101 1451 104
+ 101 1451 105
+ MF = 4 MT = 2 NEUTRONS ELASTIC SCATTERING ANGULAR 101 1451 106
+ DISTRIBUTIONS ARE GIVEN BY LEGENDRE 101 1451 107
+ POLYNOMIAL COEFFICIENTS IN CMS. A WEAK 101 1451 108
+ ANISOTROPY OF SCATTERING IS APPEAR STARTING 101 1451 109
+ FROM HUNDREDS KEV. DATA CORRESPOND TO DODDER 101 1451 110
+ AND HALE EVALUATION PREPARED FOR ENDF/B-6 101 1451 111
+ LIBRARY. 101 1451 112
+ 101 1451 113
+ MF = 6 MT = 102 PHOTON AND DEUTERIUM RECOIL ENERGY SPECTRA 101 1451 114
+ ARE GIVEN. ISOTROPIC ANGULAR DISTRIBUTIONS IN 101 1451 115
+ CMS. THIS SPECTRA ARE TAKEN IN CMS AS 101 1451 116
+ NONDEPENDENT FROM SCATTERING ANGLE. THEY ARE 101 1451 117
+ PRESENTED AS DELTA-FUNCTION, WITH ENERGY 101 1451 118
+ POSITION LINEAR DEPENDENT FROM NEUTRON 101 1451 119
+ ENERGY. 101 1451 120
+ 101 1451 121
+ REFERENCES 101 1451 122
+ 101 1451 123
+ 1. KINSEY R., ENDF/B-5 SUMMARY DOCUMENTATION, ENDF-201. 101 1451 124
+ NEW-YORK, 1979. 101 1451 125
+ 2. MUGHABGHAB S.F. DIVADEENAM M., HOLDEN N.E. NEUTRON 101 1451 126
+ CROSS SECTIONS. V.1. NEUTRON RESONANCE PARAMETERS AND 101 1451 127
+ THERMAL CROSS SECTIONS NNDC BNL NY ACADEMIC PRESS, 101 1451 128
+ 1981. 101 1451 129
+ 3. ABAGYAN L.P.,YUDKEVICH M.S. VOPROSY ATOMNOJ NAUKI I 101 1451 130
+ TEKHNIKI,SER. YADERNYE KONSTANTY, 1(40), 1981, P.39. 101 1451 131
+ 4. ROSE P.F., DUNFORD C.L. DATA FORMATS AND PROCEDURES FOR 101 1451 132
+ THE EVALUATED DATA FILE ENDF. ENDF-102. NNDC BNL, 1988. 101 1451 133
+ 5. SEE ENDF/B-6 NEUTRON STANDARD FILE MAT=125, MF=1, 101 1451 134
+ MT=451, 1987. 101 1451 135
+ 6. HORSLEY A. NUCLEAR DATA A2, 243, 1966. 101 1451 136
+ 101 1451 137
+************************ C O N T E N T S ************************ 101 1451 138
+ (MF) (MT) (CARDS) 101 1451 139
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+-9.573000-3 2.250400-3-8.177900-5 1.804400-5 7.587300-8 3.766600-8 101 4 2 566
+ 0.000000+0 7.500000+6 0 0 6 0 101 4 2 567
+-1.025400-2 2.469800-3-1.061500-4 2.380200-5 9.178600-8 5.835400-8 101 4 2 568
+ 0.000000+0 8.000000+6 0 0 6 0 101 4 2 569
+-1.091300-2 2.683900-3-1.352000-4 3.075000-5 1.037700-7 8.775100-8 101 4 2 570
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+-1.154700-2 2.891400-3-1.693000-4 3.899900-5 1.071600-7 1.285300-7 101 4 2 572
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+-1.215400-2 3.091200-3-2.088200-4 4.865400-5 9.550800-8 1.838900-7 101 4 2 574
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+-1.327700-2 3.464700-3-3.053300-4 7.254700-5-1.005200-8 3.540700-7 101 4 2 578
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+-1.379100-2 3.637400-3-3.628100-4 8.693800-5-1.293000-7 4.782900-7 101 4 2 580
+ 0.000000+0 1.100000+7 0 0 6 0 101 4 2 581
+-1.427100-2 3.800500-3-4.266800-4 1.030300-4-3.150700-7 6.359500-7 101 4 2 582
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+-1.471700-2 3.953900-3-4.970100-4 1.208800-4-5.886800-7 8.333400-7 101 4 2 584
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+-1.512700-2 4.098000-3-5.738300-4 1.404900-4-9.756100-7 1.077400-6 101 4 2 586
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+-1.550200-2 4.233300-3-6.570900-4 1.618900-4-1.506000-6 1.375600-6 101 4 2 588
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+-1.584100-2 4.360400-3-7.466400-4 1.850500-4-2.215000-6 1.735800-6 101 4 2 590
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+-1.614500-2 4.480300-3-8.422500-4 2.099600-4-3.143100-6 2.166600-6 101 4 2 592
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+-1.684100-2 4.809100-3-1.161800-3 2.948100-4-7.736700-6 3.967600-6 101 4 2 598
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+-1.700200-2 4.913900-3-1.277500-3 3.262900-4-1.006700-5 4.765600-6 101 4 2 600
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+-1.713000-2 5.019600-3-1.396600-3 3.592600-4-1.291100-5 5.675100-6 101 4 2 602
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+-1.728200-2 5.244000-3-1.641500-3 4.295000-4-2.046100-5 7.851600-6 101 4 2 604
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+-1.697400-2 6.264600-3-2.339400-3 6.737900-4-6.481300-5 1.721100-5 101 4 2 610
+ 101 4 0 611
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+ 1.00200+ 3 1.99680+ 0 0 1 1 2 101 6102 614
+ 2 2 101 6102 615
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+ 0.00000+ 0 0.00000+ 0 1 2 1 5 101 6102 617
+ 5 2 101 6102 618
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+ 1.38540+ 3 1.00000+ 0 101 6102 620
+ 0.00000+ 0 1.00000+ 6 1 0 2 1 101 6102 621
+ 5.02286+ 5 1.00000+ 0 101 6102 622
+ 0.00000+ 0 5.00000+ 6 1 0 2 1 101 6102 623
+ 2.50729+ 6 1.00000+ 0 101 6102 624
+ 0.00000+ 0 1.00000+ 7 1 0 2 1 101 6102 625
+ 5.01668+ 6 1.00000+ 0 101 6102 626
+ 0.00000+ 0 2.00000+ 7 1 0 2 1 101 6102 627
+ 1.00460+ 7 1.00000+ 0 101 6102 628
+ 0.00000+ 0 0.00000+ 0 0 1 1 2 101 6102 629
+ 2 2 101 6102 630
+ 1.00000- 5 1.00000+ 0 2.00000+ 7 1.00000+ 0 101 6102 631
+ 0.00000+ 0 0.00000+ 0 1 2 1 5 101 6102 632
+ 5 2 101 6102 633
+ 0.00000+ 0 1.00000- 5 1 0 2 1 101 6102 634
+ 2.22324+ 6 1.00000+ 0 101 6102 635
+ 0.00000+ 0 1.00000+ 6 1 0 2 1 101 6102 636
+ 2.72234+ 6 1.00000+ 0 101 6102 637
+ 0.00000+ 0 5.00000+ 6 1 0 2 1 101 6102 638
+ 4.71734+ 6 1.00000+ 0 101 6102 639
+ 0.00000+ 0 1.00000+ 7 1 0 2 1 101 6102 640
+ 7.20795+ 6 1.00000+ 0 101 6102 641
+ 0.00000+ 0 2.00000+ 7 1 0 2 1 101 6102 642
+ 1.21787+ 7 1.00000+ 0 101 6102 643
+ 101 6 0 644
+ 101 0 0 645
+ 0 0 0 646
+ -1 0 0
diff --git a/test/periodic/db/H/1/neutron/ENDF-B6 b/test/periodic/db/H/1/neutron/ENDF-B6
new file mode 100644
index 0000000000000000000000000000000000000000..822b38c9269e4d14f89b307a4d2a217292233c75
--- /dev/null
+++ b/test/periodic/db/H/1/neutron/ENDF-B6
@@ -0,0 +1,707 @@
+H-1 (neutron) revision 1 from tape120 1 0 0 0
+ 1.001000+3 9.991700-1 0 0 0 2 125 1451 1
+ 0.000000+0 0.000000+0 0 0 0 6 125 1451 2
+ 1.000000+0 0.000000+0 0 0 10 6 125 1451 3
+ 0.000000+0 0.000000+0 0 0 90 8 125 1451 4
+ 1-H - 1 LANL EVAL-OCT89 HALE, DODDER, SICILIANO, WILSON 125 1451 5
+ NO REF TO DATE DIST-SEP91 REV1-JUL91 910806 125 1451 6
+----ENDF/B-VI MATERIAL 125 REVISION 1 125 1451 7
+-----INCIDENT NEUTRON DATA 125 1451 8
+------ENDF-6 FORMAT 125 1451 9
+ ***************************************************************** 125 1451 10
+ 125 1451 11
+ MOD1 OF ENDF/B-VI 125 1451 12
+ 125 1451 13
+ THE ONLY REVISION MADE FOR MOD1 OF ENDF/B-VI WAS TO ADD THE 125 1451 14
+ COMMENTS BELOW ON THE STANDARDS COVARIANCES. THE DESCRIPTION 125 1451 15
+ OF THE ENDF/B-VI EVALUATION IS GIVEN BELOW. 125 1451 16
+ 125 1451 17
+ ***************************************************************** 125 1451 18
+ 125 1451 19
+ ENDF/B-VI DESCRIPTION 125 1451 20
+ 125 1451 21
+ G. M. Hale, D. C. Dodder, E. R. Siciliano and W. B. Wilson 125 1451 22
+ Los Alamos National Laboratory 125 1451 23
+ Theoretical Division 125 1451 24
+ Applied Nuclear Science Group (T-2) 125 1451 25
+ Mail stop B243 125 1451 26
+ Los Alamos, New Mexico 87544 125 1451 27
+ 125 1451 28
+ this is a completely new evaluation independent of endf/b-v, 125 1451 29
+ except as noted below. 125 1451 30
+ elastic cross sections and angular distributions below 125 1451 31
+ 30 mev were determined with a new r-matrix 125 1451 32
+ calculation by hale and dodder. this calculation gives 125 1451 33
+ the endf/b-vi elastic scattering cross sections for 125 1451 34
+ hydrogen below 20 mev. 125 1451 35
+ also, elastic cross sections and angular distributions above 125 1451 36
+ 20 mev were calculated with the npscat code using phase 125 1451 37
+ shifts of arndt by siciliano and wilson. 125 1451 38
+ angular distributions at 26 mev agreed well: below this 125 1451 39
+ energy r-matrix angular distributions were used; at and 125 1451 40
+ above 26 mev phase shift angular distributions were used. 125 1451 41
+ elastic cross sections below 26 mev were taken from the 125 1451 42
+ r-matrix work; those above 30 mev were taken from the 125 1451 43
+ phase shift work. between these energies the elastic 125 1451 44
+ cross section was taken as follows: 125 1451 45
+ 125 1451 46
+ e (ev) r-matrix phase shift mf3mt2 125 1451 47
+ ---------- ----------- -------------- ---------- 125 1451 48
+ 2.6e+07 .36345 .36029 .36345 125 1451 49
+ 2.7e+07 .34859 .34811 125 1451 50
+ 2.8e+07 .33488 .33104 .33295 125 1451 51
+ 2.9e+07 .32227 .31891 125 1451 52
+ 3.0e+07 .31080 .30567 .30567 125 1451 53
+ 125 1451 54
+ 125 1451 55
+ These calculated results were merged with available n-gamma 125 1451 56
+ data by wilson. endf/b-v (n,gamma) data were used below 125 1451 57
+ 20 mev; above this energy, an approximation to the data 125 1451 58
+ of M. Bosman et al.(phys.lett.82b,212[1979]) was used. 125 1451 59
+ The (n,gamma) was adjusted to agree exactly with Mughabghab 125 1451 60
+ (1983) value at thermal (0.3326 b), and lower energies 125 1451 61
+ were modified according to 1/v law (P. Young, 10/17/89). 125 1451 62
+ The total cross section was then summed again to reflect 125 1451 63
+ the revised (n,gamma). 125 1451 64
+ 125 1451 65
+ 125 1451 66
+ mf2 mt151 was taken from endf/b-v 125 1451 67
+ 125 1451 68
+ mf12 mt102 and mf14 mt102 are also taken from ENDF/B-V. 125 1451 69
+ 125 1451 70
+ **************************************************************** 125 1451 71
+ 125 1451 72
+ STANDARDS COVARIANCES 125 1451 73
+ 125 1451 74
+ Phase 1 reviewers of the ENDF/B-VI standards cross sections have 125 1451 75
+ expressed the concern that the uncertainties resulting from the 125 1451 76
+ combination of R-matrix and simultaneous evaluations might have 125 1451 77
+ led to uncertainties that are too small. As a result, the 125 1451 78
+ Standards Subcommittee produced (at the May, 1990 CSEWG meeting) 125 1451 79
+ a set of expanded covariance estimates for the standard cross 125 1451 80
+ section reactions. These uncertainties are estimates such that 125 1451 81
+ if a modern day experiment were performed on a given standard 125 1451 82
+ cross section using the best techniques, approximately 2/3 of 125 1451 83
+ the results should fall within these expanded uncertainties. The 125 1451 84
+ expanded uncertainties for the n + H-1 total cross section are 125 1451 85
+ as follows: 125 1451 86
+ 125 1451 87
+ Energy Range Estimated Uncertainty 125 1451 88
+ (keV) (percent) 125 1451 89
+ 125 1451 90
+ 1.0E-08 - 20000 0.2 125 1451 91
+ 125 1451 92
+ **************************************************************** 125 1451 93
+ 125 1451 94
+ 1 451 102 2 125 1451 95
+ 2 151 4 0 125 1451 96
+ 3 1 110 1 125 1451 97
+ 3 2 52 1 125 1451 98
+ 3 102 53 1 125 1451 99
+ 4 2 364 1 125 1451 100
+ 12 102 4 0 125 1451 101
+ 14 102 1 0 125 1451 102
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+-2.111100-3 1.227000-3-2.149500-4 4.157700-5 8.661400-9 2.084800-8 125 4 2 660
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+-3.513800-2 1.409100-1 4.125700-3 1.645100-2-5.781900-3 9.196500-3 125 4 2 683
+-2.874500-3 1.755200-3-3.244700-4 6.198100-5 3.663900-8-1.266700-8 125 4 2 684
+ 6.101100-9-8.878600-9 125 4 2 685
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+-3.006900-3 1.850100-3-3.449500-4 6.570500-5-7.609800-9 1.162500-8 125 4 2 688
+-3.248300-8-1.548400-8 125 4 2 689
+ 0.000000+0 1.000000+8 0 0 14 0 125 4 2 690
+-3.842600-2 1.467500-1 4.366500-3 1.725300-2-5.967700-3 9.939200-3 125 4 2 691
+-3.140200-3 1.946500-3-3.658300-4 6.945200-5-9.406800-9 2.668200-8 125 4 2 692
+-3.062100-8 3.964800-8 125 4 2 693
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+ 0.000000+0 0.000000+0 0 0 0 0 12512 0 700
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+ 0.000000+0 0.000000+0 0 0 0 0 0 0 0 705
+ 0.000000+0 0.000000+0 0 0 0 0 -1 0 0 0
diff --git a/test/periodic/db/H/1/neutron/JEF-2.2 b/test/periodic/db/H/1/neutron/JEF-2.2
new file mode 100644
index 0000000000000000000000000000000000000000..5e693251993df250be454167c9407ce1190f693c
--- /dev/null
+++ b/test/periodic/db/H/1/neutron/JEF-2.2
@@ -0,0 +1,530 @@
+H/1 1
+ 1.001000+3 9.991700-1 0 0 2 0 125 1451 1
+ 0.000000+0 0.000000+0 0 0 0 6 125 1451 2
+ 1.000000+0 0.000000+0 0 0 10 22 125 1451 3
+ 0.000000+0 0.000000+0 0 0 109 11 125 1451 4
+ 1-H - 1 NEA RCOM-JUN82 SCIENTIFIC CO-ORDINATION GROUP 125 1451 5
+ DIST-JAN92 920101 125 1451 6
+----JEF-2 MATERIAL 125 125 1451 7
+-----INCIDENT NEUTRON DATA 125 1451 8
+------ENDF-6 FORMAT 125 1451 9
+****************************************************************** 125 1451 10
+* JEF-2 * 125 1451 11
+* DATA WERE TAKEN FROM ENDF/B-V(MAT=1301). * 125 1451 12
+****************************************************************** 125 1451 13
+* 30-MAY-89: NEW ELASTIC CROSS SECTIONS AND ANGULAR DISTR. 125 1451 14
+* INSERTED FROM THE PREL. ENDF/B-VI STANDARDS 125 1451 15
+* EVALUATION. TOTAL CROSS SECTION RECONSTRUCTED. 125 1451 16
+****************************************************************** 125 1451 17
+ 125 1451 18
+ LASL EVAL-AUG70 L.STEWART, R.J.LABAUVE, P.G.YOUNG 125 1451 19
+ LA-4574 (1971) DIST-MAY79 REV1-JAN77 790426 125 1451 20
+ 125 1451 21
+ 125 1451 22
+ 125 1451 23
+ CHANGES FROM ENDF/B-IV TO ENDF/B-V 125 1451 24
+ 125 1451 25
+ 1. INTERPOLATION RULES ON MT=1 AND MT=2 125 1451 26
+ 2. FILE 33 ADDED. 125 1451 27
+ 125 1451 28
+ CHANGES FROM ENDF/B-III TO ENDF/B-IV 125 1451 29
+ 125 1451 30
+ 1. TOTALS RECONSTRUCTED TO HIGHER PRECISION 125 1451 31
+ 2. THE LP FLAG HAS BEEN IMPLEMENTED IN FILE 12, MT=102 125 1451 32
+ 125 1451 33
+****************************************************************** 125 1451 34
+ 125 1451 35
+ CROSS SECTION STANDARD - HYDROGEN SCATTERING CROSS SECTION 125 1451 36
+ 125 1451 37
+ 1 KEV - 20 MEV 125 1451 38
+ 125 1451 39
+ RECOMMENDED BY CSEWG NORMALIZATION AND STANDARDS SUBCOMMITTEE 125 1451 40
+ 125 1451 41
+ FOR A COMPLETE DESCRIPTION OF VERSION IV SEE LA-6518-MS 125 1451 42
+ BY G.M.HALE, L.STEWART, AND P.G.YOUNG 125 1451 43
+ 125 1451 44
+****************************************************************** 125 1451 45
+ 125 1451 46
+ 125 1451 47
+ MF=1 125 1451 48
+ 125 1451 49
+ MT=451, ATOMIC MASS=1.007825 125 1451 50
+ 125 1451 51
+ MF=2 125 1451 52
+ 125 1451 53
+ MT=151, SCATTERING LENGTH=1.27565E-12 CM. 125 1451 54
+ 125 1451 55
+ MF=3 125 1451 56
+ 125 1451 57
+ MT= 1, TOTAL CROSS SECTIONS --- THE TOTAL CROSS SECTIONS ARE 125 1451 58
+ OBTAINED BY ADDING THE ELASTIC SCATTERING AND 125 1451 59
+ RADIATIVE CAPTURE CROSS SECTIONS AT ALL ENERGIES. 125 1451 60
+ 1.0E-05 EV TO 20 MEV. 125 1451 61
+ 125 1451 62
+ MT= 2, ELASTIC SCATTERING --- FROM AN EXTENSIVE THEORETICAL 125 1451 63
+ TREATMENT OF FAST NEUTRON MEASUREMENTS 125 1451 64
+ BY J. C. HOPKINS(LASL) AND G. BREIT(STATE 125 1451 65
+ UNIVERSITY OF NEW YORK). SEE N.D. A9, 145(1971). 125 1451 66
+ 1.0E-05 EV TO 20 MEV. 125 1451 67
+ 125 1451 68
+ MT=102, RADIATIVE CAPTURE --- THESE CROSS SECTIONS ARE TAKEN 125 1451 69
+ FROM THE PUBLICATION OF A. HORLEY WHERE A VALUE 125 1451 70
+ OF 332 MB WAS ADOPTED FOR THE THERMAL VALUE. SEE 125 1451 71
+ N.D. A2, 243(1966) ALSO P.C. 125 1451 72
+ 1.0E-05 EV TO 20 MEV. 125 1451 73
+ 125 1451 74
+ MT=251, AVERAGE VALUE OF COSINE OF SCATTERING ANGLE 125 1451 75
+ IN LAB SYSTEM (PROVIDED BY BNL). 125 1451 76
+ 1.0E-05 EV T0 20 MEV. 125 1451 77
+ 125 1451 78
+ MT=252, AVERAGE LOGARITHMIC ENERGY CHANGE PER COLLISON, 125 1451 79
+ , FROM 1.0E-05 EV TO 20 MEV. (PROVIDED BY BNL). 125 1451 80
+ 125 1451 81
+ MT=253, GAMMA, , FROM 1.0E-05 EV TO 20 MEV. 125 1451 82
+ (PROVIDED BY BNL). 125 1451 83
+ 125 1451 84
+ MF=4 125 1451 85
+ 125 1451 86
+ MT= 2, NEUTRON ELASTIC SCATTERING ANGULAR DISTRIBUTIONS IN 125 1451 87
+ THE CENTER OF MASS SYSTEM--GIVEN AS NORMALIZED 125 1451 88
+ POINTWISE PROBABILITIES. 125 1451 89
+ 125 1451 90
+ 125 1451 91
+ MF=7 125 1451 92
+ 125 1451 93
+ MT= 4, .00001 TO 5 EV FREE GAS SIGMA=20.449 BARNS. 125 1451 94
+ 125 1451 95
+ MF=12 125 1451 96
+ 125 1451 97
+ MT=102, GAMMA RAY MULTIPLICITIES --- MULTIPLICITY, (REFERRED 125 1451 98
+ TO MT=102, MF=3), IS UNITY AT ALL NEUTRON ENERGIES. 125 1451 99
+ LP=2 NOW IMPLEMENTED, THEREFORE ALL GAMMA ENERGIES 125 1451 100
+ MUST BE CALCULATED. 125 1451 101
+ 125 1451 102
+ MF=14 125 1451 103
+ 125 1451 104
+ MT=102, GAMMA RAY ANGULAR DISTRIBUTION --- ASSUMED ISOTROPIC 125 1451 105
+ AT ALL NEUTRON ENERGIES. 125 1451 106
+ 125 1451 107
+ MF=33 125 1451 108
+ 125 1451 109
+ MT=2, COVARIANCE MATRICES ADDED FOR THE ELASTIC SCATTERING BY 125 1451 110
+ D.G.FOSTER,JR. (JAN 77). 125 1451 111
+ 125 1451 112
+ 125 1451 113
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+ 2 151 4 0 125 1451 115
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diff --git a/test/periodic/db/H/1/neutron/JENDL-3.2 b/test/periodic/db/H/1/neutron/JENDL-3.2
new file mode 100644
index 0000000000000000000000000000000000000000..f50169bd1804ab156e0dddbaf89cec6b09bfebfa
--- /dev/null
+++ b/test/periodic/db/H/1/neutron/JENDL-3.2
@@ -0,0 +1,288 @@
+H/1 1
+ 1.00100+ 3 9.99167- 1 0 0 0 2 125 1451 1
+ 0.00000+ 0 0.00000+ 0 0 0 0 6 125 1451 2
+ 1.00000+ 0 0.00000+ 0 0 0 10 3 125 1451 3
+ 0.00000+ 0 0.00000+ 0 0 0 68 9 125 1451 4
+ 1-H - 1 JAERI EVAL-DEC84 K.SHIBATA 125 1451 5
+JAERI-1261 DIST-SEP89 REV2-APR93 125 1451 6
+----JENDL-3.2 MATERIAL 125 125 1451 7
+-----INCIDENT NEUTRON DATA 125 1451 8
+------ENDF-6 FORMAT 125 1451 9
+HISTORY 125 1451 10
+83-03 COMPILED BY K.SHIBATA FOR JENDL-2 125 1451 11
+ MAIN PART WAS CARRIED OVER FROM JENDL-1 DATA EVALUATED BY 125 1451 12
+ M.YAMAMOTO. DETAILS ARE GIVEN IN REF. /1/. 125 1451 13
+83-11 MF=2 WAS ADDED. THE TRANSFORMATION MATRIX GIVEN FOR MT=2 OF 125 1451 14
+ MF=4. 125 1451 15
+84-12 RE-EVALUATED BY K.SHIBATA (JAERI) FOR JENDL-3 125 1451 16
+ ELASTIC SCATTERING CROSS SECTION WAS RE-CALCULATED BELOW 125 1451 17
+ 100 KEV. 125 1451 18
+ MU-BAR WAS ALSO RE-CALCULATED. 125 1451 19
+ PHOTON-PRODUCTION CROSS SECTION WAS ADDED. 125 1451 20
+93-04 JENDL-3.2 COMPILED BY T.NAKAGAWA (NDC/JAERI) 125 1451 21
+ 125 1451 22
+ ***** MODIFIED PARTS FOR JENDL-3.2 ******************** 125 1451 23
+ (4,2) TRANSFORMATION MATRIX 125 1451 24
+ *********************************************************** 125 1451 25
+ 125 1451 26
+MF=1 GENERAL INFORMATION 125 1451 27
+ MT=451 DESCRIPTIVE DATA AND DICTIONARY 125 1451 28
+ 125 1451 29
+MF=2 RESONANCE PARAMETERS 125 1451 30
+ MT=151 SCATTERING RADIUS ONLY 125 1451 31
+ 125 1451 32
+ 125 1451 33
+MF=3 NEUTRON CROSS SECTIONS 125 1451 34
+ CALCULATED 2200M/S CROSS SECTIONS AND RES. INTEGRALS 125 1451 35
+ 2200M/S (B) RES. INTEG. (B) 125 1451 36
+ TOTAL 20.806 - 125 1451 37
+ ELASTIC 20.474 - 125 1451 38
+ CAPTURE 0.332 0.1491 125 1451 39
+ 125 1451 40
+ MT=1 TOTAL CROSS SECTION 125 1451 41
+ SUM OF ELASTIC AND CAPTURE CROSS SECTIONS 125 1451 42
+ MT=2 ELASTIC SCATTERING CROSS SECTION 125 1451 43
+ BELOW 100 KEV, CALCULATED BY USING EFFECTIVE RANGE AND 125 1451 44
+ SCATTERING LENGTH PARAMETERS OF POENITZ AND WHALEN /2/. 125 1451 45
+ ABOVE 100 KEV, THE DATA OF HOPKINS AND BREIT/3/ WERE 125 1451 46
+ RECOMMENDED. 125 1451 47
+ MT=102 CAPTURE CROSS SECTION 125 1451 48
+ THE DATA OF HORSLEY/4/ WERE RECOMMENDED. 125 1451 49
+ MT=251 MU-BAR 125 1451 50
+ CALCULATED FROM THE DATA IN MF=4. 125 1451 51
+ 125 1451 52
+MF=4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS 125 1451 53
+ MT=2 125 1451 54
+ BELOW 100 KEV, ISOTROPIC IN THE CENTER OF MASS SYSTEM WAS 125 1451 55
+ ASSUMED. ABOVE 100 KEV, THE DATA OF HOPKINS AND BREIT/3/ 125 1451 56
+ WERE RECOMMENDED. 125 1451 57
+ 125 1451 58
+MF=12 PHOTON PRODUCTION MULTIPLICITY 125 1451 59
+ MT=102 125 1451 60
+ M=1.0 125 1451 61
+ 125 1451 62
+MF=14 PHOTON ANGULAR DISTRIBUTION 125 1451 63
+ MT=102 125 1451 64
+ ASSUMED TO BE ISOTROPIC. 125 1451 65
+ 125 1451 66
+REFERENCES 125 1451 67
+ 1) IGARASI S. ET AL.: JAERI-1261 (1979). 125 1451 68
+ 2) POENITZ W.P. AND WHALEN J.F.: NUCL. PHYS. A383 (1982) 224. 125 1451 69
+ 3) HOPKINS J.C. AND BREIT G.: NUCL. DATA TABLE A9(1971) 137. 125 1451 70
+ 4) HORSLEY A.: NUCL. DATA A2(1966) 243. 125 1451 71
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+ 1.80000+ 7 2.72600- 5 1.85000+ 7 2.67300- 5 1.90000+ 7 2.62000- 5 125 3102 206
+ 1.95000+ 7 2.61200- 5 2.00000+ 7 2.60400- 5 125 3102 207
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+ 8.00000+ 5 6.73011- 1 1.00000+ 6 6.72811- 1 2.00000+ 6 6.71939- 1 125 3251 214
+ 3.00000+ 6 6.71187- 1 4.00000+ 6 6.70457- 1 5.00000+ 6 6.69753- 1 125 3251 215
+ 6.00000+ 6 6.69109- 1 7.00000+ 6 6.68524- 1 8.00000+ 6 6.67985- 1 125 3251 216
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+-1.85452- 2 1.57581- 3-6.08650- 4 9.45600- 5 125 4 2 264
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+-2.16084- 2 3.13860- 3-9.55650- 4 2.70040- 4 125 4 2 266
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+-2.39513- 2 5.16000- 3-1.32492- 3 4.34440- 4 125 4 2 268
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+-2.57875- 2 7.64770- 3-1.73304- 3 6.97400- 4 125 4 2 270
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+-2.70616- 2 1.06132- 2-2.15365- 3 1.04400- 3 125 4 2 272
+ 0.00000+ 0 2.00000+ 7 0 0 4 0 125 4 2 273
+-2.78445- 2 1.40594- 2-2.54816- 3 1.46371- 3 125 4 2 274
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+ 12514 0 284
+ 125 0 0 285
+ 0 0 0 286
+ -1 0 0
diff --git a/test/periodic/db/Pb/208/neutron/JENDL-3.2 b/test/periodic/db/Pb/208/neutron/JENDL-3.2
new file mode 100644
index 0000000000000000000000000000000000000000..18c1ec5948fa7f1c1258efc5baf568f34722afa1
--- /dev/null
+++ b/test/periodic/db/Pb/208/neutron/JENDL-3.2
@@ -0,0 +1,5474 @@
+Pb/208 1
+ 8.22080+ 4 2.06190+ 2 1 0 0 28237 1451 1
+ 0.00000+ 0 0.00000+ 0 0 0 0 68237 1451 2
+ 1.00000+ 0 0.00000+ 0 0 0 10 38237 1451 3
+ 0.00000+ 0 0.00000+ 0 0 0 225 1418237 1451 4
+ 82-PB-208 JAERI EVAL-JUL87 M.MIZUMOTO 8237 1451 5
+ DIST-SEP89 REV2-JUN94 8237 1451 6
+----JENDL-3.2 MATERIAL 8237 8237 1451 7
+-----INCIDENT NEUTRON DATA 8237 1451 8
+------ENDF-6 FORMAT 8237 1451 9
+HISTORY 8237 1451 10
+87-03 NEWLY EVALUATED FOR JENDL-3 BY M.MIZUMOTO (JAERI) 8237 1451 11
+87-11 REVISION IS RECOMMENDED. 8237 1451 12
+89-09 REVISION IS COMPLETED. 8237 1451 13
+ COMPILATION IS MADE BY T.NARITA AND T.FUKAHORI (JAERI) 8237 1451 14
+94-06 JENDL-3.2. 8237 1451 15
+ RESONANCE PARAMETERS CORRECTED BY T.NAKAGAWA 8237 1451 16
+ DATA FOR MF=3,4,5 WERE ADOPTED FROM JENDL FUSION FILE 8237 1451 17
+ GAMMA-RAY PRODUCTION DATA MODIFIED BY K.SHIBATA(JAERI) 8237 1451 18
+ COMPILED BY T.NAKAGAWA (NDC/JAERI) 8237 1451 19
+ 8237 1451 20
+ ***** MODIFIED PARTS FOR JENDL-3.2 ******************** 8237 1451 21
+ (3,4), (3,16). (3,17), (3,22), (3,51-91) 8237 1451 22
+ (4,16-91), (5,16-91) 8237 1451 23
+ THESE DATA WERE TAKEN FROM JENDL FUSION FILE. 8237 1451 24
+ (2,151) REICH-MOORE FORMULA ADOPTED, AND UPPER BOUNDARY 8237 1451 25
+ OF RESONANCE REGION WAS CHANGED FROM 0.8 TO 1 MEV 8237 1451 26
+ (3,2) 8237 1451 27
+ (12,102), (15,102) 8237 1451 28
+ *********************************************************** 8237 1451 29
+ 8237 1451 30
+ -------------------------------------------------------------8237 1451 31
+ JENDL FUSION FILE /1/ (AS OF OCT. 1993) 8237 1451 32
+ EVALUATED BY K.KOSAKO (NEDAC) AND S.CHIBA (NDC/JAERI) 8237 1451 33
+ COMPILED BY K.KOSAKO. 8237 1451 34
+ 8237 1451 35
+ DATA WERE TAKEN FROM JENDL-3.1 EXCEPT FOR THE FOLLOWING: 8237 1451 36
+ - THE INELASTIC SCATTERING CROSS SECTIONS AND ANGULAR 8237 1451 37
+ DISTRIBUTIONS OF INELASTICALLY SCATTERED NEUTRONS (EXCEPT8237 1451 38
+ CONTINUUM INELASTIC) WERE CALCULATED WITH CASTHY2Y AND 8237 1451 39
+ DWUCKY IN SINCROS-II SYSTEM/2/ INCLUDING CONTRIBUTIONS 8237 1451 40
+ FROM DIRECT REACTIONS. 8237 1451 41
+ - THE (N,2N), (N,3N), (N,NA) AND (N,NP) REACTION CROSS 8237 1451 42
+ SECTIONS (MT=16, 17, 22, 28) WERE CALCULATED BY EGNASH2 8237 1451 43
+ IN THE SINCROS-II. THE (N,2N) CROSS SECTION WAS 8237 1451 44
+ RENORMALIZED TO EXPERIMENTAL DATA. 8237 1451 45
+ - ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS WERE REPLACED 8237 1451 46
+ WITH THOSE CALCULATED BY EGNASH2. THE DDX'S OF THE 8237 1451 47
+ CONTINUUM NEUTRONS WERE CALCULATED BY KUMABE'S SYSTEMA- 8237 1451 48
+ TICS /3/ USING F15TOB /1/. THE PRECOMPOUND/COMPOUND 8237 1451 49
+ RATIO WAS CALCULATED BY THE SINCROS-II CODE SYSTEM. 8237 1451 50
+ - OPTICAL-MODEL, LEVEL DENSITY AND OTHER PARAMETERS USED IN8237 1451 51
+ THE SINCROS-II CALCULATION ARE DESCRIBED IN REF./2/. 8237 1451 52
+ LEVEL SCHEMES WERE DETERMINED ON THE BASIS OF ENSDF/4/. 8237 1451 53
+ -------------------------------------------------------------8237 1451 54
+ 8237 1451 55
+ 8237 1451 56
+MF=1 GENERAL INFORMATION 8237 1451 57
+ MT=451 DESCRIPTIVE DATA AND DICTIONARY 8237 1451 58
+ 8237 1451 59
+MF=2 RESONANCE PARAMETERS 8237 1451 60
+ MT=151 RESOLVED RESONANCE PARAMETERS FOR REICH-MOORE FORMULA 8237 1451 61
+ RESONANCE RANGES: 1.0E-5 EV TO 1.0 MEV 8237 1451 62
+ PARAMETERS WERE ADOPTED FROM HOREN+86 /5/ AND MUGHABGHAB/6/. 8237 1451 63
+ AVERAGE RADIATIVE WIDTH OF 0.18 EV WAS USED FOR THE RESONANCES 8237 1451 64
+ WHOSE VALUE WAS UNKNOWN. EFFECTIVE SCATTERING RADIUS OF 9.69 8237 1451 65
+ FM/5/ WAS ADOPTED. BACKGROUND CROSS SECTIONS WERE GIVEN TO 8237 1451 66
+ REPRODUCE THE LOW ENERGY TOTAL CROSS SECTION MEASURED AT KYOTO 8237 1451 67
+ UNIVERSITY/7/ AND THE TOTAL CROSS SECTION MEASURED BY HOREN ET 8237 1451 68
+ AL./5/ IN THE 100-460 KEV REGION. 8237 1451 69
+ 8237 1451 70
+ CALCULATED 2200-M/S CROSS SECTIONS AND RES. INTEGRALS. 8237 1451 71
+ 2200 M/S RES. INTEG. 8237 1451 72
+ ELASTIC 11.471 B - 8237 1451 73
+ CAPTURE 0.5007 MB 6.755 MB 8237 1451 74
+ TOTAL 11.472 B 8237 1451 75
+ 8237 1451 76
+MF=3 NEUTRON CROSS SECTIONS 8237 1451 77
+ BELOW 1 MEV 8237 1451 78
+ BCKGROUND CROSS SECTIONS ARE GIVEN TO THE TOTAL AND ELASTIC 8237 1451 79
+ SCATTERING CROSS SECTIONS. 8237 1451 80
+ 8237 1451 81
+ ABOVE 1 MEV 8237 1451 82
+ CROSS SECTIONS OF JENDL-3.1 WERE OBTAINED WITH AN OPTICAL AND 8237 1451 83
+ STATISTICAL MODEL CALCULATION CODE CASTHY /8/. THE OPTICAL 8237 1451 84
+ POTENTIAL PARAMETERS WERE OBTAINED BY FITTING AVERAGE TOTAL 8237 1451 85
+ CROSS SECTION OF NATURAL LEAD AS FOLLOWS, 8237 1451 86
+ V=47.0 - 0.250*E, WS = 2.30 + 0.41*E, VSO = 6.0 (MEV) 8237 1451 87
+ R0 = 1.25 , RS = 1.30 , RSO = 1.30 (FM) 8237 1451 88
+ A0 = 0.65 , B=0.48 , AS0 = 0.689 (FM) 8237 1451 89
+ LEVEL DENSITY PARAMETERS WERE DETERMINED USING LOW-LYING LEVEL 8237 1451 90
+ DATA AND OBSERVED NEUTRON RESONANCE SPACING. 8237 1451 91
+ 8237 1451 92
+ FOR JENDL-3.2, THE (N,2N), (N,3N), (N,NA) AND INELASTIC 8237 1451 93
+ SCATTERING CROSS SECTIONS WERE ADOPTED FROM JENDL FUSION FILE. 8237 1451 94
+ THEY WERE CALCULATED WITH SINCROS-II SYSTEM/2/ BY ADOPTING 8237 1451 95
+ WALTER-GUSS OMP MODIFIED BY YAMAMURO/2/ FOR NEUTRON, PEREY OMP 8237 1451 96
+ /9/ FOR PROTON, LEMOS OMP MODIFIED BY ARTHUR AND YOUNG/10/ 8237 1451 97
+ FOR ALPHA, LOHR-HAEBERLI OMP/11/ FOR DEUTERON, BECCHETTII- 8237 1451 98
+ GREENLEES OMP/12/ FOR TRITON AND HE-3, AND STANDARD LEVEL 8237 1451 99
+ DENSITY PARAMETERS OF SINCROS-II SYSTEM. 8237 1451 100
+ 8237 1451 101
+ MT=1 TOTAL 8237 1451 102
+ CALCULATED WITH CASTHY /8/. 8237 1451 103
+ 8237 1451 104
+ MT=2 ELASTIC SCATTERING 8237 1451 105
+ (TOTAL)-(ALL OTHER PARTIAL CROSS SECTIONS) 8237 1451 106
+ 8237 1451 107
+ MT=4,51-73,91 INELASTIC SCATTERING 8237 1451 108
+ THE CROSS SECTIONS WERE TAKEN FROM JENDL FUSION FILE. THE LEVEL8237 1451 109
+ SCHEME WAS ADOPTTED FROM REF./4/ CONTRIBUTIONS OF THE DIRECT 8237 1451 110
+ PROCESS WERE CALCULATED FOR THE LEVELS MARKED WITH '*'. 8237 1451 111
+ 8237 1451 112
+ NO. ENERGY(MEV) SPIN-PARITY (DIRECT PROCESS) 8237 1451 113
+ G.S. 0.0 0 + 8237 1451 114
+ 1 2.6146 3 - * 8237 1451 115
+ 2 3.1977 5 - * 8237 1451 116
+ 3 3.4751 4 - 8237 1451 117
+ 4 3.7087 5 - * 8237 1451 118
+ 5 3.9198 6 - 8237 1451 119
+ 6 3.9464 4 - 8237 1451 120
+ 7 3.9610 5 - 8237 1451 121
+ 8 3.9957 5 - 8237 1451 122
+ 9 4.0370 7 - 8237 1451 123
+ 10 4.0450 5 - 8237 1451 124
+ 11 4.0505 3 - 8237 1451 125
+ 12 4.0854 2 + * 8237 1451 126
+ 13 4.1060 3 - 8237 1451 127
+ 14 4.1253 4 - 8237 1451 128
+ 15 4.1410 2 + 8237 1451 129
+ 16 4.1590 5 - 8237 1451 130
+ 17 4.1804 5 - 8237 1451 131
+ 18 4.2054 6 - 8237 1451 132
+ 19 4.2295 2 - 8237 1451 133
+ 20 4.2300 4 - 8237 1451 134
+ 21 4.2535 3 - 8237 1451 135
+ 22 4.2624 5 - 8237 1451 136
+ 23 4.2960 5 - * 8237 1451 137
+ LEVELS ABOVE 4.296 MEV WERE ASSUMED TO BE CONTINUUM. THE DIRECT8237 1451 138
+ INELASTIC SCATTERING CROSS SECTIONS WERE CALCULATED FOR THE 8237 1451 139
+ LEVELS AT 4.3237, 4.4235, 4.698, 4.973, 5.087, 5.242, 5.345, 8237 1451 140
+ 5.483, 5.514, 5.542, 5.689, 5.813, 5.993, 6.688 AND 7.019 MEV, 8237 1451 141
+ AND ADDED TO MT=91. 8237 1451 142
+ 8237 1451 143
+ MT=16, 17, 22 (N,2N), (N,3N), (N,NA) 8237 1451 144
+ ADOPTED FROM JENDL FUSION FILE. THEORETICAL CALCULATION WAS 8237 1451 145
+ MADE WITH SINCROS-II. THE (N,2N) CROSS SECTION WAS ADJUSTED TO 8237 1451 146
+ REPRODUCE THE MEASURED ENARGY SPECTRA/13/ (FACTOR = 1.2). THE 8237 1451 147
+ DATA OF SIMAKOV ET AL. /14/ WERE ALSO TAKEN INTO CONSIDERATION. 8237 1451 148
+ 8237 1451 149
+ MT=28 (N,N'P) 8237 1451 150
+ CALCULATED WITH GNASH /15/ AND NORMALIZED TO 26 MB AT 20 MEV 8237 1451 151
+ BY WELCH+81 /16/. 8237 1451 152
+ 8237 1451 153
+ MT=102 CAPTURE 8237 1451 154
+ ESTIMATED FROM THE EXPERIMENTAL DATA BY CSIKAI+67 /17/, DRAKE+718237 1451 155
+ /18/, BERGQVIST+72 /19/, DIVEN+60 /20/ AND LEIPUNSKIJ+58 /21/. 8237 1451 156
+ 8237 1451 157
+ MT=103 (N,P) 8237 1451 158
+ CALCULATED WITH GNASH /15/ AND NORMALIZED TO 4 MB AT 18 MEV BY 8237 1451 159
+ BASS+68 /22/. 8237 1451 160
+ 8237 1451 161
+ MT=107 (N,ALPHA) 8237 1451 162
+ CALCULATED WITH GNASH /15/ AND NORMALIZED TO 1.6 MB AT 14.5 BY 8237 1451 163
+ COLEMAN+59 /23/. 8237 1451 164
+ 8237 1451 165
+ MT=251 MU-BAR 8237 1451 166
+ CALCULATED WITH CASTHY /8/. 8237 1451 167
+ 8237 1451 168
+MF=4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS 8237 1451 169
+ MT=2 8237 1451 170
+ CALCULATED WITH CASTHY /8/. 8237 1451 171
+ MT=51-73 8237 1451 172
+ TAKEN FROM JENDL FUSION FILE. CALCULATED WITH THE CASTHY AND 8237 1451 173
+ DWUCKY IN THE SINCROS-II SYSTEM. 8237 1451 174
+ MT=16, 17, 22, 28, 91 8237 1451 175
+ TAKEN FROM JENDL FUSION FILE. 8237 1451 176
+ 8237 1451 177
+MF=5 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS 8237 1451 178
+ MT=16, 17, 22, 28, 91 8237 1451 179
+ TAKEN FROM JENDL FUSION FILE. 8237 1451 180
+ 8237 1451 181
+MF=12 GAMMA-RAY MULTIPLICITY PRODUCED BY NEUTRON REACTIONS 8237 1451 182
+ MT=16,17,22,28,91,103,107 8237 1451 183
+ CALCULATED WITH GNASH /15/. 8237 1451 184
+ MT=51-73 8237 1451 185
+ TRANSITION PROBABILITIES ARE GIVEN. 8237 1451 186
+ M=102 8237 1451 187
+ FROM ENERGY BALANCE. 8237 1451 188
+ 8237 1451 189
+MF=14 ANGULAR DISTRIBUTIONS OF SECONDARY GAMMA-RAYS 8237 1451 190
+ MT=16,17,22,28,51-73,91,102,103,107 : ASSUMED ISOTROPIC. 8237 1451 191
+ 8237 1451 192
+MF=15 ENERGY DISTRIBUTION OF SECONDARY GAMMA-RAYS 8237 1451 193
+ MT=16,17,22,28,91,107 8237 1451 194
+ CALCULATED WITH THE GNASH /15/. 8237 1451 195
+ M=102 8237 1451 196
+ CALCULATED WITH CASTHY /8/. 8237 1451 197
+ 8237 1451 198
+ 8237 1451 199
+REFERENCES 8237 1451 200
+ 1) CHIBA, S. ET AL.: JAERI-M 92-027, P.35 (1992). 8237 1451 201
+ 2) YAMAMURO, N.: JAERI-M 90-006 (1990). 8237 1451 202
+ 3) KUMABE, I. ET AL.: NUCL. SCI. ENG., 104, 280 (1990). 8237 1451 203
+ 4) ENSDF: EVALUATED NUCLEAR STRUCTURE DATA FILE, BNL/NNDC. 8237 1451 204
+ 5) HOREN D. J. ET AL. : PHYS. REV. C34, 420 (1986). 8237 1451 205
+ 6) MUGHABGHAB S.F.: NEUTRON CROSS SECTIONS, VOL.1, PART B, 8237 1451 206
+ ACADEMIC PRESS (1984). 8237 1451 207
+ 7) SHCHERBAKOV O. ET AL.: 1993 FALL MEETING OF THE ATOMIC ENERGY 8237 1451 208
+ SCI. JAPAN, P.139 (1993). 8237 1451 209
+ 8) IGARASI S. AND FUKAHORI T.: JAERI 1321 (1991). 8237 1451 210
+ 9) PEREY F.G.: PHYS. REV., 131, 745 (1963). 8237 1451 211
+10) ARTHUR, E.D. AND YOUNG, P.G.: LA-8626-MS (1980). 8237 1451 212
+11) LOHR J.M. AND HAEBERLI W.: NUCL. PHYS., A232, 381 (1974). 8237 1451 213
+12) BECCHETTI F.D. JR. AND GREENLEES G.W.: "POLARIZATION 8237 1451 214
+ PHENOMENA IN NUCL. REACTIONS," UNIV. WISCONSIN PRESS, P.682 8237 1451 215
+ (1971). 8237 1451 216
+13) TAKAHASHI A. ET AL.: JAERI-M 86-080, 393 (1986). 8237 1451 217
+14) SIMAKOV S.P. ET AL: WORKSHOP ON NUCL. DATA FOR FUSION REACTOR 8237 1451 218
+ TECHNOL., DEL MAR, MAR 3-6 (1993). 8237 1451 219
+15) YOUNG P.G. AND ARTHUR E.D. : LA-6974 (1977). 8237 1451 220
+16) WELCH P. ET AL. : BAP, 26, 708 (1981). 8237 1451 221
+17) CSIKAI J. ET AL.: NUCL. PHYS. A95, 229 (1967). 8237 1451 222
+18) DRAKE D. ET AL.: PHYS. LETTERS B36, 557 (1971). 8237 1451 223
+19) BERGQVIST I. ET AL.: NUCL. PHYS. A191, 641 (1972). 8237 1451 224
+20) DIVEN B.C. ET AL. PHYS. REV. 120, 556 (1960). 8237 1451 225
+21) LEIPUNSKIJ A.I. ET AL.: 58 GENEVA, 15, 50 (1958). 8237 1451 226
+22) BASS ET AL. : EANDC(E)-89,58 (1968). 8237 1451 227
+23) COLEMAN R.F. ET AL. :PROC. ROY. SOC. (LONDON) 73 215 (1959). 8237 1451 228
+ 8237 1451 229
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diff --git a/test/periodic/db/Pb/natural/neutron/JEF-2.2 b/test/periodic/db/Pb/natural/neutron/JEF-2.2
new file mode 100644
index 0000000000000000000000000000000000000000..8c90910fc5791f4f15adf9bf5598d5c4ca8ba06e
--- /dev/null
+++ b/test/periodic/db/Pb/natural/neutron/JEF-2.2
@@ -0,0 +1,6641 @@
+Pb/0 1
+ 8.200000+4 2.054300+2 0 0 2 08200 1451 1
+ 0.000000+0 0.000000+0 0 0 0 68200 1451 2
+ 1.000000+0 0.000000+0 0 0 10 228200 1451 3
+ 0.000000+0 0.000000+0 0 0 200 908200 1451 4
+ 82-PB- 0 ECN EVAL-JUN86 H.GRUPPELAAR ET AL. 8200 1451 5
+ DIST-JAN92 920101 8200 1451 6
+----JEF-2 MATERIAL 8200 8200 1451 7
+-----INCIDENT NEUTRON DATA 8200 1451 8
+------ENDF-6 FORMAT 8200 1451 9
+******************************************************************8200 1451 10
+* JEF-2 *8200 1451 11
+* DATA TAKEN FROM EFF-1 (ENDF/B-IV REVISED BY ECN) *8200 1451 12
+******************************************************************8200 1451 13
+* * 8200 1451 14
+* *** NEUTRON DISAPPEARANCE XSECT. (MT101) ADDED AT ECN * 8200 1451 15
+* *** NO GAS PRODUCTION CROSS SECTIONS ON THIS FILE * 8200 1451 16
+* * 8200 1451 17
+***************************************************************** 8200 1451 18
+* REVISED EFF-1 EVALUATION WITH FILE 6 IN ENDF-6 FORMAT *8200 1451 19
+* -----SEE ENDFB-4 EVALUATION REPORT IN REF.(1) AND *8200 1451 20
+* -----EFF-1 REVISION REPORT IN REF.(2). *8200 1451 21
+* -----THE FORMAT OF EFF-1 IS ENDF-V SUPPLEMENTED WITH MF6 OF *8200 1451 22
+* -----ENDFB-6 FOR CONTINUUM REACTIONS, INCLUDING THE NEW DATA *8200 1451 23
+* -----TYPE MT=10 (CONTINUUM PARTICLE EMISSION ). *8200 1451 24
+* -----PROCESSING OF THE FILE6 DATA IS POSSIBLE WITH THE NEW *8200 1451 25
+* -----GROUPXS CODE, SEE REF.(7). *8200 1451 26
+* *8200 1451 27
+******************************************************************8200 1451 28
+* *8200 1451 29
+* DATA WERE TAKEN FROM ENDFB-4 AND REVISED BY H. GRUPPELAAR *8200 1451 30
+* ET AL., ECN, PETTEN FOR THE FOLLOWING REACTIONS: *8200 1451 31
+* MT= 4 TOTAL INELASTIC SCATTERING *8200 1451 32
+* THE CONTINUUM PART (MT=91) OF THE CROSS SECTION HAS *8200 1451 33
+* BEEN REVISED, SEE BELOW. *8200 1451 34
+* MT=10 CONTINUUM PARTICLE EMISSION *8200 1451 35
+* NEW QUANTITY ADDED TO FILES MF=3 AND 6 *8200 1451 36
+* FILE MF6 CONTAINS NEUTRON YIELDS AND ANGLE-ENERGY *8200 1451 37
+* DISTRIBUTIONS IN THE NEW FORMAT OF ENDF-VI. *8200 1451 38
+* THE RESULTS ARE IN REASONABLY GOOD AGREEMENT WITH *8200 1451 39
+* RECENT EXPERIMENTAL DATA AT 14-15 MEV, REFS.3-5 *8200 1451 40
+* AND OLDER DATA AT 7.5, 10 AND 12 MEV (REF.8). *8200 1451 41
+* MT=16 (N,2N) *8200 1451 42
+* COMPLETE REVISION OF FILE 3, ADDITION OF FILE 6. *8200 1451 43
+* REVISED ACCORDING TO NEW DATA AND MODEL CALCULATIONS *8200 1451 44
+* SEE REF.(2,6). *8200 1451 45
+* MT=17 (N,3N) *8200 1451 46
+* COMPLETE REVISION OF FILE 3, ADDITION OF FILE 6. *8200 1451 47
+* REVISED ACCORDING TO MODEL CALCULATIONS (REF.6). *8200 1451 48
+* MT=91 CONTINUUM INELASTIC SCATTERING *8200 1451 49
+* COMPLETE REVISION OF FILE 3, ADDITION OF FILE 6. *8200 1451 50
+* REVISED ACCORDING TO NEW MODEL CALCULATIONS (REF.6) *8200 1451 51
+* *8200 1451 52
+* *8200 1451 53
+* REFERENCES: *8200 1451 54
+* (1) C.Y.FU AND F.G.PEREY, AN EVALUATION OF NEUTRON AND *8200 1451 55
+* GAMMA-RAY-PRODUCTION CROSS SECTION DATA FOR LEAD, *8200 1451 56
+* AT.DATA AND NUCL.DATA TABLES 16 (1975),P.409 AND *8200 1451 57
+* ORNL-4765. *8200 1451 58
+* (2) H.GRUPPELAAR, H.A.J. VAN DER KAMP AND D. NIEROP, *8200 1451 59
+* REVISED CONTINUUM NEUTRON EMISSION CROSS SECTIONS FOR *8200 1451 60
+* LEAD IN THE NEW FILE6 FORMAT OF ENDFB-6, EFF-DOC-14 *8200 1451 61
+* AND TO BE PUBLISHED (1985). *8200 1451 62
+* (3) J. FREHAUT ET AL.,SYMP. NEUTRON CROSS SECTIONS FROM 10 *8200 1451 63
+* TO 50 MEV, BNL, 1980, BNL-NCS-51245,VOL.1 (1980),P.399.*8200 1451 64
+* (4) A.TAKAHASHI ET AL., A-83-01 (1982) OSAKA UNIVERSITY. *8200 1451 65
+* (5) S. IWASAKI ET AL.,INT.CONF.ON NUCLEAR DATA FOR BASIC *8200 1451 66
+* AND APPLIED SCIENCE, SANTA FE,NM, MAY 1985. *8200 1451 67
+* (6) H.GRUPPELAAR AND J.M.AKKERMANS, THE GRAPE CODE SYSTEM *8200 1451 68
+* FOR THE CALCULATION OF PRECOMPOUND AND COMPOUND NUCLEAR*8200 1451 69
+* REACTIONS - GRYPHON CODE DESCRIPTION AND MANUAL - , *8200 1451 70
+* ECN-164 (1985) NETHERLANDS ENERGY RESEARCH FOUNDATION. *8200 1451 71
+* (7) H.GRUPPELAAR, D.NIEROP AND J.M.AKKERMANS, PROCESSING *8200 1451 72
+* OF DOUBLE DIFFERENTIAL CROSS SECTIONS IN THE NEW *8200 1451 73
+* ENDF-VI FORMAT - GROUPXS CODE DESCRIPTION AND USERS' *8200 1451 74
+* MANUAL, EFF-DOC-13 AND TO BE PUBLISHED. *8200 1451 75
+ (8) A.BEYERLE ET AL.,PROC.INT.CONF.ON NUCLEAR CROSS SECTIONS8200 1451 76
+ FOR TECHNOLOGY, KNOXVILLE 1979, NBS-SP594,P.139. 8200 1451 77
+******************************************************************8200 1451 78
+ * * * * * * *8200 1451 79
+UPDATED REVIEW OF FILE CONTENTS: 8200 1451 80
+FILE 1 GENERAL INFORMATION (REVISED FOR EFF-1) 8200 1451 81
+ SECTION 451 DISCRIPTIVE DATA AND DICTIONARY 8200 1451 82
+FILE 2 RESONANCE PARAMETERS (=ENDFB-4) 8200 1451 83
+ SECTION 151 GENERAL DESIGNATION FOR RESONANCE INFORMATION 8200 1451 84
+ ONLY EFFECTIVE SCATTERING LENGTH GIVEN. TAKEN FROM BNL-325. 8200 1451 85
+FILE 3 NEUTRON CROSS SECTIONS (ENDFB-4 WITH REVISIONS FOR EFF-1) 8200 1451 86
+ SECTION 1 TOTAL INTERACTION (=ENDFB-4) 8200 1451 87
+ 0.00001 EV TO 1 KEV FROM BNL-325 8200 1451 88
+ 1 KEV TO 0.47 MEV MOSTLY FROM W. M. GOOD OF ORNL. 8200 1451 89
+ 0.47 MEV TO 20.0 MEV FROM R. B. SCHWARTZ OF NBS. 8200 1451 90
+ SECTION 2 ELASTIC SCATTERING (=ENDFB-4) 8200 1451 91
+ DERIVED BY SUBTRACTING THE NON-ELASTIC CROSS SECTION FROM THE 8200 1451 92
+ TOTAL CROSS SECTION 8200 1451 93
+ SECTION 3 NON-ELASTIC INTERACTION (=ENDFB-4) 8200 1451 94
+ CALCULATED, VERY GOOD AGREEMENT WITH EXPERIMENT 8200 1451 95
+ SECTION 4 TOTAL INELASTIC SCATTERING (REVISED FOR EFF-1) 8200 1451 96
+ CALCULATED, VERY GOOD AGREEMENT WITH EXPERIMENT 8200 1451 97
+ THE CONTINUUM PART OF THE CROSS SECTION (ABOVE 4.4 MEV) HAS 8200 1451 98
+ BEEN REVISED, SEE SECTION 91. SUM OBTAINED WITH CRECTJ5. 8200 1451 99
+ SECTION 10 CONTINUUM PARTICLE EMISSION (NEW FOR EFF-1) 8200 1451 100
+ SUM OF SECTIONS 16, 17 ,91 (NO CHARGED-PARTICLE EMISSION). 8200 1451 101
+ SECTION 16 (N,2N) REACTION (RE-EVALUATED FOR EFF-1) 8200 1451 102
+ IN AGREEMENT WITH EXPERIMENTAL DATA OF FREHAUT ET AL.(REF.3) 8200 1451 103
+ FROM THRESHOLD UPTO ABOUT 10 MEV. AT ENERGIES FROM 10 TO 8200 1451 104
+ 14.5 MEV THE EVALUATED DATA ARE SOMEWHAT HIGHER (5 PER CENT) 8200 1451 105
+ IN AGREEMENT WITH RECENT OTHER DATA AT 14 TO 15 MEV (REFS.4,5)8200 1451 106
+ SECTION 17 (N,3N) REACTION (RE-EVALUATED FOR EFF-1) 8200 1451 107
+ CALCULATED, NO DATA AVAILABLE 8200 1451 108
+ SECTION 51 THROUGH 85 INELASTIC SCATTERING EXCITING LEVELS 8200 1451 109
+ (=ENDFB-4) 8200 1451 110
+ CALCULATED, COMPARED FAVORABLY WITH EXPERIMENT. 8200 1451 111
+ 48 LEVELS IN 206, 49 LEVELS IN 207 AND 22 LEVELS IN 208 ARE 8200 1451 112
+ MERGED TO FORM 35 LEVELS IN NATURAL LEAD 8200 1451 113
+ SECTION 91 CONTINUUM INELASTIC SCATTERING (RE-EVALUATED EFF-1) 8200 1451 114
+ UPTO THE (N,2N)-THRESHOLD THIS IS EQUAL TO THE NON-ELASTIC 8200 1451 115
+ CROSS SECTION MINUS THE SUM OF ALL DISCRETE LEVEL EXCITATION 8200 1451 116
+ CROSS SECTIONS. AT HIGHER ENERGIES THE COMPETION OF (N,2N) AND8200 1451 117
+ (N,3N) FURTHER DECREASES THIS CROSS SECTION. 8200 1451 118
+ SECTION 101 NEUTRON DISAPPEARANCE (ADDED FOR EFF-1) 8200 1451 119
+ IDENTICAL TO MT=102. 8200 1451 120
+ SECTION 102 RADIATIVE CAPTURE (=ENDFB-4) 8200 1451 121
+ 0.00001 EV TO 10 EV--1/V DEPENDENCE ASSUMED WITH 0.178 BARNS 8200 1451 122
+ AT 0.0253 EV. (DATA-MODIFIED JAN.1972). 8200 1451 123
+ THE CAPTURE CROSS SECTIONS FROM 1 KEV TO 1 MEV 8200 1451 124
+ HAVE BEEN COMPLETELY REEVALUATED BASED PRIMARILY 8200 1451 125
+ ON A RECENT HIGH-RESOLUTION MEASUREMENT OF CAPTURE 8200 1451 126
+ CROSS SECTIONS FOR THE LEAD ISOTOPES 204, 206, 8200 1451 127
+ 207 AND 208 BY B. J. ALLEN ET AL. OF ORNL. 8200 1451 128
+ APPROXIMATELY 75 PER CENT OF THE CAPTURE CROSS 8200 1451 129
+ SECTIONS IN THE RANGE FROM 1 KEV TO 200 KEV WERE 8200 1451 130
+ GIVEN EXPLICITLY AS RESONANCES. CORRELATION OF 8200 1451 131
+ THESE RESONANCES WITH THE TOTAL CROSS SECTIONS 8200 1451 132
+ ENABLES US TO REFINE THE RESONANCE WIDTHS AND 8200 1451 133
+ AREAS OF THE TOTAL CROSS SECTIONS AS WELL. 8200 1451 134
+ CORRESPONDING CHANGES HAVE BEEN MADE IN THE 8200 1451 135
+ ELASTIC-SCATTERING AND NON-ELASTIC CROSS SECTIONS. 8200 1451 136
+ DETAILS OF THE ABOVE MODIFICATIONS HAVE BEEN 8200 1451 137
+ DESCRIBED IN AN ADDENDUM OF THE REPORT, EVALUATION 8200 1451 138
+ OF NEUTRON AND GAMMA-RAY-PRODUCTION CROSS SECTIONS 8200 1451 139
+ FOR LEAD, ORNL-4765, C.Y. FU AND F.G. PEREY. 8200 1451 140
+ SECTION 251 MU BAR (=ENDFB-4) 8200 1451 141
+ DERIVED FROM ELASTIC ANGULAR DISTRIBUTIONS AND KINEMATICS 8200 1451 142
+ USING THE COMPUTER PROGRAM SAD. 8200 1451 143
+ SECTION 252 XI (=ENDFB-4) 8200 1451 144
+ SEE SECTION 251. 8200 1451 145
+ SECTION 253 GAMMA (=ENDFB-4) 8200 1451 146
+ SEE SECTION 251. 8200 1451 147
+FILE 4 ANGULAR DISTRIBUTION OF SECONDARY NEUTRONS (=ENDFB-4, 8200 1451 148
+ SECTIONS MT=16,17,91 HAVE BEEN DELETED, SEE FILE 6) 8200 1451 149
+ ALL DISTRIBUTIONS ARE GIVEN IN THE LEGENDRE POLYNOMIAL 8200 1451 150
+ REPRESENTATIONS. 8200 1451 151
+ SECTION 2 ELASTIC SCATTERING (=ENDFB-4) 8200 1451 152
+ 0.00001 EV TO 5 MEV--COEFFICIENTS OBTAINED BY FITTING DATA 8200 1451 153
+ 5 MEV TO 20 MEV--OPTICAL MODEL CALCULATION. OPTICAL MODEL 8200 1451 154
+ PARAMETERS BEST FIT DATA AT 7 AND 14 MEV. 8200 1451 155
+ REPRESENTATION IS IN CENTER OF MASS SYSTEM. 8200 1451 156
+ TRANSFORMATION MATRIX IS GIVEN 8200 1451 157
+ SECTION 51 THROUGH 85 INELASTIC SCATTERING EXCITING LEVELS 8200 1451 158
+ (=ENDFB-4) 8200 1451 159
+ CALCULATED AND COMPARED FAVORABLY WITH DATA. 8200 1451 160
+ REPRESENTATION IS IN CENTER OF MASS SYSTEM. 8200 1451 161
+FILE 6 COUPLED ENERGY-ANGLE DISTRIBUTIONS (NEW FOR EFF-1) 8200 1451 162
+ ALL DISTRIBUTIONS ARE GIVEN IN THE LEGENDRE POLYNOMIAL 8200 1451 163
+ REPRESENTATION FOR THE CENTER-OF-MASS SYSTEM . 8200 1451 164
+ THE MAXIMUM ORDER EQUALS 4 (5 COEFFICIENTS). 8200 1451 165
+ THE FILE ALSO CONTAINS NEUTRON MULTIPLICITIES OR YIELDS. 8200 1451 166
+ ONLY NEUTRON DISTRIBUTIONS ARE GIVEN. 8200 1451 167
+ SECTION 10 CONTINUUM PARTICLE EMISSION (NEW FOR EFF-1) 8200 1451 168
+ SINCE CHARGED-PARTICLE EMISSION IS NOT CONSIDERED THIS 8200 1451 169
+ DATA TYPE CORRESPONDS TO CONTINUUM NEUTRON EMISSION. 8200 1451 170
+ DATA FILE OBTAINED BY SUMMATION OF SECTIONS 16,17,91 WITH 8200 1451 171
+ COMPUTER CODE NELIS BY H.GRUPPELAAR. 8200 1451 172
+ AGREEMENT WITH EXPERIMENTAL DISTRIBUTIONS AT 7.5, 10, 12 MEV 8200 1451 173
+ (REF.8) AND AT 14-15 MEV (REF.4). 8200 1451 174
+ SECTION 16 (N,2N) (NEW FOR EFF-1) 8200 1451 175
+ CALCULATED WITH COMPUTER CODE SYSTEM GRAPE (REF.6) USING 8200 1451 176
+ NUCLEAR-MODEL CODE GRYPHON AND SORTING CODE SPSORT. 8200 1451 177
+ SECTION 17 (N,3N) (NEW FOR EFF-1) 8200 1451 178
+ CALCULATED WITH COMPUTER CODE SYSTEM GRAPE (REF.6) USING 8200 1451 179
+ NUCLEAR-MODEL CODE GRYPHON AND SORTING CODE SPSORT. 8200 1451 180
+ SECTION 91 CONTINUUM INELASTIC SCATTERING (NEW FOR EFF-1) 8200 1451 181
+ CALCULATED WITH COMPUTER CODE SYSTEM GRAPE (REF.6) USING 8200 1451 182
+ NUCLEAR-MODEL CODE GRYPHON AND SORTING CODE SPSORT. 8200 1451 183
+FILE 12 MULTIPLICITIES OF GAMMA RAYS PRODUCED BY NEUTRON REACTION 8200 1451 184
+ (=ENDFB-4) 8200 1451 185
+ SECTION 3 NON-ELASTIC SCATTERING 8200 1451 186
+ COMBINED FROM CONTRIBUTIONS FROM RADIATIVE CAPTURE, INELASTIC 8200 1451 187
+ SCATTERING, N,2N), AND N,3N) REACTIONS. 8200 1451 188
+FILE 14 ANGULAR DISTRIBUTIONS OF SECONDARY GAMMA RAYS 8200 1451 189
+ (=ENDFB-4) 8200 1451 190
+ SECTION 3 NON-ELASTIC SCATTERING 8200 1451 191
+ ASSUMED ISOTROPIC. 8200 1451 192
+FILE 15 ENERGY DISTRIBUTION OF SECONDARY GAMMA RAYS 8200 1451 193
+ (=ENDFB-4) 8200 1451 194
+ SECTION 3 NON-ELASTIC SCATTERING 8200 1451 195
+ 0.00001 EV TO 10 EV--ONE SINGLE SPECTRUM RESULTING FROM 8200 1451 196
+ THERMAL NEUTRON CAPTURE IS ASSUMED VALID. 8200 1451 197
+ 1 KEV TO 573 KEV--ONE SINGLE SPECTRUM IS ASSUMED VALID WHICH 8200 1451 198
+ WAS DERIVED FROM RATHER LIMITED RESONANCE CAPTURE DATA. 8200 1451 199
+ 10 EV TO 1 KEV--LINEAR INTERPOLATION BETWEEN ABOVE TWO SPECTRA8200 1451 200
+ 573 KEV TO 20 MEV--CALCULATED SPECTRA RESULTING FROM 8200 1451 201
+ INELASTIC, N,2N) AND N,3N) REACTIONS, GIVEN FOR INTERVALS 8200 1451 202
+ VARYING FROM 0.25 TO 1.0 MEV, COMPARED FAVORABLY WITH DATA. 8200 1451 203
+ 8200 1451 204
+ 1 451 294 08200 1451 205
+ 2 151 4 08200 1451 206
+ 3 1 216 08200 1451 207
+ 3 2 209 08200 1451 208
+ 3 3 96 08200 1451 209
+ 3 4 33 08200 1451 210
+ 3 10 11 08200 1451 211
+ 3 16 9 08200 1451 212
+ 3 17 6 08200 1451 213
+ 3 51 11 08200 1451 214
+ 3 52 12 08200 1451 215
+ 3 53 11 08200 1451 216
+ 3 54 11 08200 1451 217
+ 3 55 11 08200 1451 218
+ 3 56 10 08200 1451 219
+ 3 57 10 08200 1451 220
+ 3 58 11 08200 1451 221
+ 3 59 10 08200 1451 222
+ 3 60 10 08200 1451 223
+ 3 61 10 08200 1451 224
+ 3 62 9 08200 1451 225
+ 3 63 9 08200 1451 226
+ 3 64 10 08200 1451 227
+ 3 65 10 08200 1451 228
+ 3 66 10 08200 1451 229
+ 3 67 9 08200 1451 230
+ 3 68 9 08200 1451 231
+ 3 69 8 08200 1451 232
+ 3 70 9 08200 1451 233
+ 3 71 8 08200 1451 234
+ 3 72 8 08200 1451 235
+ 3 73 8 08200 1451 236
+ 3 74 8 08200 1451 237
+ 3 75 8 08200 1451 238
+ 3 76 8 08200 1451 239
+ 3 77 8 08200 1451 240
+ 3 78 8 08200 1451 241
+ 3 79 8 08200 1451 242
+ 3 80 8 08200 1451 243
+ 3 81 8 08200 1451 244
+ 3 82 7 08200 1451 245
+ 3 83 7 08200 1451 246
+ 3 84 8 08200 1451 247
+ 3 85 8 08200 1451 248
+ 3 91 11 08200 1451 249
+ 3 101 66 08200 1451 250
+ 3 102 66 08200 1451 251
+ 4 2 76 08200 1451 252
+ 4 51 53 08200 1451 253
+ 4 52 75 08200 1451 254
+ 4 53 54 08200 1451 255
+ 4 54 57 08200 1451 256
+ 4 55 47 08200 1451 257
+ 4 56 50 08200 1451 258
+ 4 57 42 08200 1451 259
+ 4 58 66 08200 1451 260
+ 4 59 45 08200 1451 261
+ 4 60 38 08200 1451 262
+ 4 61 43 08200 1451 263
+ 4 62 37 08200 1451 264
+ 4 63 42 08200 1451 265
+ 4 64 54 08200 1451 266
+ 4 65 54 08200 1451 267
+ 4 66 54 08200 1451 268
+ 4 67 35 08200 1451 269
+ 4 68 33 08200 1451 270
+ 4 69 33 08200 1451 271
+ 4 70 48 08200 1451 272
+ 4 71 30 08200 1451 273
+ 4 72 28 08200 1451 274
+ 4 73 26 08200 1451 275
+ 4 74 26 08200 1451 276
+ 4 75 26 08200 1451 277
+ 4 76 39 08200 1451 278
+ 4 77 39 08200 1451 279
+ 4 78 24 08200 1451 280
+ 4 79 24 08200 1451 281
+ 4 80 22 08200 1451 282
+ 4 81 36 08200 1451 283
+ 4 82 22 08200 1451 284
+ 4 83 21 08200 1451 285
+ 4 84 33 08200 1451 286
+ 4 85 33 08200 1451 287
+ 6 10 1034 08200 1451 288
+ 6 16 682 08200 1451 289
+ 6 17 203 08200 1451 290
+ 6 91 929 08200 1451 291
+ 12 3 18 08200 1451 292
+ 14 3 1 08200 1451 293
+ 15 3 869 08200 1451 294
+ 8200 1 0 295
+ 8200 0 0 296
+ 8.200000+4 2.054300+2 0 0 1 08200 2151 297
+ 8.200000+4 1.000000+0 0 0 1 08200 2151 298
+ 1.000000-5 2.000000+7 0 0 0 08200 2151 299
+ 0.000000+0 9.340000-1 0 0 0 08200 2151 300
+ 8200 2 0 301
+ 8200 0 0 302
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+ 0.000000+0 0.000000+0 0 0 2 6398200 3 1 304
+ 14 5 639 2 0 08200 3 1 305
+ 1.000000-5 2.014720+1 1.000000-4 1.402530+1 3.000000-4 1.282860+18200 3 1 306
+ 7.000000-4 1.226410+1 1.000000-3 1.208930+1 1.500000-3 1.192500+18200 3 1 307
+ 2.500000-3 1.176030+1 4.000000-3 1.164170+1 2.530000-2 1.137200+18200 3 1 308
+ 4.000000-2 1.133560+1 7.000000-2 1.130100+1 1.000000+0 1.122230+18200 3 1 309
+ 1.000000+3 1.120290+1 1.680000+3 1.119970+1 1.685000+3 3.819970+18200 3 1 310
+ 1.690000+3 1.119970+1 2.000000+3 1.119960+1 2.010000+3 1.119980+18200 3 1 311
+ 2.480000+3 1.119980+1 2.485000+3 3.879980+1 2.490000+3 1.119980+18200 3 1 312
+ 3.000000+3 1.119980+1 3.010000+3 1.120000+1 3.068000+3 1.120000+18200 3 1 313
+ 3.070000+3 3.370000+1 3.072000+3 1.120000+1 3.355000+3 1.120000+18200 3 1 314
+ 3.360000+3 3.920000+1 3.365000+3 1.120000+1 4.000000+3 1.120000+18200 3 1 315
+ 4.010000+3 1.120040+1 5.000000+3 1.120040+1 5.010000+3 1.120010+18200 3 1 316
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+ 7.010000+3 1.120050+1 8.000000+3 1.120050+1 8.010000+3 1.120030+18200 3 1 318
+ 8.294000+3 1.120030+1 8.350000+3 1.745030+1 8.406000+3 1.120030+18200 3 1 319
+ 9.000000+3 1.117530+1 9.010000+3 1.117470+1 9.616000+3 1.114970+18200 3 1 320
+ 9.635000+3 1.594970+1 9.654000+3 1.114970+1 1.000000+4 1.111770+18200 3 1 321
+ 1.001000+4 1.111680+1 1.018900+4 1.109980+1 1.021000+4 1.542980+18200 3 1 322
+ 1.023100+4 1.109980+1 1.237300+4 1.099980+1 1.239000+4 1.819980+18200 3 1 323
+ 1.240700+4 1.099980+1 1.284500+4 1.089980+1 1.290000+4 1.489980+18200 3 1 324
+ 1.295500+4 1.089980+1 1.421600+4 1.079980+1 1.424000+4 1.504980+18200 3 1 325
+ 1.426400+4 1.079980+1 1.616200+4 1.069880+1 1.620000+4 1.324980+18200 3 1 326
+ 1.623800+4 1.069980+1 1.645000+4 1.064980+1 1.647000+4 2.215000+18200 3 1 327
+ 1.649000+4 1.064980+1 1.674000+4 1.059980+1 1.680000+4 3.160020+18200 3 1 328
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+ 1.983100+4 1.049980+1 2.000000+4 1.047580+1 2.001000+4 1.047410+18200 3 1 330
+ 2.189700+4 1.020010+1 2.193000+4 1.165000+1 2.196300+4 1.020010+18200 3 1 331
+ 2.541100+4 9.899740+0 2.547000+4 4.890000+1 2.552900+4 9.900040+08200 3 1 332
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+ 4.140000+4 1.870030+1 4.160000+4 1.970020+1 4.250000+4 1.650000+18200 3 1 339
+ 4.285000+4 1.587820+1 4.350000+4 1.472220+1 4.430000+4 1.330020+18200 3 1 340
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+ 5.000000+4 1.084020+1 5.001000+4 1.084000+1 5.926000+4 1.080000+18200 3 1 342
+ 5.939000+4 1.088550+1 5.952000+4 1.080000+1 6.000000+4 1.079500+18200 3 1 343
+ 6.001000+4 1.079500+1 6.402000+4 1.075000+1 6.416000+4 1.080350+18200 3 1 344
+ 6.430000+4 1.075000+1 6.608400+4 1.035000+1 6.620000+4 1.500000+18200 3 1 345
+ 6.631600+4 1.110000+1 7.000000+4 1.069400+1 7.001000+4 1.069180+18200 3 1 346
+ 7.084500+4 1.059980+1 7.100000+4 3.770020+1 7.115500+4 1.079980+18200 3 1 347
+ 7.700000+4 1.099980+1 7.800000+4 3.799980+1 7.900000+4 1.099980+18200 3 1 348
+ 8.000000+4 1.086380+1 8.001000+4 1.086190+1 8.486600+4 1.019990+18200 3 1 349
+ 8.500000+4 2.819990+1 8.513400+4 1.019990+1 8.857000+4 1.039990+18200 3 1 350
+ 8.877000+4 1.045490+1 8.897000+4 9.999990+0 8.967400+4 1.000590+18200 3 1 351
+ 8.967500+4 9.990590+0 8.967600+4 1.000000+1 9.035000+4 1.549950+18200 3 1 352
+ 9.102400+4 1.000000+1 9.188900+4 1.000000+1 9.204000+4 1.003300+18200 3 1 353
+ 9.219100+4 1.000000+1 9.275100+4 1.000000+1 9.290000+4 1.009400+18200 3 1 354
+ 9.304900+4 1.000000+1 1.000000+5 9.967630+0 1.000100+5 9.968200+08200 3 1 355
+ 1.149400+5 9.987900+0 1.149400+5 9.987900+0 1.152000+5 1.570020+18200 3 1 356
+ 1.154600+5 1.010010+1 1.154600+5 1.010010+1 1.176300+5 1.030010+18200 3 1 357
+ 1.179000+5 3.070000+1 1.181700+5 9.500000+0 1.247500+5 9.499900+08200 3 1 358
+ 1.250000+5 1.910000+1 1.252500+5 9.500000+0 1.268300+5 9.499400+08200 3 1 359
+ 1.268300+5 9.499400+0 1.268340+5 9.985460+0 1.270000+5 3.050000+18200 3 1 360
+ 1.271660+5 9.985950+0 1.271700+5 9.499900+0 1.271700+5 9.499900+08200 3 1 361
+ 1.401900+5 9.100000+0 1.401900+5 9.100000+0 1.401910+5 9.105160+08200 3 1 362
+ 1.406000+5 1.127040+1 1.410090+5 9.005400+0 1.410100+5 9.000000+08200 3 1 363
+ 1.410100+5 9.000000+0 1.464000+5 9.000000+0 1.468000+5 9.095000+08200 3 1 364
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+ 1.506300+5 1.000100+1 1.510000+5 1.699990+1 1.513700+5 9.000020+08200 3 1 366
+ 1.692000+5 8.700020+0 1.695000+5 1.575040+1 1.698000+5 8.800020+08200 3 1 367
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+ 6.000000+5 3.862400-7 7.000000+5 1.300200-7 8.000000+5 5.126600-6820015 3 6577
+ 9.000000+5 9.720800-8 1.000000+6 8.300200-8 1.100000+6 6.700500-8820015 3 6578
+ 1.200000+6 5.370600-8 1.300000+6 1.983600-7 1.400000+6 1.704900-7820015 3 6579
+ 1.500000+6 5.535900-8 1.600000+6 3.573200-8 1.700000+6 1.190200-7820015 3 6580
+ 1.800000+6 1.493300-8 1.900000+6 2.825400-9 2.000000+6 0.000000+0820015 3 6581
+ 2.100000+6 0.000000+0 2.200000+6 1.178200-8 2.300000+6 0.000000+0820015 3 6582
+ 0.000000+0 1.800000+7 0 0 1 34820015 3 6583
+ 34 1 0 0 0 0820015 3 6584
+ 0.000000+0 4.707400-7 1.000000+5 2.298400-7 2.000000+5 3.240300-7820015 3 6585
+ 3.000000+5 1.094100-6 4.000000+5 1.189300-7 5.000000+5 1.021900-6820015 3 6586
+ 6.000000+5 3.839900-7 7.000000+5 1.568700-7 8.000000+5 4.247200-6820015 3 6587
+ 9.000000+5 1.182300-7 1.000000+6 1.828700-7 1.100000+6 1.084600-7820015 3 6588
+ 1.200000+6 1.079900-7 1.300000+6 3.182000-7 1.400000+6 1.999100-7820015 3 6589
+ 1.500000+6 1.457300-7 1.600000+6 9.626000-8 1.700000+6 2.159800-7820015 3 6590
+ 1.800000+6 1.705900-7 1.900000+6 6.041500-8 2.000000+6 5.037500-8820015 3 6591
+ 2.100000+6 4.185600-8 2.200000+6 5.820300-8 2.300000+6 2.520400-8820015 3 6592
+ 2.400000+6 1.949000-8 2.500000+6 1.304600-8 2.600000+6 1.008300-8820015 3 6593
+ 2.700000+6 4.753200-9 2.800000+6 2.183600-9 2.900000+6 6.67890-10820015 3 6594
+ 3.000000+6 0.000000+0 3.100000+6 0.000000+0 3.200000+6 1.865000-9820015 3 6595
+ 3.300000+6 0.000000+0 0.000000+0 0.000000+0 0.000000+0 0.000000+0820015 3 6596
+ 0.000000+0 1.900000+7 0 0 1 48820015 3 6597
+ 48 1 0 0 0 0820015 3 6598
+ 0.000000+0 3.673000-7 1.000000+5 3.477400-7 2.000000+5 2.578300-7820015 3 6599
+ 3.000000+5 8.787300-7 4.000000+5 1.028400-7 5.000000+5 1.123600-6820015 3 6600
+ 6.000000+5 3.426600-7 7.000000+5 1.923500-7 8.000000+5 3.622400-6820015 3 6601
+ 9.000000+5 1.224000-7 1.000000+6 2.230800-7 1.100000+6 1.290200-7820015 3 6602
+ 1.200000+6 1.408200-7 1.300000+6 2.790300-7 1.400000+6 1.832100-7820015 3 6603
+ 1.500000+6 1.980100-7 1.600000+6 1.302700-7 1.700000+6 2.977700-7820015 3 6604
+ 1.800000+6 2.469700-7 1.900000+6 9.510900-8 2.000000+6 1.187800-7820015 3 6605
+ 2.100000+6 8.417900-8 2.200000+6 9.258500-8 2.300000+6 6.291500-8820015 3 6606
+ 2.400000+6 5.538000-8 2.500000+6 5.658900-8 2.600000+6 5.734500-8820015 3 6607
+ 2.700000+6 4.324900-8 2.800000+6 2.742100-8 2.900000+6 2.257300-8820015 3 6608
+ 3.000000+6 2.477100-8 3.100000+6 1.575100-8 3.200000+6 2.211500-8820015 3 6609
+ 3.300000+6 9.765900-9 3.400000+6 6.824600-9 3.500000+6 4.693700-9820015 3 6610
+ 3.600000+6 3.855200-9 3.700000+6 2.109100-9 3.800000+6 9.25800-10820015 3 6611
+ 3.900000+6 2.64950-10 4.000000+6 0.000000+0 4.100000+6 3.46290-10820015 3 6612
+ 4.200000+6 0.000000+0 4.300000+6 5.897400-9 4.400000+6 3.62590-10820015 3 6613
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+ 0.000000+0 2.000000+7 0 0 1 58820015 3 6615
+ 58 1 0 0 0 0820015 3 6616
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+ 6.000000+5 3.132700-7 7.000000+5 1.914000-7 8.000000+5 3.151300-6820015 3 6619
+ 9.000000+5 1.216500-7 1.000000+6 2.163900-7 1.100000+6 1.408200-7820015 3 6620
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+ 1.800000+6 2.559700-7 1.900000+6 1.166600-7 2.000000+6 1.552300-7820015 3 6623
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+ 3.300000+6 3.799200-8 3.400000+6 3.148400-8 3.500000+6 2.635500-8820015 3 6628
+ 3.600000+6 2.788800-8 3.700000+6 2.304600-8 3.800000+6 1.879400-8820015 3 6629
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+ 4.200000+6 7.159500-9 4.300000+6 3.472900-8 4.400000+6 6.316500-9820015 3 6631
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+ 4.800000+6 1.589700-9 4.900000+6 1.066700-9 5.000000+6 7.32850-10820015 3 6633
+ 5.100000+6 5.34240-10 5.200000+6 3.68690-10 5.300000+6 2.36290-10820015 3 6634
+ 5.400000+6 1.36320-10 5.500000+6 6.69210-11 5.600000+6 2.48110-11820015 3 6635
+ 5.700000+6 4.93150-12 0.000000+0 0.000000+0 0.000000+0 0.000000+0820015 3 6636
+ 820015 0 6637
+ 8200 0 0 6638
+ 0 0 0 6639
+ -1 0 0
diff --git a/test/periodic/db/Pb/natural/neutron/JENDL-3.2 b/test/periodic/db/Pb/natural/neutron/JENDL-3.2
new file mode 100644
index 0000000000000000000000000000000000000000..cd16c28a51833c91a059bbd4021f040ee016f249
--- /dev/null
+++ b/test/periodic/db/Pb/natural/neutron/JENDL-3.2
@@ -0,0 +1,7508 @@
+Pb/0 1
+ 8.20000+ 4 2.05435+ 2 1 0 0 28200 1451 1
+ 0.00000+ 0 0.00000+ 0 0 0 0 68200 1451 2
+ 1.00000+ 0 0.00000+ 0 0 0 10 38200 1451 3
+ 0.00000+ 0 0.00000+ 0 0 0 228 1078200 1451 4
+ 82-PB- 0 JAERI EVAL-JUL87 M.MIZUMOTO 8200 1451 5
+ DIST-SEP89 REV2-JUN94 8200 1451 6
+----JENDL-3.2 MATERIAL 8200 8200 1451 7
+-----INCIDENT NEUTRON DATA 8200 1451 8
+------ENDF-6 FORMAT 8200 1451 9
+HISTORY 8200 1451 10
+87-03 NEWLY EVALUATED FOR JENDL-3 BY M.MIZUMOTO (JAERI) 8200 1451 11
+87-11 REVISION IS RECOMMENDED. 8200 1451 12
+89-09 REVISION IS COMPLETED. 8200 1451 13
+ COMPILATION WAS MADE BY. T.NARITA AND T.FUKAHORI (JAERI) 8200 1451 14
+94-06 JENDL-3.2. 8200 1451 15
+ RESONANCE PARAMETERS CORRECTED BY T.NAKAGAWA 8200 1451 16
+ DATA FOR MF=3,4,5 WERE ADOPTED FROM JENDL FUSION FILE 8200 1451 17
+ GAMMA-RAY PRODUCTION DATA MODIFIED BY K.SHIBATA(JAERI) 8200 1451 18
+ COMPILED BY T.NAKAGAWA (NDC/JAERI) 8200 1451 19
+ 8200 1451 20
+ ***** MODIFIED PARTS FOR JENDL-3.2 ******************** 8200 1451 21
+ (3,4), (3,16). (3,17), (3,22), (3,28), (3,51-91) 8200 1451 22
+ (4,16-91), (5,16-91) 8200 1451 23
+ THESE DATA WERE TAKEN FROM JENDL FUSION FILE. 8200 1451 24
+ (2,151) REICH-MOORE FORMULA ADOPTED FOR PB-204, 206 AND 8200 1451 25
+ 208. UPPER BOUNDARIES OF RESONANCE REGIONS WERE 8200 1451 26
+ CHANGED. 8200 1451 27
+ (3,1) BELOW 1 MEV 8200 1451 28
+ (3,102) 8200 1451 29
+ (3,2) TO COMPANSATE THE ABOVE MODIFICATIONS 8200 1451 30
+ (12,102), (13,3), (13,4), (15,3), (15,102) 8200 1451 31
+ *********************************************************** 8200 1451 32
+ 8200 1451 33
+ -------------------------------------------------------------8200 1451 34
+ JENDL FUSION FILE /1/ (AS OF OCT. 1993) 8200 1451 35
+ EVALUATED BY K.KOSAKO (NEDAC) AND S.CHIBA (NDC/JAERI) 8200 1451 36
+ COMPILED BY K.KOSAKO. 8200 1451 37
+ 8200 1451 38
+ DATA WERE TAKEN FROM JENDL-3.1 EXCEPT FOR THE FOLLOWING: 8200 1451 39
+ - THE INELASTIC SCATTERING CROSS SECTIONS AND ANGULAR 8200 1451 40
+ DISTRIBUTIONS OF INELASTICALLY SCATTERED NEUTRONS (EXCEPT8200 1451 41
+ CONTINUUM INELASTIC) WERE CALCULATED WITH CASTHY2Y AND 8200 1451 42
+ DWUCKY IN SINCROS-II SYSTEM/2/ INCLUDING CONTRIBUTIONS 8200 1451 43
+ FROM DIRECT REACTIONS. 8200 1451 44
+ - THE (N,2N), (N,3N), (N,NA) AND (N,NP) REACTION CROSS 8200 1451 45
+ SECTIONS (MT=16, 17, 22, 28) WERE CALCULATED BY EGNASH2 8200 1451 46
+ IN THE SINCROS-II. THE (N,2N) CROSS SECTION WAS 8200 1451 47
+ RENORMALIZED TO EXPERIMENTAL DATA. 8200 1451 48
+ - ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS WERE REPLACED 8200 1451 49
+ WITH THOSE CALCULATED BY EGNASH2. THE DDX'S OF THE 8200 1451 50
+ CONTINUUM NEUTRONS WERE CALCULATED BY KUMABE'S SYSTEMA- 8200 1451 51
+ TICS /3/ USING F15TOB /1/. THE PRECOMPOUND/COMPOUND 8200 1451 52
+ RATIO WAS CALCULATED BY THE SINCROS-II CODE SYSTEM. 8200 1451 53
+ - OPTICAL-MODEL, LEVEL DENSITY AND OTHER PARAMETERS USED IN8200 1451 54
+ THE SINCROS-II CALCULATION ARE DESCRIBED IN REF./2/. 8200 1451 55
+ LEVEL SCHEMES WERE DETERMINED ON THE BASIS OF ENSDF/4/. 8200 1451 56
+ -------------------------------------------------------------8200 1451 57
+ 8200 1451 58
+ 8200 1451 59
+MF=1 GENERAL INFORMATION 8200 1451 60
+ MT=451 DESCRIPTIVE DATA AND DICTIONARY 8200 1451 61
+ 8200 1451 62
+MF=2 RESONANCE PARAMETERS 8200 1451 63
+ MT=151 RESOLVED RESONANCE PARAMETERS 8200 1451 64
+ RESONANCE RANGES AND FORMULA 8200 1451 65
+ PB-204: 1.0E-5 EV TO 50 KEV, MLBW 8200 1451 66
+ PB-206: 1.0E-5 EV TO 500 KEV, REICH-MOORE 8200 1451 67
+ PB-207: 1.0E-5 EV TO 475 KEV, REICH-MOORE 8200 1451 68
+ PB-208: 1.0E-5 EV TO 1 MEV, REICH-MOORE 8200 1451 69
+ PARAMETERS WERE EVALUATED FROM THE FOLLOWING EXPERIMENTAL DATA 8200 1451 70
+ AND RECOMMENDATION BY MUGHABGHAB/5/. 8200 1451 71
+ PB-204: HOREN+84 /6/ 8200 1451 72
+ PB-206: HOREN+79 /7/, MIZUMOTO+79 /8/ 8200 1451 73
+ PB-207: HOREN+78 /9/ 8200 1451 74
+ PB-208: HOREN+86 /10/ 8200 1451 75
+ 8200 1451 76
+ CALCULATED 2200-M/S CROSS SECTIONS AND RES. INTEGRALS. 8200 1451 77
+ 2200 M/S RES. INTEG. 8200 1451 78
+ ELASTIC 11.073 B - 8200 1451 79
+ CAPTURE 0.174 B 0.143 B 8200 1451 80
+ TOTAL 11.248 B - 8200 1451 81
+ 8200 1451 82
+MF=3 NEUTRON CROSS SECTIONS 8200 1451 83
+ BELOW 1 MEV, BACKGROUND CROSS SECTIONS ARE GIVEN. 8200 1451 84
+ 8200 1451 85
+ FOR JENDL-3.2, THE THRESHOLD REACTION CROSS SECTIONS WERE 8200 1451 86
+ ADOPTED FROM JENDL FUSION FILE. THEIR CALCULATION WAS MADE WITH8200 1451 87
+ SINCROS-II SYSTEM/2/ BY ADOPTING WALTER-GUSS OMP MODIFIED BY 8200 1451 88
+ YAMAMURO/2/ FOR NEUTRONS, LEMOS OMP MODIFIED BY ARTHUR AND 8200 1451 89
+ YOUNG/11/ FOR ALPHA, THE SAME OMP'S AS THE PEGASUS CALCULATION 8200 1451 90
+ FOR OTHER CHARGED PARTICLES AND STANDARD LEVEL DENSITY 8200 1451 91
+ PARAMETERS OF SINCROS-II SYSTEM. DATA FOT NATURAL PB WERE 8200 1451 92
+ CONSTRUCTED FROM DATA FOR ISOTOPES. 8200 1451 93
+ 8200 1451 94
+ MT=1 TOTAL 8200 1451 95
+ CROSS SECTIONS IN THE ENERGY RANGE FROM 1 TO 15 MEV WERE 8200 1451 96
+ OBTAINED BASED ON THE EXPERIMENTAL DATA OF SCHWARTZ+74 /12/. 8200 1451 97
+ ABOVE 15 MEV, CROSS SECTIONS WERE CALCULATED WITH AN OPTICAL AND8200 1451 98
+ STATISTICAL MODEL CODE CASTHY /13/. THE OPTICAL POTENTIAL 8200 1451 99
+ PARAMETERS WERE OBTAINED BY FITTING AVERAGE TOTAL CROSS SECTION 8200 1451 100
+ OF NATURAL LEAD AS FOLLOWS, 8200 1451 101
+ V=47.0 - 0.250*E, WS = 2.30 + 0.41*E, VSO = 6.0 (MEV) 8200 1451 102
+ R0 = 1.25 , RS = 1.30 , RSO = 1.30 (FM) 8200 1451 103
+ A0 = 0.65 , B = 0.48 , AS0 = 0.689 (FM) 8200 1451 104
+ LEVEL DENSITY PARAMETERS WERE DETERMINED USING LOW-LYING 8200 1451 105
+ LEVEL DATA AND OBSERVED NEUTRON RESONANCE SPACING. 8200 1451 106
+ 8200 1451 107
+ MT=2 ELASTIC SCATTERING 8200 1451 108
+ (TOTAL)-(ALL OTHER PARTIAL CROSS SECTIONS) 8200 1451 109
+ 8200 1451 110
+ MT=4,51-90,91 INELASTIC SCATTERING 8200 1451 111
+ TAKEN FROM JENDL FUSION FILE. THE LEVEL SCHEME WAS TAKEN FROM 8200 1451 112
+ REF./4/. THE DATA FOR SOME LEVELS WERE LUMPED AS FOLLOWS: 8200 1451 113
+ 8200 1451 114
+ MT ENERGY(MEV) PB-204 PB-206 PB-207 PB-208 8200 1451 115
+ 51 0.5697 51 8200 1451 116
+ 52 0.8031 51 8200 1451 117
+ 53 0.8977 51 52 8200 1451 118
+ 54 1.165 52 8200 1451 119
+ 55 1.2739 52 8200 1451 120
+ 56 1.3405 53 53 8200 1451 121
+ 57 1.467 54 8200 1451 122
+ 58 1.5631 54-56 8200 1451 123
+ 59 1.6334 53 8200 1451 124
+ 60 1.665 57 8200 1451 125
+ 61 1.682 58 55 8200 1451 126
+ 62 1.703 59 56 8200 1451 127
+ 63 1.7619 60,61 57 8200 1451 128
+ 64 1.9977 58 8200 1451 129
+ 65 2.149 59 8200 1451 130
+ 66 2.2002 60 8200 1451 131
+ 67 2.315 61 54 8200 1451 132
+ 68 2.379 62-64 8200 1451 133
+ 69 2.424 65 8200 1451 134
+ 70 2.6146 51 8200 1451 135
+ 71 2.6232 55,56 8200 1451 136
+ 72 2.703 57,58 8200 1451 137
+ 73 3.1977 52 8200 1451 138
+ 74 3.4751 53 8200 1451 139
+ 75 3.7087 54 8200 1451 140
+ 76 3.9198 55,56 8200 1451 141
+ 77 3.961 57,58 8200 1451 142
+ 78 4.037 59-61 8200 1451 143
+ 79 4.0854 62 8200 1451 144
+ 80 4.106 63,64 8200 1451 145
+ 81 4.141 65,66 8200 1451 146
+ 82 4.1804 67 8200 1451 147
+ 83 4.2054 68 8200 1451 148
+ 84 4.2295 69,70 8200 1451 149
+ 85 4.2535 71 8200 1451 150
+ 86 4.2624 72 8200 1451 151
+ 87 4.296 73 8200 1451 152
+ 91 1.817 91 91 91 91 8200 1451 153
+ 8200 1451 154
+ MT=16, 17, 22, 28 (N,2N), (N,3N), (N,NA), (N,NP) 8200 1451 155
+ ADOPTED FROM JENDL FUSION FILE. THEORETICAL CALCULATION WAS 8200 1451 156
+ MADE WITH SINCROS-II. THE (N,2N) CROSS SECTION WAS ADJUSTED TO 8200 1451 157
+ REPRODUCE THE MEASURED ENARGY SPECTRA/14/ (FACTOR = 1.2). THE 8200 1451 158
+ DATA OF SIMAKOV ET AL. /15/ WERE ALSO TAKEN INTO CONSIDERATION. 8200 1451 159
+ 8200 1451 160
+ MT=102 CAPTURE 8200 1451 161
+ CALCULATED WITH CASTHY /13/ FOR PB-204, PB-206 AND PB-207. FOR 8200 1451 162
+ PB-208, ESTIMATED FROM THE EXPERIMENTAL DATA. THE CAPTURE CROSS8200 1451 163
+ SECTION OF NATURAL LEAD WAS CONSTRUCTED FROM THESE ISOTOPES. 8200 1451 164
+ Q-VALUE IS WEIGHTED AVERAGE OF Q-VALUES OF ISOTOPES. 8200 1451 165
+ 8200 1451 166
+ MT=103, 107 (N,P), (N,A) 8200 1451 167
+ CALCULATED WITH GNASH /16/ FOR EACH ISOTOPE AND CONSTRUCTED 8200 1451 168
+ ACCORDING TO THEIR ABUNDANCES. 8200 1451 169
+ 8200 1451 170
+ MT=251 MU-BAR 8200 1451 171
+ CALCULATED WITH CASTHY /13/. 8200 1451 172
+ 8200 1451 173
+MF=4 ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS 8200 1451 174
+ MT=2 8200 1451 175
+ CALCULATED WITH CASTHY /13/. 8200 1451 176
+ MT=51-87 8200 1451 177
+ TAKEN FROM JENDL FUSION FILE WHICH WERE CONSTRUCTED FROM 8200 1451 178
+ ISOTOPE DATA CALCULATED WITH SINCROS-II(CASTHY AND DWUCKY). 8200 1451 179
+ MT=16,17,22,28,91 8200 1451 180
+ ADOPTED FROM JENDL FUSION FILE. 8200 1451 181
+ 8200 1451 182
+MF=5 ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS 8200 1451 183
+ MT=16,17,22,28,91 8200 1451 184
+ ADOPTED FROM JENDL FUSION FILE. 8200 1451 185
+ 8200 1451 186
+MF=12 GAMMA-RAY MULTIPLICITY PRODUCED BY NEUTRON REACTIONS 8200 1451 187
+ MT=102 (BLELOW 1.8 MEV) 8200 1451 188
+ CALCULATED FROM ENERGY BALANCE. 8200 1451 189
+ 8200 1451 190
+MF=13 GAMMA-RAY PRODUCTION CROSS SECTIONS 8200 1451 191
+ MT=3 (ABOVE 1.8 MEV) 8200 1451 192
+ CALCULATED WITH GNASH /16/ FOR EACH ISOTOPE AND CONSTRUCTED 8200 1451 193
+ ACCORDING TO THEIR ABUNDANCES. 8200 1451 194
+ MT=4 (BELOW 1.8 MEV) 8200 1451 195
+ CALCULATED FROM INELASTIC SCATTERING CROSS SECTIONS AND 8200 1451 196
+ TRANSITION PROBABILITIES OF ISOTOPES. 8200 1451 197
+ 8200 1451 198
+MF=14 ANGULAR DISTRIBUTIONS OF SECONDARY GAMMA-RAYS 8200 1451 199
+ MT=3, 4, 102 : ASSUMED ISOTROPIC. 8200 1451 200
+ 8200 1451 201
+MF=15 ENERGY DISTRIBUTION OF SECONDARY GAMMA-RAYS 8200 1451 202
+ MT=3 (ABOVE 1.8 MEV) 8200 1451 203
+ CALCULATED WITH GNASH /16/ FOR EACH ISOTOPE AND CONSTRUCTED 8200 1451 204
+ ACCORDING TO THEIR ABUNDANCES. 8200 1451 205
+ ABOVE 10 MEV, THE CALCULATED SPECTRA WERE MODIFIED SO AS TO 8200 1451 206
+ REPRODUCE THE MEASUREMENTS OF CHAPMAN ET AL./17/ 8200 1451 207
+ MT=102 (BELOW 1.8 MEV) 8200 1451 208
+ CALCULATED WITH CASTHY/13/. 8200 1451 209
+ 8200 1451 210
+REFERENCES 8200 1451 211
+ 1) CHIBA, S. ET AL.: JAERI-M 92-027, P.35 (1992). 8200 1451 212
+ 2) YAMAMURO, N.: JAERI-M 90-006 (1990). 8200 1451 213
+ 3) KUMABE, I. ET AL.: NUCL. SCI. ENG., 104, 280 (1990). 8200 1451 214
+ 4) ENSDF: EVALUATED NUCLEAR STRUCTURE DATA FILE, BNL/NNDC. 8200 1451 215
+ 5) MUGHABGHAB S.F.: NEUTRON CROSS SECTIONS, VOL.1, PART B, 8200 1451 216
+ ACADEMIC PRESS (1984). 8200 1451 217
+ 6) HOREN D.J. ET AL. : PHYS. REV. C29, 2126 (1984). 8200 1451 218
+ 7) HOREN D.J. ET AL. : PHYS. REV. C20, 478 (1979). 8200 1451 219
+ 8) MIZUMOTO M. ET AL. : PHYS. REV. C19 ,335 (1979). 8200 1451 220
+ 9) HOREN D.J. ET AL. : PHYS. REV. C18, 722 (1978). 8200 1451 221
+10) HOREN D. J. ET AL. : PHYS. REV. C34, 420 (1986). 8200 1451 222
+11) ARTHUR, E.D. AND YOUNG, P.G.: LA-8626-MS (1980). 8200 1451 223
+12) SCHWARTZ R.B. ET AL.: NBS-MONO-138 (1974), DATA IN EXFOR 8200 1451 224
+ (1971). 8200 1451 225
+13) IGARASI S. AND FUKAHORI T.: JAERI 1321 (1991). 8200 1451 226
+14) TAKAHASHI A. ET AL.: JAERI-M 86-080, 393 (1986). 8200 1451 227
+15) SIMAKOV S.P. ET AL: WORKSHOP ON NUCL. DATA FOR FUSION REACTOR 8200 1451 228
+ TECHNOL., DEL MAR, MAR 3-6 (1993). 8200 1451 229
+16) YOUNG P.G. AND ARTHUR E.D.: LA-6974 (1977). 8200 1451 230
+17) CHAPMAN G.T. ET AL.: ORNL/TM-4822 (1975). 8200 1451 231
+ 8200 1451 232
+ 1 451 339 18200 1451 233
+ 2 151 532 28200 1451 234
+ 3 1 241 28200 1451 235
+ 3 2 227 28200 1451 236
+ 3 4 59 28200 1451 237
+ 3 16 9 28200 1451 238
+ 3 17 7 28200 1451 239
+ 3 22 9 28200 1451 240
+ 3 28 9 28200 1451 241
+ 3 51 16 28200 1451 242
+ 3 52 18 28200 1451 243
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+ 3 57 16 28200 1451 248
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+ 3 60 13 28200 1451 251
+ 3 61 17 28200 1451 252
+ 3 62 15 28200 1451 253
+ 3 63 15 28200 1451 254
+ 3 64 13 28200 1451 255
+ 3 65 12 28200 1451 256
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+ 3 67 14 28200 1451 258
+ 3 68 11 28200 1451 259
+ 3 69 10 28200 1451 260
+ 3 70 19 28200 1451 261
+ 3 71 12 28200 1451 262
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+ 3 75 17 28200 1451 266
+ 3 76 15 28200 1451 267
+ 3 77 15 28200 1451 268
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diff --git a/test/periodic/db/isotopes.dat b/test/periodic/db/isotopes.dat
new file mode 100644
index 0000000000000000000000000000000000000000..3284e9f27240f7aeae293ebdfa9050fa179ce715
--- /dev/null
+++ b/test/periodic/db/isotopes.dat
@@ -0,0 +1,4002 @@
+118
+1 H Hydrogen 4
+ 1.00794 (7)
+ 8.988E-5
+ -259.34
+ -252.87
+ +1,-1
+* 1 1/2+ 7.289 99.985% (1)
+* 2 1+ 13.136 0.015% (1)
+ 3 1/2+ 14.950 12.33 y (6) B-
+ 4 2- 26.0 5.42 MeV N
+2 He Helium 8
+ 4.002602 (2)
+ 1.785E-4
+ (26 atm)
+ -268.93
+ 0
+* 3 1/2+ 14.931 0.000137% (3)
+* 4 0+ 2.425 99.999863% (3)
+ 5 3/2- 11.39 0.60 MeV (2) A ,N
+ 6 0+ 17.594 806.7 ms (15) B-
+ 7 (3/2)- 26.11 160 keV (30) N
+ 8 0+ 31.598 119.0 ms (15) B-,BN 16%
+ 9 (1/2-) 40.82 ~ 0.3 MeV N
+ 10 0+ 48.81 0.3 MeV (2) N
+3 Li Lithium 8
+ 6.941 (2)
+ 0.534 c
+ 180.5
+ 1342
+ +1
+ 4 2- 25.3 6.03 MeV P
+ 5 3/2- 11.68 ~ 1.5 MeV A ,P
+* 6 1+ 14.086 7.5% (2)
+* 7 3/2- 14.908 92.5% (2)
+ 8 2+ 20.945 838 ms (6) B-,B2A
+ 9 3/2- 24.954 178.3 ms (4) B-,BN 49.5%,BN2A
+ 10 33.44 1.2 MeV (3) N
+ 11 3/2- 40.79 8.5 ms (2) B-,BNA 0.027%
+4 Be Beryllium 9
+ 9.012182 (3)
+ 1.848 c
+ 1287
+ 2471 (5mm)
+ +2
+ 6 0+ 18.375 92 keV (6) 2P
+ 7 3/2- 15.77 53.29 d (7) EC
+ 8 0+ 4.942 6.8 EV (17) 2A
+* 9 3/2- 11.348 100%
+ 10 0+ 12.607 1.51E+6 y (6) B-
+ 11 1/2+ 20.174 13.81 s (8) B-,BA 3.1%
+ 12 0+ 25.08 23.6 ms (9) B-,BN <1%
+ 13 (1/2,5/2)+ 35.16 0.9 MeV (5) N
+ 14 0+ 39.9 4.35 ms (17) B-,BN 81%,B2N 5%
+5 B Boron 11
+ 10.811 (5)
+ 2.34 h
+ 2075
+ 4000 (subl.)
+ +3
+ 7 (3/2-) 27.87 1.4 MeV (2) P ,2P ,3P
+ 8 2+ 22.921 770 ms (3) EA,EC,E2A
+ 9 3/2- 12.416 0.54 keV (21) 2A ,P
+* 10 3+ 12.051 19.9% (2)
+* 11 3/2- 8.668 80.1% (2)
+ 12 1+ 13.369 20.20 ms (2) B-,B3A 1.58%
+ 13 3/2- 16.562 17.36 ms (16) B-
+ 14 2- 23.66 13.8 ms (10) B-
+ 15 28.97 10.5 ms (3) B-
+ 16 (0-) 37.1s N
+ 17 (3/2-) 43.7 5.08 ms (5) B-,BXN
+6 C Carbon 15
+ 12.011
+ 1.8 to 2.1 i
+ ~3550
+ 4827
+ +2,+4,-4
+ 8 0+ 35.09 230 keV (50) 2P
+ 9 (3/2-) 28.914 126.5 ms (9) EC,EP,E2A
+ 10 0+ 15.699 19.255 s (53) EC
+ 11 3/2- 10.650 20.39 m (2) EC
+* 12 0+ 98.89% (1)
+* 13 1/2- 3.125 1.11% (1)
+ 14 0+ 3.020 5730 y (40) B-
+ 15 1/2+ 9.873 2.449 s (5) B-
+ 16 0+ 13.694 0.747 s (8) B-
+ 17 21.04 193 ms (13) B-,BN 32%
+ 18 0+ 24.92 88 ms (+9-8) B-
+ 18 0+ 24.92 66 ms (+25-15) BN 19%
+ 19 32.8 49 ms (4) B- ,BN 61%
+ 20 0+ 37.6 14 ms (6) B- ,BN 72%
+ 22 0+ 52.6s > 200 NS
+7 N Nitrogen 15
+ 14.00674 (7)
+ 0.0012506 j
+ -210.00
+ -195.79
+ +1,+2,+3,+4,+5,-1,-2,-3
+ 10 39.7s
+ 11 1/2+ 25.3 1.58 MeV (+75-5) P
+ 12 1+ 17.338 11.000 ms (16) EC,E3A 3.44%
+ 13 1/2- 5.34 9.965 m (4) EC
+* 14 1+ 2.863 99.634% (9)
+* 15 1/2- 0.102 0.366% (9)
+ 16 2- 5.682 7.13 s (2) B-
+ 16m 0- 5.802 7.25 us (6) B- ,IT
+ 17 1/2- 7.87 4.173 s (4) B-,BN
+ 18 1- 13.12 624 ms (12) B-,B-A
+ 19 15.86 0.304 s (16) B-,BN ~ 62.4%
+ 20 21.77 100 ms (+30-20) B-,BN ~ 61%
+ 21 25.23 95 ms (13) B- ,BN 84%
+ 22 32.1 24 ms (7) B- ,BN 35%
+ 23 37.7s > 200 NS
+8 O Oxygen 13
+ 15.9994 (3)
+ 0.001429 k
+ -218.79
+ -182.95
+ -2
+ 12 0+ 32.06 0.40 MeV (25) P
+ 13 (3/2-) 23.111 8.58 ms (5) EC
+ 14 0+ 8.00 70.606 s (18) EC
+ 15 1/2- 2.856 122.24 s (16) EC
+* 16 0+ -4.737 99.762% (15)
+* 17 5/2+ -0.808 0.038% (3)
+* 18 0+ -0.781 0.200% (12)
+ 19 5/2+ 3.332 26.91 s (8) B-
+ 20 0+ 3.797 13.51 s (5) B-
+ 21 (1/2,3/2,5 8.06 3.42 s (10) B-
+ 22 0+ 9.28 2.25 s (15) B-
+ 23 14.6 82 ms (37) B-,BN 31%
+ 24 0+ 19.0 61 ms (26) B-,BN 58%
+9 F Fluorine 14
+ 18.9984032 (5)
+ 0.001696
+ -219.62 g
+ -188.12 g
+ -1
+ 14 (2-) 33.6s P
+ 15 (1/2+) 16.8 1.0 MeV (2) P
+ 16 0- 10.680 40 keV (20) P
+ 17 5/2+ 1.952 64.49 s (16) EC
+ 18 1+ 0.873 109.77 m (5) EC
+* 19 1/2+ -1.487 100%
+ 20 2+ -0.016 11.00 s (2) B-
+ 21 5/2+ -0.047 4.158 s (20) B-
+ 22 4+,(3+) 2.79 4.23 s (4) B-
+ 23 (3/2,5/2)+ 3.33 2.23 s (14) B-
+ 24 (1,2,3)+ 7.54 0.34 s (8) B-
+ 25 11.27 B- ,BN
+ 27 25.1 > 200 NS
+ 29 40.3s > 200 NS
+10 Ne Neon 17
+ 20.1797 (6)
+ 8.9990E-4
+ -248.59
+ -246.088 g
+ 0
+ 15 41.4s
+ 16 0+ 23.99 122 keV (37) P
+ 17 1/2- 16.49 109.2 ms (6) EC,EP,EA
+ 18 0+ 5.319 1672 ms (8) EC
+ 19 1/2+ 1.751 17.22 s (2) EC
+* 20 0+ -7.042 90.48% (3)
+* 21 3/2+ -5.732 0.27% (1)
+* 22 0+ -8.024 9.25% (3)
+ 23 5/2+ -5.154 37.24 s (12) B-
+ 24 0+ -5.948 3.38 m (2) B-
+ 25 (1/2,3/2)+ -2.06 602 ms (8) B-
+ 26 0+ 0.43 0.23 s (6) B-
+ 27 7.09 32 ms (2) B- ,BN
+ 28 0+ 11.3 14 ms (10) B- ,BN 16%
+ 29 18.0 0.2 s (1) BN ?%
+ 30 0+ 22.2 > 200 NS
+ 32 0+ 37.2s > 200 NS
+11 Na Sodium 21
+ 22.989770 (2)
+ 0.971 c
+ 97.72
+ 883
+ +1
+ 17 35.2s
+ 18 25.3s
+ 19 12.93
+ 20 2+ 6.845 447.9 ms (23) EC
+ 21 3/2+ -2.184 22.49 s (4) EC
+ 22 3+ -5.182 2.6019 y (4) EC
+* 23 3/2+ -9.53 100%
+ 24 4+ -8.418 14.9590 h (12) B-
+ 24m 1+ -7.946 20.20 ms (7) IT 99.95%,B- 0.05%
+ 25 5/2+ -9.358 59.1 s (6) B-
+ 26 3+ -6.90 1.072 s (9) B-
+ 27 5/2+ -5.58 301 ms (6) B-,BN 0.08%
+ 28 1+ -1.03 30.5 ms (4) B-,BN 0.58%
+ 29 2.62 44.9 ms (12) B-
+ 29 3/2 2.62 44.9 ms (12) BN 21.5%
+ 30 2+ 8.59 48 ms (2) B-,BN 30%,B2N 1.17%
+ 31 3/2+ 12.7 17.0 ms (4) B-,BN 37%,B2N 0.9%
+ 32 (3-,4-) 18.3 13.2 ms (4) B-,BN 24%,B2N 8%
+ 33 26 8.2 ms (4) B-,BN 52%,B2N 12%
+ 34 33s 5.5 ms (10) B-,BN ,B2N 57.5%
+ 35 41s 1.5 ms (5) B-,BN
+12 Mg Magnesium 17
+ 24.3050 (6)
+ 1.738 c
+ 650
+ 1090
+ +2
+ 20 0+ 17.57 95 ms (+80-50) EC,EP >= 3%
+ 21 (3/2,5/2)+ 10.91 122 ms (3) EC,EP 29.3%
+ 22 0+ -0.396 3.857 s (9) EC
+ 23 3/2+ -5.473 11.317 s (11) EC
+* 24 0+ -13.933 78.99% (3)
+* 25 5/2+ -13.193 10.00% (1)
+* 26 0+ -16.215 11.01% (2)
+ 27 1/2+ -14.587 9.458 m (12) B-
+ 28 0+ -15.019 20.91 h (3) B-
+ 29 3/2+ -10.66 1.30 s (12) B-
+ 30 0+ -8.88 335 ms (17) B-
+ 31 -3.22 230 ms (20) B-,BN 1.7%
+ 32 0+ -0.79 120 ms (20) B-,BN 2.4%
+ 33 5.2 90 ms (20) B-,BN 17%
+ 34 0+ 8.5 20 ms (10) B-,BN
+ 35 16.3s > 200 NS
+ 36 0+ 20.9s > 200 NS
+13 Al Aluminum 21
+ 26.981539 (5)
+ 2.6989 c
+ 660.32
+ 2519
+ +3
+ 21 26.1s < 35 NS
+ 22 18.18s 70 ms (+50-35) EC ,EP > 0%,E2P > 0%
+ 23 6.77 0.47 s (3) EC,EP
+ 24 4+ -0.054 2.053 s (4) EC,EA 0.04%
+ 24m 1+ 0.371 131.3 ms (25) IT 82%,EC 18%
+ 25 5/2+ -8.916 7.183 s (12) EC
+ 26 5+ -12.210 7.4E+5 y (3) EC
+ 26m 0+ -11.982 6.3452 s (19) EC
+* 27 5/2+ -17.197 100%
+ 28 3+ -16.851 2.2414 m (12) B-
+ 29 5/2+ -18.216 6.56 m (6) B-
+ 30 3+ -15.87 3.60 s (6) B-
+ 31 (3/2,5/2)+ -14.95 644 ms (25) B-
+ 32 1+ -11.06 33 ms (4) B-
+ 33 -8.50 > 1 us
+ 34 -2.86 60 ms (18) B-,BN 27%
+ 35 -0.0 150 ms (50) B-,BN 65%
+ 36 5.9 > 1 us
+ 37 9.6 > 1 us
+ 38 15.7s > 200 NS
+ 39 > 200 NS
+14 Si Silicon 21
+ 28.0855 (3)
+ 2.33 e
+ 1414
+ 3265
+ +2,+4,-4
+ 22 0+ 32.2s 6 ms (3) EC ,EP
+ 23 23.8s > 200 NS
+ 24 0+ 10.75 102 ms (35) EC,EP ~ 7%
+ 25 5/2+ 3.825 220 ms (3) EC,EP
+ 26 0+ -7.145 2.234 s (13) EC
+ 27 5/2+ -12.385 4.16 s (2) EC
+* 28 0+ -21.493 92.23% (1)
+* 29 1/2+ -21.895 4.67% (21)
+* 30 0+ -24.433 3.10% (1)
+ 31 3/2+ -22.949 157.3 m (3) B-
+ 32 0+ -24.081 172 y (4) B-
+ 33 -20.49 6.18 s (18) B-
+ 34 0+ -19.96 2.77 s (20) B-
+ 35 -14.36 0.78 s (12) B-
+ 36 0+ -12.4 0.45 s (6) B-,BN < 10%
+ 37 -6.5 > 1 us BN < 15%
+ 38 0+ -3.7 > 1 us
+ 39 2.1s > 1 us
+ 40 0+ 5.4s > 200 NS
+ 41 11.8s > 200 NS
+ 42 0+ > 200 NS
+15 P Phosphorus 23
+ 30.973761 (2)
+ 1.82 l
+ 44.15 l
+ 277 l
+ +3,+5,-3
+ 24 32.0s
+ 25 18.9s
+ 26 (3+) 11.0s 20 ms (+35-15) EC,EP 2%,E2P
+ 27 (1/2+) -0.74 260 ms (80) EC,EP 6%
+ 28 3+ -7.161 270.3 ms (5) EC
+ 29 1/2+ -16.952 4.140 s (14) EC
+ 30 1+ -20.201 2.498 m (4) EC
+* 31 1/2+ -24.441 100%
+ 32 1+ -24.305 14.262 d (14) B-
+ 33 1/2+ -26.338 25.34 d (12) B-
+ 34 1+ -24.558 12.43 s (8) B-
+ 35 1/2+ -24.858 47.3 s (7) B-
+ 36 -20.25 5.6 s (3) B-
+ 37 -18.99 2.31 s (13) B-
+ 38 -14.5 0.64 s (14) B-,BN < 10%
+ 39 -12.6 0.16 s (+30-10) B-,BN 41%
+ 40 -8.3 260 ms (80) B-,BN 30%
+ 41 -4.8 120 ms (20) B-,BN 30%
+ 42 0.1s 110 ms (30) B-,BN 50%
+ 43 3.1s 33 ms (3) B- ,BN
+ 44 > 200 NS
+ 45 > 200 NS
+ 46 > 200 NS
+16 S Sulfur 22
+ 32.066 (6)
+ 2.07 cm
+ 115.21 m
+ 444.60
+ +4,+6,-2
+ 27 17.5s EC
+ 28 0+ 4.1 125 ms (10) EC,EP > 0%
+ 29 5/2+ -3.16 187 ms (4) EC
+ 30 0+ -14.063 1.178 s (5) EC
+ 31 1/2+ -19.045 2.572 s (13) EC
+* 32 0+ -26.016 95.02% (9)
+* 33 3/2+ -26.586 0.75% (1)
+* 34 0+ -29.932 4.21% (8)
+ 35 3/2+ -28.846 87.51 d (12) B-
+* 36 0+ -30.664 0.02% (1)
+ 37 7/2- -26.896 5.05 m (2) B-
+ 38 0+ -26.861 170.3 m (7) B-
+ 39 (3/2,5/2,7 -23.16 11.5 s (5) B-
+ 40 0+ -22.8 8.8 s (22) B-
+ 41 -18.6 > 1 us
+ 42 0+ -17.2 0.56 s (6) B- ,BN < 4%
+ 43 -12.5 220 ms (65) B-,BN 40%
+ 44 0+ -10.9s 123 ms (10) B-,BN 18%
+ 45 -4.8s 82 ms (13) B-
+ 46 0+ > 200 NS
+ 47 > 200 NS
+ 48 0+ > 200 NS
+17 Cl Chlorine 22
+ 35.4527 (9)
+ 0.003214
+ -101.5
+ -34.04
+ +1,+5,+7,-1
+ 31 -7.06 150 ms (25) EC,EP 0.44%
+ 32 1+ -13.331 298 ms (1) EC,EA 0.01%,EP 7.0E-3%
+ 33 3/2+ -21.004 2.511 s (3) EC
+ 34 0+ -24.440 1.5264 s (14) EC
+ 34m 3+ -24.294 32.00 m (4) EC 55.4%,IT 44.6%
+* 35 3/2+ -29.014 75.77% (5)
+ 36 2+ -29.522 3.01E+5 y (2) B- 98.1%,EC 1.9%
+* 37 3/2+ -31.762 24.23% (5)
+ 38 2- -29.798 37.24 m (5) B-
+ 38m 5- -29.127 715 ms (3) IT
+ 39 3/2+ -29.800 55.6 m (2) B-
+ 40 2- -27.56 1.35 m (2) B-
+ 41 (1/2,3/2)+ -27.34 38.4 s (8) B-
+ 42 -25.0 6.8 s (3) B-
+ 43 -24.0 3.3 s (2) B-
+ 44 -20.0 0.43 s (6) B- ,BN < 8%
+ 45 -18.9 400 ms (43) B-,BN 24%
+ 46 -14.8s 0.22 s (4) B- ,BN 60%
+ 47 -11.2s > 200 NS B-,BN <= 3%
+ 48 > 200 NS
+ 49 -1.382C 170 NS GE
+ 51 > 200 NS
+18 Ar Argon 18
+ 39.948
+ 0.0017837
+ -189.35
+ -185.85
+ 0
+ 32 0+ -2.18 98 ms (2) EC,EP
+ 33 1/2+ -9.38 173.0 ms (20) EC,EP 38.7%
+ 34 0+ -18.378 844.5 ms (34) EC
+ 35 3/2+ -23.048 1.775 s (4) EC
+* 36 0+ -30.231 0.3365% (30)
+ 37 3/2+ -30.948 35.04 d (4) EC
+* 38 0+ -34.715 0.0632% (5)
+ 39 7/2- -33.242 269 y (3) B-
+* 40 0+ -35.040 99.6003% (30)
+ 41 7/2- -33.067 109.34 m (12) B-
+ 42 0+ -34.42 32.9 y (11) B-
+ 43 (3/2,5/2) -31.98 5.37 m (6) B-
+ 44 0+ -32.26 11.87 m (5) B-
+ 45 -29.72 21.48 s (15) B-
+ 46 0+ -29.72 8.4 s (6) B-
+ 49 -17.813C 170 NS GE
+ 50 0+ -14.228C 170 NS GE
+ 51 > 200 NS
+19 K Potassium 21
+ 39.0983
+ 0.862 c
+ 63.38
+ 759
+ +1
+ 35 3/2+ -11.17 190 ms (30) EC,EP 0.37%
+ 36 2+ -17.425 342 ms (2) EC,EP 0.05%,EA 3.4E-3%
+ 37 3/2+ -24.799 1.226 s (7) EC
+ 38 3+ -28.802 7.636 m (18) EC
+ 38m 0+ -28.672 923.9 ms (6) EC
+* 39 3/2+ -33.807 93.2581% (44)
+ 40 4- -33.535 1.277E+9 y (8) B- 89.28%,EC 10.72%
+* 41 3/2+ -35.559 6.7302% (44)
+ 42 2- -35.021 12.360 h (3) B-
+ 43 3/2+ -36.593 22.3 h (1) B-
+ 44 2- -35.81 22.13 m (19) B-
+ 45 3/2+ -36.61 17.3 m (6) B-
+ 46 (2-) -35.42 105 s (10) B-
+ 47 1/2+ -35.697 17.50 s (24) B-
+ 48 (2-) -32.12 6.8 s (2) B-,BN 1.14%
+ 49 (3/2+) -30.32 1.26 s (5) B-,BN 86%
+ 50 (0-,1,2-) -25.4 472 ms (4) B-,BN 29%
+ 51 (1/2+,3/2+ -22.511C 365 ms (5) B-,BN 47%
+ 52 -16.523C 105 ms (5) B-,BN > 88%
+ 53 (3/2+) -12.359C 30 ms (5) B-,BN 85%
+ 54 -5.488C 10 ms (5) B-,BN
+20 Ca Calcium 19
+ 40.078 (4)
+ 1.55 c
+ 842
+ 1484
+ +2
+ 35 4.44s 50 ms (30) EC,E2P
+ 36 0+ -6.44 102 ms (2) EC,EP ~ 20%
+ 37 3/2+ -13.16 181.1 ms (10) EC,EP 76%
+ 38 0+ -22.059 440 ms (8) EC
+ 39 3/2+ -27.276 859.6 ms (14) EC
+* 40 0+ -34.846 96.941% (18)
+ 41 7/2- -35.138 1.03E+5 y (4) EC
+* 42 0+ -38.547 0.647% (9)
+* 43 7/2- -38.408 0.135% (6)
+* 44 0+ -41.469 2.086% (12)
+ 45 7/2- -40.813 162.61 d (9) B-
+* 46 0+ -43.135 0.004% (3)
+ 47 7/2- -42.340 4.536 d (3) B-
+ 48 0+ -44.215 > 6E+18 y 2B-
+ 49 3/2- -41.290 8.718 m (6) B-
+ 50 0+ -39.572 13.9 s (6) B-
+ 51 (3/2-) -35.90 10.0 s (8) B-,BN
+ 52 0+ -32.5 4.6 s (3) B-
+ 53 (3/2-,5/2- -27.9s 90 ms (15) B-,BN > 30%
+21 Sc Scandium 21
+ 44.955910 (8)
+ 2.989 e
+ 1541
+ 2830
+ +3
+ 40 4- -20.526 182.3 ms (7) EC,EP 0.44%,EA 0.02%
+ 41 7/2- -28.642 596.3 ms (17) EC
+ 42 0+ -32.121 681.3 ms (7) EC
+ 42m 7+,(5,6)+ -31.505 61.7 s (4) EC
+ 43 7/2- -36.188 3.891 h (12) EC
+ 44 2+ -37.816 3.927 h (8) EC
+ 44m 6+ -37.545 58.6 h (1) IT 98.8%,EC 1.2%
+* 45 7/2- -41.069 100%
+ 45m 3/2+ -41.057 318 ms (7) IT
+ 46 4+ -41.759 83.79 d (4) B-
+ 46m 1- -41.616 18.75 s (4) IT
+ 47 7/2- -44.332 3.3492 d (6) B-
+ 48 6+ -44.493 43.67 h (9) B-
+ 49 7/2- -46.552 57.2 m (2) B-
+ 50 5+ -44.54 102.5 s (5) B-
+ 50m (2,3)+ -44.28 0.35 s (4) IT > 97.5%,B- < 2.5%
+ 51 (7/2)- -43.22 12.4 s (1) B-
+ 52 3+ -40.5 8.2 s (2) B-
+ 53 -38.0s > 1 us
+ 54 -34.0 > 1 us
+ 55 -30s > 1 us
+22 Ti Titanium 20
+ 47.867
+ 4.54
+ 1668
+ 3287
+ +2,+3,+4
+ 39 1.2s 26 ms (8)
+ 40 0+ -8.9 50 ms (15) EC,EP
+ 41 3/2+ -15.71s 80 ms (2) EC,EP ~100%
+ 42 0+ -25.121 199 ms (6) EC
+ 43 7/2- -29.320 509 ms (5) EC
+ 44 0+ -37.548 49 y (3) EC
+ 45 7/2- -39.007 184.8 m (5) EC
+* 46 0+ -44.125 8.25% (3)
+* 47 5/2- -44.932 7.44% (2)
+* 48 0+ -48.487 73.72% (3)
+* 49 7/2- -48.558 5.41% (2)
+* 50 0+ -51.426 5.18% (2)
+ 51 3/2- -49.727 5.76 m (1) B-
+ 52 0+ -49.464 1.7 m (1) B-
+ 53 (3/2)- -46.8 32.7 s (9) B-
+ 54 0+ -45.6 > 1 us
+ 55 -41.7 > 1 us
+ 56 0+ -39.1 > 200 NS
+ 57 -34.0s > 200 NS
+ 58 0+ > 150 NS
+23 V Vanadium 21
+ 50.9415
+ 6.11 (18.7C)
+ 1910
+ 3407
+ +2,+3,+4,+5
+ 42 -8.2s < 55 NS
+ 43 (7/2-) -18.0s > 800 ms EC
+ 44 -23.85s 90 ms (25) EC,EA
+ 44m 6+ -23.85s 155 ms IT ?%
+ 45 7/2- -31.87 547 ms (6) EC
+ 46 0+ -37.074 422.37 ms (20) EC
+ 47 3/2- -42.004 32.6 m (3) EC
+ 48 4+ -44.475 15.9735 d (25) EC
+ 49 7/2- -47.956 330 d (15) EC
+ 50 6+ -49.218 1.4E+17 y (4) EC 83%,B- 17%
+* 51 7/2- -52.198 99.750% (2)
+ 52 3+ -51.438 3.743 m (5) B-
+ 53 7/2- -51.845 1.61 m (4) B-
+ 54 3+ -49.89 49.8 s (5) B-
+ 55 (7/2-) -49.15 6.54 s (15) B-
+ 56 -46.2 > 1 us
+ 57 -44.3 > 200 NS
+ 58 -40.3 > 200 NS
+ 59 -37.9 > 200 NS B-
+ 60 -33.1 > 200 NS
+ 61 > 150 NS
+24 Cr Chromium 22
+ 51.9961 (6)
+ 7.18 to 7.20 c
+ 1907
+ 2671
+ +2,+3,+6
+ 43 (3/2+) -2.14s 21 ms (+4-3) EC ,EP ,EA ?%
+ 44 0+ -13.5s 53 ms (+4-3) EP
+ 45 -19.4s 50 ms (6) EC,EP > 27%
+ 46 0+ -29.47 0.26 s (6) EC
+ 47 3/2- -34.55 500 ms (15) EC
+ 48 0+ -42.815 21.56 h (3) EC
+ 49 5/2- -45.326 42.3 m (1) EC
+ 50 0+ -50.255 > 1.8E+17 y 2EC
+ 51 7/2- -51.445 27.702 d (4) EC
+* 52 0+ -55.413 83.789% (18)
+* 53 3/2- -55.281 9.501% (17)
+* 54 0+ -56.929 2.365% (7)
+ 55 3/2- -55.104 3.497 m (3) B-
+ 56 0+ -55.289 5.94 m (10) B-
+ 57 3/2-,5/2-, -52.39 21.1 s (10) B-
+ 58 0+ -51.9 7.0 s (3) B-
+ 59 -47.8 0.74 s (24) B-
+ 60 0+ -46.8 0.57 s (6) B-
+ 61 -42.8 > 200 NS B-
+ 62 0+ -41.2 > 200 NS
+ 63 > 150 NS
+ 64 0+ > 1 us
+25 Mn Manganese 25
+ 54.938049 (9)
+ 7.21 to 7.44 n
+ 1246
+ 2061
+ +2,+3,+4,+7
+ 46 (4+) -12.4s 41 ms (+7-6) EC ,EP
+ 47 -22.3s > 200 NS EP
+ 48 4+ -29.29s 158.1 ms (22) EC,EP 0.28%,EA <6.0E-4%
+ 49 5/2- -37.61 382.1 ms (68) EC
+ 50 0+ -42.622 283.88 ms (46) EC
+ 50m 5+ -42.393 1.75 m (3) EC
+ 51 5/2- -48.237 46.2 m (1) EC
+ 52 6+ -50.701 5.591 d (3) EC
+ 52m 2+ -50.323 21.1 m (2) EC 98.25%,IT 1.75%
+ 53 7/2- -54.684 3.74E+6 y (4) EC
+ 54 3+ -55.552 312.12 d (10) EC,B- <0.001%
+* 55 5/2- -57.707 100%
+ 56 3+ -56.906 2.5785 h (2) B-
+ 57 5/2- -57.485 85.4 s (18) B-
+ 58 3+ -55.90 65.3 s (7) B-
+ 58m + -55.90 3.0 s (1) B-
+ 59 3/2-,5/2- -55.47 4.6 s (1) B-
+ 60 0+ -52.8 51 s (6) B-
+ 60m 3+ -52.5 1.77 s (2) B- 88.5%,IT 11.5%
+ 61 (5/2)- -51.6 0.71 s (1) B-
+ 62 (3+) -48.5 0.88 s (15) B-
+ 63 -46.8 0.25 s (4) B-
+ 64 -43.1 > 200 NS
+ 65 -40.9 > 200 NS B-
+ 66 > 150 NS
+26 Fe Iron 26
+ 55.845 (2)
+ 7.874 c
+ 1538
+ 2861
+ +2,+3
+ 46 0+ 0.8s 20 ms (+20-8) EP ?%
+ 47 -6.6s 27 ms (+32-10) EP ?%
+ 48 0+ -18.1s 200 NS GE
+ 49 (7/2-) -24.6s 75 ms (10) EC,EP <= 60%
+ 50 0+ -34.47 150 ms (30) EC,EP ~ 0%
+ 51 (5/2-) -40.22 305 ms (5) EC
+ 52 0+ -48.33 8.275 h (8) EC
+ 52m (12+) -41.51 45.9 s (6) EC
+ 53 7/2- -50.941 8.51 m (2) EC
+ 53m 19/2- -47.901 2.58 m (4) IT
+* 54 0+ -56.249 5.845% (35)
+ 55 3/2- -57.475 2.73 y (3) EC
+* 56 0+ -60.601 91.754% (36)
+* 57 1/2- -60.176 2.119% (10)
+* 58 0+ -62.149 0.282% (4)
+ 59 3/2- -60.659 44.503 d (6) B-
+ 60 0+ -61.407 1.5E+6 y (3) B-
+ 61 3/2-,5/2- -58.92 5.98 m (6) B-
+ 62 0+ -58.90 68 s (2) B-
+ 63 (5/2)- -55.5 6.1 s (6) B-
+ 64 0+ -54.9 2.0 s (2) B-
+ 65 -51.3 0.4 s (2) B-
+ 66 0+ -50.3 > 200 NS
+ 67 -46.6 > 200 NS B-
+ 68 0+ -44.2s 0.10 s (6) B-
+ 69 > 150 NS
+27 Co Cobalt 27
+ 58.933200 (9)
+ 8.9 c
+ 1495
+ 2927
+ +2,+3
+ 50 -17.5s 200 NS GE
+ 52 -34.32s EC ,EP
+ 53 (7/2-) -42.64 240 ms (20) EC
+ 53m (19/2-) -39.45 247 ms (12) EC ~ 98.5%,P ~ 1.5%
+ 54 0+ -48.006 193.28 ms (14) EC
+ 54m (7)+ -47.807 1.48 m (2) EC
+ 55 7/2- -54.024 17.53 h (3) EC
+ 56 4+ -56.035 77.27 d (3) EC
+ 57 7/2- -59.340 271.79 d (9) EC
+ 58 2+ -59.842 70.82 d (3) EC
+ 58m 5+ -59.817 9.15 h (10) IT
+* 59 7/2- -62.224 100%
+ 60 5+ -61.645 1925.1 d (5) B-
+ 60m 2+ -61.586 10.467 m (6) IT 99.76%,B- 0.24%
+ 61 7/2- -62.895 1.650 h (5) B-
+ 62 2+ -61.43 1.50 m (4) B-
+ 62m 5+ -61.41 13.91 m (5) B- > 99%,IT < 1%
+ 63 (7/2)- -61.84 27.4 s (5) B-
+ 64 1+ -59.79 0.30 s (3) B-
+ 65 (7/2)- -59.16 1.20 s (6) B-
+ 66 (3+) -56.1 0.23 s (2) B-
+ 67 (7/2-) -55.3 0.42 s (7) B-
+ 68 -51.8 0.18 s (10) B-
+ 69 -51.0 0.27 s (5) B-
+ 70 -46.8s > 200 NS B-
+ 71 -45.0s 0.20 s (5) B-
+ 72 > 1 us
+28 Ni Nickel 27
+ 58.6934 (2)
+ 8.902 e
+ 1455
+ 2913
+ +2,+3
+ 50 0+ -3.8s > 150 NS
+ 51 -11.4s > 200 NS
+ 52 0+ -22.65s 38 ms (5) EC,EP 17%
+ 53 (7/2-) -29.4s 45 ms (15) EC
+ 54 0+ -39.21 EC
+ 55 7/2- -45.33 212.1 ms (38) EC
+ 56 0+ -53.90 6.077 d (12) EC
+ 57 3/2- -56.076 35.60 h (6) EC
+* 58 0+ -60.223 68.077% (9)
+ 59 3/2- -61.151 7.6E+4 y (5) EC
+* 60 0+ -64.468 26.223% (8)
+* 61 3/2- -64.217 1.140% (1)
+* 62 0+ -66.743 3.634% (2)
+ 63 1/2- -65.51 100.1 y (20) B-
+* 64 0+ -67.096 0.926% (1)
+ 65 5/2- -65.123 2.5172 h (3) B-
+ 66 0+ -66.03 54.6 h (4) B-
+ 67 (1/2-) -63.74 21 s (1) B-
+ 68 0+ -63.49 19 s (+3-6) B-
+ 69 -60.4 11.4 s (3) B-
+ 70 0+ -59.5 B-
+ 71 -55.9 1.86 s (35) B-
+ 72 0+ -54.7 2.06 s (30) B-
+ 73 -50.3s 0.90 s (15) B-
+ 74 0+ -48.7s 1.1 s (5) B-
+ 75 -44.2s > 1 us
+ 76 0+ -42.2s > 150 NS
+29 Cu Copper 28
+ 63.546 (3)
+ 8.96 c
+ 1084.62
+ 2562
+ +1,+2
+ 55 -32.1s > 200 NS EC,EP
+ 56 -38.6s > 200 NS EC ,EP
+ 57 3/2- -47.31 199.4 ms (32) EC
+ 58 1+ -51.660 3.204 s (7) EC
+ 59 3/2- -56.352 81.5 s (5) EC
+ 60 2+ -58.342 23.7 m (4) EC
+ 61 3/2- -61.980 3.333 h (5) EC
+ 62 1+ -62.795 9.74 m (2) EC
+* 63 3/2- -65.577 69.17% (3)
+ 64 1+ -65.421 12.700 h (2) EC 61%,B- 39%
+* 65 3/2- -67.260 30.83% (3)
+ 66 1+ -66.254 5.088 m (11) B-
+ 67 3/2- -67.300 61.83 h (12) B-
+ 68 1+ -65.54 31.1 s (15) B-
+ 68m (6-) -64.82 3.75 m (5) IT 84%,B- 16%
+ 69 3/2- -65.740 2.85 m (15) B-
+ 70 1+ -62.96 4.5 s (10) B-
+ 70m 3-,4-,5- -62.82 47 s (5) B-
+ 71 (3/2-) -62.76 19.5 s (16) B-
+ 72 (1+) -59.9s 6.6 s (1) B-
+ 73 -59.2s 3.9 s (3) B-
+ 74 (1+,3+) -55.8s 1.594 s (10) B-
+ 75 -54.6s 1.224 s (3) B-,BN 3.5%
+ 76m -50.7s 0.641 s (6) B-,BN 3%
+ 76n -50.7s 1.27 s (30) B-
+ 77 -49.1s 0.469 s (8) B-
+ 78 -44.9s 0.342 s (11) B-
+ 79 -42.7s 188 ms (25) B-,BN 55%
+30 Zn Zinc 29
+ 65.39 (2)
+ 7.133 e
+ 419.53
+ 907
+ +2
+ 57 (7/2-) -32.7s 40 ms (10) EC,EP >= 65%
+ 58 0+ -42.29 65 ms (9) EC
+ 59 3/2- -47.26 182.0 ms (18) EC,EP 0.1%
+ 60 0+ -54.18 2.38 m (5) EC
+ 61 3/2- -56.34 89.1 s (2) EC
+ 62 0+ -61.17 9.186 h (13) EC
+ 63 3/2- -62.210 38.47 m (5) EC
+* 64 0+ -66.000 48.6% (3)
+ 65 5/2- -65.908 244.26 d (26) EC
+* 66 0+ -68.897 27.9% (2)
+* 67 5/2- -67.877 4.1% (1)
+* 68 0+ -70.004 18.8% (4)
+ 69 1/2- -68.415 56.4 m (9) B-
+ 69m 9/2+ -67.976 13.76 h (2) IT 99.97%,B- 0.03%
+ 70 0+ -69.560 > 5E+14 y
+ 71 1/2- -67.32 2.45 m (10) B-
+ 71m 9/2+ -67.16 3.96 h (5) B-,IT <= 0.05%
+ 72 0+ -68.126 46.5 h (1) B-
+ 73 (1/2)- -65.41 23.5 s (10) B-
+ 73m (7/2+) -65.21 5.8 s (8) B- ,IT
+ 74 0+ -65.71 95.6 s (12) B-
+ 75 (7/2+) -62.47 10.2 s (2) B-
+ 76 0+ -62.0 5.7 s (3) B-
+ 77 (7/2+) -58.6 2.08 s (5) B-
+ 77m (1/2-) -57.8 1.05 s (10) IT > 50%,B- < 50%
+ 78 0+ -57.2 1.47 s (15) B-
+ 79 (9/2+) -53.4s 0.995 s (19) B-,BN 1.3%
+ 80 0+ -51.8 0.545 s (16) B-,BN 1%
+ 81 -46.1s 0.29 s (5) B-,BN 7.5%
+31 Ga Gallium 26
+ 69.723 (29.6C)
+ 5.904
+ 29.76
+ 2204
+ +3
+ 61 (3/2-) -47.3s 0.15 s (3) EC
+ 62 0+ -52.00 116.12 ms (23) EC
+ 63 3/2-,5/2- -56.69 32.4 s (5) EC
+ 64 0+ -58.835 2.630 m (11) EC
+ 65 3/2- -62.653 15.2 m (2) EC
+ 66 0+ -63.722 9.49 h (7) EC
+ 67 3/2- -66.877 3.2612 d (6) EC
+ 68 1+ -67.083 67.629 m (24) EC
+* 69 3/2- -69.321 60.108% (6)
+ 70 1+ -68.905 21.14 m (3) B- 99.59%,EC 0.41%
+* 71 3/2- -70.135 39.892% (6)
+ 72 3- -68.584 14.10 h (2) B-
+ 72m (0+) -68.464 39.68 ms (13) IT
+ 73 3/2- -69.704 4.86 h (3) B-
+ 74 (3-) -68.05 8.12 m (12) B-
+ 74m (0) -67.99 9.5 s (10) IT 75%,B- < 50%
+ 75 3/2- -68.464 126 s (2) B-
+ 76 (2+,3+) -66.20 32.6 s (6) B-
+ 77 (3/2-) -65.87 13.2 s (2) B-
+ 78 (3+) -63.66 5.09 s (5) B-
+ 79 (3/2-) -62.5 2.847 s (3) B-,BN 0.089%
+ 80 (3) -59.1 1.697 s (11) B-,BN 0.89%
+ 81 (5/2-) -58.0 1.221 s (5) B-,BN 12.3%
+ 82 (1,2,3) -52.9s 0.599 s (2) B-,BN 22.3%
+ 83 -49.5s 0.31 s (1) B-,BN 40%
+ 84 -44.4s 85 ms (10) B- ,BN 70%
+32 Ge Germanium 32
+ 72.61 (2)
+ 5.323 e
+ 938.25
+ 2833
+ +2,+4
+ 61 (3/2-) -33.7s 40 ms (15) EC,EP ~ 80%
+ 62 0+ -42.2s 0.11 s (6) EC ?%
+ 63 -46.9s 0.095 s (+23-20) EC ?%
+ 64 0+ -54.4 63.7 s (25) EC
+ 65 (3/2)- -56.41 30.9 s (5) EC
+ 66 0+ -61.62 2.26 h (5) EC
+ 67 1/2- -62.654 18.9 m (3) EC
+ 68 0+ -66.977 270.82 d (27) EC
+ 69 5/2- -67.094 39.05 h (10) EC
+* 70 0+ -70.561 21.23% (4)
+ 71 1/2- -69.905 11.43 d (3) EC
+ 71m 9/2+ -69.707 20.40 ms (17) IT
+* 72 0+ -72.585 27.66% (3)
+* 73 9/2+ -71.297 7.73% (1)
+ 73m 1/2- -71.230 0.499 s (11) IT
+* 74 0+ -73.422 35.94% (2)
+ 75 1/2- -71.856 82.78 m (4) B-
+ 75m 7/2+ -71.716 47.7 s (5) IT 99.97%,B- 0.03%
+* 76 0+ -73.213 7.44% (2)
+ 77 7/2+ -71.214 11.30 h (1) B-
+ 77m 1/2- -71.054 52.9 s (6) B- 79%,IT 21%
+ 78 0+ -71.862 88.0 m (10) B-
+ 79 (1/2)- -69.49 18.98 s (3) B-
+ 79m (7/2+) -69.30 39.0 s (10) B- 96%,IT 4%
+ 80 0+ -69.45 29.5 s (4) B-
+ 81 (9/2+) -66.3 7.6 s (6) B-
+ 81m (1/2+) -65.6 7.6 s (6) B-
+ 82 0+ -65.5 4.60 s (35) B-
+ 83 (5/2+) -61.0s 1.85 s (6) B-
+ 84 0+ -58.4s 0.947 s (11) B-,BN 10.8%
+ 85 -53.4s 0.54 s (5) B- ,BN 14%
+ 86 0+ -50.0s > 150 NS
+33 As Arsenic 26
+ 74.92160 (2)
+ 5.73 o
+ 817 (subl.)
+ 614 (subl.)>
+ +3,+5,-3
+ 65 -47.1s 0.19 s (+11-7) EC
+ 66 -51.8s 0.10 s (+7-5) EC
+ 67 (5/2-) -56.6 42.5 s (12) EC
+ 68 3 -58.9 151.6 s (8) EC
+ 69 5/2- -63.08 15.2 m (2) EC
+ 70 4(+) -64.34 52.6 m (3) EC
+ 71 5/2- -67.893 65.28 h (15) EC
+ 72 2- -68.229 26.0 h (1) EC
+ 73 3/2- -70.956 80.30 d (6) EC
+ 74 2- -70.86 17.77 d (2) EC 66%,B- 34%
+* 75 3/2- -73.032 100%
+ 76 2- -72.289 1.0778 d (20) B-
+ 77 3/2- -73.916 38.83 h (5) B-
+ 78 2- -72.816 90.7 m (2) B-
+ 79 3/2- -73.636 9.01 m (15) B-
+ 80 1+ -72.12 15.2 s (2) B-
+ 81 3/2- -72.533 33.3 s (8) B-
+ 82 (1+) -70.24 19.1 s (5) B-
+ 82m (5-) -70.24 13.6 s (4) B-
+ 83 (5/2-,3/2- -69.9 13.4 s (3) B-
+ 84 (3)- -66.1s 4.02 s (3) B-,BN 0.28%
+ 85 (3/2-) -63.5s 2.002 s (13) B-,BN 59.4%
+ 86 -59.4s 0.945 s (8) B-,BN 33%
+ 87 (3/2-) -56.3s 0.49 s (4) B-,BN 15.4%
+ 88 -51.6s > 150 NS
+ 89 > 150 NS
+34 Se Selenium 31
+ 78.96 (3)
+ 4.79 p
+ 221 p
+ 685 p
+ +4,+6,-2
+ 65 -32.9s < 50 ms EC
+ 67 -46.5s 107 ms (35) EC,EP
+ 68 0+ -54.1s 35.5 s (7) EC
+ 69 (3/2-) -56.30 27.4 s (2) EC,EP 0.05%
+ 70 0+ -61.9s 41.1 m (3) EC
+ 71 5/2- -63.1s 4.74 m (5) EC
+ 72 0+ -67.89 8.40 d (8) EC
+ 73 9/2+ -68.22 7.15 h (8) EC
+ 73m 3/2- -68.19 39.8 m (13) IT 72.6%,EC 27.4%
+* 74 0+ -72.213 0.89% (2)
+ 75 5/2+ -72.169 119.779 d (4) EC
+* 76 0+ -75.251 9.36% (11)
+* 77 1/2- -74.599 7.63% (6)
+ 77m 7/2+ -74.437 17.36 s (5) IT
+* 78 0+ -77.026 23.78% (9)
+ 79 7/2+ -75.917 6.5E+5 y LE B-
+ 79m 1/2- -75.821 3.92 m (1) IT 99.94%,B- 0.06%
+* 80 0+ -77.759 49.61% (10)
+ 81 1/2- -76.389 18.45 m (12) B-
+ 81m 7/2+ -76.286 57.28 m (2) IT 99.95%,B- 0.05%
+ 82 0+ -77.593 1.1E20 y (+3-1) 2B-
+ 83 9/2+ -75.340 22.3 m (3) B-
+ 83m 1/2- -75.112 70.1 s (4) B-
+ 84 0+ -75.95 3.1 m (1) B-
+ 85 (5/2+) -72.43 31.7 s (9) B-
+ 86 0+ -70.54 15.3 s (9) B-
+ 87 (5/2+) -66.58 5.29 s (11) B-,BN 0.36%
+ 88 0+ -63.87 1.53 s (6) B-,BN 0.99%
+ 89 (5/2+) -59.6s 0.41 s (4) B-,BN 7.8%
+ 90 0+ -56.4s > 150 NS
+ 91 -50.9s 0.27 s (5) B-,BN 21%
+35 Br Bromine 35
+ 79.904
+ 3.12 u
+ -7.2
+ 58.78
+ +1,+5,-1
+ 69? -46.7s < 100 NS P
+ 70 -51.6s 79.1 ms (8) EC
+ 70m -51.6s 2.2 s (2) EC
+ 71 (5/2)- -56.6s 21.4 s (6) EC
+ 72 3+ -59.2 78.6 s (24) EC
+ 72m 1- -59.1 10.6 s (3) IT ~100%,EC
+ 73 1/2- -63.6 3.4 m (2) EC
+ 74 (0-) -65.31 25.4 m (3) EC
+ 74m 4(+) -65.29 46 m (2) EC
+ 75 3/2- -69.14 96.7 m (13) EC
+ 76 1- -70.289 16.2 h (2) EC
+ 76m (4)+ -70.186 1.31 s (2) IT > 99.4%,EC < 0.6%
+ 77 3/2- -73.234 57.036 h (6) EC
+ 77m 9/2+ -73.128 4.28 m (10) IT
+ 78 1+ -73.452 6.46 m (4) EC >= 99.99%,B- <= 0.01
+* 79 3/2- -76.068 50.69% (7)
+ 79m 9/2+ -75.860 4.86 s (4) IT
+ 80 1+ -75.889 17.68 m (2) B- 91.7%,EC 8.3%
+ 80m 5- -75.803 4.4205 h (8) IT
+* 81 3/2- -77.974 49.31% (7)
+ 82 5- -77.496 35.30 h (2) B-
+ 82m 2- -77.450 6.13 m (5) IT 97.6%,B- 2.4%
+ 83 3/2- -79.008 2.40 h (2) B-
+ 84 2- -77.78 31.80 m (8) B-
+ 84m (5-,6-) -77.46 6.0 m (2) B-
+ 85 3/2- -78.61 2.90 m (6) B-
+ 86 (2-) -75.64 55.1 s (4) B-
+ 87 3/2- -73.85 55.60 s (15) B-,BN 2.52%
+ 88 (1,2-) -70.73 16.34 s (8) B-,BN 6.58%
+ 89 (3/2-,5/2- -68.56 4.40 s (3) B-,BN 13.8%
+ 90 -64.61 1.92 s (2) B-,BN 25.2%
+ 91 -61.55 0.541 s (5) B-,BN 20%
+ 92 (2-) -56.62 0.343 s (15) B-,BN 33.1%
+ 93 (5/2-) -53.0s 102 ms B-,BN 77%
+ 94 -48.824C 70 ms (20) B-,BN 30%
+36 Kr Krypton 31
+ 83.80
+ 0.003733
+ -157.36
+ -153.22
+ 0
+ 71 -46.1s 97 ms (9) EC,EP
+ 72 0+ -54.1 17.2 s (3) EC
+ 73 5/2- -56.9 27.0 s (12) EC,EP 0.68%
+ 74 0+ -62.17 11.50 m (11) EC
+ 75 (5/2)+ -64.24 4.3 m (2) EC
+ 76 0+ -68.98 14.8 h (1) EC
+ 77 5/2+ -70.170 74.4 m (6) EC
+ 78 0+ -74.158 2.0E+21 y GE
+ 79 1/2- -74.442 35.04 h (10) EC
+ 79m 7/2+ -74.312 50 s (3) IT
+* 80 0+ -77.893 2.25% (2)
+ 81 7/2+ -77.693 2.29E+5 y (11) EC
+ 81m 1/2- -77.502 13.10 s (3) IT,EC 2.5E-3%
+* 82 0+ -80.588 11.6% (1)
+* 83 9/2+ -79.981 11.5% (1)
+ 83m 1/2- -79.939 1.83 h (2) IT
+* 84 0+ -82.430 57.0% (3)
+ 85 9/2+ -81.478 3934.4 d (14) B-
+ 85m 1/2- -81.173 4.480 h (8) B- 78.6%,IT 21.4%
+* 86 0+ -83.262 17.3% (2)
+ 87 5/2+ -80.706 76.3 m (6) B-
+ 88 0+ -79.69 2.84 h (3) B-
+ 89 (3/2+,5/2+ -76.72 3.15 m (4) B-
+ 90 0+ -74.96 32.32 s (9) B-
+ 91 (5/2+) -71.35 8.57 s (4) B-
+ 92 0+ -68.83 1.840 s (8) B-,BN 0.03%
+ 93 (1/2+) -64.1 1.286 s (10) B-,BN 2.01%
+ 94 0+ -61.2s 0.20 s (1) B-,BN 5.7%
+ 95 -56.1s 0.78 s (3) B-
+ 96 0+ -53.3s > 50 ms
+ 97 > 150 NS B-
+37 Rb Rubidium 36
+ 85.4678 (3)
+ 1.532 c
+ 39.31
+ 688
+ +1
+ 74 (0+) -51.7 64.9 ms (5) EC
+ 75 (3/2-,5/2- -57.220 19.0 s (12) EC
+ 76 1(-) -60.477 36.5 s (6) EC
+ 77 3/2- -64.826 3.78 m (4) EC
+ 78 0(+) -66.934 17.66 m (8) EC
+ 78m 4(-) -66.831 5.74 m (5) EC 90%,IT 10%
+ 79 5/2+ -70.793 22.9 m (5) EC
+ 80 1+ -72.170 33.4 s (7) EC
+ 81 3/2- -75.455 4.576 h (5) EC
+ 81m 9/2+ -75.369 30.5 m (3) IT 97.6%,EC 2.4%
+ 82 1+ -76.187 1.273 m (2) EC
+ 82m 5- -76.118 6.472 h (6) EC,IT < 0.33%
+ 83 5/2- -79.071 86.2 d (1) EC
+ 84 2- -79.748 32.77 d (14) EC 96.2%,B- 3.8%
+ 84m 6- -79.284 20.26 m (4) IT
+* 85 5/2- -82.165 72.165% (20)
+ 86 2- -82.745 18.631 d (18) B- 99.995%,EC 5.2E-3%
+ 86m 6- -82.189 1.017 m (3) IT
+ 87 3/2- -84.593 4.75E10 y (4) B-
+ 88 2- -82.602 17.78 m (11) B-
+ 89 3/2- -81.703 15.15 m (12) B-
+ 90 0- -79.351 158 s (5) B-
+ 90m 3- -79.244 258 s (4) B- 97.4%,IT 2.6%
+ 91 3/2(-) -77.788 58.4 s (4) B-
+ 92 0- -74.81 4.492 s (20) B-,BN 0.01%
+ 93 5/2- -72.70 5.84 s (2) B-,BN 1.35%
+ 94 3(-) -68.53 2.702 s (5) B-,BN 10.01%
+ 95 5/2- -65.86 377.5 ms (8) B-,BN 8.73%
+ 96 2+ -61.23 202.8 ms (33) B-,BN 14%
+ 97 3/2+ -58.38 169.9 ms (7) B-,BN 25.1%
+ 98 (1,0) -54.27 114 ms (5) B-,BN 13.6%,B2N 0.05%
+ 98m (4,5) -54.00 96 ms (3) B-,BN ?%
+ 99 (5/2+) -50.9 50.3 ms (7) B-,BN 20.7%
+ 100 -46.7s 51 ms (8) B-,BN 5.6%
+ 101 -43.6 32 ms (4) B-,BN 31%
+ 102 37 ms (5) B-,BN 18%
+38 Sr Strontium 31
+ 87.62
+ 2.54
+ 777
+ 1382
+ +2
+ 75 -46.6s > 150 NS EC ,EP
+ 76 0+ -54.4s 8.9 s (3) EC
+ 77 (5/2+,7/2+ -58.0 9.0 s (2) EC,EP < 0.25%
+ 78 0+ -63.172 2.5 m (3) EC
+ 79 3/2(-) -65.475 2.25 m (10) EC
+ 80 0+ -70.302 106.3 m (15) EC
+ 81 1/2- -71.524 22.3 m (4) EC
+ 82 0+ -76.007 25.55 d (15) EC
+ 83 7/2+ -76.795 32.41 h (3) EC
+ 83m 1/2- -76.536 4.95 s (12) IT
+* 84 0+ -80.643 0.56% (1)
+ 85 9/2+ -81.100 64.84 d (2) EC
+ 85m 1/2- -80.861 67.63 m (4) IT 86.6%,EC 13.4%
+* 86 0+ -84.519 9.86% (1)
+* 87 9/2+ -84.876 7.00% (1)
+ 87m 1/2- -84.487 2.827 h (1) IT 99.7%,EC 0.3%
+* 88 0+ -87.918 82.58% (1)
+ 89 5/2+ -86.205 50.53 d (7) B-
+ 90 0+ -85.941 28.78 y (4) B-
+ 91 5/2+ -83.649 9.63 h (5) B-
+ 92 0+ -82.92 2.71 h (1) B-
+ 93 5/2+ -80.16 7.423 m (24) B-
+ 94 0+ -78.837 75.3 s (2) B-
+ 95 1/2+ -75.16 23.90 s (14) B-
+ 96 0+ -72.98 1.07 s (1) B-
+ 97 1/2+ -68.80 429 ms (5) B-,BN <= 0.05%
+ 98 0+ -66.61 0.653 s (2) B-,BN 0.25%
+ 99 3/2+ -62.2 0.269 s (1) B-,BN 0.1%
+ 100 0+ -60.2 202 ms (3) B-,BN 0.98%
+ 101 (5/2) -55.4 118 ms (3) B-,BN 2.52%
+ 102 0+ -53.1 69 ms (6) B-,BN 5.5%
+39 Y Yttrium 43
+ 88.90585 (2)
+ 4.469 e
+ 1526
+ 3336
+ +3
+ 78 -52.6s > 150 NS
+ 79 (5/2+) -58.4 14.8 s (6) EC,EP
+ 80 (3,4,5) -61.2s 35 s (2) EC
+ 81 (5/2+) -66.01 72.4 s (13) EC
+ 82 1+ -68.2 9.5 s (3) EC
+ 83 (9/2+) -72.33 7.08 m (6) EC
+ 83m (3/2-) -72.27 2.85 m (2) EC 60%,IT 40%
+ 84 1+ -74.2 4.6 s (2) EC
+ 84m (5-) -73.7 40 m (1) EC
+ 85 (1/2)- -77.85 2.68 h (5) EC
+ 85m 9/2+ -77.83 4.86 h (13) EC,IT <2.0E-3%
+ 86 4- -79.28 14.74 h (2) EC
+ 86m (8+) -79.06 48 m (1) IT 99.31%,EC 0.69%
+ 87 1/2- -83.015 79.8 h (3) EC
+ 87m 9/2+ -82.634 13.37 h (3) IT 98.43%,EC 1.57%
+ 88 4- -84.295 106.65 d (4) EC
+* 89 1/2- -87.702 100%
+ 89m 9/2+ -86.793 16.06 s (4) IT
+ 90 2- -86.487 64.10 h (8) B-
+ 90m 7+ -85.805 3.244 h (5) IT,B- 1.8E-3%
+ 91 1/2- -86.349 58.51 d (6) B-
+ 91m 9/2+ -85.793 49.71 m (4) IT,B- < 1.5%
+ 92 2- -84.831 3.54 h (1) B-
+ 93 1/2- -84.24 10.18 h (8) B-
+ 93m 7/2+ -83.49 0.82 s (4) IT
+ 94 2- -82.348 18.7 m (1) B-
+ 95 1/2- -81.239 10.3 m (1) B-
+ 96 0- -78.35 5.34 s (5) B-
+ 96m (8)+ -78.35 9.6 s (2) B-
+ 97 (1/2-) -76.26 3.75 s (3) B-,BN 0.058%
+ 97m (9/2)+ -75.59 1.17 s (3) B- > 99.3%,IT < 0.7%
+ 97n (27/2-) -72.74 142 ms (8) IT > 80%,B- < 20%
+ 98 (0)- -72.44 0.548 s (2) B-,BN 0.331%
+ 98m (4,5) -72.44 2.0 s (2) B- 90%,IT < 20%
+ 99 (5/2+) -70.20 1.470 s (7) B-,BN 1.9%
+ 100 1-,2- -67.30 735 ms (7) B-,BN 1.02%
+ 100m (3,4,5) -67.30 0.94 s (3) B-
+ 101 (5/2+) -64.91 448 ms (19) B-,BN 1.94%
+ 102 low -61.89 0.30 s (1) B-
+ 102 high -61.89 0.36 s (4) B-
+ 103 -58.6s 0.23 s (3)
+ 104 -54.9s > 150 NS
+ 105 > 150 NS
+40 Zr Zirconium 32
+ 91.224 (2)
+ 6.506 c
+ 1855
+ 4409
+ +4
+ 80 0+ -55.3s > 150 NS
+ 81 -58.9 15 s (5) EC,EP
+ 82 0+ -64.2 32 s (5) EC
+ 83 (1/2-) -66.46 44 s (1) EC,EP
+ 84 0+ -71.5s 25.9 m (8) EC
+ 85 7/2+ -73.2 7.86 m (4) EC
+ 85m (1/2-) -72.9 10.9 s (3) IT <= 92%,EC > 8%
+ 86 0+ -77.81 16.5 h (1) EC
+ 87 (9/2)+ -79.349 1.68 h (1) EC
+ 87m (1/2)- -79.013 14.0 s (2) IT
+ 88 0+ -83.63 83.4 d (3) EC
+ 89 9/2+ -84.869 78.41 h (12) EC
+ 89m 1/2- -84.281 4.18 m (1) IT 93.77%,EC 6.23%
+* 90 0+ -88.769 51.45% (3)
+ 90m 5- -86.450 809.2 ms (20) IT
+* 91 5/2+ -87.893 11.22% (4)
+* 92 0+ -88.456 17.15% (2)
+ 93 5/2+ -87.119 1.53E+6 y (10) B-
+* 94 0+ -87.268 17.38% (4)
+ 95 5/2+ -85.659 64.02 d (5) B-
+ 96 0+ -85.442 3.9E19 y (9) 2B-
+ 97 1/2+ -82.950 16.90 h (5) B-
+ 98 0+ -81.27 30.7 s (4) B-
+ 99 (1/2+) -77.77 2.1 s (1) B-
+ 100 0+ -76.61 7.1 s (4) B-
+ 101 (3/2+) -73.46 2.1 s (3) B-
+ 102 0+ -71.74 2.9 s (2) B-
+ 103 (5/2) -68.4 1.3 s (1) B-
+ 104 0+ -66.3s 1.2 s (3) B-
+ 105 -62.4s ~ 1 s B-
+ 106 0+ -60.2s > 150 NS
+ 107 > 150 NS
+41 Nb Niobium 44
+ 92.90638 (2)
+ 8.57 c
+ 2477
+ 4744
+ +3,+5
+ 82 -53.0s > 150 NS
+ 83 (5/2+) -59.0 4.1 s (3) EC
+ 84 (3+) -61.9s 12 s (3) EC,EP
+ 85 (9/2+) -67.2 20.9 s (7) EC
+ 86 (5+) -69.83 88 s (1) EC
+ 87 (1/2-) -74.18 3.7 m (1) EC
+ 87m (9/2+) -74.18 2.6 m (1) EC
+ 88 (8+) -76.4s 14.5 m (1) EC
+ 88m (4-) -76.4s 7.8 m (1) EC
+ 89 (1/2)- -80.58 1.18 h (10) EC
+ 89m (9/2+) -80.58 1.9 h (2) EC
+ 90 8+ -82.658 14.60 h (5) EC
+ 90m 4- -82.533 18.81 s (6) IT
+ 91 9/2+ -86.639 6.8E+2 y (13) EC
+ 91m 1/2- -86.535 60.86 d (22) IT 93%,EC 7%
+ 92 (7)+ -86.450 3.47E+7 y (24) EC,B- < 0.05%
+ 92m (2)+ -86.315 10.15 d (2) EC
+* 93 9/2+ -87.210 100%
+ 93m 1/2- -87.179 16.13 y (14) IT
+ 94 (6)+ -86.366 2.03E+4 y (16) B-
+ 94m 3+ -86.325 6.263 m (4) IT 99.5%,B- 0.5%
+ 95 9/2+ -86.783 34.975 d (7) B-
+ 95m 1/2- -86.547 86.6 h (8) IT 94.4%,B- 5.6%
+ 96 6+ -85.605 23.35 h (5) B-
+ 97 9/2+ -85.608 72.1 m (7) B-
+ 97m 1/2- -84.865 52.7 s (18) IT
+ 98 1+ -83.527 2.86 s (6) B-
+ 98m (5+) -83.443 51.3 m (4) B- 99.9%,IT < 0.2%
+ 99 9/2+ -82.33 15.0 s (2) B-
+ 99m 1/2- -81.96 2.6 m (2) B- > 96.2%,IT < 3.8%
+ 100 1+ -79.94 1.5 s (2) B-
+ 100m (4+,5+) -79.46 2.99 s (11) B-
+ 101 + -78.94 7.1 s (3) B-
+ 102m 1+ -76.35 1.3 s (2) B-
+ 102n -76.35 4.3 s (4) B-
+ 103 (5/2+) -75.32 1.5 s (2) B-
+ 104 (1+) -72.2 4.8 s (4) B-,BN 0.71%
+ 104m -72.0 0.92 s (4) B-
+ 105 (5/2+) -70.86 2.95 s (6) B-
+ 106 -67.0s 1.02 s (5) B-
+ 107 -65.0s 330 ms (50) B-
+ 108 -61.0s 0.17 s (2)
+ 109 0.6 s (3)
+ 110 > 150 NS
+42 Mo Molybdenum 33
+ 95.94
+ 10.22 c
+ 2623
+ 4639
+ +6
+ 84 0+ -55.8s > 150 NS
+ 85 -59.1s > 150 NS
+ 86 0+ -65.0s 19.6 s (11) EC
+ 87 (7/2+) -67.7 14.5 s (3) EC,EP >0%
+ 88 0+ -72.70 8.0 m (2) EC
+ 89 (9/2+) -75.00 2.04 m (11) EC
+ 89m (1/2-) -74.62 190 ms (15) IT
+ 90 0+ -80.169 5.67 h (5) EC
+ 91 9/2+ -82.21 15.49 m (1) EC
+ 91m 1/2- -81.55 65.0 s (7) IT 50.1%,EC 49.9%
+* 92 0+ -86.806 14.84% (4)
+ 93 5/2+ -86.805 4.0E+3 y (8) EC
+ 93m 21/2+ -84.380 6.85 h (7) IT 99.88%,EC 0.12%
+* 94 0+ -88.411 9.25% (3)
+* 95 5/2+ -87.709 15.92% (5)
+* 96 0+ -88.792 16.68% (5)
+* 97 5/2+ -87.542 9.55% (3)
+* 98 0+ -88.113 24.13% (7)
+ 99 1/2+ -85.967 65.94 h (1) B-
+ 100 0+ -86.185 1.2E19 y (+3-2) 2B-
+ 101 1/2+ -83.512 14.61 m (3) B-
+ 102 0+ -83.56 11.3 m (2) B-
+ 103 (3/2+) -80.85 67.5 s (15) B-
+ 104 0+ -80.33 60 s (2) B-
+ 105 (3/2+) -77.34 35.6 s (16) B-
+ 106 0+ -76.26 8.4 s (5) B-
+ 107 -72.9 3.5 s (5) B-
+ 108 0+ -71.3s 1.09 s (2) B-
+ 109 -67.4s 0.53 s (6) B-
+ 110 0+ -65.7s 0.30 s (4) B-
+ 111 > 150 NS
+ 112 0+ > 150 NS
+ 113 > 150 NS
+43 Tc Technetium 40
+ (98)
+ 11.50 t
+ 2157
+ 4265
+ +4,+6,+7
+ 86 -53.1s > 150 NS
+ 87 -59.1s > 150 NS
+ 88 (6+,7+) -62.6s 6.4 s (8) EC
+ 89 (9/2+) -67.5 12.8 s (9) EC
+ 89m (1/2-) -67.5 12.9 s (8) EC
+ 90 1+ -71.0s 8.7 s (2) EC
+ 90m 4,5,6 -70.5s 49.2 s (4) EC
+ 91 (9/2)+ -76.0 3.14 m (2) EC
+ 91m (1/2)- -75.6 3.3 m (1) EC,IT < 1%
+ 92 (8)+ -78.94 4.23 m (15) EC
+ 93 9/2+ -83.604 2.75 h (5) EC
+ 93m 1/2- -83.212 43.5 m (10) IT 76.7%,EC 23.3%
+ 94 7+ -84.155 293 m (1) EC
+ 94m (2)+ -84.080 52.0 m (10) EC,IT < 0.1%
+ 95 9/2+ -86.018 20.0 h (1) EC
+ 95m 1/2- -85.979 61 d (2) EC 96.12%,IT 3.88%
+ 96 7+ -85.819 4.28 d (7) EC
+ 96m 4+ -85.785 51.5 m (10) IT 98%,EC 2%
+ 97 9/2+ -87.221 2.6E+6 y (4) EC
+ 97m 1/2- -87.124 90.1 d (10) IT,EC < 0.34%
+ 98 (6)+ -86.429 4.2E+6 y (3) B-
+ 99 9/2+ -87.324 2.111E+5 y (12) B-
+ 99m 1/2- -87.181 6.01 h (1) IT,B- 3.7E-3%
+ 100 1+ -86.017 15.8 s (1) B-
+ 101 (9/2)+ -86.34 14.22 m (1) B-
+ 102 1+ -84.568 5.28 s (15) B-
+ 102m (4,5) -84.568 4.35 m (7) B- 98%,IT 2%
+ 103 5/2+ -84.60 54.2 s (8) B-
+ 104 (3+) -82.49 18.3 m (3) B-
+ 105 (5/2+) -82.29 7.6 m (1) B-
+ 106 (1,2) -79.78 35.6 s (6) B-
+ 107 -79.1 21.2 s (2) B-
+ 108 (2+) -75.9 5.17 s (7) B-
+ 109 -74.87s 0.87 s (4) B-
+ 110 -71.4s 0.92 s (3) B-
+ 111 -69.8s 0.30 s (3) B-
+ 112 -65.9s 0.28 s (4) B-
+ 113 -64.0s 130 ms (50) B-
+ 114 > 150 NS
+ 115 > 150 NS
+44 Ru Ruthenium 35
+ 101.07 (2)
+ 12.41 c
+ 2334
+ 4150
+ +3
+ 87 > 1.5 us
+ 88 0+ > 150 NS
+ 90 0+ -65.4s 13 s (5) EC
+ 91 (9/2+) -68.6 9 s (1) EC
+ 91m (1/2-) -68.6 7.6 s (8) EC >0%,EP >0%
+ 92 0+ -74.4s 3.65 m (5) EC
+ 93 (9/2)+ -77.27 59.7 s (6) EC
+ 93m (1/2)- -76.53 10.8 s (3) EC 78%,IT 22%
+ 94 0+ -82.56 51.8 m (6) EC
+ 95 5/2+ -83.45 1.643 h (14) EC
+* 96 0+ -86.067 5.52% (6)
+ 97 5/2+ -86.107 2.9 d (1) EC
+* 98 0+ -88.225 1.88% (6)
+* 99 5/2+ -87.618 12.7% (1)
+*100 0+ -89.22 12.6% (1)
+*101 5/2+ -87.950 17.0% (1)
+ 101 11/2- -87.423 17.5 us (4) IT
+*102 0+ -89.099 31.6% (2)
+ 103 3/2+ -87.260 39.26 d (2) B-
+ 103m 11/2- -87.022 1.69 ms (7) IT
+*104 0+ -88.092 18.7% (2)
+ 105 3/2+ -85.931 4.44 h (2) B-
+ 106 0+ -86.324 373.59 d (15) B-
+ 107 (5/2)+ -83.9 3.75 m (5) B-
+ 108 0+ -83.7 4.55 m (5) B-
+ 109 (5/2+) -80.85 34.5 s (10) B-
+ 110 0+ -80.1 14.6 s (10) B-
+ 111 -76.8s 2.12 s (7) B-
+ 112 0+ -75.9s 1.75 s (7) B-
+ 113 -72.2s 0.80 s (5) B-
+ 114 0+ -70.8s 0.57 s (5) B-
+ 115 -66.8s 0.40 s (10) B-,BN
+ 116 0+ -65.2s > 150 NS
+ 117 > 150 NS
+ 118 0+ > 150 NS
+45 Rh Rhodium 50
+ 102.90550 (2)
+ 12.41 c
+ 1964
+ 3695
+ +3
+ 89 > 1.5 us
+ 90 > 150 NS
+ 91 > 150 NS
+ 92 -63.4s > 150 NS
+ 94m (8+) -72.9s 25.8 s (2) EC
+ 94n (3+) -72.9s 70.6 s (6) EC
+ 95 (9/2)+ -78.3 5.02 m (10) EC
+ 95m (1/2)- -77.8 1.96 m (4) IT 88%,EC 12%
+ 96 (6+) -79.62 9.90 m (10) EC
+ 96m (3+) -79.57 1.51 m (2) IT 60%,EC 40%
+ 97 9/2+ -82.58 30.7 m (6) EC
+ 97m 1/2- -82.32 46.2 m (16) EC 94.4%,IT 5.6%
+ 98 (2)+ -83.17 8.7 m (2) EC
+ 98m (5+) -83.17 3.5 m (3) EC > 0%,IT
+ 99 1/2- -85.51 16.1 d (2) EC
+ 99m 9/2+ -85.45 4.7 h (1) EC > 99.84%,IT < 0.16%
+ 100 1- -85.59 20.8 h (1) EC
+ 100m (5+) -85.59 4.6 m (2) IT ~ 98.3%,EC ~ 1.7%
+ 101 1/2- -87.41 3.3 y (3) EC
+ 101m 9/2+ -87.25 4.34 d (1) EC 93.6%,IT 6.4%
+ 102 (1-,2-) -86.776 207 d (3) EC 80%,B- 20%
+ 102m 6(+) -86.635 ~ 2.9 y EC 99.73%,IT 0.23%
+*103 1/2- -88.023 100%
+ 103m 7/2+ -87.983 56.114 m (9) IT
+ 104 1+ -86.951 42.3 s (4) B- 99.55%,EC 0.45%
+ 104m 5+ -86.822 4.34 m (3) IT 99.87%,B- 0.13%
+ 105 7/2+ -87.848 35.36 h (6) B-
+ 105m 1/2- -87.718 ~ 40 s IT
+ 106 1+ -86.363 29.80 s (8) B-
+ 106m (6)+ -86.226 131 m (2) B-
+ 107 7/2+ -86.86 21.7 m (4) B-
+ 108m 1+ -85.0 16.8 s (5) B-
+ 108n (5+) -85.0 6.0 m (3) B-
+ 109 7/2+ -85.01 80 s (2) B-
+ 110m 1+ -82.9 3.2 s (2) B-
+ 110n (|>4) -82.9 28.5 s (15) B-
+ 111 (7/2+) -82.3s 11 s (1) B-
+ 112m 1+ -79.5s 3.8 s (6) B-
+ 112n |>4 -79.5s 6.8 s (2) B-
+ 113 -78.8s 2.80 s (12) B-
+ 114 (1+) -75.6s 1.85 s (5) B-
+ 114m (|>4) -75.6s 1.85 s (5) B-
+ 115 (7/2+) -74.4 0.99 s (5) B-
+ 116m 1+ -71.1s 0.68 s (6) B-
+ 116n (5,6,7) -71.1s 0.9 s (4) B-
+ 117 (7/2+) -69.5s 0.44 s (4) B-
+ 118 -65.7s > 150 NS
+ 119 -63.9s > 150 NS
+ 120 > 150 NS
+ 121 > 150 NS
+46 Pd Palladium 40
+ 106.42
+ 12.02 c
+ 1554.9
+ 2963
+ +2,+4
+ 91 > 1.5 us
+ 92 0+ > 150 NS
+ 93 -59.050C 60 s (20) EP ?%
+ 94 0+ -66.4s 9.0 s (5) EC
+ 95m (21/2+) -68.2s 13.3 s (3) EC >= 91.3%,IT <= 9.7%
+ 96 0+ -76.2 122 s (2) EC
+ 97 (5/2+) -77.8 3.10 m (9) EC
+ 98 0+ -81.29 17.7 m (3) EC
+ 99 (5/2)+ -82.15 21.4 m (2) EC
+ 100 0+ -85.23 3.63 d (9) EC
+ 101 (5/2+) -85.43 8.47 h (6) EC
+*102 0+ -87.926 1.02% (1)
+ 103 5/2+ -87.480 16.991 d (19) EC
+*104 0+ -89.392 11.14% (8)
+*105 5/2+ -88.414 22.33% (8)
+*106 0+ -89.905 27.33% (3)
+ 107 5/2+ -88.372 6.5E+6 y (3) B-
+ 107m 11/2- -88.157 21.3 s (5) IT
+*108 0+ -89.521 26.46% (9)
+ 109 5/2+ -87.603 13.7012 h (24) B-
+ 109m 11/2- -87.414 4.696 m (3) IT
+*110 0+ -88.35 11.72% (9)
+ 111 5/2+ -86.03 23.4 m (2) B-
+ 111m 11/2- -85.86 5.5 h (1) IT 73%,B- 27%
+ 112 0+ -86.34 21.03 h (5) B-
+ 113 (5/2)+ -83.69 93 s (5) B-
+ 113m (9/2-) -83.69 0.4 s (1) IT
+ 113? -83.69 100 s GE
+ 114 0+ -83.49 2.42 m (6) B-
+ 115 (5/2+) -80.40 25 s (2) B-
+ 115m (11/2-) -80.31 50 s (3) B- 92%,IT 8%
+ 116 0+ -79.95 11.8 s (4) B-
+ 117 (5/2+) -76.5s 4.3 s (3) B-
+ 117m (11/2-) -76.3s 19.1 ms (7) IT
+ 118 0+ -75.5 1.9 s (1) B-
+ 119 -72.0s 0.92 s (13) B-
+ 120 0+ -70.8s 0.5 s (1) B-
+ 121 -66.9s > 150 NS
+ 122 0+ > 150 NS
+ 123 > 150 NS
+47 Ag Silver 56
+ 107.8682 (2)
+ 10.50 c
+ 961.78
+ 2162
+ +1
+ 94 10 ms
+ 94m (9+) 0.42 s (5) EC ,EP
+ 95 2.0 s (1) EC ,EP
+ 96 (8+,9+) -64.6s 5.1 s (4) EC,EP 8%
+ 97 (9/2+) -70.8s 19 s (2) EC
+ 98 (5+) -72.9 46.7 s (9) EC
+ 99 (9/2)+ -76.7 124 s (3) EC
+ 99m (1/2-) -76.2 10.5 s (5) IT
+ 100 (5)+ -78.15 2.01 m (9) EC
+ 100m (2)+ -78.14 2.24 m (13) EC ,IT
+ 101 9/2+ -81.2 11.1 m (3) EC
+ 101m 1/2- -81.0 3.10 s (10) IT
+ 102 5+ -82.00 12.9 m (3) EC
+ 102m 2+ -81.99 7.7 m (5) EC 51%,IT 49%
+ 103 7/2+ -84.79 65.7 m (7) EC
+ 103m 1/2- -84.66 5.7 s (3) IT
+ 104 5+ -85.113 69.2 m (10) EC
+ 104m 2+ -85.106 33.5 m (20) EC 99.93%,IT < 0.07%
+ 105 1/2- -87.07 41.29 d (7) EC
+ 105m 7/2+ -87.04 7.23 m (16) IT 99.66%,EC 0.34%
+ 106 1+ -86.939 23.96 m (4) EC 99.5%,B- < 1%
+ 106m 6+ -86.849 8.28 d (2) EC
+*107 1/2- -88.405 51.839% (7)
+ 107m 7/2+ -88.312 44.3 s (2) IT
+ 108 1+ -87.603 2.37 m (1) B- 97.15%,EC 2.85%
+ 108m 6+ -87.494 418 y (21) EC 91.3%,IT 8.7%
+*109 1/2- -88.719 48.161% (7)
+ 109m 7/2+ -88.631 39.6 s (2) IT
+ 110 1+ -87.457 24.6 s (2) B- 99.7%,EC 0.3%
+ 110m 6+ -87.339 249.79 d (20) B- 98.64%,IT 1.36%
+ 111 1/2- -88.217 7.45 d (1) B-
+ 111m 7/2+ -88.157 64.8 s (8) IT 99.3%,B- 0.7%
+ 112 2(-) -86.62 3.130 h (9) B-
+ 113 1/2- -87.03 5.37 h (5) B-
+ 113m 7/2+ -86.99 68.7 s (16) IT 64%,B- 36%
+ 114 1+ -84.94 4.6 s (1) B-
+ 114m (|<6+) -84.75 1.5 ms (5) IT
+ 115 1/2- -84.99 20.0 m (5) B-
+ 115m 7/2+ -84.95 18.0 s (7) B- 79%,IT 21%
+ 116 (2)- -82.56 2.68 m (10) B-
+ 116m (5+) -82.48 8.6 s (3) B- 94%,IT 6%
+ 117 (1/2-) -82.24 72.8 s (+20-7) B- ~100%
+ 117m (7/2+) -82.21 5.34 s (5) B- 94%,IT 6%
+ 118 1(-) -79.6 3.76 s (15) B-
+ 118m 4(+) -79.5 2.0 s (2) B- 59%,IT 41%
+ 119n (7/2+) -78.56 2.1 s (1) B-
+ 119m (1/2-) -78.56 6.0 s (5) B-
+ 120 3+ -75.8 1.23 s (3) B-,BN <=0.003%
+ 120m 6- -75.6 0.32 s (4) B- ~ 63%,IT ~ 37%
+ 121 (7/2+) -74.5 0.78 s (1) B-,BN 0.08%
+ 122 (3+) -71.4s 0.48 s (8) B-,BN 0.186%
+ 123 (7/2+) -70.0s 0.309 s (15) B-,BN 0.55%
+ 124 (1,2,3)+ -66.6s 0.54 s (8) B- ,BN >=0.1%
+ 125 156 ms (7)
+ 126 97 ms (8)
+ 127 109 ms (15)
+48 Cd Cadmium 42
+ 112.411 (8)
+ 8.65 c
+ 321.07
+ 767
+ +2
+ 97m -60.386C 3 s (+4-2) EC ,EP
+ 98 0+ -67.5s 9.2 s (3) EC
+ 99 (5/2+) -69.9s 16 s (3) EC,EP 0.17%,EA <1.0E-4%
+ 100 0+ -74.3 49.1 s (5) EC
+ 101 (5/2+) -75.7 1.2 m (2) EC
+ 102 0+ -79.42 5.5 m (5) EC
+ 103 (5/2)+ -80.65 7.3 m (1) EC
+ 104 0+ -83.976 57.7 m (10) EC
+ 105 5/2+ -84.33 55.5 m (4) EC
+*106 0+ -87.134 1.25% (4)
+ 107 5/2+ -86.988 6.50 h (2) EC
+*108 0+ -89.253 0.89% (2)
+ 109 5/2+ -88.506 462.6 d (4) EC
+*110 0+ -90.349 12.49% (12)
+*111 1/2+ -89.254 12.80% (8)
+ 111m 11/2- -88.858 48.54 m (5) IT
+*112 0+ -90.581 24.13% (14)
+ 113 1/2+ -89.05 9.3E+15 y (19) B-
+ 113m 11/2- -88.786 14.1 y (5) B- 99.86%,IT 0.14%
+*114 0+ -90.021 28.73% (28)
+ 115 1/2+ -88.091 53.46 h (10) B-
+ 115m 11/2- -87.91 44.6 d (3) B-
+*116 0+ -88.719 7.49% (12)
+ 117 1/2+ -86.425 2.49 h (4) B-
+ 117m (11/2)- -86.289 3.36 h (5) B-
+ 118 0+ -86.71 50.3 m (2) B-
+ 119 3/2+ -83.91 2.69 m (2) B-
+ 119m (11/2-) -83.76 2.20 m (2) B-
+ 120 0+ -83.97 50.80 s (21) B-
+ 121 (3/2+) -80.9 13.5 s (3) B-
+ 121m (11/2-) -80.7 8.3 s (8) B-
+ 122 0+ -80.6s 5.24 s (3) B-
+ 123 (3/2)+ -77.31 2.10 s (2) B-
+ 123m (11/2-) -77.00 1.82 s (3) B- ,IT
+ 124 0+ -76.71 1.24 s (5) B-
+ 125 (3/2+) -73.32 0.65 s (2) B-
+ 125m (11/2-) -73.27 0.57 s (9) B-
+ 126 0+ -72.33 0.506 s (15) B-
+ 127 (3/2+) -68.53 0.43 s (3) B-
+ 128 0+ -67.3 0.34 s (3) B-
+ 129 0.27 s (4) B-
+ 130 0+ -64.359C 0.20 s (4) B-,BN ~ 4%
+49 In Indium 72
+ 114.818 (3)
+ 7.31 c
+ 156.60
+ 2072
+ +3
+ 98 > 1.5 us
+ 100 -63.7s 6.1 s (9) EC ,EP
+ 101 -68.4s 16 s (3) EC ~100%,EP
+ 102 (5) -70.5 24 s (4) EC
+ 103 (9/2)+ -74.60 65 s (7) EC
+ 104 (6+) -76.1 1.8 m (2) EC
+ 104m (3+) -76.0 15.7 s (5) IT 80%,EC 20%
+ 105 (9/2+) -79.48 5.07 m (7) EC
+ 105m (1/2-) -78.81 48 s (6) IT
+ 106 7+ -80.61 6.2 m (1) EC
+ 106m (3+) -80.58 5.2 m (1) EC
+ 107 9/2+ -83.56 32.4 m (3) EC
+ 107m 1/2- -82.88 50.4 s (6) IT
+ 108 7+ -84.11 58.0 m (12) EC
+ 108m 2+ -84.08 39.6 m (7) EC
+ 109 9/2+ -86.485 4.2 h (1) EC
+ 109m 1/2- -85.835 1.34 m (7) IT
+ 109n (19/2+) -84.383 0.21 s (1) IT
+ 110 7+ -86.47 4.9 h (1) EC
+ 110m 2+ -86.41 69.1 m (5) EC
+ 111 9/2+ -88.388 2.8047 d (5) EC
+ 111m 1/2- -87.851 7.7 m (2) IT
+ 112 1+ -87.994 14.97 m (10) EC 56%,B- 44%
+ 112m 4+ -87.837 20.56 m (6) IT
+*113 9/2+ -89.365 4.29% (2)
+ 113m 1/2- -88.973 1.6582 h (6) IT
+ 114 1+ -88.568 71.9 s (1) B- 99.5%,EC 0.5%
+ 114m 5+ -88.378 49.51 d (1) IT 95.6%,EC 4.4%
+ 114n 8- -88.066 43.1 ms (6) IT
+ 115 9/2+ -89.536 4.41E+14 y (25) B-
+ 115m 1/2- -89.200 4.486 h (4) IT 95%,B- 5%
+ 116 1+ -88.249 14.10 s (3) B- 99.97%,EC < 0.06%
+ 116m 5+ -88.122 54.29 m (17) B-
+ 116n 8- -87.959 2.18 s (4) IT
+ 117 9/2+ -88.941 43.2 m (3) B-
+ 117m 1/2- -88.626 116.2 m (3) B- 52.9%,IT 47.1%
+ 118 1+ -87.228 5.0 s (5) B-
+ 118m 5+ -87.168 4.45 m (5) B-
+ 118n 8- -87.028 8.5 s (3) IT 98.6%,B- 1.4%
+ 119 9/2+ -87.702 2.4 m (1) B-
+ 119m 1/2- -87.391 18.0 m (3) B- 94.4%,IT 5.6%
+ 120 1+ -85.73 3.08 s (8) B-
+ 120a (3,4,5)+ -85.73 46.2 s (8) B-
+ 120b (8-) -85.73 47.3 s (5) B-
+ 121 9/2+ -85.84 23.1 s (6) B-
+ 121m 1/2- -85.52 3.88 m (10) B- 98.8%,IT 1.2%
+ 122 1+ -83.58 1.5 s (3) B-
+ 122m 5+ -83.58 10.3 s (6) B-
+ 122n 8- -83.38 10.8 s (4) B-
+ 123 9/2+ -83.43 5.98 s (6) B-
+ 123m 1/2- -83.10 47.8 s (5) B-
+ 124 3+ -80.88 3.17 s (5) B-
+ 124m (8-) -80.69 3.4 s (5) B-
+ 125 9/2(+) -80.48 2.36 s (4) B-
+ 125m 1/2(-) -80.12 12.2 s (2) B-
+ 126 3(+) -77.81 1.60 s (10) B-
+ 126m 7,8,9 -77.71 1.64 s (5) B-
+ 127 (9/2+) -76.99 1.09 s (1) B-,BN <= 0.03%
+ 127m (1/2-) -76.53 3.66 s (4) B-,BN 0.69%
+ 128 (3)+ -74.36 0.84 s (6) B-
+ 128 (3+) -74.36 0.84 s (6) BN <= 0.038%
+ 128m (8)- -74.04 0.72 s (1) B-,BN <= 0.038%
+ 129 (9/2+) -73.0 0.61 s (1) B-,BN 0.23%
+ 129m (1/2-) -72.6 1.23 s (3) B- ~100%,BN 3.6%
+ 130 1(-) -69.99 0.26 s (1) B-,BN 1.01%
+ 130m (10-) -69.94 0.55 s (1) B-,BN <= 1.65%
+ 130n (5+) -69.59 0.542 s (9) B-,BN <= 1.65%
+ 131 (9/2+) -68.20 0.28 s (3) B-,BN <= 2%
+ 131m (1/2-) -67.84 0.35 s (5) B- >= 99.98%,BN <= 2%
+ 131n (21/2+) -63.93 0.32 s (6) B- > 99%,IT < 1%
+ 132 (7-) -63.0 0.201 s (13) B-,BN 6.2%
+ 133 -60.328C 180 ms (20) B-,BN
+50 Sn Tin 49
+ 118.710 (7)
+ 5.75 q
+ 231.93
+ 2602
+ +2,+4
+ 100 0+ -56.5s 1.0 s (+8-3) EC
+ 101 -59.6s 3 s (1) EC ,EP
+ 102 0+ -64.7s > 200 NS
+ 103 -66.9s 7 s (3) EC
+ 104 0+ -71.6 20.8 s (5) EC
+ 105 -73.23 31 s (6) EC,EP
+ 106 0+ -77.43 115 s (5) EC
+ 107 (5/2+) -78.56 2.90 m (5) EC
+ 108 0+ -82.01 10.30 m (8) EC
+ 109 5/2(+) -82.635 18.0 m (2) EC
+ 110 0+ -85.83 4.11 h (10) EC
+ 111 7/2+ -85.943 35.3 m (6) EC
+*112 0+ -88.658 0.97% (1)
+ 113 1/2+ -88.33 115.09 d (4) EC
+ 113m 7/2+ -88.252 21.4 m (4) IT 91.1%,EC 8.9%
+*114 0+ -90.557 0.65% (1)
+*115 1/2+ -90.031 0.34% (1)
+*116 0+ -91.524 14.54% (11)
+*117 1/2+ -90.397 7.68% (7)
+ 117m 11/2- -90.082 13.60 d (4) IT
+*118 0+ -91.652 24.22% (11)
+*119 1/2+ -90.066 8.58% (4)
+ 119m 11/2- -89.976 293.1 d (7) IT
+*120 0+ -91.102 32.59% (10)
+ 121 3/2+ -89.201 27.06 h (4) B-
+ 121m 11/2- -89.195 55 y (5) IT 77.6%,B- 22.4%
+*122 0+ -89.944 4.63% (3)
+ 123 11/2- -87.819 129.2 d (4) B-
+ 123m 3/2+ -87.794 40.06 m (1) B-
+*124 0+ -88.236 5.79% (5)
+ 125 11/2- -85.898 9.64 d (3) B-
+ 125m 3/2+ -85.870 9.52 m (5) B-
+ 126 0+ -86.02 ~ 1E+5 y B-
+ 127 (11/2-) -83.51 2.10 h (4) B-
+ 127m (3/2+) -83.50 4.13 m (3) B-
+ 128 0+ -83.34 59.07 m (14) B-
+ 128m (7-) -81.24 6.5 s (5) IT
+ 129 (3/2+) -80.6 2.23 m (4) B-
+ 129m (11/2-) -80.6 6.9 m (1) B- ~100%,IT 0.0002%
+ 130 0+ -80.24 3.72 m (4) B-
+ 130m (7-) -78.30 1.7 m (1) B-
+ 131 (3/2+) -77.38 56.0 s (5) B-
+ 131m (11/2-) -77.14 58.4 s (5) B-,IT <=4.0E-4%
+ 132 0+ -76.62 39.7 s (5) B-
+ 133 (7/2-) -71.1 1.20 s (5) B-,BN 0.0294%
+ 134 0+ -67.2s 1.12 s (8) B-,BN 17%
+ 135 > 150 NS
+ 136 0+ > 150 NS
+ 137 > 150 NS
+51 Sb Antimony 49
+ 121.760
+ 6.691 c
+ 630.63
+ 1587
+ +3,+5,-3
+ 103 > 1.5 us
+ 104 -59.0s 0.52 s (+18-13) EC
+ 105 -63.9s 1.3 s (2) EC
+ 108 4+ -72.5s 7.0 s (5) EC
+ 109 (5/2+) -76.25 17.0 s (7) EC
+ 110 3+ -77.5s 23.0 s (4) EC
+ 111 (5/2+) -80.8s 75 s (1) EC
+ 112 3+ -81.60 51.4 s (10) EC
+ 113 5/2+ -84.42 6.67 m (7) EC
+ 114 3+ -84.7 3.49 m (3) EC
+ 115 5/2+ -87.00 32.1 m (3) EC
+ 116 3+ -86.816 15.8 m (8) EC
+ 116m 8- -86.433 60.3 m (6) EC
+ 117 5/2+ -88.640 2.80 h (1) EC
+ 118 1+ -87.995 3.6 m (1) EC
+ 118m 8- -87.745 5.00 h (2) EC
+ 119 5/2+ -89.472 38.19 h (22) EC
+ 120 1+ -88.421 15.89 m (4) EC
+ 120m 8- -88.421 5.76 d (2) EC
+*121 5/2+ -89.589 57.21% (5)
+ 122 2- -88.324 2.7238 d (2) B- 97.59%,EC 2.41%
+ 122m (5)+ -88.187 0.53 ms (3) IT
+ 122n (8)- -88.160 4.191 m (3) IT
+*123 7/2+ -89.222 42.79% (5)
+ 124 3- -87.618 60.20 d (3) B-
+ 124m 5+ -87.607 93 s (5) IT 75%,B- 25%
+ 124n 8- -87.581 20.2 m (2) IT
+ 125 7/2+ -88.262 2.7582 y (11) B-
+ 126 (8)- -86.40 12.46 d (3) B-
+ 126m (5)+ -86.38 19.15 m (8) B- 86%,IT 14%
+ 126n (3)- -86.36 ~ 11 s
+ 127 7/2+ -86.709 3.85 d (5) B-
+ 128 8- -84.61 9.01 h (3) B-
+ 128m 5+ -84.61 10.4 m (2) B- 96.4%,IT 3.6%
+ 129 7/2+ -84.63 4.40 h (1) B-
+ 129m (19/2-) -82.77 17.7 m (1) B- 85%,IT 15%
+ 130 (8-) -82.39 39.5 m (8) B-
+ 130m (5)+ -82.39 6.3 m (2) B-
+ 131 (7/2+) -82.02 23.03 m (4) B-
+ 132 (4+) -79.92 2.79 m (5) B-
+ 132m (8-) -79.92 4.10 m (5) B-
+ 133 (7/2+) -78.96 2.5 m (1) B-
+ 134m (0-) -74.0 0.78 s (6) B-
+ 134n (7-) -74.0 10.22 s (9) B-,BN 0.091%
+ 135 (7/2+) -69.7 1.662 s (10) B-,BN 17.6%
+ 136 -65.1s 0.82 s (2) B-,BN 24%
+ 137 > 150 NS
+ 138 > 150 NS
+ 139 > 150 NS
+52 Te Tellurium 47
+ 127.60 (3)
+ 6.24 c
+ 449.51
+ 988
+ +4,+6,-2
+ 106 0+ -58.0s 60 us (+30-10) A
+ 107 -60.5s 3.1 ms (1) A 70%,EC 30%
+ 108 0+ -65.7 2.1 s (1) EC 51%,A 49%
+ 109 -67.58 4.6 s (3) EC 96%,A 4%
+ 110 0+ -72.28 18.6 s (8) EC ~100%,A ~3.0E-3%
+ 111 -73.47 19.3 s (4) EC,EP
+ 112 0+ -77.3 2.0 m (2) EC
+ 113 (7/2+) -78.3s 1.7 m (2) EC
+ 114 0+ -81.9s 15.2 m (7) EC
+ 115 7/2+ -82.4 5.8 m (2) EC
+ 115m (1/2)+ -82.3 6.7 m (4) EC,IT
+ 116 0+ -85.32 2.49 h (4) EC
+ 117 1/2+ -85.11 62 m (2) EC
+ 117m (11/2-) -84.81 103 ms (3) IT
+ 118 0+ -87.72 6.00 d (2) EC
+ 119 1/2+ -87.179 16.03 h (5) EC
+ 119m 11/2- -86.918 4.70 d (4) EC,IT 8.0E-3%
+*120 0+ -89.40 0.096% (2)
+ 121 1/2+ -88.55 16.78 d (35) EC
+ 121m 11/2- -88.26 154 d (7) IT 88.6%,EC 11.4%
+*122 0+ -90.303 2.603% (4)
+ 123 1/2+ -89.171 > 1E+13 y EC
+ 123m 11/2- -88.923 119.7 d (1) IT
+*124 0+ -90.524 4.816% (6)
+*125 1/2+ -89.028 7.139% (6)
+ 125m 11/2- -88.883 57.40 d (15) IT
+*126 0+ -90.071 18.952% (11)
+ 127 3/2+ -88.290 9.35 h (7) B-
+ 127m 11/2- -88.202 109 d (2) IT 97.6%,B- 2.4%
+ 128 0+ -88.994 7.7E24 y (4) 2B-
+ 129 3/2+ -87.005 69.6 m (3) B-
+ 129m 11/2- -86.899 33.6 d (1) IT 64%,B- 36%
+ 130 0+ -87.353 2.7E+21 y (1) 2B-
+ 131 3/2+ -85.211 25.0 m (1) B-
+ 131m 11/2- -85.029 30 h (2) B- 77.8%,IT 22.2%
+ 132 0+ -85.21 3.204 d (13) B-
+ 133 (3/2+) -82.96 12.5 m (3) B-
+ 133m (11/2-) -82.63 55.4 m (4) B- 82.5%,IT 17.5%
+ 134 0+ -82.4 41.8 m (8) B-
+ 135 (7/2-) -77.83 19.0 s (2) B-
+ 136 0+ -74.42 17.5 s (2) B-,BN 1.3%
+ 137 (7/2-) -69.6 2.49 s (5) B-,BN 2.69%
+ 138 0+ -65.9s 1.4 s (4) B-,BN 6.3%
+ 139 > 150 NS
+ 140 0+ > 150 NS
+ 141 > 150 NS
+ 142 0+ > 150 NS
+53 I Iodine 45
+ 126.90447 (3)
+ 4.93 v
+ 113.7
+ 184.4
+ +1,+5,+7,-1
+ 108 -52.6s 36 ms (6) A 91%
+ 109 -57.6 100 us (5) P
+ 110 -60.3s 0.65 s (2) EC 83%,A 17%,EP 11%
+ 111 (5/2+) -65.0s 2.5 s (2) EC 99.9%,A ~ 0.1%
+ 112 -67.1s 3.42 s (11) EC,A ~0.0012%
+ 113 5/2+ -71.12 6.6 s (2) EC,A 3.3E-7%
+ 114 (1+) -72.8s 2.1 s (2) EC,EP
+ 114m (7) -72.5s 6.2 s IT
+ 115 (5/2+) -76.4s 1.3 m (2) EC
+ 116 1+ -77.6 2.91 s (15) EC
+ 117 (5/2)+ -80.45 2.22 m (4) EC
+ 118 2- -80.67 13.7 m (5) EC
+ 118m (7-) -80.57 8.5 m (5) EC,IT > 0%
+ 119 5/2+ -83.67 19.1 m (4) EC
+ 120 2- -83.78 81.0 m (6) EC
+ 120m >3 -83.78 53 m (4) EC
+ 121 5/2+ -86.28 2.12 h (1) EC
+ 122 1+ -86.069 3.63 m (6) EC
+ 123 5/2+ -87.929 13.27 h (8) EC
+ 124 2- -87.364 4.1760 d (3) EC
+ 125 5/2+ -88.842 59.408 d (8) EC
+ 126 2- -87.916 13.11 d (5) EC 56.3%,B- 43.7%
+*127 5/2+ -88.988 100%
+ 128 1+ -87.743 24.99 m (2) B- 93.1%,EC 6.9%
+ 129 7/2+ -88.503 1.57E7 y (4) B-
+ 130 5+ -86.932 12.36 h (3) B-
+ 130m 2+ -86.892 9.0 m (1) IT 84%,B- 16%
+ 131 7/2+ -87.444 8.02070 d (11) B-
+ 132 4+ -85.70 2.295 h (13) B-
+ 132m (8-) -85.58 1.387 h (15) IT 86%,B- 14%
+ 133 7/2+ -85.88 20.8 h (1) B-
+ 133m (19/2-) -84.24 9 s (2) IT
+ 134 (4)+ -83.95 52.5 m (2) B-
+ 134m (8)- -83.64 3.60 m (10) IT 97.7%,B- 2.3%
+ 135 7/2+ -83.79 6.57 h (2) B-
+ 136 (1-) -79.50 83.4 s (10) B-
+ 136m (6-) -78.86 46.9 s (10) B-
+ 137 (7/2+) -76.50 24.5 s (2) B-,BN 6.97%
+ 138 (2-) -72.30 6.49 s (7) B-,BN 5.5%
+ 139 (7/2+) -68.84 2.280 s (11) B-,BN 10%
+ 140 (3) -64.2s 0.86 s (4) B-,BN 9.3%
+ 141 -60.5s 0.43 s (2) B-,BN 22%
+ 142 ~ 0.2 s B-
+ 143 > 150 NS
+ 144 > 150 NS
+54 Xe Xenon 46
+ 131.29 (2)
+ 0.005887
+ -111.75
+ -108.04
+ 0
+ 110 0+ -51.7s A
+ 111 -54.4s 0.74 s (20) A
+ 112 0+ -59.9 2.7 s (8) EC 99.16%,A 0.84%
+ 113 -62.06 2.74 s (8) EC 99.97%,EP 4.2%
+ 114 0+ -66.9s 10.0 s (4) EC
+ 115 (5/2+) -68.4s 18 s (4) EC,EP
+ 116 0+ -72.9s 59 s (2) EC
+ 117 5/2(+) -74.0 61 s (2) EC,EP 2.9E-3%
+ 118 0+ -78 3.8 m (9) EC
+ 119 (5/2+) -78.7 5.8 m (3) EC
+ 120 0+ -81.82 40 m (1) EC
+ 121 5/2(+) -82.55 40.1 m (20) EC
+ 122 0+ -85.17 20.1 h (1) EC
+ 123 (1/2)+ -85.25 2.08 h (2) EC
+*124 0+ -87.658 0.10% (1)
+ 125 (1/2)+ -87.190 16.9 h (2) EC
+ 125m (9/2)- -86.937 57 s (1) IT
+*126 0+ -89.174 0.09% (1)
+ 127 1/2+ -88.325 36.3446 d (28) EC
+ 127m 9/2- -88.028 69.2 s (9) IT
+*128 0+ -89.861 1.91% (3)
+*129 1/2+ -88.697 26.4% (6)
+ 129m 11/2- -88.461 8.88 d (2) IT
+*130 0+ -89.881 4.1% (1)
+*131 3/2+ -88.415 21.2% (4)
+ 131m 11/2- -88.251 11.934 d (21) IT
+*132 0+ -89.279 26.9% (5)
+ 132m (10+) -86.527 8.39 ms (11) IT
+ 133 3/2+ -87.648 5.2475 d (5) B-
+ 133m 11/2- -87.415 2.19 d (1) IT
+*134 0+ -88.124 10.4% (2)
+ 134m 7- -86.159 290 ms (17) IT
+ 135 3/2+ -86.435 9.14 h (2) B-
+ 135m 11/2- -85.908 15.29 m (5) IT,B- 0.004%
+ 136 0+ -86.424 > 9.3E+19 y 2B- ?%
+ 137 7/2- -82.378 3.818 m (13) B-
+ 138 0+ -80.12 14.08 m (8) B-
+ 139 3/2- -75.65 39.68 s (14) B-
+ 140 0+ -73.00 13.60 s (10) B-
+ 141 5/2+ -68.32 1.73 s (1) B-,BN 0.043%
+ 142 0+ -65.5 1.24 s (2) B-,BN 0.41%
+ 143 5/2- -60.4s 0.30 s (3) B-
+ 144 0+ -57.3s 1.15 s (20) B-
+ 145 0.9 s (3) B- ,BN
+ 146 0+ -52.022C > 150 NS
+ 147 -52.022C > 150 NS
+55 Cs Cesium 56
+ 132.90545 (2)
+ 1.873 c
+ 28.44
+ 671
+ +1
+ 112 -46.3s 0.5 ms (1) P ?%
+ 113 -51.7 33 us (7) P ~100%
+ 114 (1+) -54.6s 0.57 s (2) EC ~100%,EP 7%
+ 115 -59.7s 1.4 s (8) EC,EP ~ 0.07%
+ 116m (1+) -62.4 0.70 s (4) EC,EA > 0%,EP > 0%
+ 116n |>5+ -62.4 3.85 s (13) EC,EA > 0%,EP > 0%
+ 117m -66.48 6.5 s (4) EC
+ 117n -66.48 8.4 s (6) EC
+ 118 2 -68.43 14 s (2) EC,EP < 0.04%
+ 118m 6,7,8 -68.43 17 s (3) EC,EP < 0.04%
+ 119 9/2+ -72.34 43.0 s (2) EC
+ 119m 3/2(+) -72.34 30.4 s (1) EC
+ 120 high -73.90 57 s (6) EC,EP <=1.0E-5%
+ 120 2 -73.90 64 s (3) EC
+ 121 3/2(+) -77.15 128 s (4) EC
+ 121m 9/2(+) -77.08 122 s (3) EC 83%,IT 17%
+ 122 1+ -78.12 21.2 s (2) EC
+ 122m 8- -78.04 3.70 m (11) EC
+ 122n (5)- -77.99 0.36 s (2) IT
+ 123 1/2+ -81.05 5.87 m (5) EC
+ 123m (11/2)- -80.90 1.64 s (12) IT
+ 124 1+ -81.74 30.9 s (5) EC
+ 124m (7)+ -81.28 6.3 s (2) IT
+ 125 (1/2+) -84.098 45 m (1) EC
+ 126 1+ -84.35 1.63 m (3) EC
+ 127 1/2(+) -86.245 6.25 h (10) EC
+ 128 1+ -85.931 3.66 m (2) EC
+ 129 1/2+ -87.502 32.06 h (6) EC
+ 130 1+ -86.898 29.21 m (4) EC 98.4%,B- 1.6%
+ 130m 5- -86.735 3.46 m (6) IT 99.84%,EC 0.16%
+ 131 5/2+ -88.063 9.689 d (16) EC
+ 132 2+ -87.160 6.479 d (7) EC 98.13%,B- 1.87%
+*133 7/2+ -88.075 100%
+ 134 4+ -86.896 2.0648 y (10) B-,EC 3.0E-4%
+ 134m 8- -86.757 2.903 h (8) IT
+ 135 7/2+ -87.586 2.3E+6 y (3) B-
+ 135m 19/2- -85.953 53 m (2) IT
+ 136 8- -86.343 19 s (2) B- ,IT > 0%
+ 136 5+ -86.343 13.16 d (3) B-
+ 137 7/2+ -86.550 30.07 y (3) B-
+ 138 3- -82.893 33.41 m (18) B-
+ 138m 6- -82.813 2.91 m (8) IT 81%,B- 19%
+ 139 7/2+ -80.706 9.27 m (5) B-
+ 140 1- -77.06 63.7 s (3) B-
+ 141 7/2+ -74.47 24.94 s (6) B-,BN 0.035%
+ 142 0- -70.52 1.70 s (2) B-,BN 0.091%
+ 143 3/2+ -67.71 1.78 s (1) B-,BN 1.62%
+ 144 1 -63.32 1.01 s (1) B-,BN 3.2%
+ 144m (|>4) -63.32 < 1 s B-
+ 145 3/2+ -60.16 0.594 s (13) B-,BN 14.3%
+ 146 1- -55.66 0.321 s (2) B-,BN 14.2%
+ 147 (3/2+) -52.2 0.235 s (3) B-,BN 28.5%
+ 148 -47.5 140 ms (12) B-,BN 25.1%
+ 149 -44.2s > 50 ms
+ 150 > 50 ms
+ 151 > 50 ms
+56 Ba Barium 46
+ 137.327 (7)
+ 3.5 c
+ 727
+ 1897
+ +2
+ 114 0+ 0.4 s (+3-2) EC ,A <0.11%,12C <0.02%
+ 115 -48.7s 0.4 s (2) EC
+ 116 0+ -54.3s 1.35 s (15) EC
+ 117 (3/2) -57.0s 1.75 s (7) EC,EA > 0%,EP > 0%
+ 118 0+ -62.0s 5.2 s (2) EC
+ 119 (5/2+) -64 5.4 s (3) EC,EP > 0%
+ 120 0+ -68.9 32 s (5) EC
+ 121 5/2(+) -70.3 29.5 s (5) EC,EP 0.02%
+ 122 0+ -74.3s 1.95 m (15) EC
+ 123 5/2+ -75.6s 2.7 m (4) EC
+ 124 0+ -79.09 11.9 m (10) EC
+ 125 1/2(+) -79.5 3.5 m (4) EC
+ 126 0+ -82.68 100 m (2) EC
+ 127 1/2(+) -82.8 12.7 m (4) EC
+ 127m 7/2(-) -82.7 1.9 s (2) IT
+ 128 0+ -85.41 2.43 d (5) EC
+ 129 1/2+ -85.07 2.23 h (11) EC
+ 129m 7/2+ -85.06 2.17 h (4) EC > 0%
+*130 0+ -87.271 0.106% (2)
+ 130m 8- -84.796 11 ms (2) IT
+ 131 1/2+ -86.693 11.50 d (6) EC
+ 131m 9/2- -86.506 14.6 m (2) IT
+*132 0+ -88.439 0.101% (3)
+ 133 1/2+ -87.558 3854 d (4) EC
+ 133m 11/2- -87.270 38.9 h (1) IT 99.99%,EC 0.01%
+*134 0+ -88.954 2.417% (27)
+*135 3/2+ -87.855 6.592% (18)
+ 135m 11/2- -87.587 28.7 h (2) IT
+*136 0+ -88.891 7.854% (36)
+ 136m 7- -86.860 0.3084 s (19) IT
+*137 3/2+ -87.726 11.23% (4)
+ 137m 11/2- -87.064 2.552 m (1) IT
+*138 0+ -88.266 71.70% (7)
+ 139 7/2- -84.918 83.06 m (28) B-
+ 140 0+ -83.278 12.752 d (3) B-
+ 141 3/2- -79.73 18.27 m (7) B-
+ 142 0+ -77.825 10.6 m (2) B-
+ 143 5/2- -73.95 14.33 s (8) B-
+ 144 0+ -71.78 11.5 s (2) B-,BN 3.6%
+ 145 5/2- -68.05 4.31 s (16) B-
+ 146 0+ -65.04 2.22 s (7) B-
+ 147 (3/2-) -61.49 0.893 s (1) B-,BN 0.06%
+ 148 0+ -58.0 0.607 s (25) B-,BN <= 0.4%
+ 149 -54.0s 0.344 s (7) B-,BN 0.43%
+ 150 0+ -50.7s 0.3 s B-
+ 151 > 150 NS
+57 La Lanthanum 39
+ 138.9055 (2)
+ 6.145 e
+ 920
+ 3455
+ +3
+ 120 -57.7s 2.8 s (2) EC,EP
+ 121 -62.4s 5.3 s (2) EC
+ 122 -64.5s 8.7 s (7) EC,EP
+ 123 -68.7s 17 s (3) EC
+ 124 (7+) -70.3s 29 s (2) EC
+ 125 (11/2-) -73.9s 76 s (6) EC
+ 126 -75.1s 54 s (2) EC > 0%
+ 127 (3/2+) -78.1s 3.8 m (5) EC
+ 127m (11/2-) -78.1s 5.0 m (5) IT ?%
+ 128 4-,5- -78.8 5.0 m (3) EC
+ 129 3/2+ -81.35 11.6 m (2) EC
+ 129m 11/2- -81.18 0.56 s (5) IT
+ 130 3(+) -81.7s 8.7 m (1) EC
+ 131 3/2+ -83.7 59 m (2) EC
+ 132 2- -83.73 4.8 h (2) EC
+ 132m 6- -83.54 24.3 m (5) IT 76%,EC 24%
+ 133 5/2+ -85.3 3.912 h (8) EC
+ 134 1+ -85.24 6.45 m (16) EC
+ 135 5/2+ -86.65 19.5 h (2) EC
+ 136 1+ -86.02 9.87 m (3) EC
+ 136m -85.79 114 ms (3) IT
+ 137 7/2+ -87.13 6E+4 y (2) EC
+ 138 5+ -86.529 1.05E+11 y (2) EC 66.4%,B- 33.6%
+*139 7/2+ -87.235 99.9098% (2)
+ 140 3- -84.325 1.6781 d (3) B-
+ 141 (7/2+) -82.942 3.92 h (3) B-
+ 142 2- -80.037 91.1 m (5) B-
+ 143 (7/2)+ -78.19 14.2 m (1) B-
+ 144 (3-) -74.90 40.8 s (4) B-
+ 145 -72.98 24.8 s (20) B-
+ 146 2- -69.16 6.27 s (10) B-
+ 146m (6-) -69.16 10.0 s (1) B-
+ 147 (3/2+,5/2+ -67.24 4.015 s (8) B-,BN 0.04%
+ 148 (2-) -63.2 1.428 s (12) B-,BN 0.15%
+ 149 -61.3s 1.05 s (3) B-,BN 1.4%
+ 150 -57.2s 0.86 s (5) B-,BN 2.7%
+ 151 -54.6s > 150 NS
+ 152 > 150 NS
+ 153 > 150 NS
+58 Ce Cerium 41
+ 140.115 (4)
+ 6.770 e
+ 799
+ 3424
+ +3,+4
+ 122 0+ -57.7s 8.7 s (7) EC,EP
+ 123 (5/2) -60.1s 3.8 s EC,EP
+ 124 0+ -64.7s 6 s (2) EC
+ 125 (5/2+) -66.6s 9.0 s (6) EC ,EP
+ 126 0+ -70.7s 50 s (3) EC > 0%
+ 127 -72.0s 32 s (4) EC
+ 128 0+ -75.6s ~ 3 m EC
+ 129 -76.3s 3.5 m (3) EC
+ 130 0+ -79.5s 25 m (2) EC
+ 131 (7/2+) -79.7 10.2 m (3) EC
+ 131m (1/2+) -79.7 5.0 m (10) EC
+ 132 0+ -82.4s 3.51 h (11) EC
+ 132m (8-,9-) -80.1s 13 ms (1) IT
+ 133 9/2- -82.4s 4.9 h (4) EC
+ 133m 1/2+ -82.4s 97 m (4) EC
+ 134 0+ -84.7 3.16 d (4) EC
+ 135 1/2(+) -84.63 17.7 h (2) EC
+ 135m 11/2(-) -84.18 20 s (1) IT
+*136 0+ -86.49 0.19% (1)
+ 137 3/2+ -85.90 9.0 h (3) EC
+ 137m 11/2- -85.65 34.4 h (3) IT 99.22%,EC 0.78%
+*138 0+ -87.57 0.25% (1)
+ 138m 7- -85.44 8.65 ms (20) IT
+ 139 3/2+ -86.957 137.640 d (23) EC
+ 139m 11/2- -86.203 54.8 s (10) IT
+*140 0+ -88.087 88.48% (10)
+ 141 7/2- -85.444 32.501 d (5) B-
+ 142 0+ -84.542 > 5E+16 y 2B- ?%
+ 143 3/2- -81.616 33.039 h (6) B-
+ 144 0+ -80.441 284.893 d (8) B-
+ 145 (3/2-) -77.10 3.01 m (6) B-
+ 146 0+ -75.70 13.52 m (13) B-
+ 147 (5/2-) -72.18 56.4 s (10) B-
+ 148 0+ -70.4 56 s (1) B-
+ 149 -66.80 5.3 s (2) B-
+ 150 0+ -65.0 4.0 s (6) B-
+ 151 -61.5s 1.02 s (6) B-
+ 152 0+ -59.0s 1.4 s (2) B-
+ 153 -55.0s > 150 NS
+ 154 0+ > 150 NS
+ 155 > 150 NS
+59 Pr Praseodymium 37
+ 140.90765 (2) (6.64s)
+ 6.773 r
+ 931
+ 3510
+ +3
+ 121 -42.847C 1.4 s (8) EC
+ 124 -53.0s 1.2 s (2) EC ,EP
+ 126 -60.3s 3.1 s (3) EC > 0%,EP
+ 127 -64.4s 15.1 s CA EC
+ 128 -66.3s 3.1 s (2) EC ,EP
+ 129 -70.0s 24 s (5) EC > 0%
+ 130 -71.4s 40.0 s (4) EC
+ 131 (3/2+) -74.5 1.53 m (5) EC
+ 131m (11/2-) -74.3 5.7 s (2) IT 95%,EC 5%
+ 132 -75.3s 1.6 m (3) EC
+ 133 5/2(+) -78.1s 6.5 m (3) EC
+ 134 2- -78.5s 17 m (2) EC
+ 134m (5-) -78.5s ~ 11 m EC
+ 135 3/2(+) -80.9 24 m (2) EC
+ 136 2+ -81.37 13.1 m (1) EC
+ 137 5/2+ -83.20 1.28 h (3) EC
+ 138 1+ -83.14 1.45 m (5) EC
+ 138m 7- -82.77 2.12 h (4) EC
+ 139 5/2+ -84.828 4.41 h (4) EC
+ 140 1+ -84.699 3.39 m (1) EC
+*141 5/2+ -86.025 100%
+ 142 2- -83.797 19.12 h (4) B- 99.98%,EC 0.02%
+ 142m 5- -83.793 14.6 m (5) IT
+ 143 7/2+ -83.077 13.57 d (2) B-
+ 144 0- -80.759 17.28 m (5) B-
+ 144m 3- -80.700 7.2 m (3) IT 99.93%,B- 0.07%
+ 145 7/2+ -79.636 5.984 h (10) B-
+ 146 (2)- -76.74 24.15 m (18) B-
+ 147 (3/2+) -75.47 13.4 m (4) B-
+ 148 1- -72.5 2.27 m (4) B-
+ 148m (4) -72.4 2.0 m (1) B-
+ 149 (5/2+) -70.99 2.26 m (7) B-
+ 150 (1)- -68.00 6.19 s (16) B-
+ 151 (3/2-,5/2- -66.79 18.90 s (7) B-
+ 152 (4-) -63.5s 3.63 s (12) B-
+ 153 -61.5s 4.3 s (2) B-
+ 154 (3+,2+) -57.7s 2.3 s (1) B-
+60 Nd Neodymium 36
+ 144.24 (3)
+ 7.008
+ 1016
+ 3066
+ +3
+ 127 -55.4s 1.8 s (4) EC ,EP
+ 128 0+ -60.2s EC
+ 129 (5/2+) -62.2s 4.9 s (2) EC ,EP
+ 130 0+ -66.3s 28 s (3) EC
+ 131 (5/2) -67.9 27 s (2) EC,EP
+ 132 0+ -71.6s 1.75 m (17) EC
+ 133 -72.5s 70 s (10) EC
+ 133m (9/2-) -72.5s < 2 m EC
+ 134 0+ -75.8s 8.5 m (15) EC
+ 135 9/2(-) -76.2s 12.4 m (6) EC
+ 135m -76.2s 5.5 m (5) EC
+ 136 0+ -79.16 50.65 m (33) EC
+ 137 1/2+ -79.51 38.5 m (15) EC
+ 137m 11/2- -78.99 1.60 s (15) IT
+ 138 0+ -82.0s 5.04 h (9) EC
+ 139 3/2+ -82.04 29.7 m (5) EC
+ 139m 11/2- -81.81 5.50 h (20) EC 88.2%,IT 11.8%
+ 140 0+ -84.48 3.37 d (2) EC
+ 140m 7- -82.26 0.60 ms (5) IT
+ 141 3/2+ -84.202 2.49 h (3) EC
+ 141m 11/2- -83.445 62.0 s (8) IT,EC < 0.05%
+*142 0+ -85.959 27.13% (12)
+*143 7/2- -84.011 12.18% (6)
+ 144 0+ -83.757 2.29E+15 y (16) A
+*145 7/2- -81.441 8.30% (6)
+*146 0+ -80.935 17.19% (9)
+ 147 5/2- -78.156 10.98 d (1) B-
+*148 0+ -77.417 5.76% (3)
+ 149 5/2- -74.385 1.728 h (1) B-
+ 150 0+ -73.693 > 1.1E19 y 2B- ?%
+ 151 (3/2)+ -70.956 12.44 m (7) B-
+ 152 0+ -70.16 11.4 m (2) B-
+ 153 (1/2:5/2) -67.1s 28.9 s (4) B-
+ 154 0+ -65.6s 25.9 s (2) B-
+ 155 -62.0s 8.9 s (2) B-
+ 156 0+ -60.1s 5.47 s (11) B-
+61 Pm Promethium 38
+ (145)
+ 7.264 e
+ 1042
+ 3000
+ +3
+ 130 -55.5s 2.2 s (5) EC,EP
+ 132 (3+) -61.7s 6.3 s (7) EC,EP ~5.0E-5%
+ 133 -65.5s 12 s (3) EC
+ 134 (2+) -66.9s ~ 5 s EC
+ 134m (5+) -66.9s 22 s (1) EC
+ 135 (11/2-) -70.1s 40 s (3) EC
+ 136 (2+) -71.3 47 s (2) EC
+ 136 5(+),6- -71.3 107 s (6) EC
+ 137 11/2- -73.9s 2.4 m (1) EC
+ 138 1+ -75.1s 10 s (2) EC
+ 138m (3+) -75.1s 3.24 m (5) EC
+ 138n (5-) -75.1s 3.24 m EC
+ 139 (5/2)+ -77.52 4.15 m (5) EC
+ 139m (11/2)- -77.33 180 ms (20) IT,EC ?%
+ 140 1+ -78.39 9.2 s (2) EC
+ 140m 8- -78.39 5.95 m (5) EC
+ 141 5/2+ -80.49 20.90 m (5) EC
+ 142 1+ -81.09 40.5 s (5) EC
+ 143 5/2+ -82.970 265 d (7) EC
+ 144 5- -81.425 363 d (14) EC
+ 145 5/2+ -81.278 17.7 y (4) EC,A 3E-07%
+ 146 3- -79.463 5.53 y (5) EC 66%,B- 34%
+ 147 7/2+ -79.052 2.6234 y (2) B-
+ 148 1- -76.878 5.370 d (9) B-
+ 148m 6- -76.740 41.29 d (11) B- 95%,IT 5%
+ 149 7/2+ -76.075 53.08 h (5) B-
+ 150 (1-) -73.61 2.68 h (2) B-
+ 151 5/2+ -73.399 28.40 h (4) B-
+ 152 1+ -71.27 4.12 m (8) B-
+ 152m 4- -71.12 7.52 m (8) B-
+ 152n (8) -71.10 13.8 m (2) B- ~100%,IT ~ 0%
+ 153 5/2- -70.67 5.4 m (2) B-
+ 154 (0,1) -68.4 1.73 m (10) B-
+ 154m (3,4) -68.4 2.68 m (7) B-
+ 155 (5/2-) -67.0s 41.5 s (2) B-
+ 156 4(-) -64.22 26.70 s (10) B-
+ 157 (5/2-) -62.2s 10.56 s (10) B-
+ 158 -59.0s 4.8 s (5) B-
+62 Sm Samarium 34
+ 150.36 (3)(7.40s)
+ 7.520 r
+ 1072
+ 1790
+ +2,+3
+ 131 -51.283C 1.2 s (2) EC,EP > 0%
+ 132 0+ -55.973C 4.0 s (3) EC,EP
+ 133 (5/2+) -57.1s 2.9 s (2) EC,EP
+ 134 0+ -61.5s 10 s (1) EC
+ 135 (7/2+) -63.0s 10 s (2) EC,EP
+ 136 0+ -66.8s 47 s (2) EC
+ 137 (9/2-) -67.9s 45 s (1) EC
+ 138 0+ -71.2s 3.1 m (2) EC
+ 139 (1/2)+ -72.1 2.57 m (10) EC
+ 139m (11/2)- -71.6 10.7 s (6) IT 93.7%,EC 6.3%
+ 140 0+ -75.4s 14.82 m (12) EC
+ 141 1/2+ -75.94 10.2 m (2) EC
+ 141m 11/2- -75.77 22.6 m (2) EC 99.69%,IT 0.31%
+ 142 0+ -78.99 72.49 m (5) EC
+ 143 3/2+ -79.527 8.83 m (1) EC
+ 143m 11/2- -78.773 66 s (2) IT 99.76%,EC 0.24%
+ 143n 23/2- -76.732 30 ms (3) IT
+*144 0+ -81.975 3.1% (1)
+ 145 7/2- -80.661 340 d (3) EC
+ 146 0+ -81.005 10.3E+7 y (5) A
+ 147 7/2- -79.276 1.06E+11 y (2) A
+ 148 0+ -79.346 7E+15 y (3) A
+ 149 7/2- -77.147 > 2E+15 y A ?%
+*150 0+ -77.061 7.4% (1)
+ 151 5/2- -74.586 90 y (8) B-
+*152 0+ -74.772 26.7% (2)
+ 153 3/2+ -72.569 46.27 h (1) B-
+*154 0+ -72.465 22.7% (2)
+ 155 3/2- -70.201 22.3 m (2) B-
+ 156 0+ -69.372 9.4 h (2) B-
+ 157 (3/2-) -66.8 482 s (4) B-
+ 158 0+ -65.3s 5.30 m (3) B-
+ 159 (5/2-) -62.2s 11.37 s (15) B-
+ 160 0+ -60.3s 9.6 s (3) B-
+63 Eu Europium 37
+ 151.965 (9)
+ 5.244 e
+ 822
+ 1596
+ +2,+3
+ 134 -50.615C 0.5 s (2) EC,EP > 0%
+ 135 -54.3s 1.5 s (2) EC
+ 136 (7+) -56.4s 3.3 s (3) EC,EP 0.09%
+ 136 (3+) -56.4s 3.7 s (3) EC,EP 0.09%
+ 137 (11/2-) -60.4s 11 s (2) EC
+ 138 (6-) -62.0s 12.1 s (6) EC
+ 139 (11/2)- -65.4s 17.9 s (6) EC
+ 140 1+ -67.0s 1.51 s (2) EC
+ 140m (5-) -66.8s 125 ms (2) IT,EC < 1%
+ 141 5/2+ -70.4 41.4 s (7) EC
+ 141m 11/2- -70.3 2.7 s (3) IT 87%,EC 13%
+ 142 1+ -71.63 2.4 s (2) EC
+ 142m 8- -71.63 1.22 m (2) EC
+ 143 5/2+ -74.36 2.57 m (3) EC
+ 144 1+ -75.65 10.2 s (3) EC
+ 145 5/2+ -78.001 5.93 d (4) EC
+ 146 4- -77.127 4.59 d (3) EC
+ 147 5/2+ -77.555 24.1 d (6) EC,A 2.2E-3%
+ 148 5- -76.24 54.5 d (5) EC,A 9.4E-7%
+ 149 5/2+ -76.454 93.1 d (4) EC
+ 150 5(-) -74.800 36.9 y (9) EC
+ 150m 0- -74.758 12.8 h (1) B- 89%,EC 11%
+*151 5/2+ -74.663 47.8% (15)
+ 152 3- -72.898 13.537 y (6) EC 72.1%,B- 27.9%
+ 152m 0- -72.852 9.3116 h (13) B- 72%,EC 28%
+ 152n 8- -72.750 96 m (1) IT
+*153 5/2+ -73.377 52.2% (15)
+ 154 3- -71.748 8.593 y (4) B- 99.98%,EC 0.02%
+ 154m (8-) -71.603 46.3 m (4) IT
+ 155 5/2+ -71.828 4.7611 y (13) B-
+ 156 0+ -70.094 15.19 d (8) B-
+ 157 5/2+ -69.471 15.18 h (3) B-
+ 158 (1-) -67.21 45.9 m (2) B-
+ 159 5/2+ -66.057 18.1 m (1) B-
+ 160 1(-) -63.4s 38 s (4) B-
+ 161 -61.8s 26 s (3) B-
+ 162 -58.6s 10.6 s (10) B-
+64 Gd Gadolinium 31
+ 157.25 (3)
+ 7.901 e
+ 1314
+ 3264
+ +3
+ 137 -51.6s 7 s (3) EC
+ 139 -57.7s 4.9 s (10) EC ,EP
+ 140 0+ -61.5s 15.8 s (4) EC
+ 141 (1/2+) -63.1s 14 s (4) EC,EP 0.03%
+ 141m (11/2-) -62.8s 24.5 s (5) EC 89%,IT 11%
+ 142 0+ -67.1s 70.2 s (6) EC
+ 143 (1/2)+ -68.4 39 s (2) EC
+ 143m (11/2-) -68.2 112 s (2) EC
+ 144 0+ -71.9s 4.5 m (1) EC
+ 145 1/2+ -72.95 23.0 m (4) EC
+ 145m 11/2- -72.20 85 s (3) IT 94.3%,EC 5.7%
+ 146 0+ -76.097 48.27 d (10) EC
+ 147 7/2- -75.367 38.06 h (12) EC
+ 148 0+ -76.279 74.6 y (30) A
+ 149 7/2- -75.135 9.28 d (10) EC,A 4.3E-4%
+ 150 0+ -75.771 1.79E+6 y (8) A
+ 151 7/2- -74.199 124 d (1) EC,A 1.0E-6%
+ 152 0+ -74.716 1.08E14 y (8) A
+ 153 3/2- -72.892 241.6 d (2) EC
+*154 0+ -73.716 2.18% (3)
+*155 3/2- -72.080 14.80% (5)
+ 155m 11/2- -71.959 31.97 ms (27) IT
+*156 0+ -72.545 20.47% (4)
+*157 3/2- -70.834 15.65% (3)
+*158 0+ -70.700 24.84% (12)
+ 159 3/2- -68.572 18.479 h (4) B-
+*160 0+ -67.952 21.86% (4)
+ 161 5/2- -65.516 3.66 m (5) B-
+ 162 0+ -64.291 8.4 m (2) B-
+ 163 (5/2-) -61.5s 68 s (3) B-
+ 164 0+ -59.7s 45 s (3) B-
+65 Tb Terbium 44
+ 158.92534 (2)
+ 8.230
+ 1359
+ 3221
+ +3
+ 140 5 -51s 2.4 s (2) EC,P 0.26%
+ 141 (5/2-) -54.8s 3.5 s (2) EC
+ 141m -54.8s 7.9 s (6) EC
+ 142 1+ -57.1s 597 ms (17) EC,EP ~3.0E-7%
+ 142m (5-) -56.8s 303 ms (7) EC ,EP ,IT
+ 143 (11/2-) -61.0s 12 s (1) EC
+ 143m (5/2+) -61.0s < 21 s IT
+ 144 (1+) -63.0s ~ 1 s EC
+ 144m (6-) -62.6s 4.25 s (15) IT 66%,EC 34%
+ 145 (1/2+) -66.4 31.6 s (6) EC ?%
+ 145m (11/2-) -66.4 29.5 s (15) EC
+ 146 1+ -68.0 8 s (4) EC
+ 146m 5- -68.0 24.1 s (5) EC
+ 146n (10+) -67.2 1.18 ms (2)
+ 147 (1/2+) -70.76 1.7 h (1) EC
+ 147m (11/2)- -70.70 1.92 m (7) EC
+ 148 2- -70.59 60 m (3) EC
+ 148m 9+ -70.50 2.30 m (10) EC
+ 149 1/2+ -71.499 4.118 h (25) EC 83.3%,A 16.7%
+ 149m 11/2- -71.463 4.16 m (4) EC 99.98%,A 0.02%
+ 150 (2-) -71.115 3.48 h (16) EC,A < 0.05%
+ 150m (9+) -70.645 5.8 m (2) EC ~100%
+ 151 1/2(+) -71.633 17.609 h (1) EC,A 0.0095%
+ 151m (11/2-) -71.533 25 s (3) IT 93.8%,EC 6.2%
+ 152 2- -70.73 17.5 h (1) EC,A <7.0E-7%
+ 152m 8+ -70.22 4.2 m (1) IT 78.8%,EC 21.2%
+ 153 5/2+ -71.322 2.34 d (1) EC
+ 154 0 -70.15 21.5 h (4) EC,B- < 0.1%
+ 154m 3- -70.15 9.4 h (4) EC 78.2%,IT 21.8%
+ 154n 7- -70.15 22.7 h (5) EC 98.2%,IT 1.8%
+ 155 3/2+ -71.26 5.32 d (6) EC
+ 156 3- -70.101 5.35 d (10) EC,B-
+ 156m (7-) -70.051 24.4 h (10) IT
+ 156n (0+) -70.013 5.3 h (2) EC ,IT
+ 157 3/2+ -70.774 99 y (10) EC
+ 158 3- -69.480 180 y (11) EC 83.4%,B- 16.6%
+ 158m 0- -69.370 10.70 s (17) IT,B- < 0.6%
+*159 3/2+ -69.542 100%
+ 160 3- -67.846 72.3 d (2) B-
+ 161 3/2+ -67.472 6.88 d (3) B-
+ 162 1- -65.68 7.60 m (15) B-
+ 163 3/2+ -64.605 19.5 m (3) B-
+ 164 (5+) -62.09 3.0 m (1) B-
+ 165 (3/2+) -60.7s 2.11 m (10) B-
+66 Dy Dysprosium 35
+ 162.50 (3)
+ 8.551 e
+ 1411
+ 2561
+ +3
+ 141 (9/2-) -45.5s 0.9 s (2) EC,EP
+ 142 0+ -50.2s 2.3 s (3) EC,EP ~8.0E-5%
+ 143 -52.2s 3.9 s (4) EC ,EP
+ 144 0+ -56.8s 9.1 s (4) EC,EP
+ 145 (1/2+) -58.7s 10.5 s (15) EC
+ 145m (11/2-) -58.7s 13.6 s (10) EC
+ 146 0+ -62.9 33.2 s (7) EC
+ 146m 10+ -59.9 150 ms (20) IT
+ 147 1/2+ -64.38 40 s (10) EC,EP > 0%
+ 147m 11/2- -63.63 55.7 s (7) EC 65%,IT 35%
+ 148 0+ -67.91 3.1 m (1) EC
+ 149 (7/2-) -67.69 4.20 m (14) EC
+ 149m (27/2-) -65.03 0.490 s (15) IT 99.3%,EC 0.7%
+ 150 0+ -69.321 7.17 m (5) EC 64%,A 36%
+ 151 7/2(-) -68.762 17.9 m (3) EC 94.4%,A 5.6%
+ 152 0+ -70.128 2.38 h (2) EC 99.9%,A 0.1%
+ 153 7/2(-) -69.151 6.4 h (1) EC 99.991%,A 9.4E-3%
+ 154 0+ -70.400 3.0E+6 y (15) A
+ 155 3/2- -69.16 9.9 h (2) EC
+*156 0+ -70.534 0.06% (1)
+ 157 3/2- -69.432 8.14 h (4) EC
+ 157m 11/2- -69.233 21.6 ms (16) IT
+*158 0+ -70.417 0.10% (1)
+ 159 3/2- -69.177 144.4 d (2) EC
+*160 0+ -69.682 2.34% (5)
+*161 5/2+ -68.065 18.9% (1)
+*162 0+ -68.190 25.5% (2)
+*163 5/2- -66.390 24.9% (2)
+*164 0+ -65.977 28.2% (2)
+ 165 7/2+ -63.621 2.334 h (1) B-
+ 165m 1/2- -63.513 1.257 m (6) IT 97.76%,B- 2.24%
+ 166 0+ -62.593 81.6 h (1) B-
+ 167 (1/2-) -59.94 6.20 m (8) B-
+ 168 0+ -58.5s 8.7 m (3) B-
+ 169 (5/2-) -55.6 39 s (8) B-
+67 Ho Holmium 48
+ 164.93032 (2)
+ 8.795 e
+ 1472
+ 2694
+ +3
+ 144 -45.0s 0.7 s (1) EC ,EP
+ 146 (10+) -52.2s 3.6 s (3) EC,EP
+ 147 (11/2-) -56.2s 5.8 s (4) EC,EP
+ 148 1+ -58.5s 2.2 s (11) EC
+ 148m 6- -58.5s 9.3 s (2) EC,EP 0.08%
+ 149 (11/2-) -61.67 21.1 s (2) EC
+ 149m (1/2+) -61.62 56 s (3) EC
+ 150 2- -62.08s 72 s (4) EC
+ 150m (9)+ -61.28s 23.3 s (3) EC
+ 151 (11/2-) -63.63 35.2 s (1) EC 78%,A 22%
+ 151m (1/2+) -63.59 47.2 s (10) A ~ 80%,EC ?%
+ 152 2- -63.65 161.8 s (3) EC 88%,A 12%
+ 152m 9+ -63.49 50.0 s (4) EC 89.2%,A 10.8%
+ 153 11/2- -65.023 2.02 m (3) EC 99.95%,A 0.05%
+ 153m 1/2+ -64.955 9.3 m (5) EC 99.82%,A 0.18%
+ 154 (2)- -64.648 11.76 m (19) EC 99.98%,A 0.02%
+ 154m 8+ -64.328 3.10 m (14) EC,A <1.0E-3%
+ 155 5/2+ -66.06 48 m (1) EC
+ 156 (5+) -65.5s 56 m (1) EC
+ 156m (2+) -65.4s 9.5 s (15) IT
+ 157 7/2- -66.89 12.6 m (2) EC
+ 158 5+ -66.18 11.3 m (4) EC
+ 158m 2- -66.11 28 m (2) IT > 81%,EC < 19%
+ 158n (9+) -66.00 21.3 m (23) EC ~ 93%
+ 159 7/2- -67.339 33.05 m (11) EC
+ 159m 1/2+ -67.133 8.30 s (8) IT
+ 160 5+ -66.39 25.6 m (3) EC
+ 160m 2- -66.33 5.02 h (5) IT 65%,EC 35%
+ 160n (9+) -66.22 3 s IT
+ 161 7/2- -67.206 2.48 h (5) EC
+ 161m 1/2+ -66.995 6.76 s (7) IT
+ 162 1+ -66.050 15.0 m (10) EC
+ 162m 6- -65.944 67.0 m (7) IT 62%,EC 38%
+ 163 7/2- -66.387 4570 y (25) EC
+ 163m 1/2+ -66.089 1.09 s (3) IT
+ 164 1+ -64.990 29 m (1) EC 60%,B- 40%
+ 164m 6- -64.850 37.5 m (+15-5) IT
+*165 7/2- -64.907 100%
+ 166 0- -63.080 26.763 h (4) B-
+ 166m (7)- -63.074 1.20E3 y (18) B-
+ 167 7/2- -62.292 3.1 h (1) B-
+ 168 3+ -60.08 2.99 m (7) B-
+ 168m (6+) -60.03 132 s (4) IT >= 99.5%,B- <= 0.5%
+ 169 7/2- -58.81 4.7 m (1) B-
+ 170 (6+) -56.25 2.76 m (5) B-
+ 170m (1+) -56.13 43 s (2) B-
+ 171 (7/2-) -54.5 53 s (2) B-
+ 172 -51.709C 25 s (3) B-
+68 Er Erbium 34
+ 167.26 (3)
+ 9.066 e
+ 1529
+ 2862
+ +3
+ 146 0+ -44.8s 1.7 s (6) EC ,EP > 0%
+ 147 (11/2-) -47.1s 2.5 s (2) EC,EP > 0%
+ 147m (1/2+) -47.1s ~ 2.5 s EC,EP > 0%
+ 148 0+ -51.8s 4.6 s (2) EC
+ 149 (1/2+) -53.9s 4 s (2) EC,EP 7%
+ 149m (11/2-) -53.2s 8.9 s (2) EC 96.5%,IT 3.5%
+ 150 0+ -58.0s 18.5 s (7) EC
+ 151 (7/2-) -58.4s 23.5 s (13) EC
+ 151m (27/2-) -55.8s 0.58 s (2) IT 95.3%,EC 4.7%
+ 152 0+ -60.55 10.3 s (1) A 90%,EC 10%
+ 153 (7/2-) -60.46 37.1 s (2) A 53%,EC 47%
+ 154 0+ -62.617 3.73 m (9) EC 99.53%,A 0.47%
+ 155 7/2- -62.22 5.3 m (3) EC 99.98%,A 0.02%
+ 156 0+ -64.1s 19.5 m (10) EC,A 5E-06%
+ 157 3/2- -63.42 18.65 m (10) EC ~100%,A < 0.02%
+ 157m (9/2+) -63.27 76 ms (6) IT
+ 158 0+ -65.3s 2.29 h (6) EC
+ 159 3/2- -64.571 36 m (1) EC
+ 160 0+ -66.06 28.58 h (9) EC
+ 161 3/2- -65.203 3.21 h (3) EC
+*162 0+ -66.346 0.14% (1)
+ 163 5/2- -65.177 75.0 m (4) EC
+*164 0+ -65.952 1.61% (2)
+ 165 5/2- -64.531 10.36 h (4) EC
+*166 0+ -64.934 33.6% (2)
+*167 7/2+ -63.299 22.95% (15)
+ 167m 1/2- -63.091 2.269 s (6) IT
+*168 0+ -62.999 26.8% (2)
+ 169 1/2- -60.931 9.40 d (2) B-
+*170 0+ -60.118 14.9% (2)
+ 171 5/2- -57.728 7.516 h (2) B-
+ 172 0+ -56.493 49.3 h (3) B-
+ 173 (7/2-) -53.7s 1.4 m (1) B-
+ 174 0+ -52.1s 3.3 m (2) B-
+69 Tm Thulium 44
+ 168.93421 (2)
+ 9.321 e
+ 1545
+ 1946
+ +3
+ 146 (5-,6-) -30.8s 62 ms (+19-14) P
+ 146m (10+) -30.8s 206 ms (25) P
+ 147 (11/2-) -36.4s 0.559 s (26) EC ~ 90%,P ~ 10%
+ 147m -36.4s 0.39 ms (8) P
+ 148n (10+) -39.8s 0.7 s (2) EC
+ 149 (11/2-) -44.4s 0.9 s (2) EC,EP 0.2%
+ 150 (6-) -47.1s 2.2 s (2) EC
+ 150m (10+) -46.5s 5.2 ms (3) IT
+ 151 (11/2-) -50.9s 4.17 s (10) EC
+ 151m (1/2+) -50.9s 6.6 s (14) EC
+ 152 (2-) -51.9s 8.0 s (10) EC
+ 152m (9)+ -51.9s 5.2 s (6) EC
+ 153 (11/2-) -54.00 1.48 s (1) A 91%,EC 9%
+ 153m (1/2+) -53.96 2.5 s (2) A 95%,EC 5%
+ 154 (2-) -54.6s 8.1 s (3) EC 56%,A 44%
+ 154m (9+) -54.6s 3.30 s (7) A 90%,EC 10%,IT
+ 155 (11/2-) -56.64 21.6 s (2) EC 98.1%,A 1.9%
+ 155m (1/2+) -56.60 45 s (3) EC > 92%,A < 8%
+ 156 2- -56.89 83.8 s (18) EC 99.94%,A 0.06%
+ 156m -56.89 19 s (3) A ?%
+ 157 1/2+ -58.9 3.63 m (9) EC
+ 158 2- -58.8s 3.98 m (6) EC
+ 159 5/2+ -60.7 9.13 m (16) EC
+ 160 1- -60.2 9.4 m (3) EC
+ 160m 5 -60.1 74.5 s (15) IT 85%,EC 15%
+ 161 7/2+ -62.04 30.2 m (8) EC
+ 162 1- -61.54 21.70 m (19) EC
+ 162m 5+ -61.47 24.3 s (17) IT 82%,EC 18%
+ 163 1/2+ -62.738 1.810 h (5) EC
+ 164 1+ -61.99 2.0 m (1) EC
+ 164 6- -61.99 5.1 m (1) IT ~ 80%,EC ~ 20%
+ 165 1/2+ -62.939 30.06 h (3) EC
+ 166 2+ -61.89 7.70 h (3) EC
+ 167 1/2+ -62.551 9.25 d (2) EC
+ 168 3+ -61.320 93.1 d (2) EC 99.99%,B- 0.01%
+*169 1/2+ -61.282 100%
+ 170 1- -59.804 128.6 d (3) B- 99.85%,EC 0.15%
+ 171 1/2+ -59.219 1.92 y (1) B-
+ 172 2- -57.383 63.6 h (2) B-
+ 173 (1/2+) -56.262 8.24 h (8) B-
+ 174 (4)- -53.87 5.4 m (1) B-
+ 175 (1/2+,3/2+ -52.32 15.2 m (5) B-
+ 176 (4+) -49.6s 1.9 m (1) B-
+ 177 (1/2+) -47.8s 85 s (+10-15) B-
+70 Yb Ytterbium 34
+ 173.04 (3)
+ 6.903 r
+ 824
+ 1194
+ +2,+3
+ 151 (1/2+) -41.7s 1.6 s (1) EC,EP
+ 151m (11/2-) -41.7s 1.6 s (1) EC,EP
+ 152 0+ -46.4s 3.04 s (6) EC,EP
+ 153 (7/2-) -47.3s 4.2 s (1) A 50%,EC 50%
+ 154 0+ -50.1s 0.404 s (14) A 92.8%,EC 7.2%
+ 155 (7/2-) -50.7s 1.75 s (5) A 89%,EC 11%
+ 156 0+ -53.31 26.1 s (7) EC 90%,A 10%
+ 157 7/2- -53.41 38.6 s (10) EC 99.5%,A 0.5%
+ 158 0+ -56.021 1.49 m (13) EC,A ~2.1E-3%
+ 159 5/2(-) -55.7 1.58 m (14) EC
+ 160 0+ -58.2s 4.8 m (2) EC
+ 161 3/2- -57.9s 4.2 m (2) EC
+ 162 0+ -59.8s 18.87 m (19) EC
+ 163 3/2- -59.4 11.05 m (25) EC
+ 164 0+ -61.0s 75.8 m (17) EC
+ 165 5/2- -60.18 9.9 m (3) EC
+ 166 0+ -61.591 56.7 h (1) EC
+ 167 5/2- -60.596 17.5 m (2) EC
+*168 0+ -61.577 0.13% (1)
+ 169 7/2+ -60.373 32.026 d (5) EC
+ 169m 1/2- -60.349 46 s (2) IT
+*170 0+ -60.772 3.05% (6)
+*171 1/2- -59.315 14.3% (2)
+*172 0+ -59.264 21.9% (3)
+*173 5/2- -57.560 16.12% (21)
+*174 0+ -56.953 31.8% (4)
+ 175 7/2- -54.704 4.185 d (1) B-
+*176 0+ -53.497 12.7% (2)
+ 176m (8-) -52.447 11.4 s (3) IT >= 90%,B- < 10%
+ 177 (9/2+) -50.992 1.911 h (3) B-
+ 177m (1/2-) -50.661 6.41 s (3) IT
+ 178 0+ -49.70 74 m (3) B-
+ 179 (1/2-) -46.7s 8.0 m (4) B-
+ 180 0+ -44.688C 2.4 m (5) B-
+71 Lu Lutetium 57
+ 174.967
+ 9.841 e
+ 1663
+ 3393
+ +3
+ 150 -25.1s 35 ms (10) P 80%
+ 151 (11/2-) -30.7s 90 ms (10) P 70%
+ 152 (5-,6-) -34.1s 0.7 s (1) EC,EP 15%
+ 153 (11/2-) -38.5s P ?%
+ 154m (7+) -40.0s 1.12 s (8) EC ~100%
+ 155 (1/2+,3/2+ -42.7s 140 ms (20) A ,EC
+ 155m (11/2-) -42.7s 68 ms (5) A 79%,EC 21%
+ 155n (25/2-) -40.9s 2.60 ms (7) A ~100%
+ 156m -43.9s 0.179 s (13) A >= 75%,EC <= 25%
+ 156n -43.9s 0.73 s (15) A ~ 95%,EC ~ 5%
+ 157 (1/2+,3/2+ -46.48 7.4 s (14) A ?%,EC ?%
+ 157m (11/2-) -46.45 5.0 s (4) EC 94%,A 6%
+ 158 -47.3s 10.4 s (1) EC 99.09%,A 0.91%
+ 159 -49.68 12.1 s (10) EC,A 0.04%
+ 160 -50.3s 36.1 s (3) EC,A <=1.0E-4%
+ 160m -50.3s 40 s (1) EC,A ?%
+ 161 (5/2+) -52.6s 72 s EC
+ 161m (9/2-) -52.5s 7.3 ms (4) IT
+ 162 (1-) -52.6s 1.37 m (2) EC
+ 162m (4-) -52.6s 1.5 m EC
+ 162n -52.6s 1.9 m EC
+ 163 (1/2-) -54.8 238 s (8) EC
+ 164 -54.7s 3.14 m (3) EC
+ 165 (7/2+) -56.26 10.74 m (10) EC
+ 165? 1/2+ -56.26 12 m
+ 166 (6-) -56.1 2.65 m (10) EC
+ 166m (3-) -56.1 1.41 m (10) EC 58%,IT 42%
+ 166n (0-) -56.1 2.12 m (10) EC > 80%,IT < 20%
+ 167 7/2+ -57.5 51.5 m (10) EC
+ 168 (6-) -57.10 5.5 m (1) EC
+ 168m 3+ -56.88 6.7 m (4) EC > 95%,IT < 5%
+ 169 7/2+ -58.08 34.06 h (5) EC
+ 169m 1/2- -58.051 160 s (10) IT
+ 170 0+ -57.31 2.00 d (3) EC
+ 170m (4)- -57.22 0.67 s (10) IT
+ 171 7/2+ -57.836 8.24 d (3) EC
+ 171m 1/2- -57.765 79 s (2) IT
+ 172 4- -56.744 6.70 d (3) EC
+ 172m 1- -56.702 3.7 m (5) IT
+ 173 7/2+ -56.889 1.37 y (1) EC
+ 174 (1)- -55.579 3.31 y (5) EC
+ 174m (6)- -55.408 142 d (2) IT 99.38%,EC 0.62%
+*175 7/2+ -55.174 97.41% (2)
+ 176 7- -53.391 3.73E10 y (5) B-
+ 176m 1- -53.268 3.6832 h (7) B- 99.91%,EC 0.1%
+ 177 7/2+ -52.392 6.734 d (12) B-
+ 177m 23/2- -51.422 160.4 d (3) B- 78.3%,IT 21.7%
+ 178 1(+) -50.346 28.4 m (2) B-
+ 178m (9-) -50.226 23.1 m (3) B-
+ 179 7/2(+) -49.067 4.59 h (6) B-
+ 179m 1/2(+) -48.475 3.1 ms (9) IT
+ 180 (3)+ -46.69 5.7 m (1) B-
+ 181 (7/2+) -44.9s 3.5 m (3) B-
+ 182 (0,1,2) -41.603C 2.0 m (2) B-
+ 183 (7/2+) -39.755C 58 s (4) B-
+ 184 high -36.088C 20 s (3) B-
+ 184m low -36.088C ? B-
+72 Hf Hafnium 41
+ 178.49 (2)
+ 13.31 c
+ 2233
+ 4603
+ +4
+ 154 0+ -33.3s 2 s (1) EC ~100%,A ~ 0%
+ 155 -34.7s 0.89 s (12) EC,A
+ 156 0+ -38.0s 25 ms (4) A >= 81%
+ 157 -39.0s 110 ms (6) A 86%,EC 14%
+ 158 0+ -42.2s 2.86 s (18) EC 56%,A 44%
+ 159 -43.0s 5.6 s (4) EC 59%,A 41%
+ 160 0+ -45.98 13.0 s (15) EC 97.7%,A 2.3%
+ 161 -46.27 16.8 s (8) EC >= 99.71%,A <= 0.29%
+ 162 0+ -49.18 37.6 s (8) EC 99.99%,A 6.3E-3%
+ 163 -49.3s 40.0 s (6) EC
+ 164 0+ -51.8s 111 s (8) EC
+ 165 (5/2-) -51.7s 76 s (4) EC
+ 166 0+ -53.8s 6.77 m (30) EC
+ 167 (5/2-) -53.5s 2.05 m (5) EC
+ 168 0+ -55.3s 25.95 m (20) EC
+ 169 (5/2)- -54.81 3.24 m (4) EC
+ 170 0+ -56.2s 16.01 h (13) EC
+ 171 (7/2+) -55.4s 12.1 h (4) EC
+ 172 0+ -56.39 1.87 y (3) EC
+ 173 1/2- -55.3s 23.6 h (1) EC
+ 174 0+ -55.851 2.0E15 y (4) A
+ 175 5/2- -54.488 70 d (2) EC
+*176 0+ -54.582 5.206% (5)
+*177 7/2- -52.890 18.606% (4)
+ 177m 23/2+ -51.575 1.08 s (6) IT
+ 177n 37/2- -50.150 51.4 m (5) IT
+*178 0+ -52.445 27.297% (4)
+ 178m 8- -51.298 4.0 s (2) IT
+ 178n 16+ -49.999 31 y (1) IT
+*179 9/2+ -50.473 13.629% (6)
+ 179m 1/2- -50.098 18.67 s (4) IT
+ 179n 25/2- -49.367 25.05 d (25) IT
+*180 0+ -49.79 35.100% (7)
+ 180m 8- -48.649 5.5 h (1) IT 99.7%,B- 0.3%
+ 181 1/2- -47.414 42.39 d (6) B-
+ 182 0+ -46.060 9E+6 y (2) B-
+ 182m 8- -44.887 61.5 m (15) B- 58%,IT 42%
+ 183 (3/2-) -43.29 1.067 h (17) B-
+ 184 0+ -41.50 4.12 h (5) B-
+ 184m 8- -41.50 48 s (10) B-
+ 185 -38.164C 3.5 m (6) B-
+73 Ta Tantalum 38
+ 180.9479
+ 16.654
+ 3017
+ 5458
+ +5
+ 156 (2-) -26.4s 0.11 s (+6-3) EC 50%,P 50%
+ 157 -29.7s 5.3 ms (18) A > 77%
+ 158 -31.3s 36.8 ms (16) A 93%,EC 7%
+ 159 -34.5s 0.57 s (18) A 80%,EC 20%
+ 160 -35.9s 1.5 s (2) EC 66%,A 34%
+ 161 -38.77 3.00 s (15) EC ~ 95%,A ~ 5%
+ 162 -39.9s 3.60 s (15) EC 99.92%,A 0.08%
+ 163 -42.51 11.0 s (8) EC ~ 99.72%,A ~ 0.28%
+ 164 (3+) -43.2s 14.2 s (3) EC
+ 165 -45.8s 31.0 s (15) EC
+ 166 (2)+ -46.1s 31.5 s (20) EC
+ 167 -48.5s 1.33 m (7) EC
+ 168 (2-,3+) -48.6s 2.0 m (1) EC
+ 169 (5/2-) -50.4s 4.9 m (4) EC
+ 170 (3+) -50.2s 6.76 m (6) EC
+ 171 (5/2-) -51.7s 23.3 m (3) EC
+ 172 (3+) -51.5 36.8 m (3) EC
+ 173 5/2- -52.5s 3.14 h (13) EC
+ 174 3(+) -52.01 1.05 h (3) EC
+ 175 7/2+ -52.5s 10.5 h (2) EC
+ 176 (1)- -51.47 8.09 h (5) EC
+ 177 7/2+ -51.724 56.56 h (6) EC
+ 178 1+ -50.5 9.31 m (3) EC
+ 178 (7)- -50.5 2.36 h (8) EC
+ 178m (15-) -49.1 60 ms (5) IT
+ 179 7/2+ -50.362 1.82 y (3) EC
+ 179m (25/2+) -49.044 9.0 ms (2) IT
+ 179n (37/2+) -47.721 52 ms (3) IT
+ 180 1+ -48.936 8.152 h (6) EC 86%,B- 14%
+ 180m 9- -48.861 > 1.2E+15 y B- ?%,EC ?%
+*181 7/2+ -48.441 99.988% (2)
+ 182 3- -46.433 114.43 d (3) B-
+ 182m 5+ -46.417 283 ms (3) IT
+ 182n 10- -45.913 15.84 m (10) IT
+ 183 7/2+ -45.296 5.1 d (1) B-
+ 184 (5-) -42.84 8.7 h (1) B-
+ 185 (7/2+) -41.40 49.4 m (15) B-
+ 186 2,3 -38.61 10.5 m (5) B-
+74 W Tungsten 37
+ 183.84
+ 19.3 c
+ 3422
+ 5555
+ +6
+ 158 0+ -24.3s 0.9 ms (3) A
+ 159 -25.8s 7.3 ms (27) A ~ 99.5%,EC ~ 0.5%
+ 160 0+ -29.5s 81 ms (15) A >= 54%
+ 161 -30.7s 410 ms (40) A ~ 82%,EC ~ 18%
+ 162 0+ -34.1s 1.39 s (4) EC 53%,A 47%
+ 163 -35.1s 2.75 s (25) EC 59%,A 41%
+ 164 0+ -38.28 6.4 s (8) EC 97.4%,A 2.6%
+ 165 -38.81 5.1 s (5) EC,A < 0.2%
+ 166 0+ -41.90 18.8 s (4) EC 99.97%,A 0.04%
+ 167 -42.2s 19.9 s (5) A ,EC
+ 168 0+ -44.8s 51 s (2) EC ~100%,A 3.2E-3%
+ 169 (5/2-) -44.9s 80 s (6) EC
+ 170 0+ -47.2s 2.42 m (4) EC
+ 171 (5/2-) -47.2s 2.38 m (4) EC
+ 172 0+ -49.0s 6.6 m (9) EC
+ 173 5/2- -48.5s 7.6 m (2) EC
+ 174 0+ -50.2s 31 m (1) EC
+ 175 (1/2-) -49.6s 35.2 m (6) EC
+ 176 0+ -50.7s 2.5 h (1) EC
+ 177 (1/2-) -49.7s 135 m (3) EC
+ 178 0+ -50.4 21.6 d (3) EC
+ 179 (7/2)- -49.30 37.05 m (16) EC
+ 179m (1/2)- -49.08 6.40 m (7) IT 99.72%,EC 0.28%
+*180 0+ -49.644 0.120% (1)
+ 180m 8- -48.115 5.47 ms (9) IT
+ 181 9/2+ -48.253 121.2 d (2) EC
+*182 0+ -48.246 26.498% (29)
+ 183 1/2- -46.366 > 1.1E+17 y
+ 183m 11/2+ -46.057 5.2 s (3) IT
+ 184 0+ -45.706 > 3E+17 y A ?%
+ 185 3/2- -43.389 75.1 d (3) B-
+ 185m 11/2+ -43.192 1.67 m (3) IT
+*186 0+ -42.512 28.426% (37)
+ 187 3/2- -39.907 23.72 h (6) B-
+ 188 0+ -38.669 69.4 d (5) B-
+ 189 (3/2-) -35.5 11.5 m (3) B-
+ 190 0+ -34.3 30.0 m (15) B-
+75 Re Rhenium 43
+ 186.207
+ 21.02 c
+ 3186
+ 5596
+ +4,+6,+7
+ 160 -17.2s 0.64 ms (8) P 89%,A 11%
+ 161 -20.8s 15 ms (4) A ~100%
+ 162 -22.6s 0.10 s (3) EC < 97%,A > 3%
+ 163 -26.0s 260 ms (40) A 64%,EC 36%
+ 164 -27.5s 0.88 s (24) A ~ 58%,EC ~ 42%
+ 165 -30.69 2.4 s (6) EC 87%,A 13%
+ 166 -31.9s 2.8 s (3) A
+ 167 (1/2) -34.8s 3.4 s (4) A ~100%
+ 167 (1/2) -34.8s 6.2 s (5) EC ~ 99%,A ~ 1%
+ 168 (5+,6+,7+) -35.8s 4.4 s (1) EC ~100%,A ~5.0E-3%
+ 169 -38.4s 8.1 s (5) EC ~100%,A ~1.0E-4%
+ 169m -38.4s 16.3 s (8) A ~100%
+ 170 (5+) -39.0s 9.2 s (2) EC
+ 171 (9/2-) -41.5s 15.2 s (4) EC
+ 172m (5) -41.6s 15 s (3) EC
+ 172n (2) -41.6s 55 s (5) EC
+ 173 (5/2-) -43.7s 1.98 m (26) EC
+ 174 -43.7s 2.40 m (4) EC
+ 175 (5/2-) -45.3s 5.89 m (5) EC
+ 176 3(+) -45.1s 5.3 m (3) EC
+ 177 (5/2-) -46.3s 14 m (1) EC
+ 178 (3+) -45.8 13.2 m (2) EC
+ 179 (5/2)+ -46.59 19.5 m (1) EC
+ 180 (1)- -45.84 2.44 m (6) EC
+ 181 5/2+ -46.51 19.9 h (7) EC
+ 182 7+ -45.4 64.0 h (5) EC
+ 182m 2+ -45.4 12.7 h (2) EC
+ 183 5/2+ -45.810 70.0 d (14) EC
+ 183m (25/2)+ -43.903 1.04 ms (5) IT
+ 184 3(-) -44.224 38.0 d (5) EC
+ 184m 8(+) -44.036 169 d (8) IT 75.4%,EC 24.6%
+*185 5/2+ -43.822 37.40% (2)
+ 186 1- -41.930 89.25 h (7) B- 93.1%
+ 186 1- -41.930 90.64 h (9) EC 6.9%
+ 186m (8+) -41.781 2.0E+5 y (5) IT,B- < 10%
+ 187 5/2+ -41.218 4.35E10 y (13) B-,A <1.0E-4%
+ 188 1- -39.018 17.021 h (25) B-
+ 188m (6)- -38.846 18.59 m (4) IT
+ 189 5/2+ -37.979 24.3 h (4) B-
+ 190 (2)- -35.6 3.1 m (3) B-
+ 190m (6-) -35.4 3.2 h (2) B- 54.4%,IT 45.6%
+ 191 (3/2+,1/2+ -34.35 9.8 m (5) B-
+ 192 -31.7s 16 s (1) B-
+76 Os Osmium 41
+ 190.23 (3)
+ 22.57
+ 3033
+ 5012
+ +3,+4
+ 162 0+ -15.1s 1.9 ms (7) A
+ 163 -16.7s ? A ,EC
+ 164 0+ -20.6s 41 ms (20) A ~ 98%,EC ~ 2%
+ 165 -21.9s 73 ms (8) A > 60%,EC < 40%
+ 166 0+ -25.6s 194 ms (17) A 72%,EC 18%
+ 167 -26.7s 0.83 s (12) A 67%,EC 33%
+ 168 0+ -30.04 2.2 s (1) EC 51%,A 49%
+ 169 -30.7 3.4 s (2) EC 89%,A 11%
+ 170 0+ -33.93 7.1 s (2) EC 88%,A 12%
+ 171 (5/2-) -34.4s 8.0 s (7) EC 98.3%,A 1.7%
+ 172 0+ -37.2s 19.2 s (5) EC 99.8%,A 0.2%
+ 173 (5/2-) -37.5s 16 s (5) EC 99.98%,A 0.02%
+ 174 0+ -39.9s 44 s (4) EC 99.98%,A 0.02%
+ 175 (5/2-) -40.0s 1.4 m (1) EC
+ 176 0+ -41.9s 3.6 m (5) EC
+ 177 (1/2-) -41.9s 2.8 m (3) EC
+ 178 0+ -43.4 5.0 m (4) EC
+ 179 (1/2-) -42.9s 6.5 m (3) EC
+ 180 0+ -44.4s 21.5 m (4) EC
+ 181 1/2- -43.6s 105 m (3) EC
+ 181m (7/2)- -43.5s 2.7 m (1) EC
+ 182 0+ -44.54 22.10 h (25) EC
+ 183 9/2+ -43.7s 13.0 h (5) EC
+ 183m 1/2- -43.5s 9.9 h (3) EC 85%,IT 15%
+ 184 0+ -44.255 > 5.6E13 y
+ 185 1/2- -42.809 93.6 d (5) EC
+ 186 0+ -43.000 2.0E+15 y (11) A
+*187 1/2- -41.221 1.6% (1)
+*188 0+ -41.139 13.3% (2)
+*189 3/2- -38.988 16.1% (3)
+ 189m 9/2- -38.957 5.8 h (1) IT
+*190 0+ -38.708 26.4% (4)
+ 190m (10)- -37.003 9.9 m (1) IT
+ 191 9/2- -36.396 15.4 d (1) B-
+ 191m 3/2- -36.322 13.10 h (5) IT
+*192 0+ -35.882 41.0% (3)
+ 192m (10-) -33.867 5.9 s (1) IT > 87%,B- < 13%
+ 193 3/2- -33.396 30.11 h (1) B-
+ 194 0+ -32.436 6.0 y (2) B-
+ 195 -29.7 6.5 m B-
+ 196 0+ -28.30 34.9 m (2) B-
+77 Ir Iridium 52
+ 192.217 (3) (17C)
+ 22.42
+ 2446
+ 4428
+ +3,+4
+ 166 -13.5s > 5 ms A 99%
+ 167 -17.1s > 5 ms A,P
+ 168 -18.7s ? A
+ 169 -21.99 0.4 s (1) A ~100%,EC ,P
+ 170 -23.3s 1.05 s (15) A 75%,EC 25%
+ 171 -26.3s 1.5 s (1) A ~100%,EC ,P
+ 172 (3+) -27.3s 4.4 s (3) EC 98%,A ~ 2%
+ 172m (7+) -27.2s 2.0 s (1) EC 77%,A 23%
+ 173n (3/2+,5/2+ -30.1s 9.0 s (8) EC > 93%,A < 7%
+ 173m (11/2-) -30.1s 2.20 s (5) EC 88%,A 12%
+ 174 (3+) -30.9s 9 s (2) EC 99.6%,A 0.4%
+ 174m (7+) -30.7s 4.9 s (3) EC 97.48%,A 00.52%
+ 175 (5/2-) -33.4s 9 s (2) EC 99.15%,A 0.85%
+ 176 -34.0s 8 s (1) EC 97.9%,A 2.1%
+ 177 (5/2-) -36.2s 30 s (2) EC 99.94%,A 0.06%
+ 178 -36.3s 12 s (2) EC
+ 179 (5/2)- -38.1s 79 s (1) EC
+ 180 -38.0s 1.5 m (1) EC
+ 181 (5/2)- -39.5s 4.90 m (15) EC
+ 182 (5+) -38.9 15 m (1) EC
+ 183 5/2- -40.2s 57 m (4) EC
+ 184 5- -39.7 3.09 h (3) EC
+ 185 5/2- -40.4s 14.4 h (1) EC
+ 186 5+ -39.17 16.64 h (3) EC
+ 186m 2- -39.17 2.0 h (1) EC,IT > 0%
+ 187 3/2+ -39.718 10.5 h (3) EC
+ 187m 9/2- -39.532 30.3 ms (6) IT
+ 188 1- -38.329 41.5 h (5) EC
+ 188m -38.329 4.2 ms (2) IT
+ 189 3/2+ -38.46 13.2 d (1) EC
+ 189m 11/2- -38.08 13.3 ms (3) IT
+ 189n (25/2+) -36.12 3.7 ms (2) IT
+ 190 (4)+ -36.7 11.78 d (10) EC
+ 190m (7)+ -36.7 1.2 h IT
+ 190n (11)- -36.5 3.25 h (20) EC 94.4%,IT 5.6%
+*191 3/2+ -36.71 37.3% (5)
+ 191m 11/2- -36.539 4.94 s (3) IT
+ 191n -34.663 5.5 s (7) IT
+ 192 4(+) -34.836 73.830 d (18) B- 95.24%,EC 4.76%
+ 192m 1(-) -34.779 1.45 m (5) IT 99.98%,B- 0.02%
+ 192n (9) -34.681 241 y (9) IT
+*193 3/2+ -34.537 62.7% (5)
+ 193m 11/2- -34.457 10.53 d (4) IT
+ 194 1- -32.532 19.15 h (3) B-
+ 194m (10,11) -32.342 171 d (11) B-
+ 195 3/2+ -31.693 2.5 h (2) B-
+ 195m 11/2- -31.593 3.8 h (2) B- 95%,IT 5%
+ 196 (0-) -29.45 52 s (1) B-
+ 196m (10,11-) -29.04 1.40 h (2) B- ~100%,IT < 0.3%
+ 197 3/2+ -28.28 5.8 m (5) B-
+ 197m 11/2- -28.17 8.9 m (3) B- 99.75%,IT 0.25%
+ 198 -25.8s 8 s (1) B-
+78 Pt Platinum 42
+ 195.08 (3)
+ 21.45 c
+ 1768.4
+ 3825
+ +2,+4
+ 168 0+ -11.1s ? A
+ 169 -12.6s 2.5 ms (+25-10) A
+ 170 0+ -16.5s 6 ms (+5-2) A
+ 171 -17.6s 25 ms (9) A ~ 99%,EC ~ 1%
+ 172 0+ -21.15 0.104 s (7) A 94%,EC 6%
+ 173 -21.9 342 ms (18) A 84%,EC 16%
+ 174 0+ -25.32 0.90 s (1) A 83%,EC 17%
+ 175 -25.8s 2.52 s (8) A 64%,EC 36%
+ 176 0+ -28.9s 6.33 s (15) EC 62%,A 38%
+ 177 (5/2-) -29.4s 11 s (1) EC 94.4%,A 5.6%
+ 178 0+ -31.9s 21.1 s (6) EC 92.3%,A 7.7%
+ 179 1/2- -32.3s 21.2 s (4) EC 99.76%,A 0.24%
+ 180 0+ -34.3s 52 s (3) EC,A ~ 0.3%
+ 181 1/2- -34.3s 51 s (5) EC,A ~ 0.06%
+ 182 0+ -36.1 2.2 m (1) EC 99.96%,A 0.04%
+ 183 1/2- -35.7s 6.5 m (10) EC,A ~1.3E-3%
+ 183m (7/2)- -35.6s 43 s (5) EC,A <4.0E-4%
+ 184 0+ -37.4s 17.3 m (2) EC,A ~0.001%
+ 184m 8- -35.5s 1.01 ms (5) IT
+ 185 9/2+ -36.6s 70.9 m (24) EC,A ?%
+ 185m 1/2- -36.5s 33.0 m (8) EC > 98%,IT < 2%
+ 186 0+ -37.79 2.0 h (1) EC,A ~1.4E-4%
+ 187 3/2- -36.6s 2.35 h (3) EC
+ 188 0+ -37.823 10.2 d (3) EC,A 2.6E-5%
+ 189 3/2- -36.49 10.87 h (12) EC
+ 190 0+ -37.325 6.5E11 y (3) A
+ 191 3/2- -35.691 2.96 d (4) EC
+*192 0+ -36.296 0.79% (6)
+ 193 1/2- -34.480 50 y (9) EC
+ 193m 13/2+ -34.330 4.33 d (3) IT
+*194 0+ -34.779 32.9% (6)
+*195 1/2- -32.813 33.8% (6)
+ 195m 13/2+ -32.554 4.02 d (1) IT
+*196 0+ -32.664 25.3% (6)
+ 197 1/2- -30.439 19.8915 h (19) B-
+ 197m 13/2+ -30.039 95.41 m (18) IT 96.7%,B- 3.3%
+*198 0+ -29.924 7.2% (2)
+ 199 5/2- -27.409 30.80 m (21) B-
+ 199m (13/2)+ -26.985 13.6 s (4) IT
+ 200 0+ -26.62 12.5 h (3) B-
+ 201 (5/2-) -23.74 2.5 m (1) B-
+ 202 0+ 44 h (15) B-
+79 Au Gold 52
+ 196.96655 (2)
+ ~19.3 c
+ 1064.18
+ 2856
+ +1,+3
+ 171 A ,P
+ 172 -9.2s 4 ms (1) A,P < 2%
+ 173 -12.7 59 ms (+45-18) A
+ 174 -14.0s 120 ms (20) A >0%
+ 175 -17.1s 200 ms (22) A 94%,EC 6%
+ 176 -18.4s 1.25 s (30) A ,EC
+ 177 -21.2s 1.18 s (7) EC >= 60%,A <= 40%
+ 178 -22.4s 2.6 s (5) EC <= 60%,A >= 40%
+ 179 -24.9s 7.1 s (3) EC 78%,A 22%
+ 180 -25.7s 8.1 s (3) EC <= 98.2%,A >= 1.8%
+ 181 5/2- -28.0s 11.4 s (5) EC 98.5%,A 1.5%
+ 182 -28.3s 15.6 s (4) EC 99.87%,A 0.13%
+ 183 (5/2)- -30.2s 42.0 s (12) EC 99.64%,A 0.36%
+ 184 5+ -30.2s 12.0 s (2) EC
+ 184m 2+ -30.2s 53.0 s (14) EC 99.98%,A 0.02%
+ 185 5/2- -31.9s 4.25 m (6) EC 99.74%,A 0.26%
+ 185m -31.9s 6.8 m (3) EC,IT
+ 186 3- -31.7 10.7 m (5) EC
+ 187 1/2+ -33.0s 8.4 m (3) EC,A 3.0E-3%
+ 187m 9/2- -32.9s 2.3 s (1) IT
+ 188 1(-) -32.52s 8.84 m (6) EC
+ 189 1/2+ -33.6s 28.7 m (3) EC,A <3.0E-5%
+ 189m 11/2- -33.4s 4.59 m (11) EC,IT > 0%
+ 190 1- -32.88 42.8 m (10) EC,A <1.0E-6%
+ 190m (11-) -32.88 125 ms (20) IT ?%
+ 191 3/2+ -33.86 3.18 h (8) EC
+ 191m (11/2-) -33.59 0.92 s (11) IT
+ 192 1- -32.78 4.94 h (9) EC
+ 192m (11-) -32.78 160 ms (20) IT ?%
+ 193 3/2+ -33.412 17.65 h (15) EC
+ 193m 11/2- -33.122 3.9 s (3) IT 99.97%,EC ~ 0.03%
+ 194 1- -32.29 38.02 h (10) EC
+ 194m (5+) -32.18 600 ms (8) IT
+ 194n (11-) -31.81 420 ms (10) IT
+ 195 3/2+ -32.586 186.10 d (5) EC
+ 195m 11/2- -32.267 30.5 s (2) IT
+ 196 2- -31.158 6.183 d (10) EC 92.5%,B- 7.5%
+ 196m 5+ -31.073 8.1 s (2) IT
+ 196n 12- -30.562 9.7 h (1) IT
+*197 3/2+ -31.158 100%
+ 197m 11/2- -30.749 7.73 s (6) IT
+ 198 2- -29.598 2.69517 d (21) B-
+ 198m (12-) -28.786 2.27 d (2) IT
+ 199 3/2+ -29.111 3.139 d (7) B-
+ 199m (11/2)- -28.562 0.44 ms (3) IT
+ 200 1(-) -27.28 48.4 m (3) B-
+ 200m 12- -26.31 18.7 h (5) B- 82%,IT 18%
+ 201 3/2+ -26.40 26 m (1) B-
+ 202 (1-) -24.4 28.8 s (19) B-
+ 203 3/2+ -23.14 60 s (6) B-
+ 204 (2-) -20.9s 39.8 s (9) B-
+ 205 3/2+ 31 s (2) B-
+80 Hg Mercury 42
+ 200.59 (2)
+ 13.546 c
+ -38.83
+ 356.73
+ +1,+2
+ 175 -8.2s 20 ms (+40-13) A
+ 176 0+ -11.80 34 ms (+18-9) A ~100%
+ 177 -12.7 0.130 s (5) A 85%,EC 15%
+ 178 0+ -16.32 0.254 s (19) A ~ 70%,EC ~ 30%
+ 179 -17.0s 1.09 s (4) A ~ 53%,EC ~ 47%
+ 180 0+ -20.2s 3.0 s (2) EC 51%,A 49%
+ 181 1/2(-) -20.7s 3.6 s (3) EC 64%,A 36%
+ 182 0+ -23.5s 10.83 s (6) EC 84.8%,A 15.2%
+ 183 1/2- -23.9s 9.4 s (7) EC 74.5%,A 25.5%
+ 184 0+ -26.2s 30.6 s (3) EC 98.89%,A 1.11%
+ 185 1/2- -26.1s 49.1 s (10) EC 94%,A 6%
+ 185m 13/2+ -26.0s 21.6 s (15) IT 54%,EC 46%
+ 186 0+ -28.4 1.38 m (7) EC 99.98%,A 0.02%
+ 187 13/2+ -28.1s 2.4 m (3) EC,A >1.2E-4%
+ 187m 3/2- -28.1s 1.9 m (3) EC,A >2.5E-4%
+ 188 0+ -30.2s 3.25 m (15) EC,A 3.7E-5%
+ 189 3/2- -29.7s 7.6 m (1) EC,A <3.0E-5%
+ 189m 13/2+ -29.7s 8.6 m (1) EC,A <3.0E-5%
+ 190 0+ -31.4s 20.0 m (5) EC,A <5.0E-5%
+ 191 (3/2-) -30.68 49 m (10) EC
+ 191m 13/2+ -30.68 50.8 m (15) EC
+ 192 0+ -32.1s 4.85 h (20) EC
+ 193 3/2- -31.07 3.80 h (15) EC
+ 193m 13/2+ -30.93 11.8 h (2) EC 92.9%,IT 7.1%
+ 194 0+ -32.25 520 y (32) EC
+ 195 1/2- -31.08 9.9 h (5) EC
+ 195m 13/2+ -30.90 41.6 h (8) IT 54.2%,EC 45.8%
+*196 0+ -31.844 0.15% (1)
+ 197 1/2- -30.558 64.14 h (5) EC
+ 197m 13/2+ -30.259 23.8 h (1) IT 91.4%,EC 8.6%
+*198 0+ -30.971 9.97% (8)
+*199 1/2- -29.564 16.87% (10)
+ 199m 13/2+ -29.032 42.6 m (2) IT
+*200 0+ -29.520 23.10% (16)
+*201 3/2- -27.679 13.18% (8)
+*202 0+ -27.362 29.86% (20)
+ 203 5/2- -25.284 46.612 d (18) B-
+*204 0+ -24.708 6.87% (4)
+ 205 1/2- -22.304 5.2 m (1) B-
+ 206 0+ -20.96 8.15 m (10) B-
+ 207 (9/2+) -16.3 2.9 m (2) B-
+ 208 0+ 42 m (+23-12) B-
+81 Tl Thallium 55
+ 204.3833 (2)
+ 11.85 c
+ 304
+ 1473
+ +1,+3
+ 177 -2.9s < 1 us
+ 179 -7.8s 0.16 s (+9-4) A ~100%
+ 179m (9/2-) -7.8s 1.4 ms (5) A ~100%
+ 180 -9.1s 1.9 s (9) EF ~1E-04%,A
+ 181 (1/2+) -12.2s 3.4 s (6) EC ?%
+ 182 (7+) -13.4s 3.1 s (10) EC > 96%,A < 4%
+ 183 (1/2+) -16.2s 6.9 s (7) EC > 0%
+ 183m (9/2-) -15.7s 60 ms (15) IT ?%,A <0.01%
+ 184 (2+) -17.0s 11 s (1) EC 97.9%,A 2.1%
+ 185 (1/2+) -19.5s 19.5 s (5) EC
+ 185m (9/2-) -19.0s 1.83 s (12) A ,IT
+ 186 (7+) -20.0s 27.5 s (10) EC,A 6.0E-4%
+ 186m (10-) -19.6s 2.9 s (2) IT
+ 187 (1/2+) -22.2s ~ 51 s EC,A > 0%
+ 187m (9/2-) -21.9s 15.60 s (12) EC,IT,A > 0%
+ 188n (2-) -22.4s 71 s (2) EC
+ 188m (7+) -22.4s 71 s (1) EC
+ 189 (1/2+) -24.5s 2.3 m (2) EC
+ 189m (9/2-) -24.2s 1.4 m (1) EC,IT < 4%
+ 190n (2)- -24.4s 2.6 m (3) EC
+ 190m (7+) -24.4s 3.7 m (3) EC
+ 191 (1/2+) -26.2s ? EC ?%
+ 191m 9/2(-) -25.9s 5.22 m (16) EC
+ 192n (2-) -25.9s 9.6 m (4) EC
+ 192m (7+) -25.9s 10.8 m (2) EC
+ 193 1/2(+) -27.4s 21.6 m (8) EC
+ 193m (9/2-) -27.1s 2.11 m (15) IT 75%,EC 25%
+ 194 2- -27.0s 33.0 m (5) EC,A <1.0E-7%
+ 194m (7+) -27.0s 32.8 m (2) EC
+ 195 1/2+ -28.3s 1.16 h (5) EC
+ 195m 9/2- -27.8s 3.6 s (4) IT
+ 196 2- -27.5s 1.84 h (3) EC
+ 196m (7+) -27.1s 1.41 h (2) EC 95.5%,IT 4.5%
+ 197 1/2+ -28.37 2.84 h (4) EC
+ 197m 9/2- -27.77 0.54 s (1) IT
+ 198 2- -27.51 5.3 h (5) EC
+ 198m 7+ -26.97 1.87 h (3) EC 54%,IT 46%
+ 198n (10-) -26.77 32.1 ms (10) IT
+ 199 1/2+ -28.12 7.42 h (8) EC
+ 199m 9/2- -27.37 28.4 ms (2) IT
+ 200 2- -27.064 26.1 h (1) EC
+ 200m 7+ -26.310 34.3 ms (10) IT
+ 201 1/2+ -27.20 72.912 h (17) EC
+ 201m (9/2-) -26.28 2.035 ms (7) IT
+ 202 2- -26.00 12.23 d (2) EC
+*203 1/2+ -25.776 29.524% (14)
+ 204 2- -24.360 3.78 y (2) B- 97.1%,EC 2.9%
+*205 1/2+ -23.835 70.476% (14)
+ 206 0- -22.268 4.199 m (15) B-
+ 206m (12-) -19.625 3.74 m (3) IT
+ 207 1/2+ -21.045 4.77 m (2) B-
+ 207m 11/2- -19.697 1.33 s (11) IT
+ 208 5(+) -16.763 3.053 m (4) B-
+ 209 (1/2+) -13.648 2.20 m (7) B-
+ 210 (5+) -9.26 1.30 m (3) B-,BN 7.0E-3%
+82 Pb Lead 47
+ 207.2
+ 11.35 c
+ 327.46
+ 1749
+ +2,+4
+ 181 (13/2+) -2.9 45 ms (20) A,EC ~ 2%
+ 182 0+ -6.82 55 ms (+40-35) A
+ 183 (1/2-) -7.5s 300 ms (80) A ~94%,EC ~ 6%
+ 184 0+ -11.0s 0.55 s (6) A ,EC ?%
+ 185 -11.6s 4.1 s (3) A
+ 186 0+ -14.6s 4.7 s (1) A
+ 187m -15.0s 15.2 s (3) A ,EC
+ 187n (13/2+) -15.0s 18.3 s (3) EC > 90%,A < 10%
+ 188 0+ -17.6s 25.5 s (1) EC 78%,A 22%
+ 189 -17.8s 51 s (3) EC > 99%,A ~ 0.4%
+ 190 0+ -20.3 1.2 m (1) EC 99.1%,A 0.9%
+ 191 (3/2-) -20.3s 1.33 m (8) EC 99.99%,A 0.01%
+ 191m (13/2+) -20.2s 2.18 m (8) EC,A ~ 0.02%
+ 192 0+ -22.6s 3.5 m (1) EC 99.99%,A 6.2E-3%
+ 193 (3/2-) -22.3s ? EC
+ 193m (13/2+) -22.2s 5.8 m (2) EC
+ 194 0+ -24.2s 12.0 m (5) EC,A 7.3E-6%
+ 195 3/2- -23.8s ~ 15 m EC
+ 195m 13/2+ -23.6s 15.0 m (12) EC
+ 196 0+ -25.4s 37 m (3) EC ~100%,A <=3.0E-5%
+ 197 3/2- -24.8s 8 m (2) EC
+ 197m 13/2+ -24.5s 43 m (1) EC 81%,IT 19%
+ 198 0+ -26.10s 2.40 h (10) EC
+ 199 3/2- -25.24 90 m (10) EC
+ 199m 13/2+ -24.81 12.2 m (3) IT 93%,EC 7%
+ 200 0+ -26.25 21.5 h (4) EC
+ 201 5/2- -25.29 9.33 h (3) EC
+ 201m 13/2+ -24.66 61 s (2) IT > 99%,EC < 1%
+ 202 0+ -25.948 52.5E+3 y (28) EC,A < 1%
+ 202m 9- -23.778 3.53 h (1) IT 90.5%,EC 9.5%
+ 203 5/2- -24.801 51.873 h (9) EC
+ 203m 13/2+ -23.976 6.3 s (2) IT
+ 203n 29/2- -21.852 0.48 s (2) IT
+ 204 0+ -25.124 1.4E+17 y GE A ?%
+ 204m 9- -22.938 67.2 m (3) IT
+ 205 5/2- -23.784 1.53E+7 y (7) EC
+ 205m 13/2+ -22.770 5.54 ms (10) IT
+*206 0+ -23.801 24.1% (1)
+*207 1/2- -22.467 22.1% (1)
+ 207m 13/2+ -20.834 0.806 s (6) IT
+*208 0+ -21.764 52.4% (1)
+ 209 9/2+ -17.628 3.253 h (14) B-
+ 210 0+ -14.742 22.3 y (2) B-,A 1.9E-6%
+ 211 9/2+ -10.496 36.1 m (2) B-
+ 212 0+ -7.557 10.64 h (1) B-
+ 213 (9/2+) -3.17s 10.2 m (3) B-
+ 214 0+ -0.188 26.8 m (9) B-
+83 Bi Bismuth 56
+ 208.98038 (2)
+ 9.747 c
+ 271.40
+ 1564
+ +3,+5
+ 187 (9/2-) -6.1s 35 ms (4) A > 50%
+ 187m (1/2+) -6.0s 0.8 ms (6) A > 50%
+ 188n -7.3s 44 ms (3) A ,EC
+ 188m -7.3s 0.21 s (9) A ,EC
+ 189 (9/2-) -9.8s 680 ms (30) A > 50%,EC < 50%
+ 189m (1/2+) -9.7s 7.0 ms (2) A > 50%,EC < 50%
+ 190n (3+) -10.7s 5.7 s (8) A ~ 90%,EC ~ 10%
+ 190m (10-) -10.7s 5.9 s (6) A 70%,EC 30%
+ 191 (9/2-) -13.0s 12 s (1) A 60%,EC 40%
+ 191m (1/2+) -12.7s 150 ms (15) A 75%,EC <= 25%
+ 192 (3+) -13.6s 34.6 s (9) EC 88%,A 12%
+ 192m (10-) -13.5s 40.6 s (4) EC 90%,A 10%
+ 193 (9/2-) -15.8s 67 s (3) EC 95%,A 5%
+ 193m (1/2+) -15.5s 3.2 s (7) A 90%,EC ~ 10%
+ 194 (3+) -16.1s 95 s (3) EC,A 0.46%
+ 194m (6+,7+) -16.1s 92 s (5) EC 99.93%,A 0.07%
+ 194n (10-) -16.1s 115 s (4) EC 99.8%,A 0.2%
+ 195 (9/2-) -17.9s 183 s (4) EC 99.97%,A 0.03%
+ 195m (1/2+) -17.5s 87 s (1) EC 67%,A 33%
+ 196 (3+) -18.1 308 s (12) EC ~100%,A 1.2E-3%
+ 196m (7+) -17.9 0.6 s (5) EC > 0%
+ 196n (10-) -17.8 240 s (3) EC 74.2%,IT 25.8%
+ 197 (9/2-) -19.6 9.33 m (50) EC,A 1.0E-4%
+ 197m (1/2+) -19.1 5.04 m (16) A 55%,EC 45%,IT < 0.3%
+ 198 (2+,3+) -19.5 10.3 m (3) EC
+ 198m (7+) -19.5 11.6 m (3) EC
+ 198n (10-) -19.3 7.7 s (5) IT
+ 199 9/2- -20.89 27 m (1) EC
+ 199m (1/2+) -20.21 24.70 m (15) EC >= 98%,IT <= 2%
+ 200 7+ -20.36 36.4 m (5) EC
+ 200m (2+) -20.36 31 m (2) EC > 90%,IT < 10%
+ 200n (10-) -19.93 0.40 s (5) IT
+ 201 9/2- -21.45 108 m (3) EC,A <1.0E-4%
+ 201m 1/2+ -20.60 59.1 m (6) EC > 93%,IT <= 6.8%
+ 202 5+ -20.79 1.72 h (5) EC,A <1E-05%
+ 203 9/2- -21.55 11.76 h (5) EC,A ~1.0E-5%
+ 203m 1/2+ -20.45 303 ms (5) IT
+ 204 6+ -20.69 11.22 h (10) EC
+ 204m 10- -19.88 13.0 ms (1) IT
+ 204n (17+) -17.85 1.07 ms (3) IT
+ 205 9/2- -21.076 15.31 d (4) EC
+ 206 6(+) -20.043 6.243 d (3) EC
+ 207 9/2- -20.069 31.55 y (5) EC
+ 208 (5)+ -18.884 3.68E+5 y (4) EC
+ 208m (10)- -17.313 2.58 ms (4) IT
+*209 9/2- -18.273 100%
+ 210 1- -14.806 5.013 d (5) B-,A 1.3E-4%
+ 210m 9- -14.535 3.04E+6 y (6) A
+ 211 9/2- -11.869 2.14 m (2) A 99.72%,B- 0.28%
+ 212 1(-) -8.131 60.55 m (6) B- 64.06%,A 35.94%
+ 212m (9-) -7.881 25.0 m (2) A 67%,B- 33%
+ 212n -6.221 7.0 m (3) B- ~100%
+ 213 9/2- -5.241 45.59 m (6) B- 97.91%,A 2.09%
+ 214 1- -1.21 19.9 m (4) B- 99.98%,A 0.02%
+ 215 1.71 7.6 m (2) B-
+ 216 5.77s 3.6 m (4) B-
+84 Po Polonium 39
+ (209)
+ 9.32 r
+ 254
+ -
+ +2,+4
+ 190 0+ -4.6s 9.6 ms (+47-44) A
+ 191 -5.1s 15.5 ms (+60-35) A
+ 192 0+ -7.9s 0.034 s (3) A ~ 99%,EC ~ 1%
+ 193 -8.3s 0.45 s (4) A
+ 193m -8.3s 0.24 s (1) A
+ 194 0+ -10.9 0.392 s (4) A
+ 195 (3/2-) -11.1s 4.64 s (9) A 75%,EC 25%
+ 195m (13/2+) -10.9s 1.92 s (2) A ~ 90%,EC ~ 10%
+ 196 0+ -13.5s 5.8 s (2) A ~ 98%,EC ~ 2%
+ 197 (3/2-) -13.4s 53.6 s (10) EC 56%,A 44%
+ 197m (13/2+) -13.2s 25.8 s (2) A 84%,EC 16%,IT 0.01%
+ 198 0+ -15.5s 1.76 m (3) A 57%,EC 43%
+ 199 (3/2-) -15.3s 5.48 m (16) EC 92.5%,A 7.5%
+ 199m 13/2+ -15.0s 4.17 m (4) EC 73.5%,A 24%
+ 200 0+ -17.0s 11.5 m (1) EC 88.9%,A 11.1%
+ 201 3/2- -16.6s 15.3 m (2) EC 98.4%,A 1.6%
+ 201m 13/2+ -16.1s 8.9 m (2) IT 56%,EC 41%
+ 202 0+ -17.98s 44.7 m (5) EC 98%,A 2%
+ 203 5/2- -17.31 36.7 m (5) EC 99.89%,A 0.11%
+ 203m 13/2+ -16.67 45 s (2) IT ~100%,A ~ 0.04%
+ 204 0+ -18.34 3.53 h (2) EC 99.34%,A 0.66%
+ 205 5/2- -17.54 1.66 h (2) EC 99.96%,A 0.04%
+ 206 0+ -18.197 8.8 d (1) EC 94.55%,A 5.45%
+ 207 5/2- -17.160 5.80 h (2) EC 99.98%,A 0.02%
+ 207m 19/2- -15.777 2.79 s (8) IT
+ 208 0+ -17.484 2.898 y (2) A,EC
+ 209 1/2- -16.380 102 y (5) A 99.52%,EC 0.48%
+ 210 0+ -15.969 138.376 d (2) A
+ 211 9/2+ -12.448 0.516 s (3) A
+ 211m (25/2+) -10.986 25.2 s (6) A 99.98%,IT 0.02%
+ 212 0+ -10.385 0.299 us (2) A
+ 212m (18+) -7.463 45.1 s (6) A 99.93%,IT 0.07%
+ 213 9/2+ -6.667 4.2 us (8) A
+ 214 0+ -4.484 164.3 us (20) A
+ 214m 0+ -3.069 99 PS (3) IT 99.86%,A 0.14%
+ 215 9/2+ -0.544 1.781 ms (4) A,B- 2.3E-4%
+ 216 0+ 1.774 0.145 s (2) A
+ 217 5.91s < 10 s A > 95%,B- < 5%
+ 218 0+ 8.351 3.10 m (1) A 99.98%,B- 0.02%
+85 At Astatine 40
+ (210)
+ -
+ 302
+ -
+ -
+ 194 -0.7s 0.18 s (8) A
+ 195 -3.2s ? A > 75%,EC < 25%
+ 196 -4.0s 0.3 s (1) A > 0%
+ 197 (9/2-) -6.3s 0.35 s (4) A 96%,EC 4%
+ 197m (1/2+) -6.2s 3.7 s (25) A,EC
+ 198 (3+) -6.7s 4.2 s (3) A 90%,EC 10%
+ 198m (10-) -6.6s 1.0 s (2) A 84%,EC 16%
+ 199 (9/2-) -8.7s 7.2 s (5) A 90%,EC 10%
+ 200 (3+) -9.0 43 s (1) A 57%,EC 43%
+ 200m (7+) -8.9 47 s (1) EC ~ 57%,A 43%
+ 200n (10-) -8.7 3.5 s (2) IT ~ 84%,A ~ 10.5%
+ 201 (9/2-) -10.7 89 s (3) A 71%,EC 29%
+ 202 (2+,3+) -10.8 184 s (1) EC <= 87%,A >= 13%
+ 202m (7+) -10.7 182 s (2) EC 91.3%,A 8.7%
+ 202n (10-) -10.3 0.46 s (5) IT ,A 9.6E-2%
+ 203 9/2- -12.26 7.4 m (2) EC 69%,A 31%
+ 204 7+ -11.87 9.2 m (2) EC 96.2%,A 3.8%
+ 204m (10-) -11.28 108 ms (10) IT
+ 205 9/2- -13.01 26.2 m (5) EC 90%,A 10%
+ 206 (5)+ -12.48 30.0 m (6) EC 99.11%,A 0.89%
+ 207 9/2- -13.25 1.80 h (4) EC 91.4%,A 8.6%
+ 208 6+ -12.51 1.63 h (3) EC 99.45%,A 0.55%
+ 209 9/2- -12.894 5.41 h (5) EC 95.9%,A 4.1%
+ 210 (5)+ -11.987 8.1 h (4) EC 99.82%,A 0.18%
+ 211 9/2- -11.661 7.214 h (7) EC 58.2%,A 41.8%
+ 212 (1-) -8.630 0.314 s (2) A,EC < 0.03%
+ 212m (9-) -8.408 0.119 s (3) A > 99%,IT < 1%
+ 213 9/2- -6.594 125 NS (6) A
+ 214 1- -3.394 558 NS (10) A
+ 214m -3.335 265 NS (30) A
+ 214n 9- -3.163 760 NS (15) A
+ 215 9/2- -1.266 0.10 ms (2) A
+ 216 1(-) 2.24 0.30 ms (3) A,EC <0.006%,B- <3E-07%
+ 217 9/2- 4.386 32.3 ms (4) A 99.99%,B- 0.01%
+ 218 (2-) 8.09 1.6 s (4) A 99.9%,B- 0.1%
+ 219 10.52 56 s (3) A ~ 97%,B- ~ 3%
+ 220 14.25s 3.71 m (4) B-
+ 221 16.673C 2.3 m (2) B-
+ 222 54 s (10) B-
+ 223 23.396C 50 s (7) B-
+86 Rn Radon 37
+ (222)
+ 0.00973
+ -71
+ -61.7
+ 0
+ 198 0+ -1.1 ? A ,EC
+ 198m 0+ -1.1 50 ms (9) A ,EC ,IT
+ 199 (3/2-) -1.6s 0.62 s (3) A 94%,EC 6%
+ 199m (13/2+) -1.6s 0.32 s (2) A 97%,EC 3%
+ 200 0+ -4.0s 1.06 s (2) A ~ 98%,EC ~ 2%
+ 201 (3/2-) -4.2s 7.0 s (4) A ~ 80%,EC ~ 20%
+ 201m (13/2+) -3.9s 3.8 s (4) A ~ 90%,EC ~ 10%
+ 202 0+ -6.3s 9.85 s (20) EC < 30%,A
+ 203 (3/2,5/2)- -6.2s 45 s (3) A 66%,EC 34%
+ 203m (13/2+) -5.9s 28 s (2) A ~ 80%,EC ~ 20%
+ 204 0+ -8.0s 1.24 m (3) A 73%,EC 27%
+ 205 5/2- -7.8s 2.8 m (1) EC 77%,A 23%
+ 206 0+ -9.17s 5.67 m (17) A 62%,EC 38%
+ 207 5/2- -8.64 9.25 m (17) EC 79%,A 21%
+ 208 0+ -9.66 24.35 m (14) A 62%,EC 38%
+ 209 5/2- -8.96 28.5 m (10) EC 83%,A 17%
+ 210 0+ -9.61 2.4 h (1) A 96%,EC 4%
+ 211 1/2- -8.770 14.6 h (2) EC 72.7%,A 27.4%
+ 212 0+ -8.674 23.9 m (12) A
+ 213 (9/2+) -5.712 25.0 ms (2) A
+ 214 0+ -4.335 0.27 us (2) A
+ 214m 6+ -2.892 0.7 NS (3) IT,A > 0%
+ 214n 8+ -2.710 6.5 NS (30) IT ~ 90%,A ~ 10%
+ 215 9/2+ -1.184 2.30 us (10) A
+ 216 0+ 0.240 45 us (5) A
+ 217 9/2+ 3.647 0.54 ms (5) A
+ 218 0+ 5.204 35 ms (5) A
+ 219 5/2+ 8.826 3.96 s (1) A
+ 220 0+ 10.604 55.6 s (1) A
+ 221 7/2(+) 14.49s 25 m (2) B- 78%,A 22%
+ 222 0+ 16.366 3.8235 d (3) A
+ 223 7/2 20.183C 23.2 m (4) B-
+ 224 0+ 22.461C 107 m (3) B-
+ 225 7/2- 26.537C 4.5 m (3) B-
+ 226 0+ 29.021C 6.0 m (5) B-
+ 227 33.160C 22.5 s (7) B-
+ 228 0+ 65 s (2) B-
+87 Fr Francium 39
+ (223)
+ -
+ 27
+ -
+ +1
+ 201 (9/2-) 3.7s 48 ms (15) A,EC < 1%
+ 202 (3+) 3.1s 0.34 s (4) A <= 97%,EC >= 3%
+ 202m (10-) 3.2s ~ 0.34 s A <= 94%,EC >= 6%
+ 203 (9/2-) 1.0s 0.55 s (2) A ~ 95%,EC ~ 5%
+ 204 (3+) 0.6 1.7 s (3) A ~ 80%,EC ~ 20%
+ 204m (7+) 0.6 2.6 s (3) A
+ 204n (10-) 0.9 ~ 1 s A,IT
+ 205 (9/2-) -1.2 3.85 s (10) A,EC < 1%
+ 206 (2+,3+) -1.4 15.9 s (2) A ,EC
+ 206m (7+) -1.4 15.9 s ? A <= 84%
+ 206n (10-) -0.7 0.7 s (1) A ,IT ?%
+ 207 9/2- -2.93 14.8 s (1) A 95%,EC 5%
+ 208 7+ -2.67 59.1 s (3) A 90%,EC 10%
+ 209 9/2- -3.80 50.0 s (3) A 89%,EC 11%
+ 210 6+ -3.35 3.18 m (6) A 60%,EC 40%
+ 211 9/2- -4.16 3.10 m (2) A > 80%,EC < 20%
+ 212 5+ -3.56 20.0 m (6) EC 57%,A 43%
+ 213 9/2- -3.564 34.6 s (3) A 99.45%,EC 0.55%
+ 214 (1-) -0.974 5.0 ms (2) A
+ 214m (8-) -0.852 3.35 ms (5) A
+ 215 9/2- 0.304 86 NS (5) A
+ 216 (1-) 2.97 0.70 us (2) A,EC <2E-07%
+ 217 9/2- 4.301 16 us (2) A
+ 218 (1-) 7.046 1.0 ms (6) A
+ 218m 7.132 22.0 ms (5) A
+ 219 9/2- 8.608 20 ms (2) A
+ 220 1+ 11.469 27.4 s (3) A 99.65%,B- 0.35%
+ 221 5/2- 13.269 4.9 m (2) A,B- < 0.1%,14C 9E-13%
+ 222 2- 16.34 14.2 m (3) B-
+ 223 3/2(-) 18.379 22.00 m (7) B- 99.99%,A 6.0E-3%
+ 224 1(-) 21.64 3.30 m (10) B-
+ 225 3/2- 23.85 4.0 m (2) B-
+ 226 1 27.3 48 s (1) B-
+ 227 1/2+ 29.66 2.47 m (3) B-
+ 228 2- 33.3 39 s (1) B-
+ 229 (1/2+) 36.159C 50.2 s (4) B-
+ 230 40.011C 19.1 s (5) B-
+ 231 43.025C 17.5 s (8) B-
+ 232 5 s (1) B-
+88 Ra Radium 33
+ (226)
+ 5?
+ 700
+ -
+ +2
+ 204 0+ 6.0s 45 ms (+55-21) A
+ 205 5.8s 0.22 s (6) A ,EC
+ 206 0+ 3.5s 0.24 s (2) A ~100%
+ 207 (5/2-,3/2- 3.5s 1.3 s (2) A ~ 90%,EC ~ 10%
+ 207m (13/2+) 3.9s 55 ms (10) IT 85%,A 15%,EC ~ 0.35%
+ 208 0+ 1.7s 1.3 s (2) A 95%,EC 5%
+ 209 5/2- 1.8s 4.6 s (2) A ~ 90%,EC ~ 10%
+ 210 0+ 0.42s 3.7 s (2) A ~ 96%,EC ~ 4%
+ 211 5/2(-) 0.83 13 s (2) A > 93%,EC < 7%
+ 212 0+ -0.19 13.0 s (2) A ~ 90%,EC ~ 15%
+ 213 1/2- 0.32 2.74 m (6) A 80%,EC 20%
+ 213m 2.09 2.1 ms (1) IT ~ 99%,A ~ 1%
+ 214 0+ 0.08 2.46 s (3) A 99.94%,EC 0.06%
+ 215 (9/2+) 2.519 1.59 ms (9) A
+ 216 0+ 3.277 182 NS (10) A,EC
+ 217 (9/2+) 5.874 1.7 us (1) A
+ 218 0+ 6.64 15.6 us (1) A
+ 219 (7/2)+ 9.37 10 ms (3) A
+ 220 0+ 10.26 17 ms (2) A
+ 221 5/2+ 12.957 28 s (2) A,14C 1E-12%
+ 222 0+ 14.309 38.0 s (5) A,14C 2.3E-8%
+ 223 3/2+ 17.230 11.435 d (4) A,14C 6.4E-8%
+ 224 0+ 18.818 3.66 d (4) A,12C 4.3E-9%
+ 225 1/2+ 21.986 14.9 d (2) B-
+ 226 0+ 23.661 1600 y (7) A,14C 3E-9%
+ 227 3/2+ 27.171 42.2 m (5) B-
+ 228 0+ 28.935 5.75 y (3) B-
+ 229 5/2(+) 32.43 4.0 m (2) B-
+ 230 0+ 34.54 93 m (2) B-
+ 231 (7/2-,1/2+ 38.562C 103 s (3) B-
+ 232 0+ 41.092C 250 s (50) B-
+ 233 30 s (5) B-
+ 234 0+ 47.999C 30 s (10) B-
+89 Ac Actinium 31
+ (227)
+ 10.07 t
+ 1051
+ 3198
+ +3
+ 207 22 ms (+40-9) A
+ 208 (3+) 95 ms (+24-16) A ~ 99%
+ 208m (10-) 25 ms (+9-5) A ~ 90%
+ 209 (9/2-) 8.9 0.10 s (5) A ~ 99%,EC ~ 1%
+ 210 8.6 0.35 s (5) A ~ 96%,EC ~ 4%
+ 211 7.12 0.25 s (5) A ~100%
+ 212 7.27 0.93 s (5) A ~ 97%,EC ~ 3%
+ 213 6.13 0.80 s (5) A
+ 214 6.42 8.2 s (2) A >= 89%,EC <= 11%
+ 215 9/2- 6.01 0.17 s (1) A 99.91%,EC 0.09%
+ 216 (1-) 8.11 ~ 0.33 ms A
+ 216m (9-) 8.11 0.33 ms (2) A
+ 217 9/2- 8.69 69 NS (4) A,EC <= 2%
+ 218 10.83 1.06 us (9) A
+ 219 9/2- 11.56 11.8 us (15) A
+ 220 13.74 26.1 ms (5) A,EC 5E-04%
+ 221 14.51 52 ms (2) A
+ 222 (1-) 16.60 5.0 s (5) A 99%,EC <= 2%
+ 222m 16.60 63 s (4) A >= 88%,IT <= 10%
+ 223 (5/2-) 17.816 2.10 m (5) A 99%,EC 1%
+ 224 0- 20.221 2.9 h (2) EC 90.9%,A 9.1%
+ 225 (3/2-) 21.629 10.0 d (1) A
+ 226 (1) 24.302 29.4 h (1) B- 83%,EC 17%
+ 227 3/2- 25.846 21.773 y (3) B- 98.62%,A 1.38%
+ 228 3(+) 28.889 6.15 h (2) B-,A 5.5E-6%
+ 229 (3/2+) 30.67 62.7 m (5) B-
+ 230 (1+) 33.56 122 s (3) B-
+ 231 (1/2+) 35.91 7.5 m (1) B-
+ 232 (1+) 39.14 119 s (5) B-
+ 233 (1/2+) 41.603C 145 s (10) B-
+ 234 45.199C 44 s (7) B-
+90 Th Thorium 29
+ 232.03805 (2)
+ 11.72
+ 1750
+ 4788
+ +4
+ 210 0+ 9 ms+17-4 A
+ 211 37 ms+28-11 A
+ 212 0+ 12.0s 30 ms (+20-10) A,EC ~ 0.3%
+ 213 12.1s 140 ms (25) A
+ 214 0+ 10.67s 100 ms (25) A
+ 215 (1/2-) 10.92 1.2 s (2) A
+ 216 0+ 10.29 0.028 s (2) A,EC ~0.006%
+ 216 (8+,11-) 12.32 0.18 ms (4) IT ~ 97%,A ~ 3%
+ 217 (9/2+) 12.17 0.252 ms (7) A
+ 218 0+ 12.36 109 NS (13) A
+ 219 14.46 1.05 us (3) A
+ 220 0+ 14.65 9.7 us (6) A,EC 2E-07%
+ 221 (7/2+) 16.93 1.68 ms (6) A
+ 222 0+ 17.19 2.2 ms (2) A
+ 223 (5/2)+ 19.36 0.60 s (2) A
+ 224 0+ 19.99 1.05 s (2) A
+ 225 (3/2)+ 22.304 8.72 m (4) A ~ 90%,EC ~ 10%
+ 226 0+ 23.185 30.6 m (1) A
+ 227 (1/2+) 25.802 18.72 d (2) A
+ 228 0+ 26.763 1.9131 y (9) A,20O 1E-11%
+ 229 5/2+ 29.579 7880 y (120) A
+ 230 0+ 30.856 7.538E+4 y (30) A,SF <=5.E-11%
+ 231 5/2+ 33.810 25.52 h (1) B-,A ~1.0E-8%
+ 232 0+ 35.443 1.405E10 y (6) A,SF <1.0E-9%
+ 233 1/2+ 38.728 22.3 m (1) B-
+ 234 0+ 40.610 24.10 d (3) B-
+ 235 (1/2+) 44.25 7.1 m (2) B-
+ 236 0+ 46.706C 37.5 m (2) B-
+ 237 5.0 m (9) B-
+91 Pa Protactinium 28
+ (231)
+ 15.37 t
+ 1572
+ -
+ +4,+5
+ 213 5.3 ms (+40-16) A
+ 214 17 ms (3) A
+ 215 17.7 15 ms (4) A
+ 216 17.71 105 ms (12) A ~ 80%,EC ~ 20%
+ 217 17.04 3.4 ms (2) A
+ 217m 18.89 1.5 ms (2) A
+ 218 18.64 0.11 ms (2) A
+ 219 9/2- 18.52 53 NS (10) A
+ 220 20.37 0.78 us (16) A ?%
+ 221 9/2- 20.37 5.9 us (17) A
+ 222 22.05s 3.3 ms (3) A
+ 223 22.32 5 ms (1) A
+ 224 23.86 0.95 s (15) A 99.9%,EC 0.1%
+ 225 24.33 1.7 s (2) A
+ 226 26.01 1.8 m (2) A 74%,EC 26%
+ 227 (5/2-) 26.821 38.3 m (3) A 85%,EC 15%
+ 228 (3+) 28.874 22 h (1) EC 98.15%,A 1.85%
+ 229 (5/2+) 29.895 1.50 d (5) EC 99.52%,A 0.48%
+ 230 (2-) 32.166 17.4 d (5) EC 91.6%,B- 8.4%
+ 231 3/2- 33.420 32760 y (110) A,SF <=3.0E-10%
+ 232 (2-) 35.938 1.31 d (2) B-,EC 3.0E-3%
+ 233 3/2- 37.483 26.967 d (2) B-
+ 234 4+ 40.337 6.70 h (5) B-
+ 234m (0-) 40.411 1.17 m (3) B- 99.84%,IT 0.16%
+ 235 (3/2-) 42.32 24.5 m (2) B-
+ 236 1(-) 45.3 9.1 m (1) B-
+ 237 (1/2+) 47.64 8.7 m (2) B-
+ 238 (3-) 50.76 2.3 m (1) B-,SF <2.6E-6%
+92 U Uranium 26
+ 238.0289
+ ~18.95
+ 1135
+ 4131
+ +3,+4,+5,+6
+ 218 0+ 21.88s 1.5 ms (+73-7) A
+ 219 23.2s 42 us (+34-13) A
+ 222 0+ 24.3s 1.0 us (+10-4) A
+ 223 25.82 18 us (+10-5) A
+ 224 0+ 25.70 1.0 ms (4) A
+ 225 27.37 95 ms (15) A
+ 226 0+ 27.32 0.20 s (5) A
+ 227 (3/2+) 29.00 1.1 m (1) A
+ 228 0+ 29.22 9.1 m (2) A > 95%,EC < 5%
+ 229 (3/2+) 31.204 58 m (3) EC ~ 80%,A ~ 20%
+ 230 0+ 31.603 20.8 d A
+ 231 (5/2-) 33.78 4.2 d (1) EC
+ 231 (3/2+,5/2+ 33.78 4.2 d (1) A ~ 4E-3%
+ 232 0+ 34.601 68.9 y (4) A,Ne 9E-10%
+ 233 5/2+ 36.912 1.592E+5 y (2) A,SF <6.0E-9%
+ 234 0+ 38.140 2.455E+5 y (6) A,SF 1.7E-9%,Mg 1E-11%
+ 235 7/2- 40.913 703.8E+6 y (5) A,SF 7.0E-9%,Ne 8E-10%
+ 235m 1/2+ 40.913 ~ 25 m IT
+ 236 0+ 42.440 2.342E7 y (3) A,SF 9.6E-8%
+ 236m 42.440 121 NS (2) SF 0.013%
+ 237 1/2+ 45.385 6.75 d (1) B-
+ 238 0+ 47.305 4.468E+9 y (3) A,SF 0.5E-4%
+ 238m 0+ 47.305 267 NS (3) SF 0.015%
+ 239 5/2+ 50.570 23.45 m (2) B-
+ 240 0+ 52.708 14.1 h (1) B-,A
+ 242 0+ 58.830C 16.8 m (5) B-
+93 Np Neptunium 23
+ (237)
+ 20.25 c
+ 644
+ 3902
+ +3,+4,+5,+6
+ 226 32.7s 31 ms (8) A
+ 227 32.56 0.51 s (6) A
+ 228 33.7s 1.07 m (3) EC ,EF
+ 229 33.76 3.85 m (14) A > 50%,EC < 50%
+ 230 35.21 4.6 m (3) EC <= 97%,A >= 3%
+ 231 (5/2) 35.61 48.8 m (2) EC 98%,A 2%
+ 232 (4+) 37.30s 14.7 m (3) EC
+ 233 (5/2+) 38.1s 36.2 m (1) EC,A <=1.0E-3%
+ 234 (0+) 39.950 4.4 d (1) EC
+ 235 5/2+ 41.037 396.1 d (12) EC,A 2.6E-3%
+ 236 (6-) 43.38 154E+3 y (6) EC 87.3%,B- 12.5%
+ 236m 1 43.44 22.5 h (4) EC 52%,B- 48%
+ 237 5/2+ 44.867 2.144E+6 y (7) A,SF <= 2E-10%
+ 237m 47.667 45 NS (5) SF
+ 238 2+ 47.450 2.117 d (2) B-
+ 239 5/2+ 49.304 2.3565 d (4) B-
+ 240 (5+) 52.32 61.9 m (2) B-
+ 240m 1(+) 52.32 7.22 m (2) B- 99.89%,IT 0.11%
+ 241 (5/2+) 54.26 13.9 m (2) B-
+ 242 (1+) 57.4 2.2 m (2) B-
+ 242 (6) 57.4 5.5 m (1) B-
+ 243 (5/2-) 59.92 1.85 m (15) B-
+ 244 (7-) 63.45C 2.29 m (16)
+94 Pu Plutonium 25
+ (244)
+ 19.84 e
+ 640
+ 3228
+ +3,+4,+5,+6
+ 228 0+ ? A ,SF
+ 229 ? A
+ 230 0+ 36.92 ~ 200 s A
+ 232 0+ 38.36 34.1 m (7) EC 80%,A 20%
+ 233 40.05 20.9 m (4) EC 99.88%,A 0.12%
+ 234 0+ 40.338 8.8 h (1) EC ~ 94%,A ~ 6%
+ 235 (5/2+) 42.20s 25.3 m (5) EC,A 2.7E-3%
+ 236 0+ 42.893 2.858 y (8) A,SF 1.4E-7%
+ 237 7/2- 45.087 45.2 d (1) EC,A 4.2E-3%
+ 237m 1/2+ 45.233 0.18 s (2) IT
+ 237n 47.687 85 NS (15) SF
+ 237m 47.987 1.1 us (1) SF
+ 238 0+ 46.158 87.7 y (3) A,SF 1.9E-7%
+ 239 1/2+ 48.583 24110 y (30) A,SF 3E-10%
+ 240 0+ 50.121 6564 y (11) A,SF 5.7E-6%
+ 241 5/2+ 52.950 14.35 y (10) B-,A 2.5E-3%,SF < 2E-14
+ 242 0+ 54.712 3.733E+5 y (12) A,SF 5.5E-4%
+ 242m 0+ 54.712 3.5 NS (6) SF
+ 242n 0+ 54.712 28 NS SF
+ 243 7/2+ 57.749 4.956 h (3) B-
+ 244 0+ 59.799 8.08E+7 y (10) A 99.88%,SF 0.12%
+ 244m 0+ 59.799 400 PS (100) SF
+ 245 (9/2-) 63.10 10.5 h (1) B-
+ 246 0+ 65.39 10.84 d (2) B-
+ 247 69.405C 2.27 d (23) B-
+95 Am Americium 24
+ (243)
+ 13.67 c
+ 1176
+ -
+ +3,+4,+5,+6
+ 232 43.437C 79 s (2) EC ~ 98%,A ~ 2%
+ 234 44.5s 2.32 m (8) EC 99.96%,A 0.04%
+ 235 44.7s ?
+ 236 46.17s A ,EC
+ 237 5/2(-) 46.8s 73.0 m (10) EC 99.98%,A 0.03%
+ 237m 49.2s 5 NS (2) SF
+ 238 1+ 48.42 98 m (2) EC > 99.99%,A 0.0001%
+ 239 (5/2)- 49.386 11.9 h (1) EC 99.99%,A 0.01%
+ 240 (3-) 51.50 50.8 h (3) EC,A 1.9E-4%
+ 241 5/2- 52.929 432.2 y (7) A,SF 4E-10%
+ 241m 55.129 1.2 us (3) SF
+ 242 1- 55.463 16.02 h (2) B- 82.7%,EC 17.3%
+ 242m 5- 55.512 141 y (2) IT 99.54%,A 0.46%
+ 242n 57.663 14.0 ms SF ,IT ,A < 1.5%
+ 243 5/2- 57.167 7370 y (40) A,SF 3.7E-9%
+ 244 (6-) 59.875 10.1 h (1) B-
+ 244m 59.875 ~ 6.5 us SF
+ 244n 59.875 0.90 ms (15) SF
+ 244m 1+ 59.963 ~ 26 m B- 99.96%,EC 0.04%
+ 245 (5/2)+ 61.893 2.05 h (1) B-
+ 246 (7-) 64.99 39 m (3) B-
+ 246m 2(-) 64.99 25.0 m (2) B-,IT < 0.01%
+ 247 (5/2) 67.23s 23.0 m (13) B-
+ 248 70.5s ? B-
+96 Cm Curium 22
+ (247)
+ 13.51 t
+ 1345
+ -
+ +3
+ 232 0+ 1 m ? SF < 30.3%
+ 235 48.0s ?
+ 236 0+ 47.9s A ,EC
+ 238 0+ 49.38 2.4 h (1) EC >= 90%,A <= 10%
+ 239 (7/2-) 51.09s ~ 2.9 h EC,A < 0.1%
+ 240 0+ 51.715 27 d (1) A > 99.5%,EC < 0.5%
+ 241 1/2+ 53.697 32.8 d (2) EC 99%,A 1%
+ 242 0+ 54.798 162.79 d (9) A,SF 6.2E-6%
+ 242m 54.798 40 PS (15) SF
+ 242n 57.598 180 NS (70) SF ?%,IT ?%
+ 243 5/2+ 57.176 29.1 y (1) A 99.71%,EC 0.29%
+ 244 0+ 58.447 18.10 y (2) A,SF 1.3E-4%
+ 244m 0+ 58.447 > 500 NS SF
+ 244n 6+ 59.487 34 ms (2) SF <=.77E-9%
+ 245 7/2+ 60.999 8500 y (100) A,SF 6.1E-7%
+ 246 0+ 62.612 4730 y (100) A 99.97%,SF 0.03%
+ 247 9/2- 65.527 1.56E+7 y (5) A
+ 248 0+ 67.386 3.40E+5 y (4) A 91.74%,SF 8.26%
+ 249 1/2(+) 70.743 64.15 m (3) B-
+ 250 0+ 72.98 ~ 9700 y SF ~ 80%,A ~ 11%
+ 251 (1/2+) 76.64 16.8 m (2) B-
+ 252 0+ C < 2 d B-
+97 Bk Berkelium 17
+ (247)
+ 14
+ 1050
+ -
+ +3,+4
+ 238 54.3s 144 s (5) EC,EF 0.048%
+ 240 55.7s 4.8 m (8) EC ~100%,EF w%
+ 241 (7/2+) 56.1s ?
+ 242 57.8s 7.0 m (13) EC
+ 242m 57.8s 9.5 NS (20) SF > 0%
+ 242n 57.8s 600 NS (100) SF > 0%
+ 243 (3/2-) 58.685 4.5 h (2) EC ~ 99.85%,A ~ 0.15%
+ 244 (1-) 60.70 4.35 h (15) EC 99.994%,A 6.0E-3%
+ 244m 60.70 820 NS (60) SF
+ 245 3/2- 61.809 4.94 d (3) EC 99.88%,A 0.12%
+ 246 2(-) 63.96 1.80 d (2) EC,A < 0.2%
+ 247 (3/2-) 65.482 1380 y (250) A
+ 248 1(-) 68.10 23.7 h (2) B- 70%,EC 30%
+ 248 (6+) 68.10 > 9 y A > 70%
+ 249 7/2+ 69.843 320 d (6) B-,A 1.4E-3%,SF 4.7E-8%
+ 250 2- 72.945 3.217 h (5) B-
+ 251 (3/2-) 75.22 55.6 m (11) B-,A ~1.0E-5%
+98 Cf Californium 19
+ (251)
+ 900
+ -
+ -
+ +3
+ 238 0+ 1 s ? SF < 25%
+ 239 58.3s 39 s (+37-12) A > 50%,EC ?%
+ 240 0+ 58.0s 1.06 m (15) A ~100%
+ 241 59.4s 3.78 m (70) EC ~ 75%,A ~ 25%
+ 242 0+ 59.33 3.49 m (12) A > 0%
+ 243 (1/2+) 60.9s 10.7 m (5) EC ~ 86%,A ~ 14%
+ 244 0+ 61.469 19.4 m (6) A
+ 245 (5/2+) 63.377 45.0 m (15) EC 64%,A 36%
+ 246 0+ 64.085 35.7 h (5) A,EC <5.0E-4%
+ 247 (7/2+) 66.128 3.11 h (3) EC 99.97%,A 0.04%
+ 248 0+ 67.233 333.5 d (28) A,SF 0.0029%
+ 249 9/2- 69.719 351 y (2) A,SF 5.2E-7%
+ 250 0+ 71.165 13.08 y (9) A 99.92%,SF 0.08%
+ 251 1/2+ 74.127 898 y (44) A
+ 252 0+ 76.027 2.645 y (8) A 96.91%,SF 3.09%
+ 253 (7/2+) 79.293 17.81 d (8) B- 99.69%,A 0.31%
+ 254 0+ 81.33 60.5 d (2) SF 99.69%,A 0.31%
+ 255 (9/2+) 84.8s 85 m (18) B-
+ 256 0+ C 12.3 m (12) SF,B- < 1%,A ~1.0E-6%
+99 Es Einsteinium 19
+ (252)
+ 860
+ -
+ -
+ +3
+ 242 64.9s ~ 7 s EC ,EF
+ 243 64.9s 21 s (2) EC <= 70%,A >= 30%
+ 244 66.0s 37 s (4) EC 96%,A 4%
+ 245 (3/2-) 66.4s 1.1 m (1) EC 60%,A 40%
+ 246 (4-,6+) 68.0s 7.7 m (5) EC 90.1%,A 9.9%
+ 247 (7/2+) 68.60s 4.55 m (26) EC ~ 93%,A ~ 7%
+ 248 (2-,0+) 70.29 27 m (4) EC > 99%,A ~ 0.25%
+ 249 7/2(+) 71.17s 102.2 m (6) EC 99.43%,A 0.57%
+ 250 (6+) 73.27s 8.6 h (1) EC > 97%,A < 3%
+ 250m 1(-) 73.27s 2.22 h (5) EC >= 99%,A <= 1%
+ 251 (3/2-) 74.504 33 h (1) EC 99.51%,A 0.49%
+ 252 (5-) 77.29 471.7 d (19) A 76%,EC 24%,B- ~ 0.01%
+ 253 7/2+ 79.008 20.47 d (3) A,SF 8.7E-6%
+ 254 (7+) 81.988 275.7 d (5) A,EC <1.0E-4%
+ 254m 2+ 82.066 39.3 h (2) B- 98%,IT < 3%
+ 255 (7/2+) 84.08 39.8 d (12) B- 92%,A 8%,SF 4.1E-3%
+ 256 (1+) 87.15s 25.4 m (24) B-
+ 256m (8+) 87.15s ~ 7.6 h B-
+ 257 89.4s 2 s ? SF ?%
+100 Fm Fermium 21
+ (257)
+ 1527
+ -
+ -
+ +3
+ 242 0+ 68.353C 0.8 ms (2) SF > 0%
+ 243 69.4s 0.18 s (+8-4) A,SF <= 0.36%
+ 244 0+ 69.1s 3.3 ms (4) SF
+ 245 70.2s 4.2 s (13) A,SF <= 0.11%
+ 246 0+ 70.12 1.1 s (2) A 92%,SF 8%,EC <= 1%
+ 247? 71.5s 35 s (4) A >= 50%,EC <= 50%
+ 247m 71.5s 9.2 s (23) A
+ 248 0+ 71.90 36 s (3) A 99%,EC ~ 1%
+ 249 (7/2+) 73.6s 2.6 m (7) EC ~ 85%,A ~ 15%
+ 250 0+ 74.07 30 m (3) A > 90%,EC < 10%
+ 250m 75.07 1.8 s (1) IT > 80%,SF <0.8E-4%
+ 251 (9/2-) 75.978 5.30 h (8) EC 98.2%,A 1.8%
+ 252 0+ 76.810 25.39 h (5) A,SF 0.0023%
+ 253 1/2+ 79.340 3.00 d (12) EC 88%,A 12%
+ 254 0+ 80.897 3.240 h (2) A 99.94%,SF 0.06%
+ 255 7/2+ 83.793 20.07 h (7) A,SF 2.4E-5%
+ 256 0+ 85.479 157.6 m (13) SF 91.9%,A 8.1%
+ 257 (9/2+) 88.581 100.5 d (2) A 99.79%,SF 0.21%
+ 258 0+ 90.5s 370 us (43) SF
+ 259 93.7s 1.5 s (3) SF
+ 260 0+ ~ 4 ms SF
+101 Md Mendelevium 16
+ (258)
+ 827
+ -
+ -
+ +2,+3
+ 247 76.1s 2.9 s (17) A
+ 248 77.1s 7 s (3) EC 80%,A 20%,SF <= 0.05
+ 249 77.3s 24 s (4) A ~ 70%,EC ~ 30%
+ 250 78.7s 52 s (6) EC 93%,A 7%
+ 251 79.1s 4.0 m (5) EC >= 90%,A <= 10%
+ 252 80.7s 4.8 m (+8-5) EC
+ 253 81.3s ~ 6 m EC
+ 254 83.6s 10 m (3) EC
+ 254 83.6s 28 m (8) EC
+ 255 (7/2-) 84.835 27 m (2) EC 92%,A 8%,SF <= 0.15%
+ 256 (0-,1-) 87.61 78.1 m (18) EC 90.7%,A 9.3%
+ 257 (7/2-) 88.990 5.52 h (5) EC 90%,A 10%,SF < 1%
+ 258 (1-) 91.684 60 m (2) EC
+ 258 (8-) 91.684 51.5 d (3) A,SF <= 0.003%
+ 259 (7/2-) 93.6s 1.60 h (6) SF ~100%,A < 3%
+ 260 96.6s 27.8 d (8) SF > 73%,A < 25%
+102 No Nobelium 13
+ (259)
+ 827
+ -
+ -
+ +2,+3
+ 250 0+ C 0.25 ms (5) SF,A ~ 0.05%
+ 251 82.8s 0.8 s (3) A ~100%,EC ~ 1%
+ 252 0+ 82.87 2.30 s (22) A 73.1%,SF 26.9%
+ 253 (9/2-) 84.5s 1.7 m (3) A ~ 80%,EC ~ 20%
+ 254 0+ 84.72 55 s (3) A 90%,EC 10%,SF 0.25%
+ 254m 85.22 0.28 s (4) IT > 80%,SF >= 0.2%
+ 255 (1/2+) 86.85 3.1 m (2) A 61.4%,EC 38.6%
+ 256 0+ 87.817 2.91 s (5) A 99.5%,SF 0.5%
+ 257 (7/2+) 90.22 25 s (2) A ~100%
+ 258 0+ 91.5s 1.2 ms (2) SF,A 0.001%
+ 259 (9/2+) 94.1s 58 m (5) A 75%,EC 25%,SF < 10%
+ 260 0+ 95.6s 106 ms (8) SF
+ 262 0+ 100.2s ~ 5 ms SF
+103 Lr Lawrencium 11
+ (261)
+ 1627
+ -
+ -
+ +3
+ 252 C ~ 1 s A ~ 90%,EC ~ 10%
+ 253 88.7s 1.3 s (+6-3) A 90%,SF < 20%
+ 254 89.9s 13 s (2) A 78%,EC 22%,SF < 0.1%
+ 255 90.1s 22 s (4) A 85%,EC < 30%
+ 256 92.0s 28 s (3) A > 80%,EC < 20%
+ 257 (9/2+) 92.7s 0.646 s (25) A,SF <=.65E-3%
+ 258 94.9s 3.9 s (4) A > 95%,EC < 5%
+ 259 95.93s 6.1 s (4) A 80%,SF 20%,EC < 0.5%
+ 260 98.3s 180 s (30) A 75%,EC ~ 15%
+ 261 99.6s 39 m (12) SF
+ 262 102.3s 3.6 h (3) EC ,SF < 10%
+104 Rf Rutherfordium 10
+ -
+ -
+ -
+ -
+ -
+ 253 C ~ 1.8 s A ~ 50%,SF ~ 50%
+ 254 0+ C 0.5 ms (2) SF,A ~ 0.3%
+ 255 (9/2-) 94.s 1.5 s (2) SF 52%,A 48%
+ 256 0+ 94.25 6.7 ms (2) SF 98%,A 2.2%
+ 257 (7/2+) 96.2s 4.7 s (3) A 79.6%,EC 18%
+ 258 0+ 96.4s 12 ms (2) SF ~ 87%,A ~ 13%
+ 259 98.38s 3.1 s (7) A 93%,SF 7%,EC ~ 0.3%
+ 260 0+ 99.2s 20.1 ms (7) SF ~ 98%,A ~ 2%
+ 261 101.5s 65 s (10) A > 80%,EC <= 10%
+ 262 0+ 102.5s 1.2 s (+10-5) SF
+105 Ha Hahnium 10
+ -
+ -
+ -
+ -
+ -
+ 255 C 1.6 s (+6-4) A ~ 80%,SF ~ 20%
+ 256 C 2.6 s (+14-8) A <= 90%,SF <= 40%
+ 257 100.5s 1.3 s (+5-3) A 82%,SF 17%,EC 1%
+ 258 101.8s 4.4 s (+9-6) A 67%,EC 33%,SF < 1%
+ 258 101.8s 20 s (10) EC
+ 259 102.2s ? A
+ 260 103.8s 1.52 s (13) A >= 90%,SF <= 10%
+ 261 104.4s 1.8 s (4) A > 50%,SF < 50%
+ 262 106.5s 34 s (4) A 64%,SF 33%,EC ~ 3%
+ 263 107.4s 27 s (+10-7) SF ~ 57%,A ~ 43%
+106 Sg Seaborgium 6
+ -
+ -
+ -
+ -
+ -
+ 259 (1/2+) 106.8s 0.9 s (2) A > 80%,SF < 20%
+ 260 0+ 106.60 3.6 ms (+9-6) A 50%,SF 50%
+ 261 108.4s 0.23 s (3) A > 90%,SF < 10%
+ 263 110.5s 0.8 s (2) SF ~ 70%,A ~ 30%
+ 265 113.1s ~ 16 s A ,SF <50%
+ 266 0+ 114.0s ~ 20 s A ,SF <50%
+107 Ns Nielsbohrium 4
+ -
+ -
+ -
+ -
+ -
+ 260 C A
+ 261 113.4s 11.8 ms (+53-28) A > 90%,SF < 10%
+ 262 114.7s 102 ms (26) A >= 80%,SF <= 20%
+ 262m 115.0s 8.0 ms (21) A > 70%,SF < 30%
+108 Hs Hassium 5
+ -
+ -
+ -
+ -
+ -
+ 263 < 1 s A
+ 264 0+ 119.8 0.08 ms (+40-4) A,SF < 1.5%
+ 265 121.6s 1.8 ms (+22-7) A ~100%,SF <= 9%
+ 267 60 ms (+30-15) A
+ 267 33 ms (17)
+109 Mt Meitnerium 2
+ -
+ -
+ -
+ -
+ -
+ 266 128.4s 3.4 ms (+61-13) A ~100%,SF <= 5.5%
+ 268 70 ms (65) A
+110 Uun Ununnilium 5
+ -
+ -
+ -
+ -
+ -
+ 267? ~ 3 us A
+ 269 0.17 ms (+16-6) A
+ 271 1.1 ms (+6-3) A
+ 271 0.06 s (+27-3) A
+ 272 0+ ~ 8.6 ms SF
+111 Uuu Unununium 1
+ -
+ -
+ -
+ -
+ -
+ 272 1.5 ms (+20-5) A
+112 Uub Ununbium 0
+113 Uut Ununtrium 0
+114 Uuq Ununquadium 0
+115 Uup Ununpentium 0
+116 Uuh Ununhexium 0
+117 Uus Ununseptium 0
+118 Uuo Ununoctium 0
diff --git a/test/periodic/db/mt.dat b/test/periodic/db/mt.dat
new file mode 100644
index 0000000000000000000000000000000000000000..47962b9cd970d99a79fe8659b7950af6dd327dc7
--- /dev/null
+++ b/test/periodic/db/mt.dat
@@ -0,0 +1,2015 @@
+340
+1 (n,total)
+Neutron total cross section. Sum of MT=2, 4, 5, 11, 16-18,
+22-26, 28-37, 41-42, 44-45, and 102-117.
+
+Redundant. Undefined for incident charged particles.
+
+2 (z,z0)
+Elastic scattering cross section for incident particles.
+
+
+
+3 (z,nonelastic)
+Nonelastic cross section. Sum of MT=4, 5, 11, 16-18, 22-26,
+28-37, 41-42, 44-45, 102-117.
+
+Redundant. For photon production only.
+
+4 (z,n)
+Production of one neutron in the exit channel. Sum of
+MT=50-91.
+
+Redundant. For incident neutrons, this is total inelastic
+scattering (MT=50 is undefined for neutrons).
+
+5 (z,anything)
+Sum of all reactions not given explicitly in another MT
+number. This is a partial reaction to be added to
+obtain MT=1.
+
+Each particles can be identified and its multiplicity given
+in File 6. Not allowed in Files 4, 5.
+
+10 (z,continuum)
+Total continuum reaction; exclues all discrete reactions.
+
+Redundant; to be used for derived files only.
+
+11 (z,2nd)
+Production of two neutrons and a deuteron, plus a residual.
+
+
+
+16 (z,2n)
+Production of two neutrons, plus a residual.
+
+
+
+17 (z,2n)
+Production of three neutrons, plus a residual.
+
+
+
+18 (z,fission)
+Total fission. Equal to the sum of MT=19, 20, 21, and 38,
+if present.
+
+Redundant if MT=19 is present. Basic otherwise.
+
+19 (z,f)
+First-chance fission.
+
+
+
+20 (z,nf)
+Second-chance fission.
+
+
+
+21 (z,2nf)
+Third-chance fission.
+
+
+
+22 (z,na)
+Production of a neutron and alpha particle, plus a residual.
+
+
+
+23 (z,n3a)
+Production of a neutron and three alpha particles, plus a residual.
+
+
+
+24 (z,2na)
+Production of two neutrons and an alpha particle, plus a residual.
+
+
+
+25 (z,3na)
+Production of three neutrons and an alpha particle, plus a residual.
+
+
+
+27 (z,abs)
+Absorption. Sum of MT=18 and MT=102-117.
+
+Redundant. Rarely used.
+
+28 (z,np)
+Production of a neutron and a proton, plus a residual.
+
+
+
+29 (z,n2a)
+Production of a neutron and two alpha particles, plus a residual.
+
+
+
+30 (z,2n2a)
+Production of two neutrons and two alpha particles, plus a residual.
+
+
+
+32 (z,nd)
+Production of a neutron and a deuteron, plus a residual.
+
+
+
+33 (z,nt)
+Production of a neutron and a triton, plus a residual.
+
+
+
+34 (z,n3He)
+Production of a neutron and a 3He particle,
+plus a residual.
+
+
+
+35 (z,nd2a)
+Production of a neutron, a deuteron, and two alpha particles,
+plus a residual.
+
+
+
+36 (z,nt2a)
+Production of a neutron, a triton, and two alpha particles,
+plus a residual.
+
+
+
+37 (z,4n)
+Production of four neutrons, plus a residual.
+
+
+
+38 (z,3nf)
+Fourth-change fission.
+
+
+
+41 (z,2np)
+Production of two neutrons and a proton, plus a residual.
+
+
+
+42 (z,3np)
+Production of three neutrons and a proton, plus a residual.
+
+
+
+44 (z,n2p)
+Production of a neutron and two protons, plus a residual.
+
+
+
+45 (z,npa)
+Production of a neutron, a proton, and an alpha particle,
+plus a residual.
+
+
+
+50 (z,n0)
+Production of a neutron, leaving the residual nucleus in the
+ground state.
+
+Not allowed for incident neutrons. Use MT=2.
+
+51 (z,n1)
+Production of a neutron, leaving the residual nucleus in the
+first excited state.
+
+
+
+52 (z,n2)
+Production of a neutron, leaving the residual nucleus in the
+2nd excited state.
+
+
+
+53 (z,n3)
+Production of a neutron, leaving the residual nucleus in the
+3rd excited state.
+
+
+
+54 (z,n4)
+Production of a neutron, leaving the residual nucleus in the
+4th excited state.
+
+
+
+55 (z,n5)
+Production of a neutron, leaving the residual nucleus in the
+5th excited state.
+
+
+
+56 (z,n6)
+Production of a neutron, leaving the residual nucleus in the
+6th excited state.
+
+
+
+57 (z,n7)
+Production of a neutron, leaving the residual nucleus in the
+7th excited state.
+
+
+
+58 (z,n8)
+Production of a neutron, leaving the residual nucleus in the
+8th excited state.
+
+
+
+59 (z,n9)
+Production of a neutron, leaving the residual nucleus in the
+9th excited state.
+
+
+
+60 (z,n10)
+Production of a neutron, leaving the residual nucleus in the
+10th excited state.
+
+
+
+61 (z,n11)
+Production of a neutron, leaving the residual nucleus in the
+11th excited state.
+
+
+
+62 (z,n12)
+Production of a neutron, leaving the residual nucleus in the
+12th excited state.
+
+
+
+63 (z,n13)
+Production of a neutron, leaving the residual nucleus in the
+13th excited state.
+
+
+
+64 (z,n14)
+Production of a neutron, leaving the residual nucleus in the
+14th excited state.
+
+
+
+65 (z,n15)
+Production of a neutron, leaving the residual nucleus in the
+15th excited state.
+
+
+
+66 (z,n16)
+Production of a neutron, leaving the residual nucleus in the
+16th excited state.
+
+
+
+67 (z,n17)
+Production of a neutron, leaving the residual nucleus in the
+17th excited state.
+
+
+
+68 (z,n18)
+Production of a neutron, leaving the residual nucleus in the
+18th excited state.
+
+
+
+69 (z,n19)
+Production of a neutron, leaving the residual nucleus in the
+19th excited state.
+
+
+
+70 (z,n20)
+Production of a neutron, leaving the residual nucleus in the
+20th excited state.
+
+
+
+71 (z,n21)
+Production of a neutron, leaving the residual nucleus in the
+21th excited state.
+
+
+
+72 (z,n22)
+Production of a neutron, leaving the residual nucleus in the
+22th excited state.
+
+
+
+73 (z,n23)
+Production of a neutron, leaving the residual nucleus in the
+23th excited state.
+
+
+
+74 (z,n24)
+Production of a neutron, leaving the residual nucleus in the
+24th excited state.
+
+
+
+75 (z,n25)
+Production of a neutron, leaving the residual nucleus in the
+25th excited state.
+
+
+
+76 (z,n26)
+Production of a neutron, leaving the residual nucleus in the
+26th excited state.
+
+
+
+77 (z,n27)
+Production of a neutron, leaving the residual nucleus in the
+27th excited state.
+
+
+
+78 (z,n28)
+Production of a neutron, leaving the residual nucleus in the
+28th excited state.
+
+
+
+79 (z,n29)
+Production of a neutron, leaving the residual nucleus in the
+29th excited state.
+
+
+
+80 (z,n30)
+Production of a neutron, leaving the residual nucleus in the
+30th excited state.
+
+
+
+81 (z,n31)
+Production of a neutron, leaving the residual nucleus in the
+31th excited state.
+
+
+
+82 (z,n32)
+Production of a neutron, leaving the residual nucleus in the
+32th excited state.
+
+
+
+83 (z,n33)
+Production of a neutron, leaving the residual nucleus in the
+33th excited state.
+
+
+
+84 (z,n34)
+Production of a neutron, leaving the residual nucleus in the
+34th excited state.
+
+
+
+85 (z,n35)
+Production of a neutron, leaving the residual nucleus in the
+35th excited state.
+
+
+
+86 (z,n36)
+Production of a neutron, leaving the residual nucleus in the
+36th excited state.
+
+
+
+87 (z,n37)
+Production of a neutron, leaving the residual nucleus in the
+37th excited state.
+
+
+
+88 (z,n38)
+Production of a neutron, leaving the residual nucleus in the
+38th excited state.
+
+
+
+89 (z,n39)
+Production of a neutron, leaving the residual nucleus in the
+39th excited state.
+
+
+
+90 (z,n40)
+Production of a neutron, leaving the residual nucleus in the
+40th excited state.
+
+
+
+91 (z,nc)
+Production of a neutron in the continuum not included in the
+above discrete representation.
+
+
+
+101 (z,disap)
+Disappearance. Sum of MT=102-117.
+
+Redundant. Rarely used.
+
+102 (z,gamma)
+Radiative capture.
+
+
+
+103 (z,p)
+Production of a proton, plus a residual. Sum of MT=600-649,
+if they are present.
+
+For incident protons, this is inelastic scattering, and MT=600 is
+undefined (use MT=2).
+
+104 (z,d)
+Production of a deuteron, plus a residual. Sum of MT=650-699,
+if they are present.
+
+For incident deuterons, this is inelastic scattering, and MT=650 is
+undefined (use MT=2).
+
+105 (z,t)
+Production of a triton, plus a residual. Sum of MT=700-749,
+if they are present.
+
+For incident tritons, this is inelastic scattering, and MT=700 is
+undefined (use MT=2).
+
+106 (z,3He)
+Production of a <SUP3He particles, plus a residual. Sum
+of MT=750-799, if they are present.
+
+For incident 3He particles, this is inelastic scattering,
+and MT=750 is undefined (use MT=2).
+
+107 (z,a)
+Production of an alpha particle, plus a residual. Sum of MT=800-849,
+if they are present.
+
+For incident alphas, this is inelastic scattering, and MT=800 is
+undefined (use MT=2).
+
+108 (z,2a)
+Production of two alphas, plus a residual.
+
+
+
+109 (z,3a)
+Production of three alphas, plus a residual.
+
+
+
+111 (z,2p)
+Production of two protons, plus a residual.
+
+
+
+112 (z,pa)
+Production of a proton and an alpha particle, plus a residual.
+
+
+
+113 (z,t2a)
+Production of a triton and two alphas, plus a residual.
+
+
+
+114 (z,d2a)
+Production of a deuteron and two alphas, plus a residual.
+
+
+
+115 (z,pd)
+Production of a proton and a deuteron, plus a residual.
+
+
+
+116 (z,pt)
+Production of a proton and a triton, plus a residual.
+
+
+
+117 (z,da)
+Production of a deuteron and an alpha particle, plus a residual.
+
+
+
+600 (z,p0)
+Production of a proton, leaving the residual nucleus in the
+ground state.
+
+Not allowed for incident protons. Use MT=2.
+
+601 (z,p1)
+Production of a proton, leaving the residual nucleus in the
+first excited state.
+
+
+
+602 (z,p2)
+Production of a proton, leaving the residual nucleus in the
+2nd excited state.
+
+
+
+603 (z,p3)
+Production of a proton, leaving the residual nucleus in the
+3rd excited state.
+
+
+
+604 (z,p4)
+Production of a proton, leaving the residual nucleus in the
+4th excited state.
+
+
+
+605 (z,p5)
+Production of a proton, leaving the residual nucleus in the
+5th excited state.
+
+
+
+606 (z,p6)
+Production of a proton, leaving the residual nucleus in the
+6th excited state.
+
+
+
+607 (z,p7)
+Production of a proton, leaving the residual nucleus in the
+7th excited state.
+
+
+
+608 (z,p8)
+Production of a proton, leaving the residual nucleus in the
+8th excited state.
+
+
+
+609 (z,p9)
+Production of a proton, leaving the residual nucleus in the
+9th excited state.
+
+
+
+610 (z,p10)
+Production of a proton, leaving the residual nucleus in the
+10th excited state.
+
+
+
+611 (z,p11)
+Production of a proton, leaving the residual nucleus in the
+11th excited state.
+
+
+
+612 (z,p12)
+Production of a proton, leaving the residual nucleus in the
+12th excited state.
+
+
+
+613 (z,p13)
+Production of a proton, leaving the residual nucleus in the
+13th excited state.
+
+
+
+614 (z,p14)
+Production of a proton, leaving the residual nucleus in the
+14th excited state.
+
+
+
+615 (z,p15)
+Production of a proton, leaving the residual nucleus in the
+15th excited state.
+
+
+
+616 (z,p16)
+Production of a proton, leaving the residual nucleus in the
+16th excited state.
+
+
+
+617 (z,p17)
+Production of a proton, leaving the residual nucleus in the
+17th excited state.
+
+
+
+618 (z,p18)
+Production of a proton, leaving the residual nucleus in the
+18th excited state.
+
+
+
+619 (z,p19)
+Production of a proton, leaving the residual nucleus in the
+19th excited state.
+
+
+
+620 (z,p20)
+Production of a proton, leaving the residual nucleus in the
+20th excited state.
+
+
+
+621 (z,p21)
+Production of a proton, leaving the residual nucleus in the
+21th excited state.
+
+
+
+622 (z,p22)
+Production of a proton, leaving the residual nucleus in the
+22th excited state.
+
+
+
+623 (z,p23)
+Production of a proton, leaving the residual nucleus in the
+23th excited state.
+
+
+
+624 (z,p24)
+Production of a proton, leaving the residual nucleus in the
+24th excited state.
+
+
+
+625 (z,p25)
+Production of a proton, leaving the residual nucleus in the
+25th excited state.
+
+
+
+626 (z,p26)
+Production of a proton, leaving the residual nucleus in the
+26th excited state.
+
+
+
+627 (z,p27)
+Production of a proton, leaving the residual nucleus in the
+27th excited state.
+
+
+
+628 (z,p28)
+Production of a proton, leaving the residual nucleus in the
+28th excited state.
+
+
+
+629 (z,p29)
+Production of a proton, leaving the residual nucleus in the
+29th excited state.
+
+
+
+630 (z,p30)
+Production of a proton, leaving the residual nucleus in the
+30th excited state.
+
+
+
+631 (z,p31)
+Production of a proton, leaving the residual nucleus in the
+31th excited state.
+
+
+
+632 (z,p32)
+Production of a proton, leaving the residual nucleus in the
+32th excited state.
+
+
+
+633 (z,p33)
+Production of a proton, leaving the residual nucleus in the
+33th excited state.
+
+
+
+634 (z,p34)
+Production of a proton, leaving the residual nucleus in the
+34th excited state.
+
+
+
+635 (z,p35)
+Production of a proton, leaving the residual nucleus in the
+35th excited state.
+
+
+
+636 (z,p36)
+Production of a proton, leaving the residual nucleus in the
+36th excited state.
+
+
+
+637 (z,p37)
+Production of a proton, leaving the residual nucleus in the
+37th excited state.
+
+
+
+638 (z,p38)
+Production of a proton, leaving the residual nucleus in the
+38th excited state.
+
+
+
+639 (z,p39)
+Production of a proton, leaving the residual nucleus in the
+39th excited state.
+
+
+
+640 (z,p40)
+Production of a proton, leaving the residual nucleus in the
+40th excited state.
+
+
+
+641 (z,p41)
+Production of a proton, leaving the residual nucleus in the
+41th excited state.
+
+
+
+642 (z,p42)
+Production of a proton, leaving the residual nucleus in the
+42th excited state.
+
+
+
+643 (z,p43)
+Production of a proton, leaving the residual nucleus in the
+43th excited state.
+
+
+
+644 (z,p44)
+Production of a proton, leaving the residual nucleus in the
+44th excited state.
+
+
+
+645 (z,p45)
+Production of a proton, leaving the residual nucleus in the
+45th excited state.
+
+
+
+646 (z,p46)
+Production of a proton, leaving the residual nucleus in the
+46th excited state.
+
+
+
+647 (z,p47)
+Production of a proton, leaving the residual nucleus in the
+47th excited state.
+
+
+
+648 (z,p48)
+Production of a proton, leaving the residual nucleus in the
+48th excited state.
+
+
+
+649 (z,pc)
+Production of a proton in the continuum not included in the
+above discrete representation.
+
+
+
+650 (z,d0)
+Production of a deuteron, leaving the residual nucleus in the
+ground state.
+
+Not allowed for incident deuterons. Use MT=2.
+
+651 (z,d1)
+Production of a deuteron, leaving the residual nucleus in the
+first excited state.
+
+
+
+652 (z,d2)
+Production of a deuteron, leaving the residual nucleus in the
+2nd excited state.
+
+
+
+653 (z,d3)
+Production of a deuteron, leaving the residual nucleus in the
+3rd excited state.
+
+
+
+654 (z,d4)
+Production of a deuteron, leaving the residual nucleus in the
+4th excited state.
+
+
+
+655 (z,d5)
+Production of a deuteron, leaving the residual nucleus in the
+5th excited state.
+
+
+
+656 (z,d6)
+Production of a deuteron, leaving the residual nucleus in the
+6th excited state.
+
+
+
+657 (z,d7)
+Production of a deuteron, leaving the residual nucleus in the
+7th excited state.
+
+
+
+658 (z,d8)
+Production of a deuteron, leaving the residual nucleus in the
+8th excited state.
+
+
+
+659 (z,d9)
+Production of a deuteron, leaving the residual nucleus in the
+9th excited state.
+
+
+
+660 (z,d10)
+Production of a deuteron, leaving the residual nucleus in the
+10th excited state.
+
+
+
+661 (z,d11)
+Production of a deuteron, leaving the residual nucleus in the
+11th excited state.
+
+
+
+662 (z,d12)
+Production of a deuteron, leaving the residual nucleus in the
+12th excited state.
+
+
+
+663 (z,d13)
+Production of a deuteron, leaving the residual nucleus in the
+13th excited state.
+
+
+
+664 (z,d14)
+Production of a deuteron, leaving the residual nucleus in the
+14th excited state.
+
+
+
+665 (z,d15)
+Production of a deuteron, leaving the residual nucleus in the
+15th excited state.
+
+
+
+666 (z,d16)
+Production of a deuteron, leaving the residual nucleus in the
+16th excited state.
+
+
+
+667 (z,d17)
+Production of a deuteron, leaving the residual nucleus in the
+17th excited state.
+
+
+
+668 (z,d18)
+Production of a deuteron, leaving the residual nucleus in the
+18th excited state.
+
+
+
+669 (z,d19)
+Production of a deuteron, leaving the residual nucleus in the
+19th excited state.
+
+
+
+670 (z,d20)
+Production of a deuteron, leaving the residual nucleus in the
+20th excited state.
+
+
+
+671 (z,d21)
+Production of a deuteron, leaving the residual nucleus in the
+21th excited state.
+
+
+
+672 (z,d22)
+Production of a deuteron, leaving the residual nucleus in the
+22th excited state.
+
+
+
+673 (z,d23)
+Production of a deuteron, leaving the residual nucleus in the
+23th excited state.
+
+
+
+674 (z,d24)
+Production of a deuteron, leaving the residual nucleus in the
+24th excited state.
+
+
+
+675 (z,d25)
+Production of a deuteron, leaving the residual nucleus in the
+25th excited state.
+
+
+
+676 (z,d26)
+Production of a deuteron, leaving the residual nucleus in the
+26th excited state.
+
+
+
+677 (z,d27)
+Production of a deuteron, leaving the residual nucleus in the
+27th excited state.
+
+
+
+678 (z,d28)
+Production of a deuteron, leaving the residual nucleus in the
+28th excited state.
+
+
+
+679 (z,d29)
+Production of a deuteron, leaving the residual nucleus in the
+29th excited state.
+
+
+
+680 (z,d30)
+Production of a deuteron, leaving the residual nucleus in the
+30th excited state.
+
+
+
+681 (z,d31)
+Production of a deuteron, leaving the residual nucleus in the
+31th excited state.
+
+
+
+682 (z,d32)
+Production of a deuteron, leaving the residual nucleus in the
+32th excited state.
+
+
+
+683 (z,d33)
+Production of a deuteron, leaving the residual nucleus in the
+33th excited state.
+
+
+
+684 (z,d34)
+Production of a deuteron, leaving the residual nucleus in the
+34th excited state.
+
+
+
+685 (z,d35)
+Production of a deuteron, leaving the residual nucleus in the
+35th excited state.
+
+
+
+686 (z,d36)
+Production of a deuteron, leaving the residual nucleus in the
+36th excited state.
+
+
+
+687 (z,d37)
+Production of a deuteron, leaving the residual nucleus in the
+37th excited state.
+
+
+
+688 (z,d38)
+Production of a deuteron, leaving the residual nucleus in the
+38th excited state.
+
+
+
+689 (z,d39)
+Production of a deuteron, leaving the residual nucleus in the
+39th excited state.
+
+
+
+690 (z,d40)
+Production of a deuteron, leaving the residual nucleus in the
+40th excited state.
+
+
+
+691 (z,d41)
+Production of a deuteron, leaving the residual nucleus in the
+41th excited state.
+
+
+
+692 (z,d42)
+Production of a deuteron, leaving the residual nucleus in the
+42th excited state.
+
+
+
+693 (z,d43)
+Production of a deuteron, leaving the residual nucleus in the
+43th excited state.
+
+
+
+694 (z,d44)
+Production of a deuteron, leaving the residual nucleus in the
+44th excited state.
+
+
+
+695 (z,d45)
+Production of a deuteron, leaving the residual nucleus in the
+45th excited state.
+
+
+
+696 (z,d46)
+Production of a deuteron, leaving the residual nucleus in the
+46th excited state.
+
+
+
+697 (z,d47)
+Production of a deuteron, leaving the residual nucleus in the
+47th excited state.
+
+
+
+698 (z,d48)
+Production of a deuteron, leaving the residual nucleus in the
+48th excited state.
+
+
+
+699 (z,dc)
+Production of a deuteron in the continuum not included in the
+above discrete representation.
+
+
+
+700 (z,t0)
+Production of a triton, leaving the residual nucleus in the
+ground state.
+
+Not allowed for incident tritons. Use MT=2.
+
+701 (z,t1)
+Production of a triton, leaving the residual nucleus in the
+first excited state.
+
+
+
+702 (z,t2)
+Production of a triton, leaving the residual nucleus in the
+2nd excited state.
+
+
+
+703 (z,t3)
+Production of a triton, leaving the residual nucleus in the
+3rd excited state.
+
+
+
+704 (z,t4)
+Production of a triton, leaving the residual nucleus in the
+4th excited state.
+
+
+
+705 (z,t5)
+Production of a triton, leaving the residual nucleus in the
+5th excited state.
+
+
+
+706 (z,t6)
+Production of a triton, leaving the residual nucleus in the
+6th excited state.
+
+
+
+707 (z,t7)
+Production of a triton, leaving the residual nucleus in the
+7th excited state.
+
+
+
+708 (z,t8)
+Production of a triton, leaving the residual nucleus in the
+8th excited state.
+
+
+
+709 (z,t9)
+Production of a triton, leaving the residual nucleus in the
+9th excited state.
+
+
+
+710 (z,t10)
+Production of a triton, leaving the residual nucleus in the
+10th excited state.
+
+
+
+711 (z,t11)
+Production of a triton, leaving the residual nucleus in the
+11th excited state.
+
+
+
+712 (z,t12)
+Production of a triton, leaving the residual nucleus in the
+12th excited state.
+
+
+
+713 (z,t13)
+Production of a triton, leaving the residual nucleus in the
+13th excited state.
+
+
+
+714 (z,t14)
+Production of a triton, leaving the residual nucleus in the
+14th excited state.
+
+
+
+715 (z,t15)
+Production of a triton, leaving the residual nucleus in the
+15th excited state.
+
+
+
+716 (z,t16)
+Production of a triton, leaving the residual nucleus in the
+16th excited state.
+
+
+
+717 (z,t17)
+Production of a triton, leaving the residual nucleus in the
+17th excited state.
+
+
+
+718 (z,t18)
+Production of a triton, leaving the residual nucleus in the
+18th excited state.
+
+
+
+719 (z,t19)
+Production of a triton, leaving the residual nucleus in the
+19th excited state.
+
+
+
+720 (z,t20)
+Production of a triton, leaving the residual nucleus in the
+20th excited state.
+
+
+
+721 (z,t21)
+Production of a triton, leaving the residual nucleus in the
+21th excited state.
+
+
+
+722 (z,t22)
+Production of a triton, leaving the residual nucleus in the
+22th excited state.
+
+
+
+723 (z,t23)
+Production of a triton, leaving the residual nucleus in the
+23th excited state.
+
+
+
+724 (z,t24)
+Production of a triton, leaving the residual nucleus in the
+24th excited state.
+
+
+
+725 (z,t25)
+Production of a triton, leaving the residual nucleus in the
+25th excited state.
+
+
+
+726 (z,t26)
+Production of a triton, leaving the residual nucleus in the
+26th excited state.
+
+
+
+727 (z,t27)
+Production of a triton, leaving the residual nucleus in the
+27th excited state.
+
+
+
+728 (z,t28)
+Production of a triton, leaving the residual nucleus in the
+28th excited state.
+
+
+
+729 (z,t29)
+Production of a triton, leaving the residual nucleus in the
+29th excited state.
+
+
+
+730 (z,t30)
+Production of a triton, leaving the residual nucleus in the
+30th excited state.
+
+
+
+731 (z,t31)
+Production of a triton, leaving the residual nucleus in the
+31th excited state.
+
+
+
+732 (z,t32)
+Production of a triton, leaving the residual nucleus in the
+32th excited state.
+
+
+
+733 (z,t33)
+Production of a triton, leaving the residual nucleus in the
+33th excited state.
+
+
+
+734 (z,t34)
+Production of a triton, leaving the residual nucleus in the
+34th excited state.
+
+
+
+735 (z,t35)
+Production of a triton, leaving the residual nucleus in the
+35th excited state.
+
+
+
+736 (z,t36)
+Production of a triton, leaving the residual nucleus in the
+36th excited state.
+
+
+
+737 (z,t37)
+Production of a triton, leaving the residual nucleus in the
+37th excited state.
+
+
+
+738 (z,t38)
+Production of a triton, leaving the residual nucleus in the
+38th excited state.
+
+
+
+739 (z,t39)
+Production of a triton, leaving the residual nucleus in the
+39th excited state.
+
+
+
+740 (z,t40)
+Production of a triton, leaving the residual nucleus in the
+40th excited state.
+
+
+
+741 (z,t41)
+Production of a triton, leaving the residual nucleus in the
+41th excited state.
+
+
+
+742 (z,t42)
+Production of a triton, leaving the residual nucleus in the
+42th excited state.
+
+
+
+743 (z,t43)
+Production of a triton, leaving the residual nucleus in the
+43th excited state.
+
+
+
+744 (z,t44)
+Production of a triton, leaving the residual nucleus in the
+44th excited state.
+
+
+
+745 (z,t45)
+Production of a triton, leaving the residual nucleus in the
+45th excited state.
+
+
+
+746 (z,t46)
+Production of a triton, leaving the residual nucleus in the
+46th excited state.
+
+
+
+747 (z,t47)
+Production of a triton, leaving the residual nucleus in the
+47th excited state.
+
+
+
+748 (z,t48)
+Production of a triton, leaving the residual nucleus in the
+48th excited state.
+
+
+
+749 (z,tc)
+Production of a triton in the continuum not included in the
+above discrete representation.
+
+
+
+750 (z,3He0)
+Production of a 3He particle, leaving the residual
+nucleus in the ground state.
+
+Not allowed for incident 3He particles. Use MT=2.
+
+751 (z,3He1)
+Production of a 3He particle, leaving the residual
+nucleus in the first excited state.
+
+
+
+752 (z,3He2)
+Production of a 3He particle, leaving the residual
+nucleus in the 2nd excited state.
+
+
+
+753 (z,3He3)
+Production of a 3He particle, leaving the residual
+nucleus in the 3rd excited state.
+
+
+
+754 (z,3He4)
+Production of a 3He particle, leaving the residual
+nucleus in the 4th excited state.
+
+
+
+755 (z,3He5)
+Production of a 3He particle, leaving the residual
+nucleus in the 5th excited state.
+
+
+
+756 (z,3He6)
+Production of a 3He particle, leaving the residual
+nucleus in the 6th excited state.
+
+
+
+757 (z,3He7)
+Production of a 3He particle, leaving the residual
+nucleus in the 7th excited state.
+
+
+
+758 (z,3He8)
+Production of a 3He particle, leaving the residual
+nucleus in the 8th excited state.
+
+
+
+759 (z,3He9)
+Production of a 3He particle, leaving the residual
+nucleus in the 9th excited state.
+
+
+
+760 (z,3He10)
+Production of a 3He particle, leaving the residual
+nucleus in the 10th excited state.
+
+
+
+761 (z,3He11)
+Production of a 3He particle, leaving the residual
+nucleus in the 11th excited state.
+
+
+
+762 (z,3He12)
+Production of a 3He particle, leaving the residual
+nucleus in the 12th excited state.
+
+
+
+763 (z,3He13)
+Production of a 3He particle, leaving the residual
+nucleus in the 13th excited state.
+
+
+
+764 (z,3He14)
+Production of a 3He particle, leaving the residual
+nucleus in the 14th excited state.
+
+
+
+765 (z,3He15)
+Production of a 3He particle, leaving the residual
+nucleus in the 15th excited state.
+
+
+
+766 (z,3He16)
+Production of a 3He particle, leaving the residual
+nucleus in the 16th excited state.
+
+
+
+767 (z,3He17)
+Production of a 3He particle, leaving the residual
+nucleus in the 17th excited state.
+
+
+
+768 (z,3He18)
+Production of a 3He particle, leaving the residual
+nucleus in the 18th excited state.
+
+
+
+769 (z,3He19)
+Production of a 3He particle, leaving the residual
+nucleus in the 19th excited state.
+
+
+
+770 (z,3He20)
+Production of a 3He particle, leaving the residual
+nucleus in the 20th excited state.
+
+
+
+771 (z,3He21)
+Production of a 3He particle, leaving the residual
+nucleus in the 21th excited state.
+
+
+
+772 (z,3He22)
+Production of a 3He particle, leaving the residual
+nucleus in the 22th excited state.
+
+
+
+773 (z,3He23)
+Production of a 3He particle, leaving the residual
+nucleus in the 23th excited state.
+
+
+
+774 (z,3He24)
+Production of a 3He particle, leaving the residual
+nucleus in the 24th excited state.
+
+
+
+775 (z,3He25)
+Production of a 3He particle, leaving the residual
+nucleus in the 25th excited state.
+
+
+
+776 (z,3He26)
+Production of a 3He particle, leaving the residual
+nucleus in the 26th excited state.
+
+
+
+777 (z,3He27)
+Production of a 3He particle, leaving the residual
+nucleus in the 27th excited state.
+
+
+
+778 (z,3He28)
+Production of a 3He particle, leaving the residual
+nucleus in the 28th excited state.
+
+
+
+779 (z,3He29)
+Production of a 3He particle, leaving the residual
+nucleus in the 29th excited state.
+
+
+
+780 (z,3He30)
+Production of a 3He particle, leaving the residual
+nucleus in the 30th excited state.
+
+
+
+781 (z,3He31)
+Production of a 3He particle, leaving the residual
+nucleus in the 31th excited state.
+
+
+
+782 (z,3He32)
+Production of a 3He particle, leaving the residual
+nucleus in the 32th excited state.
+
+
+
+783 (z,3He33)
+Production of a 3He particle, leaving the residual
+nucleus in the 33th excited state.
+
+
+
+784 (z,3He34)
+Production of a 3He particle, leaving the residual
+nucleus in the 34th excited state.
+
+
+
+785 (z,3He35)
+Production of a 3He particle, leaving the residual
+nucleus in the 35th excited state.
+
+
+
+786 (z,3He36)
+Production of a 3He particle, leaving the residual
+nucleus in the 36th excited state.
+
+
+
+787 (z,3He37)
+Production of a 3He particle, leaving the residual
+nucleus in the 37th excited state.
+
+
+
+788 (z,3He38)
+Production of a 3He particle, leaving the residual
+nucleus in the 38th excited state.
+
+
+
+789 (z,3He39)
+Production of a 3He particle, leaving the residual
+nucleus in the 39th excited state.
+
+
+
+790 (z,3He40)
+Production of a 3He particle, leaving the residual
+nucleus in the 40th excited state.
+
+
+
+791 (z,3He41)
+Production of a 3He particle, leaving the residual
+nucleus in the 41th excited state.
+
+
+
+792 (z,3He42)
+Production of a 3He particle, leaving the residual
+nucleus in the 42th excited state.
+
+
+
+793 (z,3He43)
+Production of a 3He particle, leaving the residual
+nucleus in the 43th excited state.
+
+
+
+794 (z,3He44)
+Production of a 3He particle, leaving the residual
+nucleus in the 44th excited state.
+
+
+
+795 (z,3He45)
+Production of a 3He particle, leaving the residual
+nucleus in the 45th excited state.
+
+
+
+796 (z,3He46)
+Production of a 3He particle, leaving the residual
+nucleus in the 46th excited state.
+
+
+
+797 (z,3He47)
+Production of a 3He particle, leaving the residual
+nucleus in the 47th excited state.
+
+
+
+798 (z,3He48)
+Production of a 3He particle, leaving the residual
+nucleus in the 48th excited state.
+
+
+
+799 (z,3Hec)
+Production of a 3He particle in the continuum not
+included in the above discrete representation.
+
+
+
+800 (z,a0)
+Production of an alpha particle, leaving the residual
+nucleus in the ground state.
+
+Not allowed for incident alphas. Use MT=2.
+
+801 (z,a1)
+Production of an alpha particle, leaving the residual
+nucleus in the first excited state.
+
+
+
+802 (z,a2)
+Production of an alpha particle, leaving the residual
+nucleus in the 2nd excited state.
+
+
+
+803 (z,a3)
+Production of an alpha particle, leaving the residual
+nucleus in the 3rd excited state.
+
+
+
+804 (z,a4)
+Production of an alpha particle, leaving the residual
+nucleus in the 4th excited state.
+
+
+
+805 (z,a5)
+Production of an alpha particle, leaving the residual
+nucleus in the 5th excited state.
+
+
+
+806 (z,a6)
+Production of an alpha particle, leaving the residual
+nucleus in the 6th excited state.
+
+
+
+807 (z,a7)
+Production of an alpha particle, leaving the residual
+nucleus in the 7th excited state.
+
+
+
+808 (z,a8)
+Production of an alpha particle, leaving the residual
+nucleus in the 8th excited state.
+
+
+
+809 (z,a9)
+Production of an alpha particle, leaving the residual
+nucleus in the 9th excited state.
+
+
+
+810 (z,a10)
+Production of an alpha particle, leaving the residual
+nucleus in the 10th excited state.
+
+
+
+811 (z,a11)
+Production of an alpha particle, leaving the residual
+nucleus in the 11th excited state.
+
+
+
+812 (z,a12)
+Production of an alpha particle, leaving the residual
+nucleus in the 12th excited state.
+
+
+
+813 (z,a13)
+Production of an alpha particle, leaving the residual
+nucleus in the 13th excited state.
+
+
+
+814 (z,a14)
+Production of an alpha particle, leaving the residual
+nucleus in the 14th excited state.
+
+
+
+815 (z,a15)
+Production of an alpha particle, leaving the residual
+nucleus in the 15th excited state.
+
+
+
+816 (z,a16)
+Production of an alpha particle, leaving the residual
+nucleus in the 16th excited state.
+
+
+
+817 (z,a17)
+Production of an alpha particle, leaving the residual
+nucleus in the 17th excited state.
+
+
+
+818 (z,a18)
+Production of an alpha particle, leaving the residual
+nucleus in the 18th excited state.
+
+
+
+819 (z,a19)
+Production of an alpha particle, leaving the residual
+nucleus in the 19th excited state.
+
+
+
+820 (z,a20)
+Production of an alpha particle, leaving the residual
+nucleus in the 20th excited state.
+
+
+
+821 (z,a21)
+Production of an alpha particle, leaving the residual
+nucleus in the 21th excited state.
+
+
+
+822 (z,a22)
+Production of an alpha particle, leaving the residual
+nucleus in the 22th excited state.
+
+
+
+823 (z,a23)
+Production of an alpha particle, leaving the residual
+nucleus in the 23th excited state.
+
+
+
+824 (z,a24)
+Production of an alpha particle, leaving the residual
+nucleus in the 24th excited state.
+
+
+
+825 (z,a25)
+Production of an alpha particle, leaving the residual
+nucleus in the 25th excited state.
+
+
+
+826 (z,a26)
+Production of an alpha particle, leaving the residual
+nucleus in the 26th excited state.
+
+
+
+827 (z,a27)
+Production of an alpha particle, leaving the residual
+nucleus in the 27th excited state.
+
+
+
+828 (z,a28)
+Production of an alpha particle, leaving the residual
+nucleus in the 28th excited state.
+
+
+
+829 (z,a29)
+Production of an alpha particle, leaving the residual
+nucleus in the 29th excited state.
+
+
+
+830 (z,a30)
+Production of an alpha particle, leaving the residual
+nucleus in the 30th excited state.
+
+
+
+831 (z,a31)
+Production of an alpha particle, leaving the residual
+nucleus in the 31th excited state.
+
+
+
+832 (z,a32)
+Production of an alpha particle, leaving the residual
+nucleus in the 32th excited state.
+
+
+
+833 (z,a33)
+Production of an alpha particle, leaving the residual
+nucleus in the 33th excited state.
+
+
+
+834 (z,a34)
+Production of an alpha particle, leaving the residual
+nucleus in the 34th excited state.
+
+
+
+835 (z,a35)
+Production of an alpha particle, leaving the residual
+nucleus in the 35th excited state.
+
+
+
+836 (z,a36)
+Production of an alpha particle, leaving the residual
+nucleus in the 36th excited state.
+
+
+
+837 (z,a37)
+Production of an alpha particle, leaving the residual
+nucleus in the 37th excited state.
+
+
+
+838 (z,a38)
+Production of an alpha particle, leaving the residual
+nucleus in the 38th excited state.
+
+
+
+839 (z,a39)
+Production of an alpha particle, leaving the residual
+nucleus in the 39th excited state.
+
+
+
+840 (z,a40)
+Production of an alpha particle, leaving the residual
+nucleus in the 40th excited state.
+
+
+
+841 (z,a41)
+Production of an alpha particle, leaving the residual
+nucleus in the 41th excited state.
+
+
+
+842 (z,a42)
+Production of an alpha particle, leaving the residual
+nucleus in the 42th excited state.
+
+
+
+843 (z,a43)
+Production of an alpha particle, leaving the residual
+nucleus in the 43th excited state.
+
+
+
+844 (z,a44)
+Production of an alpha particle, leaving the residual
+nucleus in the 44th excited state.
+
+
+
+845 (z,a45)
+Production of an alpha particle, leaving the residual
+nucleus in the 45th excited state.
+
+
+
+846 (z,a46)
+Production of an alpha particle, leaving the residual
+nucleus in the 46th excited state.
+
+
+
+847 (z,a47)
+Production of an alpha particle, leaving the residual
+nucleus in the 47th excited state.
+
+
+
+848 (z,a48)
+Production of an alpha particle, leaving the residual
+nucleus in the 48th excited state.
+
+
+
+849 (z,ac)
+Production of an alpha particle in the continuum not
+included in the above discrete representation.
+
+
+
diff --git a/test/periodic/icons/Zr-loc.gif b/test/periodic/icons/Zr-loc.gif
new file mode 100644
index 0000000000000000000000000000000000000000..9c62b327fb922175a794c1d887a8af91ca0c0789
Binary files /dev/null and b/test/periodic/icons/Zr-loc.gif differ
diff --git a/test/periodic/icons/ptable_l.xpm b/test/periodic/icons/ptable_l.xpm
new file mode 100644
index 0000000000000000000000000000000000000000..4e1a62a9f675534cfb90e98fb992ddfb76152f2f
--- /dev/null
+++ b/test/periodic/icons/ptable_l.xpm
@@ -0,0 +1,75 @@
+/* XPM */
+static char *ptable_l[] = {
+/* width height num_colors chars_per_pixel */
+" 106 60 8 1",
+/* colors */
+". c #f8fcf8",
+"# c #98ccf8",
+"a c #f8fc30",
+"b c #e80000",
+"c c #00ec00",
+"d c #b8b8b8",
+"e c #888888",
+"f c #300098",
+/* pixels */
+"bbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbb",
+"bbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbb",
+"bbeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeebb",
+"bbe....................................................................................................ebb",
+"bbe....................................................................................................ebb",
+"bbe...####.............................................................................................ebb",
+"bbe...####.....................................................................................aaaa....ebb",
+"bbe...####.....................................................................................aaaa....ebb",
+"bbe...####.....................................................................................aaaa....ebb",
+"bbe............................................................................................aaaa....ebb",
+"bbe...####.####.......................................................aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.......................................................aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.......................................................aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.......................................................aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe....................................................................................................ebb",
+"bbe...####.####.......................................................aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.......................................................aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.......................................................aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.......................................................aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe....................................................................................................ebb",
+"bbe...####.####.....bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.....bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.....bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.....bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe....................................................................................................ebb",
+"bbe...####.####.....bbbb.ffff.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.....bbbb.ffff.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.....bbbb.ffff.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####.....bbbb.ffff.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe....................................................................................................ebb",
+"bbe...####.####.....bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####...e.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####...e.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...####.####...e.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.aaaa.aaaa.aaaa.aaaa.aaaa.aaaa....ebb",
+"bbe...............e....................................................................................ebb",
+"bbe...####.####...e.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.dddd.aaaa.dddd.aaaa.dddd.aaaa....ebb",
+"bbe...####.####.e.e.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.dddd.aaaa.dddd.aaaa.dddd.aaaa....ebb",
+"bbe...####.####.e.e.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.dddd.aaaa.dddd.aaaa.dddd.aaaa....ebb",
+"bbe...####.####.e.e.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.bbbb.dddd.aaaa.dddd.aaaa.dddd.aaaa....ebb",
+"bbe.............e.e....................................................................................ebb",
+"bbe.............e.e....................................................................................ebb",
+"bbe.............e.e....................................................................................ebb",
+"bbe.............e.e....................................................................................ebb",
+"bbe.............e.e....................................................................................ebb",
+"bbe.............e.e....................................................................................ebb",
+"bbe.............e.e....................................................................................ebb",
+"bbe.............e.e.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc..............ebb",
+"bbe.............e.e.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc..............ebb",
+"bbe.............e...cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc..............ebb",
+"bbe.............e...cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc..............ebb",
+"bbe.............e......................................................................................ebb",
+"bbe.............e...cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc..............ebb",
+"bbe.............e...cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc..............ebb",
+"bbe.................cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc..............ebb",
+"bbe.................cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc.cccc..............ebb",
+"bbe....................................................................................................ebb",
+"bbe....................................................................................................ebb",
+"bbeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeeebb",
+"bbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbb",
+"bbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbbb"
+};
diff --git a/test/periodic/icons/ptable_s.xpm b/test/periodic/icons/ptable_s.xpm
new file mode 100644
index 0000000000000000000000000000000000000000..de9b43d8c283f47470f6a871fcbf24d9099fcd6b
--- /dev/null
+++ b/test/periodic/icons/ptable_s.xpm
@@ -0,0 +1,177 @@
+/* XPM */
+static char *ptable_s[] = {
+/* width height num_colors chars_per_pixel */
+" 37 24 146 2",
+/* colors */
+".. c #f8fcf8",
+".# c #f8fc00",
+".a c #f8ece8",
+".b c #f8cc30",
+".c c #f0dcd8",
+".d c #e8ecf0",
+".e c #e8dcd8",
+".f c #e0ccc8",
+".g c #d8bcb8",
+".h c #d8aca8",
+".i c #d0d4d0",
+".j c #d09c98",
+".k c #c8cce8",
+".l c #c89490",
+".m c #c88c88",
+".n c #c87858",
+".o c #c86850",
+".p c #c86048",
+".q c #c85840",
+".r c #c84838",
+".s c #c83030",
+".t c #c80000",
+".u c #c0c4e0",
+".v c #c07878",
+".w c #c02830",
+".x c #b8bcd8",
+".y c #b89c78",
+".z c #b88c68",
+".A c #b87070",
+".B c #b87050",
+".C c #b86868",
+".D c #b85040",
+".E c #b85038",
+".F c #b84838",
+".G c #b83838",
+".H c #b82830",
+".I c #b0b498",
+".J c #b0ac88",
+".K c #b05858",
+".L c #b02828",
+".M c #a8acd8",
+".N c #a8ac90",
+".O c #a89470",
+".P c #a88c68",
+".Q c #a86850",
+".R c #a85050",
+".S c #a85038",
+".T c #a84848",
+".U c #a84038",
+".V c #a83838",
+".W c #a83028",
+".X c #a82028",
+".Y c #a0a480",
+".Z c #989cd0",
+".0 c #989cc8",
+".1 c #989470",
+".2 c #988440",
+".3 c #985040",
+".4 c #984838",
+".5 c #983830",
+".6 c #906850",
+".7 c #903028",
+".8 c #902828",
+".9 c #902030",
+"#. c #901828",
+"## c #901818",
+"#a c #900808",
+"#b c #888cc8",
+"#c c #887060",
+"#d c #887058",
+"#e c #884838",
+"#f c #883830",
+"#g c #883028",
+"#h c #882838",
+"#i c #882828",
+"#j c #881820",
+"#k c #881010",
+"#l c #880808",
+"#m c #803040",
+"#n c #787058",
+"#o c #785040",
+"#p c #784838",
+"#q c #783848",
+"#r c #783038",
+"#s c #782830",
+"#t c #782028",
+"#u c #781820",
+"#v c #7070b8",
+"#w c #703850",
+"#x c #703028",
+"#y c #685040",
+"#z c #684838",
+"#A c #684050",
+"#B c #683848",
+"#C c #683028",
+"#D c #682838",
+"#E c #682028",
+"#F c #681828",
+"#G c #681818",
+"#H c #6060f8",
+"#I c #6060b8",
+"#J c #603830",
+"#K c #5858b0",
+"#L c #584050",
+"#M c #583848",
+"#N c #583038",
+"#O c #582838",
+"#P c #582820",
+"#Q c #582018",
+"#R c #581818",
+"#S c #5050a8",
+"#T c #505068",
+"#U c #504860",
+"#V c #484058",
+"#W c #483848",
+"#X c #482018",
+"#Y c #481818",
+"#Z c #4040a8",
+"#0 c #403850",
+"#1 c #403830",
+"#2 c #402028",
+"#3 c #401820",
+"#4 c #400810",
+"#5 c #3838a8",
+"#6 c #381828",
+"#7 c #302838",
+"#8 c #302820",
+"#9 c #301818",
+"a. c #300810",
+"a# c #282898",
+"aa c #282028",
+"ab c #202030",
+"ac c #201010",
+"ad c #200810",
+"ae c #200808",
+"af c #181898",
+"ag c #181820",
+"ah c #181018",
+"ai c #100810",
+"aj c #100808",
+"ak c #080890",
+"al c #080888",
+"am c #080810",
+"an c #006000",
+"ao c #0000c8",
+"ap c #000000",
+/* pixels */
+"aoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoao..",
+"aoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoaoao..",
+"..........................................................................",
+"..........................................................................",
+"#H#H.................................................................#.#..",
+"#H#H.................................................................#.#..",
+"#H#H#H#H.........................................#.#.#.#.#.#.#.#.#.#.#.#..",
+"#H#H#H#H.........................................#.#.#.#.#.#.#.#.#.#.#.#..",
+"#H#H#H#H.........................................#.#.#.#.#.#.#.#.#.#.#.#..",
+"#H#H#H#H.........................................#.#.#.#.#.#.#.#.#.#.#.#..",
+"#H#H#H#H.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.#.#.#.#.#.#.#.#.#.#.#.#..",
+"#H#H#H#H.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.#.#.#.#.#.#.#.#.#.#.#.#..",
+"#H#H#H#H.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.#.#.#.#.#.#.#.#.#.#.#.#..",
+"#H#H#H#H.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.#.#.#.#.#.#.#.#.#.#.#.#..",
+"#H#H#H#H.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.#.#.#.#.#.#.#.#.#.#.#.#..",
+"#H#H#H#H.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.#.#.#.#.#.#.#.#.#.#.#.#..",
+"#H#H#H#H.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.u.u.#.#.u.u.#.#.u.u.#.#..",
+"#H#H#H#H.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.t.u.u.#.#.u.u.#.#.u.u.#.#..",
+"..........................................................................",
+"..........................................................................",
+"........anananananananananananananananananananananananananananan..........",
+"........anananananananananananananananananananananananananananan..........",
+"........anananananananananananananananananananananananananananan..........",
+"........anananananananananananananananananananananananananananan.........."
+};
diff --git a/test/periodic/icons/topbar.gif b/test/periodic/icons/topbar.gif
new file mode 100644
index 0000000000000000000000000000000000000000..85baf7a26d7fae9bc02ee6f9dc0f10973059fefd
Binary files /dev/null and b/test/periodic/icons/topbar.gif differ