]>
Commit | Line | Data |
---|---|---|
da32329d AM |
1 | /////////////////////////////////////////////////////////////////////////// |
2 | // | |
3 | // Copyright 2010 | |
4 | // | |
5 | // This file is part of starlight. | |
6 | // | |
7 | // starlight is free software: you can redistribute it and/or modify | |
8 | // it under the terms of the GNU General Public License as published by | |
9 | // the Free Software Foundation, either version 3 of the License, or | |
10 | // (at your option) any later version. | |
11 | // | |
12 | // starlight is distributed in the hope that it will be useful, | |
13 | // but WITHOUT ANY WARRANTY; without even the implied warranty of | |
14 | // MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the | |
15 | // GNU General Public License for more details. | |
16 | // | |
17 | // You should have received a copy of the GNU General Public License | |
18 | // along with starlight. If not, see <http://www.gnu.org/licenses/>. | |
19 | // | |
20 | /////////////////////////////////////////////////////////////////////////// | |
21 | // | |
22 | // File and Version Information: | |
75ce6a3a | 23 | // $Rev:: 193 $: revision of last commit |
24 | // $Author:: jnystrand $: author of last commit | |
25 | // $Date:: 2014-12-01 20:39:46 +0100 #$: date of last commit | |
da32329d AM |
26 | // |
27 | // Description: | |
28 | // | |
29 | // | |
30 | // | |
31 | /////////////////////////////////////////////////////////////////////////// | |
32 | ||
33 | ||
34 | #include <iostream> | |
35 | #include <fstream> | |
36 | #include <cmath> | |
37 | ||
38 | #include "starlightconstants.h" | |
39 | #include "narrowResonanceCrossSection.h" | |
40 | ||
41 | ||
42 | using namespace std; | |
43 | using namespace starlightConstants; | |
44 | ||
45 | ||
46 | //______________________________________________________________________________ | |
47 | narrowResonanceCrossSection::narrowResonanceCrossSection(const beamBeamSystem& bbsystem) | |
48 | :photonNucleusCrossSection(bbsystem) | |
49 | { | |
50 | _narrowYmax = inputParametersInstance.maxRapidity(); | |
51 | _narrowYmin = -1.0*_narrowYmax; | |
52 | _narrowNumY = inputParametersInstance.nmbRapidityBins(); | |
53 | _Ep = inputParametersInstance.protonEnergy(); | |
54 | } | |
55 | ||
56 | ||
57 | //______________________________________________________________________________ | |
58 | narrowResonanceCrossSection::~narrowResonanceCrossSection() | |
59 | { } | |
60 | ||
61 | ||
62 | //______________________________________________________________________________ | |
63 | void | |
64 | narrowResonanceCrossSection::crossSectionCalculation(const double) // _bwnormsave (unused) | |
65 | { | |
66 | // This subroutine calculates the vector meson cross section assuming | |
67 | // a narrow resonance. For reference, see STAR Note 386. | |
68 | ||
da32329d AM |
69 | double W,dY; |
70 | double y1,y2,y12,ega1,ega2,ega12; | |
75ce6a3a | 71 | double csgA1,csgA2,csgA12,int_r,dR; |
da32329d | 72 | double Eth; |
75ce6a3a | 73 | int J,NY,beam; |
da32329d AM |
74 | |
75 | NY = _narrowNumY; | |
76 | dY = (_narrowYmax-_narrowYmin)/double(NY); | |
77 | ||
78 | cout<<" Using Narrow Resonance ..."<<endl; | |
79 | ||
80 | W = getChannelMass(); | |
81 | Eth=0.5*(((W+protonMass)*(W+protonMass)- | |
82 | protonMass*protonMass)/(_Ep+sqrt(_Ep*_Ep-protonMass*protonMass))); | |
83 | ||
84 | cout<<" gamma+nucleon Threshold: "<<Eth<<endl; | |
85 | int_r=0.; | |
75ce6a3a | 86 | |
87 | int A_1 = getbbs().beam1().A(); | |
88 | int A_2 = getbbs().beam2().A(); | |
da32329d | 89 | |
75ce6a3a | 90 | // Do this first for the case when the first beam is the photon emitter |
91 | // Treat pA separately with defined beams | |
92 | // The variable beam (=1,2) defines which nucleus is the target | |
da32329d AM |
93 | for(J=0;J<=(NY-1);J++){ |
94 | ||
95 | y1 = _narrowYmin + double(J)*dY; | |
96 | y2 = _narrowYmin + double(J+1)*dY; | |
97 | y12 = 0.5*(y1+y2); | |
98 | ||
75ce6a3a | 99 | if( A_2 == 1 && A_1 != 1 ){ |
100 | // pA, first beam is the nucleus and is in this case the target | |
101 | // Egamma = 0.5*W*exp(-Y); | |
102 | ega1 = 0.5*W*exp(-y1); | |
103 | ega2 = 0.5*W*exp(-y2); | |
104 | ega12 = 0.5*W*exp(-y12); | |
105 | beam = 1; | |
106 | } else if( A_1 ==1 && A_2 != 1){ | |
107 | // pA, second beam is the nucleus and is in this case the target | |
108 | // Egamma = 0.5*W*exp(Y); | |
109 | ega1 = 0.5*W*exp(y1); | |
110 | ega2 = 0.5*W*exp(y2); | |
111 | ega12 = 0.5*W*exp(y12); | |
112 | beam = 2; | |
113 | } else { | |
114 | // Egamma = 0.5*W*exp(Y); | |
115 | ega1 = 0.5*W*exp(y1); | |
116 | ega2 = 0.5*W*exp(y2); | |
117 | ega12 = 0.5*W*exp(y12); | |
118 | beam = 2; | |
119 | } | |
120 | ||
121 | // ega1 = 0.5*W*exp(y1); | |
122 | // ega2 = 0.5*W*exp(y2); | |
123 | // ega12 = 0.5*W*exp(y12); | |
da32329d AM |
124 | |
125 | if(ega1 < Eth) | |
126 | continue; | |
127 | if(ega2 > maxPhotonEnergy()) | |
128 | continue; | |
129 | ||
75ce6a3a | 130 | csgA1=getcsgA(ega1,W,beam); |
da32329d AM |
131 | |
132 | // Middle Point =====>>> | |
75ce6a3a | 133 | csgA12=getcsgA(ega12,W,beam); |
da32329d AM |
134 | |
135 | // Second Point =====>>> | |
75ce6a3a | 136 | csgA2=getcsgA(ega2,W,beam); |
da32329d AM |
137 | |
138 | // Sum the contribution for this W,Y. | |
75ce6a3a | 139 | dR = ega1*photonFlux(ega1,beam)*csgA1; |
140 | dR = dR + 4.*ega12*photonFlux(ega12,beam)*csgA12; | |
141 | dR = dR + ega2*photonFlux(ega2,beam)*csgA2; | |
da32329d AM |
142 | dR = dR*(dY/6.); |
143 | ||
75ce6a3a | 144 | // cout<<" y: "<<y12<<" egamma: "<<ega12<<" flux: "<<photonFlux(ega12,beam)<<" sigma_gA: "<<10000000.*csgA12<<" dsig/dy (microb): "<<10000.*dR/dY<<endl; |
da32329d | 145 | |
da32329d AM |
146 | int_r = int_r+dR; |
147 | } | |
75ce6a3a | 148 | |
149 | // Repeat the loop for the case when the second beam is the photon emitter. | |
150 | // Don't repeat for pA | |
151 | if( !( (A_2 == 1 && A_1 != 1) || (A_1 == 1 && A_2 != 1) ) ){ | |
152 | for(J=0;J<=(NY-1);J++){ | |
153 | ||
154 | y1 = _narrowYmin + double(J)*dY; | |
155 | y2 = _narrowYmin + double(J+1)*dY; | |
156 | y12 = 0.5*(y1+y2); | |
157 | ||
158 | beam = 1; | |
159 | ega1 = 0.5*W*exp(-y1); | |
160 | ega2 = 0.5*W*exp(-y2); | |
161 | ega12 = 0.5*W*exp(-y12); | |
162 | ||
163 | if(ega2 < Eth) | |
164 | continue; | |
165 | if(ega1 > maxPhotonEnergy()) | |
166 | continue; | |
167 | ||
168 | csgA1=getcsgA(ega1,W,beam); | |
169 | ||
170 | // Middle Point =====>>> | |
171 | csgA12=getcsgA(ega12,W,beam); | |
172 | ||
173 | // Second Point =====>>> | |
174 | csgA2=getcsgA(ega2,W,beam); | |
175 | ||
176 | // Sum the contribution for this W,Y. | |
177 | dR = ega1*photonFlux(ega1,beam)*csgA1; | |
178 | dR = dR + 4.*ega12*photonFlux(ega12,beam)*csgA12; | |
179 | dR = dR + ega2*photonFlux(ega2,beam)*csgA2; | |
180 | dR = dR*(dY/6.); | |
181 | ||
182 | // cout<<" y: "<<y12<<" egamma: "<<ega12<<" flux: "<<photonFlux(ega12,beam)<<" sigma_gA: "<<10000000.*csgA12<<" dsig/dy (microb): "<<10000.*dR/dY<<endl; | |
183 | ||
184 | int_r = int_r+dR; | |
185 | } | |
186 | } | |
da32329d AM |
187 | cout<<" Cross section (mb): " <<10.*int_r<<endl; |
188 | } |