Import Geant4 10.6.0 source tree

source/processes/electromagnetic/standard/include/G4BetheHeitler5DModel.hh

@@ -41,6 +41,10 @@
 //          version (Denis Bernard)
 // 04-06-18 Performance optimization of the final state sampling (M. Novak)
 // 10-04-19 CLHEP for boost and rotation, remove local functions (IgS)
+// 02-09-19 Set base class to be G4PairProductionRelModel that can provide 
+//          accurate sections now from threshold to very high energies
+//          including the LPM effect. (M. Novak)
+// 14-10-19 Muon's pair genaration in SampleSecondaries
 //
 // Class Description:
 //
@@ -53,11 +57,11 @@
 #ifndef G4BetheHeitler5DModel_h
 #define G4BetheHeitler5DModel_h 1
 
-#include "G4BetheHeitlerModel.hh"
+#include "G4PairProductionRelModel.hh"
 
 class G4IonTable;
 
-class G4BetheHeitler5DModel : public G4BetheHeitlerModel
+class G4BetheHeitler5DModel : public G4PairProductionRelModel
 {
 
 public:
@@ -77,6 +81,10 @@ public:
 
   inline void SetVerbose(G4int val) { fVerbose = val; }
 
+  // Only e+, e+ or mu+, mu- pairs supported
+  void SetLeptonPair(const G4ParticleDefinition* p1,
+		     const G4ParticleDefinition* p2);
+
 private:
 
   // hide assignment operator
@@ -86,10 +94,20 @@ private:
   G4double MaxDiffCrossSection(const G4double* par, G4double eZ,
                                G4double e, G4double loge) const;
 
+  inline void SetConversionMode(G4int to) { fConvMode = to; }
+
   G4IonTable* theIonTable;
 
   G4int  fVerbose;
   G4int  fConversionType;
   G4bool iraw;
+
+  const G4ParticleDefinition*  fLepton1;
+  const G4ParticleDefinition*  fLepton2;
+
+  G4int     fConvMode;
+  const G4ParticleDefinition*  fTheMuPlus;
+  const G4ParticleDefinition*  fTheMuMinus;
+
 };
 #endif