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Please see the license in the file LICENSE and URL above * 16 // * for the full disclaimer and the limitatio 16 // * for the full disclaimer and the limitation of liability. * 17 // * 17 // * * 18 // * This code implementation is the result 18 // * This code implementation is the result of the scientific and * 19 // * technical work of the GEANT4 collaboratio 19 // * technical work of the GEANT4 collaboration. * 20 // * By using, copying, modifying or distri 20 // * By using, copying, modifying or distributing the software (or * 21 // * any work based on the software) you ag 21 // * any work based on the software) you agree to acknowledge its * 22 // * use in resulting scientific publicati 22 // * use in resulting scientific publications, and indicate your * 23 // * acceptance of all terms of the Geant4 Sof 23 // * acceptance of all terms of the Geant4 Software license. * 24 // ******************************************* 24 // ******************************************************************** 25 // 25 // 26 // author: Vladimir.Grichine@cern.ch 26 // author: Vladimir.Grichine@cern.ch 27 // 27 // 28 // Implements data from: Barashenkov V.S., Nuc 28 // Implements data from: Barashenkov V.S., Nucleon-Nucleus Cross Section, 29 // Preprint JINR P2-89-770, p. 12, Dubna 1989 29 // Preprint JINR P2-89-770, p. 12, Dubna 1989 (scanned version from KEK) 30 // Based on G. Folger version of G4PiNuclearCr 30 // Based on G. Folger version of G4PiNuclearCrossSection class 31 // 31 // 32 // Modified: 16.08.2018 V.Ivanchenko - major u << 32 // Modified: >> 33 // 05.03.07 V.Ivanchenko - add IfZAApplicable, remove "debug" >> 34 // 11.09.09 V.Ivanchenko - fixed bug in interpolation 33 // 35 // 34 36 35 #include "G4NucleonNuclearCrossSection.hh" 37 #include "G4NucleonNuclearCrossSection.hh" >> 38 #include "G4SystemOfUnits.hh" 36 #include "G4DynamicParticle.hh" 39 #include "G4DynamicParticle.hh" 37 #include "G4ParticleDefinition.hh" << 40 #include "G4Neutron.hh" 38 #include "G4ComponentBarNucleonNucleusXsc.hh" << 41 #include "G4Proton.hh" >> 42 >> 43 // factory >> 44 #include "G4CrossSectionFactory.hh" >> 45 // >> 46 G4_DECLARE_XS_FACTORY(G4NucleonNuclearCrossSection); >> 47 >> 48 >> 49 // Group 1: He, Be, C for 44 energies >> 50 >> 51 const G4double G4NucleonNuclearCrossSection::e1[44] = >> 52 { >> 53 0.014, 0.015, 0.017, 0.02, 0.022, 0.025, 0.027, 0.03, 0.035, 0.04, >> 54 0.045, 0.05, 0.06, 0.07, 0.08, 0.09, 0.1, 0.12, 0.14, 0.15, >> 55 0.16, 0.18, 0.20, 0.25, 0.30, 0.35, 0.4, 0.5, 0.6, 0.7, >> 56 0.8, 0.9, 1.0, 1.5, 2.0, 3.0, 5.0, 7.0, 10.0, 20.0, >> 57 50.0, 100.0, 500.0, 1000.0 >> 58 }; >> 59 >> 60 const G4double G4NucleonNuclearCrossSection::he_m_t[44] = >> 61 { >> 62 1090, 1020, 915, 800, 710, 640, 600, 560, 500, 440, 390, 360, 295, 256, 220, 192, >> 63 168, 136, 120, 116, 114, 110, 107, 104, 106, 108, 110, 120, 126, 135, 140, 144, 146, >> 64 148, 152, 150, 146, 142, 138, 132, 129, 126, 127, 128 >> 65 }; >> 66 const G4double G4NucleonNuclearCrossSection::he_m_in[44] = >> 67 { >> 68 0, 5, 10, 20, 35, 55, 70, 80, 90, 105, 115, 115, 100, 90, 86, 84, 84, 82, 80, 80, 80, 80, >> 69 79, 78, 80, 84, 88, 94, 100, 105, 108, 108, 108, 112, 114, 114, 112, 110, 108, 106, 104, >> 70 101, 102, 102 >> 71 }; >> 72 const G4double G4NucleonNuclearCrossSection::he_p_in[44] = >> 73 { >> 74 0, 2, 3, 13, 30, 50, 65, 77, 90, 105, 115, 115, 100, 90, 86, 84, 84, 82, 80, 80, 80, 80, >> 75 79, 78, 80, 84, 88, 94, 100, 105, 108, 108, 108, 112, 114, 114, 112, 110, 108, 106, 104, >> 76 101, 102, 102 >> 77 }; >> 78 >> 79 const G4double G4NucleonNuclearCrossSection::be_m_t[44] = >> 80 { >> 81 1490, 1460, 1400, 1350, 1270, 1200, 1160, 1100, 1000, 910, 810, 740, 625, 575, 455, 406, >> 82 365, 310, 275, 262, 255, 240, 235, 225, 225, 230, 238, 252, 270, 282, 288, 290, 294, 303, >> 83 303, 300, 292, 284, 277, 267, 263, 264, 268, 268 >> 84 }; >> 85 const G4double G4NucleonNuclearCrossSection::be_m_in[44] = >> 86 { >> 87 650, 640, 617, 595, 555, 520, 495, 470, 430, 385, 350, 320, 270, 250, 210, 190, 185, 178, >> 88 175, 175, 175, 175, 175, 170, 170, 172, 176, 184, 194, 200, 209, 213, 214, 216, 216, 212, >> 89 210, 210, 210, 210, 210, 210, 210, 210 >> 90 }; >> 91 const G4double G4NucleonNuclearCrossSection::be_p_in[44] = >> 92 { >> 93 490, 540, 580, 545, 525, 495, 470, 450, 420, 370, 340, 310, 262, 242, 205, 185, 180, 175, >> 94 172, 175, 175, 175, 175, 170, 170, 172, 176, 184, 194, 200, 209, 213, 214, 216, 216, 212, >> 95 210, 210, 210, 210, 210, 210, 210, 210 >> 96 }; >> 97 >> 98 const G4double G4NucleonNuclearCrossSection::c_m_t[44] = >> 99 { >> 100 1240, 1370, 1450, 1455, 1445, 1385, 1345, 1290, 1210, 1110, 1020, 940, 800, 700, 604, 530, >> 101 475, 396, 350, 336, 320, 303, 294, 280, 280, 286, 296, 314, 330, 344, 356, 360, 364, 384, >> 102 388, 384, 364, 352, 344, 330, 324, 324, 332, 332 >> 103 }; >> 104 const G4double G4NucleonNuclearCrossSection::c_m_in[44] = >> 105 { >> 106 590, 570, 542, 510, 500, 460, 445, 430, 395, 380, 350, 330, 295, 270, 255, 240, 228, 222, >> 107 216, 216, 210, 210, 210, 208, 210, 214, 216, 228, 240, 248, 254, 257, 260, 262, 260, 256, >> 108 252, 252, 250, 250, 248, 248, 248, 248 >> 109 }; >> 110 const G4double G4NucleonNuclearCrossSection::c_p_in[44] = >> 111 { >> 112 310, 330, 400, 440, 450, 435, 430, 420, 385, 370, 340, 320, 288, 263, 249, 234, 222, 216, >> 113 210, 211, 205, 208, 210, 208, 210, 214, 216, 228, 240, 248, 254, 257, 260, 262, 260, 256, >> 114 252, 252, 250, 250, 248, 248, 248, 248 >> 115 }; >> 116 >> 117 // Group 2: N, O, Na for 44 energies (e1=e2) >> 118 >> 119 const G4double G4NucleonNuclearCrossSection::e2[44] = >> 120 { >> 121 0.014, 0.015, 0.017, .02, 0.022, 0.025, 0.027, 0.03, 0.035, .04, 0.045, 0.05, .06, 0.07, >> 122 .08, 0.09, .1, .12, .14, .15, .16, .18, .20, .25, .30, .35, .4 , 0.5, 0.6, 0.7, 0.8, >> 123 0.9, 1, 1.5, 2, 3, 5, 7, 10, >> 124 20, 50, 100, 500, 1000 >> 125 }; >> 126 >> 127 const G4double G4NucleonNuclearCrossSection::n_m_t[44] = >> 128 { >> 129 1420,1480, 1537, 1550, 1525, 1500, 1480, 1425, 1340, 1260, 1175, 1090, 930, 805, 690, 612, >> 130 552, 462, 402, 384, 372, 350, 345, 326, 324, 328, 336, 356, 372, 388, 400, 408, 415, 430, >> 131 435, 432, 415, 402, 390, 375, 367, 370, 382, 385 >> 132 }; >> 133 const G4double G4NucleonNuclearCrossSection::n_m_in[44] = >> 134 { >> 135 680, 665, 625, 580, 562, 525, 510, 485, 450, 435, 410, 387, 340, 310, 290, 280, 276, 274, >> 136 260, 258, 254, 247, 245, 240, 240, 244, 250, 260, 268, 275, 280, 285, 290, 295, 300, 294, >> 137 292, 290, 285, 285, 282, 282, 282, 282 >> 138 }; >> 139 const G4double G4NucleonNuclearCrossSection::n_p_in[44] = >> 140 { >> 141 420, 440, 470, 490, 497, 500, 480, 462, 440, 425, 400, 377, 333, 303, 284, 274, 270, 268, >> 142 254, 252, 247, 245, 245, 240, 240, 244, 250, 260, 268, 275, 280, 285, 290, 295, 300, 294, >> 143 292, 290, 285, 285, 282, 282, 282, 282 >> 144 }; >> 145 >> 146 const G4double G4NucleonNuclearCrossSection::o_m_t[44] = >> 147 { >> 148 1520, 1570, 1630, 1660, 1647, 1623, 1595, 1555, 1475, 1395, 1290, 1207, 1035, 925, 816, >> 149 720, 645, 540, 462, 438, 415, 392, 378, 362, 361, 381, 390, 403, 417, 440, 460, 470, >> 150 479, 498, 504, 498, 477, 457, 443, 427, 420, 425, 429, 430 >> 151 }; >> 152 const G4double G4NucleonNuclearCrossSection::o_m_in[44] = >> 153 { >> 154 750, 740, 700, 650, 620, 575, 555, 530, 505, 462, 435, 420, 375, 345, 320, 310, 300, 293, >> 155 288, 282, 282, 280, 276, 270, 271, 275, 280, 290, 295, 304, 310, 315, 318, 332, 335, 330, >> 156 323, 320, 317, 315, 315, 315, 315, 315 >> 157 }; >> 158 const G4double G4NucleonNuclearCrossSection::o_p_in[44] = >> 159 { >> 160 460, 485, 510, 535, 537, 532, 520, 500, 460, 432, 405, 390, 350, 320, 310, 304, 293, 287, >> 161 283, 279, 279, 278, 276, 270, 271, 275, 280, 290, 295, 304, 310, 315, 318, 332, 335, 330, >> 162 323, 320, 317, 315, 315, 315, 315, 315 >> 163 }; >> 164 >> 165 const G4double G4NucleonNuclearCrossSection::na_m_t[44] = >> 166 { >> 167 1570, 1620, 1695, 1730, 1750, 1760, 1755, 1740, 1710, 1643, 1560, 1480, 1343, 1220, 1073, >> 168 953, 860, 720, 618, 582, 546, 522, 504, 484, 492, 500, 512, 538, 560, 586, 608, 622, 632, >> 169 660, 668, 664, 640, 616, 596, 568, 568, 568, 568, 568 >> 170 }; >> 171 const G4double G4NucleonNuclearCrossSection::na_m_in[44] = >> 172 { >> 173 960, 930, 890, 822, 790, 750, 725, 686, 620, 600, 575, 540, 497, 450, 414, 390, 380, 372, >> 174 354, 360, 355, 354, 350, 350, 350, 356, 364, 384, 392, 400, 408, 410, 420, 408, 412, 420, >> 175 411, 409, 407, 403, 400, 400, 400, 400 >> 176 }; >> 177 const G4double G4NucleonNuclearCrossSection::na_p_in[44] = >> 178 { >> 179 600, 617, 660, 675, 680, 680, 670, 650, 575, 550, 525, 490, 450, 420, 385, 367, 360, 350, >> 180 350, 350, 345, 347, 350, 350, 350, 356, 364, 384, 392, 400, 408, 410, 420, 408, 412, 420, >> 181 411, 409, 407, 403, 400, 400, 400, 400 >> 182 }; >> 183 >> 184 // Al, Si, Ca for 45 energies >> 185 >> 186 const G4double G4NucleonNuclearCrossSection::e3[45] = >> 187 { >> 188 0.014, 0.015, 0.016, 0.017, .02, 0.022, 0.025, 0.027, 0.03, 0.035, .04, 0.045, 0.05, .06, 0.07, >> 189 .08, 0.09, .1, .12, .14, .15, .16, .18, .20, .25, .30, .35, 0.4, 0.5, 0.6, >> 190 0.7, 0.8, 0.9, 1, 1.5, 2, 3, 5, 7, 10, 20, 50, 100, 500, 1000 >> 191 }; >> 192 >> 193 const G4double G4NucleonNuclearCrossSection::al_m_t[45] = >> 194 { >> 195 1735, 1750, 1760, 1795, 1830, 1855, 1885, 1895, 1900, 1870, 1835, 1785, 1710, 1522, 1350, >> 196 1212, 1080, 972, 816, 720, 678, 642, 600, 567, 558, 560, 578, 592, 616, 644, >> 197 672, 688, 708, 720, 736, 754, 736, 706, 680, 672, 646, 632, 632, 632, 632 >> 198 }; >> 199 const G4double G4NucleonNuclearCrossSection::al_m_in[45] = >> 200 { >> 201 1000, 990, 975, 950, 905, 875, 825, 800, 762, 690, 652, 610, 570, 495, 480, >> 202 456, 444, 432, 420, 420, 420, 420, 410, 410, 400, 402, 404, 408, 424, 438, >> 203 448, 450, 454, 456, 472, 480, 466, 456, 452, 448, 444, 440, 440, 440, 440 >> 204 }; >> 205 const G4double G4NucleonNuclearCrossSection::al_p_in[45] = >> 206 { >> 207 650, 682, 690, 715, 750, 762, 750, 740, 720, 655, 617, 575, 540, 470, 455, >> 208 // 532, 420, 408, 400, 403, 403, 408, 406, 404, 400, 402, 404, 408, 424, 438, >> 209 432, 420, 408, 400, 403, 403, 408, 406, 404, 400, 402, 404, 408, 424, 438, >> 210 448, 450, 454, 456, 472, 480, 466, 456, 452, 448, 444, 440, 440, 440, 440 >> 211 }; >> 212 >> 213 const G4double G4NucleonNuclearCrossSection::si_m_t[45] = >> 214 { >> 215 1810, 1833, 1850, 1872, 1920, 1950, 1995, 2020, 2035, 2000, 1930, 1850, 1760, 1570, 1400, >> 216 1255, 1110, 1008, 846, 742, 696, 671, 623, 588, 584, 584, 602, 618, 645, 679, >> 217 708, 727, 746, 757, 769, 782, 771, 734, 710, 698, 672, 654, 650, 650, 650 >> 218 }; >> 219 const G4double G4NucleonNuclearCrossSection::si_m_in[45] = >> 220 { >> 221 1060, 1035, 1015, 990, 935, 900, 860, 830, 790, 725, 665, 630, 600, 520, 504, >> 222 486, 470, 456, 444, 432, 432, 432, 418, 418, 415, 412, 416, 422, 440, 460, >> 223 472, 476, 479, 480, 492, 496, 488, 472, 472, 464, 460, 452, 448, 448, 448 >> 224 }; >> 225 const G4double G4NucleonNuclearCrossSection::si_p_in[45] = >> 226 { >> 227 670, 700, 725, 750, 780, 780, 770, 757, 735, 690, 635, 585, 570, 490, 475, >> 228 460, 446, 431, 423, 425, 425, 425, 425, 422, 422, 412, 416, 422, 440, 460, >> 229 472, 476, 479, 480, 492, 496, 488, 472, 472, 464, 460, 452, 448, 448, 448 >> 230 }; >> 231 >> 232 const G4double G4NucleonNuclearCrossSection::ca_m_t[45] = >> 233 { >> 234 2180, 2130, 2095, 2075, 2115, 2150, 2220, 2250, 2300, 2365, 2360, 2280, 2180, 2000, >> 235 1805, 1650, 1500, 1340, 1140, 990, 940, 890, 825, 790, 770, 773, 787, 800, 830, 870, >> 236 905, 930, 950, 965, 990, 1002, 990, 965, 945, 925, 892, 860, 860, 860, 860 >> 237 }; >> 238 const G4double G4NucleonNuclearCrossSection::ca_m_in[45] = >> 239 { >> 240 1240, 1225, 1200, 1180, 1125, 1090, 1045, 1020, 980, 925, 880, 825, 770, 680, 640, >> 241 620, 615, 600, 580, 565, 560, 560, 560, 550, 535, 530, 540, 550, 570, 595, 610, 615, >> 242 620, 622, 629, 630, 620, 612, 607, 592, 587, 580, 580, 580, 580 >> 243 }; >> 244 const G4double G4NucleonNuclearCrossSection::ca_p_in[45] = >> 245 { >> 246 770, 800, 823, 850, 900, 925, 935, 920, 895, 835, 800, 750, 715, 640, 605, 590, 588, >> 247 573, 555, 543, 540, 540, 540, 535, 530, 530, 540, 550, 570, 595, 610, 615, >> 248 620, 622, 629, 630, 620, 612, 607, 592, 587, 580, 580, 580, 580 >> 249 }; >> 250 >> 251 // Fe, Cu, Mo for 47 energies >> 252 >> 253 const G4double G4NucleonNuclearCrossSection::e4[47] = >> 254 { >> 255 0.014, 0.015, 0.017, .02, 0.022, 0.025, 0.027, 0.03, 0.033, 0.035, 0.037, .04, 0.045, >> 256 0.05, 0.055, .06, 0.07, .08, 0.09, .1, .12, .14, .15, .16, .18, .20, .25, .30, .35, >> 257 .4 , 0.5, 0.6, 0.7, 0.8, 0.9, 1, 1.5, 2, 3, 5, 7, 10, >> 258 20, 50, 100, 500, 1000 >> 259 }; >> 260 >> 261 const G4double G4NucleonNuclearCrossSection::fe_m_t[47] = >> 262 { >> 263 2580, 2490, 2370, 2282, 2275, 2285, 2320, 2370, 2432, 2445, 2460, 2485, 2530, 2540, >> 264 2517, 2480, 2290, 2110, 1940, 1790, 1510, 1290, 1220, 1150, 1070, 1030, 1013, 1020, >> 265 1030, 1043, 1075, 1110, 1133, 1163, 1185, 1225, 1252, 1260, 1260, 1233, 1207, 1185, >> 266 1140, 1110, 1110, 1110, 1110 >> 267 }; >> 268 const G4double G4NucleonNuclearCrossSection::fe_m_in[47] = >> 269 { >> 270 1440, 1433, 1390, 1325, 1280, 1260, 1215, 1180, 1140, 1110, 1080, 1040, 990, 955, 920, >> 271 885, 835, 800, 780, 765, 750, 725, 720, 720, 710, 700, 700, 700, 712, 705, 735, 750, >> 272 765, 775, 780, 795, 810, 813, 810, 784, 757, 743, 735, 720, 720, 720, 720 >> 273 }; >> 274 const G4double G4NucleonNuclearCrossSection::fe_p_in[47] = >> 275 { >> 276 900, 960, 1070, 1090, 1115, 1120, 1115, 1080, 1045, 1025, 1000, 960, 900, 885, 865, 790, >> 277 765, 740, 720, 700, 697, 697, 697, 697, 695, 690, 688, 690, 712, 705, 735, 750, >> 278 765, 775, 780, 795, 810, 813, 810, 784, 757, 743, 735, 720, 720, 720, 720 >> 279 }; >> 280 >> 281 const G4double G4NucleonNuclearCrossSection::cu_m_t[47] = >> 282 { >> 283 2920, 2800, 2615, 2480, 2455, 2430, 2440, 2460, 2500, 2530, 2560, 2615, 2690, 2720, >> 284 2700, 2645, 2500, 2320, 2140, 1970, 1670, 1460, 1380, 1285, 1200, 1160, 1140, 1147, >> 285 1163, 1170, 1200, 1237, 1265, 1285, 1305, 1328, 1375, 1390, 1395, 1370, 1335, 1315, >> 286 1270, 1230, 1230, 1230, 1230 >> 287 }; >> 288 const G4double G4NucleonNuclearCrossSection::cu_m_in[47] = >> 289 { >> 290 1540, 1535, 1500, 1445, 1407, 1380, 1330, 1300, 1285, 1270, 1240, 1190, 1090, 1010, >> 291 940, 920, 860, 835, 820, 810, 800, 780, 775, 770, 760, 760, 758, 765, 765, 770, 795, >> 292 810, 825, 830, 840, 848, 870, 870, 868, 840, 825, 810, 803, 795, 795, 795, 795 >> 293 }; >> 294 const G4double G4NucleonNuclearCrossSection::cu_p_in[47] = >> 295 { >> 296 935, 1000, 1060, 1190, 1220, 1250, 1240, 1210, 1150, 1130, 1115, 1050, 985, 950, 890, >> 297 870, 820, 800, 785, 780, 770, 750, 745, 740, 735, 735, 745, 760, 762, 770, 795, >> 298 810, 825, 830, 840, 848, 870, 870, 868, 840, 825, 810, 803, 795, 795, 795, 795 >> 299 }; >> 300 >> 301 const G4double G4NucleonNuclearCrossSection::mo_m_t[47] = >> 302 { >> 303 4150, 4040, 3800, 3490, 3300, 3060, 2960, 2845, 2785, 2820, 2850, 2980, 3170, 3230, >> 304 3270, 3280, 3225, 3075, 2895, 2710, 2355, 2060, 1925, 1800, 1630, 1560, 1540, 1550, >> 305 1570, 1590, 1650, 1685, 1715, 1740, 1760, 1780, 1850, 1880, 1858, 1815, 1790, 1782, >> 306 1720, 1690, 1690, 1690, 1690 >> 307 }; >> 308 const G4double G4NucleonNuclearCrossSection::mo_m_in[47] = >> 309 { >> 310 1790, 1775, 1740, 1680, 1640, 1580, 1550, 1510, 1460, 1440, 1418, 1380, 1330, 1280, >> 311 1240, 1200, 1155, 1140, 1110, 1110, 1080, 1065, 1050, 1050, 1025, 1020, 1015, 1020, >> 312 1022, 1026, 1060, 1085, 1100, 1110, 1120, 1127, 1150, 1160, 1140, 1100, 1085, 1080, >> 313 1070, 1070, 1070, 1070, 1070 >> 314 }; >> 315 const G4double G4NucleonNuclearCrossSection::mo_p_in[47] = >> 316 { >> 317 1025, 1080, 1190, 1380, 1440, 1495, 1475, 1420, 1350, 1310, 1300, 1290, 1250, 1200, >> 318 1170, 1130, 1095, 1060, 1040, 1022, 1020, 1016, 1016, 1016, 1016, 1012, 1005, 1005, >> 319 1005, 1010, 1060, 1085, 1100, 1110, 1120, 1127, 1150, 1160, 1140, 1100, 1085, 1080, >> 320 1070, 1070, 1070, 1070, 1070 >> 321 }; >> 322 >> 323 // Cd, Sn, W for 48 energies >> 324 >> 325 const G4double G4NucleonNuclearCrossSection::e5[48] = >> 326 { >> 327 0.014, 0.015, 0.017, 0.018, .02, 0.022, 0.025, 0.027, 0.03, 0.033, 0.035, .04, >> 328 0.045, 0.05, 0.055, .06, .065, 0.07, .08, 0.09, .1, .12, .14, .15, .16, .18, >> 329 .20, .25, .30, .35, .4 , 0.5, 0.6, 0.7, 0.8, 0.9, 1, 1.5, 2, 3, 5, 7, 10, 20, >> 330 50, 100, 500, 1000 >> 331 }; >> 332 >> 333 const G4double G4NucleonNuclearCrossSection::cd_m_t[48] = >> 334 { >> 335 4420, 4280, 4170, 4070, 3860, 3680, 3420, 3280, 3125, 3060, 3080, 3190, 3350, 3445, >> 336 3510, 3540, 3560, 3550, 3460, 3300, 3030, 2640, 2340, 2190, 2070, 1950, 1770, 1732, >> 337 1740, 1760, 1780, 1832, 1885, 1925, 1945, 1960, 1980, 2070, 2080, 2065, 2040, 2022, >> 338 1980, 1940, 1870, 1870, 1870, 1870 >> 339 }; >> 340 const G4double G4NucleonNuclearCrossSection::cd_m_in[48]= >> 341 { >> 342 1920, 1910, 1880, 1860, 1840, 1800, 1760, 1720, 1675, 1630, 1600, 1520, 1465, 1420, >> 343 1390, 1340, 1310, 1280, 1275, 1235, 1225, 1200, 1170, 1170, 1170, 1165, 1145, 1140, >> 344 1140, 1135, 1160, 1180, 1220, 1240, 1250, 1260, 1265, 1270, 1275, 1250, 1222, 1222, >> 345 1220, 1215, 1190, 1190, 1190, 1190 >> 346 }; >> 347 const G4double G4NucleonNuclearCrossSection::cd_p_in[48] = >> 348 { >> 349 1020, 1100, 1225, 1290, 1440, 1520, 1575, 1560, 1518, 1460, 1420, 1400, 1365, 1340, >> 350 1300, 1280, 1260, 1200, 1190, 1160, 1125, 1125, 1125, 1125, 1125, 1125, 1120, 1120, >> 351 1120, 1118, 1146, 1180, 1220, 1240, 1250, 1260, 1265, 1270, 1275, 1250, 1222, 1222, >> 352 1220, 1215, 1190, 1190, 1190, 1190 >> 353 }; >> 354 >> 355 const G4double G4NucleonNuclearCrossSection::sn_m_t[48] = >> 356 { >> 357 4420, 4400, 4260, 4150, 3980, 3770, 3530, 3370, 3245, 3180, 3170, 3260, 3400, 3500, >> 358 3560, 3610, 3650, 3680, 3580, 3390, 3190, 2760, 2430, 2295, 2175, 1990, 1880, 1810, >> 359 1820, 1840, 1865, 1940, 1985, 2020, 2040, 2060, 2080, 2160, 2185, 2180, 2110, 2105, >> 360 2080, 2050, 1980, 1980, 1980, 1980 >> 361 }; >> 362 const G4double G4NucleonNuclearCrossSection::sn_m_in[48] = >> 363 { >> 364 1945, 1940, 1905, 1890, 1860, 1830, 1780, 1755, 1717, 1680, 1645, 1570, 1500, 1455, >> 365 1410, 1370, 1340, 1320, 1290, 1285, 1260, 1240, 1235, 1212, 1200, 1200, 1200, 1190, >> 366 1190, 1200, 1210, 1240, 1270, 1285, 1300, 1300, 1310, 1320, 1320, 1290, 1240, 1240, >> 367 1240, 1240, 1240, 1240, 1240, 1240 >> 368 }; >> 369 const G4double G4NucleonNuclearCrossSection::sn_p_in[48] = >> 370 { >> 371 1020, 1080, 1270, 1335, 1465, 1505, 1610, 1610, 1550, 1535, 1500, 1440, 1407, 1370, >> 372 1340, 1300, 1285, 1260, 1230, 1215, 1200, 1180, 1170, 1170, 1165, 1165, 1170, 1165, >> 373 1165, 1183, 1195, 1240, 1270, 1285, 1300, 1300, 1310, 1320, 1320, 1290, 1240, 1240, >> 374 1240, 1240, 1240, 1240, 1240, 1240 >> 375 }; >> 376 >> 377 const G4double G4NucleonNuclearCrossSection::w_m_t[48] = >> 378 { >> 379 5320, 5430, 5480, 5450, 5330, 5190, 4960, 4790, 4550, 4340, 4200, 4070, 4000, 4030, >> 380 4125, 4220, 4270, 4390, 4440, 4360, 4200, 3800, 3380, 3200, 3040, 2790, 2660, 2575, >> 381 2575, 2600, 2640, 2690, 2755, 2790, 2812, 2837, 2850, 2950, 3000, 2970, 2940, 2910, >> 382 2880, 2820, 2730, 2730, 2730, 2730 >> 383 }; >> 384 const G4double G4NucleonNuclearCrossSection::w_m_in[48] = >> 385 { >> 386 2440, 2400, 2370, 2350, 2310, 2270, 2220, 2195, 2150, 2100, 2070, 2010, 1945, 1900, >> 387 1850, 1820, 1780, 1760, 1730, 1720, 1680, 1680, 1660, 1660, 1650, 1650, 1640, 1640, >> 388 1612, 1615, 1625, 1640, 1700, 1720, 1730, 1740, 1750, 1780, 1780, 1750, 1740, 1735, >> 389 1710, 1695, 1680, 1680, 1680, 1680 >> 390 }; >> 391 const G4double G4NucleonNuclearCrossSection::w_p_in[48] = >> 392 { >> 393 950, 1020, 1240, 1400, 1560, 1670, 1760, 1830, 1850, 1855, 1870, 1840, 1800, 1770, >> 394 1740, 1715, 1680, 1670, 1650, 1620, 1610, 1600, 1600, 1600, 1600, 1600, 1600, 1595, >> 395 1585, 1595, 1615, 1640, 1700, 1720, 1730, 1740, 1750, 1780, 1780, 1750, 1740, 1735, >> 396 1710, 1695, 1680, 1680, 1680, 1680 >> 397 }; >> 398 >> 399 // Pb, U for 46 energies >> 400 >> 401 const G4double G4NucleonNuclearCrossSection::e6[46] = >> 402 { >> 403 0.014, 0.015, 0.017, 0.019, 0.02, 0.022, 0.025, 0.027, 0.03, 0.035, >> 404 0.04, 0.045, 0.05, 0.055, 0.06, 0.07, 0.08, 0.09, 0.1, 0.12, >> 405 0.14, 0.15, 0.16, 0.18, 0.20, 0.25, 0.30, 0.35, 0.4 , 0.5, >> 406 0.6, 0.7, 0.8, 0.9, 1.0, 1.5, 2.0, 3.0, 5.0, 7.0, >> 407 10.0, 20.0, 50.0, 100.0, 500.0, 1000.0 >> 408 }; >> 409 >> 410 const G4double G4NucleonNuclearCrossSection::pb_m_t[46] = >> 411 { >> 412 5300, 5440, 5720, 5880, 5765, 5745, 5480, 5280, 4970, 4550, 4390, 4300, 4265, 4325, >> 413 4450, 4540, 4740, 4710, 4600, 4100, 3660, 3480, 3300, 3000, 2890, 2865, 2855, 2850, >> 414 2865, 2920, 2955, 3000, 3030, 3060, 3105, 3240, 3290, 3270, 3240, 3180, 3090, 3060, >> 415 2970, 2970, 2970, 2970 >> 416 >> 417 }; >> 418 const G4double G4NucleonNuclearCrossSection::pb_m_in[46] = >> 419 { >> 420 2580, 2550, 2505, 2462, 2460, 2435, 2380, 2355, 2280, 2180, 2170, 2130, 2080, 2035, >> 421 1980, 1940, 1900, 1870, 1840, 1800, 1800, 1800, 1780, 1760, 1760, 1740, 1730, 1725, >> 422 1740, 1785, 1815, 1835, 1860, 1890, 1895, 1920, 1920, 1890, 1850, 1835, 1830, 1830, >> 423 1830, 1830, 1830, 1830 >> 424 }; >> 425 const G4double G4NucleonNuclearCrossSection::pb_p_in[46] = >> 426 { >> 427 900, 1060, 1200, 1420, 1515, 1620, 1750, 1800, 1915, 2030, 1960, 1940, 1910, 1860, >> 428 1840, 1780, 1770, 1760, 1740, 1720, 1725, 1740, 1740, 1730, 1720, 1700, 1710, 1720, >> 429 1730, 1740, 1815, 1835, 1860, 1890, 1895, 1920, 1920, 1890, 1850, 1835, 1830, 1830, >> 430 1830, 1830, 1830, 1830 >> 431 }; >> 432 >> 433 const G4double G4NucleonNuclearCrossSection::u_m_t[46] = >> 434 { >> 435 5800, 5940, 6160, 6345, 6360, 6350, 6170, 6020, 5760, 5350, 4990, 4800, 4710, 4690, >> 436 4760, 5040, 5190, 5200, 5080, 4600, 4120, 3920, 3720, 3420, 3240, 3150, 3160, 3180, >> 437 3210, 3240, 3280, 3350, 3390, 3435, 3480, 3560, 3585, 3580, 3540, 3500, 3470, 3410, >> 438 3335, 3335, 3335, 3335 >> 439 }; >> 440 const G4double G4NucleonNuclearCrossSection::u_m_in[46] = >> 441 { >> 442 2820, 2770, 2700, 2660, 2645, 2620, 2580, 2550, 2515, 2450, 2390, 2320, 2260, 2225, >> 443 2200, 2140, 2080, 2060, 2040, 2000, 1980, 1965, 1960, 1930, 1920, 1890, 1905, 1920, >> 444 1945, 1970, 1985, 2010, 2040, 2070, 2080, 2090, 2095, 2080, 2063, 2060, 2050, 2040, >> 445 2005, 2005, 2005, 2005 >> 446 }; >> 447 const G4double G4NucleonNuclearCrossSection::u_p_in[46] = >> 448 { >> 449 800, 900, 1100, 1300, 1410, 1510, 1680, 1800, 2000, 2200, 2080, 2060, 2035, 2100, >> 450 2030, 2030, 2000, 1960, 1960, 1960, 1940, 1925, 1920, 1905, 1890, 1860, 1880, 1910, >> 451 1930, 1945, 1985, 2010, 2040, 2070, 2080, 2090, 2095, 2080, 2063, 2060, 2050, 2040, >> 452 2005, 2005, 2005, 2005 >> 453 }; >> 454 >> 455 using namespace std; 39 456 40 ////////////////////////////////////////////// 457 /////////////////////////////////////////////////////////////////////////////// 41 458 42 G4NucleonNuclearCrossSection::G4NucleonNuclear 459 G4NucleonNuclearCrossSection::G4NucleonNuclearCrossSection() 43 : G4VCrossSectionDataSet(Default_Name()) << 460 : G4VCrossSectionDataSet(Default_Name()), >> 461 fTotalXsc(0.0), fElasticXsc(0.0) 44 { 462 { 45 fBarash = new G4ComponentBarNucleonNucleusXs << 463 theNeutron = G4Neutron::Neutron(); >> 464 theProton = G4Proton::Proton(); >> 465 >> 466 // He, Be, C >> 467 >> 468 thePimData.push_back(new G4PiData(he_m_t, he_m_in, e1, 44)); >> 469 thePipData.push_back(new G4PiData(he_m_t, he_p_in, e1, 44)); >> 470 >> 471 thePimData.push_back(new G4PiData(be_m_t, be_m_in, e1, 44)); >> 472 thePipData.push_back(new G4PiData(be_m_t, be_p_in, e1, 44)); >> 473 >> 474 thePimData.push_back(new G4PiData(c_m_t, c_m_in, e1, 44)); >> 475 thePipData.push_back(new G4PiData(c_m_t, c_p_in, e1, 44)); >> 476 >> 477 // N, O, Na >> 478 >> 479 thePimData.push_back(new G4PiData(n_m_t, n_m_in, e2, 44)); >> 480 thePipData.push_back(new G4PiData(n_m_t, n_p_in, e2, 44)); >> 481 >> 482 thePimData.push_back(new G4PiData(o_m_t, o_m_in, e2, 44)); >> 483 thePipData.push_back(new G4PiData(o_m_t, o_p_in, e2, 44)); >> 484 >> 485 thePimData.push_back(new G4PiData(na_m_t, na_m_in, e2, 44)); >> 486 thePipData.push_back(new G4PiData(na_m_t, na_p_in, e2, 44)); >> 487 >> 488 // Al, Si, Ca >> 489 >> 490 thePimData.push_back(new G4PiData(al_m_t, al_m_in, e3, 45)); >> 491 thePipData.push_back(new G4PiData(al_m_t, al_p_in, e3, 45)); >> 492 >> 493 thePimData.push_back(new G4PiData(si_m_t, si_m_in, e3, 45)); >> 494 thePipData.push_back(new G4PiData(si_m_t, si_p_in, e3, 45)); >> 495 >> 496 thePimData.push_back(new G4PiData(ca_m_t, ca_m_in, e3, 45)); >> 497 thePipData.push_back(new G4PiData(ca_m_t, ca_p_in, e3, 45)); >> 498 >> 499 // Fe, Cu, Mo >> 500 >> 501 thePimData.push_back(new G4PiData(fe_m_t, fe_m_in, e4, 47)); >> 502 thePipData.push_back(new G4PiData(fe_m_t, fe_p_in, e4, 47)); >> 503 >> 504 thePimData.push_back(new G4PiData(cu_m_t, cu_m_in, e4, 47)); >> 505 thePipData.push_back(new G4PiData(cu_m_t, cu_p_in, e4, 47)); >> 506 >> 507 thePimData.push_back(new G4PiData(mo_m_t, mo_m_in, e4, 47)); >> 508 thePipData.push_back(new G4PiData(mo_m_t, mo_p_in, e4, 47)); >> 509 >> 510 // Cd, Sn, W >> 511 >> 512 thePimData.push_back(new G4PiData(cd_m_t, cd_m_in, e5, 48)); >> 513 thePipData.push_back(new G4PiData(cd_m_t, cd_p_in, e5, 48)); >> 514 >> 515 thePimData.push_back(new G4PiData(sn_m_t, sn_m_in, e5, 48)); >> 516 thePipData.push_back(new G4PiData(sn_m_t, sn_p_in, e5, 48)); >> 517 >> 518 thePimData.push_back(new G4PiData(w_m_t, w_m_in, e5, 48)); >> 519 thePipData.push_back(new G4PiData(w_m_t, w_p_in, e5, 48)); >> 520 >> 521 // Pb, U >> 522 >> 523 thePimData.push_back(new G4PiData(pb_m_t, pb_m_in, e6, 46)); >> 524 thePipData.push_back(new G4PiData(pb_m_t, pb_p_in, e6, 46)); >> 525 >> 526 thePimData.push_back(new G4PiData(u_m_t, u_m_in, e6, 46)); >> 527 thePipData.push_back(new G4PiData(u_m_t, u_p_in, e6, 46)); >> 528 >> 529 theZ.push_back(2); // He >> 530 theZ.push_back(4); // Be >> 531 theZ.push_back(6); // C >> 532 theZ.push_back(7); // N >> 533 theZ.push_back(8); // O >> 534 theZ.push_back(11); // Na >> 535 theZ.push_back(13); // Al >> 536 theZ.push_back(14); // Si >> 537 theZ.push_back(20); // Ca >> 538 theZ.push_back(26); // Fe >> 539 theZ.push_back(29); // Cu >> 540 theZ.push_back(42); // Mo >> 541 theZ.push_back(48); // Cd >> 542 theZ.push_back(50); // Sn >> 543 theZ.push_back(74); // W >> 544 theZ.push_back(82); // Pb >> 545 theZ.push_back(92); // U >> 546 46 } 547 } 47 548 48 ////////////////////////////////////////////// << 549 /////////////////////////////////////////////////////////////////////////////// >> 550 // 49 551 50 G4bool G4NucleonNuclearCrossSection::IsElement << 552 G4NucleonNuclearCrossSection::~G4NucleonNuclearCrossSection() 51 const G4DynamicParticle*, G4int Z, cons << 52 { 553 { 53 return (Z > 1); << 554 std::for_each(thePimData.begin(), thePimData.end(), G4PiData::Delete()); >> 555 std::for_each(thePipData.begin(), thePipData.end(), G4PiData::Delete()); 54 } 556 } 55 557 56 ////////////////////////////////////////////// 558 //////////////////////////////////////////////////////////////////////////// >> 559 // 57 560 58 G4double G4NucleonNuclearCrossSection::GetElem << 561 G4bool 59 const G4DynamicParticle* dp, G4int Z, << 562 G4NucleonNuclearCrossSection::IsElementApplicable(const G4DynamicParticle* aParticle, >> 563 G4int Z, >> 564 const G4Material*) 60 { 565 { 61 ComputeCrossSections(dp->GetDefinition(), dp << 566 G4bool result = false; 62 return fInelasticXsc; << 567 if(aParticle->GetDefinition() == theNeutron ) result = true; >> 568 if(aParticle->GetDefinition() == theProton) result = true; >> 569 if(Z < 2) result = false; >> 570 if(aParticle->GetKineticEnergy() > 999.9*GeV) result = false; >> 571 return result; 63 } 572 } 64 573 65 ////////////////////////////////////////////// 574 //////////////////////////////////////////////////////////////////////////// >> 575 // >> 576 >> 577 G4double >> 578 G4NucleonNuclearCrossSection::GetElementCrossSection(const G4DynamicParticle* aParticle, >> 579 G4int Z, const G4Material*) >> 580 { >> 581 G4double kineticEnergy = aParticle->GetKineticEnergy(); >> 582 >> 583 G4double result = 0; >> 584 // G4cout<<"Z = "<<Z<<G4endl; >> 585 >> 586 size_t it = 0; >> 587 size_t itmax = theZ.size() - 1; >> 588 for(; it <= itmax; ++it) { if(Z <= theZ[it]) { break; } } >> 589 if( it > itmax ) { it = itmax; } >> 590 G4int Z1, Z2; >> 591 G4double x1, x2, xt1, xt2; >> 592 >> 593 std::vector<G4PiData *> * theData = &thePimData; >> 594 if(aParticle->GetDefinition() == theProton) { theData = &thePipData; } >> 595 >> 596 if( theZ[it] == Z ) >> 597 { >> 598 result = (*theData)[it]->ReactionXSection(kineticEnergy); >> 599 fTotalXsc = (*theData)[it]->TotalXSection(kineticEnergy); >> 600 } >> 601 else >> 602 { >> 603 if(0 == it) { it = 1; } >> 604 x1 = (*theData)[it-1]->ReactionXSection(kineticEnergy); >> 605 xt1 = (*theData)[it-1]->TotalXSection(kineticEnergy); >> 606 Z1 = theZ[it-1]; >> 607 x2 = (*theData)[it]->ReactionXSection(kineticEnergy); >> 608 xt2 = (*theData)[it]->TotalXSection(kineticEnergy); >> 609 Z2 = theZ[it]; >> 610 >> 611 result = Interpolate(Z1, Z2, Z, x1, x2); >> 612 fTotalXsc = Interpolate(Z1, Z2, Z, xt1, xt2); >> 613 } >> 614 >> 615 fElasticXsc = fTotalXsc - result; >> 616 if( fElasticXsc < 0.) { fElasticXsc = 0.; } 66 617 67 void G4NucleonNuclearCrossSection::ComputeCros << 618 return result; 68 const G4ParticleDefinition* pd, << 69 G4double kinEnergy, G4int Z) << 70 { << 71 fBarash->ComputeCrossSections(pd, kinEnergy, << 72 fTotalXsc = fBarash->GetTotalXsc(); << 73 fInelasticXsc = fBarash->GetInelasticXsc(); << 74 fElasticXsc = fBarash->GetElasticXsc(); << 75 } 619 } 76 620 77 ////////////////////////////////////////////// << 621 ///////////////////////////////////////////////////////////////////////////// >> 622 // >> 623 >> 624 G4double G4NucleonNuclearCrossSection:: >> 625 Interpolate(G4int Z1, G4int Z2, G4int Z, G4double x1, G4double x2) >> 626 { >> 627 // Nucleon numbers obtained from G4NistManager G4 8.0 >> 628 >> 629 static const G4double alpha = 2./3.; >> 630 >> 631 static const G4double A[92] = >> 632 { >> 633 1.0001, 4.0000, 6.9241, 9.0000, 10.801, 12.011, 14.004, 16.004, 19.000, 20.188, >> 634 23.000, 24.320, 27.000, 28.109, 31.000, 32.094, 35.484, 39.985, 39.135, 40.116, >> 635 45.000, 47.918, 50.998, 52.055, 55.000, 55.910, 59.000, 58.760, 63.617, 65.468, >> 636 69.798, 72.691, 75.000, 79.042, 79.986, 83.887, 85.557, 87.710, 89.000, 91.318, >> 637 93.000, 96.025, 98.000, 101.16, 103.00, 106.51, 107.96, 112.51, 114.91, 118.81, >> 638 121.86, 127.70, 127.00, 131.39, 133.00, 137.42, 139.00, 140.21, 141.00, 144.32, >> 639 145.00, 150.45, 152.04, 157.33, 159.00, 162.57, 165.00, 167.32, 169.00, 173.10, >> 640 175.03, 178.54, 181.00, 183.89, 186.25, 190.27, 192.25, 195.11, 197.00, 200.63, >> 641 204.41, 207.24, 209.00, 209.00, 210.00, 222.00, 223.00, 226.00, 227.00, 232.00, >> 642 231.00, 237.98 >> 643 }; >> 644 static G4ThreadLocal G4bool NeedInit = true; >> 645 >> 646 static G4ThreadLocal G4double A75[92]; >> 647 >> 648 if ( NeedInit ) >> 649 { >> 650 for (G4int i=0; i<92; ++i) >> 651 { >> 652 A75[i] = std::pow(A[i], alpha); // interpolate by square ~ A^(2/3) >> 653 } >> 654 NeedInit=false; >> 655 } >> 656 >> 657 // for tabulated data, cross section scales with A^(2/3) >> 658 G4double r1 = x1 / A75[Z1-1] * A75[Z-1]; >> 659 G4double r2 = x2 / A75[Z2-1] * A75[Z-1]; >> 660 G4double result = 0.5*(r1+r2); >> 661 >> 662 // More precise average >> 663 if(Z1 != Z2) { >> 664 G4double alp1 = (A[Z-1] - A[Z1-1]); >> 665 G4double alp2 = (A[Z2-1] - A[Z-1]); >> 666 result = (r1*alp2 + r2*alp1)/(alp1 + alp2); >> 667 } >> 668 // G4cout << "x1/2, z1/2 z" <<x1<<" "<<x2<<" "<<Z1<<" "<<Z2<<" "<<Z<<G4endl; >> 669 // G4cout << "res1/2 " << r1 <<" " << r2 <<" " << result<< G4endl; >> 670 return result; >> 671 } 78 672 79 void 673 void 80 G4NucleonNuclearCrossSection::CrossSectionDesc 674 G4NucleonNuclearCrossSection::CrossSectionDescription(std::ostream& outFile) const 81 { 675 { 82 outFile << "G4NucleonNuclearCrossSection is 676 outFile << "G4NucleonNuclearCrossSection is a variant of the Barashenkov\n" 83 << "cross section parameterization t 677 << "cross section parameterization to be used of protons and\n" 84 << "nucleons on targets heavier than 678 << "nucleons on targets heavier than hydrogen. It is intended for\n" 85 << "use as a cross section component 679 << "use as a cross section component and is currently used by\n" 86 << "G4BGGNucleonInelasticXS. It is 680 << "G4BGGNucleonInelasticXS. It is valid for incident energies up\n" 87 << "to 1 TeV.\n"; 681 << "to 1 TeV.\n"; 88 } 682 } 89 << 90 ////////////////////////////////////////////// << 91 683 92 684