Geant4 11.1.1
Toolkit for the simulation of the passage of particles through matter
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GFlashSamplingShowerTuning.hh
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25//
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28//
29//---------------------------------------------------------------
30// GEANT 4 class header file
31//
32// GFlashSamplingShowerTuning
33//
34// Class description:
35//
36// Tuning class for GFlash homogeneous shower parameterisation.
37// Definitions:
38// <t>: shower center of gravity
39// T: Depth at shower maximum
40// Ec: Critical energy
41// X0: Radiation length
42// y = E/Ec
43//
44// Please, see hep-ex/0001020 for details.
45
46// Author: Joanna Weng - 11.2005
47//
48// Usage: use new statement for new instance of class, do not delete.
49// The instance of class will be deleted in
50// GFlashSamplingShowerParameterisation Destructor.
51//---------------------------------------------------------------
52#ifndef GFlashSamplingShowerTuning_hh
53#define GFlashSamplingShowerTuning_hh
54
56
58{
59 public:
60
63
64
65 public: // with description
66
67 G4double ParsAveT1(){ return -0.55;} // t1
68 G4double ParsAveT2(){ return -0.69;} // t2
69 // T_sam = log(exp( log T_hom) + t1*Fs-1 + t2*(1-ehat))
70
71 G4double ParsAveA1(){ return -0.476; } // a1
72 // alpha_sam = log(exp(log alphah_hom) +(a1*Fs-1))
73
74 G4double ParsSigLogT1(){ return -2.5;} // t1
75 G4double ParsSigLogT2(){ return 1.25;} // t2
76 // std::sqrt(var(ln(T_sam))) = 1/(t+t2*ln(y))
77
78 G4double ParsSigLogA1(){ return -0.82;} // a1
79 G4double ParsSigLogA2(){ return 0.79; } // a2
80 // std::sqrt(var(ln(alpha_sam))) = 1/(a1+a2*ln(y))
81
82 G4double ParsRho1(){ return 0.784; } // r1
83 G4double ParsRho2(){ return -0.023;} // r2
84 // Correlation(ln(T),ln(alpha))=r1+r2*ln(y)
85
86 // Radial profiles
87 // f(r) := (1/dE(t))(dE(t,r)/dr)
88 // Ansatz:
89 // f(r) = p(2*r*Rc**2)/(r**2+Rc**2)**2+(1-p)*(2*r*Rt**2)/(r**2+Rt**2)**2,
90 // 0<p<1
91
92 G4double ParsRC1(){ return -0.0203; } // c1
93 G4double ParsRC2(){ return 0.0397; } // c2
94 // Rc_sam = Rc_hom + c1 * (1-ehat) + c2 *Fs-1*exp (-tau)
95
96 G4double ParsRT1(){ return -0.14; } // t1
97 G4double ParsRT2(){ return -0.495; } // t2
98 // Rt_sam = Rc_hom + t1 * (1-ehat) + t2 *Fs-1*exp (-tau)
99
100 G4double ParsWC1(){ return 0.348; } // c1
101 G4double ParsWC2(){ return -0.642;} // c2
102 // W_sam = W_hom + (1-ehat)*(c1 + c2 *Fs-1 * exp (- (tau -1 )**2))
103
104 // Fluctuations on radial profiles through number of spots
105 // The total number of spots needed for a shower is
106
107 G4double ParsSpotN1(){ return 10.3; } // n1
108 G4double ParsSpotN2(){ return 0.959;} // n2
109 // Ns = n1*ln(Z)(E/GeV)**n2
110
111 // The number of spots per longitudinal interval is:
112 // (1/Ns)(dNs(t)/dt) = f(t)
113 // = (beta*t)**(alpha-1)*beta*std::exp(-beta*t)/Gamma(alpha)
114 // <t> = alpha_s/beta_s
115 // Ts = (alpha_s-1)/beta_s
116 // and
117 // Ts = T*(t1+t2*Z)
118 // alpha_s = alpha*(a1+a2*Z)
119
120 G4double ParsSpotT1(){ return 0.813; } // t1
121 G4double ParsSpotT2(){ return 0.0019;} // t2
122
123 G4double ParsSpotA1(){ return 0.844; } //a1
124 G4double ParsSpotA2(){ return 0.0026;} //a2
125
126 // Resolution
127
128 G4double ConstantResolution(){ return 0.00; }
129 G4double NoiseResolution() { return 0.00; } // not used
130 G4double SamplingResolution(){ return 0.11; } // not used
131
132};
133
134#endif
double G4double
Definition: G4Types.hh:83