diff --git a/NPLib/Physics/CMakeLists.txt b/NPLib/Physics/CMakeLists.txt
index 86f1a1b922f3c77f9006fc8ab7c8d72c89216db8..02cf69825ff129124df7a827be3c897be0ba6bf6 100644
--- a/NPLib/Physics/CMakeLists.txt
+++ b/NPLib/Physics/CMakeLists.txt
@@ -6,6 +6,10 @@ add_custom_command(OUTPUT NPQFSDict.cxx COMMAND ${CMAKE_BINARY_DIR}/scripts/buil
add_custom_command(OUTPUT NPDecayDict.cxx COMMAND ${CMAKE_BINARY_DIR}/scripts/build_dict.sh NPDecay.h NPDecayDict.cxx NPDecay.rootmap libNPPhysics.so NPDecayLinkDef.h DEPENDS NPDecay.h NPDecayLinkDef.h)
+add_custom_command(OUTPUT NPFissionDecayDict.cxx COMMAND ${CMAKE_BINARY_DIR}/scripts/build_dict.sh NPFissionDecay.h NPFissionDecayDict.cxx NPFissionDecay.rootmap libNPPhysics.so NPFissionDecayLinkDef.h DEPENDS NPFissionDecay.h NPFissionDecayLinkDef.h)
+
+add_custom_command(OUTPUT GEFDict.cxx COMMAND ${CMAKE_BINARY_DIR}/scripts/build_dict.sh GEF.h GEFDict.cxx GEF.rootmap libNPPhysics.so GEFLinkDef.h DEPENDS GEF.h GEFLinkDef.h)
+
add_custom_command(OUTPUT NPEnergyLossDict.cxx COMMAND ${CMAKE_BINARY_DIR}/scripts/build_dict.sh NPEnergyLoss.h NPEnergyLossDict.cxx NPEnergyLoss.rootmap libNPPhysics.so NPEnergyLossLinkDef.h DEPENDS NPEnergyLoss.h NPEnergyLossLinkDef.h)
add_custom_command(OUTPUT TInitialConditionsDict.cxx COMMAND ${CMAKE_BINARY_DIR}/scripts/build_dict.sh TInitialConditions.h TInitialConditionsDict.cxx TInitialConditions.rootmap libNPInitialConditions.so DEPENDS TInitialConditions.h)
@@ -14,7 +18,9 @@ add_custom_command(OUTPUT TInteractionCoordinatesDict.cxx COMMAND ${CMAKE_BINARY
add_custom_command(OUTPUT TReactionConditionsDict.cxx COMMAND ${CMAKE_BINARY_DIR}/scripts/build_dict.sh TReactionConditions.h TReactionConditionsDict.cxx TReactionConditions.rootmap libNPReactionConditions.so DEPENDS TReactionConditions.h)
-add_library(NPPhysics SHARED NPDecay.cxx NPBeam.cxx NPEnergyLoss.cxx NPFunction.cxx NPParticle.cxx NPReaction.cxx NPQFS.cxx NPParticleDict.cxx NPReactionDict.cxx NPQFSDict.cxx NPEnergyLossDict.cxx )
+add_custom_command(OUTPUT TFissionConditionsDict.cxx COMMAND ${CMAKE_BINARY_DIR}/scripts/build_dict.sh TFissionConditions.h TFissionConditionsDict.cxx TFissionConditions.rootmap libNPFissionConditions.so DEPENDS TFissionConditions.h)
+
+add_library(NPPhysics SHARED GEF.cxx NPFissionDecay.cxx NPDecay.cxx NPBeam.cxx NPEnergyLoss.cxx NPFunction.cxx NPParticle.cxx NPReaction.cxx NPQFS.cxx NPParticleDict.cxx NPReactionDict.cxx NPQFSDict.cxx NPEnergyLossDict.cxx )
target_link_libraries(NPPhysics ${ROOT_LIBRARIES} Physics NPCore)
add_library(NPInitialConditions SHARED TInitialConditions.cxx TInitialConditionsDict.cxx )
@@ -26,4 +32,8 @@ target_link_libraries(NPInteractionCoordinates ${ROOT_LIBRARIES} )
add_library(NPReactionConditions SHARED TReactionConditions.cxx TReactionConditionsDict.cxx)
target_link_libraries(NPReactionConditions ${ROOT_LIBRARIES} )
-install(FILES NPDecay.h NPBeam.h NPEnergyLoss.h NPFunction.h NPParticle.h NPNucleus.h NPReaction.h NPQFS.h TInitialConditions.h TInteractionCoordinates.h TReactionConditions.h DESTINATION ${CMAKE_INCLUDE_OUTPUT_DIRECTORY})
+add_library(NPFissionConditions SHARED TFissionConditions.cxx TFissionConditionsDict.cxx)
+target_link_libraries(NPFissionConditions ${ROOT_LIBRARIES} )
+
+
+install(FILES GEF.h NPFissionDecay.h NPDecay.h NPBeam.h NPEnergyLoss.h NPFunction.h NPParticle.h NPNucleus.h NPReaction.h NPQFS.h TInitialConditions.h TInteractionCoordinates.h TReactionConditions.h TFissionConditions.h DESTINATION ${CMAKE_INCLUDE_OUTPUT_DIRECTORY})
diff --git a/NPLib/Physics/GEF.cxx b/NPLib/Physics/GEF.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..81e57315e1cf9316d00a096836a95fa868e59be8
--- /dev/null
+++ b/NPLib/Physics/GEF.cxx
@@ -0,0 +1,5055 @@
+#include "GEF.h"
+
+GEF::GEF(NPL::Particle FissNucl)
+{
+ FIS = FissNucl;
+ Afis = FIS.GetA();
+ Zfis = FIS.GetZ();
+
+ ReadBEldmTF();
+ ReadBEexp();
+ ReadDEFOtab();
+ ReadShellMO();
+ ReadNucProp();
+ ReadGEFParameters();
+
+ pi = TMath::Pi();
+ rn = new TRandom3();
+ Init();
+ FissionGENERAL();
+}
+
+GEF::~GEF(void){}
+
+void GEF::Init(void)
+{
+ Ngtot = 0;
+ Nglight = 0;
+ Ngheavy = 0;
+ Egtot1000 = 0;
+ DZ_S2_lowE = 0;
+
+ N_Error_Max = 10;
+ I_Error = 0;
+ I_DelGam = 0;
+ P_Z_CN = Zfis;
+ P_A_CN = Afis;
+ P_E_exc = 0;
+ P_I_rms_CN = 0;
+ I_A_CN = P_A_CN;
+ I_Z_CN = P_Z_CN;
+
+ // Use nominal parameter values:
+ P_DZ_Mean_S1 = _P_DZ_Mean_S1;
+ P_DZ_Mean_S2 = _P_DZ_Mean_S2;
+ P_DZ_Mean_S3 = _P_DZ_Mean_S3;
+ P_DZ_Mean_S4 = _P_DZ_Mean_S4;
+ P_Z_Curv_S1 = _P_Z_Curv_S1;
+ P_Z_Curv_S2 = _P_Z_Curv_S2;
+ S2leftmod = _S2leftmod;
+ P_A_Width_S2 = _P_A_Width_S2;
+ P_Z_Curv_S3 = _P_Z_Curv_S3;
+ P_Z_Curv_S4 = _P_Z_Curv_S4;
+ Delta_S0 = _Delta_S0;
+ P_Shell_S1 = _P_Shell_S1;
+ P_Shell_S2 = _P_Shell_S2;
+ P_Shell_S3 = _P_Shell_S3;
+ P_Shell_S4 = _P_Shell_S4;
+ T_low_S1 = _T_low_S1;
+ T_low_S2 = _T_low_S2;
+ T_low_S3 = _T_low_S3;
+ T_low_S4 = _T_low_S4;
+ T_low_SL = _T_low_SL;
+ P_att_pol = _P_att_pol;
+ P_att_rel = _P_att_rel;
+ HOMPOL = _HOMPOL;
+ POLARadd = _POLARadd;
+ Jscaling = _Jscaling;
+
+
+ // Control parameters:
+ B_F = 0; // Fission barrier
+ B_F_ld = 0; // Fission barrier, liquid drop
+ E_B = 0; // Outer fission barrier
+ E_B_ld = 0; // Outer fission barrier, liquid drop
+ R_E_exc_Eb = 0; // Energy above outer barrier
+ R_E_exc_GS = 0; // Energy above ground state
+ P_Z_Mean_S0 = 0; // Mean Z of Mode 1
+ P_Z_Mean_S1 = 52.8; // Mean Z of Mode 1
+ P_Z_Mean_S2 = 55; // Mean Z of Mode 2
+ P_Z_Mean_S3 = 65; // Mean Z of Mode 3
+ P_Z_Mean_S4 = 42.05; // Mean Z of Mode 4
+ NC_Mode_0 = 0; // Mean N of symm. Mode
+ NC_Mode_1 = 0; // Mean N of Mode 1
+ NC_Mode_2 = 0; // Mean N of Mode 2
+ NC_Mode_3 = 0; // Mean N of Mode 3
+ NC_Mode_4 = 0;
+ B_S1 = 0; // Barrier S1, relative to SL
+ B_S2 = 0; // Barrier S2, relative to SL
+ B_S3 = 0; // Barrier S3, relative to SL
+ B_S4 = 0;
+ B_S11 = 0; // Barrier S11, relative to SL
+ B_S22 = 0; // Barrier S22, relative to SL
+ DES11ZPM = 0; // Mod. of eff. barrier due to ZPM in overlap
+ Delta_NZ_Pol = 0; // Polarization for 132Sn
+ Yield_Mode_0 = 0; // Relative yield of SL
+ Yield_Mode_1 = 0; // Relative yield of S1
+ Yield_Mode_2 = 0; // Relative yield of S2
+ Yield_Mode_3 = 0; // Relative yield of S3
+ Yield_Mode_4 = 0; // Relative yield of S4
+ Yield_Mode_11 = 0; // Relative yield of S11
+ Yield_Mode_22 = 0; // Relative yield of S22
+ P_POL_CURV_S0 = 0; // Stiffnes in N/Z
+ T_Coll_Mode_0 = 0; // Effective collective temperature
+ E_Exc_S0 = 0; // Energy over barrier of symmetric channel
+ E_Exc_S1 = 0; // Energy over barrier of S1 channel
+ E_Exc_S2 = 0; // Energy over barrier of S2 channel
+ E_Exc_S3 = 0; // Energy over barrier of S3 channel
+ E_Exc_S4 = 0; // Energy over barrier of S4 channel
+ E_Exc_S11 = 0; // Energy over barrier of S11 channel
+ E_Exc_S22 = 0; // Energy over barrier of S22 channel
+ E_POT_SCISSION = 0; // Potential-energy gain saddle-scission
+ E_diss_Scission = 0; // Dissipated energy between saddle and scission
+ EINTR_SCISSION = 0; // Intrinsic excitation energy at scission
+ EeffS1 = 0; // Governs S1 reduction
+ Sigpol_Mode_0 = 0; // Width of isobaric Z distribution
+}
+
+void GEF::ReadBEldmTF(void)
+{
+ char filename[256];
+ char *fname;
+ Float_t temp;
+ for(int i=0;i<204;i++)
+ for(int j=0;j<137;j++)
+ BEldmTF[i][j]=0;
+ int counter=0;
+
+ fname = getenv("NPTOOL");
+ sprintf(filename,"%s/NPLib/Physics/PAR_GEF/BEldmTF.dat",fname);
+
+ ifstream file(filename);
+ string line;
+ if (!file)
+ cout << "Couldn't open file : " << filename << endl ;
+ else
+ {
+ //cout << "File : " << filename << endl;
+ for(int i=0;i<3;i++)
+ {
+ getline(file,line);
+ //cout<<line<<endl;
+ }
+ while(getline(file,line))
+ {
+ istringstream read (line);
+ //cout<<line<<endl;
+ while(read)
+ {
+ read>>temp;
+ if((counter/136+1)<204&&(counter%136+1)<137)
+ {
+ BEldmTF[counter/136+1][counter%136+1] = temp;
+ //cout<<"i: "<< counter/136+1<< " j: "<<counter%136+1<<" "<<BEldmTF[counter/136+1][counter%136+1]<<endl;
+ }
+ counter++;
+ }
+ counter--; //while(read) it is satisifed one more time at the end of each line
+ }
+ }
+}
+
+void GEF::ReadBEexp(void)
+{
+ char filename[256];
+ char *fname;
+ int zz, aa;
+ float temp;
+ for(int i=0;i<204;i++)
+ for(int j=0;j<137;j++)
+ BEexp[i][j]=-1.e11;
+
+ fname = getenv("NPTOOL");
+ sprintf(filename,"%s/NPLib/Physics/PAR_GEF/BEexp.dat",fname);
+
+ ifstream file(filename);
+ string line;
+ if (!file)
+ cout << "Couldn't open file : " << filename << endl ;
+ else
+ {
+ //cout << "File : " << filename << endl;
+ for(int i=0;i<3;i++)
+ {
+ getline(file,line);
+ //cout<<line<<endl;
+ }
+ while(getline(file,line))
+ {
+ istringstream read (line);
+ read>>zz>>aa>>temp;
+ BEexp[aa-zz][zz]=temp;
+ //cout<<zz<<" "<<aa<<" "<<BEexp[aa-zz][zz]<<endl;
+ }
+ }
+}
+
+void GEF::ReadDEFOtab(void)
+{
+ char filename[256];
+ char *fname;
+ int zz, nn;
+ float temp1,temp2NotUsed;
+ for(int i=0;i<237;i++)
+ for(int j=0;j<137;j++)
+ DEFOtab[i][j]=0.;
+
+ fname = getenv("NPTOOL");
+ sprintf(filename,"%s/NPLib/Physics/PAR_GEF/DEFO.dat",fname);
+
+ ifstream file(filename);
+ string line;
+ if (!file)
+ cout << "Couldn't open file : " << filename << endl ;
+ else
+ {
+ //cout << "File : " << filename << endl;
+ while(getline(file,line))
+ {
+ istringstream read (line);
+ read>>zz>>nn>>temp1>>temp2NotUsed;
+ DEFOtab[nn][zz]=temp1;
+ //cout<<zz<<" "<<nn<<" "<<DEFOtab[nn][zz]<<endl;
+ }
+ }
+}
+
+void GEF::ReadShellMO(void)
+{
+ char filename[256];
+ char *fname;
+ Float_t temp;
+ for(int i=0;i<204;i++)
+ for(int j=0;j<137;j++)
+ ShellMO[i][j]=0;
+ int counter=0;
+
+ fname = getenv("NPTOOL");
+ sprintf(filename,"%s/NPLib/Physics/PAR_GEF/ShellMO.dat",fname);
+
+ ifstream file(filename);
+ string line;
+ if (!file)
+ cout << "Couldn't open file : " << filename << endl ;
+ else
+ {
+ //cout << "File : " << filename << endl;
+ for(int i=0;i<2;i++)
+ {
+ getline(file,line);
+ //cout<<line<<endl;
+ }
+ while(getline(file,line))
+ {
+ istringstream read (line);
+ //cout<<line<<endl;
+ while(read)
+ {
+ read>>temp;
+ if((counter/136+1)<204&&(counter%136+1)<137)
+ {
+ ShellMO[counter/136+1][counter%136+1] = temp;
+ //cout<<"i: "<< counter/136+1<< " j: "<<counter%136+1<<" "<<ShellMO[counter/136+1][counter%136+1]<<endl;
+ }
+ counter++;
+ }
+ counter--; //while(read) it is satisifed one more time at the end of each line
+ }
+ }
+}
+
+void GEF::ReadNucProp(void)
+{
+ char filename[256];
+ char *fname;
+ int index,zz, aa,iso;
+ float spin;
+ for(int i=0;i<112;i++)
+ for(int j=0;j<280;j++)
+ R_SPI[i][j]=0.;
+
+ fname = getenv("NPTOOL");
+ sprintf(filename,"%s/NPLib/Physics/PAR_GEF/NucPropNUBASE.dat",fname);
+
+ ifstream file(filename);
+ string line;
+ if (!file)
+ cout << "Couldn't open file : " << filename << endl ;
+ else
+ {
+ for(int i=0;i<9;i++)
+ getline(file,line);
+ while(getline(file,line))
+ {
+ istringstream read (line);
+ read>>index>>zz>>aa>>iso>>spin;
+ if(iso==0)
+ R_SPI[zz][aa]=spin;
+ }
+ }
+}
+
+void GEF::ReadGEFParameters(void)
+{
+ char filename[256];
+ char *fname;
+ char temp[256];
+ float PARAM[96];
+ for(int i=0;i<96;i++)
+ PARAM[i]=0.;
+
+ fname = getenv("NPTOOL");
+ sprintf(filename,"%s/NPLib/Physics/PAR_GEF/GEFParameters.dat",fname);
+
+ ifstream file(filename);
+ string line;
+ if (!file)
+ cout << "Couldn't open file : " << filename << endl ;
+ else
+ {
+ //cout << "File : " << filename << endl;
+ for(int i=0;i<96;i++)
+ {
+ getline(file,line);
+ istringstream read (line);
+ read>>temp>>PARAM[i];
+ //cout<<PARAM[i]<<endl;
+ }
+ }
+
+ Emax_valid = PARAM[0];
+ Eexc_min_multi = PARAM[1];
+ _Delta_S0 = PARAM[2];
+ EOscale = PARAM[3];
+ Emode = int(PARAM[4]);
+ D_Par_Fac = PARAM[5];
+ _P_DZ_Mean_S1 = PARAM[6];
+ _P_DZ_Mean_S2 = PARAM[7];
+ _P_DZ_Mean_S3 = PARAM[8];
+ _P_DZ_Mean_S4 = PARAM[9];
+ ZC_Mode_4L = PARAM[10];
+ _P_Z_Curv_S1 = PARAM[11];
+ P_Z_Curvmod_S1 = PARAM[12];
+ _P_Z_Curv_S2 = PARAM[13];
+ _S2leftmod = PARAM[14];
+ P_Z_Curvmod_S2 = PARAM[15];
+ _P_A_Width_S2 = PARAM[16];
+ P_Cut_S2 = PARAM[17];
+ _P_Z_Curv_S3 = PARAM[18];
+ P_Z_Curvmod_S3 = PARAM[19];
+ P_Z_Curv_SL4 = PARAM[20];
+ P_Z_Sigma_SL4 = PARAM[21];
+ _P_Z_Curv_S4 = PARAM[22];
+ P_Z_Curvmod_S4 = PARAM[23];
+ _P_Shell_S1 = PARAM[24];
+ _P_Shell_S2 = PARAM[25];
+ _P_Shell_S3 = PARAM[26];
+ P_Shell_SL4 = PARAM[27];
+ _P_Shell_S4 = PARAM[28];
+ P_S4_NZmod = PARAM[29];
+ PZ_S3_olap_pos = PARAM[30];
+ PZ_S3_olap_curv = PARAM[31];
+ ETHRESHSUPPS1 = PARAM[32];
+ ESIGSUPPS1 = PARAM[33];
+ Level_S11 = PARAM[34];
+ Shell_fading = PARAM[35];
+ _T_low_S1 = PARAM[36];
+ _T_low_S2 = PARAM[37];
+ _T_low_S3 = PARAM[38];
+ _T_low_S4 = PARAM[39];
+ _T_low_SL = PARAM[40];
+ T_low_S11 = PARAM[41];
+ _P_att_pol = PARAM[42];
+ P_att_pol2 = PARAM[43];
+ P_att_pol3 = PARAM[44];
+ _P_att_rel = PARAM[45];
+ dE_Defo_S1 = PARAM[46];
+ dE_Defo_S2 = PARAM[47];
+ dE_Defo_S3 = PARAM[48];
+ dE_Defo_S4 = PARAM[49];
+ betaL0 = PARAM[50];
+ betaL1 = PARAM[51];
+ betaH0 = PARAM[52];
+ betaH1 = PARAM[53];
+ kappa = PARAM[54];
+ TCOLLFRAC = PARAM[55];
+ ECOLLFRAC = PARAM[56];
+ TFCOLL = PARAM[57];
+ TCOLLMIN = PARAM[58];
+ ESHIFTSASCI_intr = PARAM[59];
+ ESHIFTSASCI_coll = PARAM[60];
+ EDISSFRAC = PARAM[61];
+ Epot_shift = PARAM[62];
+ SIGDEFO = PARAM[63];
+ SIGDEFO_0 = PARAM[64];
+ SIGDEFO_slope = PARAM[65];
+ SIGENECK = PARAM[66];
+ EexcSIGrel = PARAM[67];
+ DNECK = PARAM[68];
+ FTRUNC50 = PARAM[69];
+ ZTRUNC50 = PARAM[70];
+ FTRUNC28 = PARAM[71];
+ ZTRUNC28 = PARAM[72];
+ ZMAX_S2 = PARAM[73];
+ NTRANSFEREO = PARAM[74];
+ NTRANSFERE = PARAM[75];
+ Csort = PARAM[76];
+ PZ_EO_symm = PARAM[77];
+ PN_EO_Symm = PARAM[78];
+ R_EO_THRESH = PARAM[79];
+ R_EO_SIGMA = PARAM[80];
+ R_EO_MAX = PARAM[81];
+ _POLARadd = PARAM[82];
+ POLARfac = PARAM[83];
+ T_POL_RED = PARAM[84];
+ _HOMPOL = PARAM[85];
+ ZPOL1 = PARAM[86];
+ P_n_x = PARAM[87];
+ Tscale = PARAM[88];
+ Econd = PARAM[89];
+ T_orbital = PARAM[90];
+ _Jscaling = PARAM[91];
+ Spin_odd = PARAM[92];
+ Esort_extend = PARAM[93];
+ Esort_slope = PARAM[94];
+ Esort_slope_S0 = PARAM[95];
+
+}
+
+float GEF::Max(float a, float b)
+{
+ if(a>b)
+ return a;
+ else
+ return b;
+}
+float GEF::Min(float a, float b)
+{
+ if(a<b)
+ return a;
+ else
+ return b;
+}
+float GEF::Erf(float x)
+{
+ /* Sergei Winitzki, 2008: relative accuracy < 1.4E-4 */
+ // Dim As Single a = 0.147
+ // Const As Single b = 1.27324 // 4/pi,
+ // Const As Single pi = 3.14159
+ // Dim As Single Result
+ // Result = Sqr(1.E0 - exp(-x^2 * (b + a * x^2) / (1.E0 - a * x^2) ) )
+ // If x < 0 Then Result = - Result
+ // WiErf = Result
+ return 1. - Erfc(x);
+}
+float GEF::Erfc(float x)
+{
+ /* Complementary error function from numerical recipes */
+ double t,z,r;
+ z = abs(x);
+ t = 1./(1. + 0.5 * z);
+ r = t*exp(-z*z-1.26551223+t*(1.00002368+t*(0.37409196+t*(0.09678418+t*(-0.18628806+t*(0.27886807+t*(-1.13520398+t*(1.48851587+t*(-0.82215223+t*0.17087277)))))))));
+ if (x < 0)
+ return 2. - r;
+ else
+ return r;
+}
+float GEF::Tanh(float x)
+{
+ float Result;
+ if( x >= 0)
+ Result = (1 - exp(-2*x))/(1 + exp(-2*x));
+ else
+ Result = (exp(2*x) - 1)/(exp(2*x) + 1);
+ return Result;
+}
+float GEF::Coth(float x)
+{
+ float Result;
+ if(x >= 0)
+ Result = (1 + exp(-2*x))/(1 - exp(-2*x));
+ else
+ Result = (exp(2*x) + 1)/(exp(2*x) - 1);
+ return Result;
+}
+float GEF::Log10(float R)
+{
+ return log(R) / log(10);
+}
+float GEF::Bell(float xpos, float xleft, float xright)
+{
+ // Bell-shaped curve, maximum = 1, zero for x < xleft and x > xright
+ float x,y;
+ if((xpos - xleft) > 1.e-3 && (xright - xpos) > 1.e-3)
+ {
+ x = (xpos - xleft) / (xright - xleft);
+ y = (pow(x,2) * pow(1-x,2))/0.0625;
+ }
+ else
+ y = 0;
+ return y;
+}
+float GEF::Csng(int a)
+{
+ return 1.*a;
+}
+int GEF::CInt(float a)
+{
+ return int(a);
+}
+float GEF::Mod(float a, float b)
+{
+ return a - int(a/b)*b;
+}
+float GEF::FLOOR(float a)
+{
+ return int(a);
+}
+float GEF::CEIL(float a)
+{
+ if (a>FLOOR(a))
+ return FLOOR(a)+1;
+ else
+ return a;
+}
+int GEF::Sgn(float a)
+{
+ if(a!=0)
+ return int(a/abs(a));
+ else
+ return 0;
+}
+
+void GEF::FissionGENERAL()
+{
+ float ZsqrA_fis;
+
+ //ZsqrA_fis = Csng(I_Z_CN^2) / Csng(I_A_CN);
+ ZsqrA_fis = pow(I_Z_CN,2)/I_A_CN;
+ Escission_lim = 0;//900.0 * exp(-ZsqrA_fis/13.0); // from PRC 86 (2012) 034605
+ CentralZ_FM();
+ I_N_CN = I_A_CN - I_Z_CN;
+ MeanDefScission();
+ MeanZ_asA();
+ RelationsZ_A_FM();
+ FissionBarriers();
+ PolarizationStiffness();
+
+}
+
+void GEF::CentralZ_FM(void)
+{
+ /* Central Z values of fission modes */
+ /* Test of barrier height for compact fission */
+ /* Dim As Single Fbarr_shell
+ Dim As Single Fbarr_macro
+ Fbarr_shell = 1.44 * (I_C_CN/2)^2 / (1.4 * 2 * (I_A_CN/2)^(1/3))
+ Fbarr_macro = 1.44 * (I_C_CN/2)^2 / (1.4 * 2 * (I_A_CN/2)^(1/3)) */
+
+ /* Fit to positions of fission channels (Boeckstiegel et al., 2008) */
+ /* P_DZ_Mean_S1 and P_DZ_Mean_S2 allow for slight adjustments */
+
+ float R_Z_mod, R_A_mod,R_corr2;
+ R_Z_mod = Csng(I_Z_CN);
+ R_A_mod = Csng(I_A_CN);
+ R_corr2 = 0.055 * (R_A_mod - R_Z_mod*236/92) ;
+ // * SL (S0) : *
+ ZC_Mode_0 = R_Z_mod * 0.5; /* Central Z value of SL mode */
+ // * S1 : *
+ ZC_Mode_1 = (55.8 - 54.5) / (1.56 - 1.50) *
+ (pow(R_Z_mod,1.3) / R_A_mod - 1.50) + 51.5 + P_DZ_Mean_S1 + R_corr2;
+ // * S2: *
+ ZC_Mode_2 = (55.8 - 54.5) / (1.56 - 1.50) *
+ (pow(R_Z_mod,1.3) / R_A_mod - 1.50) + 54.5 + P_DZ_Mean_S2 + R_corr2;
+ // * S3: *
+ // ZC_Mode_3 = ZC_Mode_2 + 4.5E0 + P_DZ_Mean_S3
+ ZC_Mode_3 = ZC_Mode_2 + 4.87 + P_DZ_Mean_S3;
+ ZC_Mode_3_shift = - 0.015 * (ZC_Mode_3 - ZC_Mode_0);
+
+ ZC_Mode_3 = ZC_Mode_2 + 5.5 + P_DZ_Mean_S3;
+ ZC_Mode_3_shift = - 0.035 * (ZC_Mode_3 - ZC_Mode_0);
+
+ ZC_Mode_3 = ZC_Mode_3 + ZC_Mode_3_shift;
+ // To account for ZCN-dependent shift of S3 towards minimum of mac. potential
+ // * S4: *
+ // Do not delete these lines (,because this is a very good fit!):
+ // ZC_Mode_4 = 38.5 + (I_A_CN-I_Z_CN-110)*0.12 - (I_A_CN-I_Z_CN-110)^2 * 0.009 _
+ // - (I_Z_CN-77)*0.34 + P_DZ_Mean_S4
+ // assumption: mode position moves with Z and A (adjusted to exp. data
+ // of Itkis and Andreyev et al.
+ // ZC_Mode_4 = - (55.8E0 - 54.5E0) / (1.56E0 - 1.50E0) * _
+ // (R_Z_mod^1.3E0 / I_A_CN - 1.50E0) + 37.5 + P_DZ_Mean_S4 - R_corr2 _
+ // + 0.035 * (I_A_CN- I_Z_CN - 100) //fits Tl201 (itkis), but not so well Po194,196 (Andreyev)
+ // corresponding P_DZ_Mean_S4 = -0.5
+ ZC_Mode_4 = 35.5 + Csng(I_A_CN - I_Z_CN - 100) * 0.11 + P_DZ_Mean_S4; // mean Z of light fragment in Mode 4
+
+ // Print "R_corr2: ",R_corr2
+ // Print "Mode 2, Z and N:", ZC_Mode_2, ZC_Mode_2 / P_Z_CN * (P_A_CN-P_Z_CN)
+ // Print "Mode 4, Z and N:", ZC_Mode_4, ZC_Mode_4 / P_Z_CN * (P_A_CN-P_Z_CN)
+
+ /*>*/
+ P_Z_Mean_S0 = ZC_Mode_0; /* Copy to global parameter */
+ P_Z_Mean_S1 = ZC_Mode_1; /* Copy to global parameter */
+ P_Z_Mean_S2 = ZC_Mode_2; /* " */
+ P_Z_Mean_S3 = ZC_Mode_3; /* " */
+ P_Z_Mean_S4 = ZC_Mode_4; /* " */
+ /*<*/
+}
+
+void GEF::MeanDefScission(void)
+{
+ /* Mean deformation at scission as a function of mass */
+ /* Mode 0: liquid drop */
+ beta1_prev = 0.3;
+ beta2_prev = 0.3;
+ beta1_opt = beta1_prev;
+ beta2_opt = beta2_prev;
+ for(int i = 10;i<=(I_Z_CN - 10);i++)
+ {
+ IZ1 = i;
+ Z1 = Csng(IZ1);
+ IZ2 = I_Z_CN - IZ1;
+ Z2 = Csng(IZ2);
+ A1 = Z1 / Csng(I_Z_CN) * Csng(I_A_CN);
+ A2 = I_A_CN - A1;
+
+ // Deformed shell below Z=50, valid for S0 at low E*
+ Beta[0][1][IZ1] = beta_light(IZ1,betaL0,betaL1) - 0.1;
+ // Lower deformation than S1/S2, because Coulomb repulsion from deformed heavy fragment is weaker.
+ Beta[0][2][IZ2] = beta_light(IZ2,betaL0,betaL1) - 0.1; // "
+ E_defo = LyMass(Z1,A1,Beta[0][1][IZ1]) - LyMass(Z1,A1,0.0);
+ Edefo[0][1][IZ1] = E_defo;
+ E_defo = LyMass(Z2,A2,Beta[0][2][IZ2]) - LyMass(Z2,A2,0.0);
+ Edefo[0][2][IZ2] = E_defo;
+
+ Beta_Equi(A1,A2,Z1,Z2,DNECK,beta1_prev,beta2_prev,beta1_opt,beta2_opt);
+
+ // Deformation by macroscopic model, valid for S0 at high E*
+ //Print "Mode 0, Z1,Z2,beta1,beta2 ";Z1;" ";Z2;" ";beta1_opt,beta2_opt
+ //Print Z1;" ";Z2;" ";beta1_opt,beta2_opt
+ Beta[1][1][IZ1] = beta1_opt; /* "light" fragment */
+ // Beta(4,1,IZ1) = beta1_opt
+ Beta[1][2][IZ2] = beta2_opt; /* "heavy" fragment */
+ // Beta(4,2,IZ2) = beta2_opt
+ beta1_prev = beta1_opt;
+ beta2_prev = beta2_opt;
+ E_defo = LyMass(Z1,A1,beta1_opt) - LyMass(Z1,A1,0.0);
+ Edefo[1][1][IZ1] = E_defo; /* "light" fragment */
+ // Edefo(4,1,IZ1) = E_defo
+ E_defo = LyMass(Z2,A2,beta2_opt) - LyMass(Z2,A2,0.0);
+ Edefo[1][2][IZ2] = E_defo; /* "heavy" fragment */
+ // Edefo(4,2,IZ2) = E_defo
+ }
+
+ /* Mode 1: deformed shells (light) and spherical (heavy) */
+ for(int i = 10;i<=(I_Z_CN - 10);i++)
+ {
+ Z1 = Csng(i);
+ Z2 = Csng(I_Z_CN) - Z1;
+ A1 = (Z1 - 0.5) / Csng(I_Z_CN) * Csng(I_A_CN); /* polarization roughly considered */
+ A2 = Csng(I_A_CN) - A1;
+ if(I_Z_CN * 0.5 < ZC_Mode_1)
+ {
+ // Beta_opt_light(A1,A2,Z1,Z2,dneck,0,rbeta_ld)
+ /* nu_mean of Cf requires shells in the light fragment: */
+ // rbeta = beta_light(I,betaL0,betaL1) - 0.1
+ // smaller than general deformation of light fragment
+ // (less neck influence due to spherical heavy fragment)
+ rbeta = beta_light(i,betaL0,betaL1);
+ if(rbeta < 0)
+ rbeta = 0;
+ }
+ else
+ {
+ rbeta = beta_heavy(i,betaH0,betaH1); // equal to S2 channel
+ if(rbeta < 0)
+ rbeta = 0;
+ }
+ Beta[2][1][i] = rbeta; /* "light" fragment */
+ E_defo = LyMass(Z1,A1,rbeta) - LyMass(Z1,A1,0.0);
+ Edefo[2][1][i] = E_defo; /* "light" fragment */
+ }
+
+ for(int i = 10;i<=(I_Z_CN - 10);i++)
+ {
+ rbeta = 0;
+ Beta[2][2][i] = rbeta;
+ Edefo[2][2][i] = 0; /* "heavy" fragment (at S1 shell) */
+ }
+ /* Mode 2: deformed shells (light and heavy) */
+ for(int i = 10;i<=(I_Z_CN - 10);i++)
+ {
+ Z1 = Csng(i);
+ Z2 = Csng(I_Z_CN) - Z1;
+ A1 = (Z1 - 0.5) / Csng(I_Z_CN) * Csng(I_A_CN); /* polarization roughly considered */
+ A2 = Csng(I_A_CN) - A1;
+ if(I_Z_CN * 0.5 < ZC_Mode_2)
+ {
+ // Beta_opt_light(A1,A2,Z1,Z2,dneck,beta_heavy(Z2),rbeta_ld)
+ rbeta = beta_light(i,betaL0,betaL1); // general deformation of light fragment
+ if(rbeta < 0)
+ rbeta = 0; // negative values replaced by 0
+ }
+ else
+ rbeta = beta_heavy(i,betaH0,betaH1); // equal to S2 channel
+ Beta[3][1][i] = rbeta;
+ E_defo = LyMass(Z1,A1,rbeta) - LyMass(Z1,A1,0.0);
+ Edefo[3][1][i] = E_defo;
+ }
+ for(int i = 10;i<=(I_Z_CN - 10);i++)
+ {
+ rbeta = beta_heavy(i,betaH0,betaH1); /* "heavy" fragment (at S2 shell)*/
+ if(rbeta < 0)
+ rbeta = 0; // negative values replaced by 0
+ Beta[3][2][i] = rbeta;
+ Z1 = Csng(i);
+ A1 = (Z1 + 0.5) / Csng(I_Z_CN) * Csng(I_A_CN); /* polarization roughly considered */
+ E_defo = LyMass(Z1,A1,rbeta) - LyMass(Z1,A1,0.0);
+ Edefo[3][2][i] = E_defo;
+ }
+ /* Mode 3 */
+ for(int i = 10;i<=(I_Z_CN - 10);i++)
+ {
+ Z1 = Csng(i);
+ Z2 = Csng(I_Z_CN) - Z1;
+ A1 = (Z1 - 0.5) / Csng(I_Z_CN) * Csng(I_A_CN); /* polarization roughly considered */
+ A2 = Csng(I_A_CN) - A1;
+ rbeta = beta_light(i,betaL0,betaL1);
+ rbeta = Max(rbeta-0.10,0.0); /* for low nu-bar of lightest fragments */
+ // Beta_opt_light(A1,A2,Z1,Z2,dneck,beta_heavy(Z2,betaH0,betaH1),rbeta)
+ Beta[4][1][i] = rbeta;
+ E_defo = LyMass(Z1,A1,rbeta) - LyMass(Z1,A1,0.0);
+ Edefo[4][1][i] = E_defo;
+ }
+ for(int i = 10;i<=(I_Z_CN - 10);i++)
+ {
+ rbeta = beta_heavy(i,betaH0,betaH1) + 0.3; // Shift from isotopic distributions of S3 nuclei in 239Pu(nth,f)
+ if(rbeta < 0)
+ rbeta = 0;
+ Beta[4][2][i] = rbeta;
+ Z1 = Csng(i);
+ A1 = (Z1 + 0.5) / Csng(I_Z_CN) * Csng(I_A_CN); /* polarization roughly considered */
+ E_defo = LyMass(Z1,A1,rbeta) - LyMass(Z1,A1,0.0);
+ Edefo[4][2][i] = E_defo;
+ }
+ /* Mode 4: (Channel S4, (fissioning nucleus in the Z=80 region), Zfrag around 38 */
+ for(int i = 10;i<=(I_Z_CN - 10);i++) // heavy fragment
+ {
+ Z1 = Csng(i);
+ A1 = Z1 / Csng(I_Z_CN) * Csng(I_A_CN); /* charge polarization neglected */
+ rbeta = Beta[3][1][i]; // Deformation like the light fragment of S2 in the actinides
+ if(rbeta < 0)
+ rbeta = 0;
+ Beta[5][1][i] = rbeta;
+ Beta[5][2][i] = rbeta;
+ E_defo = LyMass(Z1,A1,rbeta) - LyMass(Z1,A1,0.0);
+ Edefo[5][1][i] = E_defo; /* light fragment */
+ Edefo[5][2][i] = E_defo; /* heavy fragment */
+ }
+ /* Mode 5: (Channel ST1 in both fragments) */
+ for(int i = 10; i<=(I_Z_CN - 10);i++)
+ {
+ Z1 = Csng(i);
+ Z2 = Csng(I_Z_CN) - Z1;
+ rbeta = Beta[2][2][i];
+ if(rbeta < 0)
+ rbeta = 0;
+ Beta[6][1][int(Z1)] = rbeta;
+ Beta[6][2][int(Z1)] = rbeta;
+ }
+
+ /* Mode 6: (Channel ST2 in both fragments) */
+ for(int i=10;i<=(I_Z_CN - 10);i++)
+ {
+ Z1 = Csng(i);
+ Z2 = Csng(I_Z_CN) - Z1;
+ rbeta = Beta[3][2][i];
+ if(rbeta < 0)
+ rbeta = 0;
+ Beta[7][1][int(Z1)] = rbeta;
+ Beta[7][2][int(Z1)] = rbeta;
+ }
+}
+
+void GEF::MeanZ_asA(void)
+{
+ /* Mean Z as a function of mass */
+ /* Mode 0 */
+ for(int I = 10;I<=(I_A_CN - 10);I++)
+ {
+ ZUCD = Csng(I) / Csng(I_A_CN) * Csng(I_Z_CN);
+ beta1 = Beta[1][1][int(ZUCD + 0.5)];
+ beta2 = Beta[1][2][int(I_Z_CN - ZUCD + 0.5)];
+ Z1 = Z_equi(I_Z_CN,I, I_A_CN - I, beta1, beta2, DNECK,0);
+ Zmean[0][1][I] = Z1;
+ Zshift[0][1][I] = Z1 - ZUCD;
+ Zmean[0][2][I_A_CN - I] = I_Z_CN - Z1;
+ Zshift[0][2][I_A_CN - I] = ZUCD - Z1;
+ ZshiftOriginal[0][1][I]=Zshift[0][1][I];
+ ZshiftOriginal[0][2][I_A_CN - I]=Zshift[0][2][I_A_CN - I];
+ }
+ /* Mode 1 */
+ for(int I = 10;I<=(I_A_CN - 10);I++)
+ {
+ ZUCD = Csng(I) / Csng(I_A_CN) * Csng(I_Z_CN);
+ Z = ZUCD + ZPOL1; /* Charge polarisation is considered in a crude way */
+ beta1 = Beta[2][1][CInt(Z)]; /* "light" fragment */
+ Z = ZUCD - ZPOL1;
+ beta2 = Beta[2][2][CInt(I_Z_CN-Z)]; /* "heavy" fragment at S1 shell */
+ if(Csng(I_Z_CN) * 0.5 < ZC_Mode_1)
+ {
+ Z1 = Z_equi(I_Z_CN,I, I_A_CN - I, beta1, beta2, DNECK,1);
+ Z1 = Z1 + POLARadd;
+ }
+ else
+ Z1 = Z_equi(I_Z_CN,I, I_A_CN - I, beta1, beta2, DNECK,1);
+ Z1 = Z1 + ZPOL1; /* Charge polarization by shell */
+ if((I_Z_CN - Z1) < 50. && (Csng(I_Z_CN) - Z1) > Z1)
+ Z1 = Csng(I_Z_CN) - 50.; /* Z of mean heavy fragment not below 50 */
+ Zmean[1][1][I] = Z1;
+ Zshift[1][1][I] = Z1 - ZUCD; // neutron-deficient
+ Zmean[1][2][I_A_CN - I] = Csng(I_Z_CN) - Z1;
+ Zshift[1][2][I_A_CN - I] = ZUCD - Z1; // neutron rich at shell
+ ZshiftOriginal[1][1][I]=Zshift[1][1][I];
+ ZshiftOriginal[1][2][I_A_CN - I]=Zshift[1][2][I_A_CN - I];
+ }
+ /* Mode 2 */
+ for(int I = 10;I<=(I_A_CN - 10);I++)
+ {
+ ZUCD = Csng(I) / Csng(I_A_CN) * Csng(I_Z_CN);
+ Z = ZUCD; /* Charge polarisation is here neglected */
+ beta1 = Beta[3][1][CInt(Z)];
+ beta2 = Beta[3][2][CInt(I_Z_CN-Z)];
+ if(Csng(I_Z_CN) * 0.5 < ZC_Mode_2)
+ {
+ Z1 = Z_equi(I_Z_CN,I, I_A_CN-I, beta1, beta2, DNECK,2);
+ Z1 = Z1 + POLARadd;
+ // Polarization caused by N=50 shell (assumption)
+ Z1 = Z1 - 0.55 * Bell(Csng(I)-Z1,45,49.5);
+ }
+ else
+ Z1 = Z_equi(I_Z_CN,I, I_A_CN-I, beta1, beta2, DNECK,2);
+ Zmean[2][1][I] = Z1;
+ Zshift[2][1][I] = Z1 - ZUCD; // neutron deficient
+ Zmean[2][2][I_A_CN - I] = Csng(I_Z_CN) - Z1;
+ Zshift[2][2][I_A_CN - I] = ZUCD - Z1; // neutron rich at shell
+ ZshiftOriginal[2][1][I]=Zshift[2][1][I];
+ ZshiftOriginal[2][2][I_A_CN - I]=Zshift[2][2][I_A_CN - I];
+ }
+ /* Mode 3 */
+ for(int I = 10;I<=(I_A_CN - 10);I++)
+ {
+ ZUCD = Csng(I) / Csng(I_A_CN) * Csng(I_Z_CN);
+ Z = ZUCD; /* Charge polarisation is here neglected */
+ beta1 = Beta[4][1][CInt(Z)];
+ beta2 = Beta[4][2][I_Z_CN-CInt(Z)];
+ Z1 = Z_equi(I_Z_CN,I, I_A_CN - I, beta1, beta2, DNECK,3);
+ Z1 = Z1 + POLARadd;
+ // Polarization caused by N=50 shell (assumption)
+ Z1 = Z1 - 0.55 * Bell(Csng(I)-Z1,45,49.5);
+ // POLARadd+0.15,POLARfac) // Stronger charge polarization in S3, heavy fragment //!!! KHS
+ // POLARadd+0.4,POLARfac) // Stronger charge polarization in S3, heavy fragment
+ Zmean[3][1][I] = Z1;
+ Zshift[3][1][I] = Z1 - ZUCD;
+ Zmean[3][2][I_A_CN - I] = Csng(I_Z_CN) - Z1;
+ Zshift[3][2][I_A_CN - I] = ZUCD - Z1;
+ ZshiftOriginal[3][1][I]=Zshift[3][1][I];
+ ZshiftOriginal[3][2][I_A_CN - I]=Zshift[3][2][I_A_CN - I];
+ }
+ /* Mode 4 (Charge polarization of heavy fragment assumed to be equal to light fragment in S2 in the actinides) */
+ for(int I = 10;I<=(I_A_CN - 10);I++) // Loop is over the "second" (heavy) fragment!
+ {
+ ZUCD = Csng(I) / Csng(I_A_CN) * Csng(I_Z_CN);
+ Z = ZUCD; /* Charge polarisation is here neglected */
+ beta1 = Beta[5][1][CInt(I_Z_CN-Z)]; // light fragment
+ beta2 = Beta[5][2][CInt(Z)]; // heavy fragment
+ Z2 = Z_equi(I_Z_CN,I, I_A_CN-I, beta2, beta1, DNECK,4);
+ Z2 = Z2 + POLARadd;
+ // Polarization caused by N=50 shell (assumption)
+ // Z2 = Z2 - 0.55 * Bell(Csng(I)-Z1,45,49.5)
+ Zmean[4][2][I] = Z2;
+ //Print "Z2UCD,Z2",ZUCD,Z2-POLARadd,Z2
+ Zshift[4][2][I] = Z2 - ZUCD; // neutron deficient
+ Zmean[4][1][I_A_CN - I] = Csng(I_Z_CN) - Z2;
+ Zshift[4][1][I_A_CN - I] = ZUCD - Z2; // neutron rich at shell
+ ZshiftOriginal[4][2][I]=Zshift[4][2][I];
+ ZshiftOriginal[4][1][I_A_CN - I]=Zshift[4][1][I_A_CN - I];
+ }
+}
+
+void GEF::RelationsZ_A_FM(void)
+{
+ // Mode 0
+ RZpol = 0;
+ for(int I = 1;I<= 3;I++)
+ {
+ RA = (ZC_Mode_0 - RZpol) * Csng(I_A_CN) / Csng(I_Z_CN);
+ RZpol = Zshift[0][2][CInt(RA)]; // heavy fragment
+ }
+ AC_Mode_0 = (ZC_Mode_0 - RZpol) * Csng(I_A_CN) / Csng(I_Z_CN); /// mean position in mass ///
+ NC_Mode_0 = AC_Mode_0 - ZC_Mode_0;
+ // Mode 1
+ RZpol = 0;
+ for(int I = 1;I<= 3;I++)
+ {
+ RA = (ZC_Mode_1 - RZpol) * Csng(I_A_CN) / Csng(I_Z_CN);
+ RZpol = Zshift[1][2][CInt(RA)]; // heavy fragment
+ }
+ AC_Mode_1 = (ZC_Mode_1 - RZpol) * Csng(I_A_CN) / Csng(I_Z_CN);
+ NC_Mode_1 = AC_Mode_1 - ZC_Mode_1;
+ // Mode 2
+ RZpol = 0;
+ for(int I = 1;I<= 3;I++)
+ {
+ RA = (ZC_Mode_2 - RZpol) * Csng(I_A_CN) / Csng(I_Z_CN);
+ RZpol = Zshift[2][2][CInt(RA)]; // heavy fragment
+ }
+ AC_Mode_2 = (ZC_Mode_2 - RZpol) * Csng(I_A_CN) / Csng(I_Z_CN);
+ NC_Mode_2 = AC_Mode_2 - ZC_Mode_2;
+ // Mode 3
+ RZpol = 0;
+ for(int I = 1;I<= 3;I++)
+ {
+ RA = (ZC_Mode_3 - RZpol) * Csng(I_A_CN) / Csng(I_Z_CN);
+ RZpol = Zshift[3][2][CInt(RA)]; // heavy fragment
+ }
+ AC_Mode_3 = (ZC_Mode_3 - RZpol) * Csng(I_A_CN) / Csng(I_Z_CN);
+ NC_Mode_3 = AC_Mode_3 - ZC_Mode_3;
+ // Mode 4
+ RZpol = 0;
+ for(int I = 1;I<= 3;I++)
+ {
+ RA = (ZC_Mode_4 - RZpol) * Csng(I_A_CN) / Csng(I_Z_CN);
+ RZpol = Zshift[4][1][CInt(RA)]; // light fragment
+ }
+ AC_Mode_4 = (ZC_Mode_4 - RZpol) * Csng(I_A_CN) / Csng(I_Z_CN); // light fragment
+ NC_Mode_4 = AC_Mode_4 - ZC_Mode_4; // light fragment
+}
+
+void GEF::FissionBarriers(void)
+{
+ /* Fission barriers -> global parameters */
+ B_F = BFTF(Csng(I_Z_CN),Csng(I_A_CN),1);
+ B_F_ld = BFTF(Csng(I_Z_CN),Csng(I_A_CN),0);
+ E_B = BFTFB(Csng(I_Z_CN),Csng(I_A_CN),1);
+ E_B_ld = BFTFB(Csng(I_Z_CN),Csng(I_A_CN),0);
+}
+
+void GEF::PolarizationStiffness(void)
+{
+ RZ = Csng(I_Z_CN) * 0.5;
+ RA = Csng(I_A_CN) * 0.5;
+ beta1 = Beta[1][1][CInt(RZ)];
+ beta2 = Beta[1][2][CInt(RZ)];
+ R_Pol_Curv_S0 = ( LyMass( RZ - 1.E0, RA, beta1 ) + LyMass( RZ + 1.0E0, RA, beta2 ) +
+ LyMass( RZ + 1.0E0, RA, beta1 ) + LyMass( RZ - 1.0E0, RA, beta2 ) +
+ ECOUL( RZ - 1.0E0, RA, beta1, RZ + 1.0E0, RA, beta2, DNECK) +
+ ECOUL( RZ + 1.0E0, RA, beta1,RZ - 1.0E0, RA, beta2, DNECK) -
+ 2.0E0*ECOUL( RZ, RA, beta1, RZ, RA, beta2, DNECK) -
+ 2.0E0*LyMass( RZ, RA, beta1 ) - 2.0E0*LyMass( RZ, RA, beta2) ) * 0.5;
+
+ P_POL_CURV_S0= R_Pol_Curv_S0;
+
+ // Assumption: stiffenss is dominated (and thus well represented) by the macroscopic potential
+ R_Pol_Curv_S1 = R_Pol_Curv_S0;
+ R_Pol_Curv_S2 = R_Pol_Curv_S0;
+ R_Pol_Curv_S3 = R_Pol_Curv_S0;
+ R_Pol_Curv_S4 = R_Pol_Curv_S0;
+}
+
+
+
+
+
+
+
+
+
+float GEF::Getyield(float E_rel,float E_ref, float T_low, float T_high)
+{
+ // Erel: Energy relative to the barrier
+ // T_low: Effective temperature below barrier
+ // T_high: Effective temperature above barrier/
+ float Exp1;
+ float Yield;
+
+ Exp1 = E_rel/T_low - E_ref/0.4; //energy far below barrier // Subtraction of E_ref/0.4 to prevent numerical problems.
+ if(Exp1<-50)
+ Yield = 0.;
+ else
+ Yield = exp(E_rel / T_high - E_ref/0.4) * 1. / (1. + exp(-E_rel/ (T_high*T_low/(T_high-T_low))));
+
+ return Max(Yield,0.0);
+}
+
+float GEF::F1(float Z_S_A)
+{
+ // Fit to the lower part of the data
+ float Result;
+ Result = exp(-9.05 + 4.58 *log(Z_S_A/2.3));
+ return Result;
+}
+
+float GEF::F2(float Z_S_A)
+{
+ // Fit to the upper part of the data
+ float Result;
+ Result = exp(12.08 - 3.27 * log(Z_S_A/2.3));
+ return Result;
+}
+
+float GEF::Masscurv(float Z, float A, float RL, float kappa)
+{
+ // Fit to Data of Fig. 7 of
+ // "Shell effect in the symmetric-modal fission of pre-actinide nuclei"
+ // S. I. Mulgin, K.-H. Schmidt, A. Grewe, S. V. Zhdanov
+ // Nucl. Phys. A 640 (1998) 375 (From fit of the width of the mass distributions.)
+ float RI, Result1, Result2, Result;
+ float Z_square_over_A;
+ float ZsqrA;
+ float c_rot = 600.0;
+
+ Z_square_over_A = Z*Z/A;
+ RI = (A - 2*Z)/A;
+ ZsqrA = Z_square_over_A * (1. - kappa * pow(RI,2)) /(1. - kappa * pow((226. - 2.*91.)/226.,2)) + c_rot * pow(RL,2) / pow(A,7.0/3.0);// Hasse & Myers
+ Result1 = F1(ZsqrA);
+ Result2 = F2(ZsqrA);
+ Result = Min(Result1,Result2);
+ return Result;
+}
+
+float GEF::Masscurv1(float Z, float A, float RL, float kappa)
+{
+ // Fit to Data of Fig. 7 of
+ // "Shell effect in the symmetric-modal fission of pre-actinide nuclei"
+ // S. I. Mulgin, K.-H. Schmidt, A. Grewe, S. V. Zhdanov
+ // Nucl. Phys. A 640 (1998) 375 (The left part assumed to be valid for the yields of the fission channels.)
+ float RI,Result1, Result2, Result ;
+ float Z_square_over_A;
+ float ZsqrA;
+ float c_rot = 600.0;
+
+ Z_square_over_A = Z*Z/A;
+ RI = (A - 2*Z)/A;
+ ZsqrA = Z_square_over_A * (1. - kappa * pow(RI,2)) / (1. - kappa * pow((226. - 2.*91.)/226.,2))+ c_rot * pow(RL,2) / pow(A,7.0/3.0); // Hasse & Myers
+
+ if(ZsqrA < 36.0) // adjusted to Y(S2) in light nuclei (80<Z<92)
+ ZsqrA = ZsqrA + 0.9 * (36.0 - ZsqrA) ;
+ Result1 = F1(ZsqrA);
+ Result2 = F2(ZsqrA);
+
+ return Result1;
+}
+
+float GEF::De_Saddle_Scission(float Z_square_over_Athird,float ESHIFTSASCI)
+{
+ // Energy release between saddle and scission
+ // M. Asghar, R. W. Hasse, J. Physique C 6 (1984) 455
+ float Result;
+ Result = (31. - 11.) / (1550. - 1300.) * (Z_square_over_Athird - 1300. + ESHIFTSASCI) + 11.;
+ // This formula with ESHIFTSASCI = 0 is the parameterisation of the results
+ // of Ashgar and Hasse, JPC 6 (1984) 455, see
+ // F. Rejmund, A. V. Ignatyuk, A. R. Junghans, K.-H. Schmidt
+ // Nucl. Phys. A 678 (2000) 215
+ Result = Max(Result,0.0);
+ return Result;
+}
+
+float GEF::TEgidy(float A,float DU, float Fred)
+{
+ // Temperature parameter of the constant-temperature formula for the nuclear level density.
+ // Input parameters: A = Mass number of nucleus, DU = Shell effect (corrected for pairing:P=0 for odd-A nuclei)
+ // From "Correlations between the nuclear level density parameters"
+ // Dorel Bucurescu, Till von Egidy
+ // Phys. Rev. C 72 (2005) 067304 and
+ // "Systematics of nuclear level density parameters"
+ // Dorel Bucurescu, Till von Egidy
+ // J. Phys. G: Nucl. Part. Phys. 31 (2005) S1675 and
+ // "Systematics of nuclear level density parameters"
+ // Till von Egidy, Dorel Bucurescu
+ // Phys. Rev. C 72 (2005) 044311
+ float Temp_smooth,Temp,T_Fac;
+ Temp_smooth = 1.0 / (0.0570 * pow(A,0.6666667));
+ Temp = 1.0 / ( (0.0570 + 0.00193*DU) * pow(A,0.6666667)); // from PRC 80 (2009) 054310
+ T_Fac = Temp / Temp_smooth;
+ Temp = Temp * Fred; // (For influence of deformation)
+ return Temp;
+}
+
+float GEF::TRusanov(float E, float A)
+{
+ // Fermi-gas level density, parameterisation of Rusanov et al.
+ return sqrt(E / (0.094 * A) );
+}
+
+float GEF::LyMass(float Z, float A, float beta)
+{
+ // liquid-drop mass, Myers & Swiatecki, Lysekil, 1967
+ // pure liquid drop, without pairing and shell effects
+ // On input: Z nuclear charge of nucleus
+ // N number of neutrons in nucleus
+ // beta deformation of nucleus
+ // On output: binding energy of nucleus
+
+ float N;
+ float alpha;
+ float XCOM,XVS,XE,EL;
+
+ N = A - Z;
+ alpha = sqrt(5./(4.*pi)) * beta;
+ XCOM = 1. - 1.7826 * pow((A - 2.*Z)/A,2);
+ // factor for asymmetry dependence of surface and volume term
+ XVS = - XCOM * (15.4941*A - 17.9439*pow(A,2./3.)*(1.+0.4*pow(alpha,2)));
+ // sum of volume and surface energy
+ XE = Z*Z * (0.7053/pow(A,1./3.)*(1.-0.2*pow(alpha,2))- 1.1529/A);
+ EL = XVS + XE;
+ // EL = EL + LyPair(Z,A);
+ return EL;
+}
+
+float GEF::LyPair(int Z, int A)
+{
+ // Calculates pairing energy
+ // odd-odd nucleus: Lypair = 0
+ // even-odd nucleus: Lypair = -12/sqr(A)
+ // even-even nucleus: Lypair = -2*12/sqr(A)
+ float E_PAIR;
+ E_PAIR = - 12. / sqrt(Csng(A)) * Csng( ( (Z+1)%2 + (A-Z+1)%2) );
+ return E_PAIR;
+}
+
+float GEF::TFPair(int Z, int A)
+{
+ // Pairing energy from Thomas-Fermi model of Myers and Swiatecki
+ // Shifted that TFPair is zero for odd-odd nuclei
+ int N;
+ float E_Pair;
+ N = A - Z;
+ if(Z%2==0 && N%2 == 0)// even-even
+ E_Pair = - 4.8 / pow(Z,0.333333) - 4.8 / pow(N,0.333333) + 6.6 / pow(A,0.666666);
+ if(Z%2==0 && N%2 == 1) // even Z, odd N
+ E_Pair = - 4.8 / pow(Z,0.333333) + 6.6 / pow(A,0.666666);
+ if(Z%2==1 && N%2 == 0) // odd Z, even N
+ E_Pair = - 4.8 / pow(N,0.333333) + 6.6 / pow(A,0.666666);
+ if(Z%2==1 && N%2 == 1) // odd N, odd N
+ E_Pair = 0.0;
+
+ return E_Pair;
+}
+
+float GEF::Pmass(float Z, float A, float beta)
+{
+ // Liquid-drop model of Pearson, 2001
+ float N,EA,BE;
+ float avol = -15.65;
+ float asf = 17.63;
+ float r0 = 1.233;
+ float asym = 27.72;
+ float ass = -25.60;
+ float alpha;
+ N = A - Z;
+ alpha = sqrt(5./(4.*pi)) * beta;
+ EA = avol + asf * pow(A,-0.333333)*(1.+0.4*pow(alpha,2)) + 0.6 * 1.44 * Z*Z / (pow(A,1.333333) * r0 )*(1.-0.2*pow(alpha,2)) + (asym + ass * pow(A,2-0.333333)) * pow(N-Z,2) / pow(A,2);
+ BE = EA * A;
+ return BE;
+}
+
+float GEF::FEDEFOP(float Z, float A, float beta)
+{
+ // According to liquid-drop model of Pearson 2001
+ float asf = 17.63;
+ float r0 = 1.233;
+ float N,Alpha;
+ N = A - Z;
+ Alpha = sqrt(5./(4.*pi)) * beta;
+ return asf * pow(A,0.666667)*(0.4*pow(Alpha,2)) - 0.6 * 1.44 * Z*Z / (pow(A,0.333333) * r0 )*(0.2*pow(Alpha,2));
+}
+
+float GEF::FEDEFOLys(float Z, float A, float beta)
+{
+ return LyMass(Z,A,beta) - LyMass(Z,A,0.0);
+}
+
+float GEF::LDMass(float Z, float A, float beta)
+{
+ float N,BEtab;
+ N = A - Z;
+ BEtab = BEldmTF[CInt(N)][CInt(Z)] + 2.0 * 12.0 / sqrt(Csng(A)) - 0.00001433*pow(Z,2.39);
+ // The values in BEtab are the negative binding energies!
+ // Pairing in Thomas Fermi masses is zero for Z,N even !
+ if(BEtab == 0.0)
+ {
+ BEtab = LyMass(Z,A,0.0);
+ cout<< "Warning: Binding energy of Z="<<Z<<", A="<<A<<" not in mass table, replaced by LYMASS"<<endl;
+ cout<< "I_Mode = "<<I_Mode<<endl;
+ }
+ return BEtab + FEDEFOLys(Z,A,beta);
+}
+
+float GEF::AME2012(int IZ, int IA)
+{
+ // Masses from the 2003 mass evaluation, complemented by TF masses
+ // and Lysekil masses.
+ float BEexpval;
+ float Z,A,N;
+ int INeu;
+ INeu = IA - IZ;
+ A = Csng(IA);
+ Z = Csng(IZ);
+ N = A - Z;
+ BEexpval = BEexp[INeu][IZ];
+ if(BEexpval > -1.e10)
+ return BEexpval;
+ else
+ return LDMass(Z,A,0.0) + U_SHELL(IZ,IA) + LyPair(IZ,IA);
+}
+
+float GEF::U_SHELL(int Z, int A)
+{
+ int N;
+ float Res;
+ N = A - Z;
+ Res = ShellMO[N][Z];
+ if(Res>0.0)
+ Res = 0.3 * Res; // KHS (12. Feb. 2012)
+ // The positive shell effects for deformed nuclei seem to be too positive
+ // This gives too many high-energetic prompt neutrons.
+ return Res;
+}
+
+float GEF::U_SHELL_exp(int IZ, int IA)
+{
+ float Res;
+ float Z,A;
+ Z = Csng(IZ);
+ A = Csng(IA);
+ // Res = 2.0 * ( AME2012(IZ,IA) - Lypair(IZ,IA) - LDMass(Z,A,0.0) )
+ // - 0.25 * ( AME2012(IZ,IA-1) - Lypair(IZ,IA-1) - LDMass(Z,A-1.0,0.0) )
+ // - 0.25 * ( AME2012(IZ,IA+1) - Lypair(IZ,IA+1) - LDMass(Z,A+1.0,0.0) )
+ // - 0.25 * ( AME2012(IZ+1,IA+1) - Lypair(IZ+1,IA+1) - LDMass(Z+1.0,A+1.0,0.0) )
+ // - 0.25 * ( AME2012(IZ-1,IA-1) - Lypair(IZ-1,IA-1) - LDMass(Z-1.0,A-1.0,0.0) )
+ Res = 0.5 * ( AME2012(IZ,IA) - LyPair(IZ,IA) - LDMass(Z,A,0.0) )
+ + 0.125 * ( AME2012(IZ,IA-1) - LyPair(IZ,IA-1) - LDMass(Z,A-1.0,0.0) )
+ + 0.125 * ( AME2012(IZ,IA+1) - LyPair(IZ,IA+1) - LDMass(Z,A+1.0,0.0) )
+ + 0.125 * ( AME2012(IZ+1,IA+1) - LyPair(IZ+1,IA+1) - LDMass(Z+1.0,A+1.0,0.0) )
+ + 0.125 * ( AME2012(IZ-1,IA-1) - LyPair(IZ-1,IA-1) - LDMass(Z-1.0,A-1.0,0.0) );
+ return Res;
+}
+
+float GEF::U_SHELL_EO_exp(int IZ, int IA)
+{
+ // Returns experimental shell and even-odd staggering,
+ // just the difference of experimental and macroscopic mass.
+ float Res;
+ float Z,A;
+ Z = Csng(IZ);
+ A = Csng(IA);
+ Res = AME2012(IZ,IA) - LDMass(Z,A,0.0);
+ return Res;
+}
+
+float GEF::U_MASS(float Z, float A)
+{
+ // LD + congruence energy + shell (no pairing)
+ float BE;
+ if((Z<0) |(A<0))
+ cout<<"U_Mass: Z, A: "<<Z<<" "<<A<<endl;
+
+ BE = LDMass(Z,A,0.0) + U_SHELL(CInt(Z),CInt(A));
+ // BE = AME2012(Cint(Z),Cint(A)) - Lypair(Z,A)
+ // BE = Lymass(Z,A,0.0) + U_Shell(CInt(Z),CInt(A))
+ // BE = Lymass(Z,A,0.0)
+ return BE;
+}
+
+float GEF::ECOUL(float Z1, float A1, float beta1, float Z2, float A2, float beta2, float d)
+{
+ // Coulomb potential between two nuclei
+ // surfaces are in a distance of d
+ // in a tip to tip configuration
+ // approximate formulation
+ // On input: Z1 nuclear charge of first nucleus
+ // A1 mass number of irst nucleus
+ // beta1 deformation of first nucleus
+ // Z2 nuclear charge of second nucleus
+ // A2 mass number of second nucleus
+ // beta2 deformation of second nucleus
+ // d distance of surfaces of the nuclei
+
+ float N1,N2,REcoul;
+ float dtot;
+ float r0 = 1.16;
+
+ N1 = A1 - Z1;
+ N2 = A2 - Z2;
+ dtot = r0 *( pow(Z1+N1,0.3333333) * (1.+0.6666667*beta1)
+ + pow(Z2+N2,0.3333333) * (1.+0.6666667*beta2) ) + d;
+ REcoul = Z1 * Z2 * 1.44 / dtot;
+ return REcoul;
+}
+
+float GEF::beta_light(int Z, float betaL0, float betaL1)
+{
+ // Deformation of light fission fragment for S1 and S2
+ // Systematic correlation Z vs. beta for deformed shells
+ // Z of fission fragment
+ float beta;
+ beta = (Z - betaL0) * betaL1/20.;
+ return beta;
+}
+
+float GEF::beta_heavy(int Z, float betaH0, float betaH1)
+{
+ // Deformation of heavy fission fragment for S2
+ // Systematic correlation Z vs. beta for deformed shells
+ // Z of fission fragment
+ float beta;
+ beta = (Z - betaH0) * betaH1/20.;
+ return beta;
+}
+
+float GEF::Z_equi(int ZCN, int A1, int A2, float beta1, float beta2, float d, int Imode)
+{
+ // Determines the minimum potential of the scission-point configuration
+ // represented by two deformed nuclei divided by a tip distance d.
+ // A1, A2, beta1, beta2, d are fixed, Z1 is searched for and returned on output.
+ // ZCN: Z of fissioning nucleus
+ // A1: A of first fission fragment
+ // A2: A of second fission fragment
+ // beta1: deformation of first fission fragment
+ // beta2: deformation of second fission fragment
+ // d: tip distance
+
+ float RZ_equi;
+ float RA1,RA2,RZCN,RACN;
+ float Z1UCD,Z2UCD;
+ float re1,re2,re3,eps1,eps2,DZ_Pol; // help variables
+ RA1 = Csng(A1);
+ RA2 = Csng(A2);
+ RZCN = Csng(ZCN);
+ RACN = RA1 + RA2;
+ Z1UCD = RA1 / (RA1 + RA2) * RZCN;
+ Z2UCD = RZCN - Z1UCD;
+ re1 = LyMass( Z1UCD-1., RA1, beta1 ) +
+ LyMass( Z2UCD+1., RA2, beta2 ) +
+ ECOUL( Z1UCD-1., RA1, beta1, Z2UCD+1., RA2, beta2, d );
+ re2 = LyMass( Z1UCD, RA1, beta1) +
+ LyMass( Z2UCD, RA2, beta2) +
+ ECOUL( Z1UCD, RA1, beta1, Z2UCD, RA2, beta2, d );
+ re3 = LyMass( Z1UCD+1., RA1, beta1 ) +
+ LyMass( Z2UCD-1., RA2, beta2 ) +
+ ECOUL( Z1UCD+1., RA1, beta1, Z2UCD-1., RA2, beta2, d );
+ eps2 = ( re1 - 2.*re2 + re3 ) / 2.;
+ eps1 = ( re3 - re1 ) / 2.;
+ DZ_Pol = -eps1 / ( 2. * eps2 );
+ if((DZ_Pol>2) | (DZ_Pol<-2))
+ DZ_Pol = 0.;
+ RZ_equi = Z1UCD + DZ_Pol;
+ return RZ_equi;
+}
+
+void GEF::Beta_opt_light(float A1, float A2, float Z1, float Z2, float d, float beta2_imposed, float &beta1_opt)
+{
+ /// Determines the optimum deformation of the light fragment when the deformation of the heavy fragment is imposed.
+ float beta1,dbeta1,beta1_prev,beta1_next;
+ float Uguess,Uplus,Uminus,Uprev,Unext;
+ int I;
+ beta1 = 0.5;
+ dbeta1 = 0.01;
+ Uguess = LyMass(Z1, A1, beta1) +
+ LyMass(Z2, A2, beta2_imposed) +
+ ECOUL(Z1, A1, beta1, Z2, A2, beta2_imposed, d);
+ Uplus = LyMass(Z1, A1, beta1 + dbeta1) +
+ LyMass(Z2, A2, beta2_imposed) +
+ ECOUL(Z1, A1, beta1 + dbeta1, Z2, A2, beta2_imposed, d);
+ Uminus = LyMass(Z1, A1, beta1 - dbeta1) +
+ LyMass(Z2, A2, beta2_imposed) +
+ ECOUL(Z1, A1, beta1 - dbeta1, Z2, A2, beta2_imposed, d);
+ if(Uplus>Uguess && Uminus>Uguess)
+ beta1_opt = beta1;
+ else
+ {
+ if(Uplus < Uguess)
+ dbeta1 = 0.01;
+ if(Uminus < Uguess)
+ dbeta1 = -0.01;
+ Unext = Uguess;
+ beta1_next = beta1;
+ for(int i=1;i<=10000;i++)
+ {
+ beta1_prev = beta1_next;
+ Uprev = Unext;
+ beta1_next = beta1_prev + dbeta1;
+ Unext = LyMass(Z1, A1, beta1_next) +
+ LyMass(Z2, A2, beta2_imposed) +
+ ECOUL(Z1, A1, beta1_next, Z2, A2, beta2_imposed, d);
+ if(Unext>=Uprev)
+ break;
+ if(i==1000)
+ cout<< "Loop overflow in Beta_opt_light"<<endl;
+ }
+ beta1_opt = beta1_prev;
+ }
+}
+
+void GEF::Beta_Equi(float A1, float A2, float Z1, float Z2, float d, float beta1prev, float beta2prev, float &beta1opt, float &beta2opt)
+{
+ // Determines the minimum potential of the scission-point configuration
+ // represented by two deformed nuclei, divided by a tip distance d.
+ // A1, A2, Z1, Z2, d are fixed, beta1 and beta2 are searched for and returned on output
+
+ int B_analytical = 0;
+ // Switch to use the analytical approximation
+ // that replaces the long numerical calculation.
+ float x,y,xcoul;
+ float xcoul236U = 1369.64;
+ float beta1,beta2;
+ float U,Uprev,Ulast,Ubest,Uopt;
+ float sbeta1 = 0;
+ float sbeta2 = 0;
+ int N,N1,N2;
+ int Nopt = 0;
+ float eps = 5.e-4;
+
+ if(B_analytical == 0) // Numerical algorithm
+ {
+ beta1 = beta1prev;
+ beta2 = beta2prev;
+ Uprev = LyMass(Z1,A1,beta1) + LyMass(Z2,A2,beta2) + ECOUL(Z1,A1,beta1,Z2,A2,beta2,d);
+ Uopt = Uprev;
+
+ // Test slope of variation of U
+ beta1 = beta1prev + eps;
+
+ U = 1.e30;
+ beta2 = beta2prev;
+ for(int i=1;i<=CInt(beta2prev/eps);i++)
+ {
+ beta2 = beta2 - eps;
+ Ulast = U;
+ U = LyMass(Z1,A1,beta1) + LyMass(Z2,A2,beta2) + ECOUL(Z1,A1,beta1,Z2,A2,beta2,d);
+ if(U>Ulast)
+ break;
+ else
+ Ubest = U;
+ }
+ if(Ubest < Uopt)
+ {
+ Uopt = Ubest;
+ sbeta1 = eps;
+ sbeta2 = -eps;
+ }
+
+ U = 1.e30;
+ beta2 = beta2prev;
+ for(int i=1;i<=CInt((1 - beta2prev)/eps);i++)
+ {
+ beta2 = beta2 + eps;
+ Ulast = U;
+ U = LyMass(Z1,A1,beta1) + LyMass(Z2,A2,beta2) + ECOUL(Z1,A1,beta1,Z2,A2,beta2,d);
+ if(U > Ulast)
+ break;
+ else
+ Ubest = U;
+ }
+ if(Ubest < Uopt)
+ {
+ Uopt = Ubest;
+ sbeta1 = eps;
+ sbeta2 = eps;
+ }
+
+ beta1 = beta1prev - eps;
+ U = 1.e30;
+ beta2 = beta2prev;
+ for(int i=1;i<=CInt(beta2prev/eps);i++)
+ {
+ beta2 = beta2 - eps;
+ Ulast = U;
+ U = LyMass(Z1,A1,beta1) + LyMass(Z2,A2,beta2) + ECOUL(Z1,A1,beta1,Z2,A2,beta2,d);
+ if(U > Ulast)
+ break;
+ else
+ Ubest = U;
+ }
+ if(Ubest < Uopt)
+ {
+ Uopt = Ubest;
+ sbeta1 = -eps;
+ sbeta2 = -eps;
+ }
+
+ U = 1.e30;
+ beta2 = beta2prev;
+ for(int i=1;i<=CInt((1-beta2prev)/eps);i++)
+ {
+ beta2 = beta2 + eps;
+ Ulast = U;
+ U = LyMass(Z1,A1,beta1) + LyMass(Z2,A2,beta2) + ECOUL(Z1,A1,beta1,Z2,A2,beta2,d);
+ if(U > Ulast)
+ break;
+ else
+ Ubest = U;
+ }
+ if(Ubest < Uopt)
+ {
+ Uopt = Ubest;
+ sbeta1 = -eps;
+ sbeta2 = eps;
+ }
+
+ Ubest = LyMass(Z1,A1,beta1prev) + LyMass(Z2,A2,beta2prev)
+ + ECOUL(Z1,A1,beta1prev,Z2,A2,beta2prev,d);
+ U = LyMass(Z1,A1,beta1prev+Csng(sbeta1)) +
+ LyMass(Z2,A2,beta2prev+Csng(sbeta2)) +
+ ECOUL(Z1,A1,beta1prev+sbeta1,Z2,A2,beta2prev+Csng(sbeta2),d);
+
+ for(N=1;N<=1000;N++)
+ {
+ for(N1 =1;N1<=N;N1++)
+ {
+ N2 = N-N1;
+ beta1 = beta1prev + sbeta1*N1;
+ beta2 = beta2prev + sbeta2*N2;
+ U = LyMass(Z1,A1,beta1) + LyMass(Z2,A2,beta2) + ECOUL(Z1,A1,beta1,Z2,A2,beta2,d);
+ if(U < Ubest)
+ {
+ Ubest = U;
+ beta1opt = beta1;
+ beta2opt = beta2;
+ Nopt = N;
+ }
+ }
+ if(N-Nopt > 2)
+ break;
+ }
+ if(N>998)
+ cout<<"Beta_Equi not converged: "<<Z1<<" "<<N<<endl;
+ }
+ else // Analytical approximation
+ { // Must be adapted if the relevant parameters of GEF are modified!
+ xcoul = pow(Z1 + Z2,2) / pow(A1 + A2,1.0/3.0);
+ x = pow(Z1 / (Z1 + Z2),xcoul/xcoul236U);
+ y = 1.2512e-4 + 0.00122851*x - 0.00267707*pow(x,2) + 0.00372901*pow(x,3) - 0.00219903*pow(x,4);
+ beta1opt = y * xcoul ;
+ x = pow(Z2 / (Z1 + Z2),xcoul/xcoul236U);
+ y = 1.2512e-4 + 0.00122851*x - 0.00267707*pow(x,2) + 0.00372901*pow(x,3) - 0.00219903*pow(x,4);
+ beta2opt = y * xcoul ;
+ }
+}
+
+void GEF::Eva(int Ilh, float Z_CN, float A_CN, float E_INIT, float T, float J_frag, float &Z_RES, float &A_RES, float &E_FINAL, float *Array_En, float *Array_Tn, float *Array_Eg0)
+{
+ // Z_CN,A_CN,E_init Parameters of initial nucleus
+ // Z_RES,A_RES,E_FINAL after evaporation
+ // T temperature coefficient of level density (not used)
+ // Array_En kinetic energies of neutrons
+ // Array_Tn neutron emission time after scission
+ // Array_Eg0 energies of statistical gammas
+ static float E_MIN = 0; // Final energy for evaporation chain
+ float SN,SNeff,SNmean,SNexp,SNld; // Neutron separation energy
+ float RShell;
+ int ITry,Ifold;
+ float Ai,Af,Zi,Zf,Ni,Nf,Ei,Ef;
+ float bshift,bshiftm;
+ float Tm, Td, Tf, Tmean, TCT;
+ float Gamma_n,Gamma_g,Pgamma;
+ float rho,rhom;
+ float alev;
+ float g_koeff;
+ float E_kin;
+ float Tn,Tn_acc;
+ float J_crit; // critical angular momentum (disappearance of pairing)
+ float J_crit_shell;
+ float Fred; // reduction of pairing gap by ang. momentum
+ float Fred_shell; // reduction of shell
+ int In_gamma; // counts gammas for Array_Eg0()
+ bool B_Expmass = 1; // use mass model or empirical masses
+
+ E_MIN = E_FINAL;
+ In_gamma = 0;
+ Tn_acc = 0 ;
+ Ifold = 1;
+ Ai = A_CN;
+ Zi = Z_CN;
+ Ei = E_INIT;
+ J_crit = 12. * sqrt(Ai/100.0); // L. G. Moretto, Nucl. Phys. A 185 (1972) 145
+ J_crit_shell = 30.;
+
+ if( J_frag >= J_crit)
+ Fred = 0.;
+ else
+ Fred = 0.65 * sqrt(1.0 - J_frag/J_crit); // L. G. Moretto, Nucl. Phys. A 185 (1972) 145
+
+ if(J_frag >= J_crit_shell)
+ Fred_shell = 0.;
+ else
+ Fred_shell = 0.9 - J_frag/J_crit_shell;
+
+ // Shell effects included
+ if(B_Expmass == 0)
+ {
+ SN = U_MASS(Zi,Ai-1.) + Fred * LyPair(Zi,Ai-1.) - (U_MASS(Zi,Ai) + Fred * LyPair(Zi,Ai)) ;
+ SNeff = U_MASS(Zi,Ai-1.) - U_MASS(Zi,Ai) ; // with shells, without pairing
+ // SNmean = 0.5 * (U_MASS(Zi,Ai-2.) - U_MASS(Zi,Ai));
+ }
+ else
+ {
+ SNexp = ( AME2012(Zi,Ai-1) - AME2012(Zi,Ai) ); // empirical
+ SNeff = U_MASS(Zi,Ai-1.) - U_MASS(Zi,Ai); // with shells, without pairing
+ SNld = LDMass(Zi,Ai-1.,0.0) - LDMass(Zi,Ai,0.0); // no shells, no pairing
+ SN = Fred_shell * (Fred * SNexp + (1.0 - Fred) * SNeff) + (1.0 - Fred_shell) * SNld;
+ }
+
+ // Shell effects excluded
+ // SN = LDMass(Zi,Ai-1.,0.0) + LyPair(Zi,Ai-1.) - (LDMass(Zi,Ai,0.0) + LyPair(Zi,Ai)) ;
+ // SNeff = LDMass(Zi,Ai-1.,0.0) - LDMass(Zi,Ai,0.0) ;
+
+ Zf = Zi;
+ Af = Ai;
+ Ef = Ei;
+
+ while(Ei-SN>E_MIN)
+ {
+ // Treat gamma competition
+ Tm = U_Temp(Zi,Ai,Ei,1,1,Tscale,Econd); // emitting nucleus
+ Td = U_Temp(Zi,Ai-1,Ei-SNeff,1,1,Tscale,Econd);
+
+ if(Ilh > 0) // Emission from fragments
+ {
+ Gamma_g = 0.624 * pow(Ai,1.6) * pow(Tm,5); // in meV (Ignatyuk, Bologna)
+ Gamma_g = Gamma_g * 1.e-9; // in MeV
+ }
+ else // Emission between saddle and scission
+ Gamma_g = 0;
+ Tmean = (Tm + Td)/2;
+ // Gamma_n = pow(Ai-1,0.66667) * 0.0302 * pow(Td,2) / exp(SNeff/Tmean) // in MeV (Moretto)
+ Gamma_n = pow(Ai-1,0.66667) * 0.13 * pow(Td,2) / exp(SNeff/Td); // in MeV (Mor. PRC 54,3062)
+ // Cut the distribution at the ground-state energy:
+ Gamma_n = Gamma_n - pow(Ai-1,0.66667) * 0.13 * pow(Td,2) / exp((SNeff+Ei)/Td);
+ Tn = PExp(0.658 / Gamma_n); // in units of 10^-21 s (hbar=0.658zs*MeV)
+ // ? Tn = Tn * 2; // Due to pre-exponential factor of Maxwellian, Tn is about 2 times to large
+ Tn_acc = Tn_acc + Tn;
+ // Influence on lev.dens. of pairing at low E*
+ // (Constant temperature assumed)
+ if(Ei-SN < abs(Fred * LyPair(Zi,Ai-1))) // rest energy below mean g.s. of odd-odd nuclei
+ {
+ if( (Mod(Zi,2) < 0.5) | (Mod(Ai-Zi-1,2) < 0.5)) // even Z or even N
+ Gamma_n = exp(-12./sqrt(Ai)/Td) * Gamma_n;
+ if((Mod(Zi,2) < 0.5) && (Mod(Ai-Zi-1,2) < 0.5)) //n Z and even N
+ // For low level density below pairing gap in even-even nuclei
+ Gamma_n = exp(-12./sqrt(Ai)/Td) * Gamma_n;
+ }
+ // Reduces the even-odd effect in neutron number
+ // due to low level density below the pairing gap
+
+ Pgamma = Gamma_g / (Gamma_g + Gamma_n);
+
+ if(rn->Rndm()<Pgamma) //gamma will be emitted
+ {
+ In_gamma = In_gamma + 1;
+ //Scope //I don't konw what is doing this Scope (Diego)
+ int N;
+ float Eg;
+
+ Eg = P_Egamma_high(Zi,Ai,Ei);
+ Array_Eg0[In_gamma] = Eg;
+ // Accumulate E1 gammas // I comment all this because I don't know what it means, by the moment (Diego)
+ //N = CInt(Eg*1000);
+ //if( N > 0)
+ //{
+ // Ngtot = Ngtot + 1;
+ // if(Ilh == 1)
+ // Nglight = Nglight + 1;
+ // if(Ilh == 2)
+ // Ngheavy = Ngheavy + 1;
+ // Egtot1000 = Egtot1000 + EG*1000;
+ // if( N <= Ubound(Egamma))
+ // {
+ // Egamma(N) = Egamma(N) + 1;
+ // #Ifdef B_EgammaA
+ // StoreEgammaA(N,A_CN);
+ // #Endif
+ //}
+ //}
+ Ei = Ei - Eg;
+ //End Scope
+ }
+
+ if( Ei-SN <= E_MIN)
+ {
+ Zf = Zi;
+ Af = Ai;
+ Ef = Ei;
+ break;
+ }
+
+ ITry = 0;
+ bool Too_Low=true;
+ while (Too_Low)
+ {
+ Too_Low = false;
+ ITry = ITry + 1;
+ if(ITry < 99)
+ {
+ Td = U_Temp(Zi,Ai-1,Ei-SNeff,1,1,Tscale,Econd);
+ // maximum residual energy of daughter nucleus (for En_kin = 0)
+ E_kin = PMaxwellMod(Td,Ai-1); // Maxwell, with partial 1/v behaviour
+ Tf = U_Temp(Zi,Ai-1,Ei-E_kin-SNeff,1,1,Tscale,Econd);
+ // final energy of daughter nucleus with En_kin considered
+
+ // if(Ei-E_kin-2*Td > 10) // In Fermi-gas regime
+ if(Ei-E_kin-Td > 5) // to avoid Tf at negative energies
+ {
+ // if(rn->Rndm() > sqrt( exp(E_kin/Td)/ exp(E_kin/Tf) ))
+ // if (rn->Rndm() > ( Exp(E_kin/Td)/ Exp(E_kin/Tf) )^0.33333 ) // last option
+ // if (rn->Rndm() > ( Exp(E_kin/Td)/ Exp(E_kin/Tf) )^0.25 )
+ // Modified Maxwell that adapts to the Fermi-gas regime
+ if( rn->Rndm() > pow( pow(exp(E_kin/Td),2)/ exp(E_kin/Tf),0.25) )
+ Too_Low=true;
+ // adjusted to data, justification not clear
+ }
+ }
+ else
+ {
+ // E_kin too high after several attemps
+ // no neutron emitted
+ Af = Ai;
+ Zf = Zi;
+ Ef = Ei;
+ break;
+ }
+
+ if(E_kin > Ei-SN)
+ {
+ // E_kin from PMaxwell is not available
+ // Try again
+ Too_Low=true;
+ }
+ }
+ Af = Ai - 1;
+ Zf = Zi;
+ Ef = Ei - E_kin - SN;
+
+ // ANAL(EN,E_kin);
+ //ANAL(ENM(I_MODE),E_kin);
+
+ // Shell effects included //
+ if( B_Expmass == 0 )
+ {
+ SN = (U_MASS(Zf,Af-1.) + Fred * LyPair(Zf,Af-1.)) - (U_MASS(Zf,Af) + Fred * LyPair(Zf,Af));
+ SNeff = U_MASS(Zf,Af-1.) - U_MASS(Zf,Af);
+ // SNmean = 0.5 * (U_MASS(Zf,Af-2.) - U_MASS(Zf,Af));
+ }
+ else
+ {
+ SNexp = ( AME2012(Zf,Af-1) - AME2012(Zf,Af) ); // empirical
+ SNeff = U_MASS(Zf,Af-1.) - U_MASS(Zf,Af); // with shells, without pairing
+ SNld = LDMass(Zi,Ai-1.,0.0) - LDMass(Zi,Ai,0.0); // no shells, no pairing
+ SN = Fred_shell * (Fred * SNexp + (1.0 - Fred) * SNeff) + (1.0 - Fred_shell) * SNld;
+ }
+
+ // Shell effects excluded
+ // SN = LDMass(Zf,Af-1.,0.0) + Lypair(Zf,Af-1.) - (LDMass(Zf,Af,0.0) + Lypair(Zf,Af)) ;
+ // SNeff = LDMass(Zf,Af-1.,0.0) - LDMass(Zf,Af,0.0);
+
+ Ai = Af;
+ Zi = Zf;
+ Ei = Ef;
+
+ Array_En[Ifold] = E_kin * (Af-1.) / Af;
+ Array_Tn[Ifold] = Tn_acc;
+ Ifold = Ifold + 1;
+ }
+
+
+ A_RES = Af;
+ Z_RES = Zf;
+ E_FINAL = Max(Ef,0.0);
+
+}
+
+float GEF::u_accel(float A1, float Z1, float A2, float Z2, float TKE , float E0, float Tn)
+{
+ // returns the velocity of the fragment 1 after time Tn
+ //Acceleration of fission fragments by their Coulomb field
+
+ // natural constants
+ static float e2 = 1.44; // MeV
+ static float u = 931.5; // MeV / c^2
+ static float hbarc = 197; // MeV fm
+
+ // variables
+ float Ared,d0,v0;
+ float d, t, dt, a, v, v1, E;
+ float vinf; // relative velocity at infinity
+
+ Ared = A1 * A2 / (A1 + A2);
+ vinf = sqrt(TKE/Ared); // sqrt(E/A), Ekin asymmptotic in MeV
+ if((t > 100) | (TKE < E0))
+ v = vinf;
+ else
+ {
+ d0 = e2 * Z1 * Z2 / (TKE-E0); // fm
+ v0 = sqrt(E0); // sqr(E/A), Ekin at scission in MeV
+
+ d = d0;
+ v = 0;
+ dt = 0.01;
+ t=0;
+ while(t<=1) // in 10^-21 s
+ {
+ if (t >= Tn)
+ break;
+ E = E0 + e2 * Z1 * Z2 * (1/d0 - 1/d); // MeV
+ v = sqrt(E/Ared); // sqrt(E/A), E in MeV
+ d = d + v * 14 * dt; // in fm
+ t += dt;
+ }
+ dt = 0.1;
+ t=1.1;
+ while(t<=10) // in 10^-21 s
+ {
+ if(t >= Tn)
+ break;
+ E = E0 + e2 * Z1 * Z2 * (1/d0 - 1/d); // MeV
+ v = sqrt(E/Ared); // sqrt(E/A), E in MeV
+ d = d + v * 14 * dt; // in fm
+ t += dt;
+ }
+ dt = 1;
+ t=11;
+ while(t<100) // in 10^-21 s
+ {
+ if(t >= Tn)
+ break;
+ E = E0 + e2 * Z1 * Z2 * (1/d0 - 1/d); // MeV
+ v = sqrt(E/Ared); // sqrt(E/A), E in MeV
+ d = d + v * 14 * dt; // in fm
+ }
+ }
+ v1 = v * A2/(A1+A2);
+ return v1;
+}
+
+float GEF::P_Egamma_low(float Zi, float Ai, float Ei)
+{
+ // Random function, returns gamma energy in MeV
+ // For energies below Sn: no competition with neutrons
+ float Rres;
+ int N;
+ float sigMax, Eg, Erest, rhorest, fg;
+ float xran, yran;
+ float Tm;
+ float GammaExp;
+
+ float betadef = 0;
+ float gammadef = 0;
+
+ float G0[4],E0[4];
+
+ float alev;
+
+ N = CInt(Ei*10 + 0.5);
+ if( N <= 0)
+ N = 1;
+ float sigma[N]; // sigma is not normalized!
+ // (Normalization is done by Monte-Carlo procedure.)
+
+ Tm = U_Temp(Zi,Ai,Ei,1,1,Tscale,Econd);
+
+ betadef = DEFOtab[CInt(Ai-Zi)][CInt(Zi)]; // ground-state deformation
+ gammadef = -120 * betadef + 47.4; // A. Junghans
+
+ // Print Tm
+ // Tm = Tm / 2 ' + 0.1 * (1.0 / U_I_Shell(Zi,Ai) - 1)
+ // Print Tm
+ // sleep
+ // For eventual specific behaviour of gamma strength in magic nuclei
+ //betadef = 0
+ //gammadef = 0
+ if(betadef == 0 && gammadef == 0)
+ {
+ E0[2] = E0_GDR(Zi,Ai);
+ G0[2] = Width_GDR(E0[2]);
+
+ // Establish distribution
+ sigMax = 0;
+ Eg = 0.1;
+ while(Eg <= Ei)
+ {
+ N = CInt(Eg*10);
+ // sigma(N) = exp(-Eg/Tm) * Eg^2; // for testing shape of gamma-strength function
+ sigma[N] = exp(-Eg/Tm) * pow(Eg,3) * (G0[2] * Eg) / ( pow(pow(Eg,2) - pow(E0[2],2),2) + pow(G0[2],2) * pow(E0[2],2) ) ;
+ // + 0.7 * G0(2) * 4 * pi^2 * Tm^2 / E0(2)^5 )
+ // last line: correction for low gamma energy (PRC 41 (190) 1941)
+ if(sigma[N] > sigMax)
+ sigMax = sigma[N];
+ Eg += 0.1;
+ }
+ //Print "Tm,E0,G0)";Tm,E0(2),G0(2)
+ //For Eg = 0.1 To Ei Step 0.1
+ // N = CInt(Eg*10)
+ // Print Eg,sigma(N) / sigMax
+ //Next Eg
+ }
+ else
+ {
+ sigMax = 0;
+ for(int i=1;i<=3;i++)
+ {
+ E0[i] = E0_GDR(Zi,Ai) * Efac_def_GDR(betadef,gammadef,i);
+ G0[i] = Width_GDR(E0[i]);
+ // Establish distribution
+ Eg = 0.1;
+ while(Eg<=Ei)
+ {
+ N = CInt(Eg*10);
+ // sigma(N) = sigma(N) + exp(-Eg/Tm) * Eg^3 *_
+ // (G0(I) * Eg) / ( (Eg^2 - E0(I)^2)^2 + G0(I)^2 * E0(I)^2 )
+ sigma[N] = sigma[N] + exp(-Eg/Tm) * pow(Eg,3) *
+ ( (G0[i] * Eg) / ( pow(pow(Eg,2) - pow(E0[i],2),2) + pow(G0[i],2) * pow(E0[i],2) )
+ /* + 0.001 * exp(-0.5) */
+ /* + 0.7 * G0[i] * 4 * pi^2 * Tm^2 / E0[i]^5*/ ) ;
+ // exponential: M1 strength at low energy, PRL 111, 232504 (2013)
+ // last line: correction for low gamma energy (PRC 41 (1990) 1941)
+ if (sigma[N] > sigMax)
+ sigMax = sigma[N];
+ Eg += 0.1;
+ }
+ }
+ }
+ // Dice gamma energy from distribution
+ bool diceagain_gamma_low = true;
+ if(diceagain_gamma_low)
+ {
+ diceagain_gamma_low = false;
+ xran = rn->Rndm() * Ei * 10; // in units of 100 keV
+ yran = rn->Rndm() * sigMax;
+ if(yran > sigma[CInt(xran)])
+ diceagain_gamma_low = true;
+ }
+ return xran/10; // convert to MeV
+}
+
+float GEF::P_Egamma_high(float Zi, float Ai, float Ei)
+{
+ // Random function, returns gamma energy in MeV
+ // From PRL 49 (1982) 434
+ // For energies above Sn: competition with neutrons included
+ int N;
+ float sigMax, Eg;
+ float xran, yran;
+ float Tm;
+ float G0,E0;
+
+ N = CInt(Ei*10 + 0.5);
+ if(N <= 0)
+ N = 1;
+ float sigma[N]; // sigma is not normalized
+ // (Normalization is done by Monte-Carlo procedure.)
+
+ E0 = E0_GDR(Zi,Ai);
+ G0 = Width_GDR(E0);
+ Tm = U_Temp(Zi,Ai,Ei,1,1,Tscale,Econd);
+
+ //Establish distribution
+ sigMax = 0;
+ Eg = 0.1;
+ while (Eg<=Ei)
+ {
+ N = CInt(Eg*10.0);
+ sigma[N] = pow(Eg,3) / pow(Tm,2) * exp(-Eg/Tm) * (G0 * Eg) / ( pow(pow(Eg,2) - pow(E0,2),2) + pow(G0,2) * pow(E0,2));
+ if(sigma[N] > sigMax)
+ sigMax = sigma[N];
+ Eg += 0.1;
+ }
+ // Dice gamma energy from distribution
+ bool diceagain_gamma_high=true;
+ if(diceagain_gamma_high)
+ {
+ diceagain_gamma_high=false;
+ xran = rn->Rndm() * Ei * 10; // in units of 100 keV
+ yran = rn->Rndm() * sigMax;
+ if(yran > sigma[CInt(xran)])
+ diceagain_gamma_high=true;
+ }
+ return xran/10; // convert to MeV
+}
+
+float GEF::U_Ired(float Z, float A)
+{
+ // Effective moment of inertia by pairing with correction for excitation energy
+ float I_rigid_spher,IfragEff;
+
+ I_rigid_spher = pow(1.16,2) * pow(A,1.6667) / 103.8415;
+ // IfragEff = I_rigid_spher + 0.003 * A^(4.0/3.0) * U_shell(Cint(Z),Cint(A))
+ // IfragEff = I_rigid_spher + 0.005 * A^(4.0/3.0) * U_shell(Cint(Z),Cint(A))
+ // reduction due to shell (Deleplanque et al. PRC 69 (2004) 044309)
+ IfragEff = 0.45 * I_rigid_spher; // Effect of superfluidity
+ // IfragEff = 0.65 * IfragEff // Average effect of superfluidity and deformation
+
+ return IfragEff;
+}
+
+float GEF::U_IredFF(float Z, float A)
+{
+ // Effective moment of inertia by pairing with correction for excitation energy
+ // of final fission fragments
+ return U_Ired(Z,A) * U_I_Shell(Z,A);
+}
+
+float GEF::U_I_Shell(float Z, float A)
+{
+ int N_shells[7];
+ // Shell effect on the effective moment of inertia
+ float dNmin, dZmin, dNsubmin;
+ float Inv_add = 0;
+ float I_inv_add_Z = 0;
+ float I_inv_add_N = 0;
+ float I_inv_add_Nsub = 0;
+ N_shells[1] = 20;
+ N_shells[2] = 28;
+ N_shells[3] = 50;
+ N_shells[4] = 82;
+ N_shells[5] = 126;
+ N_shells[6] = 56;
+ dNmin = 100;
+ dZmin = 100;
+ dNsubmin = 100;
+ for(int i=1;i<=5;i++)
+ dZmin = Min(dZmin,abs(N_shells[i] - Z));
+ for(int i=1;i<=5;i++)
+ dNmin = Min(dNmin,abs(N_shells[i] - (A-Z)));
+ dNsubmin = abs(N_shells[6] - (A-Z));
+
+ // Effect of shells:
+ if(dZmin < 10.0)
+ {
+ // I_inv_add_Z = 0.33 * (6.0 * sqr(A/140.) - dZmin) * sqr(140./A)
+ I_inv_add_Z = 0.33 * (6.0 * sqrt(A/140.0) - dZmin) * pow(140.0/A,1.5);
+ // A^(-1/3) dependence: "A simple phenomenology for 2gamma+ states",
+ // N. V. Zamfir, D. Bucurescu, R. F. Casten, M. Ivascu,
+ // Phys. Lett. B 241 (1990) 463
+ I_inv_add_Z = Max(I_inv_add_Z,0.0);
+ }
+ if(dNmin < 10.0)
+ {
+ // I_inv_add_N = 0.42 * (8.0 * sqr(A/140.) - dNmin) * sqr(140./A)
+ I_inv_add_N = 0.42 * (8.0 * sqrt(A/140.0) - dNmin) * pow(140.0/A,1.5);
+ I_inv_add_N = Max(I_inv_add_N,0.0);
+ }
+ if(dNsubmin < 6.0)
+ {
+ // I_inv_add_Nsub = 1.7 * (4.0 - dNsubmin) * (1.0 - 0.32 * Abs(40.0-Z))
+ I_inv_add_Nsub = 1.7 * (4.0 - dNsubmin) * (1.0 - 0.18 * abs(40.0-Z));
+ // N = 56 subshell only around Z = 40
+ I_inv_add_Nsub = Max(I_inv_add_Nsub,0.0);
+ }
+ return 1.0 / (1.0 + Max(I_inv_add_N,I_inv_add_Nsub) + I_inv_add_Z);
+ //Print "*",I_inv_add_Z, I_inv_add_N, I_inv_add_Nsub,1.0 / (1.0 + Max(I_inv_add_N,I_inv_add_Nsub) + I_inv_add_Z)
+}
+
+float GEF::U_alev_ld(float Z, float A)
+{
+ // return 0.073 * A + 0.095 * A^0.666667 //Ignatyuk (1970's)
+ return 0.078 * A + 0.115 * pow(A,0.6666667); // Ignatyuk (Bologna 2000)
+ // return = 0.089 * A // only volume term
+}
+
+double GEF::U_levdens(int Z, int A, float E, int Ishell, float Ipair, float Tscale, float Econd, float af_an)
+{
+ // Comment: The normalization of the CT level density to the FG level density
+ // reduces the jump in Pf around 16 MeV and leads to a more regular
+ // evolution of Pf with N_CN and Z_CN. The absolute values of Pf are not
+ // modified very much.
+ float Etrans = 8.0; // Transition from CT to Fermi gas
+ double rho, rho1, rho2;
+ if(E < Etrans)
+ {
+ rho1 = U_levdens_FG(Z,A,Etrans,Ishell,Ipair,Tscale,Econd,af_an);
+ rho2 = U_levdens_Egidy(Z,A,Etrans,Ishell,Ipair,Tscale,Econd,af_an);
+ rho = U_levdens_Egidy(Z,A,E,Ishell,Ipair,Tscale,Econd,af_an) * rho1 / rho2;
+ // rho = U_levdens_Egidy(Z,A,E,Ishell,Ipair,Tscale,Econd,af_an)
+ }
+ else
+ {
+ // rho1 = U_levdens_FG(Z,A,Etrans,Ishell,Ipair,Tscale,Econd,af_an)
+ // rho2 = U_levdens_Egidy(Z,A,Etrans,Ishell,Ipair,Tscale,Econd,af_an)
+ // rho = U_levdens_FG(Z,A,E,Ishell,Ipair,Tscale,Econd,af_an) * rho2 / rho1
+ // normalized to FG formula at Etrans
+ rho = U_levdens_FG(Z,A,E,Ishell,Ipair,Tscale,Econd,af_an);
+ }
+ return rho;
+}
+
+double GEF::U_levdens_Egidy(int Z, int A, float E, int Ishell, int Ipair, float Tscale, float Econd, float af_an)
+{
+ // E may be given above ground state or above the macroscopic ground state
+ float Temp, DU, Ered, Rmicro, Rshell;
+ if( Ishell == 1)
+ {
+ DU = U_SHELL_exp(Z,A); // For ground state (only shell effect)
+ if(Z > 92) // hypothetical deviation in the macroscopic masses
+ DU = DU + 0.1 * (Z - 92);
+ }
+ else
+ DU = 0; // for barrier (no shell effect at all)
+ if(Ipair == 1)
+ {
+ Rmicro = - U_SHELL_EO_exp(Z,A); // microscopic effects (shell and pairing)
+ Rshell = - U_SHELL_exp(Z,A); // only shell effect
+ if(Z > 92) // hypothetical deviation in the macroscopic masses
+ {
+ Rmicro = Rmicro - 0.1 * (Z - 92);
+ Rshell = Rshell - 0.1 * (Z - 92);
+ }
+ Ered = E + Rshell - Rmicro + 2.0 * 12.0 / sqrt(A); // shift from odd-odd to even-even basis (exp)
+ // compatibility with Egidy's formula is tested (Ered = E for even-even nuclei)
+ // Ered = E + Lypair(Z,A) + 2.0 * 12.0 / sqr(A) // shift from odd-odd to even-even basis (schematic)
+ }
+ else
+ Ered = E + 2.0 * 12.0 / sqrt(A); // energy is given above the macr. ground state
+ // If Z > 92 Then // hypothetical shift of macr. masses -> lower shell effect
+ // DU = DU + 0.33 * (Z - 92)
+ // End If
+ // DU = DU + Econd
+ Temp = 1.0 / ( (0.0570 + 0.00193*DU) * pow(A,0.6666667)); // from PRC 80 (2009) 054310
+ return 1.0 / Temp * exp(Ered/Temp);
+}
+
+double GEF::U_levdens_FG(int Z, int A, float E, int Ishell, int Ipair, float Tscale, float Econd, float af_an)
+{
+ // This function calculates the level density in the FG regime,
+ // taking a high-energy value as reference,
+ // starting from the macroscopic masses with an imposed Econd.
+ // This destroys all structural effects at high E* in a well controlled way.
+ // E on input is the excitation energy above the "real" ground state
+ float Ered, DU; // energy above the fictive macroscopic ground state
+ float alev,Eshift_shell,Rmicro,Rshell;
+ double Rho1;
+ float fgamma = 0.055;
+ float F_enhance = 1.3; // normalization to CT formula
+ // float F_enhance = 0.18; // normalization to CT formula
+ if(Ishell == 1)
+ {
+ if(Ipair == 0)
+ {
+ Rshell = - U_SHELL_exp(Z,A);
+ if(Z > 92) // hypothetical deviation in the macroscopic masses
+ Rshell = Rshell - 0.1 * (Z - 92);
+ Rmicro = Rshell;
+ }
+ else
+ {
+ Rmicro = - U_SHELL_EO_exp(Z,A); // microscopic effects (shell and pairing)
+ Rshell = - U_SHELL_exp(Z,A); // only shell effect
+ if(Z > 92) // hypothetical deviation in the macroscopic masses
+ {
+ Rshell = Rshell - 0.1 * (Z - 92);
+ Rmicro = Rmicro - 0.1 * (Z - 92);
+ }
+ // Eshift_shell = Rshell*exp(-fgamma * E) // shifting the energy scale to include shell at low E*
+ // Print "*";Rmicro,Rshell;"*" // The values are positive
+ }
+ DU = Rshell;
+ // If Z > 92 Then // hypothetical shift of macr. masses -> lower shell effect
+ // DU = DU - 0.33 * (Z - 92)
+ // End If
+ // DU = DU - Econd
+ Eshift_shell = DU * (1.0 - exp(-fgamma * E)); // remove shell effect at high energies
+ // Eshift_shell = Rshell * (1.0 - exp(-fgamma * E)) // remove shell effect at high energies
+ Ered = E + Rshell - Rmicro - Econd; // origin of the FG without pairing
+ // Ered = E + Rshell + LyPair(Z,A) - Econd // origin of the FG without pairing
+ alev = U_alev_ld(Z,A);
+ // Rho0 = 1.E0/Ered^1.25 * exp(2.E0 * sqr(alev * af_an * Ered))
+ Rho1 = 1./pow(Ered,1.25) * exp(2. * sqrt(alev * af_an * (Ered - Eshift_shell)));
+ // Rho1 = exp(2.E0 * sqr(alev * an_af * (Ered - Eshift_shell)))
+ }
+ else
+ {
+ if(Ipair == 0)
+ {
+ Rshell = - U_SHELL_exp(Z,A);
+ if(Z > 92) // hypothetical deviation in the macroscopic masses
+ Rshell = Rshell - 0.1 * (Z - 92);
+ Rmicro = Rshell;
+ }
+ else
+ {
+ Rmicro = - U_SHELL_EO_exp(Z,A); // microscopic effects (shell and pairing)
+ Rshell = - U_SHELL_exp(Z,A); // only shell effect
+ if(Z > 92) // hypothetical deviation in the macroscopic masses
+ {
+ Rshell = Rshell - 0.1 * (Z - 92);
+ Rmicro = Rmicro - 0.1 * (Z - 92);
+ }
+ }
+ // Ered = E + LyPair(Z,A) - Econd
+ Ered = E + Rshell - Rmicro - Econd; // origin of the FG without pairing
+ alev = U_alev_ld(Z,A);
+ Rho1 = 1./pow(Ered,1.25) * exp(2. * sqrt(alev * af_an * Ered));
+ // Rho1 = exp(2.E0 * sqr(alev * af_an * Ered))
+ }
+ // Print "*";Rmicro,Rshell,Eshift_shell"*" // The values are positive
+ return F_enhance * Rho1;
+}
+
+float GEF::U_Temp(float Z, float A, float E, int Ishell, int Ipair, float Tscale, float Econd)
+{
+ // Temperature (modified Gilbert-Cameron composite level density)
+ // KHS (10. 2. 2012)
+ float alev ;
+ float Eeff0,Eeff1,E1,Rho0,Rho1,TCT,TFG ;
+ float fgamma = 0.055;
+ float RShell,RPair,Res;
+ // Used global parameters: Tscale
+ // alev = U_alev_ld(Z,A) * 1.1 // Factor adjusted to high-energy prompt neutrons in U235(nth,f)
+ alev = U_alev_ld(Z,A) * 0.95; // " with the correction for non-constant T (FG range)
+ // alev = U_alev_ld(Z,A)
+
+ if(Ishell == 1)
+ RShell = U_SHELL(CInt(Z),CInt(A));
+ else
+ RShell = 0.0;
+ TCT = TEgidy(A,RShell,Tscale);
+
+ if(Ipair == 1)
+ RPair = LyPair(CInt(Z),CInt(A));
+ else
+ RPair = 0.0;
+ Eeff0 = E - Econd + RPair + RShell*(1.0 - exp(-fgamma * E));
+
+ if(Eeff0 > 0.5)
+ {
+ // Eeff1 = Eeff0 + 0.1
+ E1 = E + 0.1;
+ Eeff1 = E1 - Econd + RPair + RShell*(1.0 - exp(-fgamma * E1));
+ Rho0 = 1./pow(Eeff0,1.25) * exp(2. * sqrt(alev * Eeff0));
+ Rho1 = 1./pow(Eeff1,1.25) * exp(2. * sqrt(alev * Eeff1));
+ // Rho0 = 1.E0/Eeff0 * exp(2.E0 * sqr(alev * Eeff0))
+ // Rho1 = 1.E0/Eeff1 * exp(2.E0 * sqr(alev * Eeff1))
+ TFG = 0.1/ (log(Rho1) - log(Rho0));
+ }
+ else
+ TFG = 0.0;
+
+ Res = TCT;
+ if(TFG > Res)
+ Res = TFG;
+ // If Res > 1.4 ThenRes = 1.4
+
+ return Res;
+}
+
+float GEF::U_Temp2(float Z, float A, float E, float Rshell, float Rpair, float Tscale, float Econd)
+{
+ // Temperature (modified Gilbert-Cameron composite level density)
+ // KHS (10. 2. 2012)
+ float alev;
+ float Eeff0,Eeff1,Rho0,Rho1,TCT,TFG;
+ static float fgamma = 0.055;
+ float Res;
+ // Used global parameters: Tscale
+ // alev = U_alev_ld(Z,A) * 1.1; // Factor adjusted to high-energy prompt neutrons in U235(nth,f)
+ alev = U_alev_ld(Z,A) * 0.95; // with the correction for non-constant T (FG range)
+ // alev = U_alev_ld(Z,A);
+ TCT = TEgidy(A,Rshell,Tscale);
+ Eeff0 = E - Econd + Rpair + Rshell*(1.0 - exp(-fgamma * E));
+ // Eeff0 = E - Econd + Lypair(CInt(Z),CInt(A)) + Rshell*(1.0 - exp(-fgamma * E))
+ if(Eeff0 > 0.5)
+ {
+ Eeff1 = Eeff0 + 0.1;
+ Rho0 = 1./pow(Eeff0,1.25) * exp(2. * sqrt(alev * Eeff0));
+ Rho1 = 1./pow(Eeff1,1.25) * exp(2. * sqrt(alev * Eeff1));
+ // Rho0 = 1.E0/Eeff0 * exp(2.E0 * sqr(alev * Eeff0))
+ // Rho1 = 1.E0/Eeff1 * exp(2.E0 * sqr(alev * Eeff1))
+ TFG = 0.1 / (log(Rho1) - log(Rho0));
+ }
+ else
+ TFG = 0.0;
+
+ Res = TCT;
+ if(TFG > Res)
+ Res = TFG;
+ return Res;
+}
+
+float GEF::E0_GDR(float Z, float A)
+{
+ // Calculates the centroid energy of the GDR for spherical nucleus
+ // according to the FRDM (ADNDT 59 (1995) 185 and PLB 670 (2008) 200)
+ static float epsilon = 0.0768;
+ static float J = 32.7;
+ static float Q = 29.2;
+ static float R0 = 1.16;
+ static float mstar = 874;
+ static float hbar = 197.3;
+ float Aonethird,u,N,E0;
+
+ // according to [9] in Phys. Lett. B 690 (2010) 473:
+ return 18.0/pow(A,0.333333) + 25.0 /pow(A,0.1666667);
+
+ // according to the FRDM (ADNDT 59 (1995) 185 and PLB 670 (2008) 200):
+ // Aonethird = A^0.333333
+ // N = A - Z
+ // u = (1-epsilon)/Aonethird * 3*J/Q
+ // E0_GDR = hbar /(R0*Aonethird)*sqr(8*J*A^2/ (mstar*4*N*Z) ) * _
+ // (1 + u - epsilon * (1+epsilon+3*u)/(1+epsilon+u))^(-1/2)
+}
+
+float GEF::Width_GDR(float E0)
+{
+ // Spreading width of the GDR (Nucl. Phys. A 531 (1991) 27)
+ return 1.99 * pow(E0/10,1.6);
+}
+
+float GEF::Efac_def_GDR(float Beta, float Gamma, float K)
+{
+ // Modification factors of the resonance energy due to triaxial deformation
+ // Hill-Wheeler parameterisation (PRC 89 (1953) 1102)
+ // Possible values for K: K-2 = -1, 0, 1
+ if(Beta == 0 && Gamma == 0)
+ return 1.;
+ else
+ return 1./(exp(sqrt(5./(4*pi))*Beta * cos(Gamma - 0.666667*(K-2)*pi)));
+}
+
+float GEF::GgGtot(float Z, float A, float E, float Egamma)
+{
+ // From PRL 49 (1982) 434
+ // Probability to emit a gamma of energy Egamma in competition to neutron emission
+ float EG, GG, T, SN;
+ EG = E0_GDR(Z,A);
+ GG = Width_GDR(EG);
+ T = U_Temp(Z,A,E,1,1,Tscale,Econd);
+ SN = U_MASS(Z,A-1.) + LyPair(Z,A-1.) - (U_MASS(Z,A) + LyPair(Z,A)) ;
+ return pow(Egamma,3) / pow(T,2) * exp((SN-Egamma)/T) * GG * EG / (pow(pow(Egamma,2) - pow(EG,2),2) + pow(GG,2) * pow(EG,2));
+}
+
+float GEF::E_next(float T1, float T2, float E1, float E2, float A1, float A2)
+{
+ // Samples the energy transfer in one step between two nuclei
+ // in thermal contact
+ // The energy transfer is only determined by the available phase space.
+ // Only one kind of nucleons considered!
+ // T1,T2 Temperatures of the two nuclei
+ // E1,E2 Initial energies of the two nuclei
+ // A1, A2 Mass numbers of the two nuclei
+ float E12;
+ float Delta1,Delta2; /// Pairing gaps
+ float Delta_E1,Delta_E2;
+ float E1final; // Energy 1 after transfer
+ float E1mod,E2mod;
+
+ // Assumed level densities:
+ // Even number of nucleons:
+ // 1 ground state at energy E = - 2 Delta not considered
+ // continuous level density above E = 0 : rho1,2 = a1,2 * exp(E1,2/T1,2)
+
+ E12 = E1 + E2; // Total energy
+
+ E1mod = E1;
+ E2mod = E2;
+ if(E1mod > E2mod)
+ {
+ Delta_E1 = Pexplim(-1./T1,0.0,E1mod);
+ E1mod = E1mod - Delta_E1;
+ E2mod = E2mod + Delta_E1;
+ Delta_E2 = Pexplim(-1./T2,0.0,E2mod);
+ E2mod = E2mod - Delta_E2;
+ E1mod = E1mod + Delta_E2;
+ }
+ else
+ {
+ Delta_E2 = Pexplim(-1./T2,0.0,E2mod);
+ E2mod = E2mod - Delta_E2;
+ E1mod = E1mod + Delta_E2;
+ Delta_E1 = Pexplim(-1./T1,0.0,E1mod);
+ E1mod = E1mod - Delta_E1;
+ E2mod = E2mod + Delta_E1;
+ }
+ E1final = E1mod;
+
+ /* Select;
+ When (E1 > E2) Do;
+L3:
+Delta_E1 = Pexplim(-1.E0/T1,0.0,E1);
+E1final = E1 - Delta_E1;
+Delta_E1 = Pexplim(-1.E0/T2,0.0,E12-E1final);
+E1final = E1final + Delta_E1;
+End;
+When (E1 <= E2) Do;
+L4:
+Delta_E1 = Pexplim(-1.E0/T2,0.0,E12-E1);
+E1final = E1 + Delta_E1;
+Delta_E1 = Pexplim(-1.E0/T1,0.0,E1final);
+E1final = E1final - Delta_E1;
+End;
+Otherwise Do;
+List('This should not happen.');
+End;
+End; */
+
+ return E1final;
+}
+
+float GEF::Pexplim(float R_lambda, float xmin, float xmax)
+{
+ // random number from an exponential between xmin and xmax
+ // decay constant: f(x) = exp(lambda * x) !!!
+ // xmin, xmax: limits for sampling
+ float umin, umax; // xmin, xmax transformed
+ float u; // help variable
+ float R_res; // sampled value
+
+ if(abs(R_lambda) < 1.e-30)
+ R_res = xmin + rn->Rndm() * (xmax-xmin);
+ else
+ {
+ umin = exp(xmin*R_lambda);
+ umax = exp(xmax*R_lambda);
+ u = umin + rn->Rndm() * (umax-umin);
+ R_res = 1./R_lambda * log(u);
+ }
+ return R_res;
+}
+
+float GEF::U_Even_Odd(int I_Channel, float PEO)
+{
+ //Creates even-odd fluctuations
+ float R;
+ if(I_Channel%2 == 0)
+ R = 1.0 + PEO;
+ else
+ R = 1.0 - PEO;
+ return R;
+}
+
+int GEF::EVEN_ODD(float R_ORIGIN,float R_EVEN_ODD)
+{
+ // Procedure to calculate I_OUT from R_IN in a way that ///
+ // on the average a flat distribution in R_IN results in a ///
+ // fluctuating distribution in I_OUT with an even-odd effect as ///
+ // given by R_EVEN_ODD ///
+ // ------------------------------------------------------------ ///
+ // EXAMPLES : ///
+ // ------------------------------------------------------------ ///
+ // If R_EVEN_ODD = 0 : ///
+ // CEIL(R_IN) ---- ///
+ // R_IN -> ///
+ // (somewhere in between CEIL(R_IN) and FLOOR(R_IN)) ///
+ // FLOOR(R_IN) ---- --> I_OUT ///
+ // ------------------------------------------------------------ ///
+ // If R_EVEN_ODD > 0 : ///
+ // The interval for the above treatment is ///
+ // larger for FLOOR(R_IN) = even and ///
+ // smaller for FLOOR(R_IN) = odd ///
+ // For R_EVEN_ODD < 0 : just opposite treatment ///
+ // ------------------------------------------------------------ ///
+ // ------------------------------------------------------------ ///
+ // On input: R_ORIGIN nuclear charge (real number) ///
+ // R_EVEN_ODD requested even-odd effect ///
+ // Intermediate quantity: R_IN = R_ORIGIN + 0.5 ///
+ // On output: I_OUT nuclear charge (integer) ///
+ // ------------------------------------------------------------ ///
+
+ float R_IN,R_REST,R_HELP;
+ float R_FLOOR;
+ float R_MIDDLE;
+ int I_OUT;
+
+ R_EVEN_ODD = Min(R_EVEN_ODD,1.);
+ R_IN = R_ORIGIN + 0.5;
+ R_FLOOR = FLOOR(R_IN);
+ if(abs(R_EVEN_ODD) < 1.e-3)
+ I_OUT = R_FLOOR;
+ else
+ {
+ R_REST = R_IN - R_FLOOR;
+ R_MIDDLE = R_FLOOR + 0.5;
+ if(Mod(R_FLOOR, 2) == 0) // even before modif.
+ {
+ R_HELP = R_MIDDLE + (R_REST - 0.5) * 1. / Max(0.01,(1. + R_EVEN_ODD));
+ R_HELP = Min(R_HELP,R_MIDDLE+1);
+ R_HELP = Max(R_HELP,R_MIDDLE-1);
+ }
+ else // odd before modification
+ {
+ R_HELP = R_MIDDLE + (R_REST - 0.5) * 1.E0 / Max(0.01,(1. - R_EVEN_ODD));
+ R_HELP = Min(R_HELP,R_MIDDLE+1);
+ R_HELP = Max(R_HELP,R_MIDDLE-1);
+ }
+ I_OUT = FLOOR(R_HELP);
+ }
+ return I_OUT;
+}
+
+float GEF::BFTF(float RZ, float RA, int I_Switch)
+{
+ // Fission barriers from Myers and Swiatecki, Thomas-Fermi model
+ // I_Switch: 0: liquid-drop; 1: with shells and pairing,
+ // 2: averaged over pairing, 3: with shell and pairing + pairing gap at barrier
+ // 4: liquid-drop + g.s. shell, no Z correction
+ float RN,RI,Rkappa,RS,RF,RX;
+ float RX0 = 48.5428;
+ float RX1 = 34.15;
+ float RB ;
+ int IZ,IA;
+ float bftf;
+
+ IZ = CInt(RZ);
+ IA = CInt(RA);
+ RN = RA - RZ;
+ RI = (RN-RZ) / RA;
+ Rkappa = 1.9 + (RZ - 80.) / 75.;
+ RS = pow(RA,0.666667) * (1. - Rkappa * pow(RI,2));
+ RX = pow(RZ,2) / (RA * (1. - Rkappa * pow(RI,2)));
+ if(RX < 30) // out of range
+ RF = 1.e10;
+ if(RX > RX0) // out of range
+ RF = 0.0;
+ if(RX < RX1 && RX > 30)
+ RF = 0.595553 - 0.124136 * (RX - RX1);
+ if(RX >= RX1 && RX <= RX0)
+ RF = 0.000199749 * pow(RX0 - RX,3);
+ RB = RF * RS;
+
+ switch(I_Switch)
+ {
+ case 0: //no shell, no pairing
+ {
+ bftf = RB;
+ }break;
+ case 1: // including even-odd staggering due to increased pairing strength at barrier
+ {
+ // Tentative modification from comparison with experimental fission barriers
+ // (shell correction at the barrier?)
+ if(RZ > 86.5)
+ RB = RB - 0.15 * (RZ - 86.5);
+ // If RZ > 90 Then RB = RB + 0.3 * (RZ - 90.0);
+ // If RZ > 98 Then RB = RB - 0.15 * (RZ - 98.0);
+ if(RZ > 90)
+ RB = RB + 0.35 * (RZ - 90.0);
+ if(RZ > 93)
+ RB = RB + 0.15 * (RZ - 93.0);
+ if( RZ > 95)
+ RB = RB - 0.25 * (RZ - 95.0);
+ // bftf = RB - U_Shell(IZ,IA)
+ // bftf = RB - U_Shell_exp(IZ,IA)
+ bftf = RB - U_SHELL_EO_exp(IZ,IA) + LyPair(IZ,IA) * 14.0/12.0;
+ // bftf = RB - U_Shell_EO_exp(RZ,RA) - 14.E0 / sqr(Csng(RA))
+ // * Csng( ( (RZ+1) Mod 2 + (RA-RZ+1) Mod 2) )
+ }break;
+ case 2: // averaged over even-odd staggering
+ {
+ if(RZ > 86.5)
+ RB = RB - 0.15 * (RZ - 86.5);
+ if(RZ > 90)
+ RB = RB + 0.35 * (RZ - 90.0);
+ if(RZ > 93)
+ RB = RB + 0.15 * (RZ - 93.0);
+ if(RZ > 95)
+ RB = RB - 0.25 * (RZ - 95.0);
+ bftf = RB - U_SHELL_exp(IZ,IA);
+ }break;
+ case 3: // like Case 1 but without increased pairing gap at barrier
+ {
+ if(RZ > 86.5)
+ RB = RB - 0.15 * (RZ - 86.5);
+ if(RZ > 90)
+ RB = RB + 0.35 * (RZ - 90.0);
+ if(RZ > 93)
+ RB = RB + 0.15 * (RZ - 93.0);
+ if(RZ > 95)
+ RB = RB - 0.25 * (RZ - 95.0);
+ bftf = RB - U_SHELL_EO_exp(IZ,IA);
+ }break;
+ case 4: // like case 3 but without Z correction
+ {
+ // This is the direct description from the topographic theorem.
+ bftf = RB - U_SHELL_exp(IZ,IA);
+ }break;
+ default:
+ {
+ cout<< "Undefined option in BFTF"<<endl;
+ }break;
+ }
+ /* if(I_Switch == 0)
+ bftf = RB;
+ else
+ {
+ // Tentative modification from comparison with experimental fission barriers
+ // (shell correction at the barrier?)
+ if(RZ > 86.5) RB = RB - 0.15 * (RZ - 86.5);
+ // if(RZ > 90) RB = RB + 0.3 * (RZ - 90.0);
+ // if(RZ > 98) RB = RB - 0.15 * (RZ - 98.0);
+ if(RZ > 90) RB = RB + 0.35 * (RZ - 90.0);
+ if(RZ > 93) RB = RB + 0.15 * (RZ - 93.0);
+ if(RZ > 95) RB = RB - 0.25 * (RZ - 95.0);
+ // bftf = RB - U_SHELL(IZ,IA);
+ // bftf = RB - U_SHELL_exp(IZ,IA);
+ bftf = RB - U_SHELL_EO_exp(IZ,IA) + LyPair(IZ,IA) * 14.0/12.0;
+ }*/
+ return bftf;
+}
+float GEF::BFTFA(float RZ, float RA, int I_Switch)
+{
+ // inner barrier height
+ float EA,BF0,Z4A,Z3A,DB;
+ float coeff = 0.5;
+ BF0 = BFTF(RZ,RA,I_Switch);
+ // Z4A = RZ^4 / RA
+ // EB - EA from fit to Smirenkin barriers:
+ // V. M. Kupriyanov, K. K. Istekov, B. I. Fursov, G. N. Smirenkin
+ // Sov. J. Nucl. Phys. 32 (1980) 184
+ // DB = -10.3517 + 1.6027E-5 * Z4A + 5.4945E-11 * Z4A^2 // EA - EB
+ // EB - EA from fit to data from Dahlinger et al. (KHS, 21. Dec. 2012)
+ Z3A = pow(RZ,3) / RA;
+ DB = -(5.40101 - 0.00666175*Z3A + 1.52531e-6*pow(Z3A,2));
+ if(DB > 0.0)
+ EA = BF0 - DB;
+ else
+ EA = BF0 ;
+ return EA;
+}
+
+float GEF::BFTFB(float RZ, float RA, int I_Switch)
+{
+ // outer barrier height
+ float EB,BF0,Z4A,Z3A,DB;
+ float coeff = 0.5;
+ BF0 = BFTF(RZ,RA,I_Switch);
+ // Z4A = RZ^4 / RA
+ // EB - EA from fit to Smirenkin barriers:
+ // V. M. Kupriyanov, K. K. Istekov, B. I. Fursov, G. N. Smirenkin
+ // Sov. J. Nucl. Phys. 32 (1980) 184
+ // DB = -10.3517 + 1.6027E-5 * Z4A + 5.4945E-11 * Z4A^2 // EA - EB
+ // EB - EA from fit to data from Dahlinger et al. (KHS, 21. Dec. 2012)
+ Z3A = pow(RZ,3) / RA;
+ DB = -(5.40101 - 0.00666175*Z3A + 1.52531e-6*pow(Z3A,2));
+ if(DB < 0.0)
+ EB = BF0 + DB;
+ else
+ EB = BF0;
+ return EB;
+}
+float GEF::Gaussintegral(float R_x, float R_sigma)
+{
+ // Smoothed step function. Grows from 0 to 1 around R_x
+ // with a Gauss-integral function with given sigma
+ float R_ret;
+ // Note: The variable R_sigma = standard deviation / sqr(2) !
+ R_ret = 0.5 + 0.5 * Erf(R_x / R_sigma);
+ return R_ret;
+}
+
+float GEF::U_Box(float x, float sigma, float width)
+{
+ float y;
+ // Note: The variable sigma = standard deviation / sqr(2) !
+ y = Gaussintegral(x+0.5*width,sigma) - Gaussintegral(x-0.5*width,sigma);
+ return y/width;
+}
+
+float GEF::U_Box2(float x, float sigma1, float sigma2, float width)
+{
+ float y;
+ // Note: The variable sigma = standard deviation / sqr(2) !
+ y = Gaussintegral(x+0.5*width,sigma2) - Gaussintegral(x-0.5*width,sigma1);
+ return y/width;
+}
+
+float GEF::U_Gauss(float x, float sigma)
+{
+ float y;
+ y = 1.0 / (sqrt(2.0 * pi) * sigma) * exp(-pow(x,2)/ ( 2.0 * pow(sigma,2) ) );
+ return y;
+}
+
+float GEF::U_Gauss_abs(float x, float sigma)
+{
+ float y;
+
+ y = exp(-pow(x,2)/ ( 2.0 * pow(sigma,2) ) );
+ return y;
+}
+
+float GEF::U_Gauss_mod(float x,float sigma)
+{
+ // Gaussian with Sheppard correction
+ float y;
+ float sigma_mod;
+ sigma_mod = sqrt(pow(sigma,2) + 1./12.);
+
+ y = 1.0 / (sqrt(2.0 * pi) * sigma_mod) * exp(-pow(x,2)/ ( 2.0 * pow(sigma_mod,2) ) );
+ return y;
+}
+
+float GEF::PBox(float Mean, float Sigma, float Bottom)
+{
+ // Rectangular distribution folded with a Gaussian distribution
+ float R;
+ R = PGauss(Mean,Sigma);
+ R = R + (rn->Rndm()-0.5)*Bottom;
+ return R;
+}
+
+float GEF::PBox2(float Mean, float Sigma1, float Sigma2, float Bottom)
+{
+ // Rectangular distribution folded with a Gaussian distribution.
+ // One wing is steeper.
+ // Sigma1 = lower side, Sigma2 = upper side
+ float Sigma,R;
+ Sigma = Max(Sigma1,Sigma2);
+
+ R = PGauss(Mean,Sigma);
+ R = R + (rn->Rndm()-0.5)*Bottom;
+ if(Sigma1 < Sigma2)
+ if(R < Mean - 0.5*Bottom)
+ if( rn->Rndm() > exp( -pow(R - Mean + 0.5*Bottom,2) / (2.0 * pow(Sigma1,2)) )/ exp( -pow(R - Mean + 0.5*Bottom,2) / (2.0 * pow(Sigma2,2)) ))
+ R = Mean - 0.5*Bottom + (Mean - 0.5*Bottom - R);
+
+ if(Sigma2 <= Sigma1)
+ if( R > Mean + 0.5*Bottom)
+ if( rn->Rndm() > exp( -pow(R - Mean - 0.5*Bottom,2) / (2.0 * pow(Sigma2,2)) ) / exp( -pow(R - Mean - 0.5*Bottom,2) / (2.0 * pow(Sigma1,2)) ) )
+ R = Mean + 0.5*Bottom - (R - Mean - 0.5*Bottom);
+
+ return R;
+}
+
+float GEF::PPower(int Order, float Rmin, float Rmax)
+{
+ // Random generator of a power function: (y = x^Order -> x_random = RND^(1/(Order+1))
+ // PPower = 0 at Rmin to PPower = Ymax at Rmax
+ float R;
+ R = Rmin + (Rmax-Rmin) * pow(rn->Rndm(),1.0/(Order+1));
+ return R;
+}
+
+float GEF::PPower_Griffin_v(int Order, float Rmin, float Rmax)
+{
+ // Random generator of a power function: (y = x^Order -> x_random = RND^(1/(Order+1))
+ // PPower = 0 at Rmin to PPower = Ymax at Rmax
+ float R,v_particle,RRND;
+ bool Repeat_Griffin=true;
+ while(Repeat_Griffin)
+ {
+ Repeat_Griffin=false;
+ R = Rmin + (Rmax-Rmin) * pow(rn->Rndm(),1.0/(Order));
+ v_particle = sqrt(abs((R-Rmax)/(Rmin-Rmax)));
+ RRND = rn->Rndm();
+ if(RRND > v_particle)
+ Repeat_Griffin=true;
+ }
+ return R;
+}
+
+float GEF::PPower_Griffin_E(int Order, float Rmin,float Rmax)
+{
+ // Random generator of a power function: (y = x^Order -> x_random = RND^(1/(Order+1))
+ // PPower = 0 at Rmin to PPower = Ymax at Rmax
+ float R,E_particle;
+ bool Repeat_Griffin = true;
+ while(Repeat_Griffin)
+ {
+ Repeat_Griffin = false;
+ R = Rmin + (Rmax-Rmin) * pow(rn->Rndm(),1.0/(Order));
+ E_particle = (R-Rmax)/(Rmin-Rmax);
+ if(rn->Rndm() > E_particle)
+ Repeat_Griffin = true;
+ }
+ return R;
+}
+
+float GEF::PGauss(float Mean, float Sigma)
+{
+ // Box-Mueller method
+ static int ISet = 0;
+ float V1,V2,R,Fac,GasDev,Result;
+ static float GSet;
+ if( ISet == 0)
+ {
+ bool Repeat=true;
+ while(Repeat)
+ {
+ Repeat = false;
+ V1 = 2. * rn->Rndm() - 1.;
+ V2 = 2. * rn->Rndm() - 1.;
+ R = pow(V1,2) + pow(V2,2);
+ if((R >= 1.) | (R == 0.0))
+ Repeat = true;
+ }
+ Fac = sqrt(-2. * log(R)/R);
+ GSet = V1 * Fac;
+ GasDev = V2 * Fac;
+ ISet = 1;
+ }
+ else
+ {
+ GasDev = GSet;
+ ISet = 0;
+ }
+ Result = Sigma * GasDev;
+ return Mean + Result;
+}
+
+float GEF::PLinGauss(float R_Sigma)
+{
+ // Random-number generator for linear * Gaussian function
+ // Distribution of nuclear angular momenta
+ float R_Res,B_rms;
+ B_rms = R_Sigma / sqrt(2.0); // Because the sum of two PGauss functions increases the width.
+ R_Res = abs(PGauss(0,B_rms)) + abs(PGauss(0,B_rms));
+ R_Res = R_Res + B_rms/4. * (1. - exp(-R_Res/R_Sigma));
+ // correction of shape (approximative)
+ return R_Res;
+}
+
+float GEF::U_LinGauss(float x, float R_Sigma)
+{
+ // Gaussian times a linear function
+ // Not normalized!
+ float R_Res;
+ if(R_Sigma > 0.0)
+ R_Res = x * exp(-pow(x,2)/(2.0 * pow(R_Sigma,2)));
+ else
+ R_Res = 0.0;
+ return R_Res;
+}
+
+float GEF::PExp(float R_Tau)
+{
+ // Random-number generator for an exponential distribution
+ float X1,R_Res;
+ bool Again=true;
+ while(Again)
+ {
+ Again = false;
+ X1 = rn->Rndm();
+ if(X1 > 1.e-10 && X1 < 0.99999) // for avoiding numerical problems
+ R_Res = - R_Tau * log(X1);
+ else
+ Again = true;
+ }
+
+ return R_Res;
+}
+
+float GEF::PMaxwell(float R_T)
+{
+ // Random-number generator for a surface Maxwell distribution
+ // y = x * exp(-x/T)
+ double R_Res,R_T_int;
+ R_T_int = R_T;
+ R_Res = -R_T_int * (log(rn->Rndm()) + log(rn->Rndm()));
+ return R_Res;
+}
+
+float GEF::PMaxwellv(float R_T)
+{
+ // Random generator according to a distribution similar to a
+ // Maxwell distribution with quantum-mech. x-section for neutrons
+ // (approximation by KHS)
+ // Y = SQRT(X) * EXP(-X/T)
+ float EN;
+ EN = 2. * R_T * sqrt(log(rn->Rndm()) * log(rn->Rndm()));
+ return EN;
+}
+
+float GEF::PMaxwellMod(float R_T, float R_A)
+{
+ // Random generator according to a distribution similar to a
+ // Maxwell distribution with quantum-mech. x-section for neutrons
+ // (approximation by KHS)
+ // Y = SQRT(X) * EXP(-X/T)
+ float EN;
+ if(rn->Rndm() < 3.3 / sqrt(R_A)) //according to PR-116-683 (Dostrowsky et al.)
+ EN = 2. * R_T * sqrt(log(rn->Rndm()) * log(rn->Rndm()));
+ else
+ EN = -R_T * (log(rn->Rndm()) + log(rn->Rndm()));
+ return EN;
+}
+
+float GEF::Round(float R, int N)
+{
+ // R Input value
+ // N Number of significant digits
+ float RN10, Rred, Rextended, Rrounded, Rout, Rabs;
+ int N10,Isign;
+ if(R == 0)
+ return 0;
+ else
+ {
+ Isign = Sgn(R);
+ Rabs = abs(R);
+ N10 = CInt(Log10(Rabs));
+ RN10 = pow(10,N10);
+ Rred = Rabs / RN10;
+ Rextended = Rred * pow(10,N-1);
+ Rrounded = CInt(Rextended + 0.5);
+ Rout = Rrounded / pow(10,N-1) * RN10;
+ return Isign * Rout;
+ }
+}
+
+long int GEF::Modulo(unsigned long int I, unsigned long int J)
+{
+ unsigned long int Iratio,Iresult;
+ Iratio = I / J;
+ Iresult = I - J * Iratio;
+ return Iresult;
+}
+/*
+ int GEF::PLoss(unsigned long int IL)
+ {
+// Extracts and returns number of prompt protons
+Dim As string Ctest;
+int NP;
+Ctest = Oct(IL);
+NP = 0;
+for(int i=1;i<=Len(Ctest);i++)
+if((Mid(Ctest,i,1) == "2") | (Mid(Ctest,i,1) == "4"))
+NP = NP + 1;
+return NP;
+}
+ */
+bool GEF::IsValid(int Z, int A)
+{
+ bool Ivalid;
+ Ivalid = 1;
+ // If I_A / I_Z < 210.E0/90.E0
+ if((Z < 76) || (Z > 120))
+ Ivalid = 0;
+ return Ivalid;
+ //return 1;
+}
+
+
+bool GEF::U_Valid(int I_Z, int I_A)
+{
+ bool Ivalid;
+ Ivalid = 1;
+ // If I_A / I_Z < 210.E0/90.E0
+ if((I_A / I_Z < 160. / 76.) | (I_A / I_Z > 250./90.))
+ Ivalid = 0;
+ if((I_Z < 76) | (I_Z > 120))
+ Ivalid = 0;
+ return Ivalid;
+ //return 1;
+}
+
+float GEF::U_Delta_S0(int I_Z, int I_A)
+{
+ // I_Z and I_A refer to the fissioning nucleus
+ float Delta;
+ Delta = 0;
+
+ if(I_Z == 89)
+ if(I_A == 226)
+ Delta = -0.3;
+
+ if(I_Z == 90)
+ {
+ if(I_A == 228)
+ Delta = 0.2;
+ if(I_A == 229)
+ Delta = 0.4;
+ if(I_A == 230)
+ Delta = 0.7;
+ if(I_A == 231)
+ Delta = 0.8;
+ if(I_A == 232)
+ Delta = 0.9;
+ if(I_A == 233)
+ Delta = 0.9;
+ }
+
+ if(I_Z == 92)
+ Delta = 0.2; //x
+ if(I_Z == 92 && I_A == 233)
+ Delta = 0.4; //x
+ if(I_Z == 92 && I_A == 234)
+ Delta = 0.4; //x
+
+ if(I_Z >= 93)
+ Delta = -0.3; //x
+
+ return Delta;
+}
+
+
+void GEF::PotCurv_FM(void)
+{
+ /* Potential curvatures of fission modes */
+ // For the width of the mass distribution (potential between saddle and scission):
+ // Print Spin_pre_fission, P_I_rms_CN
+ R_Z_Curv_S0 = 8. / pow(Csng(I_Z_CN),2) * Masscurv(Csng(I_Z_CN), Csng(I_A_CN), Spin_pre_fission, kappa);
+ // For the yields of the fission channels (potential near saddle):
+ R_Z_Curv1_S0 = 8. / pow(Csng(I_Z_CN),2) * Masscurv1(Csng(I_Z_CN), Csng(I_A_CN), 0.0, kappa);
+ R_A_Curv1_S0 = 8. / pow(Csng(I_A_CN),2) * Masscurv1(Csng(I_Z_CN), Csng(I_A_CN), 0.0, kappa);
+}
+
+void GEF::EnergyTrans(void)
+{
+ /*
+ switch(Emode)
+ {
+ case 0: // Energy above outer barrier given
+ {
+ R_E_exc_Eb = R_E_exc_used;
+ R_E_exc_GS = R_E_exc_used + BFTFB(Csng(I_Z_CN),Csng(I_A_CN),1);
+ }break;
+ case 1: // Energy above ground state given
+ {
+ R_E_exc_Eb = R_E_exc_used - BFTFB(Csng(I_Z_CN),Csng(I_A_CN),1);
+ R_E_exc_GS = R_E_exc_used;
+ }break;
+ case 3: // Energy above ground state given
+ {
+ R_E_exc_Eb = R_E_exc_used - BFTFB(Csng(I_Z_CN),Csng(I_A_CN),1);
+ R_E_exc_GS = R_E_exc_used;
+ }break;
+ case -1: // Energy above ground state given
+ {
+ R_E_exc_Eb = R_E_exc_used - BFTFB(Csng(I_Z_CN),Csng(I_A_CN),1);
+ R_E_exc_GS = R_E_exc_used;
+ }break;
+ case 2: // kinetic energy of neutron given (SN = neutron separation energy)
+ {
+ // SN = (U_Mass(Csng(I_Z_CN),Csng(I_A_CN-1)) + Lypair(I_Z_CN,I_A_CN-1)) _
+ // -(U_Mass(Csng(I_Z_CN),Csng(I_A_CN)) + Lypair(I_Z_CN,I_A_CN))
+ // R_E_exc_GS = R_E_exc_used + SN
+ SN = AME2012(I_Z_CN,I_A_CN-1) - AME2012(I_Z_CN,I_A_CN);
+ R_E_exc_GS = R_E_exc_used * ((P_A_CN-1) / P_A_CN) + SN; // target CN
+ R_E_exc_Eb = R_E_exc_GS - BFTFB(Csng(I_Z_CN),Csng(I_A_CN),1);
+ }break;
+ case 12: // kinetic energy of proton given (Sprot = proton separation energy)
+ {
+ // Sprot = (U_Mass(Csng(I_Z_CN-1),Csng(I_A_CN-1)) + Lypair(I_Z_CN-1,I_A_CN-1)) _
+ // -(U_Mass(Csng(I_Z_CN),Csng(I_A_CN)) + Lypair(I_Z_CN,I_A_CN))
+ // R_E_exc_GS = R_E_exc_used + Sprot
+ Sprot = AME2012(I_Z_CN-1,I_A_CN-1) - AME2012(I_Z_CN,I_A_CN);
+ R_E_exc_GS = R_E_exc_used * ((P_A_CN-1) / P_A_CN) + Sprot ;
+ R_E_exc_Eb = R_E_exc_GS - BFTFB(Csng(I_Z_CN),Csng(I_A_CN),1);
+ }break;
+ case 13: // list of energies from file
+ {
+ R_E_exc_Eb = R_E_exc_used - BFTFB(Csng(I_Z_CN),Csng(I_A_CN),1);
+ R_E_exc_GS = R_E_exc_used ;
+ }break;
+ }
+ */
+ R_E_exc_Eb = R_E_exc_used - BFTFB(Csng(I_Z_CN),Csng(I_A_CN),1);
+ R_E_exc_GS = R_E_exc_used;
+
+}
+
+void GEF::BarriersEx_FM(void)
+{
+
+ E_exc_S0_prov = R_E_exc_Eb;
+
+ /* Additional influence of N=82 assumed */
+ Delta_NZ_Pol = 82./50. - Csng(I_N_CN)/Csng(I_Z_CN);
+ R_Shell_S1_eff = P_Shell_S1 * (1.0 - P_att_rel * P_att_pol * abs(Delta_NZ_Pol));
+
+ // R_Shell_S1_eff = P_Shell_S1 * _
+ // max(1.0 - P_att_rel,(1.0 - P_att_rel* _
+ // ( Abs(Delta_NZ_Pol)/P_att_Pol + (Delta_NZ_Pol/P_att_Pol2)^2 _
+ // + Abs(Delta_NZ_Pol/P_att_Pol3)^3)))
+ // Print "4335 "; max(1.0 - P_att_rel,(1.0 - P_att_rel* _
+ // ( Abs(Delta_NZ_Pol)/P_att_Pol + (Delta_NZ_Pol/P_att_Pol2)^2 _
+ // + Abs(Delta_NZ_Pol/P_att_Pol3)^3)))
+ // Print Abs(Delta_NZ_Pol)/P_att_Pol, _
+ // (Delta_NZ_Pol/P_att_Pol2)^2, _
+ // Abs(Delta_NZ_Pol/P_att_Pol3)^3
+ //sleep
+
+ /* In Pu, the Z=50 shell meets Z=44 in the light fragment. */
+ /* A deformed shell at Z=44 is assumed to explain the enhancement _
+ of the S1 channel around Pu */
+ /* This very same shell automatically produces the double-humped */
+ /* mass distribution in 180Hg */
+ // S1_enhance = P_Shell_SL4 + _
+ // (Csng(I_Z_CN) - ZC_Mode_1 - ZC_Mode_4L)^2 * P_Z_Curv_SL4
+ // 50 instead of ZC_Mode_1, to eliminate the influenc of the mass
+ //(in agreement with experiment, e.g. 238U(nfast,f) ):
+ S1_enhance = P_Shell_SL4 + pow(Csng(I_Z_CN) - 50.0 - ZC_Mode_4L,2) * P_Z_Curv_SL4;
+
+ // S1_enhance = P_Shell_SL4 * _
+ // U_Gauss_abs(Csng(I_Z_CN) - 50.0 - 0.3 - ZC_Mode_4L,P_Z_Sigma_SL4)
+ //Print "4396: U_Gauss_abs";S1_enhance/P_Shell_SL4,R_SHell_S1_eff
+ //sleep
+
+ // S1_enhance = P_Shell_SL4 + _
+ // (Csng(I_Z_CN) - ZC_Mode_1 - ZC_Mode_4L)^2 * P_Z_Curv_SL4
+ if(S1_enhance > 0)
+ S1_enhance = 0;
+
+ if(P_Z_CN == 91)
+ S1_enhance = S1_enhance + 0.3;
+ if(P_Z_CN == 90)
+ S1_enhance = S1_enhance + 0.6;
+
+ //Print "4384 "; P_Shell_SL4, U_Gauss(Csng(I_Z_CN) - 50.0 - ZC_Mode_4L,0.3), S1_enhance
+ //sleep
+
+ // Print "3933"
+ // Print "ZC_Mode_1,ZC_Mode_4",ZC_Mode_1,ZC_Mode_4
+ // Print "Delta-Z S1-S4, S1_enhance",I_Z_CN-ZC_Mode_1 - ZC_Mode_4L, S1_enhance
+ // Print "3951"
+ R_Shell_S1_eff = R_Shell_S1_eff + S1_enhance;
+ ;
+ // Print I_Z_CN-ZC_Mode_1-ZC_Mode_4L, S1_enhance,R_Shell_S1_eff
+
+ /* The high TKE of S1 in 242Pu(sf) (and neighbours) is obtained by assuming */
+ /* that the Z=44 shell reduces the deformation of the light fragment. */
+ for(int I = 10;I<=(I_Z_CN - 10);I++)
+ {
+ Z1 = Csng(I);
+ A1 = (Z1 - 0.5) / Csng(I_Z_CN) * Csng(I_A_CN); /* polarization roughly considered */
+ // Beta(1,1,Z1) = Beta(1,1,Z1) + 0.15 * S1_enhance /* "light" fragment */
+ Beta[2][1][I] = exp(S1_enhance) * Beta[2][1][I] + (1.-exp(S1_enhance)) * (Beta[2][1][I]-0.25);
+ Beta[2][1][I] = Max(Beta[2][1][I],0.0);
+ E_defo = LyMass(Z1,A1,Beta[2][1][I]) - LyMass(Z1,A1,0.0);
+ Edefo[2][1][I] = E_defo ;/* "light" fragment */
+ }
+
+ // Influence of S2 shell in complementary fragment
+ // May be called "S12 fission channel"
+ T_asym_Mode_2 = 0.5;
+ SigZ_Mode_2 = sqrt(0.5 * T_asym_Mode_2/(P_Z_Curv_S2));
+ SigA_Mode_2 = SigZ_Mode_2 * Csng(I_A_CN) / Csng(I_Z_CN);
+ S1_enhance_S2 = P_Shell_S2 * U_Box(Csng(P_A_CN) - AC_Mode_2 - AC_Mode_1, SigA_Mode_2,P_A_Width_S2) *P_A_Width_S2;
+
+ if(S1_enhance_S2 < 0.01)
+ // Print "S1_enhance_S2 ";S1_enhance_S2
+ R_Shell_S1_eff = R_Shell_S1_eff + S1_enhance_S2;
+
+ R_Shell_S2_eff = P_Shell_S2;
+
+ // Overlap of S3 and shell in light fragment
+ R_Shell_S3_eff = P_Shell_S3 * (1.0 - 0.8* PZ_S3_olap_curv * pow(Csng(I_Z_CN) - ZC_Mode_3 - PZ_S3_olap_pos,2));
+ // Print "4450 "; P_Shell_S3 * (1.0 - 0.8 * PZ_S3_olap_curv _
+ // * (Csng(I_Z_CN) - ZC_Mode_3 - PZ_S3_olap_pos)^2) , ZC_Mode_3
+ // sleep
+ // R_Shell_S3_eff = -5.605
+ // * (Csng(I_Z_CN) - 60.5E0 - PZ_S3_olap_pos)^2)
+ R_Shell_S3_eff = Min(R_Shell_S3_eff,0.0);
+
+ // Additional empirical dependence on N/Z
+ // R_Shell_S3_eff = R_Shell_S3_eff - _
+ // 1 * ( (I_A_CN-I_Z_CN)/I_Z_CN - (236-92)/92)
+ // 5 * ( (I_A_CN-I_Z_CN)/I_Z_CN - (236-92)/92)
+
+ // R_Shell_S4_eff = 2.0 * (P_Shell_S4 + P_Z_Curv_S4*(ZC_Mode_4 - ZC_Mode_0)^2)
+ R_Shell_S4_eff = 2.0 * (P_Shell_S4 + P_Z_Curv_S4 * pow(ZC_Mode_4 - ZC_Mode_0,2));
+ // overlap of S4 in both fragments
+ if(R_Shell_S4_eff > P_Shell_S4)
+ R_Shell_S4_eff = P_Shell_S4;
+ // no overlap at large distance
+
+ E_LD_S1 = R_A_Curv1_S0 * pow(Csng(I_A_CN)/Csng(I_Z_CN)*(ZC_Mode_1 - ZC_Mode_0) ,2);
+ B_S1 = E_LD_S1 + R_Shell_S1_eff;
+ E_exc_S1_prov = E_exc_S0_prov - B_S1;
+
+ E_LD_S2 = R_A_Curv1_S0 * pow(Csng(I_A_CN)/Csng(I_Z_CN)*(ZC_Mode_2 - ZC_Mode_0) ,2);
+ B_S2 = E_LD_S2 + R_Shell_S2_eff;
+ E_exc_S2_prov = E_exc_S0_prov - B_S2;
+
+ E_LD_S3 = R_A_Curv1_S0 * pow(Csng(I_A_CN)/Csng(I_Z_CN)*(ZC_Mode_3 - ZC_Mode_0) ,2);
+ B_S3 = E_LD_S3 + R_Shell_S3_eff;
+ E_exc_S3_prov = E_exc_S0_prov - B_S3;
+
+
+ if(I_A_CN < 220) // Only here S4 is close enough to symmetry to have a chance
+ {
+ E_LD_S4 = R_A_Curv1_S0 * pow(Csng(I_A_CN)/Csng(I_Z_CN)*(ZC_Mode_4 - ZC_Mode_0) ,2);
+ // R_Shell_S4_eff = R_Shell_S4_eff * (1.0 + P_S4_NZmod * (Csng(I_A_CN)/Csng(I_Z_CN) - (180/80)) ) // variation with A/Z
+ R_Shell_S4_eff = R_Shell_S4_eff * (1.0 + P_S4_NZmod * (Csng(I_A_CN-I_Z_CN) - (112)) ); // variation with N
+ //R_Shell_S4_eff = R_Shell_S4_eff * (1.0 - 0.09 * (Csng(I_Z_CN) - 80) ) // variation with Z
+ B_S4 = E_LD_S4 + R_Shell_S4_eff;
+ E_exc_S4_prov = E_exc_S0_prov - B_S4;
+ }
+ else
+ {
+ B_S4 = 9999;
+ E_exc_S4_prov = - 9999;
+ }
+
+ /* Mode 11 (overlap of channel 1 in light and heavy fragment */
+ /* Potential depth with respect to liquid-drop potential: B_S11 */
+ // B_S11 = 2.E0 * (R_Shell_S1_eff + De_Defo_S1 _
+ // + P_Z_Curv_S1 * (ZC_Mode_1 - ZC_Mode_0)^2 ) - De_Defo_S1
+ B_S11 = 2. * (R_Shell_S1_eff + P_Z_Curv_S1 * pow(ZC_Mode_1 - ZC_Mode_0,2) );
+ // Sum of S1 shells in both fragments exact at symmetry
+
+ // Print "4475 ";R_Shell_S1_eff, B_S11
+ // Print ZC_Mode_0, ZC_Mode_1, P_Z_Curv_S1 * (ZC_Mode_1 - ZC_Mode_0)^2
+
+ // If B_S11 (see above) is higher than the shell at symmetry from only one fragment
+ // If B_S11 > R_Shell_S1_eff + P_Z_Curv_S1 * (ZC_Mode_1 - ZC_Mode_0)^2 Then
+ // B_S11 = Min(B_S11,R_Shell_S1_eff + P_Z_Curv_S1 * (ZC_Mode_1 - ZC_Mode_0)^2 )
+ // End If
+
+ DES11ZPM = 0;
+ // The S1 shells in the two fragments must be rather close to form one pocket:
+ if(B_S11 < (R_Shell_S1_eff + Level_S11))
+ // Lowering of the zero-point motion grows with the width of the potential pocket:
+ // DES11ZPM = -0.6 * Abs(ZC_Mode_1 - ZC_Mode_0)
+ DES11ZPM = -0.8 * abs(ZC_Mode_1 - ZC_Mode_0); // Fits the mass distr. of 258Fm(sf)
+
+ /* Lowering of effective barrier by lower ZPM due to larger width in
+ partial overlap region (shells in light and heavy fragment) */
+ // DES11ZPM = Level_S11 * Min(Abs(ZC_Mode_1 - ZC_Mode_0),4.E0*P_Z_Curv_S1)
+ // DES11ZPM = -0.2 * Abs(ZC_Mode_1 - ZC_Mode_0)
+
+ // Print "4473: "; R_Shell_S1_eff, B_S11, DES11ZPM
+ // Sleep
+
+ B_S11 = B_S11 + DES11ZPM;
+
+ // If B_S11 > R_Shell_S1_eff + 0.5E0 Then
+ // If B_S11 > R_Shell_S1_eff + Level_S11 Then
+ // B_S11 = 100 // S1 and S11 are exclusive
+ // Else
+ // B_S11 = Min(B_S11,R_Shell_S1_eff)
+ // End If
+
+ E_exc_S11_prov = E_exc_S0_prov - B_S11;
+
+ /* Mode 22 (overlap of channel 2 in light and heavy fragment */
+ /* Potential depth with respect to liquid-drop potential: B_S22 */
+
+ // B_S22 = 2.E0 * (E_LD_S2 + P_Shell_S2) _
+ // + 2.E0 * P_Z_Curv_S2 * (ZC_Mode_2 - ZC_Mode_0)^2 /* Parabola */
+ //Print E_LD_S2,P_Shell_S2,P_Z_Curv_S2,ZC_Mode_2,ZC_Mode_0
+ B_S22 = 2. * R_Shell_S2_eff * U_Box(Csng(P_A_CN)/2.0 - AC_Mode_2,SigA_Mode_2,P_A_Width_S2) * P_A_Width_S2;
+ // The integral of U_Box is normalized, not the height!
+ // If Abs((P_A_CN/2.E0) - AC_Mode_2) > P_A_Width_S2 Then B_S22 = 9999
+ if(P_A_CN < 226)
+ B_S22 = 9999;
+
+ E_exc_S22_prov = E_exc_S0_prov - B_S22;
+
+ E_Min_Barr = Min(0.0,B_S1);
+ E_Min_Barr = Min(E_Min_Barr,B_S2);
+ E_Min_Barr = Min(E_Min_Barr,B_S3);
+ E_Min_Barr = Min(E_Min_Barr,B_S4);
+ E_Min_Barr = Min(E_Min_Barr,B_S11);
+ E_Min_Barr = Min(E_Min_Barr,B_S22);
+
+ /* Energy minus the height of the respective fission saddle */
+ E_Exc_S0 = E_exc_S0_prov + E_Min_Barr - Delta_S0;
+ E_Exc_S1 = E_exc_S1_prov + E_Min_Barr;
+ E_Exc_S2 = E_exc_S2_prov + E_Min_Barr;
+ E_Exc_S3 = E_exc_S3_prov + E_Min_Barr;
+ E_Exc_S4 = E_exc_S4_prov + E_Min_Barr;
+ E_Exc_S11 = E_exc_S11_prov + E_Min_Barr;
+ E_Exc_S22 = E_exc_S22_prov + E_Min_Barr;
+
+ /* Energy above the lowest fission saddle */
+ E_exc_Barr = Max(E_Exc_S0,E_Exc_S1);
+ E_exc_Barr = Max(E_exc_Barr,E_Exc_S2);
+ E_exc_Barr = Max(E_exc_Barr,E_Exc_S3);
+ E_exc_Barr = Max(E_exc_Barr,E_Exc_S4);
+ E_exc_Barr = Max(E_exc_Barr,E_Exc_S11);
+ E_exc_Barr = Max(E_exc_Barr,E_Exc_S22);
+}
+
+void GEF::TCollective(void)
+{
+ /* Collective temperature used for calculating the widths
+ in mass asymmetry and charge polarization */
+
+ if(E_Exc_S0 < 0)
+ E_tunn = -E_Exc_S0;
+ else
+ E_tunn = 0;
+ R_E_exc_eff = Max(0.1,E_Exc_S0);
+ // T_Coll_Mode_0 = TFCOLL * R_E_exc_eff + _ // empirical, replaced by TRusanov
+ T_Coll_Mode_0 = TCOLLFRAC * (De_Saddle_Scission(pow(Csng(I_Z_CN),2) / pow(Csng(I_A_CN),0.33333),ESHIFTSASCI_coll) - E_tunn);
+ T_Coll_Mode_0 = Max(T_Coll_Mode_0,0.0);
+
+ //Print "4596: De_SS, E_tunn, T_Coll ";De_Saddle_Scission(I_Z_CN^2/I_A_CN^0.3333,ESHIFTSASCI_coll),E_tunn,T_Coll_Mode_0
+
+ /* Temperature description fitting to the empirical systematics of Rusanov et al. */
+ /* Here from Ye. N. Gruzintsev et al., Z. Phys. A 323 (1986) 307 */
+ /* Empirical description of the nuclear temperature according to the */
+ /* Fermi-gas description. Should be valid at higher excitation energies */
+ float T_Rusanov;
+ T_Rusanov = TRusanov(R_E_exc_eff,Csng(I_A_CN));
+ //Print "Temperatures, (GEF, Total, Rusanov): ", T_Coll_Mode_0, TFCOLL * R_E_exc_eff, T_Rusanov
+ //Print "R_E_exc_eff ",R_E_exc_eff
+
+ T_Coll_Mode_0 = Max(T_Coll_Mode_0,T_Rusanov);
+ /* Transition vom const. temp. to Fermi gas occurs around 20 MeV by MAX function */
+ // T_Pol_Mode_0 = T_Pol_Red * T_Coll_Mode_0
+
+ // Application of the statistical model, intrinsic temperature at saddle
+ T_Pol_Mode_0 = U_Temp(0.5 * Csng(I_Z_CN),0.5 *Csng(I_A_CN), R_E_exc_eff, 0, 0, Tscale, Econd);
+ // T_asym_Mode_0 = Sqr(T_Coll_Mode_0^2 + (6E0*TCOLLMIN)^2)
+ T_asym_Mode_0 = sqrt(pow(T_Coll_Mode_0,2) + pow(1.0*TCOLLMIN,2));
+ //Print "4124: T_Coll_Mode_0"; T_Coll_Mode_0
+ //sleep
+
+ E_POT_SCISSION = (De_Saddle_Scission(pow(Csng(I_Z_CN),2) / pow(Csng(I_A_CN),0.33333),ESHIFTSASCI_intr) - E_tunn) + Epot_shift;
+ E_diss_Scission = EDISSFRAC * E_POT_SCISSION;
+ //Print "4054:";EDISSFRAC,E_POT_SCISSION,E_diss_Scission
+
+ /* Suppression of S1 fission channel at very low excitation energy at scission */
+ /* The idea behind is that the binding energy at scission is such that the
+ scission configuration cannot be reached with the available excitation energy. */
+ // EeffS1 = Max(E_Exc_S1,0.0) + EDISSFRAC * E_POT_SCISSION
+ // EeffS1 = Max(0.0,EeffS1)
+
+ // Print "4104", U_Mass(I_Z_CN,I_A_CN); _
+ // 2 * U_Mass(I_Z_CN/2.0,I_A_CN/2.0) + 1.44*(I_Z_CN/2.0)^2 / _
+ // (1.5 * ( (I_A_CN/2)^0.333333 + (I_A_CN/2)^0.333333) + DNECK ); EeffS1, _
+ // - 2 * U_Mass(I_Z_CN/2.0,I_A_CN/2.0) - 1.44*(I_Z_CN/2.0)^2 / _
+ // (1.5 * ( (I_A_CN/2)^0.333333 + (I_A_CN/2)^0.333333) + DNECK ) + _
+ // + Max(E_Exc_S1,0.0) + EDISSFRAC * E_POT_SCISSION _
+ // + U_Mass(I_Z_CN,I_A_CN)
+ // EeffS1 = - 2 * U_Mass(I_Z_CN/2.0,I_A_CN/2.0) - 1.44*(I_Z_CN/2.0)^2 / _
+ // (1.6 * ( (I_A_CN/2)^0.333333 + (I_A_CN/2)^0.333333) + DNECK ) + _
+ // Max(E_Exc_S1,0.0) + EDISSFRAC * E_POT_SCISSION _
+ // + U_Mass(I_Z_CN,I_A_CN)
+ // If EeffS1 < ETHRESHSUPPS1 Then
+ // + 2.E0 * ESIGSUPPS1 Then
+ // E_Exc_S1 = E_Exc_S1 + EeffS1 - ETHRESHSUPPS1
+ // 0.5E0 * 1.5 * 12.E0 / Sqr(132.E0) * Gaussintegral(ETHRESHSUPPS1 - EeffS1,ESIGSUPPS1)
+ //// 0.5E0 * 4.E0 * 12.E0 / Sqr(132.E0) * Gaussintegral(ETHRESHSUPPS1 - EeffS1,ESIGSUPPS1)
+ // End If
+ // If EeffS2 < ETHRESHSUPPS1 + 2.E0 * ESIGSUPPS1 Then
+ // E_Exc_S1 = E_Exc_S1 - _
+ // 0.5E0 * 1.5 * 12.E0 / Sqr(132.E0) * Gaussintegral(ETHRESHSUPPS1 - EeffS2,ESIGSUPPS1)
+ // 0.5E0 * 4.E0 * 12.E0 / Sqr(132.E0) * Gaussintegral(ETHRESHSUPPS1 - EeffS2,ESIGSUPPS1)
+ // EndIf
+
+ T_low_S1_used = T_low_S1;
+
+ T_Coll_Mode_1 = TFCOLL * Max(E_Exc_S1,0.) + TCOLLFRAC * (De_Saddle_Scission(pow(I_Z_CN,2) / pow(Csng(I_A_CN),0.33333),ESHIFTSASCI_coll) - E_tunn);
+ T_Coll_Mode_1 = Max(T_Coll_Mode_1,0.0);
+ // T_Pol_Mode_1 = T_Pol_Red * T_Coll_Mode_1
+ T_Pol_Mode_1 = T_Pol_Mode_0;
+ T_asym_Mode_1 = sqrt(pow(T_Coll_Mode_1,2) + pow(4.0*TCOLLMIN,2)); // TCOLLMIN for ZPM
+
+ T_Coll_Mode_2 = TFCOLL * Max(E_Exc_S2,0.) + TCOLLFRAC * (De_Saddle_Scission(pow(Csng(I_Z_CN),2) / pow(Csng(I_A_CN),0.33333),ESHIFTSASCI_coll) - E_tunn);
+ T_Coll_Mode_2 = Max(T_Coll_Mode_2,0.0);
+ // T_Pol_Mode_2 = T_Pol_Red * T_Coll_Mode_2
+ T_Pol_Mode_2 = T_Pol_Mode_0;
+ // T_asym_Mode_2 = Sqr(T_Coll_Mode_2^2 + TCOLLMIN^2)
+ T_asym_Mode_2 = sqrt(pow(T_Coll_Mode_2,2) + 4*pow(TCOLLMIN,2));
+
+ // Dim As Single T_asym_Mode_2_dyn // Collective dynamical effect ?
+ // T_asym_Mode_2_dyn = 0.009 * (I_Z_CN^2/(I_A_CN^0.333333) - 92.0^2/(238^0.333333) )
+ // T_asym_Mode_2 = Sqr(T_asym_Mode_2^2 + T_asym_Mode_2_dyn^2)
+
+ /* T_Coll_Mode_3 = TFCOLL * Max(E_Exc_S3,0.E0) + _
+ TCOLLFRAC * (De_Saddle_Scission(Csng(I_Z_CN)^2 / _
+ Csng(I_A_CN)^0.33333E0,ESHIFTSASCI_coll) - E_tunn)
+ Print 4954, TFCOLL * Max(E_Exc_S3,0.E0),TCOLLFRAC * (De_Saddle_Scission(Csng(I_Z_CN)^2 / _
+ Csng(I_A_CN)^0.33333E0,ESHIFTSASCI_coll) - E_tunn), _
+ TCOLLFRAC * (De_Saddle_Scission(Csng(I_Z_CN)^2 / _
+ Csng(I_A_CN)^0.33333E0,ESHIFTSASCI_coll) ),E_Exc_S3, _
+ TCOLLFRAC * 0.03 * (De_Saddle_Scission(Csng(I_Z_CN)^2 / _
+ Csng(I_A_CN)^0.33333E0,ESHIFTSASCI_coll) )^2
+ sleep */
+ //T_coll_Mode_3 = 0.2 // for 239Pu(nth,f)
+ //T_coll_Mode_3 = 0.7 // for 252Cf(sf)
+ // Fit to 239Pu(nth,f) and 252Cf(sf) ( unexpectedly large variation with Z^2/A^(1/3) )
+ T_Coll_Mode_3 = TFCOLL * Max(E_Exc_S3,0.) + TCOLLFRAC * 0.03 * pow(De_Saddle_Scission(pow(Csng(I_Z_CN),2)/pow(Csng(I_A_CN),0.33333),ESHIFTSASCI_coll),2);
+ T_Coll_Mode_3 = Max(T_Coll_Mode_3,0.0);
+ // T_Pol_Mode_3 = T_Pol_Red * T_Coll_Mode_3
+ T_Pol_Mode_3 = T_Pol_Mode_0;
+ T_asym_Mode_3 = sqrt(pow(T_Coll_Mode_3,2) + pow(TCOLLMIN,2)); //!!!
+ // Dim As Single T_asym_Mode_3_dyn
+ // Adjusted to the width of Mode 3 in 252Cf(sf)
+ // May be, this is a collective dynamic effect along the fission path
+ // T_asym_Mode_3_dyn = 0.009 * (I_Z_CN^2/(I_A_CN^0.333333) - 92.0^2/(238^0.333333) )
+ // T_asym_Mode_3_dyn = 0
+ // T_asym_Mode_3 = Max(T_asym_Mode_3,T_asym_Mode_3_dyn)
+ // T_asym_Mode_3 = Sqr(T_asym_Mode_3^2 + T_asym_Mode_3_dyn^2)
+
+ //Print "4619: ";T_Coll_Mode_3,TCOLLMIN,T_asym_Mode_3
+ //sleep
+
+ T_Coll_Mode_4 = TFCOLL * Max(E_Exc_S4,0.) + TCOLLFRAC * (De_Saddle_Scission(pow(Csng(I_Z_CN),2) / pow(Csng(I_A_CN),0.33333),ESHIFTSASCI_coll) - E_tunn);
+ T_Coll_Mode_4 = Max(T_Coll_Mode_4,0.0);
+ // T_Pol_Mode_4 = T_Pol_Red * T_Coll_Mode_4
+ T_Pol_Mode_4 = T_Pol_Mode_0;
+ T_asym_Mode_4 = sqrt(pow(T_Coll_Mode_4,2) + 4.0*pow(TCOLLMIN,2)); // ZPM like S1
+}
+
+void GEF::MeanValues_FM(void)
+{
+ /* Mean values and standard deviations of fission modes */
+ SigZ_Mode_0 = sqrt(0.5 * T_asym_Mode_0/R_Z_Curv_S0);
+ //Print "4214: SIGZ_Mode_0, T_asym_Mode_0, R_Z_Curv_S0)";SigZ_Mode_0,T_asym_Mode_0,R_Z_Curv_S0
+ //sleep
+ if(T_Pol_Mode_0 > 1.e-2)
+ Sigpol_Mode_0 = sqrt(0.25 * HOMPOL / R_Pol_Curv_S0 / Tanh(HOMPOL/(2. * T_Pol_Mode_0)));
+ else
+ Sigpol_Mode_0 = sqrt(0.25 * HOMPOL / R_Pol_Curv_S0);
+ /* including influence of zero-point motion */
+
+ R_E_intr_S1 = Max(E_Exc_S1+LyPair(I_Z_CN,I_A_CN),0.0);
+ R_Att[1] = exp(-R_E_intr_S1/Shell_fading);
+ R_Att[5] = R_Att[1];
+ R_Att_Sad[1] = exp(-R_E_intr_S1/Shell_fading);
+ R_Att_Sad[5] = R_Att_Sad[1];
+ SigZ_Mode_1 = sqrt(0.5 * T_asym_Mode_1/(P_Z_Curv_S1*sqrt(R_Att[1])));
+ if(T_Pol_Mode_1 > 1.e-2)
+ Sigpol_Mode_1 = sqrt(0.25 * HOMPOL / R_Pol_Curv_S1 / Tanh(HOMPOL/(2. * T_Pol_Mode_1)));
+ else
+ Sigpol_Mode_1 = sqrt(0.25 * HOMPOL / R_Pol_Curv_S1);
+
+ R_E_intr_S2 = Max(E_Exc_S2+LyPair(I_Z_CN,I_A_CN),0.0);
+ R_Att[2] = exp(-R_E_intr_S2/Shell_fading);
+ R_Att[6] = R_Att[2];
+ R_Att_Sad[2] = exp(-R_E_intr_S2/Shell_fading);
+ R_Att_Sad[6] = R_Att_Sad[2];
+ SigZ_Mode_2 = sqrt(0.5 * T_asym_Mode_2/(P_Z_Curv_S2*sqrt(R_Att[2])));
+ SigZ_SL4 = sqrt(0.5 * T_asym_Mode_2/(P_Z_Curv_SL4*sqrt(R_Att[2])));
+
+ if(T_Pol_Mode_2 > 1.e-2)
+ Sigpol_Mode_2 = sqrt(0.25 * HOMPOL / R_Pol_Curv_S2 / Tanh(HOMPOL/(2. * T_Pol_Mode_2)));
+ else
+ Sigpol_Mode_2 = sqrt(0.25 * HOMPOL / R_Pol_Curv_S2);
+
+ R_E_intr_S3 = Max(E_Exc_S3+LyPair(I_Z_CN,I_A_CN),0.0);
+ R_Att[3] = exp(-R_E_intr_S3/Shell_fading);
+ R_Att_Sad[3] = exp(-R_E_intr_S3/Shell_fading);
+ SigZ_Mode_3 = sqrt(0.5 * T_asym_Mode_3/(P_Z_Curv_S3*sqrt(R_Att[3])));
+ if(T_Pol_Mode_3 > 1.e-2)
+ Sigpol_Mode_3 = sqrt(0.25 * HOMPOL / R_Pol_Curv_S3 / Tanh(HOMPOL/(2. * T_Pol_Mode_3)));
+ else
+ Sigpol_Mode_3 = sqrt(0.25 * HOMPOL / R_Pol_Curv_S3);
+
+ R_E_intr_S4 = Max(E_Exc_S4+LyPair(I_Z_CN,I_A_CN),0.0);
+ R_Att[4] = exp(-R_E_intr_S4/Shell_fading);
+ R_Att_Sad[4] = exp(-R_E_intr_S4/Shell_fading);
+ SigZ_Mode_4 = sqrt(0.5 * T_asym_Mode_4/(P_Z_Curv_S4*sqrt(R_Att[4])));
+ if(T_Pol_Mode_4 > 1.e-2)
+ Sigpol_Mode_4 = sqrt(0.25 * HOMPOL / R_Pol_Curv_S4 /Tanh(HOMPOL/(2. * T_Pol_Mode_4)));
+ else
+ Sigpol_Mode_4 = sqrt(0.25 * HOMPOL / R_Pol_Curv_S4);
+}
+
+void GEF::EnergyDependence(void)
+{
+ /* Energy-dependent shift of fission channels */
+ float DZ_S1,DZ_S2,DZ_S3,DZ_S4;
+ float EtotS0, EtotS2;
+ float P_Z_Curv_S1_eff;
+ P_Z_Curv_S1_eff = P_Z_Curv_S1 * P_Z_Curvmod_S1;
+ float P_Z_Curv_S2_eff;
+ P_Z_Curv_S2_eff = P_Z_Curv_S2 * P_Z_Curvmod_S2;
+ float P_Z_Curv_S3_eff;
+ P_Z_Curv_S3_eff = P_Z_Curv_S3 * P_Z_Curvmod_S3;
+ float P_Z_Curv_S4_eff;
+ P_Z_Curv_S4_eff = P_Z_Curv_S4 * P_Z_Curvmod_S4;
+
+ DZ_S1 = P_Z_Mean_S1 *
+ (P_Z_Curv_S1_eff*R_Att[1] / (R_Z_Curv_S0 + P_Z_Curv_S1_eff*R_Att[1])
+ - (P_Z_Curv_S1_eff / (R_Z_Curv_S0 + P_Z_Curv_S1_eff) ) );
+ DZ_S2 = P_Z_Mean_S2 *
+ (P_Z_Curv_S2_eff*R_Att[2] / (R_Z_Curv_S0 + P_Z_Curv_S2_eff*R_Att[2])
+ - (P_Z_Curv_S2_eff / (R_Z_Curv_S0 + P_Z_Curv_S2_eff) ) );
+ DZ_S3 = P_Z_Mean_S3 *
+ (P_Z_Curv_S3_eff*R_Att[3] / (R_Z_Curv_S0 + P_Z_Curv_S3_eff*R_Att[3])
+ - (P_Z_Curv_S3_eff / (R_Z_Curv_S0 + P_Z_Curv_S3_eff) ) );
+ DZ_S4 = Sgn(P_Z_Mean_S4 - P_Z_Mean_S0) * P_Z_Mean_S4 *
+ (P_Z_Curv_S4_eff*R_Att[4] / (R_Z_Curv_S0 + P_Z_Curv_S4_eff*R_Att[4])
+ - (P_Z_Curv_S4_eff / (R_Z_Curv_S0 + P_Z_Curv_S4_eff) ) ) ;
+
+ // Empirical shift of S2 channel at low excitation energy at scission
+ // for better reproduction of 238U(s,f) and some data for Th isotopes.
+ // Does not solve the problem of 229Th(nth,f).
+ // EtotS2 = Max(E_Exc_S2 + E_diss_Scission,0.0)
+ // If EtotS2 < 5.E0 Then
+ // DZ_S2 = DZ_S2 + (5.E0 - EtotS2) * 0.1
+ // End If
+
+ // DZ_S1 = 0
+ // DZ_S2 = 0
+ // DZ_S3 = 0
+ // DZ_S4 = 0
+
+ ZC_Mode_0 = P_Z_Mean_S0;
+ ZC_Mode_1 = P_Z_Mean_S1 + DZ_S1;
+ ZC_Mode_2 = P_Z_Mean_S2 + DZ_S2;
+ ZC_Mode_3 = P_Z_Mean_S3 + DZ_S3;
+ // ZC_Mode_4 = P_Z_Mean_S4 + DZ_S4
+ // shift is very small, because S4 exists only close to symmetry
+ ZC_Mode_4 = P_Z_Mean_S4;
+
+ /* Energy dependence of charge polarization */
+ /* Due to washing out of shells */
+
+ for(int I = 10;I<=(I_A_CN - 10);I++) // mass number
+ for(int J = 1;J<=4;J++) // fission channel
+ for(int K = 1;K<=2;K++) // light - heavy group
+ Zshift[J][K][I] = ZshiftOriginal[0][K][I] + (ZshiftOriginal[J][K][I] - ZshiftOriginal[0][K][I])*R_Att[J];
+
+ /* Energy dependence of shell-induced deformation */
+ /* Due to washing out of shells */
+ /* (Under development) */
+ /*For I = 10 To I_Z_CN - 10 // mass number
+ For J = 1 To 4 // fission channel
+ For K = 1 To 2 // light - heavy group
+ beta(J,K,I) = beta(0,K,I) + (beta(J,K,I) - beta(0,K,I))*R_Att_Sad(J)
+ if beta(J,K,I) < 0 Then
+ beta(J,K,I) = 0
+ End If
+ Z1 = I
+ Z2 = I_Z_CN - Z1
+ A1 = Z1 / Csng(I_Z_CN) * Csng(I_A_CN)
+ A2 = I_A_CN - A1
+ E_defo = Lymass(Z1,A1,beta(J,K,I)) - Lymass(Z1,A1,0.0)
+ Edefo(J,K,I) = E_defo
+ Next
+ Next
+ Next */
+}
+
+void GEF::Yields_FM(void)
+{
+ // Yield_Mode_0 = Getyield(E_Exc_S0,E_Exc_S0,T_low_SL,TEgidy(Csng(I_A_CN),0.E0,Tscale))
+ Yield_Mode_0 = Getyield(E_Exc_S0,E_Exc_S0,T_low_SL,TEgidy(Csng(I_A_CN),Delta_S0,Tscale));
+ Yield_Mode_1 = Getyield(E_Exc_S1,E_Exc_S0,T_low_S1_used,TEgidy(Csng(I_A_CN),R_Shell_S1_eff + dE_Defo_S1,Tscale));
+ /* - Getyield(E_Exc_S0 - E_ld_S1,T_low,T_high) */
+ Yield_Mode_2 = Getyield(E_Exc_S2,E_Exc_S0,T_low_S2,TEgidy(Csng(I_A_CN),R_Shell_S2_eff + dE_Defo_S2,Tscale));
+ /* - Getyield(E_Exc_S0 - E_ld_S2,T_low,T_high) */
+ Yield_Mode_3 = Getyield(E_Exc_S3,E_Exc_S0,T_low_S3,TEgidy(Csng(I_A_CN),R_Shell_S3_eff + dE_Defo_S3,Tscale));
+ /* - Getyield(E_Exc_S0 - E_ld_S3,T_low,T_high) */
+ Yield_Mode_4 = Getyield(E_Exc_S4,E_Exc_S0,T_low_S4,TEgidy(Csng(I_A_CN),R_Shell_S4_eff + dE_Defo_S4,Tscale));
+ /* - Getyield(E_Exc_S0 - E_ld_S4,T_low,T_high) */
+ //Print TEgidy(Csng(I_A_CN),0.E0,Tscale), TEgidy(Csng(I_A_CN),R_Shell_S2_eff + dE_Defo_S2,Tscale), de_Defo_S2
+ //sleep
+ if(B_S11 > B_S1)
+ Yield_Mode_11 = 0.0;
+ else
+ Yield_Mode_11 = Getyield(E_Exc_S11,E_Exc_S0, T_low_S11,TEgidy(Csng(I_A_CN),R_Shell_S1_eff + 2.* dE_Defo_S1,Tscale));
+ if(B_S22 > B_S2)
+ Yield_Mode_22 = 0.0;
+ else
+ Yield_Mode_22 = Getyield(E_Exc_S22,E_Exc_S0, T_low_S2, TEgidy(Csng(I_A_CN),R_Shell_S2_eff,Tscale));
+ Yield_Norm = Yield_Mode_0 + Yield_Mode_1 + Yield_Mode_2 + Yield_Mode_3 + Yield_Mode_4 + Yield_Mode_11 + Yield_Mode_22;
+ Yield_Mode_0 = Yield_Mode_0 / Yield_Norm;
+ Yield_Mode_1 = Yield_Mode_1 / Yield_Norm;
+ Yield_Mode_2 = Yield_Mode_2 / Yield_Norm;
+ Yield_Mode_3 = Yield_Mode_3 / Yield_Norm;
+ Yield_Mode_4 = Yield_Mode_4 / Yield_Norm;
+ Yield_Mode_11 = Yield_Mode_11 / Yield_Norm;
+ Yield_Mode_22 = Yield_Mode_22 / Yield_Norm;
+ //cout<< B_S11<<" "<<B_S1<<" "<<E_Exc_S0<<"-- "<<Yield_Mode_0<<" "<<Yield_Mode_1<<" "<<Yield_Mode_2<<" "<<Yield_Mode_3<<" "<<Yield_Mode_4<<" "<<Yield_Mode_11<<" "<<Yield_Mode_22<<endl;
+}
+
+void GEF::MassWidths_FM(void)
+{
+ SigA_Mode_0 = SigZ_Mode_0 * Csng(I_A_CN) / Csng(I_Z_CN); /* width in mass */
+ SigA_Mode_1 = SigZ_Mode_1 * Csng(I_A_CN) / Csng(I_Z_CN);
+ SigA_Mode_1 = Min(SigA_Mode_1,SigA_Mode_0); // not broader than liquid-drop
+ SigA_Mode_2 = SigZ_Mode_2 * Csng(I_A_CN) / Csng(I_Z_CN);
+ SigA_Mode_2 = Min(SigA_Mode_2,SigA_Mode_0); // not broader than liquid-drop
+ SigA_Mode_3 = SigZ_Mode_3 * Csng(I_A_CN) / Csng(I_Z_CN);
+ SigA_Mode_3 = Min(SigA_Mode_3,SigA_Mode_0);
+ SigA_Mode_4 = SigZ_Mode_4 * Csng(I_A_CN) / Csng(I_Z_CN);
+ SigA_Mode_4 = Min(SigA_Mode_4,SigA_Mode_0);
+ SigA_Mode_11 = SigZ_Mode_1 * sqrt(2.E0) * Csng(I_A_CN) / Csng(I_Z_CN);
+ SigA_Mode_11 = Min(SigA_Mode_11,SigA_Mode_0);
+ SigA_Mode_22 = SigZ_Mode_2 * sqrt(2.E0) * Csng(I_A_CN) / Csng(I_Z_CN);
+ SigA_Mode_22 = Min(SigA_Mode_22,SigA_Mode_0);
+}
+
+void GEF::ShellEff_FM(void)
+{
+ /* This is the "real" microscopic shell effect, not the effective shell-correction energy */
+ /* EShell acts on the level density and determines the T parameter */
+ for(int I = 1;I<=(I_A_CN - 1);I++)
+ {
+ for(int J = 0;J<= 4;J++)
+ EShell[J][1][I] = 0; /* Shells in "light" fragment assumed to be zero */
+ DU0 = 0;
+ EShell[0][2][I] = 0; /* Shell = 0 in symmetric mode */
+ DU1 = R_Shell_S1_eff + dE_Defo_S1; /* + R_A_Curv1_S1 * (AC_Mode_1 - Float(I,6))**2; */
+ DU1 = Min(DU1,0.); /* Technical limit */
+ EShell[1][2][I] = DU1;
+ DU2 = R_Shell_S2_eff + dE_Defo_S2; /* + R_A_Curv1_S2 * (AC_Mode_2 - Float(I,6))**2; */
+ DU2 = Min(DU2,0.); /* Technical limit */
+ EShell[2][2][I] = DU2;
+ DU3 = R_Shell_S3_eff + dE_Defo_S3; /* + R_A_Curv1_S3 * (AC_Mode_3 - Float(I,6))**2; */
+ DU3 = Min(DU3,0.); /* Technical limit */
+ EShell[3][2][I] = DU3;
+ DU4 = R_Shell_S4_eff + dE_Defo_S4; /* + R_A_Curv1_S4 * (AC_Mode_4 - Float(I,6))**2; */
+ DU4 = Min(DU4,0.); /* Technical limit */
+ EShell[4][2][I] = DU4;
+ }
+}
+
+void GEF::IntrinsicT(void)
+{
+ /* Intrinsic temperatures of fragments at scission */
+ /* Mean values */
+ T_intr_Mode_0 = TEgidy(AC_Mode_0,0.0,0.8);
+ T_intr_Mode_1_heavy = TEgidy(AC_Mode_1,R_Shell_S1_eff + dE_Defo_S1,Tscale);
+ T_intr_Mode_1_light = TEgidy(Csng(I_A_CN) - AC_Mode_1,0.0,Tscale);
+ T_intr_Mode_2_heavy = TEgidy(AC_Mode_2,R_Shell_S2_eff + dE_Defo_S2,Tscale);
+ T_intr_Mode_2_light = TEgidy(Csng(I_A_CN) - AC_Mode_2,0.0,Tscale);
+ T_intr_Mode_3_heavy = TEgidy(AC_Mode_3,R_Shell_S3_eff + dE_Defo_S3,Tscale);
+ T_intr_Mode_3_light = TEgidy(Csng(I_A_CN) - AC_Mode_3,0.0,Tscale);
+ T_intr_Mode_4_heavy = TEgidy(AC_Mode_4,R_Shell_S4_eff + dE_Defo_S4,Tscale);
+ T_intr_Mode_4_light = TEgidy(Csng(I_A_CN) - AC_Mode_4,0.0,Tscale);
+
+ /* Mass-dependent values of individual fragments */
+ /* Mode 0 */
+ for(int I = 1;I<=(I_A_CN - 1);I++)
+ {
+ T = TEgidy(Csng(I),EShell[0][1][I],Tscale);
+ Temp[0][1][I] = T; /* "light" fragment at freeze-out (somewhere before scission) */
+ T = TEgidy(Csng(I),EShell[0][2][I],Tscale);
+ Temp[0][2][I] = T; /* "heavy" fragment at freeze-out (somewhere before scission) */
+
+ T = TEgidy(Csng(I),0.0,1.0);
+ TempFF[0][1][I] = T; // FF in their ground state
+ TempFF[0][2][I] = T; // FF in their ground state
+ }
+ /* Mode 1 */
+ for(int I = 1;I<=(I_A_CN - 1);I++)
+ {
+ T = TEgidy(Csng(I),EShell[1][1][I],Tscale);
+ Temp[1][1][I] = T; /* "light" fragment */
+ T = TEgidy(Csng(I),EShell[1][2][I],Tscale);
+ Temp[1][2][I] = T; /* "heavy" fragment */
+
+ T = TEgidy(Csng(I),0.0,1.0);
+ TempFF[1][1][I] = T; // FF in their ground state
+ TempFF[1][2][I] = T; // FF in their ground state
+ }
+ /* Mode 2 */
+ for(int I = 1;I<=(I_A_CN - 1);I++)
+ {
+ T = TEgidy(Csng(I),EShell[2][1][I],Tscale);
+ Temp[2][1][I] = T; /* "light" fragment */
+ T = TEgidy(Csng(I),EShell[2][2][I],Tscale);
+ Temp[2][2][I] = T; /* "heavy" fragment */
+ /* The next section is introduced, because energy sorting is not strong enough,
+ when shells are only introduced in the heavy fragment.
+ Ad hoc assumption: For Mode 2 there are shells in both fragments of about
+ equal size. Technically, we neglect the shells in both fragments.
+ This has about the same effect for the energy sorting. */
+ T = TEgidy(Csng(I),0.0,Tscale); // FF at scssion
+ Temp[2][1][I] = T; /* "light" fragment */
+ T = TEgidy(Csng(I),0.0,Tscale); // FF at scission
+ Temp[2][2][I] = T; /* "heavy" fragment */
+
+ T = TEgidy(Csng(I),0.0,1.0); // shell effect neglected
+ TempFF[2][1][I] = T; // FFs in their ground state
+ TempFF[2][2][I] = T; // FFs in their ground state
+ }
+ /* Mode 3 */
+ for(int I = 1;I<=(I_A_CN -1);I++)
+ {
+ T = TEgidy(Csng(I),0.0,Tscale);
+ Temp[3][1][I] = T;
+ T = TEgidy(Csng(I),0.0,Tscale);
+ Temp[3][2][I] = T;
+
+ T = TEgidy(Csng(I),0.0,1.0);
+ TempFF[3][1][I] = T; // FF in their ground state
+ TempFF[3][2][I] = T; // FF in their ground state
+ }
+ /* Mode 4 */
+ for(int I = 1;I<=(I_A_CN -1);I++)
+ {
+ T = TEgidy(Csng(I),0.0,Tscale);
+ Temp[4][1][I] = T;
+ T = TEgidy(Csng(I),0.0,Tscale);
+ Temp[4][2][I] = T;
+
+ T = TEgidy(Csng(I),0.0,1.0);
+ TempFF[4][1][I] = T; // FF in their ground state
+ TempFF[4][2][I] = T ; // FF in their ground state
+ }
+}
+
+void GEF::IntrinsicEx(void)
+{
+ /*** Intrinsic excitation energy at saddle and at scission as well as ***/
+ /*** Even-odd effect in proton and neutron number for each fission mode ***/
+ for(I_Mode = 0; I_Mode<=6;I_Mode++)
+ {
+ E_coll_saddle[I_Mode] = 0;
+ if(I_Mode == 0) Etot = E_Exc_S0;
+ if(I_Mode == 1) Etot = E_Exc_S1;
+ if(I_Mode == 2) Etot = E_Exc_S2;
+ if(I_Mode == 3) Etot = E_Exc_S3;
+ if(I_Mode == 4) Etot = E_Exc_S4;
+ if(I_Mode == 5) Etot = E_Exc_S11;
+ if(I_Mode == 6) Etot = E_Exc_S22;
+
+ if(( Mod(I_Z_CN,2) + Mod(I_N_CN,2)) == 0) /* Even-even CN */
+ if(Etot > 0 && Etot < (2. * 14./sqrt(Csng(I_A_CN))) )
+ {
+ E_coll_saddle[I_Mode] = Etot;
+ Etot = 0;
+ /* Excitation below the pairing gap in even-even CN goes into collective excitations */
+ }
+ // If I_Z_CN Mod 2 + I_N_CN Mod 2 = 0 Then // even-even
+ // Ediff = Min(Etot, 14.0/sqr(Csng(I_A_CN)))
+ // End If
+ // If I_Z_CN Mod 2 + I_N_CN Mod 2 = 1 Then // even-odd or odd-even
+ // Ediff = Min(Etot, 2.0 * 14.0/sqr(Csng(I_A_CN)))
+ // End If
+ // Ediff = Max(Ediff,0.0)
+ // Etot = Etot - Ediff
+ if(Etot < 0)
+ E_tunn = -Etot;
+ else
+ E_tunn = 0;
+ Etot = Max(Etot,0.0);
+ E_POT_SCISSION = (De_Saddle_Scission(pow(Csng(I_Z_CN),2) / pow(Csng(I_A_CN),0.33333),ESHIFTSASCI_intr) ) ;
+ E_diss_Scission = EDISSFRAC * (E_POT_SCISSION - E_tunn) + Epot_shift ;
+ if(E_diss_Scission < 0)
+ E_diss_Scission = 0;
+ Etot = Etot + E_diss_Scission;
+ /* All excitation energy at saddle and part of the potential-energy gain to scission
+ go into intrinsic excitation energy at scission */
+ if(I_Mode == 2)
+ EINTR_SCISSION = Etot; /* (For Mode 2) Global parameter */
+
+ for(IA1 = 40;IA1<=(I_A_CN - 40);IA1++)
+ {
+ IA2 = I_A_CN - IA1;
+ if(I_Mode <= 4)
+ {
+ T1 = Temp[I_Mode][1][IA1];
+ T2 = Temp[I_Mode][2][IA2];
+ }
+ if(I_Mode == 5)
+ {
+ T1 = Temp[1][2][IA1];
+ T2 = Temp[1][2][IA2];
+ }
+ if(I_Mode == 6)
+ {
+ T1 = Temp[2][2][IA1];
+ T2 = Temp[2][2][IA2];
+ }
+ DT = abs(T2 - T1);
+
+ /* Even-odd effect */
+ if(Mod(I_Z_CN,2) == 0)
+ Rincr1P = exp(-Etot/PZ_EO_symm);
+ else
+ Rincr1P = 0;
+ if( Mod(I_N_CN,2) == 0)
+ Rincr1N = exp(-Etot/PN_EO_Symm);
+ else
+ Rincr1N = 0;
+
+ PEOZ[I_Mode][1][IA1] = Rincr1P;
+ PEOZ[I_Mode][2][IA2] = Rincr1P;
+ PEON[I_Mode][1][IA1] = Rincr1N;
+ PEON[I_Mode][2][IA2] = Rincr1N;
+
+ if(Etot > 0)
+ Rincr2 = Gaussintegral(DT/Etot-R_EO_THRESH,R_EO_SIGMA*(DT+0.0001));
+ /* even-odd effect due to asymmetry */
+ else // even-odd effect is already 100%
+ Rincr2 = 0;
+ Rincr2P = (R_EO_MAX - Rincr1P) * Rincr2;
+ Rincr2N = (R_EO_MAX - Rincr1N) * Rincr2;
+
+ if(IA1 <= IA2) // A1 is lighter or equal to A2
+ {
+ PEOZ[I_Mode][1][IA1] = PEOZ[I_Mode][1][IA1] + Rincr2P;
+ if(Mod(I_Z_CN,2) == 0)
+ PEOZ[I_Mode][2][IA2] = PEOZ[I_Mode][2][IA2] + Rincr2P;
+ else
+ PEOZ[I_Mode][2][IA2] = PEOZ[I_Mode][2][IA2] - Rincr2P;
+ PEON[I_Mode][1][IA1] = PEON[I_Mode][1][IA1] + Rincr2N;
+ if(Mod(I_N_CN,2) == 0)
+ PEON[I_Mode][2][IA2] = PEON[I_Mode][2][IA2] + Rincr2N;
+ else
+ PEON[I_Mode][2][IA2] = PEON[I_Mode][2][IA2] - Rincr2N;
+ }
+ else
+ {
+ PEOZ[I_Mode][1][IA1] = PEOZ[I_Mode][2][IA1];
+ PEON[I_Mode][1][IA1] = PEON[I_Mode][2][IA1];
+ PEOZ[I_Mode][2][IA2] = PEOZ[I_Mode][1][IA2];
+ PEON[I_Mode][2][IA2] = PEON[I_Mode][1][IA2];
+ }
+ /* Else
+ PEOZ(I_Mode,2,IA2) = _
+ PEOZ(I_Mode,1,IA2) + Rincr2P
+ IF I_Z_CN Mod 2 = 0 Then
+ PEOZ(I_Mode,1,IA1) = _
+ PEOZ(I_Mode,1,IA1) + Rincr2P
+ Else
+ PEOZ(I_Mode,1,IA1) = _
+ PEOZ(I_Mode,1,IA1) - Rincr2P
+ End if
+ PEON(I_Mode,2,IA2) = _
+ PEON(I_Mode,2,IA2) + Rincr2N
+ IF I_N_CN Mod 1 = 0 Then
+ PEON(I_Mode,1,IA1) = _
+ PEON(I_Mode,1,IA1) + Rincr2N
+ Else
+ PEON(I_Mode,1,IA1) = _
+ PEON(I_Mode,1,IA1) - Rincr2N
+ End if
+ End If */
+ PEOZ[I_Mode][1][IA1] = PEOZ[I_Mode][1][IA1] * EOscale;
+ PEOZ[I_Mode][2][IA2] = PEOZ[I_Mode][2][IA2] * EOscale;
+ PEON[I_Mode][1][IA1] = PEON[I_Mode][1][IA1] * EOscale;
+ PEON[I_Mode][2][IA2] = PEON[I_Mode][2][IA2] * EOscale;
+
+ /* For T1 = 0.5 To 1 Step 0.05
+ T2 = 1 - T1
+ Print T1,T2, 1.E - Gaussintegral(T2-T1,0.1)
+ Next T1
+ Sleep */
+
+ /* Energy sorting */
+ /* E1 = Etot * Gaussintegral(T2-T1,0.03); */
+ if(abs(T1-T2) < 1.e-6)
+ E1 = 0.5E0 * Etot;
+ else
+ {
+ // E1ES = Csort * T1 * T2 / ( Abs(T1 - T2) )
+ if(I_Mode == 0)
+ E1ES = Etot * Gaussintegral(T2-T1,Esort_slope_S0);
+ else
+ E1ES = Etot * Gaussintegral(T2-T1,Esort_slope);
+ E1ES = Min(E1ES,0.5E0*Etot);
+ /* Asymptotic value after "complete" energy sorting */
+ E1FG = Etot * IA1 / I_A_CN; /* in Fermi-gas regime */
+
+ /* The following section assumes T=const in the superfluid regime
+ If Etot < 13 Then E1 = E1ES // complete energy sorting
+ If Etot >= 13 and Etot <= 20 Then // transition region
+ E1 = E1ES + (Etot-13)/7*(E1FG-E1ES)
+ End If
+ If Etot > 20 Then E1 = E1FG // Fermi-gas regime */
+
+ /* The following section extends energy sorting to higher energies */
+ if(Etot < 13 * Esort_extend) // complete energy sorting
+ E1 = E1ES;
+ else if(Etot >= 13 * Esort_extend && Etot <= 20 * Esort_extend) // transition region
+ E1 = E1ES + (Etot-13 * Esort_extend)/7*(E1FG-E1ES);
+ else if(Etot > 20 * Esort_extend)
+ E1 = E1FG; // Fermi-gas regime */
+ }
+ E2 = Etot - E1;
+ EPART[I_Mode][1][IA1] = Max(E1,0.0); /* Mean E* in light fragment */
+ EPART[I_Mode][2][IA2] = Max(E2,0.0); /* Mean E* in heavy fragment */
+ }
+ }
+}
+
+void GEF::FF_angularMomentum(void)
+{
+ // RMS angular momentum of fission fragments
+ // Following Naik et al., EPJ A 31 (2007) 195 and
+ // S. G. Kadmensky, Phys. At. Nucl. 71 (2008) 1193
+
+ float AUCD; // UCD fragment mass
+ float I_rigid_spher; // I rigid for spherical shape
+ float I_rigid; // I rigid for deformed scission shape
+ float I_eff; // I with reduction due to pairing
+ float alph; // deformation parameter
+ float E_exc; // Excitation energy
+ float J_rms; // rms angular momentum
+ int ZT,AT; // Z and A of target nucleus
+ float I_ISO; // ISO number
+
+ // CN spin
+ ZT = P_Z_CN;
+ // AT = I_A_CN
+ AT = P_A_CN;
+ if(Emode == 2)
+ AT = P_A_CN -1;
+ if(Emode == 12)
+ {
+ AT = P_A_CN -1;
+ ZT = P_Z_CN -1;
+ }
+
+ // Spin_CN = P_J_CN
+ // P_I_rms_CN = P_J_CN
+
+ int I_E_iso=0; //Only Ground STATE
+ if(I_E_iso == 0) // fissioning nucleus or target in ground state
+ {
+ if(P_I_rms_CN == 0)
+ {
+ if(AT == 0)
+ Spin_CN = 0;
+ else
+ Spin_CN = R_SPI[ZT][AT];
+ }
+ else
+ Spin_CN = P_I_rms_CN;
+ }
+ /*
+ else // fissioning nucleus or target in isomeric state
+ {
+ if (N_ISO_MAT(I_MAT) < I_E_iso) //??????????????????
+ {
+ cout<<"The isomer is not in the table of nuclear properties."<<endl;
+ cout<<"Z, A, #iso "<<ZT<<" "<<AT<<" "<<I_E_iso<<endl;
+ cout<< "Please restart GEF."<<endl;
+ }
+ Spin_CN = NucTab(I_MAT + I_E_iso).R_SPI; //??????????????????
+ }*/
+
+ // Print "ZT, AT, I_MAT",ZT, AT, I_MAT
+ // Print "SPIN_CN",Spin_CN
+ // Sleep
+ Spin_pre_fission = Spin_CN; // target or CN ground-state spin
+ // Incoming neutron (spin + orbital)
+ if(Emode == 2)
+ // 2/3 * 1.16 * sqr(2 * 939.65) / 197.33 = 0.1699
+ if(R_E_exc_used > 0)
+ Spin_pre_fission = sqrt(pow(Spin_CN,2) + pow(0.5,2) + pow(0.1699 * pow(AT,0.333333) * sqrt(R_E_exc_used),2));
+ if(Emode == 12) // preliminary (because Coulomb barrier neglected)
+ if(R_E_exc_used > 0)
+ Spin_pre_fission = sqrt(pow(Spin_CN,2) + pow(0.5,2) + pow(0.1699 * pow(AT,0.333333) * sqrt(R_E_exc_used),2));
+
+ for(IZ1 = 10;IZ1<=(I_Z_CN - 10);IZ1++)
+ {
+ AUCD = CInt(Csng(IZ1) * Csng(I_A_CN) / Csng(I_Z_CN));
+ for(IA1 = CInt(AUCD - 15);IA1<= CInt(AUCD + 15);IA1++)
+ {
+ IN1 = IA1 - IZ1;
+ if(IA1 - IZ1 >= 10)
+ {
+ // Rigid momentum of inertia for spherical nucleus
+ I_rigid_spher = pow(1.16,2) * pow(Csng(IA1),1.6667) / 103.8415;
+ // unit: hbar^2/MeV
+ for(I_Mode = 0;I_Mode<=6;I_Mode++)
+ {
+ // First (normally light) fission fragment:
+ beta1 = Beta[I_Mode+1][1][IZ1]; //I_Mode+1 because there is I_Mode = -1 for Beta[][][]
+ alph = beta1 / sqrt(4. * pi / 5.);
+ I_rigid = I_rigid_spher * (1. + 0.5*alph + 9./7.*pow(alph,2));
+ // From Hasse & Myers, Geometrical Relationships ...
+ E_exc = EPART[I_Mode][1][IA1];
+ if(E_exc < 0)
+ E_exc = 0;
+ T = U_Temp(Csng(IZ1),Csng(IA1),E_exc,1,1,Tscale,Econd);
+ // T = sqr(T^2 + 0.8^2) // For ZPM
+ // T = T_orbital
+ // T = sqr(T^2 + T_orbital^2)
+ if(T_orbital > 0.1)
+ T = T_orbital / Tanh(T_orbital/T); // T_orbital represents the ZPM
+
+ I_eff = I_rigid * (1. - 0.8 * exp(-0.693 * E_exc / 5.));
+ J_rms = sqrt(2. * I_eff * T);
+
+ J_rms = J_rms * Jscaling;
+
+ if((Mod(IZ1,2) == 1) | (Mod(IN1,2) == 1) )
+ J_rms = J_rms + Spin_odd * pow(Csng(IA1)/140.0,0.66667);
+ // Max(0,1 - (E_exc-1)/9) // empirical
+ // Additional angular momentum of unpaired proton.
+ // See also Tomar et al., Pramana 68 (2007) 111
+
+ // Print Z1,I_Mode,beta1,T,E_exc,Spin_CN
+ // Print " ",I_rigid_spher,I_rigid,I_eff,J_rms
+
+ J_rms = sqrt(pow(J_rms,2) + pow(IA1/I_A_CN * Spin_pre_fission,2));
+
+ SpinRMSNZ[I_Mode][1][IA1-IZ1][IZ1] = J_rms;
+
+ // Print
+ // Print IA1,T,E_exc,I_rigid_spher,I_rigid,I_eff,J_rms
+
+ // Second (normally heavy) fission fragment:
+
+ beta2 = Beta[I_Mode+1][2][IZ1];
+ alph = beta2 / sqrt(4. * pi / 5.);
+ I_rigid = I_rigid_spher * (1. + 0.5*alph + 9./7.*pow(alph,2));
+ // From Hasse & Myers, Geometrical Relationships ...
+ E_exc = EPART[I_Mode][2][IA1];
+ if(E_exc < 0)
+ E_exc = 0;
+ T = U_Temp(Csng(IZ1),Csng(IA1),E_exc,1,1,Tscale,Econd);
+ // T = sqr(T^2 + 0.8^2) // For ZPM
+ // T = T_orbital
+ // T = sqr(T^2 + T_orbital^2)
+ if(T_orbital > 0.1)
+ T = T_orbital / Tanh(T_orbital/T); // T_orbital represents the ZPM
+ I_eff = I_rigid * (1. - 0.8 * exp(-0.693 * E_exc / 5.));
+ J_rms = sqrt(2. * I_eff * T);
+
+ J_rms = J_rms * Jscaling;
+
+ if((Mod(IZ1,2) == 1) | (Mod(IN1,2)== 1))
+ J_rms = J_rms + Spin_odd * pow(Csng(IA1)/140.0,0.66667);
+ // Max(0,1 - (E_exc-1)/9) // empirical
+ // Additional angular momentum of unpaired proton.
+ // See also Tomar et al., Pramana 68 (2007) 111
+
+ J_rms = sqrt(pow(J_rms,2) + pow(IA1/I_A_CN * Spin_pre_fission,2));
+
+ SpinRMSNZ[I_Mode][2][IA1-IZ1][IZ1] = J_rms;
+
+ // Print IA1,T,E_exc,I_rigid_spher,I_rigid,I_eff,J_rms
+
+ }
+ }
+ }
+ }
+}
+
+
+void GEF::FissionModeChoise(void)
+{
+ /* Chosing fission mode*/
+ float R_Sum_0,R_Sum_1,R_Sum_2,R_Sum_3,R_Sum_4,R_Sum_5,R_Sum_6;
+ float R_Choice,Rincr;
+ R_Choice = rn->Rndm();
+ R_Sum_0 = Yield_Mode_0;
+ R_Sum_1 = R_Sum_0 + Yield_Mode_1;
+ R_Sum_2 = R_Sum_1 + Yield_Mode_2;
+ R_Sum_3 = R_Sum_2 + Yield_Mode_3;
+ R_Sum_4 = R_Sum_3 + Yield_Mode_4;
+ R_Sum_5 = R_Sum_4 + Yield_Mode_11;
+ R_Sum_6 = R_Sum_5 + Yield_Mode_22;
+ I_Mode = 6;
+ if(R_Choice < R_Sum_0) I_Mode = 0;
+ if(R_Choice >= R_Sum_0 && R_Choice < R_Sum_1) I_Mode = 1;
+ if(R_Choice >= R_Sum_1 && R_Choice < R_Sum_2) I_Mode = 2;
+ if(R_Choice >= R_Sum_2 && R_Choice < R_Sum_3) I_Mode = 3;
+ if(R_Choice >= R_Sum_3 && R_Choice < R_Sum_4) I_Mode = 4;
+ if(R_Choice >= R_Sum_4 && R_Choice < R_Sum_5) I_Mode = 5;
+ if(R_Choice >= R_Sum_5 && R_Choice < R_Sum_6) I_Mode = 6;
+ // Mode_Events(I_Mode) = Mode_Events(I_Mode) + 1
+ // Mode_Events(10) = Mode_Events(10) + 1 //For normalization
+}
+
+void GEF::ZAChoise(void)
+{
+ bool DiceA=true;
+ while(DiceA)
+ {
+ DiceA = false;
+ switch(I_Mode)
+ {
+ case 0:
+ {
+ R_A_heavy = PGauss(AC_Mode_0,SigA_Mode_0); /* random choice of mass */
+ RZpol = Zshift[0][2][CInt(R_A_heavy)]; /* local polarization */
+ RZ = R_A_heavy * I_Z_CN / I_A_CN + RZpol; /* mean position in Z for given mass */
+ R_Z_Heavy = PGauss(RZ,Sigpol_Mode_0); /* random choice of Z */
+ }break;
+ case 1:
+ {
+ R_A_heavy = PGauss(AC_Mode_1,SigA_Mode_1);
+ RZpol = Zshift[1][2][CInt(R_A_heavy)]; /* local polarization */
+ RZ = R_A_heavy * I_Z_CN / I_A_CN + RZpol;
+ R_Z_Heavy = PGauss(RZ,Sigpol_Mode_1);
+ }break;
+ case 2:
+ {
+ Iguess = 0;
+ bool Next2 = true;
+ while(Next2)
+ {
+ Next2=false;
+ Iguess = Iguess + 1;
+
+ R_A_heavy = PBox2(AC_Mode_2,SigA_Mode_2*S2leftmod,SigA_Mode_2,P_A_Width_S2);
+ RZpol = Zshift[2][2][CInt(R_A_heavy)];
+ RZ = R_A_heavy * I_Z_CN / I_A_CN + RZpol ;
+ RN = R_A_heavy - RZ;
+ // if(Iguess < 1.e3)
+ // if(Rtest > Gaussintegral(RN-82,1.5*SigZ_Mode_2))
+ // Next2 = true;
+ // if (Iguess < 1.e3)
+ // if (Rtest > Gaussintegral(RZ-ZTRUNC50,FTRUNC50*SigZ_Mode_2))
+ // if ( (Rtest > 0.5 * ERF((RZ-ZTRUNC50)/(FTRUNC50*SigZ_Mode_2)) + 0.5) |( Rtest > 0.5 * ERF((I_Z_CN - RZ - ZTRUNC28)/(FTRUNC28*SigZ_Mode_2)) + 0.5))
+ // Next2 = true;
+ }
+ /* truncation below Z = 35 and below Z = 50 due to properties of deformed shells */
+ R_Z_Heavy = PGauss(RZ,Sigpol_Mode_2);
+ }break;
+ case 3:
+ {
+ R_A_heavy = PGauss(AC_Mode_3,SigA_Mode_3);
+ RZpol = Zshift[3][2][CInt(R_A_heavy)];
+ RZ = R_A_heavy * I_Z_CN / I_A_CN + RZpol;
+ R_Z_Heavy = PGauss(RZ,Sigpol_Mode_3);
+ }break;
+ case 4:
+ {
+ if(ZC_Mode_4 > ZC_Mode_0)
+ R_A_heavy = PGauss(AC_Mode_4,SigA_Mode_4);
+ else
+ R_A_heavy = I_A_CN - PGauss(AC_Mode_4,SigA_Mode_4);
+ //AC_Mode_4 refers to the light fragment
+ RZpol = Zshift[4][2][CInt(R_A_heavy)];
+ RZ = R_A_heavy * I_Z_CN / I_A_CN + RZpol;
+ R_Z_Heavy = PGauss(RZ,Sigpol_Mode_4);
+ }break;
+ case 5:
+ {
+ R_A_heavy = PGauss(AC_Mode_0,SigA_Mode_11);
+ RZ = R_A_heavy * I_Z_CN / I_A_CN;
+ R_Z_Heavy = PGauss(RZ,Sigpol_Mode_0);
+ }break;
+ case 6:
+ {
+ R_A_heavy = PGauss(AC_Mode_0,SigA_Mode_22);
+ RZ = R_A_heavy * I_Z_CN / I_A_CN;
+ R_Z_Heavy = PGauss(RZ,Sigpol_Mode_0);
+ }break;
+ default:
+ {
+ cout<< "Wrong I_Mode"<<endl;
+ }break;
+ }
+
+ R_Z_Light = I_Z_CN - R_Z_Heavy;
+ R_A_light = I_A_CN - R_A_heavy;
+
+ if((R_A_heavy < 1) | (R_A_light < 1))
+ DiceA = true;
+ if(R_A_heavy < R_A_light)
+ DiceA = true;
+ }
+ /* Diego --- They are only for spectra proposes
+ // Pre-neutron Z distribution, without even-odd effect
+
+ I = CInt(R_Z_Heavy)
+ If I >= Lbound(ZPROV) and I <= Ubound(Zprov) Then
+ ZPROV(I) = ZPROV(I) + Racc
+ ZMPROV(I_Mode,I) = ZMPROV(I_Mode,I) + Racc
+ End If
+ I = CInt(R_Z_Light)
+ If I >= Lbound(ZPROV) and I <= Ubound(Zprov) Then
+ ZPROV(I) = ZPROV(I) + Racc
+ ZMPROV(I_Mode,I) = ZMPROV(I_Mode,I) + Racc
+ End If
+
+ // Provisional mass distribution, pre-neutron,
+ // directly deduced from Z distribution with UCD assumption
+
+ APROV(CInt(R_Z_Heavy * I_A_CN / I_Z_CN + 0.5)) = _
+ APROV(CInt(R_Z_Heavy * I_A_CN / I_Z_CN + 0.5)) + Racc
+ APROV(CInt(R_Z_Light * I_A_CN / I_Z_CN + 0.5)) = _
+ APROV(CInt(R_Z_Light * I_A_CN / I_Z_CN + 0.5)) + Racc
+ AMPROV(I_Mode,CInt(R_Z_Heavy * I_A_CN / I_Z_CN + 0.5)) = _
+ AMPROV(I_Mode,CInt(R_Z_Heavy * I_A_CN / I_Z_CN + 0.5)) + Racc
+ AMPROV(I_Mode,CInt(R_Z_Light * I_A_CN / I_Z_CN + 0.5)) = _
+ AMPROV(I_Mode,CInt(R_Z_Light * I_A_CN / I_Z_CN + 0.5)) + Racc
+ */
+
+ /* Round on integer values with even-odd effect */
+
+ R_N_heavy = R_A_heavy - R_Z_Heavy;
+
+ I_N_heavy_sad = EVEN_ODD(R_N_heavy,PEON[I_Mode][2][CInt(R_A_heavy)]);
+ I_Z_heavy_sad = EVEN_ODD(R_Z_Heavy,PEOZ[I_Mode][2][CInt(R_A_heavy)]);
+ I_A_heavy_sad = I_N_heavy_sad + I_Z_heavy_sad;
+
+ I_N_light_sad = I_N_CN - I_N_heavy_sad;
+ I_Z_light_sad = I_Z_CN - I_Z_heavy_sad;
+ I_A_light_sad = I_A_CN - I_A_heavy_sad;
+
+ I_A_sad = I_A_CN;
+ I_Z_sad = I_Z_CN;
+ I_N_sad = I_N_CN;
+
+ Qvalue = AME2012(I_Z_sad,I_A_sad) - (AME2012(I_Z_heavy_sad,I_A_heavy_sad) + AME2012(I_Z_light_sad,I_A_light_sad));
+
+ E_intr_light = EPART[I_Mode][1][I_A_light_sad];
+ E_intr_heavy = EPART[I_Mode][2][I_A_heavy_sad];
+
+}
+
+void GEF::N_Saddle_Scission(void)
+{
+ float E_Final_Light,J_Frag_light,TlightFF,R_Z_light_sci,R_A_light_sci;
+ float E_Final_Heavy,J_Frag_heavy,TheavyFF,R_Z_heavy_sci,R_A_heavy_sci;
+ float Array_E_n1_ss[51];
+ float Array_E_n2_ss[51];
+
+ TlightFF = 1; //not used
+ TheavyFF = 1; //not used
+
+ I_nu_ss = 0;
+
+ if(E_intr_light + E_intr_heavy > Escission_lim)
+ {
+ for(int i = 1; i<=50;i++)
+ {
+ Array_E_n1_ss[i] = 0;
+ Array_Tn[i] = 0;
+ Array_E_n1_frag1[i] = 0;
+ }
+ E_Final_Light = Escission_lim * Csng(I_A_light_sad) / Csng(I_A_sad) - 9;
+ J_Frag_light = 0;
+ // Eva(0,I_Z_light_sad,I_A_light_sad,E_intr_light,TlightFF,J_Frag_light,R_Z_light_sci,
+ // R_A_light_sci,E_Final_Light,Array_E_n1_ss,Array_Tn,Array_Eg0_light);
+ Eva(0,I_Z_light_sad,I_A_light_sad,E_intr_light,TlightFF,J_Frag_light,R_Z_light_sci,
+ R_A_light_sci,E_Final_Light,Array_E_n1_frag1,Array_Tn,Array_Eg0_light);
+
+ for(int i = 1;i<= 50;i++)
+ {
+ //cout << Array_E_n1_frag1[i] << endl;
+ if(Array_E_n1_ss[i] == 0)
+ break;
+ I_nu_ss = I_nu_ss + 1;
+ }
+ I_A_light_sci = R_A_light_sci;
+ I_Z_light_sci = R_Z_light_sci;
+ I_N_light_sci = I_A_light_sci - I_Z_light_sci;
+ E_intr_light = E_Final_Light;
+
+ for(int i = 1;i<=50;i++)
+ {
+ Array_E_n2_ss[i] = 0;
+ Array_Tn[i] = 0;
+ Array_E_n2_frag2[i] = 0;
+ }
+ E_Final_Heavy = Escission_lim * Csng(I_A_heavy_sad) / Csng(I_A_sad) - 9;
+ J_Frag_heavy = 0;
+ // Eva(0,I_Z_heavy_sad,I_A_heavy_sad,E_intr_heavy,TheavyFF,J_Frag_heavy,R_Z_heavy_sci,
+ // R_A_heavy_sci,E_Final_Heavy,Array_E_n2_ss,Array_Tn,Array_Eg0_heavy);
+ Eva(0,I_Z_heavy_sad,I_A_heavy_sad,E_intr_heavy,TheavyFF,J_Frag_heavy,R_Z_heavy_sci,
+ R_A_heavy_sci,E_Final_Heavy,Array_E_n2_frag2,Array_Tn,Array_Eg0_heavy);
+
+ for(int i = 1;i<=50;i++)
+ {
+ if(Array_E_n2_ss[i] == 0)
+ break;
+ I_nu_ss = I_nu_ss + 1;
+ }
+ I_A_heavy_sci = R_A_heavy_sci;
+ I_Z_heavy_sci = R_Z_heavy_sci;
+ I_N_heavy_sci = I_A_heavy_sci - I_Z_heavy_sci;
+ E_intr_heavy = E_Final_Heavy;
+
+ I_A_sci = I_A_light_sci + I_A_heavy_sci;
+ I_Z_sci = I_Z_light_sci + I_Z_heavy_sci;
+ I_N_sci = I_N_light_sci + I_N_heavy_sci;
+ }
+ else
+ {
+ I_A_light_sci = I_A_light_sad;
+ I_Z_light_sci = I_Z_light_sad;
+ I_N_light_sci = I_N_light_sad;
+ I_A_heavy_sci = I_A_heavy_sad;
+ I_Z_heavy_sci = I_Z_heavy_sad;
+ I_N_heavy_sci = I_N_heavy_sad;
+ I_A_sci = I_A_light_sad + I_A_heavy_sad;
+ I_Z_sci = I_Z_light_sad + I_Z_heavy_sad;
+ I_N_sci = I_N_light_sad + I_N_heavy_sad;
+ }
+}
+
+void GEF::FragmentsEnergy(void)
+{
+ if(I_Mode == 0)
+ {
+ // Transition from shell-defined to macroscopic shape with increasing E*
+ // RW_mac = relative macroscopic influence
+
+ float EtotS0;
+ EtotS0 = Max(E_Exc_S0 + E_diss_Scission,0.0);
+ RW_mac = Gaussintegral(EtotS0-20.0,5.0);
+ /* Only deformation energy: */
+ Eexc_light_mean = (1.0 - RW_mac) * Edefo[0][1][I_Z_light_sci] + RW_mac * Edefo[1][1][I_Z_light_sci];
+ Eexc_heavy_mean = (1.0 - RW_mac) * Edefo[0][2][I_Z_heavy_sci] + RW_mac * Edefo[1][2][I_Z_heavy_sci];
+
+ RS = SIGDEFO_0 ;
+ // RS = SIGDEFO_0 * Sqr(T_Pol_Mode_0 / TEgidy(P_A_CN,0.0,1.0))
+ // Scaling with Sqr(intrinsic temperature / const. T value)
+ ESIGDEFOlight =
+ ( LyMass(I_Z_light_sci,I_A_light_sci,Beta[I_Mode+1][1][I_Z_light_sci] + RS) -
+ LyMass(I_Z_light_sci,I_A_light_sci,Beta[I_Mode+1][1][I_Z_light_sci] ));
+ ESIGDEFOheavy =
+ ( LyMass(I_Z_heavy_sci,I_A_heavy_sci,Beta[I_Mode+1][2][I_Z_heavy_sci] + RS) -
+ LyMass(I_Z_heavy_sci,I_A_heavy_sci,Beta[I_Mode+1][2][I_Z_heavy_sci] ));
+ }
+ if(I_Mode > 0 && I_Mode <= 4)
+ {
+ Eexc_light_mean = Edefo[I_Mode+1][1][I_Z_light_sci]; /* Only deformation energy */
+ Eexc_heavy_mean = Edefo[I_Mode+1][2][I_Z_heavy_sci]; /* Only deformation energy */
+ // RS = SIGDEFO/Sqr(R_Att_Sad(I_Mode))
+ RS = SIGDEFO;
+ ESIGDEFOlight =
+ ( LyMass(I_Z_light_sci,I_A_light_sci,Beta[I_Mode+1][1][I_Z_light_sci] + RS) -
+ LyMass(I_Z_light_sci,I_A_light_sci,Beta[I_Mode+1][1][I_Z_light_sci] ));
+ ESIGDEFOheavy =
+ ( LyMass(I_Z_heavy_sci,I_A_heavy_sci,Beta[I_Mode+1][2][I_Z_heavy_sci] + RS) -
+ LyMass(I_Z_heavy_sci,I_A_heavy_sci,Beta[I_Mode+1][2][I_Z_heavy_sci] ));
+
+ // If beta(I_MOde,1,I_Z_light) > 0.68 Then
+ // ESIGDEFOlight = 0.4*ESIGDEFOlight
+ // End If
+ }
+ if(I_Mode == 5)
+ {
+ Eexc_heavy_mean = Edefo[2][2][I_Z_heavy_sci];
+ Eexc_light_mean = Edefo[2][2][I_Z_light_sci]; /* Shell effect stored for "heavy" fragment */
+ // RS = SIGDEFO/Sqr(R_Att_Sad(I_Mode))
+ RS = SIGDEFO;
+ ESIGDEFOheavy =
+ ( LyMass(I_Z_heavy_sci,I_A_heavy_sci,Beta[2][2][I_Z_heavy_sci] + RS) -
+ LyMass(I_Z_heavy_sci,I_A_heavy_sci,Beta[2][2][I_Z_heavy_sci] ));
+ ESIGDEFOlight =
+ ( LyMass(I_Z_light_sci,I_A_light_sci,Beta[3][2][I_Z_light_sci] + RS) -
+ LyMass(I_Z_light_sci,I_A_light_sci,Beta[3][2][I_Z_light_sci] ));
+ }
+ if(I_Mode == 6)
+ {
+ Eexc_heavy_mean = Edefo[3][2][I_Z_heavy_sci];
+ Eexc_light_mean = Edefo[3][2][I_Z_light_sci]; /* Shell effect stored for "heavy" fragment */
+ // RS = SIGDEFO/Sqr(R_Att_Sad(I_Mode))
+ RS = SIGDEFO;
+ ESIGDEFOheavy =
+ ( LyMass(I_Z_heavy_sci,I_A_heavy_sci,Beta[3][2][I_Z_heavy_sci] + RS) -
+ LyMass(I_Z_heavy_sci,I_A_heavy_sci,Beta[3][2][I_Z_heavy_sci] ));
+ ESIGDEFOlight =
+ ( LyMass(I_Z_light_sci,I_A_light_sci,Beta[3][2][I_Z_light_sci] + RS) -
+ LyMass(I_Z_light_sci,I_A_light_sci,Beta[3][2][I_Z_light_sci] ));
+ }
+ if(Eexc_heavy_mean < 0)
+ Eexc_heavy_mean = 0;
+ if(Eexc_light_mean < 0)
+ Eexc_light_mean = 0;
+
+ /* Deformation of heavy and light fragment assumed to be uncorrelated */
+
+ TKEmin = 1.44 * I_Z_light_sci * I_Z_heavy_sci / (3.0 * (pow(I_A_light_sci,0.33333) + pow(I_A_heavy_sci,0.3333)));
+ /* TKEmin for limiting the excitation energies of the fragments */
+ if(Qvalue-TKEmin < 0)
+ {
+ cout<<"<W> Estimated TKEmin > Qvalue: TKEmin = "<<TKEmin<<", Qvalue = "<<Qvalue<<endl;
+ cout<< " A_heavy = "<<I_A_heavy_sci<<", A_light; "<<I_A_light_sci<<", Mode = "<<I_Mode<<endl;
+ cout<< " Z_heavy = "<<I_Z_heavy_sci<<", Z_light; "<<I_Z_light_sci<<", Mode = "<<I_Mode<<endl;
+ TKEmin = Qvalue - 1;
+ }
+ // Limitation of E* to avoid impossible values: Switch from shell-shape to macroscopic shape
+ if(Eexc_light_mean > (Qvalue-TKEmin) * I_A_heavy_sci / I_A_sci)
+ Eexc_light_mean = Edefo[1][1][I_Z_light_sci];
+ if(Eexc_heavy_mean > (Qvalue-TKEmin) * I_A_light_sci / I_A_sci)
+ Eexc_heavy_mean = Edefo[1][2][I_Z_heavy_sci];
+
+ // Contribution to width of TKE and TXE by fluctuation of neck length
+ // ESIGDEFOlight = sqr(ESIGDEFOLight^2 + (SIGENECK * R_Z_Light * R_Z_heavy)^2)
+ // ESIGDEFOheavy = sqr(ESIGDEFOheavy^2 + (SIGENECK * R_Z_light * R_Z_heavy)^2)
+
+ Eexc_light = -1.;
+ while((Eexc_light < 0.) | (Eexc_light > (Qvalue-TKEmin) * I_A_heavy_sci / I_A_sci))
+ Eexc_light = PGauss(Eexc_light_mean,ESIGDEFOlight);
+ Eexc_heavy = -1.;
+ while((Eexc_heavy < 0.) | (Eexc_heavy > (Qvalue-TKEmin) * I_A_light_sci / I_A_sci))
+ Eexc_heavy = PGauss(Eexc_heavy_mean,ESIGDEFOheavy);
+ // If Eexc_light_mean > 50 or Eexc_heavy_mean > 50 Then
+ // Print "Mode,Zlight,Alight,Eexc_light_mean",I_Mode,I_Z_light,I_A_light,Eexc_light_mean
+ // Print "Mode,Zheavy,Aheavy,Eexc_heavy_mean",I_Mode,I_Z_heavy,I_A_heavy,Eexc_heavy_mean
+ // End If
+
+ /* Assumption: width in TKE is the */
+ /* quadratic sum of widths in defo and coll. */
+ /* Remark of caution: The width of the TKE for fixed mass contains often
+ several fission modes. The width in Lang et al. for fixed Z contains several A,
+ which contributes already with about 3% to the width. Therefore, the
+ width in TXE (or TKE) for fixed A and fixed mode may be much smaller than
+ 4 or 5 percent! */
+
+
+ /* Temperatures of fragments */
+
+ if (I_Mode <= 4)
+ {
+ Tlight = Temp[I_Mode][1][I_A_light_sci];
+ Theavy = Temp[I_Mode][2][I_A_heavy_sci];
+ }
+ if(I_Mode == 5)
+ {
+ Tlight = Temp[1][2][I_A_light_sci];
+ Theavy = Temp[1][2][I_A_heavy_sci];
+ }
+ if(I_Mode == 6)
+ {
+ Tlight = Temp[2][2][I_A_light_sci];
+ Theavy = Temp[2][2][I_A_heavy_sci];
+ }
+
+ /* Intrinsic excitation energies of fragments */
+
+ float Delta_E_Q;
+ int I_E_Q;
+ float E_intr_tot, Sigma_E_intr;
+
+ E_intr_light_mean = EPART[I_Mode][1][I_A_light_sci];
+ E_intr_heavy_mean = EPART[I_Mode][2][I_A_heavy_sci];
+
+ if(I_Mode == 0)
+ {
+ // At high E*(CN), where the SL (S0) mode is dominant,
+ // TKE is only a macroscopic quantity, microscopic contributions
+ // must be suppressed.
+ // TKE is derived from empirical formula.
+
+ I_E_Q = 0;
+ bool Repeat_E_Q=true;
+ while(Repeat_E_Q)
+ {
+ Repeat_E_Q=false;
+ I_E_Q = I_E_Q + 1;
+ E_intr_light = -1.;
+ E_intr_tot = E_intr_light_mean + E_intr_heavy_mean;
+ if(E_intr_tot < 10)
+ // Fit function: Fluctuation of energy division from
+ // width of phase-space factor with Fermi-gas level density
+ // (below 10 MeV: constant-T level density).
+ // Fluctuation of E_intr_tot not changed.
+ Sigma_E_intr = E_intr_tot * 0.47 * exp(-sqrt(10/160)) / I_E_Q / 2.35;
+ else
+ Sigma_E_intr = E_intr_tot * 0.47 * exp(-sqrt(E_intr_tot/160)) / I_E_Q / 2.35;
+
+ E_intr_light = PGauss(E_intr_light_mean, Sigma_E_intr);
+ E_intr_heavy = E_intr_tot - E_intr_light;
+ // Print
+ // Print "At scission ";I_A_light;I_A_heavy;E_intr_light,E_intr_heavy
+
+ // Add E* gain after scission due to shell and pairing of fragments.
+ // This way, they are removed from TKE (further down in the code).
+ // This is reasonable, because fragment shell and pairing energies appear after scisssion.
+ // Thus, they do not appear in the TKE.
+ E_intr_light = E_intr_light -
+ AME2012(I_Z_light_sci,I_A_light_sci) + LDMass(I_Z_light_sci,I_A_light_sci,0.) // shell and pairing
+ - 2.0 * 12.0 / sqrt(I_A_light_sci); // general shift
+ E_intr_heavy = E_intr_heavy -
+ AME2012(I_Z_heavy_sci,I_A_heavy_sci) + LDMass(I_Z_heavy_sci,I_A_heavy_sci,0.) // shell and pairing
+ - 2.0 * 12.0 / sqrt(I_A_heavy_sci); // general shift
+ float Epre_mean,TKE_mac,TKE1,TKE2,dmod;
+ Epre_mean = 0.4 * De_Saddle_Scission(pow(I_Z_CN,2)/pow(I_A_CN,0.333333),ESHIFTSASCI_coll);
+ // Mean pre-scission kinetic energy
+ dmod = (DNECK + 1); // adjusted to TKE of 250Fm(E*=45 MeV) (in conflict with Loveland 1970?)
+ TKE_mac = 1.44*I_Z_light_sci*I_Z_heavy_sci/
+ (1.16*(pow(I_A_light_sci,0.33333)*(1.0+0.66667*Beta[1][1][I_Z_light_sci]) +
+ pow(I_A_heavy_sci,0.33333)*(1.0+0.66667*Beta[1][2][I_Z_heavy_sci])) + dmod)
+ - 1.44*pow(I_Z_sci/2,2) /
+ (1.16*( pow(I_A_sci/2,0.33333)*(1.0+0.66667*Beta[1][1][I_Z_sci/2]) +
+ pow(I_A_sci/2,0.33333)*(1.0+0.66667*Beta[1][2][I_Z_sci/2])) + DNECK);
+ // (Variation of TKE from macroscopic formula of Wilkins et al.
+ // relative to value at symmetry.)
+ Delta_E_Q = - AME2012(I_Z_sci,I_A_sci) + LDMass(I_Z_sci,I_A_sci,0.)
+ + LyMass(I_Z_light_sci,I_A_light_sci,0.) + LyMass(I_Z_heavy_sci,I_A_heavy_sci,0.)
+ - LyMass(I_Z_sci,I_A_sci,0)
+ - (LyMass(I_Z_sci/2,I_A_sci/2,0.) + LyMass(I_Z_sci/2,I_A_sci/2,0.) - LyMass(I_Z_sci,I_A_sci,0))
+ + TKE_mac // replace macr. variation of Q value by Wilkins formula
+ + Epre_mean; // add pre-scission TKE
+ // Print "Delta_E_Q",Delta_E_Q,I_Z_sci,I_A_sci,TKE_mac,Epre_mean
+ // positives Delta_E_Q (ohne TKE_mac) erhöht TKE in den Flanken (mehr als TKE_mac)
+ // positives Epre_mean erhöht TKE
+ // positives TKE_mac vermindert TKE in den Flanken
+
+ E_intr_light = E_intr_light - I_A_light_sci/I_A_sci * (Delta_E_Q);
+ E_intr_heavy = E_intr_heavy - I_A_heavy_sci/I_A_sci * (Delta_E_Q);
+ E_intr_light_S0_mac = Max(0.0,E_intr_light);
+ E_intr_heavy_S0_mac = Max(0.0,E_intr_heavy);
+
+ // Print, "After fission: ";E_intr_light,E_intr_heavy
+
+ if((E_intr_light_S0_mac < 0) | (E_intr_heavy_S0_mac < 0))
+ {
+ if(I_E_Q < 3)
+ {
+ cout<< "Reapeat_E_Q"<<endl;
+ Repeat_E_Q=true;
+ }
+ cout<<"6326: E_intr_light/heavy = "<<E_intr_light<<"/"<<E_intr_heavy<<endl;
+ cout<<"6327: Mean values: "<<E_intr_light_mean<<" "<<E_intr_heavy_mean<<endl;
+ E_intr_light_S0_mac = Max(0.0,E_intr_light);
+ E_intr_heavy_S0_mac = Max(0.0,E_intr_heavy);
+ }
+ }
+ //--------------------------------------------------------
+ float TXE_shift,EtotS0;
+ TXE_shift=EtotS0=0;
+ if(Mod(I_Z_CN,2) == 0)
+ // Even-odd fluctuation of TXE acc. to Lang et al. NPA 345 (1980) 34
+ // Lower TXE for completely paired configuration at scission.
+ // Only the even-odd effect at symmetry is considered, because the
+ // energy gain by the asymmetry-driven even-odd effect goes to E_intr
+ // of the heavy fragment due to energy sorting.
+ if(Mod(I_Z_light_sci,2) == 0)
+ if(rn->Rndm() < PEOZ[I_Mode][1][int(0.5*I_A_sci)])
+ TXE_shift = -12./sqrt(I_A_sci);
+
+ E_intr_light_S0_mic = E_intr_light_mean + TXE_shift * E_intr_light_mean / (E_intr_light_mean + E_intr_heavy_mean);
+ if(E_intr_light_S0_mic < 0.)
+ E_intr_light_S0_mic = 0.;
+ E_intr_heavy_S0_mic = E_intr_heavy_mean + TXE_shift * E_intr_heavy_mean / (E_intr_heavy_mean + E_intr_light_mean);
+ if(E_intr_heavy_S0_mic < 0.)
+ E_intr_heavy_S0_mic = 0.;
+
+ E_intr_light_S0_mic = E_intr_light_S0_mic - LyPair(I_Z_heavy_sci,I_A_heavy_sci);
+ E_intr_heavy_S0_mic = E_intr_heavy_S0_mic - LyPair(I_Z_heavy_sci,I_A_heavy_sci);
+
+ //--------------------------------------------------------
+
+ EtotS0 = Max(E_Exc_S0 + E_diss_Scission,0.0);
+ RW_mac = Gaussintegral(EtotS0-20.0,5.0);
+ E_intr_light_mean = (1.0 - RW_mac) * E_intr_light_S0_mic + RW_mac * E_intr_light_S0_mac;
+ E_intr_heavy_mean = (1.0 - RW_mac) * E_intr_heavy_S0_mic + RW_mac * E_intr_heavy_S0_mac;
+
+ //--------------------------------------------------------
+
+ E_intr_light = -1.;
+ while(E_intr_light < 0.)
+ E_intr_light = PGauss(E_intr_light_mean,EexcSIGrel* sqrt(2) * 0.5*sqrt(pow(E_diss_Scission,2)+pow(SIGENECK,2))+0.5);
+ E_intr_heavy = -1.;
+ while (E_intr_heavy < 0.)
+ E_intr_heavy = PGauss(E_intr_heavy_mean,EexcSIGrel* sqrt(2) * 0.5*sqrt(pow(E_diss_Scission,2)+pow(SIGENECK,2))+0.5);
+
+ //--------------------------------------------------------
+
+ if((E_intr_light < 0)|(E_intr_heavy < 0))
+ cout<< "E_intr < 0"<<E_intr_light<<" "<<E_intr_heavy<<endl;
+ }
+ else // If I_Mode <> 0
+ {
+ float TXE_shift=0;
+ if(Mod(I_Z_CN,2) == 0)
+ // Even-odd fluctuation of TXE acc. to Lang et al. NPA 345 (1980) 34
+ // Lower TXE for completely paired configuration at scission.
+ // Only the even-odd effect at symmetry is considered, because the
+ // energy gain by the asymmetry-driven even-odd effect goes to E_intr
+ // of the heavy fragment due to energy sorting.
+ if(Mod(I_Z_light_sci,2) == 0)
+ if(rn->Rndm() < PEOZ[I_Mode][1][int(0.5*I_A_sci)])
+ TXE_shift = -12./sqrt(I_A_sci);
+
+ E_intr_light_mean = E_intr_light_mean + TXE_shift * E_intr_light_mean / (E_intr_light_mean + E_intr_heavy_mean);
+ if(E_intr_light_mean < 0.)
+ E_intr_light_mean = 0.;
+ E_intr_heavy_mean = E_intr_heavy_mean + TXE_shift * E_intr_heavy_mean / (E_intr_heavy_mean + E_intr_light_mean);
+ if(E_intr_heavy_mean < 0.)
+ E_intr_heavy_mean = 0.;
+
+ E_intr_light = -1.;
+ while(E_intr_light < 0.)
+ {
+ E_intr_light = PGauss(E_intr_light_mean,EexcSIGrel* sqrt(2) * 0.5*sqrt(pow(E_diss_Scission,2)+pow(SIGENECK,2))+0.5);
+ E_intr_light = E_intr_light - LyPair(I_Z_light_sci,I_A_light_sci);
+ }
+ E_intr_heavy = -1.;
+ while(E_intr_heavy < 0.)
+ {
+ E_intr_heavy = PGauss(E_intr_heavy_mean,EexcSIGrel* sqrt(2) * 0.5*sqrt(pow(E_diss_Scission,2)+pow(SIGENECK,2))+0.5);
+ E_intr_heavy = E_intr_heavy - LyPair(I_Z_heavy_sci,I_A_heavy_sci);
+ }
+ //Print "6331: ";I_mode,E_intr_light_mean,E_intr_light
+ //Print "6332: ";I_mode,E_intr_heavy_mean,E_intr_heavy
+ //Print "6333: ";EexcSIGrel,E_diss_Scission,SIGENECK
+
+ // E_intr_light = E_intr_light - Lypair(I_Z_light,I_A_light)
+ // E_intr_heavy = E_intr_heavy - Lypair(I_Z_heavy,I_A_heavy)
+ /* Staggering of BE of fragments by pairing */
+ /* Assumption: pairing only felt in the lowest nuclear levels, */
+ /* at the end of the evaporation cascade */
+ /* (This should be a good assumption for higher excitation energies. */
+ /* Some deviations occur due to the even-odd effect at low exc. energies. */
+
+ } // If I_Mode <> 0
+
+ Qvalue = AME2012(I_Z_sci,I_A_sci) - (AME2012(I_Z_heavy_sci,I_A_heavy_sci) + AME2012(I_Z_light_sci,I_A_light_sci));
+
+ Eexc_light = Eexc_light + E_intr_light;
+ Eexc_heavy = Eexc_heavy + E_intr_heavy;
+ /* Now: deformation + intrinsic excitation energy */
+ /* Collective energy of fragments */
+
+ Ecoll_mean = ECOLLFRAC * (De_Saddle_Scission(pow(I_Z_CN,2) / pow(I_A_CN,0.33333),ESHIFTSASCI_coll) - E_tunn);
+
+ if(Ecoll_mean < 0.)
+ Ecoll_mean = 0.;
+
+ /* Experimental data of prompt neutron yields show an enhancement of the */
+ /* neutron yield for odd-Z CN, corresponding to an enhanced E* by about 1.6 MeV */
+ /* The enhancement is equally shared to the light and the heavy fragment. */
+ /* The neutron number of the CN has no influence. */
+ /* The origin of this effect is not clear. */
+ /* By technical reasons, this additional energy is introduced here into the */
+ /* collective energy at scission, because this energy is divided equally between both fragments. */
+ /* KHS, 31. Jan. 2012 */
+ // If (I_Z_CN Mod 2) = 1 Then Ecoll_mean = Ecoll_mean + 1.6
+ // This is not used any more. It seems to be wrong or to be replaced by something else.
+
+ // Assuming positive correlation of Ecoll_heavy and Ecoll_light.
+ // This is probably not realistic!
+ // See Nix & Swiatecki, Nucl. Phys. 71 (1965) 1
+ /* Ecoll = -1.
+ While Ecoll < 0.
+ Ecoll = PGauss(Ecoll_mean,EexcSIGrel* Ecoll_mean)
+ Wend
+ Ecoll = Ecoll + E_coll_saddle(I_Mode)
+ Ecoll_heavy = 0.5E0 * Ecoll
+ Ecoll_light = 0.5E0 * Ecoll */
+
+ // Assuming no correlation (partly positive, partly negative correlation)
+ // See Nix & Swiatecki, Nucl. Phys. 71 (1965) 1
+
+ float Rmean,Rsigma;
+ Rmean = 0.5 * Ecoll_mean;
+ Rsigma = sqrt(0.5) * EexcSIGrel * Ecoll_mean;
+ Ecoll_light = -1;
+ while(Ecoll_light < 0.)
+ Ecoll_light = PGauss(Rmean,Rsigma);
+ Ecoll_light = Ecoll_light + 0.5 * E_coll_saddle[I_Mode];
+ Ecoll_heavy = -1.;
+ while(Ecoll_heavy < 0.)
+ Ecoll_heavy = PGauss(Rmean,Rsigma);
+ Ecoll_heavy = Ecoll_heavy + 0.5E0 * E_coll_saddle[I_Mode];
+ Ecoll = Ecoll_heavy + Ecoll_light;
+
+ Eexc_light = Eexc_light + Ecoll_light;
+ Eexc_heavy = Eexc_heavy + Ecoll_heavy;
+ /* Now: also collective excitation energy added */
+
+
+ /* Excitation energy not including the rotational energy at scission: */
+
+ /*** Angular momentum of fragments ***/
+
+ float J_Frag_light,J_Frag_heavy;
+ float J_Frag_rot_light,J_Frag_rot_heavy; // collective spin
+ float N_J_attempt;
+ N_J_attempt = 0;
+
+ bool J_attempt=true;
+ while(J_attempt)
+ {
+ J_attempt=false;
+ N_J_attempt = N_J_attempt + 1;
+ if(I_Mode <= 4)
+ {
+ J_Frag_light = PLinGauss(SpinRMSNZ[I_Mode][1][I_N_light_sci][I_Z_light_sci]/sqrt(2.0)) - 0.5;
+ J_Frag_heavy = PLinGauss(SpinRMSNZ[I_Mode][2][I_N_heavy_sci][I_Z_heavy_sci]/sqrt(2.0)) - 0.5;
+ }
+ if(I_Mode == 5)
+ {
+ J_Frag_light = PLinGauss(SpinRMSNZ[1][2][I_N_light_sci][I_Z_light_sci]/sqrt(2.0)) - 0.5;
+ J_Frag_heavy = PLinGauss(SpinRMSNZ[1][2][I_N_heavy_sci][I_Z_heavy_sci]/sqrt(2.0)) - 0.5;
+ }
+ if(I_Mode == 6)
+ {
+ J_Frag_light = PLinGauss(SpinRMSNZ[2][2][I_N_light_sci][I_Z_light_sci]/sqrt(2.0)) - 0.5;
+ J_Frag_heavy = PLinGauss(SpinRMSNZ[2][2][I_N_heavy_sci][I_Z_heavy_sci]/sqrt(2.0)) - 0.5;
+ }
+
+ if(J_Frag_light < 0)
+ J_Frag_light = 0;
+
+ if(J_Frag_heavy < 0)
+ J_Frag_heavy = 0;
+
+ IfragEff_light = U_Ired(I_Z_light_sci,I_A_light_sci);
+ Erotlight = J_Frag_light*(J_Frag_light+1)/(2*IfragEff_light);
+ // rotational energy at scission
+
+ IfragEff_heavy = U_Ired(I_Z_heavy_sci,I_A_heavy_sci);
+ Erotheavy = J_Frag_heavy*(J_Frag_heavy+1)/(2*IfragEff_heavy);
+ // rotational energy at scission
+
+
+ float TXE, E_total;
+ /* Kinetic energies of fragments */
+
+ // TXE includes E*_CN
+
+ TXE = Eexc_light + Eexc_heavy + Erotlight + Erotheavy; // provisional value
+
+ E_total = Qvalue + R_E_exc_GS;
+ TKE = E_total - TXE;
+
+ static int Ntimes = 0;
+ if(TKE < 0)
+ {
+ // If TKE < 0 Or I_Mode =0 Then
+ if(N_J_attempt <= 3)
+ J_attempt=true;
+ float TXEcorr;
+ cout<< "<E> Event with excessive excitation energy found."<<endl;;
+ cout<< "I_A_light,I_Z_light,I_A_heavy,I_Z_heavy: "<<I_A_light_sci<<" "<<I_Z_light_sci<<" "<<I_A_heavy_sci<<" "<<I_Z_heavy_sci<<endl;
+ cout<< "Q value,TKE; "<<Qvalue<<" "<<TKE<<endl;
+ cout<< "Eexc_light,Eexc_heavy,Erot_light,Erot_heavy: "<<Eexc_light<<" "<<Eexc_heavy<<" "<<Erotlight<<" "<<Erotheavy<<endl;
+ cout<< "J_rms_light,J_rms_heavy: "<<SpinRMSNZ[I_Mode][1][I_N_light_sci][I_Z_light_sci]<<" "<<SpinRMSNZ[I_Mode][2][I_N_heavy_sci][I_Z_heavy_sci]<<endl;
+ cout<< "J_light,J_heavy "<<J_Frag_light<<" "<<J_Frag_heavy<<endl;
+ cout<< "Ecoll_light,Eintr_light: "<<Ecoll_light<<" "<<E_intr_light<<endl;
+ cout<< "Ecoll_heavy,Eintr_heavy: "<<Ecoll_heavy<<" "<<E_intr_heavy<<endl;
+ if(I_Mode == 0)
+ {
+ cout<<"I_Mode,Edefo(light),Edefo_mic(heavy),Edefo_mac(heavy): "<<I_Mode<<" "<< Edefo[I_Mode+1][1][I_Z_light_sci]<<" "<<Edefo[0][2][I_Z_heavy_sci]<<" "<<Edefo[I_Mode+1][2][I_Z_heavy_sci]<<endl;
+ cout<<"E_intr_light_S0_mic,..mac,..heavy_S0_mic,..heavy_S0_mac: "<<E_intr_light_S0_mic<<" "<<E_intr_light_S0_mac<<" "<<E_intr_heavy_S0_mic<<" "<<E_intr_heavy_S0_mac<<endl;
+ }
+ else
+ cout<< "I_Mode,Edefo(light),Edefo_(heavy): "<<I_Mode<<" "<<Edefo[I_Mode+1][1][I_Z_light_sci]<<" "<<Edefo[I_Mode+1][2][I_Z_heavy_sci]<<endl;
+ TXEcorr = TXE + TKE - 1;
+ TKE = 1;
+ Eexc_light = Eexc_light * TXEcorr/TXE;
+ Eexc_heavy = Eexc_heavy * TXEcorr/TXE;
+ TXE = TXEcorr;
+ Ntimes = Ntimes + 1;
+ if(Ntimes > 99)
+ {
+ cout<< "<S> Calculation stopped due to numerical problem."<<endl;
+ exit(-1);
+ }
+ }
+
+ }
+ TXElight = Eexc_light + Erotlight; // final values
+ TXEheavy = Eexc_heavy + Erotheavy; // " "
+
+ // Print Erotlight,Erotlight_FF,Erotheavy,Erotheavy_FF
+
+
+ TXE = TXElight + TXEheavy; // " "
+
+
+ Ekinlight_sci = TKE * I_A_heavy_sci / I_A_sci;
+ Ekinheavy_sci = TKE * I_A_light_sci / I_A_sci;
+ // Print 7058,TKE,I_A_light_sci,I_A_heavy_sci
+ // Print "7057 ";I_A_light_sci,Erotlight+Erotheavy,TXE,TKE,Qvalue, _
+ // AME2012(I_Z_sci,I_A_sci) - _
+ // (AME2012(I_Z_heavy_sci,I_A_heavy_sci) _
+ // + AME2012(I_Z_light_sci,I_A_light_sci))
+
+ // cout<< Ekinlight_sci<<" "<<Ekinheavy_sci<<endl;
+}
+
+void GEF::FromCMtoLAB(void)
+{
+ Thcm_light = acos(rn->Rndm()*2.-1.);
+ Thcm_heavy = pi-Thcm_light;
+ Phcm_light = rn->Rndm()*2*pi-pi;
+ if(Phcm_light == 0)
+ Phcm_heavy = pi;
+ else
+ Phcm_heavy = Phcm_light - Phcm_light/abs(Phcm_light)*pi;
+
+ float Gfis,Bfis;
+ Gfis = 1.;
+ if(Afis>0){
+ //Gfis = FIS.GetEnergy()/(FIS.Mass()+Ex)+1.;
+ Gfis = Efis/(FIS.Mass()+Ex)+1.;
+ }
+ Bfis = sqrt(1.-1./pow(Gfis,2));
+
+ float M_light,M_heavy;
+ M_light=M_heavy=0;
+ M_light = AME2012(I_Z_light_sci,I_A_light_sci)+I_Z_light_sci*(931.494+7.28897061)+(I_A_light_sci-I_Z_light_sci)*(931.494+8.0713171);
+ M_heavy = AME2012(I_Z_heavy_sci,I_A_heavy_sci)+I_Z_heavy_sci*(931.494+7.28897061)+(I_A_heavy_sci-I_Z_heavy_sci)*(931.494+8.0713171);
+ float Gcm_light, Gcm_heavy;
+ float Bcm_light, Bcm_heavy;
+ Gcm_light=Gcm_heavy=1.;
+ if(M_light>0)
+ Gcm_light = Ekinlight_sci/M_light+1.;
+ if(M_heavy>0)
+ Gcm_heavy = Ekinheavy_sci/M_heavy+1.;
+ Bcm_light = sqrt(1.-1./pow(Gcm_light,2));
+ Bcm_heavy = sqrt(1.-1./pow(Gcm_heavy,2));
+
+ //cout << Ekinlight_sci << " " << Ekinheavy_sci << " " << Ekinlight_sci+ Ekinheavy_sci << endl;
+
+ KElab_light = KElab_heavy= 0;
+ KElab_light = (Gfis*Gcm_light*M_light +Gfis*Bfis*Gcm_light*Bcm_light*M_light*cos(Thcm_light))-M_light;
+ KElab_heavy = (Gfis*Gcm_heavy*M_heavy +Gfis*Bfis*Gcm_heavy*Bcm_heavy*M_heavy*cos(Thcm_heavy))-M_heavy;
+
+ Glab_light=Glab_heavy=1.;
+ if(M_light>0)
+ Glab_light = KElab_light/M_light+1.;
+ if(M_heavy>0)
+ Glab_heavy = KElab_heavy/M_heavy+1.;
+ Blab_light = sqrt(1.-1./pow(Glab_light,2));
+ Blab_heavy = sqrt(1.-1./pow(Glab_heavy,2));
+ vlab_light = Blab_light*29.9792458;
+ vlab_heavy=Blab_heavy*29.9792458;
+
+ //Note that I am not taking account the angle of the fissioning system
+ Thlab_light = Thlab_heavy=0;
+ if(Blab_light>0)
+ Thlab_light = acos(1./Glab_light/Blab_light*(Gfis*Bfis*Gcm_light+Gfis*Gcm_light*Bcm_light*cos(Thcm_light)));
+ if(Blab_heavy>0)
+ Thlab_heavy = acos(1./Glab_heavy/Blab_heavy*(Gfis*Bfis*Gcm_heavy+Gfis*Gcm_heavy*Bcm_heavy*cos(Thcm_heavy)));
+ Phlab_light = Phcm_light;
+ Phlab_heavy = Phcm_heavy;
+
+ //Thlablab_light = acos(-1.*sin(Thlab_light)*cos(Phlab_light)*sin(FIS->GetThfis())-sin(Thlab_light)*sin(Phlab_light)*sin(FIS->GetThfis())+cos(Thlab_light)*cos(FIS->GetThfis()));
+ //cout<<Thlab_light*180./pi<<" "<<Thlablab_light*180./pi<<endl;
+}
+
+///////////////////////////////////CHARGE STATES = f(Z,vlab) from E. Baron NIM A 328,177 (1993)//////////////////
+float Qmean_Baron_lowZ(float Z, float v)
+{
+ float par[2]={-83.275,0.447};
+ float beta = v/29.9792458;
+ return Z*(1.-1.*exp(par[0]*beta/pow(Z,par[1])));
+}
+float Qmean_Baron(float Z, float v)
+{
+ float par[3]={-12.905,0.2124,-0.00122};
+ float qmean1 = Qmean_Baron_lowZ(Z,v);
+ float qmean2 = qmean1*(1.-exp(par[0]+par[1]*Z+par[2]*Z*Z));
+ if(Z<54)
+ return qmean1;
+ else
+ return qmean2;
+}
+
+float Qsigma_Baron(float Z, float v)
+{
+ float par[5]={0.5,1.67,0.07535,0.19,-0.2654};
+ float qmean1 = Qmean_Baron_lowZ(Z,v);
+ float sigma1 = par[0]*sqrt(qmean1*(1.-pow(qmean1/Z,par[1])));
+ float sigma2 = sqrt(qmean1*(par[2]+par[3]*qmean1/Z+par[4]*pow(qmean1/Z,2)));
+ if(Z<54)
+ return sigma1;
+ else
+ return sigma2;
+}
+///////////////////////////////////////////////////////////////////////////////////////////////////////////////////
+
+void GEF::FissionProbability(void)
+{
+ // This section is for calculating the first-chance fission probablity for a large
+ // range of excitation energy with an analytical function (4<Ex<80)MeV.
+ // In contrast to the Monte-Carlo method, used for the "normal" calculation,
+ // this works also for very low fission probabilities.
+ float E_left;
+ int Z_left,A_left;
+ float SNTF,SNTFnopair,SNmean;
+ float SP,BP,SPTF,SPTFnopair,SPmean,BPmean,BPnopair;
+ float BF,BFNP,BFMNP,BFA,BFANP,BFB,BFBNP,BFM;
+ float af_an;
+ float Ztrans = 86.0;
+ float dZtrans = 2;
+ float DUN,DU;
+ double Rho_cn;
+ float G,GN,GP,GF;
+ float T_n,T_f,T_p,Tm;
+ float FtunnA,FtunnB;
+ float hbom = 1.; // effective curvature of fission barrier
+ float Tequi = hbom /(2 * pi); // equivalent temperature parameter
+ float F1_coll = 10;
+ float F1_diss = 20;
+ float GA = (0.14 / sqrt(pi/2)); // triaxiality (compared to quadrupole deformation)
+ float GB = 0.5; // mass asymmetry (compared to quadrupole deformation)
+ float GAmod,GBmod;
+ float DUF = 0; // Shell effect at barrier
+ float ypsilon,l_lim_2;
+ float Frot;
+ float Red_diss;
+ float Ggamma;
+ if(Ex<4)
+ PF=0;
+ else
+ {
+ E_left = Ex;
+ Z_left = P_Z_CN;
+ A_left = P_A_CN;
+ SN = AME2012(Z_left,A_left-1) - AME2012(Z_left,A_left);
+ SNTF = U_MASS(Z_left,A_left-1) + LyPair(Z_left,A_left-1) - (U_MASS(Z_left,A_left) + LyPair(Z_left,A_left));
+ SNTFnopair = U_MASS(Z_left,A_left-1) - U_MASS(Z_left,A_left);
+ SNmean = 0.5 * (U_MASS(Z_left,A_left-2) - U_MASS(Z_left,A_left));
+
+ SP = AME2012(Z_left-1,A_left-1) - AME2012(Z_left,A_left);
+ BP = SP + 1.44 * (Z_left-1) / (2.0 * (1 + pow(A_left-1,0.333333)));
+ SPTF = U_MASS(Z_left-1,A_left-1) + LyPair(Z_left-1,A_left-1) - (U_MASS(Z_left,A_left) + LyPair(Z_left,A_left));
+ SPTFnopair = U_MASS(Z_left-1,A_left-1) - U_MASS(Z_left,A_left);
+ BPnopair = SPTFnopair + 1.44 * (Z_left-1) / (2.0 * (1 + pow(A_left-1,0.333333)));
+ SPmean = 0.5 * (U_MASS(Z_left-2,A_left-2) - U_MASS(Z_left,A_left));
+ BPmean = SPmean + 1.44 * (Z_left-1) / (2.0 * (1 + pow(A_left-1,0.333333)));
+
+ BF = BFTF(P_Z_CN,A_left,1); // with shell and enhanced pairing at barrier
+ BFNP = BFTF(P_Z_CN,A_left,3); // no enhanced pairing at barrier
+ // BFLD = BFTF(P_Z_CN,A_left,0) // liquid drop
+ // BFA = BFTFA(P_Z_CN,A_left,1) // with shell and enhanced pairing at barrier
+ BFA = BFTFA(P_Z_CN,A_left,1) + 10 / sqrt(A_left) * Mod(A_left-P_Z_CN + 1,2);
+ // e-o in levdens at Bf
+ BFANP = BFTFA(P_Z_CN,A_left,3); // no enhanced pairing at barrier
+ BFB = BFTFB(P_Z_CN,A_left,1) + 10 / sqrt(A_left) * Mod(A_left-P_Z_CN + 1,2);
+ // e-o-in levdens at Bf
+ BFBNP = BFTFB(P_Z_CN,A_left,3); // no enhanced pairing at barrier
+ BFM = Max(BFA,BFB); // highest saddle
+ BFMNP = Max(BFANP,BFBNP); // highest saddle without enhanced pairing
+ af_an = 1.2 - 0.2 * Gaussintegral(P_Z_CN - Ztrans, dZtrans);
+ DUN = U_SHELL(P_Z_CN,A_left-1);
+ DU = U_SHELL(P_Z_CN,A_left);
+ Rho_cn = U_levdens(P_Z_CN,A_left, E_left, 1, 1, Tscale, Econd,1);
+ // Smean = 0.5 * (SNmean + BFMNP)
+ if(E_left > SN)
+ {
+ T_n = U_Temp(P_Z_CN,A_left-1,E_left-SN,1,1,Tscale,Econd);
+ GN = pow(A_left-1,0.66667) * 0.13 * pow(T_n,2) * U_levdens(P_Z_CN,A_left-1,E_left-SN,1,1,Tscale,Econd,1) / Rho_cn;
+ }
+ else
+ GN = 0;
+ if(E_left > BP)
+ {
+ T_p = U_Temp(Z_left-1,A_left-1,E_left-BP,1,1,Tscale,Econd);
+ GP = pow(A_left-1,0.666667) * 0.13 * pow(T_p,2) * U_levdens(Z_left-1,A_left-1,E_left-BP,1,1,Tscale,Econd,1) / Rho_cn;
+ }
+ else
+ GP = 0;
+
+ float FcollA, EcollA, FcollB, EcollB;
+ EcollA = E_left - BFANP;
+ if(EcollA < 0)
+ EcollA = 0;
+ FcollA = GA / (1. - (1. - GA) * exp(-EcollA/F1_coll));
+ FtunnA = 1./(1.+exp(-(E_left-BFA)/Tequi));
+ GAmod = GA / (FtunnA * FcollA);
+ EcollB = E_left - BFBNP;
+ if(EcollB < 0)
+ EcollB = 0;
+ FcollB = GB / (1. - (1. - GB) * exp(-EcollB/F1_coll));
+ FtunnB = 1./(1.+exp(-(E_left-BFB)/Tequi));
+ GBmod = GB / (FtunnB * FcollB);
+ T_f = U_Temp2(P_Z_CN,A_left,E_left-BFMNP,DUF,0,Tscale,Econd);
+ G = GAmod * exp((BFANP-BFMNP)/T_f) + GBmod * exp((BFBNP-BFMNP)/T_f);
+ ypsilon = 1.0 - pow(P_Z_CN,2) / (P_A_CN * 50.0); // 1 - fissility
+ ypsilon = Max(ypsilon,0.1); // limitation for very heavy nuclei
+ l_lim_2 = pow(15.0,2) / (ypsilon/0.28) * T_f / TEgidy(P_A_CN,DUF,1.0); // Hasse & Myers
+ Frot = exp( pow(P_I_rms_CN,2)/l_lim_2 ); // enhancement of GF by angular momentum
+ GF = T_f / G * U_levdens(P_Z_CN,A_left-1,E_left-BFMNP,0,0,Tscale,Econd,af_an) / Rho_cn * Frot;
+ Red_diss = exp(-(E_left - BFMNP)/(F1_diss));
+ GF = GF * Red_diss;
+ // Low level density below the pairing gap
+ /* If P_Z_CN Mod 2 = 0 And A_left Mod 2 = 0 Then
+ If E_left - BFM < 2 * 12 / sqr(A_left) Then
+ GF = GF * Max(0.01 + 0.99*(Abs( (E_left-BFM) / (2*12/sqr(A_left) )) ),0.1 )
+ End If
+ Else
+ If P_Z_CN Mod 2 = 0 Or (A_left - P_Z_CN) Mod 2 = 0 Then
+ If E_left - BFM < 12 / sqr(A_left) Then
+ GF = GF * Max(0.01 + 0.99*(Abs( (E_left-BFM) / (12/sqr(A_left) )) ),0.1 )
+ End If
+ End If
+ End If */
+
+ Tm = U_Temp(P_Z_CN,A_left,E_left,1,0,Tscale,Econd); // emitting nucleus
+ Ggamma = 0.624 * pow(A_left,1.6) * pow(Tm,5); // in meV (Ignatyuk, Bologna)
+ Ggamma = Ggamma * 1.e-9; // in MeV
+
+ PF = GF / (GF + GN + GP + Ggamma); // Pfis does not include multi-chance fission
+ }
+ // cout<<"Ex: "<<Ex<<" PF: "<<PF<<endl;
+}
+
+
+void GEF::InitCompound(double vEx, double vEfis, double vLfis, double vThfis, double vPhfis)
+{
+ Ex = vEx;
+ Efis = vEfis;
+ Lfis = vLfis;
+ Thfis = vThfis;
+ Phfis = vPhfis;
+}
+
+void GEF::Treat(void)
+{
+ /*Ex = FIS.GetExcitationEnergy();
+ Lfis = 0;
+ Efis = FIS.GetEnergy();
+ Thfis = 0;
+ Phfis = 0;*/
+
+ P_E_exc = Ex;
+ P_I_rms_CN = Lfis;
+ Spin_pre_fission = P_I_rms_CN; //???????
+ PotCurv_FM();
+ R_E_exc_used = P_E_exc;
+ EnergyTrans();
+ BarriersEx_FM();
+ TCollective();
+ MeanValues_FM();
+ EnergyDependence();
+ RelationsZ_A_FM();//second interaccion after energy dependence
+ Yields_FM();
+ MassWidths_FM();
+ ShellEff_FM();
+
+ IntrinsicT();
+ IntrinsicEx();
+#ifndef GEF_SIMPLE
+ FF_angularMomentum();
+#endif
+
+ FissionModeChoise();
+ ZAChoise();
+ N_Saddle_Scission();
+ FragmentsEnergy();
+ FissionProbability();
+
+ FromCMtoLAB();
+
+ Qffl = Qffh = 0;
+ Qffl = int(rn->Gaus(Qmean_Baron(1.*I_Z_light_sci, vlab_light),Qsigma_Baron(1.*I_Z_light_sci, vlab_light)) +.5);
+ Qffh = int(rn->Gaus(Qmean_Baron(1.*I_Z_heavy_sci, vlab_heavy),Qsigma_Baron(1.*I_Z_heavy_sci, vlab_heavy))+0.5);
+ Brhoffl = Brhoffh=0.;
+ if(Qffl>0)
+ Brhoffl = 3.105*I_A_light_sci/Qffl*Blab_light*Glab_light;
+ if(Qffh>0)
+ Brhoffh = 3.105*I_A_heavy_sci/Qffh*Blab_heavy*Glab_heavy;
+}
+
+/*void GEF::outAttach(TTree *outT)
+ {
+ outT->Branch("Zffl",&I_Z_light_sci,"Zffl/I");
+ outT->Branch("Zffh",&I_Z_heavy_sci,"Zffh/I");
+ outT->Branch("Affl",&I_A_light_sci,"Affl/I");
+ outT->Branch("Affh",&I_A_heavy_sci,"Affh/I");
+ outT->Branch("Qffl",&Qffl,"Qffl/I");
+ outT->Branch("Qffh",&Qffh,"Qffh/I");
+ outT->Branch("KECMffl",&Ekinlight_sci,"KECMffl/F");
+ outT->Branch("KECMffh",&Ekinheavy_sci,"KECMffh/F");
+ outT->Branch("ThCMffl",&Thcm_light,"ThCMffl/F");
+ outT->Branch("ThCMffh",&Thcm_heavy,"ThCMffh/F");
+ outT->Branch("PhCMffl",&Phcm_light,"PhCMffl/F");
+ outT->Branch("PhCMffh",&Phcm_heavy,"PhCMffh/F");
+ outT->Branch("KELabffl",&KElab_light,"KELabffl/F");
+ outT->Branch("KELabffh",&KElab_heavy,"KELabffh/F");
+ outT->Branch("VLabffl",&vlab_light,"VLabffl/F");
+ outT->Branch("VLabffh",&vlab_heavy,"VLabffh/F");
+ outT->Branch("ThLabffl",&Thlab_light,"Thlabffl/F");
+ outT->Branch("ThLabffh",&Thlab_heavy,"Thlabffh/F");
+ outT->Branch("PhLabffl",&Phlab_light,"Phlabffl/F");
+ outT->Branch("PhLabffh",&Phlab_heavy,"Phlabffh/F");
+ outT->Branch("Brhoffl",&Brhoffl,"Brhoffl/F");
+ outT->Branch("Brhoffh",&Brhoffh,"Brhoffh/F");
+// outT->Branch("ThLabLabffl",&Thlablab_light,"ThLabLabffl/F");
+outT->Branch("FissionProb",&PF,"FissionProb/F");
+
+
+}*/
+
+
+
+
+
+
diff --git a/NPLib/Physics/GEF.h b/NPLib/Physics/GEF.h
new file mode 100644
index 0000000000000000000000000000000000000000..35add9b016b64443995d8653cf599a24cf900dc6
--- /dev/null
+++ b/NPLib/Physics/GEF.h
@@ -0,0 +1,584 @@
+#ifndef GEF_CLASS
+#define GEF_CLASS
+
+#include <iostream>
+#include <iomanip>
+#include <sstream>
+#include <fstream>
+#include <algorithm>
+#include <exception>
+#include <vector>
+#include <list>
+#include <stdlib.h>
+#include <stdio.h>
+#include <math.h>
+#include <cstring>
+#include <string>
+#include <ctime>
+#include <fcntl.h>
+#include <unistd.h>
+
+#include <sys/stat.h>
+#include <time.h>
+#include <typeinfo>
+
+#include <TROOT.h>
+#include <TFile.h>
+#include <TDirectory.h>
+#include <TObject.h>
+#include <TTree.h>
+#include <TVector3.h>
+#include <TLorentzVector.h>
+#include <TMath.h>
+#include <TKey.h>
+#include <TRandom3.h>
+
+using namespace std;
+
+//#endif
+
+//#define GEF_SIMPLE
+
+// NPTool headers
+#include "NPParticle.h"
+
+class GEF
+{
+public:
+ GEF(NPL::Particle FissNucl);
+ ~GEF(void);
+
+ inline double GetBrhoffl(void){return Brhoffl;}
+ inline double GetBrhoffh(void){return Brhoffh;}
+ inline double GetThffl(void){return Thlab_light;}
+ inline double GetThffh(void){return Thlab_heavy;}
+ inline double GetPhffl(void){return Phlab_light;}
+ inline double GetPhffh(void){return Phlab_heavy;}
+ inline float GetKEffl(void){return KElab_light;}
+ inline float GetKEffh(void){return KElab_heavy;}
+ inline float GetVffl(void){return vlab_light;}
+ inline float GetVffh(void){return vlab_heavy;}
+ inline int GetZffl(void){return I_Z_light_sci;}
+ inline int GetZffh(void){return I_Z_heavy_sci;}
+ inline int GetAffl(void){return I_A_light_sci;}
+ inline int GetAffh(void){return I_A_heavy_sci;}
+
+ float* GetNeutronEnergyFrag1() {return Array_E_n1_frag1;}
+ float* GetNeutronEnergyFrag2() {return Array_E_n2_frag2;}
+ float GetTKE() {return TKE;}
+ float GetKE1() {return Ekinlight_sci;}
+ float GetKE2() {return Ekinheavy_sci;}
+
+ void Treat(void);
+ void InitCompound(double vEx, double vEfis, double vLfis=0, double vThfis=0, double vPhfis=0);
+ bool IsValid(int Z, int A);
+
+private:
+ NPL::Particle FIS;
+ Int_t Afis;
+ Int_t Zfis;
+ Float_t Ex;
+ Float_t Lfis; //hbar
+ Float_t Efis;
+ Float_t Thfis;
+ Float_t Phfis;
+
+ Float_t BEldmTF[204][137]; //[N][Z]
+ void ReadBEldmTF(void);
+ Float_t BEexp[204][137]; //[N][Z]
+ void ReadBEexp(void);
+ Float_t DEFOtab[237][137]; //[N][Z]
+ void ReadDEFOtab(void);
+ Float_t ShellMO[204][137]; //[N][Z]
+ void ReadShellMO(void);
+ Float_t R_SPI[112][284]; //[Z][A] //Spin ground-states
+ void ReadNucProp(void);
+
+ void ReadGEFParameters(void);
+ void Init(void);
+
+ float Max(float a, float b);
+ float Min(float a, float b);
+ float Erf(float x);
+ float Erfc(float x);
+ float Tanh(float x);
+ float Coth(float x);
+ float Log10(float R);
+ float Bell(float xpos, float xleft, float xright);
+ float Csng(int a);
+ int CInt(float a);
+ float Mod(float a, float b);
+ float FLOOR(float a);
+ float CEIL(float a);
+ int Sgn(float a);
+
+ void FissionGENERAL(void);
+ void CentralZ_FM(void);
+ void MeanDefScission(void);
+ void MeanZ_asA(void);
+ void RelationsZ_A_FM(void);
+ void PotCurv_FM(void);
+ void EnergyTrans(void);
+ void FissionBarriers(void);
+ void BarriersEx_FM(void);
+ void TCollective(void);
+ void PolarizationStiffness(void);
+ void MeanValues_FM(void);
+ void EnergyDependence(void);
+ void Yields_FM(void);
+ void MassWidths_FM(void);
+ void ShellEff_FM(void);
+ void IntrinsicT(void);
+ void IntrinsicEx(void);
+ void FF_angularMomentum(void);
+
+ void FissionModeChoise(void);
+ void ZAChoise(void);
+ void N_Saddle_Scission(void);
+ void FragmentsEnergy(void);
+ void FromCMtoLAB(void);
+ void FissionProbability(void);
+
+
+ float Getyield(float E_rel,float E_ref, float T_low, float T_high);
+ float F1(float Z_S_A);
+ float F2(float Z_S_A);
+ float Masscurv(float Z, float A, float RL, float kappa);
+ float Masscurv1(float Z,float A, float RL, float kappa);
+ float De_Saddle_Scission(float Z_square_over_Athird,float ESHIFTSASCI);
+ float TEgidy(float A,float DU, float Fred);
+ float TRusanov(float E, float A);
+ float LyMass(float Z, float A, float beta);
+ float LyPair(int Z, int A);
+ float TFPair(int Z, int A);
+ float Pmass(float Z, float A, float beta);
+ float FEDEFOLys(float Z, float A, float beta);
+ float FEDEFOP(float Z, float A, float beta);
+ float LDMass(float Z, float A, float beta);
+ float AME2012(int IZ, int IA);
+ float U_SHELL(int Z, int A);
+ float U_SHELL_exp(int IZ, int IA);
+ float U_SHELL_EO_exp(int IZ, int IA);
+ float U_MASS(float Z, float A);
+ float ECOUL(float Z1, float A1, float beta1, float Z2, float A2, float beta2, float d);
+ float beta_light(int Z, float betaL0, float betaL1);
+ float beta_heavy(int Z, float betaH0, float betaH1);
+ float Z_equi(int ZCN, int A1, int A2, float beta1, float beta2, float d, int Imode);
+ void Beta_opt_light(float A1, float A2, float Z1, float Z2, float d, float beta2_imposed, float &beta1_opt);
+ void Beta_Equi(float A1, float A2, float Z1, float Z2, float d, float beta1prev, float beta2prev, float &beta1opt, float &beta2opt);
+ void Eva(int Ilh, float Z_CN, float A_CN, float E_INIT, float T, float J_frag, float &Z_RES, float &A_RES, float &E_FINAL, float *Array_En, float *Array_Tn, float *Array_Eg0); // it is not well translated from Visual BASIC need to be checked
+ float u_accel(float A1, float Z1, float A2, float Z2, float TKE , float E0, float Tn);
+ float P_Egamma_high(float Zi, float Ai, float Ei);
+ float P_Egamma_low(float Zi, float Ai, float Ei);
+ float U_Ired(float Z, float A);
+ float U_IredFF(float Z, float A);
+ float U_I_Shell(float Z, float A);
+ float U_alev_ld(float Z, float A);
+ float U_Temp(float Z, float A, float E, int Ishell, int Ipair, float Tscale, float Econd);
+ double U_levdens_Egidy(int Z, int A, float E, int Ishell, int Ipair, float Tscale, float Econd, float af_an);
+ double U_levdens_FG(int Z, int A, float E, int Ishell, int Ipair, float Tscale, float Econd, float af_an);
+ double U_levdens(int Z, int A, float E, int Ishell, float Ipair, float Tscale, float Econd, float af_an);
+ float U_Temp2(float Z, float A, float E, float Rshell, float Rpair, float Tscale, float Econd);
+ float E0_GDR(float Z, float A);
+ float Width_GDR(float E0);
+ //float Sigma_GDR(float Z, float A, float E, float E0, float WidthK);//function not defined in GEF
+ float Efac_def_GDR(float Beta, float Gamma, float K);
+ // float TK_GDR(float Z, float A, float E); //function not defined in GEF
+ float GgGtot(float Z, float A, float E, float Egamma);
+ float E_next(float T1, float T2, float E1, float E2, float A1, float A2);
+ int EVEN_ODD(float R_ORIGIN,float R_EVEN_ODD);
+ float U_Even_Odd(int I_Channel, float PEO);
+ float BFTF(float RZ, float RA, int I_Switch);
+ float BFTFA(float RZ, float RA, int I_Switch);
+ float BFTFB(float RZ, float RA, int I_Switch);
+ float Gaussintegral(float R_x, float R_sigma);
+
+ float U_Box(float x, float sigma, float width);
+ float U_Box2(float x, float sigma1, float sigma2, float width);
+ float U_Gauss(float x, float sigma);
+ float U_Gauss_abs(float x, float sigma);
+ float U_Gauss_mod(float x,float sigma);
+ float U_LinGauss(float x, float R_Sigma);
+ float Round(float R, int N);
+ float Pexplim(float R_lambda, float xmin, float xmax);
+ float PBox(float Mean, float Sigma, float Bottom);
+ float PBox2(float Mean, float Sigma1, float Sigma2, float Bottom);
+ float PPower(int Order, float Rmin, float Rmax);
+ float PPower_Griffin_v(int Order, float Rmin, float Rmax);
+ float PPower_Griffin_E(int Order, float Rmin,float Rmax);
+ float PGauss(float Mean, float Sigma);
+ float PLinGauss(float R_Sigma);
+ float PExp(float R_Tau);
+ float PMaxwell(float R_T);
+ float PMaxwellMod(float R_T, float R_A);
+ float PMaxwellv(float R_T);
+ long int Modulo(unsigned long int I, unsigned long int J);
+ //int PLoss(unsigned long int IL); //I don't know yet how to translate this function to C++
+ bool U_Valid(int I_Z, int I_A);
+ float U_Delta_S0(int I_Z, int I_A);
+
+
+ float pi;
+ TRandom3 *rn;
+
+ //Internal variables
+
+ int I_N_CN; // Neutron number of fissioning nucleus
+ float T_Coll_Mode_1,T_Coll_Mode_2,T_Coll_Mode_3,T_Coll_Mode_4;
+ float T_asym_Mode_1,T_asym_Mode_2,T_asym_Mode_3,T_asym_Mode_4,T_asym_Mode_0;
+ float Sigpol_Mode_1,Sigpol_Mode_2,Sigpol_Mode_3,Sigpol_Mode_4;
+ float R_Z_Curv_S0,R_Z_Curv1_S0,R_A_Curv1_S0;
+ float ZC_Mode_0,ZC_Mode_1,ZC_Mode_2,ZC_Mode_3,ZC_Mode_4;
+ float ZC_Mode_3_shift;
+ float SigZ_Mode_0,SigZ_Mode_1,SigZ_Mode_2,SigZ_Mode_3,SigZ_Mode_4;
+ float SigZ_SL4;
+ float SN,Sprot;
+ float E_exc_S0_prov,E_exc_S1_prov,E_exc_S2_prov,E_exc_S3_prov,E_exc_S4_prov;
+ float E_exc_S11_prov,E_exc_S22_prov;
+ float E_exc_Barr;
+ float E_LD_S1,E_LD_S2,E_LD_S3,E_LD_S4;
+ float R_Shell_S1_eff,R_Shell_S2_eff,R_Shell_S3_eff,R_Shell_S4_eff;
+ float Yield_Norm;
+ float R_E_exc_eff;
+ float R_Z_Heavy,R_Z_Light;
+ int I_Mode;
+ float T_Pol_Mode_0,T_Pol_Mode_1,T_Pol_Mode_2,T_Pol_Mode_3,T_Pol_Mode_4;
+ float E_Min_Barr;
+ float RI;
+ float rbeta, beta1, beta2;
+ float rbeta_ld, rbeta_shell;
+ float ZUCD;
+ float Z;
+ float E_tunn;
+ float beta1_opt,beta2_opt,beta1_prev,beta2_prev;
+ float Z1,Z2;
+ int IZ1,IN1,IZ2,IN2;
+ float A1,A2;
+ int IA1,IA2;
+ float E_defo;
+ float R_Pol_Curv_S0, R_Pol_Curv_S1, R_Pol_Curv_S2,R_Pol_Curv_S3,R_Pol_Curv_S4;
+ float RA,RZ;
+ float SigA_Mode_0, SigA_Mode_1, SigA_Mode_2,SigA_Mode_3,SigA_Mode_4;
+ float AC_Mode_0, AC_Mode_1, AC_Mode_2, AC_Mode_3, AC_Mode_4;
+ float R_A_heavy, R_A_light;
+ float RZpol;
+
+ float Eexc_light,Eexc_heavy;
+
+ float T_intr_Mode_0,T_intr_Mode_1_heavy,T_intr_Mode_1_light;
+ float T_intr_Mode_2_heavy,T_intr_Mode_2_light;
+ float T_intr_Mode_3_heavy,T_intr_Mode_3_light;
+ float T_intr_Mode_4_heavy,T_intr_Mode_4_light;
+ float T;
+ float DU0,DU1,DU2,DU3,DU4;
+
+ float E_intr,E_intr_light,E_intr_heavy;
+ float E_intr_light_S0_mac,E_intr_heavy_S0_mac,RW_mac;
+ float E_intr_light_S0_mic,E_intr_heavy_S0_mic;
+ float E_intr_light_mean,E_intr_heavy_mean;
+ float Eexc_heavy_mean, Eexc_light_mean;
+ float Ecoll,Ecoll_mean,Ecoll_heavy,Ecoll_light;
+ const static float E_EXC_TRUE,E_EXC_ISO; // Excitation energy of isomeric state
+ float Qvalue,TKEmin;
+ float Rtest;
+ float Theavy,Tlight;
+
+ float T_low_S1_used;
+ float SigA_Mode_11,SigA_Mode_22;
+ int Ngtot;
+ int Nglight;
+ int Ngheavy;
+ float Egtot1000;
+ float S1_enhance, S2_enhance, S1_enhance_S2;
+ float DZ_S2_lowE;
+ int I_A_CN,I_Z_CN;
+ float R_E_exc_used;
+
+ float TKE, TKE_post, Ekinlight, Ekinheavy, Ekinlight_post, Ekinheavy_post;
+ float Ekinlight_sci, Ekinheavy_sci;
+ float vkinlight,vkinheavy;
+
+ // float Beta(-1 To 6,1 To 2,150);
+ // -1: microscopic; 0: macroscopic for S0 fission channel
+ float Beta[8][3][151]; //******remember to add Beta[a+1][b][c] in the translation***********
+ float Edefo[6][3][151];//******remember to add Edefo[a+1][b][c] in the translation***********
+ float Zmean[5][3][351];
+ float Zshift[5][3][351];
+ float ZshiftOriginal[5][3][351];
+ float Temp[5][3][351];
+ float TempFF[5][3][351];
+ float EShell[5][3][351];
+ float PEOZ[7][3][351];
+ float PEON[7][3][351]; //pre-neutron evaporation
+ float EPART[7][3][351];
+ float SpinRMSNZ[7][3][201][151];
+
+ // Input parameters:
+
+ //Dim As String kin // Key input
+ //Dim As String Cyesno
+ const static int I_thread=0; // Thread number of this process
+ // Dim Shared As UByte B_Error_On = 0 // Error analysis required
+ //Dim As UByte B_Error_Analysis
+ int N_Error_Max; // Number of different random parameter sets
+ int I_Error; // Counts the parameter sets
+ // I_Error runs from 0 to N_Error_Max - 1!
+ //Dim As UByte B_Random_on = 0 // Write ENDF random files
+ int I_DelGam;
+ int P_Z_CN; //`Z of fissioning nucleus
+ int P_A_CN; // A of fissioning nucleus
+ float P_E_exc; // Energy above lowest outer barrier EB
+
+ //Dim As UByte B_Double_Covar = 0 // Option: covariances for yields of 2 fragments
+ int I_Double_Covar; // Sequence of calculations for 2 fragments
+ int N_Double_Covar;
+ int P_Z_CN_Double;
+ int P_A_CN_Double;
+ float P_E_exc_Double;
+
+ float P_I_rms_CN; // rms initial angular momentum
+
+
+ //Model parameters of GEF
+
+ float Emax_valid; // Maximum allowed excitation energy
+ float Eexc_min_multi; // Threshold for calc. of multi-chance fission
+ float _Delta_S0; // Shell effect for SL, for individual systems
+ float EOscale; // Scaling factor for even-odd structure in yields
+ int Emode ; // 0: E over BF_B; 1: E over gs; 2: E_neutron; 12: E_proton
+ float D_Par_Fac; // Scales the variation of perturbed parameters
+ float _P_DZ_Mean_S1;
+ float _P_DZ_Mean_S2;
+ float _P_DZ_Mean_S3; // Shift of mean Z of Mode 3
+ float _P_DZ_Mean_S4; // Shell for structure at A around 190
+ float ZC_Mode_4L; // enhances S1
+ float _P_Z_Curv_S1;
+ float P_Z_Curvmod_S1; // Scales energy-dependent shift
+ float _P_Z_Curv_S2;
+ float _S2leftmod; // Asymmetry in diffuseness of S2 mass peak
+ float P_Z_Curvmod_S2; // Scales energy-dependent shift
+ float _P_A_Width_S2; // A width of Mode 2 (box)
+ float P_Cut_S2; // Divide S2 into two modes, S2a and S2b
+ float _P_Z_Curv_S3;
+ float P_Z_Curvmod_S3; // Scales energy-dependent shift
+ float P_Z_Curv_SL4;
+ float P_Z_Sigma_SL4;
+ float _P_Z_Curv_S4;
+ float P_Z_Curvmod_S4; // Scales energy-dependent shift
+ float _P_Shell_S1; // Shell effect for Mode 1 (S1)
+ float _P_Shell_S2; // Shell effect for Mode 2 (S2)
+ float _P_Shell_S3; // Shell effect for Mode 3 (SA)
+ float P_Shell_SL4; // Shell enhancing S1
+ float _P_Shell_S4; // Shell effect for Mode 4
+ float P_S4_NZmod; // Variation of S4 shell with N_CN (reference: 180Hg)
+ float PZ_S3_olap_pos; // Pos. of S3 shell in light fragment (in Z)
+ float PZ_S3_olap_curv;
+ float ETHRESHSUPPS1;
+ float ESIGSUPPS1;
+ float Level_S11; // Level for mode S11
+ float Shell_fading; // fading of shell effect with E*
+ float _T_low_S1;
+ float _T_low_S2; // Slope parameter for tunneling
+ float _T_low_S3; // Slope parameter for tunneling
+ float _T_low_S4; // Slope parameter for tunneling
+ float _T_low_SL; // Slope parameter for tunneling
+ float T_low_S11; // Slope parameter for tunneling
+ float _P_att_pol; // Attenuation length of 132Sn shell
+ float P_att_pol2;
+ float P_att_pol3;
+ float _P_att_rel; // Relative portion of attenuation
+ float dE_Defo_S1; // Deformation energy expense for Mode 1
+ float dE_Defo_S2; // Deformation energy expense for Mode 2
+ float dE_Defo_S3; // Deformation energy expense for Mode 3
+ float dE_Defo_S4; // Deformation energy expense for Mode 4
+ float betaL0;
+ float betaL1;
+ float betaH0; // Offset for deformation of heavy fragment
+ float betaH1;
+ float kappa; // N/Z dedendence of A-asym. potential
+ float TCOLLFRAC; // Tcoll per energy gain from saddle to scission
+ float ECOLLFRAC;
+ float TFCOLL;
+ float TCOLLMIN;
+ float ESHIFTSASCI_intr; // Shift of saddle-scission energy
+ float ESHIFTSASCI_coll; // Shift of saddle-scission energy
+ float EDISSFRAC;
+ float Epot_shift;
+ float SIGDEFO;
+ float SIGDEFO_0;
+ float SIGDEFO_slope;
+ float SIGENECK; // Width of TXE by fluctuation of neck length
+ float EexcSIGrel;
+ float DNECK; // Tip distance at scission / fm
+ float FTRUNC50; // Truncation near Z = 50
+ float ZTRUNC50; // Z value for truncation
+ float FTRUNC28; // Truncation near Z = 28
+ float ZTRUNC28; // Z value for truncation
+ float ZMAX_S2; // Maximum Z of S2 channel in light fragment
+ float NTRANSFEREO; // Steps for E sorting for even-odd effect
+ float NTRANSFERE; // Steps for E sorting for energy division
+ float Csort; // Smoothing of energy sorting
+ float PZ_EO_symm; // Even-odd effect in Z at symmetry
+ float PN_EO_Symm; // Even-odd effect in N at symmetry
+ float R_EO_THRESH; // Threshold for asymmetry-driven even-odd effect
+ float R_EO_SIGMA;
+ float R_EO_MAX; // Maximum even-odd effect
+ float _POLARadd; // Offset for enhanced polarization
+ float POLARfac; // Enhancement of polarization of ligu. drop
+ float T_POL_RED; // Reduction of temperature for sigma(Z)
+ float _HOMPOL; // hbar omega of polarization oscillation
+ float ZPOL1; // Extra charge polarization of S1
+ float P_n_x; // Enhanced inverse neutron x section
+ float Tscale;
+ float Econd;
+ float T_orbital; // From orbital ang. momentum
+ float _Jscaling; // General scaling of fragment angular momenta
+ float Spin_odd; // RMS Spin enhancement for odd Z
+ float Esort_extend; // Extension of energy range for E-sorting
+ float Esort_slope; // Onset of E-sorting around symmetry
+ float Esort_slope_S0; // Onset of E-sorting around symmetry for S0 channel
+
+ // Control parameters:
+ float B_F; // Fission barrier
+ float B_F_ld; // Fission barrier, liquid drop
+ float E_B; // Outer fission barrier
+ float E_B_ld; // Outer fission barrier, liquid drop
+ float R_E_exc_Eb; // Energy above outer barrier
+ float R_E_exc_GS; // Energy above ground state
+ float P_Z_Mean_S0; // Mean Z of Mode 1
+ float P_Z_Mean_S1; // Mean Z of Mode 1
+ float P_Z_Mean_S2; // Mean Z of Mode 2
+ float P_Z_Mean_S3; // Mean Z of Mode 3
+ float P_Z_Mean_S4; // Mean Z of Mode 4
+ float NC_Mode_0; // Mean N of symm. Mode
+ float NC_Mode_1; // Mean N of Mode 1
+ float NC_Mode_2; // Mean N of Mode 2
+ float NC_Mode_3; // Mean N of Mode 3
+ float NC_Mode_4;
+ float B_S1; // Barrier S1, relative to SL
+ float B_S2; // Barrier S2, relative to SL
+ float B_S3; // Barrier S3, relative to SL
+ float B_S4;
+ float B_S11; // Barrier S11, relative to SL
+ float B_S22; // Barrier S22, relative to SL
+ float DES11ZPM; // Mod. of eff. barrier due to ZPM in overlap
+ float Delta_NZ_Pol; // Polarization for 132Sn
+ float Yield_Mode_0; // Relative yield of SL
+ float Yield_Mode_1; // Relative yield of S1
+ float Yield_Mode_2; // Relative yield of S2
+ float Yield_Mode_3; // Relative yield of S3
+ float Yield_Mode_4; // Relative yield of S4
+ float Yield_Mode_11; // Relative yield of S11
+ float Yield_Mode_22; // Relative yield of S22
+ float P_POL_CURV_S0; // Stiffnes in N/Z
+ float T_Coll_Mode_0; // Effective collective temperature
+ float E_Exc_S0; // Energy over barrier of symmetric channel
+ float E_Exc_S1; // Energy over barrier of S1 channel
+ float E_Exc_S2; // Energy over barrier of S2 channel
+ float E_Exc_S3; // Energy over barrier of S3 channel
+ float E_Exc_S4; // Energy over barrier of S4 channel
+ float E_Exc_S11; // Energy over barrier of S11 channel
+ float E_Exc_S22; // Energy over barrier of S22 channel
+ float E_POT_SCISSION; // Potential-energy gain saddle-scission
+ float E_diss_Scission; // Dissipated energy between saddle and scission
+ float EINTR_SCISSION; // Intrinsic excitation energy at scission
+ float EeffS1; // Governs S1 reduction
+ float Sigpol_Mode_0; // Width of isobaric Z distribution
+
+
+ //more parameters
+ float P_DZ_Mean_S1;
+ float P_DZ_Mean_S2;
+ float P_DZ_Mean_S3;
+ float P_DZ_Mean_S4;
+ float P_Z_Curv_S1;
+ float P_Z_Curv_S2;
+ float S2leftmod;
+ float P_A_Width_S2;
+ float P_Z_Curv_S3;
+ float P_Z_Curv_S4;
+ float Delta_S0;
+ float P_Shell_S1;
+ float P_Shell_S2;
+ float P_Shell_S3;
+ float P_Shell_S4;
+ float T_low_S1;
+ float T_low_S2;
+ float T_low_S3;
+ float T_low_S4;
+ float T_low_SL;
+ float P_att_pol;
+ float P_att_rel;
+ float HOMPOL;
+ float POLARadd;
+ float Jscaling;
+
+ float Escission_lim;
+
+ float Spin_CN;
+ float Spin_pre_fission;
+ float Spin_gs_light;
+ float Spin_gs_heavy;
+
+ float R_E_intr_S1, R_E_intr_S2, R_E_intr_S3; // intrinsic exc. energies at barrier
+ float R_E_intr_S4;
+ float R_Att[7]; // attenuation of shell
+ float R_Att_Sad[7];
+
+ float Etot,E1FG,E1ES;
+ float Rincr1P,Rincr1N,Rincr2,Rincr2P,Rincr2N;
+ float T1,T2,E1,E2;
+ float E_coll_saddle[7];
+ float Ediff;
+ float DT;
+
+ float R_A_help,RN;
+ int Iguess;
+
+ float R_N_heavy;
+ int I_Z_sad, I_N_sad, I_A_sad;
+ int I_Z_heavy_sad, I_A_heavy_sad;
+ int I_Z_light_sad, I_A_light_sad;
+ int I_N_heavy_sad, I_N_light_sad;
+ int I_Z_sci, I_N_sci, I_A_sci; //sci: values at scission, before prompt-neutron emission
+ int I_Z_light_sci, I_N_light_sci, I_A_light_sci;
+ int I_Z_heavy_sci, I_N_heavy_sci, I_A_heavy_sci;
+ int I_Z_post, I_N_post, I_A_post;
+ int I_Z_light_post, I_N_light_post, I_A_light_post;
+ int I_Z_heavy_post, I_N_heavy_post, I_A_heavy_post;
+ float ESIGDEFOlight,ESIGDEFOheavy;
+ float RS;
+
+ float I_nu_ss;
+ //Input/Return parameters of subroutine Eva:
+ float Array_E_n1_frag1[51]; // neutron energy array in fragment frame
+ float Array_v_n1_frag1[51];
+ float Array_vlong_n1_frag1[51]; // neutron velocity array longitudinal
+ float Array_vperp_n1_frag1[51]; // neutron velocity array perpendicular
+ float Array_E_n2_frag2[51]; // neutron energy array in fragment frame
+ float Array_v_n2_frag2[51];
+ float Array_vlong_n2_frag2[51]; // neutron velocity array longitudinal
+ float Array_vperp_n2_frag2[51]; // neutron velocity array perpendicular
+ float Array_Tn[51]; // neutron decay times after scission
+ float Array_Eg0_light[101]; // statistical gamma energy array
+ float Array_Eg0_heavy[101]; // statistical gamma energy array
+
+ float TXE,Erotlight,Erotheavy,TXElight,TXEheavy;
+ float IfragEff_light,IfragEff_heavy;
+
+ float Thcm_light,Thcm_heavy;
+ float Phcm_light,Phcm_heavy;
+ float KElab_light, KElab_heavy;
+ float Glab_light, Glab_heavy;
+ float Blab_light, Blab_heavy;
+ float vlab_light,vlab_heavy;
+ int Qffl,Qffh;
+ float Thlab_light,Thlab_heavy;
+ float Phlab_light,Phlab_heavy;
+ float Brhoffl,Brhoffh;
+ //float Thlablab_light,Thlablab_heavy;
+ //float Phlablab_light,Phlablab_heavy;
+ float PF;
+
+};
+#endif
diff --git a/NPLib/Physics/NPFissionDecay.cxx b/NPLib/Physics/NPFissionDecay.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..f2563bfceb4950b69b1bff5c90408b806b3a7315
--- /dev/null
+++ b/NPLib/Physics/NPFissionDecay.cxx
@@ -0,0 +1,196 @@
+/*****************************************************************************
+ * Copyright (C) 2009-2016 this file is part of the NPTool Project *
+ * *
+ * For the licensing terms see $NPTOOL/Licence/NPTool_Licence *
+ * For the list of contributors see $NPTOOL/Licence/Contributors *
+ *****************************************************************************/
+
+/*****************************************************************************
+ * *
+ * Original Author : Pierre Morfouace contact: pierre.morfouace2@cea.fr *
+ * *
+ * Creation Date : Octobre 2020 *
+ * Last update : *
+ *---------------------------------------------------------------------------*
+ * Decription: *
+ * This Class hold data for fission decay of a given nuclei *
+ * *
+ * *
+ * *
+ *---------------------------------------------------------------------------*
+ * Comment: *
+ * *
+ * *
+ * *
+ *****************************************************************************/
+#include "NPFissionDecay.h"
+#include <iostream>
+#include "NPOptionManager.h"
+#include "NPFunction.h"
+#include "NPCore.h"
+#include "TF1.h"
+#include "TRandom.h"
+////////////////////////////////////////////////////////////////////////////////
+//////////////////////////// Fission Decay //////////////////////////////////////
+////////////////////////////////////////////////////////////////////////////////
+
+NPL::FissionDecay::FissionDecay(std::string compound, std::string fission_model){
+
+ m_FissionModelName = fission_model;
+ m_CompoundName = compound;
+}
+
+////////////////////////////////////////////////////////////////////////////////
+void NPL::FissionDecay::ReadConfiguration(NPL::InputParser parser){
+ vector<NPL::InputBlock*> blocks = parser.GetAllBlocksWithToken("FissionDecay");
+
+ if(blocks.size()>0 && NPOptionManager::getInstance()->GetVerboseLevel())
+ cout << endl << "\033[1;35m//// Fission decay found" << std::endl;
+
+ std::vector<std::string> token =
+ {"CompoundNucleus","FissionModel","Shoot_FF","Shoot_neutron","Shoot_gamma"};
+
+ unsigned int size = blocks.size();
+ for(unsigned int i = 0 ; i < size ; i++){
+ if(blocks[i]->HasTokenList(token)){
+ m_CompoundName = blocks[i]->GetString("CompoundNucleus");
+ m_FissionModelName = blocks[i]->GetString("FissionModel");
+ m_shoot_FF = blocks[i]->GetInt("Shoot_FF");
+ m_shoot_neutron = blocks[i]->GetInt("Shoot_neutron");
+ m_shoot_gamma = blocks[i]->GetInt("Shoot_gamma");
+
+ m_Compound = NPL::Particle(m_CompoundName);
+ if(m_FissionModelName=="GEF") m_FissionModel = new GEF(m_Compound);
+ }
+ else{
+ cout << "ERROR: check your input file formatting \033[0m" << endl;
+ exit(1);
+ }
+ }
+}
+
+
+////////////////////////////////////////////////////////////////////////////////
+bool NPL::FissionDecay::GenerateEvent(string CompoundName, double MEx,double MEK,double MPx,double MPy,double MPz,
+ std::vector<NPL::Particle>& FissionFragments, std::vector<double>& Ex,
+ std::vector<double>& DEK,
+ std::vector<double>& DPx,std::vector<double>& DPy,std::vector<double>& DPz,
+ double& TKE, double &KE1, double& KE2){
+
+ bool worked=false;
+
+ FissionFragments.clear();
+ Ex.clear();
+ DEK.clear();
+ DPx.clear();
+ DPy.clear();
+ DPz.clear();
+
+ TVector3 Momentum(MPx,MPy,MPz);
+ Momentum.Unit();
+ double Theta = Momentum.Theta();
+ double Phi = Momentum.Phi();
+
+ m_Compound = NPL::Particle(CompoundName);
+ m_Compound.SetExcitationEnergy(MEx);
+ m_Compound.SetKineticEnergy(MEK);
+ if(m_FissionModelName=="GEF"){
+ if(m_FissionModel->IsValid(m_Compound.GetZ(), m_Compound.GetA())){
+ worked=true;
+ m_FissionModel->InitCompound(MEx,MEK);
+ m_FissionModel->Treat();
+
+ int Ah = m_FissionModel->GetAffh();
+ int Zh = m_FissionModel->GetZffh();
+ int Al = m_FissionModel->GetAffl();
+ int Zl = m_FissionModel->GetZffl();
+
+ double KEl = m_FissionModel->GetKEffl();
+ double KEh = m_FissionModel->GetKEffh();
+
+ NPL::Particle FFl = NPL::Particle(Zl,Al);
+ NPL::Particle FFh = NPL::Particle(Zh,Ah);
+ FFl.SetKineticEnergy(KEl);
+ FFh.SetKineticEnergy(KEh);
+
+ FissionFragments.push_back(FFl);
+ FissionFragments.push_back(FFh);
+ Ex.push_back(0);
+ Ex.push_back(0);
+ DEK.push_back(KEl);
+ DEK.push_back(KEh);
+
+ double Massl = FFl.Mass();
+ double Massh = FFh.Mass();
+ double El = KEl+Massl;
+ double Eh = KEh+Massh;
+
+ double Pl = sqrt(El*El-Massl*Massl);
+ double Ph = sqrt(Eh*Eh-Massh*Massh);
+
+ double Thetal = m_FissionModel->GetThffl();
+ double Thetah = m_FissionModel->GetThffh();
+ double Phil = m_FissionModel->GetPhffl();
+ double Phih = m_FissionModel->GetPhffh();
+
+ /*cout << endl;
+ cout << "A-> " << Al << " / " << Ah << endl;
+ cout << "Z-> " << Zl << " / " << Zh << endl;
+ cout << "Phi-> " << Phil << " / " << Phih << endl;
+ cout << "Theta-> " << Thetal << " / " << Thetah << endl;
+ cout << "KE-> " << KEl << " / " << KEh << endl;*/
+ TVector3 Momentuml = Pl * TVector3(sin(Thetal)*cos(Phil),
+ sin(Thetal)*sin(Phil),
+ cos(Thetal));
+
+ TVector3 Momentumh = Ph * TVector3(sin(Thetah)*cos(Phih),
+ sin(Thetah)*sin(Phih),
+ cos(Thetah));
+
+ DPx.push_back(Momentuml.X());
+ DPx.push_back(Momentumh.X());
+ DPy.push_back(Momentuml.Y());
+ DPy.push_back(Momentumh.Y());
+ DPz.push_back(Momentuml.Z());
+ DPz.push_back(Momentumh.Z());
+
+ TKE = m_FissionModel->GetTKE();
+ KE1 = m_FissionModel->GetKE1();
+ KE2 = m_FissionModel->GetKE2();
+
+ // Neutron emission
+ float* En1;
+ En1 = m_FissionModel->GetNeutronEnergyFrag1();
+ /*cout << "----- Neutron energy: " << endl;
+ for(int i=0; i<51; i++) {
+ cout << "En= " << En1[i] << endl;
+ }*/
+ }
+ }
+ return worked;
+}
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
+
diff --git a/NPLib/Physics/NPFissionDecay.h b/NPLib/Physics/NPFissionDecay.h
new file mode 100644
index 0000000000000000000000000000000000000000..48e28ec7f2647320cf76c7dbd5aa06a3fa88a519
--- /dev/null
+++ b/NPLib/Physics/NPFissionDecay.h
@@ -0,0 +1,81 @@
+#ifndef NPFISSIONDECAY_H
+#define NPFISSIONDECAY_H
+/*****************************************************************************
+ * Copyright (C) 2009-2016 this file is part of the NPTool Project *
+ * *
+ * For the licensing terms see $NPTOOL/Licence/NPTool_Licence *
+ * For the list of contributors see $NPTOOL/Licence/Contributors *
+ *****************************************************************************/
+
+/*****************************************************************************
+ * *
+ * Original Author : Pierre Morfouace contact: pierre.morfouace2@cea.fr *
+ * *
+ * Creation Date : Octobre 2020 *
+ * Last update : *
+ *---------------------------------------------------------------------------*
+ * Decription: *
+ * This Class hold data for fission decay of a given nuclei *
+ * *
+ * *
+ * *
+ *---------------------------------------------------------------------------*
+ * Comment: *
+ * *
+ * *
+ * *
+ * *
+ *****************************************************************************/
+// C++ header
+#include <string>
+#include <vector>
+#include <set>
+
+// NPL Header
+#include "NPInputParser.h"
+#include "NPParticle.h"
+#include "GEF.h"
+
+namespace NPL{
+ class FissionDecay{
+ public:
+ FissionDecay(){};
+ FissionDecay(std::string compound, std::string fission_model);
+ ~FissionDecay(){};
+
+ public:
+ void ReadConfiguration(std::string Path);
+ void ReadConfiguration(NPL::InputParser parser);
+
+ private:
+ GEF* m_FissionModel;
+ std::string m_FissionModelName;
+ std::string m_CompoundName;
+ NPL::Particle m_Compound;
+ double m_MotherMass;
+ std::vector<std::string> m_FissionFragmentName;
+ std::vector<NPL::Particle> m_FissionFragment;
+ std::vector<double> m_FissionFragmentMasses;
+
+ bool m_shoot_FF;
+ bool m_shoot_neutron;
+ bool m_shoot_gamma;
+
+ public:
+ // Given Energy and Momentum direction of the compound,
+ // Send back Momemtum and Energy of fission fragments
+ // Return false if the fission is not possible
+ bool GenerateEvent(string CompoundName, double MEx,double MEK,double MPx, double MPy,double MPz,
+ std::vector<NPL::Particle>& FissionFragments, std::vector<double>& Ex,
+ std::vector<double>& DEK,
+ std::vector<double>& DPx,std::vector<double>& DPy,std::vector<double>& DPz,
+ double& TKE, double& KE1, double& KE2);
+
+ public:// Getter
+ inline std::vector<std::string> GetFissionFragmentName() {return m_FissionFragmentName;};
+ inline std::vector<NPL::Particle> GetFissionFragment() {return m_FissionFragment;};
+ inline NPL::Particle GetCompound() {return m_Compound;};
+ inline std::string GetCompoundName() {return m_CompoundName;};
+ };
+ }
+#endif
diff --git a/NPLib/Physics/PAR_GEF/BEexp.dat b/NPLib/Physics/PAR_GEF/BEexp.dat
new file mode 100644
index 0000000000000000000000000000000000000000..529f6a9efdba88470d6ff40db4b7f9aaeb836112
--- /dev/null
+++ b/NPLib/Physics/PAR_GEF/BEexp.dat
@@ -0,0 +1,3356 @@
+' This table was produced from the 2012 Mass evaluation.
+' It contains experimental masses and systematic estimations.
+' See kh/Dokumente/Literature/Full-Text-Special/Masses-2012/MakeTable.jbas.
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\ No newline at end of file
diff --git a/NPLib/Physics/PAR_GEF/BEldmTF.dat b/NPLib/Physics/PAR_GEF/BEldmTF.dat
new file mode 100644
index 0000000000000000000000000000000000000000..424a7cfcd359a3b327e4b1fd8d696ef9d915a52f
--- /dev/null
+++ b/NPLib/Physics/PAR_GEF/BEldmTF.dat
@@ -0,0 +1,1410 @@
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diff --git a/NPLib/Physics/PAR_GEF/DEFO.dat b/NPLib/Physics/PAR_GEF/DEFO.dat
new file mode 100644
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+ 120 199 0.331 0.007
+ 120 200 0.331 -0.001
+ 120 201 0.331 -0.001
+ 120 202 0.331 -0.001
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+ 120 206 0.322 -0.003
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+ 120 208 0.324 -0.028
+ 120 209 0.325 -0.046
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+ 120 211 0.335 -0.06
+ 120 212 0.335 -0.059
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+ 120 214 0.17 0.02
+ 120 215 0.135 -0.009
+ 120 216 0.116 -0.027
+ 120 217 0.108 -0.044
+ 120 218 0.108 -0.044
+ 120 219 0.108 -0.044
+ 121 169 -0.138 0.015
+ 121 170 -0.138 0.016
+ 121 171 -0.138 0.023
+ 121 172 -0.138 0.023
+ 121 173 -0.122 0.021
+ 121 174 0.072 -0.046
+ 121 175 0.072 -0.047
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+ 121 177 -0.087 -0.012
+ 121 178 -0.07 -0.013
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+ 121 183 0 -0.008
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+ 121 189 0.003 -0.005
+ 121 190 0.003 -0.005
+ 121 191 0.004 -0.012
+ 121 192 0.005 -0.004
+ 121 193 0.005 -0.01
+ 121 194 0.006 -0.003
+ 121 195 0.531 0.133
+ 121 196 0.531 0.134
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+ 121 198 0.543 0.111
+ 121 199 0.341 0.002
+ 121 200 0.331 0.007
+ 121 201 0.331 -0.001
+ 121 202 0.331 0.007
+ 121 203 0.331 0.007
+ 121 204 0.331 0.006
+ 121 205 0.331 0.006
+ 121 206 0.331 -0.001
+ 121 207 0.332 -0.01
+ 121 208 -0.471 0.031
+ 121 209 0.334 -0.043
+ 121 210 0.335 -0.051
+ 121 211 0.335 -0.06
+ 121 212 0.335 -0.059
+ 121 213 0.406 0.077
+ 121 214 0.17 0.027
+ 121 215 0.17 0.02
+ 121 216 0.143 -0.001
+ 121 217 0.116 -0.028
+ 121 218 0.108 -0.044
+ 122 172 -0.155 0.025
+ 122 173 -0.138 0.023
+ 122 174 -0.13 0.015
+ 122 175 0.08 -0.046
+ 122 176 -0.096 -0.011
+ 122 177 -0.096 -0.02
+ 122 178 0.009 -0.024
+ 122 179 0.009 -0.015
+ 122 180 0.418 0.026
+ 122 181 -0.008 -0.008
+ 122 182 0 -0.008
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+ 122 186 0.001 -0.007
+ 122 187 0.003 -0.006
+ 122 188 0.003 -0.005
+ 122 189 0.004 -0.004
+ 122 190 0.005 -0.004
+ 122 191 0.005 -0.011
+ 122 192 0.006 -0.003
+ 122 193 0.007 -0.009
+ 122 194 0.007 -0.002
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+ 122 196 0.541 0.128
+ 122 197 0.542 0.121
+ 122 198 0.543 0.112
+ 122 199 0.543 0.103
+ 122 200 0.331 0.007
+ 122 201 0.331 0
+ 122 202 0.331 0.007
+ 122 203 0.331 0.007
+ 122 204 0.331 0.007
+ 122 205 0.331 -0.001
+ 122 206 0.331 -0.001
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+ 122 209 0.334 -0.043
+ 122 210 0.335 -0.051
+ 122 211 0.335 -0.059
+ 122 212 0.336 -0.059
+ 122 213 0.336 -0.068
+ 122 214 0.189 0.022
+ 122 215 0.18 0.021
+ 122 216 0.17 0.02
+ 122 217 0.161 0.01
+ 123 174 -0.173 0.026
+ 123 175 -0.205 0.047
+ 123 176 -0.205 0.047
+ 123 177 -0.213 0.055
+ 123 178 0.408 0.029
+ 123 179 0.408 0.029
+ 123 180 0.418 0.026
+ 123 181 -0.008 -0.015
+ 123 182 0 -0.008
+ 123 183 0 -0.008
+ 123 184 0 0
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+ 123 186 0.003 -0.006
+ 123 187 0.004 -0.005
+ 123 188 0.004 -0.004
+ 123 189 0.005 -0.004
+ 123 190 0.005 -0.003
+ 123 191 0.006 -0.01
+ 123 192 0.006 -0.003
+ 123 193 0.007 -0.009
+ 123 194 0.007 -0.002
+ 123 195 0.531 0.133
+ 123 196 0.531 0.134
+ 123 197 0.542 0.121
+ 123 198 0.543 0.111
+ 123 199 0.543 0.103
+ 123 200 0.341 0.002
+ 123 201 0.331 0
+ 123 202 0.331 0.007
+ 123 203 0.331 0.008
+ 123 204 0.331 0.007
+ 123 205 0.331 0
+ 123 206 0.331 -0.001
+ 123 207 0.332 -0.009
+ 123 208 0.332 -0.018
+ 123 209 0.334 -0.043
+ 123 210 0.335 -0.05
+ 123 211 0.335 -0.059
+ 123 212 0.336 -0.059
+ 123 213 0.336 -0.068
+ 123 214 0.197 0.031
+ 123 215 0.189 0.022
+ 123 216 0.18 0.021
+ 124 176 0.053 -0.031
+ 124 177 0.045 -0.023
+ 124 178 0.409 0.022
+ 124 179 0.409 0.022
+ 124 180 0.419 0.017
+ 124 181 0.419 0.018
+ 124 182 0 -0.008
+ 124 183 0 -0.008
+ 124 184 0.001 0.001
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+ 124 186 0.004 -0.005
+ 124 187 0.005 -0.004
+ 124 188 0.005 -0.004
+ 124 189 0.006 -0.003
+ 124 190 0.006 -0.003
+ 124 191 0.007 -0.009
+ 124 192 0.007 -0.002
+ 124 193 0.422 -0.016
+ 124 194 0.531 0.134
+ 124 195 0.531 0.134
+ 124 196 0.541 0.129
+ 124 197 0.542 0.121
+ 124 198 0.543 0.112
+ 124 199 0.543 0.103
+ 124 200 0.543 0.103
+ 124 201 0.331 0
+ 124 202 0.331 0
+ 124 203 0.331 0.008
+ 124 204 0.331 0
+ 124 205 0.331 0
+ 124 206 0.331 0
+ 124 207 0.333 -0.017
+ 124 208 0.333 -0.025
+ 124 209 0.334 -0.043
+ 124 210 0.335 -0.05
+ 124 211 0.336 -0.059
+ 124 212 0.336 -0.059
+ 124 213 0.336 -0.067
+ 124 214 -0.486 0.045
+ 124 215 0.198 0.024
+ 125 178 0.419 0.017
+ 125 179 0.409 0.022
+ 125 180 0.419 0.018
+ 125 181 -0.008 -0.008
+ 125 182 0 -0.008
+ 125 183 0 -0.008
+ 125 184 0.002 0.002
+ 125 185 0.004 -0.004
+ 125 186 0 0
+ 125 187 0.005 -0.003
+ 125 188 0.005 0.005
+ 125 189 0.006 0.005
+ 125 190 0.006 0.006
+ 125 191 0.007 -0.002
+ 125 192 0.007 0.006
+ 125 193 0.423 -0.016
+ 125 194 0.531 0.134
+ 125 195 0.531 0.134
+ 125 196 0.532 0.124
+ 125 197 0.542 0.121
+ 125 198 0.543 0.111
+ 125 199 0.543 0.103
+ 125 200 0.543 0.103
+ 125 201 0.331 0.001
+ 125 202 0.543 0.102
+ 125 203 0.331 0.008
+ 125 204 0.331 0.001
+ 125 205 0.331 0
+ 125 206 0.341 -0.006
+ 125 207 0.333 -0.017
+ 125 208 0.342 -0.022
+ 125 209 0.334 -0.042
+ 125 210 0.335 -0.05
+ 125 211 0.336 -0.059
+ 125 212 0.336 -0.058
+ 125 213 0.336 -0.059
+ 125 214 -0.486 0.052
+ 126 180 0.419 0.018
+ 126 181 0.419 0.018
+ 126 182 0.001 -0.007
+ 126 183 0.002 -0.006
+ 126 184 0 0
+ 126 185 0.005 -0.004
+ 126 186 0.005 0.004
+ 126 187 0.006 -0.003
+ 126 188 0.006 -0.003
+ 126 189 0.006 -0.002
+ 126 190 0.007 -0.002
+ 126 191 0.007 -0.002
+ 126 192 0.008 -0.001
+ 126 193 0.433 -0.02
+ 126 194 0.433 -0.021
+ 126 195 0.531 0.134
+ 126 196 0.541 0.129
+ 126 197 0.542 0.121
+ 126 198 0.543 0.112
+ 126 199 0.543 0.103
+ 126 200 0.543 0.103
+ 126 201 0.331 0.001
+ 126 202 0.331 0.001
+ 126 203 0.332 0.001
+ 126 204 0.331 0.001
+ 126 205 0.332 -0.008
+ 126 206 0.332 -0.008
+ 126 207 0.333 -0.017
+ 126 208 0.334 -0.033
+ 126 209 0.334 -0.042
+ 126 210 0.335 -0.05
+ 126 211 0.336 -0.058
+ 126 212 0.336 -0.058
+ 126 213 0.336 -0.067
+ 127 183 0.004 -0.005
+ 127 184 0.005 -0.004
+ 127 185 0.005 -0.011
+ 127 186 0.006 -0.003
+ 127 187 0.006 -0.01
+ 127 188 0.007 -0.002
+ 127 189 0.007 -0.009
+ 127 190 0.008 -0.008
+ 127 191 0.445 -0.024
+ 127 192 0.433 -0.019
+ 127 193 0.434 -0.029
+ 127 194 0.434 -0.029
+ 127 195 0.531 0.134
+ 127 196 0.541 0.129
+ 127 197 0.542 0.121
+ 127 198 0.543 0.112
+ 127 199 0.543 0.103
+ 127 200 0.543 0.103
+ 127 201 0.543 0.102
+ 127 202 0.543 0.102
+ 127 203 0.332 0.001
+ 127 204 0.332 0.001
+ 127 205 0.332 -0.008
+ 127 206 0.342 -0.015
+ 127 207 0.333 -0.024
+ 127 208 0.343 -0.031
+ 127 209 0.344 -0.047
+ 127 210 0.345 -0.056
+ 127 211 0.336 -0.058
+ 127 212 0.336 -0.058
+ 128 185 0.005 -0.003
+ 128 186 0.006 -0.003
+ 128 187 0.006 -0.003
+ 128 188 0.007 -0.002
+ 128 189 0.007 -0.002
+ 128 190 0.008 -0.001
+ 128 191 0.445 -0.024
+ 128 192 0.445 -0.024
+ 128 193 0.434 -0.029
+ 128 194 0.434 -0.029
+ 128 195 0.424 -0.033
+ 128 196 0.542 0.121
+ 128 197 0.542 0.121
+ 128 198 0.543 0.112
+ 128 199 0.543 0.103
+ 128 200 0.543 0.103
+ 128 201 0.543 0.103
+ 128 202 0.543 0.102
+ 128 203 0.332 -0.008
+ 128 204 0.332 -0.008
+ 128 205 0.332 -0.008
+ 128 206 0.333 -0.017
+ 128 207 0.333 -0.024
+ 128 208 0.334 -0.033
+ 128 209 0.335 -0.05
+ 128 210 0.336 -0.058
+ 128 211 0.336 -0.058
+ 129 187 0.007 -0.009
+ 129 188 0.007 -0.002
+ 129 189 0.445 -0.022
+ 129 190 0.445 -0.023
+ 129 191 0.446 -0.032
+ 129 192 0.446 -0.033
+ 129 193 0.435 -0.037
+ 129 194 0.435 -0.038
+ 129 195 0.425 -0.042
+ 129 196 0.542 0.121
+ 129 197 0.543 0.112
+ 129 198 0.543 0.112
+ 129 199 0.543 0.103
+ 129 200 0.543 0.103
+ 129 201 0.543 0.103
+ 129 202 0.543 0.102
+ 129 203 0.332 -0.007
+ 129 204 0.332 -0.008
+ 129 205 0.332 -0.008
+ 129 206 0.333 -0.016
+ 129 207 0.334 -0.033
+ 129 208 0.407 -0.083
+ 129 209 0.398 -0.085
+ 129 210 0.345 -0.056
+ 130 189 0.008 -0.001
+ 130 190 0.008 -0.001
+ 130 191 0.456 -0.038
+ 130 192 0.446 -0.041
+ 130 193 0.446 -0.042
+ 130 194 0.435 -0.046
+ 130 195 0.542 0.121
+ 130 196 0.542 0.121
+ 130 197 0.543 0.112
+ 130 198 0.543 0.112
+ 130 199 0.543 0.103
+ 130 200 0.543 0.103
+ 130 201 0.332 -0.008
+ 130 202 0.543 0.103
+ 130 203 0.332 -0.007
+ 130 204 0.332 -0.008
+ 130 205 0.333 -0.016
+ 130 206 0.333 -0.024
+ 130 207 0.42 -0.106
+ 130 208 0.408 -0.092
+ 130 209 0.399 -0.094
+ 131 192 0.446 -0.041
+ 131 193 0.447 -0.051
+ 131 194 0.447 -0.052
+ 131 195 0.542 0.122
+ 131 196 0.543 0.112
+ 131 197 0.543 0.112
+ 131 198 0.543 0.112
+ 131 199 0.543 0.103
+ 131 200 0.543 0.103
+ 131 201 0.543 0.103
+ 131 202 0.543 0.103
+ 131 203 0.332 -0.007
+ 131 204 0.333 -0.016
+ 131 205 0.333 -0.016
+ 131 206 0.43 -0.104
+ 131 207 0.42 -0.106
+ 131 208 0.42 -0.098
+ 132 194 0.448 -0.061
+ 132 195 0.542 0.122
+ 132 196 0.543 0.112
+ 132 197 0.543 0.112
+ 132 198 0.542 0.112
+ 132 199 0.543 0.103
+ 132 200 0.543 0.103
+ 132 201 0.332 -0.007
+ 132 202 0.332 -0.007
+ 132 203 0.323 -0.01
+ 132 204 0.333 -0.016
+ 132 205 0.333 -0.024
+ 132 206 0.334 -0.033
+ 132 207 0.421 -0.115
+ 133 196 0.542 0.112
+ 133 197 0.542 0.112
+ 133 198 0.542 0.113
+ 133 199 0.543 0.103
+ 133 200 0.45 -0.089
+ 133 201 0.332 -0.007
+ 133 202 0.333 -0.016
+ 133 203 0.323 -0.009
+ 133 204 0.323 -0.01
+ 133 205 0.333 -0.024
+ 133 206 0.441 -0.119
+ 134 198 0.45 -0.088
+ 134 199 0.451 -0.096
+ 134 200 0.45 -0.097
+ 134 201 0.332 -0.007
+ 134 202 0.323 -0.009
+ 134 203 0.323 -0.009
+ 134 204 0.313 -0.012
+ 134 205 0.313 -0.012
+ 135 201 0.323 -0.009
+ 135 202 0.323 -0.009
+ 135 203 0.313 -0.012
+ 135 204 0.313 -0.012
+ 136 203 0.303 -0.005
\ No newline at end of file
diff --git a/NPLib/Physics/PAR_GEF/GEFParameters.dat b/NPLib/Physics/PAR_GEF/GEFParameters.dat
new file mode 100644
index 0000000000000000000000000000000000000000..5ff35d6998c88ab6844ef033ce9a7e3d546eff1f
--- /dev/null
+++ b/NPLib/Physics/PAR_GEF/GEFParameters.dat
@@ -0,0 +1,96 @@
+ Emax_valid 100 // Maximum allowed excitation energy
+ Eexc_min_multi 3 // Threshold for calc. of multi-chance fission
+ _Delta_S0 0 // Shell effect for SL, for individual systems
+ EOscale 1.0 // Scaling factor for even-odd structure in yields
+ Emode 1 // 0: E over BF_B 1: E over gs 2: E_neutron 12: E_proton
+ D_Par_Fac 1 // Scales the variation of perturbed parameters
+ _P_DZ_Mean_S1 -0.3
+ _P_DZ_Mean_S2 -0.4
+ _P_DZ_Mean_S3 0.2 // Shift of mean Z of Mode 3
+ _P_DZ_Mean_S4 0 // Shell for structure at A around 190
+ ZC_Mode_4L 44.4
+ _P_Z_Curv_S1 0.38
+ P_Z_Curvmod_S1 1.75 // Scales energy-dependent shift
+ _P_Z_Curv_S2 0.098
+ _S2leftmod 0.75 // Asymmetry in diffuseness of S2 mass peak
+ P_Z_Curvmod_S2 10 // Scales energy-dependent shift
+ _P_A_Width_S2 11.5 // A width of Mode 2 (box)
+ P_Cut_S2 0 // Divide S2 into two modes, S2a and S2b
+ _P_Z_Curv_S3 0.09
+ P_Z_Curvmod_S3 10 // Scales energy-dependent shift
+ P_Z_Curv_SL4 0.07
+ P_Z_Sigma_SL4 1.15
+ _P_Z_Curv_S4 0.05
+ P_Z_Curvmod_S4 10 // Scales energy-dependent shift
+ _P_Shell_S1 -3.0 // Shell effect for Mode 1 (S1)
+ _P_Shell_S2 -4.4 // Shell effect for Mode 2 (S2)
+ _P_Shell_S3 -7.2 // Shell effect for Mode 3 (SA)
+ P_Shell_SL4 -0.4
+ _P_Shell_S4 -1.0 // Shell effect for Mode 4
+ P_S4_NZmod -0.06 // Variation of S4 shell with N/Z (reference: 180Hg)
+ PZ_S3_olap_pos 39.7 // Pos. of S3 shell in light fragment (in Z)
+ PZ_S3_olap_curv 0.0045
+ ETHRESHSUPPS1 10.85
+ ESIGSUPPS1 1.0
+ Level_S11 1.6
+ Shell_fading 50 // fading of shell effect with E*
+ _T_low_S1 0.31
+ _T_low_S2 0.31 // Slope parameter for tunneling
+ _T_low_S3 0.31 // Slope parameter for tunneling
+ _T_low_S4 0.31 // Slope parameter for tunneling
+ _T_low_SL 0.31 // Slope parameter for tunneling
+ T_low_S11 0.36 // Slope parameter for tunneling
+ _P_att_pol 2.5
+ P_att_pol2 0
+ P_att_pol3 0
+ _P_att_rel 1 // Relative portion of attenuation
+ dE_Defo_S1 -2.8 // Deformation energy expense for Mode 1
+ dE_Defo_S2 0 // Deformation energy expense for Mode 2
+ dE_Defo_S3 0 // Deformation energy expense for Mode 3
+ dE_Defo_S4 0 // Deformation energy expense for Mode 4
+ betaL0 27.6
+ betaL1 0.67
+ betaH0 46.24 // Offset for deformation of heavy fragment
+ betaH1 0.60
+ kappa 0 // N/Z dedendence of A-asym. potential
+ TCOLLFRAC 0.04 // Tcoll per energy gain from saddle to scission
+ ECOLLFRAC 0.055 // Fraction of pot. energy gain from saddle to scission, going into coll. excitations
+ TFCOLL 0.034
+ TCOLLMIN 0.12
+ ESHIFTSASCI_intr -67 // Shift of saddle-scission energy
+ ESHIFTSASCI_coll -90 // Shift of saddle-scission energy
+ EDISSFRAC 0.35
+ Epot_shift 0
+ SIGDEFO 0.165
+ SIGDEFO_0 0.165
+ SIGDEFO_slope 0
+ SIGENECK 5.0 // Width of TXE by fluctuation of neck length
+ EexcSIGrel 0.7
+ DNECK 1 // Tip distance at scission / fm
+ FTRUNC50 1 // Truncation near Z 50
+ ZTRUNC50 50 // Z value for truncation
+ FTRUNC28 0.56 // Truncation near Z 28
+ ZTRUNC28 30.5 // Z value for truncation
+ ZMAX_S2 60 // Maximum Z of S2 channel in light fragment
+ NTRANSFEREO 6 // Steps for E sorting for even-odd effect
+ NTRANSFERE 12 // Steps for E sorting for energy division
+ Csort 0.5 // Smoothing of energy sorting
+ PZ_EO_symm 2.6 // Even-odd effect in Z at symmetry
+ PN_EO_Symm 2.6 // Even-odd effect in N at symmetry
+ R_EO_THRESH 0.398 // Threshold for asymmetry-driven even-odd effect
+ R_EO_SIGMA 2.0
+ R_EO_Max 0.6
+ _POLARadd 0.35 // Offset for enhanced polarization
+ POLARfac 1 // Enhancement of polarization of liqu. drop
+ T_POL_RED 0.01 // Reduction of temperature for sigma(Z)
+ _HOMPOL 1.3 // hbar omega of polarization oscillation
+ ZPOL1 0 // Extra charge polarization of S1
+ P_n_x 0 // Enhanced inverse neutron x section
+ Tscale 1
+ Econd 2
+ T_orbital 0 // From orbital ang. momentum
+ _Jscaling 1.0 // General scaling of fragment angular momenta
+ Spin_odd 0.4 // RMS Spin enhancement for odd Z
+ Esort_extend 1.5 // Extension of energy range for E-sorting
+ Esort_slope 0.04 // Onset of E-sorting around symmetry
+ Esort_slope_S0 0.2 // Onset of E-sorting around symmetry for S0 channel
diff --git a/NPLib/Physics/PAR_GEF/NucPropNUBASE.dat b/NPLib/Physics/PAR_GEF/NucPropNUBASE.dat
new file mode 100644
index 0000000000000000000000000000000000000000..e079af1aeaba290bd8aae6061f6798ae6ecffa26
--- /dev/null
+++ b/NPLib/Physics/PAR_GEF/NucPropNUBASE.dat
@@ -0,0 +1,5159 @@
+NuclideData:
+' Data extracted from NUBASE 2016.
+' MAT no., Z, A, Isomer, Spin, Parity, AWR, EXC
+' In NucPropNUBASE, AWR is the mass excess!!!
+' The MAT numbers are determined by counting.
+' They differ from the original MAT no. of JEFF 3.1.1!
+' This is necessary, because the GEFY tables cover nuclides
+' beyond the range of MAT numbers of JEFF 3.1.1.
+Data _
+ 1 0 1 0 0.5 1 8071.317 0 "t=613.9s" _
+ 2 1 1 0 0.5 1 7288.970 0 "t=stbl" _
+ 3 1 2 0 1 1 13135.721 0 "t=stbl" _
+ 4 1 3 0 0.5 1 14949.809 0 "t=12.32y" _
+ 5 2 3 0 0.5 1 14931.217 0 "t=stbl" _
+ 6 3 3 0 -77.777 0 28670 0 "t=p-unst" _
+ 7 1 4 0 2 -1 24620 0 "t=139ys" _
+ 8 2 4 0 0 1 2424.915 0 "t=stbl" _
+ 9 3 4 0 2 -1 25320 0 "t=91ys" _
+ 10 1 5 0 0.5 1 32890 0 "t=>910ys" _
+ 11 2 5 0 1.5 -1 11231 0 "t=700ys" _
+ 12 3 5 0 1.5 -1 11680 0 "t=370ys" _
+ 13 4 5 0 0.5 1 37140 0 "t=?" _
+ 14 1 6 0 2 -1 41880 0 "t=290ys" _
+ 15 2 6 0 0 1 17592.10 0 "t=806.92ms" _
+ 16 3 6 0 1 1 14086.878 0 "t=stbl" _
+ 17 4 6 0 0 1 18375 0 "t=5.0zs" _
+ 18 5 6 0 2 -1 47320 0 "t=p-unst#" _
+ 19 1 7 0 0.5 1 49140 0 "t=500#ys" _
+ 20 2 7 0 1.5 -1 26073 0 "t=2.51zs" _
+ 21 3 7 0 1.5 -1 14907.105 0 "t=stbl" _
+ 22 4 7 0 1.5 -1 15769.00 0 "t=53.22d" _
+ 23 5 7 0 1.5 -1 27677 0 "t=570ys" _
+ 24 2 8 0 0 1 31609.68 0 "t=119.1ms" _
+ 25 3 8 0 2 1 20945.80 0 "t=839.40ms" _
+ 26 4 8 0 0 1 4941.67 0 "t=81.9as" _
+ 27 5 8 0 2 1 22921.6 0 "t=770ms" _
+ 28 6 8 0 0 1 35064 0 "t=3.5zs" _
+ 29 2 9 0 0.5 1 40940 0 "t=2.5zs" _
+ 30 3 9 0 1.5 -1 24954.90 0 "t=178.3ms" _
+ 31 4 9 0 1.5 -1 11348.45 0 "t=stbl" _
+ 32 5 9 0 1.5 -1 12416.5 0 "t=800zs" _
+ 33 6 9 0 1.5 -1 28911.0 0 "t=126.5ms" _
+ 34 2 10 0 0 1 49200 0 "t=3.1zs" _
+ 35 3 10 0 1 -1 33053 0 "t=2.0zs" _
+ 36 3 10 1 1 1 33250 0.2 "t=3.7zs" _
+ 37 3 10 2 2 1 33530 0.48 "t=1.35zs" _
+ 38 4 10 0 0 1 12607.49 0 "t=1.51My" _
+ 39 5 10 0 3 1 12050.609 0 "t=stbl" _
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+ 1985 53 122 0 1 1 -86080 0 "t=3.63m" _
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+ 2003 48 123 0 1.5 1 -77414.2 0 "t=2.10s" _
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+ 2013 51 123 2 11.5 1 -86610.7 2.6134 "t=65us" _
+ 2014 52 123 0 0.5 1 -89172.2 0 "t=stbl" _
+ 2015 52 123 1 5.5 -1 -88924.7 0.24747 "t=119.2d" _
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+ 4934 99 253 0 3.5 1 79010.5 0 "t=20.47d" _
+ 4935 100 253 0 0.5 1 79345.7 0 "t=3.00d" _
+ 4936 100 253 1 5.5 -1 79697 0.351 "t=560ns" _
+ 4937 101 253 0 3.5 -1 81170 0 "t=12m" _
+ 4938 102 253 0 4.5 -1 84359 0 "t=1.56m" _
+ 4939 102 253 1 2.5 1 84526 0.16734 "t=30.3us" _
+ 4940 102 253 2 12.5 1 85560 1.2 "t=706us" _
+ 4941 103 253 0 3.5 -1 88580 0 "t=632ms" _
+ 4942 103 253 1 0.5 -1 88610 0.03 "t=1.32s" _
+ 4943 104 253 0 3.5 1 93560 0 "t=13ms" _
+ 4944 104 253 1 0.5 -1 93760 0.2 "t=52us" _
+ 4945 97 254 0 -77.777 0 84390 0 "t=1#m" _
+ 4946 98 254 0 0 1 81341 0 "t=60.5d" _
+ 4947 99 254 0 7 1 81991 0 "t=275.7d" _
+ 4948 99 254 1 2 1 82075 0.0842 "t=39.3h" _
+ 4949 100 254 0 0 1 80902.8 0 "t=3.240h" _
+ 4950 101 254 0 0 -1 83450 0 "t=10m" _
+ 4951 101 254 1 3 -1 83500 0.05 "t=28m" _
+ 4952 102 254 0 0 1 84723 0 "t=51.2s" _
+ 4953 102 254 1 8 -1 86018 1.295 "t=264.9ms" _
+ 4954 102 254 2 16 1 87940 3.22 "t=183.8us" _
+ 4955 103 254 0 -77.777 0 89870 0 "t=17.1s" _
+ 4956 104 254 0 0 1 93200 0 "t=23.2us" _
+ 4957 104 254 1 8 -1 94500 1.3 "t=4.7us" _
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+ 4960 99 255 0 3.5 1 84089 0 "t=39.8d" _
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+ 4964 102 255 1 5.5 -1 87020 0.21 "t=1#s" _
+ 4965 103 255 0 0.5 -1 89947 0 "t=31.1s" _
+ 4966 103 255 1 3.5 -1 89988 0.041 "t=2.54s" _
+ 4967 103 255 2 7.5 1 90741 0.794 "t=<1us" _
+ 4968 104 255 0 4.5 -1 94330 0 "t=1.66s" _
+ 4969 104 255 1 2.5 1 94480 0.15 "t=50us" _
+ 4970 105 255 0 -77.777 0 99590 0 "t=1.7s" _
+ 4971 98 256 0 0 1 87040 0 "t=12.3m" _
+ 4972 99 256 0 1 1 87190 0 "t=25.4m" _
+ 4973 99 256 1 8 1 87190 0 "t=7.6h" _
+ 4974 100 256 0 0 1 85487 0 "t=157.6m" _
+ 4975 101 256 0 7 -1 87460 0 "t=30#m" _
+ 4976 101 256 1 1 -1 87620 0.16 "t=77m" _
+ 4977 102 256 0 0 1 87822 0 "t=2.91s" _
+ 4978 103 256 0 -77.777 0 91750 0 "t=27s" _
+ 4979 104 256 0 0 1 94222 0 "t=6.67ms" _
+ 4980 104 256 1 5 -1 95340 1.12 "t=25us" _
+ 4981 104 256 2 8 -1 95620 1.4 "t=17us" _
+ 4982 105 256 0 -77.777 0 100500 0 "t=1.7s" _
+ 4983 99 257 0 3.5 1 89400 0 "t=7.7d" _
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+ 4985 101 257 0 3.5 -1 88993.1 0 "t=5.52h" _
+ 4986 102 257 0 1.5 1 90247 0 "t=24.5s" _
+ 4987 103 257 0 0.5 -1 92670 0 "t=6.0s" _
+ 4988 104 257 0 0.5 1 95866 0 "t=4.82s" _
+ 4989 104 257 1 5.5 -1 95940 0.073 "t=4.3s" _
+ 4990 104 257 2 10.5 1 97022 1.155 "t=106us" _
+ 4991 105 257 0 4.5 1 100210 0 "t=2.3s" _
+ 4992 105 257 1 0.5 -1 100350 0.14 "t=670ms" _
+ 4993 99 258 0 -77.777 0 92700 0 "t=3#m" _
+ 4994 100 258 0 0 1 90430 0 "t=370us" _
+ 4995 101 258 0 8 -1 91687 0 "t=51.5d" _
+ 4996 101 258 1 1 -1 91690 0 "t=57.0m" _
+ 4997 102 258 0 0 1 91480 0 "t=1.2ms" _
+ 4998 103 258 0 -77.777 0 94780 0 "t=3.6s" _
+ 4999 104 258 0 0 1 96340 0 "t=13.8ms" _
+ 5000 105 258 0 -77.777 0 101800 0 "t=4.5s" _
+ 5001 105 258 1 -77.777 0 101860 0.06 "t=1.9s" _
+ 5002 106 258 0 0 1 105240 0 "t=2.7ms" _
+ 5003 100 259 0 1.5 1 93700 0 "t=1.5s" _
+ 5004 101 259 0 3.5 -1 93620 0 "t=1.60h" _
+ 5005 102 259 0 4.5 1 94079 0 "t=58m" _
+ 5006 103 259 0 0.5 -1 95850 0 "t=6.2s" _
+ 5007 104 259 0 3.5 1 98360 0 "t=2.63s" _
+ 5008 105 259 0 4.5 1 101990 0 "t=510ms" _
+ 5009 106 259 0 5.5 -1 106520 0 "t=402ms" _
+ 5010 106 259 1 0.5 1 106610 0.087 "t=226ms" _
+ 5011 100 260 0 0 1 95770 0 "t=1#m" _
+ 5012 101 260 0 -77.777 0 96550 0 "t=27.8d" _
+ 5013 102 260 0 0 1 95610 0 "t=106ms" _
+ 5014 103 260 0 -77.777 0 98280 0 "t=3.0m" _
+ 5015 104 260 0 0 1 99150 0 "t=21ms" _
+ 5016 105 260 0 -77.777 0 103670 0 "t=1.52s" _
+ 5017 106 260 0 0 1 106548 0 "t=4.95ms" _
+ 5018 107 260 0 -77.777 0 113320 0 "t=41ms" _
+ 5019 101 261 0 3.5 -1 98580 0 "t=40#m" _
+ 5020 102 261 0 1.5 1 98460 0 "t=3#h" _
+ 5021 103 261 0 -77.777 0 99560 0 "t=39m" _
+ 5022 104 261 0 1.5 1 101320 0 "t=2.2s" _
+ 5023 104 261 1 4.5 1 101390 0.07 "t=20s" _
+ 5024 105 261 0 -77.777 0 104310 0 "t=4.7s" _
+ 5025 106 261 0 1.5 1 108005 0 "t=183ms" _
+ 5026 106 261 1 5.5 -1 108110 0.1 "t=9.3us" _
+ 5027 107 261 0 2.5 -1 113130 0 "t=12.8ms" _
+ 5028 101 262 0 -77.777 0 101630 0 "t=3#m" _
+ 5029 102 262 0 0 1 100100 0 "t=~5ms" _
+ 5030 103 262 0 -77.777 0 102100 0 "t=~4h" _
+ 5031 104 262 0 0 1 102390 0 "t=250ms" _
+ 5032 104 262 1 0 0 103390 1 "t=47ms" _
+ 5033 105 262 0 -77.777 0 106250 0 "t=34s" _
+ 5034 106 262 0 0 1 108370 0 "t=10.9ms" _
+ 5035 107 262 0 -77.777 0 114540 0 "t=84ms" _
+ 5036 107 262 1 -77.777 0 114760 0.21 "t=9.5ms" _
+ 5037 102 263 0 -77.777 0 103130 0 "t=20#m" _
+ 5038 103 263 0 -77.777 0 103730 0 "t=5#h" _
+ 5039 104 263 0 1.5 1 104760 0 "t=11m" _
+ 5040 105 263 0 -77.777 0 107110 0 "t=29s" _
+ 5041 106 263 0 3.5 1 110190 0 "t=940ms" _
+ 5042 106 263 1 1.5 1 110240 0.051 "t=420ms" _
+ 5043 107 263 0 -77.777 0 114500 0 "t=200#ms" _
+ 5044 108 263 0 1.5 1 119680 0 "t=760us" _
+ 5045 108 263 1 5.5 -1 120000 0.32 "t=760us" _
+ 5046 102 264 0 0 1 105010 0 "t=1#m" _
+ 5047 103 264 0 -77.777 0 106380 0 "t=10#h" _
+ 5048 104 264 0 0 1 106080 0 "t=1#h" _
+ 5049 105 264 0 -77.777 0 109360 0 "t=3#m" _
+ 5050 106 264 0 0 1 110780 0 "t=47ms" _
+ 5051 107 264 0 -77.777 0 116060 0 "t=1.07s" _
+ 5052 108 264 0 0 1 119563 0 "t=540us" _
+ 5053 103 265 0 -77.777 0 108230 0 "t=10#h" _
+ 5054 104 265 0 1.5 1 108690 0 "t=1.6m" _
+ 5055 105 265 0 -77.777 0 110480 0 "t=15#m" _
+ 5056 106 265 0 4.5 1 112790 0 "t=9.2s" _
+ 5057 106 265 1 1.5 1 112860 0.06 "t=16.4s" _
+ 5058 107 265 0 -77.777 0 116420 0 "t=1.19s" _
+ 5059 108 265 0 1.5 1 120900 0 "t=1.96ms" _
+ 5060 108 265 1 4.5 1 121130 0.229 "t=360us" _
+ 5061 109 265 0 -77.777 0 126680 0 "t=2#ms" _
+ 5062 103 266 0 -77.777 0 111620 0 "t=21h" _
+ 5063 104 266 0 0 1 110080 0 "t=4#h" _
+ 5064 105 266 0 -77.777 0 112740 0 "t=80m" _
+ 5065 106 266 0 0 1 113620 0 "t=390ms" _
+ 5066 107 266 0 -77.777 0 118100 0 "t=2.5s" _
+ 5067 108 266 0 0 1 121140 0 "t=3.02ms" _
+ 5068 108 266 1 9 -1 122240 1.1 "t=280ms" _
+ 5069 109 266 0 -77.777 0 127960 0 "t=1.2ms" _
+ 5070 109 266 1 -77.777 0 129100 1.14 "t=6ms" _
+ 5071 104 267 0 -77.777 0 113440 0 "t=2.5h" _
+ 5072 105 267 0 -77.777 0 114070 0 "t=100m" _
+ 5073 106 267 0 -77.777 0 115810 0 "t=1.8m" _
+ 5074 107 267 0 -77.777 0 118770 0 "t=22s" _
+ 5075 108 267 0 2.5 1 122650 0 "t=55ms" _
+ 5076 108 267 1 -77.777 0 122690 0.039 "t=990us" _
+ 5077 109 267 0 -77.777 0 127790 0 "t=10#ms" _
+ 5078 110 267 0 1.5 1 133880 0 "t=10us" _
+ 5079 104 268 0 0 1 115480 0 "t=1#h" _
+ 5080 105 268 0 -77.777 0 117060 0 "t=29h" _
+ 5081 106 268 0 0 1 116800 0 "t=2#m" _
+ 5082 107 268 0 -77.777 0 120810 0 "t=25#s" _
+ 5083 108 268 0 0 1 122830 0 "t=1.42s" _
+ 5084 109 268 0 5 1 129150 0 "t=27ms" _
+ 5085 110 268 0 0 1 133650 0 "t=100#us" _
+ 5086 105 269 0 -77.777 0 119150 0 "t=3#h" _
+ 5087 106 269 0 -77.777 0 119760 0 "t=5m" _
+ 5088 107 269 0 -77.777 0 121480 0 "t=1#m" _
+ 5089 108 269 0 4.5 1 124560 0 "t=16s" _
+ 5090 109 269 0 -77.777 0 129370 0 "t=100#ms" _
+ 5091 110 269 0 4.5 1 134830 0 "t=230us" _
+ 5092 105 270 0 -77.777 0 122310 0 "t=2.0h" _
+ 5093 106 270 0 0 1 121490 0 "t=3#m" _
+ 5094 107 270 0 -77.777 0 124230 0 "t=3.8m" _
+ 5095 108 270 0 0 1 125110 0 "t=9s" _
+ 5096 109 270 0 -77.777 0 130710 0 "t=6.3ms" _
+ 5097 110 270 0 0 1 134680 0 "t=205us" _
+ 5098 110 270 1 10 -1 136070 1.39 "t=10ms" _
+ 5099 106 271 0 -77.777 0 124760 0 "t=3.1m" _
+ 5100 107 271 0 -77.777 0 125920 0 "t=10m" _
+ 5101 108 271 0 -77.777 0 127740 0 "t=10#s" _
+ 5102 109 271 0 -77.777 0 131100 0 "t=400#ms" _
+ 5103 110 271 0 6.5 -1 135950 0 "t=90ms" _
+ 5104 110 271 1 4.5 1 136020 0.068 "t=1.7ms" _
+ 5105 106 272 0 0 1 126580 0 "t=4#m" _
+ 5106 107 272 0 -77.777 0 128790 0 "t=11.3s" _
+ 5107 108 272 0 0 1 129010 0 "t=10#s" _
+ 5108 109 272 0 -77.777 0 133580 0 "t=400#ms" _
+ 5109 110 272 0 0 1 136020 0 "t=200#ms" _
+ 5110 111 272 0 5 1 142770 0 "t=4.5ms" _
+ 5111 106 273 0 -77.777 0 130020 0 "t=5#m" _
+ 5112 107 273 0 -77.777 0 130630 0 "t=1#m" _
+ 5113 108 273 0 1.5 1 131890 0 "t=1060ms" _
+ 5114 109 273 0 -77.777 0 134710 0 "t=800#ms" _
+ 5115 110 273 0 6.5 -1 138360 0 "t=240us" _
+ 5116 110 273 1 1.5 1 138560 0.198 "t=120ms" _
+ 5117 111 273 0 -77.777 0 142700 0 "t=2#ms" _
+ 5118 107 274 0 -77.777 0 133680 0 "t=60s" _
+ 5119 108 274 0 0 1 133490 0 "t=500#ms" _
+ 5120 109 274 0 -77.777 0 137250 0 "t=850ms" _
+ 5121 110 274 0 0 1 139200 0 "t=10#ms" _
+ 5122 111 274 0 -77.777 0 144610 0 "t=29ms" _
+ 5123 107 275 0 -77.777 0 135690 0 "t=5#m" _
+ 5124 108 275 0 -77.777 0 136620 0 "t=290ms" _
+ 5125 109 275 0 -77.777 0 138830 0 "t=117ms" _
+ 5126 110 275 0 -77.777 0 141570 0 "t=10#ms" _
+ 5127 111 275 0 -77.777 0 145300 0 "t=5#ms" _
+ 5128 108 276 0 0 1 138290 0 "t=100#ms" _
+ 5129 109 276 0 -77.777 0 141320 0 "t=630ms" _
+ 5130 109 276 1 -77.777 0 141570 0.25 "t=10s" _
+ 5131 110 276 0 0 1 142540 0 "t=100#ms" _
+ 5132 111 276 0 -77.777 0 147490 0 "t=10#ms" _
+ 5133 108 277 0 1.5 1 141490 0 "t=11ms" _
+ 5134 108 277 1 -77.777 0 141590 0.1 "t=110s" _
+ 5135 109 277 0 -77.777 0 142970 0 "t=9s" _
+ 5136 110 277 0 5.5 1 145140 0 "t=6ms" _
+ 5137 111 277 0 -77.777 0 148340 0 "t=10#ms" _
+ 5138 109 278 0 -77.777 0 145740 0 "t=7s" _
+ 5139 110 278 0 0 1 146380 0 "t=270#ms" _
+ 5140 111 278 0 -77.777 0 150520 0 "t=8ms" _
+ 5141 109 279 0 -77.777 0 147500 0 "t=30#s" _
+ 5142 110 279 0 -77.777 0 149130 0 "t=210ms" _
+ 5143 111 279 0 -77.777 0 151780 0 "t=180ms" _
+ 5144 110 280 0 0 1 150520 0 "t=11s" _
+ 5145 111 280 0 -77.777 0 153890 0 "t=4.3s" _
+ 5146 110 281 0 1.5 1 153430 0 "t=14s" _
+ 5147 110 281 1 -77.777 0 153470 0.04 "t=0.9s" _
+ 5148 111 281 0 -77.777 0 155300 0 "t=24s" _
+ 5149 111 282 0 -77.777 0 157800 0 "t=1.6m" _
+ 5150 111 283 0 -77.777 0 159280 0 "t=30#s"
diff --git a/NPLib/Physics/PAR_GEF/ShellMO.dat b/NPLib/Physics/PAR_GEF/ShellMO.dat
new file mode 100644
index 0000000000000000000000000000000000000000..944cd105a4d2a3cefc71178f3853e800e9d1c43e
--- /dev/null
+++ b/NPLib/Physics/PAR_GEF/ShellMO.dat
@@ -0,0 +1,1071 @@
+ShellData:
+/' Moeller's shell effects recommended by Myers and Swiatecki '/
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+0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0.11 0.07 -0.2
+-0.26 -0.6 -0.71 -0.98 -1.12 -1.57 -1.5 -1.93 -2.06 -2.47 -2.46 -2.77 -2.64
+-2.99 -2.88 -3.06 -2.97 -3.08 -2.72 -2.61 -2.23 -2.14 -1.93 -1.96 -1.72 -1.8
+-1.71 -1.94 -1.82 -2.04 -2.09 -2.46 -2.56 -2.91 -2.89 -7.09 -3.35 -7.94 -8.34
+-8.93 -9.24 -9.87 -4.6 -4.87 -5.15 -5.59 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
+0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0
+0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 -2.2 -2.38 -2.26
+-0.83 -1.01 -1.4 -1.39 -1.8 -1.97 -2.44 -2.47 -2.86 -2.94 -3.14 -2.97 -3.32
+-3.17 -3.32 -3.2 -3.3 -2.94 -2.82 -2.45 -2.35 -2.1 -2.03 -1.87 -1.92 -1.83
+-1.99 -1.99 -2.18 -2.22 -2.47 -2.57 -2.93 -3 -3.38 -3.44 -3.81 -3.79 -4.16
+-4.26 -4.64 -4.8 -5.2 -5.34 -5.84 -6.12
\ No newline at end of file
diff --git a/NPLib/Physics/TFissionConditions.cxx b/NPLib/Physics/TFissionConditions.cxx
new file mode 100644
index 0000000000000000000000000000000000000000..40d0d27c8763ba6bb98840b224fdc61364a8457b
--- /dev/null
+++ b/NPLib/Physics/TFissionConditions.cxx
@@ -0,0 +1,84 @@
+/*****************************************************************************
+ * Copyright (C) 2009-2016 this file is part of the NPTool Project *
+ * *
+ * For the licensing terms see $NPTOOL/Licence/NPTool_Licence *
+ * For the list of contributors see $NPTOOL/Licence/Contributors *
+ *****************************************************************************/
+
+/*****************************************************************************
+ * Original Author: Pierre Morfouace address: pierre.morfouace2@cea.fr *
+ * *
+ * Creation Date : 01/10/20 *
+ * Last update : *
+ *---------------------------------------------------------------------------*
+ * Decription: This class records all the information concerning the fission *
+ * fragment and the Ex of the fissioning system *
+ *---------------------------------------------------------------------------*
+ * Comment: *
+ * *
+ * *
+ *****************************************************************************/
+
+#include <iostream>
+using namespace std;
+
+#include "TFissionConditions.h"
+
+ClassImp(TFissionConditions)
+ ////////////////////////////////////////////////////////////////////////////////
+ TFissionConditions::TFissionConditions(){
+ }
+////////////////////////////////////////////////////////////////////////////////
+TFissionConditions::~TFissionConditions(){
+}
+////////////////////////////////////////////////////////////////////////////////
+void TFissionConditions::Clear(){
+ // Fissionning system
+ fFC_A_CN = -10;
+ fFC_Z_CN = -10;
+ fFC_Ex_CN = -10;
+ fFC_ELab_CN = -10;
+ fFC_ThetaLab_CN = -10;
+
+ // Fission process
+ fFC_TKE = -10;
+ fFC_KE1 = -10;
+ fFC_KE2 = -10;
+ fFC_Neutron_Multiplicity = -10;
+
+ // Fission Fragments
+ fFC_Fragment_Name.clear();
+ fFC_Fragment_A.clear();
+ fFC_Fragment_Z.clear();
+ fFC_Fragment_Theta.clear();
+ fFC_Fragment_Phi.clear();
+ fFC_Fragment_Kinetic_Energy.clear();
+ fFC_Fragment_Brho.clear();
+ fFC_Fragment_Momentum_Direction_X.clear();
+ fFC_Fragment_Momentum_Direction_Y.clear();
+ fFC_Fragment_Momentum_Direction_Z.clear();
+}
+////////////////////////////////////////////////////////////////////////////////
+void TFissionConditions::Dump() const{
+ cout << "--------- Fission Condition Dump ---------" << endl ;
+
+ // Fissionning system
+ cout << "\t ---- Fissionning system ---- " << endl;
+ cout << "\t Z: " << fFC_Z_CN << endl;
+ cout << "\t A: " << fFC_A_CN << endl;
+ cout << "\t Ex: " << fFC_Ex_CN << endl;
+ cout << "\t TKE: " << fFC_TKE << endl;
+ cout << "\t Neutron Mult: " << fFC_Neutron_Multiplicity << endl;
+
+
+ // Fission fragments
+ unsigned int size = fFC_Fragment_A.size();
+ for(unsigned int i = 0 ; i < size; i ++){
+ cout << "\t ---- Particle " << i << " ---- " << endl;
+ cout << "\t Fragment Z: " << fFC_Fragment_Z[i] << endl;
+ cout << "\t Fragment A: " << fFC_Fragment_A[i] << endl;
+ }
+
+
+}
+
diff --git a/NPLib/Physics/TFissionConditions.h b/NPLib/Physics/TFissionConditions.h
new file mode 100644
index 0000000000000000000000000000000000000000..759e093788e87eb3a547444dec0426d2b1fc3450
--- /dev/null
+++ b/NPLib/Physics/TFissionConditions.h
@@ -0,0 +1,134 @@
+#ifndef TFISSIONCONDITIONS_H
+#define TFISSIONCONDITIONS_H
+/*****************************************************************************
+ * Copyright (C) 2009-2016 this file is part of the NPTool Project *
+ * *
+ * For the licensing terms see $NPTOOL/Licence/NPTool_Licence *
+ * For the list of contributors see $NPTOOL/Licence/Contributors *
+ *****************************************************************************/
+
+/*****************************************************************************
+ * Original Author: Pierre Morfouace address: pierre.morfouace2@cea.fr *
+ * *
+ * Creation Date : 01/10/20 *
+ * Last update : *
+ *---------------------------------------------------------------------------*
+ * Decription: This class records all the information concerning the fission *
+ * fragments and the Ex of the fissionning system *
+ *---------------------------------------------------------------------------*
+ * Comment: *
+ * *
+ * *
+ *****************************************************************************/
+
+
+
+// STL Header
+#include <vector>
+#include <string>
+#include <cmath>
+using namespace std ;
+
+// Root Header
+#include "TObject.h"
+#include "TVector3.h"
+
+// NPTOOL headers
+#include "NPGlobalSystemOfUnits.h"
+#include "NPPhysicalConstants.h"
+#ifdef NP_SYSTEM_OF_UNITS_H
+using namespace NPUNITS;
+#endif
+
+class TFissionConditions : public TObject{
+ private:
+
+ // Fissionning system
+ int fFC_A_CN;
+ int fFC_Z_CN;
+ double fFC_Ex_CN;
+ double fFC_ELab_CN;
+ double fFC_ThetaLab_CN;
+
+ // Fission Process
+ double fFC_TKE;
+ double fFC_KE1;
+ double fFC_KE2;
+ int fFC_Neutron_Multiplicity;
+
+ // Fission Fragments
+ vector<string> fFC_Fragment_Name;
+ vector<int> fFC_Fragment_Z;
+ vector<int> fFC_Fragment_A;
+ vector<double> fFC_Fragment_Theta;
+ vector<double> fFC_Fragment_Phi;
+ vector<double> fFC_Fragment_Kinetic_Energy;
+ vector<double> fFC_Fragment_Brho;
+ vector<double> fFC_Fragment_Momentum_Direction_X;
+ vector<double> fFC_Fragment_Momentum_Direction_Y;
+ vector<double> fFC_Fragment_Momentum_Direction_Z;
+
+ public:
+ TFissionConditions();
+ virtual ~TFissionConditions();
+
+ void Clear();
+ void Clear(const Option_t*) {Clear();};
+ void Dump() const;
+
+ ///////////////////// SETTERS ////////////////////////
+ // Fissionning system parameter
+ void SetA_CN (const int A_CN) {fFC_A_CN = A_CN;}//!
+ void SetZ_CN (const int Z_CN) {fFC_Z_CN = Z_CN;}//!
+ void SetEx_CN (const double Ex_CN) {fFC_Ex_CN = Ex_CN;}//!
+ void SetELab_CN (const double ELab_CN) {fFC_ELab_CN = ELab_CN;}//!
+ void SetThetaLab_CN (const double Theta_CN) {fFC_ThetaLab_CN = Theta_CN;}//!
+
+ // Fission process
+ void Set_TKE (const double E) {fFC_TKE = E;}//!
+ void Set_KE1 (const double E) {fFC_KE1 = E;}//!
+ void Set_KE2 (const double E) {fFC_KE2 = E;}//!
+ void SetNeutronMultiplicity (const int mult) {fFC_Neutron_Multiplicity = mult;}//!
+
+ // Fission Fragments
+ void SetFragmentName (const string name) {fFC_Fragment_Name.push_back(name);}//!
+ void SetFragmentZ (const int Z) {fFC_Fragment_Z.push_back(Z);}//!
+ void SetFragmentA (const int A) {fFC_Fragment_A.push_back(A);}//!
+ void SetFragmentTheta (const double Theta) {fFC_Fragment_Theta.push_back(Theta);}//!
+ void SetFragmentPhi (const double Phi) {fFC_Fragment_Phi.push_back(Phi);}//!
+ void SetFragmentKineticEnergy (const double E) {fFC_Fragment_Kinetic_Energy.push_back(E);}//!
+ void SetFragmentBrho (const double Brho) {fFC_Fragment_Brho.push_back(Brho);}//!
+ void SetFragmentMomentumX (const double P) {fFC_Fragment_Momentum_Direction_X.push_back(P);}//!
+ void SetFragmentMomentumY (const double P) {fFC_Fragment_Momentum_Direction_Y.push_back(P);}//!
+ void SetFragmentMomentumZ (const double P) {fFC_Fragment_Momentum_Direction_Z.push_back(P);}//!
+
+ ///////////////////// GETTERS ////////////////////////
+ // Fissionning system parameter
+ int GetA_CN() const {return fFC_A_CN;}//!
+ int GetZ_CN() const {return fFC_Z_CN;}//!
+ double GetEx_CN() const {return fFC_Ex_CN;}//!
+ double GetELab_CN() const {return fFC_ELab_CN;}//!
+ double GetThetaLab_CN() const {return fFC_ThetaLab_CN;}//!
+
+ // Fission Process
+ double GetTKE() const {return fFC_TKE;}//!
+ double GetKE1() const {return fFC_KE1;}//!
+ double GetKE2() const {return fFC_KE2;}//!
+ int GetNeutronMultiplicity() const {return fFC_Neutron_Multiplicity;}//!
+
+ // emmitted particles
+ string GetFragmentName (const int &i) const {return fFC_Fragment_Name[i];}//!
+ int GetFragmentZ (const int &i) const {return fFC_Fragment_Z[i];}//!
+ int GetFragmentA (const int &i) const {return fFC_Fragment_A[i];}//!
+ double GetFragmentTheta (const int &i) const {return fFC_Fragment_Theta[i];}//!
+ double GetFragmentPhi (const int &i) const {return fFC_Fragment_Phi[i];}//!
+ double GetFragmentKineticEnergy (const int &i) const {return fFC_Fragment_Kinetic_Energy[i];}//!
+ double GetFragmentBrho (const int &i) const {return fFC_Fragment_Brho[i];}//!
+ double GetFragmentMomentumX (const int &i) const {return fFC_Fragment_Momentum_Direction_X[i];}//!
+ double GetFragmentMomentumY (const int &i) const {return fFC_Fragment_Momentum_Direction_Y[i];}//!
+ double GetFragmentMomentumZ (const int &i) const {return fFC_Fragment_Momentum_Direction_Z[i];}//!
+
+ ClassDef(TFissionConditions, 1) // TFissionConditions structure
+};
+
+#endif
diff --git a/NPSimulation/Core/Target.cc b/NPSimulation/Core/Target.cc
index e743109de5861b91d1852c39275c18e7c6a04218..00af9656aee65bd38c4e0d5f1dee0e9b520176cb 100644
--- a/NPSimulation/Core/Target.cc
+++ b/NPSimulation/Core/Target.cc
@@ -51,6 +51,7 @@ using namespace CLHEP ;
#include "Target.hh"
#include "MaterialManager.hh"
#include "Decay.hh"
+#include "FissionDecay.hh"
// NPL
#include "NPOptionManager.h"
#include "NPInputParser.h"
@@ -465,6 +466,9 @@ void Target::SetReactionRegion(){
m_ReactionModel.push_back(fsm);
fsm = new NPS::Decay("Decay",m_ReactionRegion);
m_ReactionModel.push_back(fsm);
+ fsm = new NPS::FissionDecay("FissionDecay",m_ReactionRegion);
+ m_ReactionModel.push_back(fsm);
+
}
//....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
diff --git a/NPSimulation/Process/CMakeLists.txt b/NPSimulation/Process/CMakeLists.txt
index 7f9dfac741476858b29702be2ce1a94ca1fbf255..85bae1eac9ec01ddc83bacfa83ce354ca9275e30 100644
--- a/NPSimulation/Process/CMakeLists.txt
+++ b/NPSimulation/Process/CMakeLists.txt
@@ -3,14 +3,14 @@ if(Geant4_VERSION_MAJOR GREATER 9)
if(Geant4_VERSION_MINOR GREATER 4)
message("Compiling with NeutronHPphysics")
-add_library(NPSProcess SHARED Decay.cc BeamReaction.cc FastDriftElectron.cc NPIonIonInelasticPhysic.cc PhysicsList.cc G4DriftElectron.cc G4IonizationWithDE.cc G4DriftElectronPhysics.cc G4DEAbsorption.cc G4DEAmplification.cc G4DETransport.cc menate_R.cc NeutronHPphysics.cc NeutronHPMessenger.cc)
+ add_library(NPSProcess SHARED FissionDecay.cc Decay.cc BeamReaction.cc FastDriftElectron.cc NPIonIonInelasticPhysic.cc PhysicsList.cc G4DriftElectron.cc G4IonizationWithDE.cc G4DriftElectronPhysics.cc G4DEAbsorption.cc G4DEAmplification.cc G4DETransport.cc menate_R.cc NeutronHPphysics.cc NeutronHPMessenger.cc)
add_definitions(-DUSE_NEUTRONHP)
else ()
message("Compiling WITHOUT NeutronHPphysics, install geant4 10.5 or greater for this physics list")
-add_library(NPSProcess SHARED Decay.cc BeamReaction.cc FastDriftElectron.cc NPIonIonInelasticPhysic.cc PhysicsList.cc G4DriftElectron.cc G4IonizationWithDE.cc G4DriftElectronPhysics.cc G4DEAbsorption.cc G4DEAmplification.cc G4DETransport.cc menate_R.cc)
+ add_library(NPSProcess SHARED FissionDecay.cc Decay.cc BeamReaction.cc FastDriftElectron.cc NPIonIonInelasticPhysic.cc PhysicsList.cc G4DriftElectron.cc G4IonizationWithDE.cc G4DriftElectronPhysics.cc G4DEAbsorption.cc G4DEAmplification.cc G4DETransport.cc menate_R.cc)
endif()
endif()
-target_link_libraries(NPSProcess ${ROOT_LIBRARIES} ${Geant4_LIBRARIES} ${NPLib_LIBRARIES} -lNPInitialConditions -lNPInteractionCoordinates -lNPReactionConditions)
+ target_link_libraries(NPSProcess ${ROOT_LIBRARIES} ${Geant4_LIBRARIES} ${NPLib_LIBRARIES} -lNPInitialConditions -lNPInteractionCoordinates -lNPReactionConditions -lNPFissionConditions)
diff --git a/NPSimulation/Process/FissionDecay.cc b/NPSimulation/Process/FissionDecay.cc
new file mode 100644
index 0000000000000000000000000000000000000000..a3c5e2178d8f72e2bc968aad3e6a1b9cd21c66a9
--- /dev/null
+++ b/NPSimulation/Process/FissionDecay.cc
@@ -0,0 +1,230 @@
+/*****************************************************************************
+ * Copyright (C) 2009-2016 this file is part of the NPTool Project *
+ * *
+ * For the licensing terms see $NPTOOL/Licence/NPTool_Licence *
+ * For the list of contributors see $NPTOOL/Licence/Contributors *
+ *****************************************************************************/
+
+/*****************************************************************************
+ * Original Author: Pierre Morfouace address: pierre.morfouace2@cea.fr *
+ * *
+ * Creation Date : Octobre 2020 *
+ * Last update : *
+ *---------------------------------------------------------------------------*
+ * Decription: *
+ * Use to kill the beam track and replace it with the fission products *
+ * *
+ * *
+ * *
+ *---------------------------------------------------------------------------*
+ * Comment: *
+ * *
+ *****************************************************************************/
+
+#include <iostream>
+#include <string>
+#include <set>
+#include "NPFunction.h"
+#include "FissionDecay.hh"
+#include "NPOptionManager.h"
+#include "NPInputParser.h"
+#include "G4VPhysicalVolume.hh"
+#include "G4Electron.hh"
+#include "G4Gamma.hh"
+#include "G4SystemOfUnits.hh"
+#include "G4ParticleTable.hh"
+#include "G4IonTable.hh"
+#include "RootOutput.h"
+
+using namespace NPS;
+////////////////////////////////////////////////////////////////////////////////
+FissionDecay::FissionDecay(G4String modelName,G4Region* envelope) :
+ G4VFastSimulationModel(modelName, envelope) {
+ ReadConfiguration();
+ m_PreviousEnergy=0 ;
+ m_PreviousLength=0 ;
+ }
+
+
+////////////////////////////////////////////////////////////////////////////////
+FissionDecay::FissionDecay(G4String modelName) :
+ G4VFastSimulationModel(modelName) {
+ }
+
+////////////////////////////////////////////////////////////////////////////////
+FissionDecay::~FissionDecay() {
+}
+
+////////////////////////////////////////////////////////////////////////////////
+void FissionDecay::AttachFissionConditions(){
+ if(RootOutput::getInstance()->GetTree()->FindBranch("FissionConditions"))
+ RootOutput::getInstance()->GetTree()->SetBranchAddress("FissionConditions", &m_FissionConditions);
+}
+
+////////////////////////////////////////////////////////////////////////////////
+void FissionDecay::ReadConfiguration(){
+ NPL::InputParser input(NPOptionManager::getInstance()->GetReactionFile());
+ m_FissionDecay.ReadConfiguration(input);
+ std::string Mother = m_FissionDecay.GetCompoundName();
+
+ m_CompoundParticle = NPL::Particle(Mother);
+
+ m_CompoundName = NPL::ChangeNameToG4Standard(Mother,true);
+
+ m_FissionConditions = new TFissionConditions();
+ AttachFissionConditions();
+ if(!RootOutput::getInstance()->GetTree()->FindBranch("FissionConditions"))
+ RootOutput::getInstance()->GetTree()->Branch("FissionConditions", "TFissionConditions", &m_FissionConditions);
+
+
+}
+
+////////////////////////////////////////////////////////////////////////////////
+G4bool FissionDecay::IsApplicable( const G4ParticleDefinition& particleType) {
+ m_CurrentName = particleType.GetParticleName();
+ // Extract Ex from name
+ if(m_CurrentName.find("[")!=std::string::npos)
+ m_ExcitationEnergy = atof(m_CurrentName.substr(m_CurrentName.find("[")+1,m_CurrentName.find("]")-1).c_str())*keV;
+ else
+ m_ExcitationEnergy=0;
+
+ // Strip name from excitation energy
+ m_CurrentName = m_CurrentName.substr(0,m_CurrentName.find("["));
+ if (m_CompoundName==m_CurrentName) {
+ return true;
+ }
+ return false;
+}
+
+////////////////////////////////////////////////////////////////////////////////
+G4bool FissionDecay::ModelTrigger(const G4FastTrack& fastTrack) {
+ bool Trigger = true;
+
+ m_FissionConditions->Clear();
+
+ m_PreviousEnergy=fastTrack.GetPrimaryTrack()->GetKineticEnergy();
+ // To be coded;
+
+ return Trigger;
+}
+
+////////////////////////////////////////////////////////////////////////////////
+void FissionDecay::DoIt(const G4FastTrack& fastTrack,G4FastStep& fastStep){
+ // Get the track info
+ const G4Track* PrimaryTrack = fastTrack.GetPrimaryTrack();
+ G4ThreeVector pdirection = PrimaryTrack->GetMomentum().unit();
+ G4ThreeVector localdir = fastTrack.GetPrimaryTrackLocalDirection();
+
+ G4ThreeVector worldPosition = PrimaryTrack->GetPosition();
+ G4ThreeVector localPosition = fastTrack.GetPrimaryTrackLocalPosition();
+
+ double energy = PrimaryTrack->GetKineticEnergy();
+ double time = PrimaryTrack->GetGlobalTime();
+
+ // Randomize within the step
+ // Assume energy loss is linear within the step
+ // Assume no scattering
+ double rand = G4RandFlat::shoot();
+ double length = rand*(m_PreviousLength);
+ energy += (1-rand)*(m_PreviousEnergy-energy);
+ G4ThreeVector ldir = pdirection;
+ ldir*=length;
+ localPosition = localPosition - ldir;
+ //////////////////////////////////////////////////
+ //////Define the kind of particle to shoot////////
+ //////////////////////////////////////////////////
+ std::vector<NPL::Particle> FissionFragment;
+ std::vector<double> Ex;
+ std::vector<double> DEK;
+ std::vector<double> DPx;
+ std::vector<double> DPy;
+ std::vector<double> DPz;
+ double TKE, KE1, KE2;
+
+
+ m_FissionDecay.GenerateEvent(NPL::ChangeNameFromG4Standard(m_CurrentName),m_ExcitationEnergy,energy,
+ pdirection.x(),pdirection.y(),pdirection.z(),
+ FissionFragment, Ex,DEK,DPx,DPy,DPz,
+ TKE, KE1, KE2);
+
+ /////////////////////////////////////////////////
+ // Fillion the attached Fission condition Tree //
+ /////////////////////////////////////////////////
+ // Fissionning system
+ m_FissionConditions->SetZ_CN(m_CompoundParticle.GetZ());
+ m_FissionConditions->SetA_CN(m_CompoundParticle.GetA());
+ m_FissionConditions->SetEx_CN(m_ExcitationEnergy);
+ m_FissionConditions->SetELab_CN(energy);
+
+ // Fission Process
+ m_FissionConditions->Set_TKE(TKE);
+ m_FissionConditions->Set_KE1(KE1);
+ m_FissionConditions->Set_KE2(KE2);
+
+ G4ParticleDefinition* FissionFragmentDef;
+ unsigned int size = FissionFragment.size();
+
+ if(size == 0)
+ return;
+
+ // Get Neutron Multiplicity
+ int Zsum = FissionFragment[0].GetZ() + FissionFragment[1].GetZ();
+ int Asum = FissionFragment[0].GetA() + FissionFragment[1].GetA();
+ if(Zsum == m_CompoundParticle.GetZ())
+ m_FissionConditions->SetNeutronMultiplicity(m_CompoundParticle.GetA()-Asum);
+
+ for(unsigned int i = 0 ; i < size ; i++){
+ // Get the decaying particle
+ int FFZ = FissionFragment[i].GetZ();
+ int FFA = FissionFragment[i].GetA();
+ FissionFragmentDef=NULL;
+
+ // Set the momentum direction
+ G4ThreeVector Momentum (DPx[i],DPy[i],DPz[i]);
+ Momentum=Momentum.unit();
+
+ double Brho = FissionFragment[i].GetBrho();
+
+ m_FissionConditions->SetFragmentZ(FFZ);
+ m_FissionConditions->SetFragmentA(FFA);
+ m_FissionConditions->SetFragmentKineticEnergy(DEK[i]);
+ m_FissionConditions->SetFragmentBrho(Brho);
+ m_FissionConditions->SetFragmentTheta(Momentum.theta()/deg);
+ m_FissionConditions->SetFragmentPhi(Momentum.phi()/deg);
+ m_FissionConditions->SetFragmentMomentumX(DPx[i]);
+ m_FissionConditions->SetFragmentMomentumX(DPy[i]);
+ m_FissionConditions->SetFragmentMomentumX(DPz[i]);
+
+ // neutral particle
+ if(FFZ==0){
+ if(FFA==1)
+ FissionFragmentDef=G4ParticleTable::GetParticleTable()->FindParticle("neutron");
+
+ else if(FFA==0){
+ FissionFragmentDef=G4ParticleTable::GetParticleTable()->FindParticle("gamma");
+ }
+
+ }
+ // proton
+ else if (FFZ==1 && FFA==1 )
+ FissionFragmentDef=G4ParticleTable::GetParticleTable()->FindParticle("proton");
+ // the rest
+ else
+ FissionFragmentDef=G4ParticleTable::GetParticleTable()->GetIonTable()->GetIon(FFZ, FFA, Ex[i]);
+
+
+ G4DynamicParticle DynamicFissionFragment(FissionFragmentDef,Momentum,DEK[i]);
+ fastStep.CreateSecondaryTrack(DynamicFissionFragment, localPosition, time);
+ }
+
+ if(size){
+ // Set the end of the step conditions
+ fastStep.SetPrimaryTrackFinalKineticEnergyAndDirection(0,pdirection);
+ fastStep.SetPrimaryTrackFinalPosition(worldPosition);
+ fastStep.SetTotalEnergyDeposited(0);
+ fastStep.SetPrimaryTrackFinalTime (time);
+ fastStep.KillPrimaryTrack();
+ fastStep.SetPrimaryTrackPathLength(0.0);
+ }
+
+}
diff --git a/NPSimulation/Process/FissionDecay.hh b/NPSimulation/Process/FissionDecay.hh
new file mode 100644
index 0000000000000000000000000000000000000000..d4aa9cf20838fe35fd28f3c54993f3759386a36d
--- /dev/null
+++ b/NPSimulation/Process/FissionDecay.hh
@@ -0,0 +1,64 @@
+/*****************************************************************************
+ * Copyright (C) 2009-2016 this file is part of the NPTool Project *
+ * *
+ * For the licensing terms see $NPTOOL/Licence/NPTool_Licence *
+ * For the list of contributors see $NPTOOL/Licence/Contributors *
+ *****************************************************************************/
+
+/*****************************************************************************
+ * Original Author: Pierre Morfouace pierre.morfouace2@cea.fr *
+ * *
+ * Creation Date : Octobre 2020 *
+ * Last update : *
+ *---------------------------------------------------------------------------*
+ * Decription: *
+ * *
+* *
+ * *
+ *---------------------------------------------------------------------------*
+ * Comment: *
+ * *
+ *****************************************************************************/
+
+#ifndef FissionDecay_h
+#define FissionDecay_h
+
+#include "G4VFastSimulationModel.hh"
+#include "PhysicsList.hh"
+#include "NPFissionDecay.h"
+#include "TFissionConditions.h"
+class G4VPhysicalVolume;
+
+////////////////////////////////////////////////////////////////////////////////
+namespace NPS{
+
+class FissionDecay : public G4VFastSimulationModel{
+ public:
+ FissionDecay (G4String, G4Region*);
+ FissionDecay (G4String);
+ ~FissionDecay();
+
+ public:
+ void ReadConfiguration();
+ virtual G4bool IsApplicable(const G4ParticleDefinition&);
+ virtual G4bool ModelTrigger(const G4FastTrack &);
+ virtual void DoIt(const G4FastTrack&, G4FastStep&);
+
+ private:
+ NPL::FissionDecay m_FissionDecay;
+ NPL::Particle m_CompoundParticle;
+ std::string m_CompoundName;
+ std::string m_CurrentName;
+ double m_ExcitationEnergy;
+ double m_PreviousEnergy;
+ double m_PreviousLength;
+
+ private:
+ TFissionConditions* m_FissionConditions;
+
+ public:
+ void AttachFissionConditions();
+};
+}
+
+#endif