Geant4-11
G4ChipsHyperonElasticXS.cc
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29// G4 Physics class: G4ChipsHyperonElasticXS for pA elastic cross sections
30// Created: M.V. Kossov, CERN/ITEP(Moscow), 5-Feb-2010
31// The last update: M.V. Kossov, CERN/ITEP (Moscow) 5-Feb-2010
32//
33// -------------------------------------------------------------------------------
34// Short description: Interaction cross-sections for the elastic process.
35// Class extracted from CHIPS and integrated in Geant4 by W.Pokorski
36// -------------------------------------------------------------------------------
37//
38
40#include "G4SystemOfUnits.hh"
41#include "G4DynamicParticle.hh"
43#include "G4Lambda.hh"
44#include "G4SigmaPlus.hh"
45#include "G4SigmaMinus.hh"
46#include "G4SigmaZero.hh"
47#include "G4XiMinus.hh"
48#include "G4XiZero.hh"
49#include "G4OmegaMinus.hh"
50#include "G4Nucleus.hh"
51#include "G4ParticleTable.hh"
52#include "G4NucleiProperties.hh"
53#include "G4IonTable.hh"
54#include "G4Exp.hh"
55#include "G4Log.hh"
56#include "G4Pow.hh"
57
58// factory
60//
62
63G4ChipsHyperonElasticXS::G4ChipsHyperonElasticXS():G4VCrossSectionDataSet(Default_Name()), nPoints(128), nLast(nPoints-1)
64{
65 lPMin=-8.; //Min tabulatedLogarithmMomentum(D)
66 lPMax= 8.; //Max tabulatedLogarithmMomentum(D)
67 dlnP=(lPMax-lPMin)/nLast;// LogStep inTable (D)
68 onlyCS=true;//Flag toCalculOnlyCS(not Si/Bi)(L)
69 lastSIG=0.; //Last calculated cross section (L)
70 lastLP=-10.;//LastLog(mom_of IncidentHadron)(L)
71 lastTM=0.; //Last t_maximum (L)
72 theSS=0.; //TheLastSqSlope of 1st difr.Max(L)
73 theS1=0.; //TheLastMantissa of 1st difrMax(L)
74 theB1=0.; //TheLastSlope of 1st difructMax(L)
75 theS2=0.; //TheLastMantissa of 2nd difrMax(L)
76 theB2=0.; //TheLastSlope of 2nd difructMax(L)
77 theS3=0.; //TheLastMantissa of 3d difr.Max(L)
78 theB3=0.; //TheLastSlope of 3d difruct.Max(L)
79 theS4=0.; //TheLastMantissa of 4th difrMax(L)
80 theB4=0.; //TheLastSlope of 4th difructMax(L)
81 lastTZ=0; // Last atomic number of the target
82 lastTN=0; // Last # of neutrons in the target
83 lastPIN=0.; // Last initialized max momentum
84 lastCST=0; // Elastic cross-section table
85 lastPAR=0; // ParametersForFunctionCalculation
86 lastSST=0; // E-dep ofSqardSlope of 1st difMax
87 lastS1T=0; // E-dep of mantissa of 1st dif.Max
88 lastB1T=0; // E-dep of the slope of 1st difMax
89 lastS2T=0; // E-dep of mantissa of 2nd difrMax
90 lastB2T=0; // E-dep of the slope of 2nd difMax
91 lastS3T=0; // E-dep of mantissa of 3d difr.Max
92 lastB3T=0; // E-dep of the slope of 3d difrMax
93 lastS4T=0; // E-dep of mantissa of 4th difrMax
94 lastB4T=0; // E-dep of the slope of 4th difMax
95 lastN=0; // The last N of calculated nucleus
96 lastZ=0; // The last Z of calculated nucleus
97 lastP=0.; // LastUsed inCrossSection Momentum
98 lastTH=0.; // Last threshold momentum
99 lastCS=0.; // Last value of the Cross Section
100 lastI=0; // The last position in the DAMDB
101}
102
104{
105 std::vector<G4double*>::iterator pos;
106 for (pos=CST.begin(); pos<CST.end(); pos++)
107 { delete [] *pos; }
108 CST.clear();
109 for (pos=PAR.begin(); pos<PAR.end(); pos++)
110 { delete [] *pos; }
111 PAR.clear();
112 for (pos=SST.begin(); pos<SST.end(); pos++)
113 { delete [] *pos; }
114 SST.clear();
115 for (pos=S1T.begin(); pos<S1T.end(); pos++)
116 { delete [] *pos; }
117 S1T.clear();
118 for (pos=B1T.begin(); pos<B1T.end(); pos++)
119 { delete [] *pos; }
120 B1T.clear();
121 for (pos=S2T.begin(); pos<S2T.end(); pos++)
122 { delete [] *pos; }
123 S2T.clear();
124 for (pos=B2T.begin(); pos<B2T.end(); pos++)
125 { delete [] *pos; }
126 B2T.clear();
127 for (pos=S3T.begin(); pos<S3T.end(); pos++)
128 { delete [] *pos; }
129 S3T.clear();
130 for (pos=B3T.begin(); pos<B3T.end(); pos++)
131 { delete [] *pos; }
132 B3T.clear();
133 for (pos=S4T.begin(); pos<S4T.end(); pos++)
134 { delete [] *pos; }
135 S4T.clear();
136 for (pos=B4T.begin(); pos<B4T.end(); pos++)
137 { delete [] *pos; }
138 B4T.clear();
139}
140
141void
143{
144 outFile << "G4ChipsHyperonElasticXS provides the elastic cross\n"
145 << "section for hyperon nucleus scattering as a function of incident\n"
146 << "momentum. The cross section is calculated using M. Kossov's\n"
147 << "CHIPS parameterization of cross section data.\n";
148}
149
151 const G4Element*,
152 const G4Material*)
153{
154 return true;
155}
156
157// The main member function giving the collision cross section (P is in IU, CS is in mb)
158// Make pMom in independent units ! (Now it is MeV)
160 const G4Isotope*,
161 const G4Element*,
162 const G4Material*)
163{
164 G4double pMom=Pt->GetTotalMomentum();
165 G4int tgN = A - tgZ;
166 G4int pdg = Pt->GetDefinition()->GetPDGEncoding();
167
168 return GetChipsCrossSection(pMom, tgZ, tgN, pdg);
169}
170
172{
173
174 G4bool fCS = false;
175 G4double pEn=pMom;
176
177 onlyCS=fCS;
178
179 G4bool in=false; // By default the isotope must be found in the AMDB
180 lastP = 0.; // New momentum history (nothing to compare with)
181 lastN = tgN; // The last N of the calculated nucleus
182 lastZ = tgZ; // The last Z of the calculated nucleus
183 lastI = colN.size(); // Size of the Associative Memory DB in the heap
184 if(lastI) for(G4int i=0; i<lastI; i++) // Loop over proj/tgZ/tgN lines of DB
185 { // The nucleus with projPDG is found in AMDB
186 if(colN[i]==tgN && colZ[i]==tgZ) // Isotope is foind in AMDB
187 {
188 lastI=i;
189 lastTH =colTH[i]; // Last THreshold (A-dependent)
190 if(pEn<=lastTH)
191 {
192 return 0.; // Energy is below the Threshold value
193 }
194 lastP =colP [i]; // Last Momentum (A-dependent)
195 lastCS =colCS[i]; // Last CrossSect (A-dependent)
196 // if(std::fabs(lastP/pMom-1.)<tolerance) //VI (do not use tolerance)
197 if(lastP == pMom) // Do not recalculate
198 {
199 CalculateCrossSection(fCS,-1,i,pPDG,lastZ,lastN,pMom); // Update param's only
200 return lastCS*millibarn; // Use theLastCS
201 }
202 in = true; // This is the case when the isotop is found in DB
203 // Momentum pMom is in IU ! @@ Units
204 lastCS=CalculateCrossSection(fCS,-1,i,pPDG,lastZ,lastN,pMom); // read & update
205 if(lastCS<=0. && pEn>lastTH) // Correct the threshold
206 {
207 lastTH=pEn;
208 }
209 break; // Go out of the LOOP with found lastI
210 }
211 } // End of attampt to find the nucleus in DB
212 if(!in) // This nucleus has not been calculated previously
213 {
215 lastCS=CalculateCrossSection(fCS,0,lastI,pPDG,lastZ,lastN,pMom);//calculate&create
216 if(lastCS<=0.)
217 {
218 lastTH = 0; //ThresholdEnergy(tgZ, tgN); // The Threshold Energy which is now the last
219 if(pEn>lastTH)
220 {
221 lastTH=pEn;
222 }
223 }
224 colN.push_back(tgN);
225 colZ.push_back(tgZ);
226 colP.push_back(pMom);
227 colTH.push_back(lastTH);
228 colCS.push_back(lastCS);
229 return lastCS*millibarn;
230 } // End of creation of the new set of parameters
231 else
232 {
233 colP[lastI]=pMom;
235 }
236 return lastCS*millibarn;
237}
238
239// Calculation of total elastic cross section (p in IU, CS in mb) @@ Units (?)
240// F=0 - create AMDB, F=-1 - read&update AMDB, F=1 - update AMDB (sinchro with higher AMDB)
242 G4int PDG, G4int tgZ, G4int tgN, G4double pIU)
243{
244 G4double pMom=pIU/GeV; // All calculations are in GeV
245 onlyCS=CS; // Flag to calculate only CS (not Si/Bi)
246 lastLP=G4Log(pMom); // Make a logarithm of the momentum for calculation
247 if(F) // This isotope was found in AMDB =>RETRIEVE/UPDATE
248 {
249 if(F<0) // the AMDB must be loded
250 {
251 lastPIN = PIN[I]; // Max log(P) initialised for this table set
252 lastPAR = PAR[I]; // Pointer to the parameter set
253
254 lastCST = CST[I]; // Pointer to the total sross-section table
255 lastSST = SST[I]; // Pointer to the first squared slope
256 lastS1T = S1T[I]; // Pointer to the first mantissa
257 lastB1T = B1T[I]; // Pointer to the first slope
258 lastS2T = S2T[I]; // Pointer to the second mantissa
259 lastB2T = B2T[I]; // Pointer to the second slope
260 lastS3T = S3T[I]; // Pointer to the third mantissa
261 lastB3T = B3T[I]; // Pointer to the rhird slope
262 lastS4T = S4T[I]; // Pointer to the 4-th mantissa
263 lastB4T = B4T[I]; // Pointer to the 4-th slope
264 }
266 {
267 lastPIN=GetPTables(lastLP,lastPIN,PDG,tgZ,tgN);// Can update upper logP-Limit in tabs
268 PIN[I]=lastPIN; // Remember the new P-Limit of the tables
269 }
270 }
271 else // This isotope wasn't initialized => CREATE
272 {
273 lastPAR = new G4double[nPoints]; // Allocate memory for parameters of CS function
274 lastPAR[nLast]=0; // Initialization for VALGRIND
275 lastCST = new G4double[nPoints]; // Allocate memory for Tabulated CS function
276 lastSST = new G4double[nPoints]; // Allocate memory for Tabulated first sqaredSlope
277 lastS1T = new G4double[nPoints]; // Allocate memory for Tabulated first mantissa
278 lastB1T = new G4double[nPoints]; // Allocate memory for Tabulated first slope
279 lastS2T = new G4double[nPoints]; // Allocate memory for Tabulated second mantissa
280 lastB2T = new G4double[nPoints]; // Allocate memory for Tabulated second slope
281 lastS3T = new G4double[nPoints]; // Allocate memory for Tabulated third mantissa
282 lastB3T = new G4double[nPoints]; // Allocate memory for Tabulated third slope
283 lastS4T = new G4double[nPoints]; // Allocate memory for Tabulated 4-th mantissa
284 lastB4T = new G4double[nPoints]; // Allocate memory for Tabulated 4-th slope
285 lastPIN = GetPTables(lastLP,lPMin,PDG,tgZ,tgN); // Returns the new P-limit for tables
286 PIN.push_back(lastPIN); // Fill parameters of CS function to AMDB
287 PAR.push_back(lastPAR); // Fill parameters of CS function to AMDB
288 CST.push_back(lastCST); // Fill Tabulated CS function to AMDB
289 SST.push_back(lastSST); // Fill Tabulated first sq.slope to AMDB
290 S1T.push_back(lastS1T); // Fill Tabulated first mantissa to AMDB
291 B1T.push_back(lastB1T); // Fill Tabulated first slope to AMDB
292 S2T.push_back(lastS2T); // Fill Tabulated second mantissa to AMDB
293 B2T.push_back(lastB2T); // Fill Tabulated second slope to AMDB
294 S3T.push_back(lastS3T); // Fill Tabulated third mantissa to AMDB
295 B3T.push_back(lastB3T); // Fill Tabulated third slope to AMDB
296 S4T.push_back(lastS4T); // Fill Tabulated 4-th mantissa to AMDB
297 B4T.push_back(lastB4T); // Fill Tabulated 4-th slope to AMDB
298 } // End of creation/update of the new set of parameters and tables
299 // =-----------= NOW Update (if necessary) and Calculate the Cross Section =-----------=
301 {
302 lastPIN = GetPTables(lastLP,lastPIN,PDG,tgZ,tgN);
303 }
304 if(!onlyCS) lastTM=GetQ2max(PDG, tgZ, tgN, pMom); // Calculate (-t)_max=Q2_max (GeV2)
305 if(lastLP>lPMin && lastLP<=lastPIN) // Linear fit is made using precalculated tables
306 {
307 if(lastLP==lastPIN)
308 {
309 G4double shift=(lastLP-lPMin)/dlnP+.000001; // Log distance from lPMin
310 G4int blast=static_cast<int>(shift); // this is a bin number of the lower edge (0)
311 if(blast<0 || blast>=nLast)G4cout<<"G4QHyperElCS::CCS:b="<<blast<<","<<nLast<<G4endl;
312 lastSIG = lastCST[blast];
313 if(!onlyCS) // Skip the differential cross-section parameters
314 {
315 theSS = lastSST[blast];
316 theS1 = lastS1T[blast];
317 theB1 = lastB1T[blast];
318 theS2 = lastS2T[blast];
319 theB2 = lastB2T[blast];
320 theS3 = lastS3T[blast];
321 theB3 = lastB3T[blast];
322 theS4 = lastS4T[blast];
323 theB4 = lastB4T[blast];
324 }
325 }
326 else
327 {
328 G4double shift=(lastLP-lPMin)/dlnP; // a shift from the beginning of the table
329 G4int blast=static_cast<int>(shift); // the lower bin number
330 if(blast<0) blast=0;
331 if(blast>=nLast) blast=nLast-1; // low edge of the last bin
332 shift-=blast; // step inside the unit bin
333 G4int lastL=blast+1; // the upper bin number
334 G4double SIGL=lastCST[blast]; // the basic value of the cross-section
335 lastSIG= SIGL+shift*(lastCST[lastL]-SIGL); // calculated total elastic cross-section
336 if(!onlyCS) // Skip the differential cross-section parameters
337 {
338 G4double SSTL=lastSST[blast]; // the low bin of the first squared slope
339 theSS=SSTL+shift*(lastSST[lastL]-SSTL); // the basic value of the first sq.slope
340 G4double S1TL=lastS1T[blast]; // the low bin of the first mantissa
341 theS1=S1TL+shift*(lastS1T[lastL]-S1TL); // the basic value of the first mantissa
342 G4double B1TL=lastB1T[blast]; // the low bin of the first slope
343 theB1=B1TL+shift*(lastB1T[lastL]-B1TL); // the basic value of the first slope
344 G4double S2TL=lastS2T[blast]; // the low bin of the second mantissa
345 theS2=S2TL+shift*(lastS2T[lastL]-S2TL); // the basic value of the second mantissa
346 G4double B2TL=lastB2T[blast]; // the low bin of the second slope
347 theB2=B2TL+shift*(lastB2T[lastL]-B2TL); // the basic value of the second slope
348 G4double S3TL=lastS3T[blast]; // the low bin of the third mantissa
349 theS3=S3TL+shift*(lastS3T[lastL]-S3TL); // the basic value of the third mantissa
350 G4double B3TL=lastB3T[blast]; // the low bin of the third slope
351 theB3=B3TL+shift*(lastB3T[lastL]-B3TL); // the basic value of the third slope
352 G4double S4TL=lastS4T[blast]; // the low bin of the 4-th mantissa
353 theS4=S4TL+shift*(lastS4T[lastL]-S4TL); // the basic value of the 4-th mantissa
354 G4double B4TL=lastB4T[blast]; // the low bin of the 4-th slope
355 theB4=B4TL+shift*(lastB4T[lastL]-B4TL); // the basic value of the 4-th slope
356 }
357 }
358 }
359 else lastSIG=GetTabValues(lastLP, PDG, tgZ, tgN); // Direct calculation beyond the table
360 if(lastSIG<0.) lastSIG = 0.; // @@ a Warning print can be added
361 return lastSIG;
362}
363
364// It has parameter sets for all tZ/tN/PDG, using them the tables can be created/updated
366 G4int tgZ, G4int tgN)
367{
368 // @@ At present all nA==pA ---------> Each neucleus can have not more than 51 parameters
369 static const G4double pwd=2727;
370 const G4int n_hypel=33; // #of parameters for pp-elastic (<nPoints=128)
371 // -0- -1- -2- -3- -4- -5- -6--7--8--9--10--11--12-13--14-
372 G4double hyp_el[n_hypel]={1.,.002,.12,.0557,3.5,6.72,99.,2.,3.,5.,74.,3.,3.4,.2,.17,
373 .001,8.,.055,3.64,5.e-5,4000.,1500.,.46,1.2e6,3.5e6,5.e-5,
374 1.e10,8.5e8,1.e10,1.1,3.4e6,6.8e6,0.};
375 // -15--16- -17- -18- -19- -20- -21- -22- -23- -24- -25-
376 // -26- -27- -28- -29- -30- -31- -32-
377 //AR-04Jun2014 if(PDG!=3222 && PDG>3000 && PDG<3335)
378 if(PDG>3000 && PDG<3335)
379 {
380 // -- Total pp elastic cross section cs & s1/b1 (main), s2/b2 (tail1), s3/b3 (tail2) --
381 //p2=p*p;p3=p2*p;sp=sqrt(p);p2s=p2*sp;lp=log(p);dl1=lp-(3.=par(3));p4=p2*p2; p=|3-mom|
382 //CS=2.865/p2s/(1+.0022/p2s)+(18.9+.6461*dl1*dl1+9./p)/(1.+.425*lp)/(1.+.4276/p4);
383 // par(0) par(7) par(1) par(2) par(4) par(5) par(6)
384 //dl2=lp-5., s1=(74.+3.*dl2*dl2)/(1+3.4/p4/p)+(.2/p2+17.*p)/(p4+.001*sp),
385 // par(8) par(9) par(10) par(11) par(12)par(13) par(14)
386 // b1=8.*p**.055/(1.+3.64/p3); s2=5.e-5+4000./(p4+1500.*p); b2=.46+1.2e6/(p4+3.5e6/sp);
387 // par(15) par(16) par(17) par(18) par(19) par(20) par(21) par(22) par(23)
388 // s3=5.e-5+1.e10/(p4*p4+8.5e8*p2+1.e10); b3=1.1+3.4e6/(p4+6.8e6); ss=0.
389 // par(24) par(25) par(26) par(27) par(28) par(29) par(30) par(31)
390 //
391 if(lastPAR[nLast]!=pwd) // A unique flag to avoid the repeatable definition
392 {
393 if ( tgZ == 1 && tgN == 0 )
394 {
395 for (G4int ip=0; ip<n_hypel; ip++) lastPAR[ip]=hyp_el[ip]; // Hyperon+P
396 }
397 else
398 {
399 G4double a=tgZ+tgN;
400 G4double sa=std::sqrt(a);
401 G4double ssa=std::sqrt(sa);
402 G4double asa=a*sa;
403 G4double a2=a*a;
404 G4double a3=a2*a;
405 G4double a4=a3*a;
406 G4double a5=a4*a;
407 G4double a6=a4*a2;
408 G4double a7=a6*a;
409 G4double a8=a7*a;
410 G4double a9=a8*a;
411 G4double a10=a5*a5;
412 G4double a12=a6*a6;
413 G4double a14=a7*a7;
414 G4double a16=a8*a8;
415 G4double a17=a16*a;
416 //G4double a20=a16*a4;
417 G4double a32=a16*a16;
418 // Reaction cross-section parameters (pel=peh_fit.f)
419 lastPAR[0]=4./(1.+22/asa); // p1
420 lastPAR[1]=2.36*asa/(1.+a*.055/ssa); // p2
421 lastPAR[2]=(1.+.00007*a3/ssa)/(1.+.0026*a2); // p3
422 lastPAR[3]=1.76*a/ssa+.00003*a3; // p4
423 lastPAR[4]=(.03+200./a3)/(1.+1.E5/a3/sa); // p5
424 lastPAR[5]=5.; // p6
425 lastPAR[6]=0.; // p7 not used
426 lastPAR[7]=0.; // p8 not used
427 lastPAR[8]=0.; // p9 not used
428 // @@ the differential cross-section is parameterized separately for A>6 & A<7
429 if(a<6.5)
430 {
431 G4double a28=a16*a12;
432 // The main pre-exponent (pel_sg)
433 lastPAR[ 9]=4000*a; // p1
434 lastPAR[10]=1.2e7*a8+380*a17; // p2
435 lastPAR[11]=.7/(1.+4.e-12*a16); // p3
436 lastPAR[12]=2.5/a8/(a4+1.e-16*a32); // p4
437 lastPAR[13]=.28*a; // p5
438 lastPAR[14]=1.2*a2+2.3; // p6
439 lastPAR[15]=3.8/a; // p7
440 // The main slope (pel_sl)
441 lastPAR[16]=.01/(1.+.0024*a5); // p1
442 lastPAR[17]=.2*a; // p2
443 lastPAR[18]=9.e-7/(1.+.035*a5); // p3
444 lastPAR[19]=(42.+2.7e-11*a16)/(1.+.14*a); // p4
445 // The main quadratic (pel_sh)
446 lastPAR[20]=2.25*a3; // p1
447 lastPAR[21]=18.; // p2
448 lastPAR[22]=2.4e-3*a8/(1.+2.6e-4*a7); // p3
449 lastPAR[23]=3.5e-36*a32*a8/(1.+5.e-15*a32/a); // p4
450 // The 1st max pre-exponent (pel_qq)
451 lastPAR[24]=1.e5/(a8+2.5e12/a16); // p1
452 lastPAR[25]=8.e7/(a12+1.e-27*a28*a28); // p2
453 lastPAR[26]=.0006*a3; // p3
454 // The 1st max slope (pel_qs)
455 lastPAR[27]=10.+4.e-8*a12*a; // p1
456 lastPAR[28]=.114; // p2
457 lastPAR[29]=.003; // p3
458 lastPAR[30]=2.e-23; // p4
459 // The effective pre-exponent (pel_ss)
460 lastPAR[31]=1./(1.+.0001*a8); // p1
461 lastPAR[32]=1.5e-4/(1.+5.e-6*a12); // p2
462 lastPAR[33]=.03; // p3
463 // The effective slope (pel_sb)
464 lastPAR[34]=a/2; // p1
465 lastPAR[35]=2.e-7*a4; // p2
466 lastPAR[36]=4.; // p3
467 lastPAR[37]=64./a3; // p4
468 // The gloria pre-exponent (pel_us)
469 lastPAR[38]=1.e8*G4Exp(.32*asa); // p1
470 lastPAR[39]=20.*G4Exp(.45*asa); // p2
471 lastPAR[40]=7.e3+2.4e6/a5; // p3
472 lastPAR[41]=2.5e5*G4Exp(.085*a3); // p4
473 lastPAR[42]=2.5*a; // p5
474 // The gloria slope (pel_ub)
475 lastPAR[43]=920.+.03*a8*a3; // p1
476 lastPAR[44]=93.+.0023*a12; // p2
477 }
478 else
479 {
480 G4double p1a10=2.2e-28*a10;
481 G4double r4a16=6.e14/a16;
482 G4double s4a16=r4a16*r4a16;
483 // a24
484 // a36
485 // The main pre-exponent (peh_sg)
486 lastPAR[ 9]=4.5*G4Pow::GetInstance()->powA(a,1.15); // p1
487 lastPAR[10]=.06*G4Pow::GetInstance()->powA(a,.6); // p2
488 lastPAR[11]=.6*a/(1.+2.e15/a16); // p3
489 lastPAR[12]=.17/(a+9.e5/a3+1.5e33/a32); // p4
490 lastPAR[13]=(.001+7.e-11*a5)/(1.+4.4e-11*a5); // p5
491 lastPAR[14]=(p1a10*p1a10+2.e-29)/(1.+2.e-22*a12); // p6
492 // The main slope (peh_sl)
493 lastPAR[15]=400./a12+2.e-22*a9; // p1
494 lastPAR[16]=1.e-32*a12/(1.+5.e22/a14); // p2
495 lastPAR[17]=1000./a2+9.5*sa*ssa; // p3
496 lastPAR[18]=4.e-6*a*asa+1.e11/a16; // p4
497 lastPAR[19]=(120./a+.002*a2)/(1.+2.e14/a16); // p5
498 lastPAR[20]=9.+100./a; // p6
499 // The main quadratic (peh_sh)
500 lastPAR[21]=.002*a3+3.e7/a6; // p1
501 lastPAR[22]=7.e-15*a4*asa; // p2
502 lastPAR[23]=9000./a4; // p3
503 // The 1st max pre-exponent (peh_qq)
504 lastPAR[24]=.0011*asa/(1.+3.e34/a32/a4); // p1
505 lastPAR[25]=1.e-5*a2+2.e14/a16; // p2
506 lastPAR[26]=1.2e-11*a2/(1.+1.5e19/a12); // p3
507 lastPAR[27]=.016*asa/(1.+5.e16/a16); // p4
508 // The 1st max slope (peh_qs)
509 lastPAR[28]=.002*a4/(1.+7.e7/G4Pow::GetInstance()->powA(a-6.83,14)); // p1
510 lastPAR[29]=2.e6/a6+7.2/G4Pow::GetInstance()->powA(a,.11); // p2
511 lastPAR[30]=11.*a3/(1.+7.e23/a16/a8); // p3
512 lastPAR[31]=100./asa; // p4
513 // The 2nd max pre-exponent (peh_ss)
514 lastPAR[32]=(.1+4.4e-5*a2)/(1.+5.e5/a4); // p1
515 lastPAR[33]=3.5e-4*a2/(1.+1.e8/a8); // p2
516 lastPAR[34]=1.3+3.e5/a4; // p3
517 lastPAR[35]=500./(a2+50.)+3; // p4
518 lastPAR[36]=1.e-9/a+s4a16*s4a16; // p5
519 // The 2nd max slope (peh_sb)
520 lastPAR[37]=.4*asa+3.e-9*a6; // p1
521 lastPAR[38]=.0005*a5; // p2
522 lastPAR[39]=.002*a5; // p3
523 lastPAR[40]=10.; // p4
524 // The effective pre-exponent (peh_us)
525 lastPAR[41]=.05+.005*a; // p1
526 lastPAR[42]=7.e-8/sa; // p2
527 lastPAR[43]=.8*sa; // p3
528 lastPAR[44]=.02*sa; // p4
529 lastPAR[45]=1.e8/a3; // p5
530 lastPAR[46]=3.e32/(a32+1.e32); // p6
531 // The effective slope (peh_ub)
532 lastPAR[47]=24.; // p1
533 lastPAR[48]=20./sa; // p2
534 lastPAR[49]=7.e3*a/(sa+1.); // p3
535 lastPAR[50]=900.*sa/(1.+500./a3); // p4
536 }
537 // Parameter for lowEnergyNeutrons
538 lastPAR[51]=1.e15+2.e27/a4/(1.+2.e-18*a16);
539 }
541 // and initialize the zero element of the table
542 G4double lp=lPMin; // ln(momentum)
543 G4bool memCS=onlyCS; // ??
544 onlyCS=false;
545 lastCST[0]=GetTabValues(lp, PDG, tgZ, tgN); // Calculate AMDB tables
546 onlyCS=memCS;
547 lastSST[0]=theSS;
548 lastS1T[0]=theS1;
549 lastB1T[0]=theB1;
550 lastS2T[0]=theS2;
551 lastB2T[0]=theB2;
552 lastS3T[0]=theS3;
553 lastB3T[0]=theB3;
554 lastS4T[0]=theS4;
555 lastB4T[0]=theB4;
556 }
557 if(LP>ILP)
558 {
559 G4int ini = static_cast<int>((ILP-lPMin+.000001)/dlnP)+1; // already inited till this
560 if(ini<0) ini=0;
561 if(ini<nPoints)
562 {
563 G4int fin = static_cast<int>((LP-lPMin)/dlnP)+1; // final bin of initialization
564 if(fin>=nPoints) fin=nLast; // Limit of the tabular initialization
565 if(fin>=ini)
566 {
567 G4double lp=0.;
568 for(G4int ip=ini; ip<=fin; ip++) // Calculate tabular CS,S1,B1,S2,B2,S3,B3
569 {
570 lp=lPMin+ip*dlnP; // ln(momentum)
571 G4bool memCS=onlyCS;
572 onlyCS=false;
573 lastCST[ip]=GetTabValues(lp, PDG, tgZ, tgN); // Calculate AMDB tables (ret CS)
574 onlyCS=memCS;
575 lastSST[ip]=theSS;
576 lastS1T[ip]=theS1;
577 lastB1T[ip]=theB1;
578 lastS2T[ip]=theS2;
579 lastB2T[ip]=theB2;
580 lastS3T[ip]=theS3;
581 lastB3T[ip]=theB3;
582 lastS4T[ip]=theS4;
583 lastB4T[ip]=theB4;
584 }
585 return lp;
586 }
587 else G4cout<<"*Warning*G4ChipsHyperonElasticXS::GetPTables: PDG="<<PDG
588 <<", Z="<<tgZ<<", N="<<tgN<<", i="<<ini<<" > fin="<<fin<<", LP="<<LP
589 <<" > ILP="<<ILP<<" nothing is done!"<<G4endl;
590 }
591 else G4cout<<"*Warning*G4ChipsHyperonElasticXS::GetPTables: PDG="<<PDG
592 <<", Z="<<tgZ<<", N="<<tgN<<", i="<<ini<<">= max="<<nPoints<<", LP="<<LP
593 <<" > ILP="<<ILP<<", lPMax="<<lPMax<<" nothing is done!"<<G4endl;
594 }
595 } else {
596 // G4cout<<"*Error*G4ChipsHyperonElasticXS::GetPTables: PDG="<<PDG<<", Z="<<tgZ
597 // <<", N="<<tgN<<", while it is defined only for Hyperons"<<G4endl;
598 // throw G4QException("G4ChipsHyperonElasticXS::GetPTables:onlyaBA implemented");
600 ed << "PDG = " << PDG << ", Z = " << tgZ << ", N = " << tgN
601 << ", while it is defined only for Hyperons" << G4endl;
602 G4Exception("G4ChipsHyperonElasticXS::GetPTables()", "HAD_CHPS_0000",
603 FatalException, ed);
604 }
605 return ILP;
606}
607
608// Returns Q2=-t in independent units (MeV^2) (all internal calculations are in GeV)
610{
612 static const G4double third=1./3.;
613 static const G4double fifth=1./5.;
614 static const G4double sevth=1./7.;
615 //AR-04Jun2014 if(PDG==3222 || PDG<3000 || PDG>3334)G4cout<<"*Warning*G4QHyElCS::GET:PDG="<<PDG<<G4endl;
616 if(PDG<3000 || PDG>3334)G4cout<<"*Warning*G4QHyElCS::GET:PDG="<<PDG<<G4endl;
617 if(onlyCS)G4cout<<"*Warning*G4ChipsHyperonElasticXS::GetExchanT: onlyCS=1"<<G4endl;
618 if(lastLP<-4.3) return lastTM*GeVSQ*G4UniformRand();// S-wave for p<14 MeV/c (kinE<.1MeV)
619 G4double q2=0.;
620 if(tgZ==1 && tgN==0) // ===> p+p=p+p
621 {
623 G4double R1=(1.-G4Exp(-E1));
625 G4double R2=(1.-G4Exp(-E2*E2*E2));
627 G4double R3=(1.-G4Exp(-E3));
628 G4double I1=R1*theS1/theB1;
629 G4double I2=R2*theS2;
630 G4double I3=R3*theS3;
631 G4double I12=I1+I2;
632 G4double rand=(I12+I3)*G4UniformRand();
633 if (rand<I1 )
634 {
635 G4double ran=R1*G4UniformRand();
636 if(ran>1.) ran=1.;
637 q2=-G4Log(1.-ran)/theB1;
638 }
639 else if(rand<I12)
640 {
641 G4double ran=R2*G4UniformRand();
642 if(ran>1.) ran=1.;
643 q2=-G4Log(1.-ran);
644 if(q2<0.) q2=0.;
646 }
647 else
648 {
649 G4double ran=R3*G4UniformRand();
650 if(ran>1.) ran=1.;
651 q2=-G4Log(1.-ran)/theB3;
652 }
653 }
654 else
655 {
656 G4double a=tgZ+tgN;
658 G4double R1=(1.-G4Exp(-E1));
659 G4double tss=theSS+theSS; // for future solution of quadratic equation (imediate check)
661 G4double E2=lastTM*tm2*theB2; // power 3 for lowA, 5 for HighA (1st)
662 if(a>6.5)E2*=tm2; // for heavy nuclei
663 G4double R2=(1.-G4Exp(-E2));
665 if(a>6.5)E3*=tm2*tm2*tm2; // power 1 for lowA, 7 (2nd) for HighA
666 G4double R3=(1.-G4Exp(-E3));
668 G4double R4=(1.-G4Exp(-E4));
669 G4double I1=R1*theS1;
670 G4double I2=R2*theS2;
671 G4double I3=R3*theS3;
672 G4double I4=R4*theS4;
673 G4double I12=I1+I2;
674 G4double I13=I12+I3;
675 G4double rand=(I13+I4)*G4UniformRand();
676 if(rand<I1)
677 {
678 G4double ran=R1*G4UniformRand();
679 if(ran>1.) ran=1.;
680 q2=-G4Log(1.-ran)/theB1;
681 if(std::fabs(tss)>1.e-7) q2=(std::sqrt(theB1*(theB1+(tss+tss)*q2))-theB1)/tss;
682 }
683 else if(rand<I12)
684 {
685 G4double ran=R2*G4UniformRand();
686 if(ran>1.) ran=1.;
687 q2=-G4Log(1.-ran)/theB2;
688 if(q2<0.) q2=0.;
689 if(a<6.5) q2=G4Pow::GetInstance()->powA(q2,third);
690 else q2=G4Pow::GetInstance()->powA(q2,fifth);
691 }
692 else if(rand<I13)
693 {
694 G4double ran=R3*G4UniformRand();
695 if(ran>1.) ran=1.;
696 q2=-G4Log(1.-ran)/theB3;
697 if(q2<0.) q2=0.;
698 if(a>6.5) q2=G4Pow::GetInstance()->powA(q2,sevth);
699 }
700 else
701 {
702 G4double ran=R4*G4UniformRand();
703 if(ran>1.) ran=1.;
704 q2=-G4Log(1.-ran)/theB4;
705 if(a<6.5) q2=lastTM-q2; // u reduced for lightA (starts from 0)
706 }
707 }
708 if(q2<0.) q2=0.;
709 if(!(q2>=-1.||q2<=1.))G4cout<<"*NAN*G4QHyElasticCrossSect::GetExchangeT:-t="<<q2<<G4endl;
710 if(q2>lastTM)
711 {
712 q2=lastTM;
713 }
714 return q2*GeVSQ;
715}
716
717// Returns B in independent units (MeV^-2) (all internal calculations are in GeV) see ExT
719{
721 if(onlyCS)G4cout<<"*Warning*G4ChipsHyperonElasticXS::GetSlope: onlCS=true"<<G4endl;
722 if(lastLP<-4.3) return 0.; // S-wave for p<14 MeV/c (kinE<.1MeV)
723 //AR-04Jun2014 if(PDG==3222 || PDG<3000 || PDG>3334)
724 if(PDG<3000 || PDG>3334)
725 {
726 // G4cout<<"*Error*G4ChipsHyperonElasticXS::GetSlope: PDG="<<PDG<<", Z="<<tgZ
727 // <<", N="<<tgN<<", while it is defined only for Hyperons"<<G4endl;
728 // throw G4QException("G4ChipsHyperonElasticXS::GetSlope: HypA are implemented");
730 ed << "PDG = " << PDG << ", Z = " << tgZ << ", N = " << tgN
731 << ", while it is defined only for Hyperons" << G4endl;
732 G4Exception("G4ChipsHyperonElasticXS::GetSlope()", "HAD_CHPS_0000",
733 FatalException, ed);
734 }
735 if(theB1<0.) theB1=0.;
736 if(!(theB1>=-1.||theB1<=1.)) G4cout<<"*NAN*G4QHyElasticCrossS::Getslope:"<<theB1<<G4endl;
737 return theB1/GeVSQ;
738}
739
740// Returns half max(Q2=-t) in independent units (MeV^2)
742{
744 return lastTM*HGeVSQ;
745}
746
747// lastLP is used, so calculating tables, one need to remember and then recover lastLP
749 G4int tgN)
750{
751 //AR-04Jun2014 if(PDG==3222 || PDG<3000 || PDG>3334) G4cout<<"*Warning*G4QHypElCS::GTV:P="<<PDG<<G4endl;
752 if(PDG<3000 || PDG>3334) G4cout<<"*Warning*G4QHypElCS::GTV:P="<<PDG<<G4endl;
753
754
755 //AR-24Apr2018 Switch to allow transuranic elements
756 const G4bool isHeavyElementAllowed = true;
757 if(tgZ<0 || ( !isHeavyElementAllowed && tgZ>92))
758 {
759 G4cout<<"*Warning*G4QHyperonElastCS::GetTabValue:(1-92) NoIsotopesFor Z="<<tgZ<<G4endl;
760 return 0.;
761 }
762 G4int iZ=tgZ-1; // Z index
763 if(iZ<0)
764 {
765 iZ=0; // conversion of the neutron target to the proton target
766 tgZ=1;
767 tgN=0;
768 }
769 G4double p=G4Exp(lp); // momentum
770 G4double sp=std::sqrt(p); // sqrt(p)
771 G4double p2=p*p;
772 G4double p3=p2*p;
773 G4double p4=p3*p;
774 if ( tgZ == 1 && tgN == 0 ) // Hyperon+P
775 {
776 G4double dl2=lp-lastPAR[9];
777 theSS=lastPAR[32];
778 theS1=(lastPAR[10]+lastPAR[11]*dl2*dl2)/(1.+lastPAR[12]/p4/p)+
779 (lastPAR[13]/p2+lastPAR[14]*p)/(p4+lastPAR[15]*sp);
780 theB1=lastPAR[16]*G4Pow::GetInstance()->powA(p,lastPAR[17])/(1.+lastPAR[18]/p3);
781 theS2=lastPAR[19]+lastPAR[20]/(p4+lastPAR[21]*p);
782 theB2=lastPAR[22]+lastPAR[23]/(p4+lastPAR[24]/sp);
783 theS3=lastPAR[25]+lastPAR[26]/(p4*p4+lastPAR[27]*p2+lastPAR[28]);
784 theB3=lastPAR[29]+lastPAR[30]/(p4+lastPAR[31]);
785 theS4=0.;
786 theB4=0.;
787 // Returns the total elastic pim-p cross-section (to avoid spoiling lastSIG)
788 G4double dp=lp-lastPAR[4];
789 return lastPAR[0]/(lastPAR[1]+p2*(lastPAR[2]+p2))+(lastPAR[3]*dp*dp+lastPAR[5]+
790 lastPAR[6]/p2)/(1.+lastPAR[7]/sp+lastPAR[8]/p4);
791 }
792 else
793 {
794 G4double p5=p4*p;
795 G4double p6=p5*p;
796 G4double p8=p6*p2;
797 G4double p10=p8*p2;
798 G4double p12=p10*p2;
799 G4double p16=p8*p8;
800 //G4double p24=p16*p8;
801 G4double dl=lp-5.;
802 G4double a=tgZ+tgN;
803 G4double pah=G4Pow::GetInstance()->powA(p,a/2);
804 G4double pa=pah*pah;
805 G4double pa2=pa*pa;
806 if(a<6.5)
807 {
808 theS1=lastPAR[9]/(1.+lastPAR[10]*p4*pa)+lastPAR[11]/(p4+lastPAR[12]*p4/pa2)+
809 (lastPAR[13]*dl*dl+lastPAR[14])/(1.+lastPAR[15]/p2);
810 theB1=(lastPAR[16]+lastPAR[17]*p2)/(p4+lastPAR[18]/pah)+lastPAR[19];
811 theSS=lastPAR[20]/(1.+lastPAR[21]/p2)+lastPAR[22]/(p6/pa+lastPAR[23]/p16);
812 theS2=lastPAR[24]/(pa/p2+lastPAR[25]/p4)+lastPAR[26];
813 theB2=lastPAR[27]*G4Pow::GetInstance()->powA(p,lastPAR[28])+lastPAR[29]/(p8+lastPAR[30]/p16);
814 theS3=lastPAR[31]/(pa*p+lastPAR[32]/pa)+lastPAR[33];
815 theB3=lastPAR[34]/(p3+lastPAR[35]/p6)+lastPAR[36]/(1.+lastPAR[37]/p2);
816 theS4=p2*(pah*lastPAR[38]*G4Exp(-pah*lastPAR[39])+
817 lastPAR[40]/(1.+lastPAR[41]*G4Pow::GetInstance()->powA(p,lastPAR[42])));
818 theB4=lastPAR[43]*pa/p2/(1.+pa*lastPAR[44]);
819 }
820 else
821 {
822 theS1=lastPAR[9]/(1.+lastPAR[10]/p4)+lastPAR[11]/(p4+lastPAR[12]/p2)+
823 lastPAR[13]/(p5+lastPAR[14]/p16);
824 theB1=(lastPAR[15]/p8+lastPAR[19])/(p+lastPAR[16]/G4Pow::GetInstance()->powA(p,lastPAR[20]))+
825 lastPAR[17]/(1.+lastPAR[18]/p4);
826 theSS=lastPAR[21]/(p4/G4Pow::GetInstance()->powA(p,lastPAR[23])+lastPAR[22]/p4);
827 theS2=lastPAR[24]/p4/(G4Pow::GetInstance()->powA(p,lastPAR[25])+lastPAR[26]/p12)+lastPAR[27];
829 theS3=lastPAR[32]/G4Pow::GetInstance()->powA(p,lastPAR[35])/(1.+lastPAR[36]/p12)+
830 lastPAR[33]/(1.+lastPAR[34]/p6);
831 theB3=lastPAR[37]/p8+lastPAR[38]/p2+lastPAR[39]/(1.+lastPAR[40]/p8);
832 theS4=(lastPAR[41]/p4+lastPAR[46]/p)/(1.+lastPAR[42]/p10)+
833 (lastPAR[43]+lastPAR[44]*dl*dl)/(1.+lastPAR[45]/p12);
834 theB4=lastPAR[47]/(1.+lastPAR[48]/p)+lastPAR[49]*p4/(1.+lastPAR[50]*p5);
835 }
836 // Returns the total elastic (n/p)A cross-section (to avoid spoiling lastSIG)
837 G4double dlp=lp-lastPAR[5]; // ax
838 // p1 p2 p3 p4 p5
839 return (lastPAR[0]*dlp*dlp+lastPAR[1])/(1.+lastPAR[2]/p)+lastPAR[3]/(p3+lastPAR[4]);
840 }
841 return 0.;
842} // End of GetTableValues
843
844// Returns max -t=Q2 (GeV^2) for the momentum pP(GeV) and the target nucleus (tgN,tgZ)
846 G4double pP)
847{
848 static const G4double mLamb= G4Lambda::Lambda()->GetPDGMass()*.001; // MeV to GeV
849 static const G4double mLa2= mLamb*mLamb;
850 G4double pP2=pP*pP; // squared momentum of the projectile
851 if(tgZ || tgN>-1) // --> Hyperon-A
852 {
853 G4double mt=G4ParticleTable::GetParticleTable()->GetIonTable()->GetIon(tgZ,tgZ+tgN,0)->GetPDGMass()*.001; // Target mass in GeV
854
855 G4double dmt=mt+mt;
856 G4double mds=dmt*std::sqrt(pP2+mLa2)+mLa2+mt*mt; // Mondelstam mds (@@ other hyperons?)
857 return dmt*dmt*pP2/mds;
858 }
859 else
860 {
861 // G4cout<<"*Error*G4ChipsHyperonElasticXS::GetQ2ma:PDG="<<PDG<<",Z="<<tgZ<<",N="
862 // <<tgN<<", while it is defined only for p projectiles & Z_target>0"<<G4endl;
863 // throw G4QException("G4ChipsHyperonElasticXS::GetQ2max: only HyperA implemented");
865 ed << "PDG = " << PDG << ", Z = " << tgZ << ", N = " << tgN
866 << ", while it is defined only for p projectiles & Z_target>0" << G4endl;
867 G4Exception("G4ChipsHyperonElasticXS::GetQ2max()", "HAD_CHPS_0000",
868 FatalException, ed);
869 return 0;
870 }
871}
G4_DECLARE_XS_FACTORY(G4ChipsHyperonElasticXS)
static const G4double pos
@ FatalException
void G4Exception(const char *originOfException, const char *exceptionCode, G4ExceptionSeverity severity, const char *description)
Definition: G4Exception.cc:35
std::ostringstream G4ExceptionDescription
Definition: G4Exception.hh:40
G4double G4Exp(G4double initial_x)
Exponential Function double precision.
Definition: G4Exp.hh:179
G4double G4Log(G4double x)
Definition: G4Log.hh:226
static constexpr double gigaelectronvolt
Definition: G4SIunits.hh:194
static constexpr double millibarn
Definition: G4SIunits.hh:86
static constexpr double GeV
Definition: G4SIunits.hh:203
double G4double
Definition: G4Types.hh:83
bool G4bool
Definition: G4Types.hh:86
int G4int
Definition: G4Types.hh:85
const G4double A[17]
#define G4endl
Definition: G4ios.hh:57
G4GLOB_DLL std::ostream G4cout
#define G4UniformRand()
Definition: Randomize.hh:52
std::vector< G4double > colCS
std::vector< G4double * > S2T
G4double CalculateCrossSection(G4bool CS, G4int F, G4int I, G4int pPDG, G4int Z, G4int N, G4double pP)
G4double GetQ2max(G4int pPDG, G4int tgZ, G4int tgN, G4double pP)
G4double GetPTables(G4double lpP, G4double lPm, G4int PDG, G4int tZ, G4int tN)
virtual G4double GetChipsCrossSection(G4double momentum, G4int Z, G4int N, G4int pdg)
std::vector< G4double * > S1T
virtual G4bool IsIsoApplicable(const G4DynamicParticle *Pt, G4int Z, G4int A, const G4Element *elm, const G4Material *mat)
G4double GetTabValues(G4double lp, G4int pPDG, G4int tgZ, G4int tgN)
std::vector< G4double * > B4T
std::vector< G4double * > S3T
std::vector< G4double > colTH
std::vector< G4double * > B3T
std::vector< G4double * > B2T
std::vector< G4double * > CST
G4double GetSlope(G4int tZ, G4int tN, G4int pPDG)
std::vector< G4double * > S4T
G4double GetExchangeT(G4int tZ, G4int tN, G4int pPDG)
std::vector< G4double > colP
std::vector< G4double * > SST
std::vector< G4double > PIN
std::vector< G4double * > PAR
virtual void CrossSectionDescription(std::ostream &) const
std::vector< G4double * > B1T
virtual G4double GetIsoCrossSection(const G4DynamicParticle *, G4int tgZ, G4int A, const G4Isotope *iso=0, const G4Element *elm=0, const G4Material *mat=0)
G4ParticleDefinition * GetDefinition() const
G4double GetTotalMomentum() const
G4ParticleDefinition * GetIon(G4int Z, G4int A, G4int lvl=0)
Definition: G4IonTable.cc:522
static G4Lambda * Lambda()
Definition: G4Lambda.cc:107
G4IonTable * GetIonTable() const
static G4ParticleTable * GetParticleTable()
static G4Pow * GetInstance()
Definition: G4Pow.cc:41
G4double powA(G4double A, G4double y) const
Definition: G4Pow.hh:230