]>
Commit | Line | Data |
---|---|---|
63ba5337 | 1 | // PartonDistributions.cc is a part of the PYTHIA event generator. |
2 | // Copyright (C) 2012 Torbjorn Sjostrand. | |
3 | // PYTHIA is licenced under the GNU GPL version 2, see COPYING for details. | |
4 | // Please respect the MCnet Guidelines, see GUIDELINES for details. | |
5 | ||
6 | // Function definitions (not found in the header) for the PDF, LHAPDF, | |
7 | // GRV94L, CTEQ5L, MSTWpdf, CTEQ6pdf, GRVpiL, PomFix, PomH1FitAB, | |
8 | // PomH1Jets and Lepton classes. | |
9 | ||
10 | #include "PartonDistributions.h" | |
11 | #include "LHAPDFInterface.h" | |
12 | ||
13 | namespace Pythia8 { | |
14 | ||
15 | //========================================================================== | |
16 | ||
17 | // Base class for parton distribution functions. | |
18 | ||
19 | //-------------------------------------------------------------------------- | |
20 | ||
21 | // Resolve valence content for assumed meson. Possibly modified later. | |
22 | ||
23 | void PDF::setValenceContent() { | |
24 | ||
25 | // Subdivide meson by flavour content. | |
26 | if (idBeamAbs < 100 || idBeamAbs > 1000) return; | |
27 | int idTmp1 = idBeamAbs/100; | |
28 | int idTmp2 = (idBeamAbs/10)%10; | |
29 | ||
30 | // Find which is quark and which antiquark. | |
31 | if (idTmp1%2 == 0) { | |
32 | idVal1 = idTmp1; | |
33 | idVal2 = -idTmp2; | |
34 | } else { | |
35 | idVal1 = idTmp2; | |
36 | idVal2 = -idTmp1; | |
37 | } | |
38 | if (idBeam < 0) { | |
39 | idVal1 = -idVal1; | |
40 | idVal2 = -idVal2; | |
41 | } | |
42 | ||
43 | // Special case for Pomeron, to start off. | |
44 | if (idBeamAbs == 990) { | |
45 | idVal1 = 1; | |
46 | idVal2 = -1; | |
47 | } | |
48 | } | |
49 | ||
50 | //-------------------------------------------------------------------------- | |
51 | ||
52 | // Standard parton densities. | |
53 | ||
54 | double PDF::xf(int id, double x, double Q2) { | |
55 | ||
56 | // Need to update if flavour, x or Q2 changed. | |
57 | // Use idSav = 9 to indicate that ALL flavours are up-to-date. | |
58 | // Assume that flavour and antiflavour always updated simultaneously. | |
59 | if ( (abs(idSav) != abs(id) && idSav != 9) || x != xSav || Q2 != Q2Sav) | |
60 | {idSav = id; xfUpdate(id, x, Q2); xSav = x; Q2Sav = Q2;} | |
61 | ||
62 | // Baryon and nondiagonal meson beams: only p, pbar, pi+, pi- for now. | |
63 | if (idBeamAbs == 2212 || idBeamAbs == 211) { | |
64 | int idNow = (idBeam > 0) ? id : -id; | |
65 | int idAbs = abs(id); | |
66 | if (idNow == 0 || idAbs == 21) return max(0., xg); | |
67 | if (idNow == 1) return max(0., xd); | |
68 | if (idNow == -1) return max(0., xdbar); | |
69 | if (idNow == 2) return max(0., xu); | |
70 | if (idNow == -2) return max(0., xubar); | |
71 | if (idNow == 3) return max(0., xs); | |
72 | if (idNow == -3) return max(0., xsbar); | |
73 | if (idAbs == 4) return max(0., xc); | |
74 | if (idAbs == 5) return max(0., xb); | |
75 | if (idAbs == 22) return max(0., xgamma); | |
76 | return 0.; | |
77 | ||
78 | // Diagonal meson beams: only pi0, Pomeron for now. | |
79 | } else if (idBeam == 111 || idBeam == 990) { | |
80 | int idAbs = abs(id); | |
81 | if (id == 0 || idAbs == 21) return max(0., xg); | |
82 | if (id == idVal1 || id == idVal2) return max(0., xu); | |
83 | if (idAbs <= 2) return max(0., xubar); | |
84 | if (idAbs == 3) return max(0., xs); | |
85 | if (idAbs == 4) return max(0., xc); | |
86 | if (idAbs == 5) return max(0., xb); | |
87 | if (idAbs == 22) return max(0., xgamma); | |
88 | return 0.; | |
89 | ||
90 | ||
91 | // Lepton beam. | |
92 | } else { | |
93 | if (id == idBeam ) return max(0., xlepton); | |
94 | if (abs(id) == 22) return max(0., xgamma); | |
95 | return 0.; | |
96 | } | |
97 | ||
98 | } | |
99 | ||
100 | //-------------------------------------------------------------------------- | |
101 | ||
102 | // Only valence part of parton densities. | |
103 | ||
104 | double PDF::xfVal(int id, double x, double Q2) { | |
105 | ||
106 | // Need to update if flavour, x or Q2 changed. | |
107 | // Use idSav = 9 to indicate that ALL flavours are up-to-date. | |
108 | // Assume that flavour and antiflavour always updated simultaneously. | |
109 | if ( (abs(idSav) != abs(id) && idSav != 9) || x != xSav || Q2 != Q2Sav) | |
110 | {idSav = id; xfUpdate(id, x, Q2); xSav = x; Q2Sav = Q2;} | |
111 | ||
112 | // Baryon and nondiagonal meson beams: only p, pbar, pi+, pi- for now. | |
113 | if (idBeamAbs == 2212) { | |
114 | int idNow = (idBeam > 0) ? id : -id; | |
115 | if (idNow == 1) return max(0., xdVal); | |
116 | if (idNow == 2) return max(0., xuVal); | |
117 | return 0.; | |
118 | } else if (idBeamAbs == 211) { | |
119 | int idNow = (idBeam > 0) ? id : -id; | |
120 | if (idNow == 2 || idNow == -1) return max(0., xuVal); | |
121 | return 0.; | |
122 | ||
123 | // Diagonal meson beams: only pi0, Pomeron for now. | |
124 | } else if (idBeam == 111 || idBeam == 990) { | |
125 | if (id == idVal1 || id == idVal2) return max(0., xuVal); | |
126 | return 0.; | |
127 | ||
128 | // Lepton beam. | |
129 | } else { | |
130 | if (id == idBeam) return max(0., xlepton); | |
131 | return 0.; | |
132 | } | |
133 | ||
134 | } | |
135 | ||
136 | //-------------------------------------------------------------------------- | |
137 | ||
138 | // Only sea part of parton densities. | |
139 | ||
140 | double PDF::xfSea(int id, double x, double Q2) { | |
141 | ||
142 | // Need to update if flavour, x or Q2 changed. | |
143 | // Use idSav = 9 to indicate that ALL flavours are up-to-date. | |
144 | // Assume that flavour and antiflavour always updated simultaneously. | |
145 | if ( (abs(idSav) != abs(id) && idSav != 9) || x != xSav || Q2 != Q2Sav) | |
146 | {idSav = id; xfUpdate(id, x, Q2); xSav = x; Q2Sav = Q2;} | |
147 | ||
148 | // Hadron beams. | |
149 | if (idBeamAbs > 100) { | |
150 | int idNow = (idBeam > 0) ? id : -id; | |
151 | int idAbs = abs(id); | |
152 | if (idNow == 0 || idAbs == 21) return max(0., xg); | |
153 | if (idBeamAbs == 2212) { | |
154 | if (idNow == 1) return max(0., xdSea); | |
155 | if (idNow == -1) return max(0., xdbar); | |
156 | if (idNow == 2) return max(0., xuSea); | |
157 | if (idNow == -2) return max(0., xubar); | |
158 | } else { | |
159 | if (idAbs <= 2) return max(0., xuSea); | |
160 | } | |
161 | if (idNow == 3) return max(0., xs); | |
162 | if (idNow == -3) return max(0., xsbar); | |
163 | if (idAbs == 4) return max(0., xc); | |
164 | if (idAbs == 5) return max(0., xb); | |
165 | if (idAbs == 22) return max(0., xgamma); | |
166 | return 0.; | |
167 | ||
168 | // Lepton beam. | |
169 | } else { | |
170 | if (abs(id) == 22) return max(0., xgamma); | |
171 | return 0.; | |
172 | } | |
173 | ||
174 | } | |
175 | ||
176 | //========================================================================== | |
177 | ||
178 | // Interface to the LHAPDF library. | |
179 | ||
180 | //-------------------------------------------------------------------------- | |
181 | ||
182 | // Definitions of static variables. | |
183 | ||
184 | string LHAPDF::latestSetName = " "; | |
185 | int LHAPDF::latestMember = -1; | |
186 | int LHAPDF::latestNSet = 0; | |
187 | ||
188 | //-------------------------------------------------------------------------- | |
189 | ||
190 | // Initialize a parton density function from LHAPDF. | |
191 | ||
192 | void LHAPDF::init(string setName, int member, Info* infoPtr) { | |
193 | ||
194 | // If already initialized then need not do anything. | |
195 | if (setName == latestSetName && member == latestMember | |
196 | && nSet == latestNSet) return; | |
197 | ||
198 | // Initialize set. If first character is '/' then assume that name | |
199 | // is given with path, else not. | |
200 | if (setName[0] == '/') LHAPDFInterface::initPDFsetM( nSet, setName); | |
201 | else LHAPDFInterface::initPDFsetByNameM( nSet, setName); | |
202 | ||
203 | // Check that not dummy library was linked and put nSet negative. | |
204 | isSet = (nSet >= 0); | |
205 | if (!isSet) { | |
206 | if (infoPtr != 0) infoPtr->errorMsg("Error from LHAPDF::init: " | |
207 | "you try to use LHAPDF but did not link it"); | |
208 | else cout << " Error from LHAPDF::init: you try to use LHAPDF " | |
209 | << "but did not link it" << endl; | |
210 | } | |
211 | ||
212 | // Initialize member. | |
213 | LHAPDFInterface::initPDFM(nSet, member); | |
214 | ||
215 | // Do not collect statistics on under/overflow to save time and space. | |
216 | LHAPDFInterface::setPDFparm( "NOSTAT" ); | |
217 | LHAPDFInterface::setPDFparm( "LOWKEY" ); | |
218 | ||
219 | // Save values to avoid unnecessary reinitializations. | |
220 | latestSetName = setName; | |
221 | latestMember = member; | |
222 | latestNSet = nSet; | |
223 | ||
224 | } | |
225 | ||
226 | //-------------------------------------------------------------------------- | |
227 | ||
228 | // Allow optional extrapolation beyond boundaries. | |
229 | ||
230 | void LHAPDF::setExtrapolate(bool extrapol) { | |
231 | ||
232 | LHAPDFInterface::setPDFparm( (extrapol) ? "EXTRAPOLATE" : "18" ); | |
233 | ||
234 | } | |
235 | ||
236 | //-------------------------------------------------------------------------- | |
237 | ||
238 | // Give the parton distribution function set from LHAPDF. | |
239 | ||
240 | void LHAPDF::xfUpdate(int , double x, double Q2) { | |
241 | ||
242 | // Let LHAPDF do the evaluation of parton densities. | |
243 | double Q = sqrt( max( 0., Q2)); | |
244 | ||
245 | // Use special call if photon included in proton (so far only MRST2004qed) | |
246 | if (latestSetName == "MRST2004qed.LHgrid" ) { | |
247 | LHAPDFInterface::evolvePDFPHOTONM( nSet, x, Q, xfArray, xPhoton); | |
248 | } | |
249 | // Else use default LHAPDF call | |
250 | else { | |
251 | LHAPDFInterface::evolvePDFM( nSet, x, Q, xfArray); | |
252 | xPhoton=0.0; | |
253 | } | |
254 | ||
255 | // Update values. | |
256 | xg = xfArray[6]; | |
257 | xu = xfArray[8]; | |
258 | xd = xfArray[7]; | |
259 | xs = xfArray[9]; | |
260 | xubar = xfArray[4]; | |
261 | xdbar = xfArray[5]; | |
262 | xsbar = xfArray[3]; | |
263 | xc = xfArray[10]; | |
264 | xb = xfArray[11]; | |
265 | xgamma = xPhoton; | |
266 | ||
267 | // Subdivision of valence and sea. | |
268 | xuVal = xu - xubar; | |
269 | xuSea = xubar; | |
270 | xdVal = xd - xdbar; | |
271 | xdSea = xdbar; | |
272 | ||
273 | // idSav = 9 to indicate that all flavours reset. | |
274 | idSav = 9; | |
275 | ||
276 | } | |
277 | ||
278 | //========================================================================== | |
279 | ||
280 | // Gives the GRV 94 L (leading order) parton distribution function set | |
281 | // in parametrized form. Authors: M. Glueck, E. Reya and A. Vogt. | |
282 | // Ref: M. Glueck, E. Reya and A. Vogt, Z.Phys. C67 (1995) 433. | |
283 | ||
284 | void GRV94L::xfUpdate(int , double x, double Q2) { | |
285 | ||
286 | // Common expressions. Constrain Q2 for which parametrization is valid. | |
287 | double mu2 = 0.23; | |
288 | double lam2 = 0.2322 * 0.2322; | |
289 | double s = (Q2 > mu2) ? log( log(Q2/lam2) / log(mu2/lam2) ) : 0.; | |
290 | double ds = sqrt(s); | |
291 | double s2 = s * s; | |
292 | double s3 = s2 * s; | |
293 | ||
294 | // uv : | |
295 | double nu = 2.284 + 0.802 * s + 0.055 * s2; | |
296 | double aku = 0.590 - 0.024 * s; | |
297 | double bku = 0.131 + 0.063 * s; | |
298 | double au = -0.449 - 0.138 * s - 0.076 * s2; | |
299 | double bu = 0.213 + 2.669 * s - 0.728 * s2; | |
300 | double cu = 8.854 - 9.135 * s + 1.979 * s2; | |
301 | double du = 2.997 + 0.753 * s - 0.076 * s2; | |
302 | double uv = grvv (x, nu, aku, bku, au, bu, cu, du); | |
303 | ||
304 | // dv : | |
305 | double nd = 0.371 + 0.083 * s + 0.039 * s2; | |
306 | double akd = 0.376; | |
307 | double bkd = 0.486 + 0.062 * s; | |
308 | double ad = -0.509 + 3.310 * s - 1.248 * s2; | |
309 | double bd = 12.41 - 10.52 * s + 2.267 * s2; | |
310 | double cd = 6.373 - 6.208 * s + 1.418 * s2; | |
311 | double dd = 3.691 + 0.799 * s - 0.071 * s2; | |
312 | double dv = grvv (x, nd, akd, bkd, ad, bd, cd, dd); | |
313 | ||
314 | // udb : | |
315 | double alx = 1.451; | |
316 | double bex = 0.271; | |
317 | double akx = 0.410 - 0.232 * s; | |
318 | double bkx = 0.534 - 0.457 * s; | |
319 | double agx = 0.890 - 0.140 * s; | |
320 | double bgx = -0.981; | |
321 | double cx = 0.320 + 0.683 * s; | |
322 | double dx = 4.752 + 1.164 * s + 0.286 * s2; | |
323 | double ex = 4.119 + 1.713 * s; | |
324 | double esx = 0.682 + 2.978 * s; | |
325 | double udb = grvw (x, s, alx, bex, akx, bkx, agx, bgx, cx, | |
326 | dx, ex, esx); | |
327 | ||
328 | // del : | |
329 | double ne = 0.082 + 0.014 * s + 0.008 * s2; | |
330 | double ake = 0.409 - 0.005 * s; | |
331 | double bke = 0.799 + 0.071 * s; | |
332 | double ae = -38.07 + 36.13 * s - 0.656 * s2; | |
333 | double be = 90.31 - 74.15 * s + 7.645 * s2; | |
334 | double ce = 0.; | |
335 | double de = 7.486 + 1.217 * s - 0.159 * s2; | |
336 | double del = grvv (x, ne, ake, bke, ae, be, ce, de); | |
337 | ||
338 | // sb : | |
339 | double sts = 0.; | |
340 | double als = 0.914; | |
341 | double bes = 0.577; | |
342 | double aks = 1.798 - 0.596 * s; | |
343 | double as = -5.548 + 3.669 * ds - 0.616 * s; | |
344 | double bs = 18.92 - 16.73 * ds + 5.168 * s; | |
345 | double dst = 6.379 - 0.350 * s + 0.142 * s2; | |
346 | double est = 3.981 + 1.638 * s; | |
347 | double ess = 6.402; | |
348 | double sb = grvs (x, s, sts, als, bes, aks, as, bs, dst, est, ess); | |
349 | ||
350 | // cb : | |
351 | double stc = 0.888; | |
352 | double alc = 1.01; | |
353 | double bec = 0.37; | |
354 | double akc = 0.; | |
355 | double ac = 0.; | |
356 | double bc = 4.24 - 0.804 * s; | |
357 | double dct = 3.46 - 1.076 * s; | |
358 | double ect = 4.61 + 1.49 * s; | |
359 | double esc = 2.555 + 1.961 * s; | |
360 | double chm = grvs (x, s, stc, alc, bec, akc, ac, bc, dct, ect, esc); | |
361 | ||
362 | // bb : | |
363 | double stb = 1.351; | |
364 | double alb = 1.00; | |
365 | double beb = 0.51; | |
366 | double akb = 0.; | |
367 | double ab = 0.; | |
368 | double bb = 1.848; | |
369 | double dbt = 2.929 + 1.396 * s; | |
370 | double ebt = 4.71 + 1.514 * s; | |
371 | double esb = 4.02 + 1.239 * s; | |
372 | double bot = grvs (x, s, stb, alb, beb, akb, ab, bb, dbt, ebt, esb); | |
373 | ||
374 | // gl : | |
375 | double alg = 0.524; | |
376 | double beg = 1.088; | |
377 | double akg = 1.742 - 0.930 * s; | |
378 | double bkg = - 0.399 * s2; | |
379 | double ag = 7.486 - 2.185 * s; | |
380 | double bg = 16.69 - 22.74 * s + 5.779 * s2; | |
381 | double cg = -25.59 + 29.71 * s - 7.296 * s2; | |
382 | double dg = 2.792 + 2.215 * s + 0.422 * s2 - 0.104 * s3; | |
383 | double eg = 0.807 + 2.005 * s; | |
384 | double esg = 3.841 + 0.316 * s; | |
385 | double gl = grvw (x, s, alg, beg, akg, bkg, ag, bg, cg, | |
386 | dg, eg, esg); | |
387 | ||
388 | // Update values | |
389 | xg = gl; | |
390 | xu = uv + 0.5*(udb - del); | |
391 | xd = dv + 0.5*(udb + del); | |
392 | xubar = 0.5*(udb - del); | |
393 | xdbar = 0.5*(udb + del); | |
394 | xs = sb; | |
395 | xsbar = sb; | |
396 | xc = chm; | |
397 | xb = bot; | |
398 | ||
399 | // Subdivision of valence and sea. | |
400 | xuVal = uv; | |
401 | xuSea = xubar; | |
402 | xdVal = dv; | |
403 | xdSea = xdbar; | |
404 | ||
405 | // idSav = 9 to indicate that all flavours reset. | |
406 | idSav = 9; | |
407 | ||
408 | } | |
409 | ||
410 | //-------------------------------------------------------------------------- | |
411 | ||
412 | double GRV94L::grvv (double x, double n, double ak, double bk, double a, | |
413 | double b, double c, double d) { | |
414 | ||
415 | double dx = sqrt(x); | |
416 | return n * pow(x, ak) * (1. + a * pow(x, bk) + x * (b + c * dx)) * | |
417 | pow(1. - x, d); | |
418 | ||
419 | } | |
420 | ||
421 | //-------------------------------------------------------------------------- | |
422 | ||
423 | double GRV94L::grvw (double x, double s, double al, double be, double ak, | |
424 | double bk, double a, double b, double c, double d, double e, double es) { | |
425 | ||
426 | double lx = log(1./x); | |
427 | return (pow(x, ak) * (a + x * (b + x * c)) * pow(lx, bk) + pow(s, al) | |
428 | * exp(-e + sqrt(es * pow(s, be) * lx))) * pow(1. - x, d); | |
429 | ||
430 | } | |
431 | ||
432 | //-------------------------------------------------------------------------- | |
433 | ||
434 | double GRV94L::grvs (double x, double s, double sth, double al, double be, | |
435 | double ak, double ag, double b, double d, double e, double es) { | |
436 | ||
437 | if(s <= sth) { | |
438 | return 0.; | |
439 | } else { | |
440 | double dx = sqrt(x); | |
441 | double lx = log(1./x); | |
442 | return pow(s - sth, al) / pow(lx, ak) * (1. + ag * dx + b * x) * | |
443 | pow(1. - x, d) * exp(-e + sqrt(es * pow(s, be) * lx)); | |
444 | } | |
445 | ||
446 | } | |
447 | ||
448 | //========================================================================== | |
449 | ||
450 | // Gives the CTEQ 5 L (leading order) parton distribution function set | |
451 | // in parametrized form. Parametrization by J. Pumplin. | |
452 | // Ref: CTEQ Collaboration, H.L. Lai et al., Eur.Phys.J. C12 (2000) 375. | |
453 | ||
454 | // The range of (x, Q) covered by this parametrization of the QCD | |
455 | // evolved parton distributions is 1E-6 < x < 1, 1.1 GeV < Q < 10 TeV. | |
456 | // In the current implementation, densities are frozen at borders. | |
457 | ||
458 | void CTEQ5L::xfUpdate(int , double x, double Q2) { | |
459 | ||
460 | // Constrain x and Q2 to range for which parametrization is valid. | |
461 | double Q = sqrt( max( 1., min( 1e8, Q2) ) ); | |
462 | x = max( 1e-6, min( 1.-1e-10, x) ); | |
463 | ||
464 | // Derived kinematical quantities. | |
465 | double y = - log(x); | |
466 | double u = log( x / 0.00001); | |
467 | double x1 = 1. - x; | |
468 | double x1L = log(1. - x); | |
469 | double sumUbarDbar = 0.; | |
470 | ||
471 | // Parameters of parametrizations. | |
472 | const double Qmin[8] = { 0., 0., 0., 0., 0., 0., 1.3, 4.5}; | |
473 | const double alpha[8] = { 0.2987216, 0.3407552, 0.4491863, 0.2457668, | |
474 | 0.5293999, 0.3713141, 0.03712017, 0.004952010 }; | |
475 | const double ut1[8] = { 4.971265, 2.612618, -0.4656819, 3.862583, | |
476 | 0.1895615, 3.753257, 4.400772, 5.562568 }; | |
477 | const double ut2[8] = { -1.105128, -1.258304e5, -274.2390, -1.265969, | |
478 | -3.069097, -1.113085, -1.356116, -1.801317 }; | |
479 | const double am[8][9][3] = { | |
480 | // d. | |
481 | { { 0.5292616E+01, -0.2751910E+01, -0.2488990E+01 }, | |
482 | { 0.9714424E+00, 0.1011827E-01, -0.1023660E-01 }, | |
483 | { -0.1651006E+02, 0.7959721E+01, 0.8810563E+01 }, | |
484 | { -0.1643394E+02, 0.5892854E+01, 0.9348874E+01 }, | |
485 | { 0.3067422E+02, 0.4235796E+01, -0.5112136E+00 }, | |
486 | { 0.2352526E+02, -0.5305168E+01, -0.1169174E+02 }, | |
487 | { -0.1095451E+02, 0.3006577E+01, 0.5638136E+01 }, | |
488 | { -0.1172251E+02, -0.2183624E+01, 0.4955794E+01 }, | |
489 | { 0.1662533E-01, 0.7622870E-02, -0.4895887E-03 } }, | |
490 | // u. | |
491 | { { 0.9905300E+00, -0.4502235E+00, 0.1624441E+00 }, | |
492 | { 0.8867534E+00, 0.1630829E-01, -0.4049085E-01 }, | |
493 | { 0.8547974E+00, 0.3336301E+00, 0.1371388E+00 }, | |
494 | { 0.2941113E+00, -0.1527905E+01, 0.2331879E+00 }, | |
495 | { 0.3384235E+02, 0.3715315E+01, 0.8276930E+00 }, | |
496 | { 0.6230115E+01, 0.3134639E+01, -0.1729099E+01 }, | |
497 | { -0.1186928E+01, -0.3282460E+00, 0.1052020E+00 }, | |
498 | { -0.8545702E+01, -0.6247947E+01, 0.3692561E+01 }, | |
499 | { 0.1724598E-01, 0.7120465E-02, 0.4003646E-04 } }, | |
500 | // g. | |
501 | { { 0.1193572E+03, -0.3886845E+01, -0.1133965E+01 }, | |
502 | { -0.9421449E+02, 0.3995885E+01, 0.1607363E+01 }, | |
503 | { 0.4206383E+01, 0.2485954E+00, 0.2497468E+00 }, | |
504 | { 0.1210557E+03, -0.3015765E+01, -0.1423651E+01 }, | |
505 | { -0.1013897E+03, -0.7113478E+00, 0.2621865E+00 }, | |
506 | { -0.1312404E+01, -0.9297691E+00, -0.1562531E+00 }, | |
507 | { 0.1627137E+01, 0.4954111E+00, -0.6387009E+00 }, | |
508 | { 0.1537698E+00, -0.2487878E+00, 0.8305947E+00 }, | |
509 | { 0.2496448E-01, 0.2457823E-02, 0.8234276E-03 } }, | |
510 | // ubar + dbar. | |
511 | { { 0.2647441E+02, 0.1059277E+02, -0.9176654E+00 }, | |
512 | { 0.1990636E+01, 0.8558918E-01, 0.4248667E-01 }, | |
513 | { -0.1476095E+02, -0.3276255E+02, 0.1558110E+01 }, | |
514 | { -0.2966889E+01, -0.3649037E+02, 0.1195914E+01 }, | |
515 | { -0.1000519E+03, -0.2464635E+01, 0.1964849E+00 }, | |
516 | { 0.3718331E+02, 0.4700389E+02, -0.2772142E+01 }, | |
517 | { -0.1872722E+02, -0.2291189E+02, 0.1089052E+01 }, | |
518 | { -0.1628146E+02, -0.1823993E+02, 0.2537369E+01 }, | |
519 | { -0.1156300E+01, -0.1280495E+00, 0.5153245E-01 } }, | |
520 | // dbar/ubar. | |
521 | { { -0.6556775E+00, 0.2490190E+00, 0.3966485E-01 }, | |
522 | { 0.1305102E+01, -0.1188925E+00, -0.4600870E-02 }, | |
523 | { -0.2371436E+01, 0.3566814E+00, -0.2834683E+00 }, | |
524 | { -0.6152826E+01, 0.8339877E+00, -0.7233230E+00 }, | |
525 | { -0.8346558E+01, 0.2892168E+01, 0.2137099E+00 }, | |
526 | { 0.1279530E+02, 0.1021114E+00, 0.5787439E+00 }, | |
527 | { 0.5858816E+00, -0.1940375E+01, -0.4029269E+00 }, | |
528 | { -0.2795725E+02, -0.5263392E+00, 0.1290229E+01 }, | |
529 | { 0.0000000E+00, 0.0000000E+00, 0.0000000E+00 } }, | |
530 | // sbar. | |
531 | { { 0.1580931E+01, -0.2273826E+01, -0.1822245E+01 }, | |
532 | { 0.2702644E+01, 0.6763243E+00, 0.7231586E-02 }, | |
533 | { -0.1857924E+02, 0.3907500E+01, 0.5850109E+01 }, | |
534 | { -0.3044793E+02, 0.2639332E+01, 0.5566644E+01 }, | |
535 | { -0.4258011E+01, -0.5429244E+01, 0.4418946E+00 }, | |
536 | { 0.3465259E+02, -0.5532604E+01, -0.4904153E+01 }, | |
537 | { -0.1658858E+02, 0.2923275E+01, 0.2266286E+01 }, | |
538 | { -0.1149263E+02, 0.2877475E+01, -0.7999105E+00 }, | |
539 | { 0.0000000E+00, 0.0000000E+00, 0.0000000E+00 } }, | |
540 | // cbar. | |
541 | { { -0.8293661E+00, -0.3982375E+01, -0.6494283E-01 }, | |
542 | { 0.2754618E+01, 0.8338636E+00, -0.6885160E-01 }, | |
543 | { -0.1657987E+02, 0.1439143E+02, -0.6887240E+00 }, | |
544 | { -0.2800703E+02, 0.1535966E+02, -0.7377693E+00 }, | |
545 | { -0.6460216E+01, -0.4783019E+01, 0.4913297E+00 }, | |
546 | { 0.3141830E+02, -0.3178031E+02, 0.7136013E+01 }, | |
547 | { -0.1802509E+02, 0.1862163E+02, -0.4632843E+01 }, | |
548 | { -0.1240412E+02, 0.2565386E+02, -0.1066570E+02 }, | |
549 | { 0.0000000E+00, 0.0000000E+00, 0.0000000E+00 } }, | |
550 | // bbar. | |
551 | { { -0.6031237E+01, 0.1992727E+01, -0.1076331E+01 }, | |
552 | { 0.2933912E+01, 0.5839674E+00, 0.7509435E-01 }, | |
553 | { -0.8284919E+01, 0.1488593E+01, -0.8251678E+00 }, | |
554 | { -0.1925986E+02, 0.2805753E+01, -0.3015446E+01 }, | |
555 | { -0.9480483E+01, -0.9767837E+00, -0.1165544E+01 }, | |
556 | { 0.2193195E+02, -0.1788518E+02, 0.9460908E+01 }, | |
557 | { -0.1327377E+02, 0.1201754E+02, -0.6277844E+01 }, | |
558 | { 0.0000000E+00, 0.0000000E+00, 0.0000000E+00 }, | |
559 | { 0.0000000E+00, 0.0000000E+00, 0.0000000E+00 } } }; | |
560 | ||
561 | // Loop over 8 different parametrizations. Check if inside allowed region. | |
562 | for (int i = 0; i < 8; ++i) { | |
563 | double answer = 0.; | |
564 | if (Q > max(Qmin[i], alpha[i])) { | |
565 | ||
566 | // Evaluate answer. | |
567 | double tmp = log(Q / alpha[i]); | |
568 | double sb = log(tmp); | |
569 | double sb1 = sb - 1.2; | |
570 | double sb2 = sb1*sb1; | |
571 | double af[9]; | |
572 | for (int j = 0; j < 9; ++j) | |
573 | af[j] = am[i][j][0] + sb1 * am[i][j][1] + sb2 * am[i][j][2]; | |
574 | double part1 = af[1] * pow( y, 1. + 0.01 * af[4]) * (1. + af[8] * u); | |
575 | double part2 = af[0] * x1 + af[3] * x; | |
576 | double part3 = x * x1 * (af[5] + af[6] * x1 + af[7] * x * x1); | |
577 | double part4 = (ut2[i] < -100.) ? ut1[i] * x1L + af[2] * x1L | |
578 | : ut1[i] * x1L + af[2] * log(x1 + exp(ut2[i])); | |
579 | answer = x * exp( part1 + part2 + part3 + part4); | |
580 | answer *= 1. - Qmin[i] / Q; | |
581 | } | |
582 | ||
583 | // Store results. | |
584 | if (i == 0) xd = x * answer; | |
585 | else if (i == 1) xu = x * answer; | |
586 | else if (i == 2) xg = x * answer; | |
587 | else if (i == 3) sumUbarDbar = x * answer; | |
588 | else if (i == 4) { xubar = sumUbarDbar / (1. + answer); | |
589 | xdbar = sumUbarDbar * answer / (1. + answer); } | |
590 | else if (i == 5) {xs = x * answer; xsbar = xs;} | |
591 | else if (i == 6) xc = x * answer; | |
592 | else if (i == 7) xb = x * answer; | |
593 | } | |
594 | ||
595 | // Subdivision of valence and sea. | |
596 | xuVal = xu - xubar; | |
597 | xuSea = xubar; | |
598 | xdVal = xd - xdbar; | |
599 | xdSea = xdbar; | |
600 | ||
601 | // idSav = 9 to indicate that all flavours reset. | |
602 | idSav = 9; | |
603 | ||
604 | } | |
605 | ||
606 | //========================================================================== | |
607 | ||
608 | // The MSTWpdf class. | |
609 | // MSTW 2008 PDF's, specifically the LO one. | |
610 | // Original C++ version by Jeppe Andersen. | |
611 | // Modified by Graeme Watt <watt(at)hep.ucl.ac.uk>. | |
612 | ||
613 | //-------------------------------------------------------------------------- | |
614 | ||
615 | // Constants: could be changed here if desired, but normally should not. | |
616 | // These are of technical nature, as described for each. | |
617 | ||
618 | // Number of parton flavours, x and Q2 grid points, | |
619 | // bins below c and b thresholds. | |
620 | const int MSTWpdf::np = 12; | |
621 | const int MSTWpdf::nx = 64; | |
622 | const int MSTWpdf::nq = 48; | |
623 | const int MSTWpdf::nqc0 = 4; | |
624 | const int MSTWpdf::nqb0 = 14; | |
625 | ||
626 | // Range of (x, Q2) grid. | |
627 | const double MSTWpdf::xmin = 1e-6; | |
628 | const double MSTWpdf::xmax = 1.0; | |
629 | const double MSTWpdf::qsqmin = 1.0; | |
630 | const double MSTWpdf::qsqmax = 1e9; | |
631 | ||
632 | // Array of x values. | |
633 | const double MSTWpdf::xxInit[65] = {0., 1e-6, 2e-6, 4e-6, 6e-6, 8e-6, | |
634 | 1e-5, 2e-5, 4e-5, 6e-5, 8e-5, 1e-4, 2e-4, 4e-4, 6e-4, 8e-4, | |
635 | 1e-3, 2e-3, 4e-3, 6e-3, 8e-3, 1e-2, 1.4e-2, 2e-2, 3e-2, 4e-2, 6e-2, | |
636 | 8e-2, 0.10, 0.125, 0.15, 0.175, 0.20, 0.225, 0.25, 0.275, 0.30, | |
637 | 0.325, 0.35, 0.375, 0.40, 0.425, 0.45, 0.475, 0.50, 0.525, 0.55, | |
638 | 0.575, 0.60, 0.625, 0.65, 0.675, 0.70, 0.725, 0.75, 0.775, 0.80, | |
639 | 0.825, 0.85, 0.875, 0.90, 0.925, 0.95, 0.975, 1.0 }; | |
640 | ||
641 | // Array of Q values. | |
642 | const double MSTWpdf::qqInit[49] = {0., 1.0, 1.25, 1.5, 0., 0., 2.5, 3.2, | |
643 | 4.0, 5.0, 6.4, 8.0, 10., 12., 0., 0., 26.0, 40.0, 64.0, 1e2, 1.6e2, | |
644 | 2.4e2, 4e2, 6.4e2, 1e3, 1.8e3, 3.2e3, 5.6e3, 1e4, 1.8e4, 3.2e4, 5.6e4, | |
645 | 1e5, 1.8e5, 3.2e5, 5.6e5, 1e6, 1.8e6, 3.2e6, 5.6e6, 1e7, 1.8e7, 3.2e7, | |
646 | 5.6e7, 1e8, 1.8e8, 3.2e8, 5.6e8, 1e9 }; | |
647 | ||
648 | //-------------------------------------------------------------------------- | |
649 | ||
650 | // Initialize PDF: read in data grid from file and set up interpolation. | |
651 | ||
652 | void MSTWpdf::init(int iFitIn, string xmlPath, Info* infoPtr) { | |
653 | ||
654 | // Choice of fit among possibilities. Counters and temporary variables. | |
655 | iFit = iFitIn; | |
656 | int i,n,m,k,l,j; | |
657 | double dtemp; | |
658 | ||
659 | // Variables used for initialising c_ij array: | |
660 | double f[np+1][nx+1][nq+1]; | |
661 | double f1[np+1][nx+1][nq+1]; // derivative w.r.t. x | |
662 | double f2[np+1][nx+1][nq+1]; // derivative w.r.t. q | |
663 | double f12[np+1][nx+1][nq+1];// cross derivative | |
664 | double f21[np+1][nx+1][nq+1];// cross derivative | |
665 | int wt[16][16]={{1,0,0,0,0,0,0,0,0,0,0,0,0,0,0,0}, | |
666 | {0,0,0,0,0,0,0,0,1,0,0,0,0,0,0,0}, | |
667 | {-3,0,0,3,0,0,0,0,-2,0,0,-1,0,0,0,0}, | |
668 | {2,0,0,-2,0,0,0,0,1,0,0,1,0,0,0,0}, | |
669 | {0,0,0,0,1,0,0,0,0,0,0,0,0,0,0,0}, | |
670 | {0,0,0,0,0,0,0,0,0,0,0,0,1,0,0,0}, | |
671 | {0,0,0,0,-3,0,0,3,0,0,0,0,-2,0,0,-1}, | |
672 | {0,0,0,0,2,0,0,-2,0,0,0,0,1,0,0,1}, | |
673 | {-3,3,0,0,-2,-1,0,0,0,0,0,0,0,0,0,0}, | |
674 | {0,0,0,0,0,0,0,0,-3,3,0,0,-2,-1,0,0}, | |
675 | {9,-9,9,-9,6,3,-3,-6,6,-6,-3,3,4,2,1,2}, | |
676 | {-6,6,-6,6,-4,-2,2,4,-3,3,3,-3,-2,-1,-1,-2}, | |
677 | {2,-2,0,0,1,1,0,0,0,0,0,0,0,0,0,0}, | |
678 | {0,0,0,0,0,0,0,0,2,-2,0,0,1,1,0,0}, | |
679 | {-6,6,-6,6,-3,-3,3,3,-4,4,2,-2,-2,-2,-1,-1}, | |
680 | {4,-4,4,-4,2,2,-2,-2,2,-2,-2,2,1,1,1,1}}; | |
681 | double xxd,d1d2,cl[16],x[16],d1,d2,y[5],y1[5],y2[5],y12[5]; | |
682 | double mc2,mb2,eps=1e-6; // q^2 grid points at mc2+eps, mb2+eps | |
683 | ||
684 | // Select which data file to read for current fit. | |
685 | if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; | |
686 | string fileName = " "; | |
687 | if (iFit == 1) fileName = "mrstlostar.00.dat"; | |
688 | if (iFit == 2) fileName = "mrstlostarstar.00.dat"; | |
689 | if (iFit == 3) fileName = "mstw2008lo.00.dat"; | |
690 | if (iFit == 4) fileName = "mstw2008nlo.00.dat"; | |
691 | ||
692 | // Open data file. | |
693 | ifstream data_file( (xmlPath + fileName).c_str() ); | |
694 | if (!data_file.good()) { | |
695 | if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " | |
696 | "did not find parametrization file ", fileName); | |
697 | else cout << " Error from MSTWpdf::init: " | |
698 | << "did not find parametrization file " << fileName << endl; | |
699 | isSet = false; | |
700 | return; | |
701 | } | |
702 | ||
703 | // Read distance, tolerance, heavy quark masses | |
704 | // and alphaS values from file. | |
705 | char comma; | |
706 | int nExtraFlavours; | |
707 | data_file.ignore(256,'\n'); | |
708 | data_file.ignore(256,'\n'); | |
709 | data_file.ignore(256,'='); data_file >> distance >> tolerance; | |
710 | data_file.ignore(256,'='); data_file >> mCharm; | |
711 | data_file.ignore(256,'='); data_file >> mBottom; | |
712 | data_file.ignore(256,'='); data_file >> alphaSQ0; | |
713 | data_file.ignore(256,'='); data_file >> alphaSMZ; | |
714 | data_file.ignore(256,'='); data_file >> alphaSorder >> comma >> alphaSnfmax; | |
715 | data_file.ignore(256,'='); data_file >> nExtraFlavours; | |
716 | data_file.ignore(256,'\n'); | |
717 | data_file.ignore(256,'\n'); | |
718 | data_file.ignore(256,'\n'); | |
719 | ||
720 | // Use c and b quark masses for outlay of qq array. | |
721 | for (int iqq = 0; iqq < 49; ++iqq) qq[iqq] = qqInit[iqq]; | |
722 | mc2=mCharm*mCharm; | |
723 | mb2=mBottom*mBottom; | |
724 | qq[4]=mc2; | |
725 | qq[5]=mc2+eps; | |
726 | qq[14]=mb2; | |
727 | qq[15]=mb2+eps; | |
728 | ||
729 | // Check that the heavy quark masses are sensible. | |
730 | if (mc2 < qq[3] || mc2 > qq[6]) { | |
731 | if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " | |
732 | "invalid mCharm"); | |
733 | else cout << " Error from MSTWpdf::init: invalid mCharm" << endl; | |
734 | isSet = false; | |
735 | return; | |
736 | } | |
737 | if (mb2 < qq[13] || mb2 > qq[16]) { | |
738 | if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " | |
739 | "invalid mBottom"); | |
740 | else cout << " Error from MSTWpdf::init: invalid mBottom" << endl; | |
741 | isSet = false; | |
742 | return; | |
743 | } | |
744 | ||
745 | // The nExtraFlavours variable is provided to aid compatibility | |
746 | // with future grids where, for example, a photon distribution | |
747 | // might be provided (cf. the MRST2004QED PDFs). | |
748 | if (nExtraFlavours < 0 || nExtraFlavours > 1) { | |
749 | if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " | |
750 | "invalid nExtraFlavours"); | |
751 | else cout << " Error from MSTWpdf::init: invalid nExtraFlavours" << endl; | |
752 | isSet = false; | |
753 | return; | |
754 | } | |
755 | ||
756 | // Now read in the grids from the grid file. | |
757 | for (n=1;n<=nx-1;n++) | |
758 | for (m=1;m<=nq;m++) { | |
759 | for (i=1;i<=9;i++) | |
760 | data_file >> f[i][n][m]; | |
761 | if (alphaSorder==2) { // only at NNLO | |
762 | data_file >> f[10][n][m]; // = chm-cbar | |
763 | data_file >> f[11][n][m]; // = bot-bbar | |
764 | } | |
765 | else { | |
766 | f[10][n][m] = 0.; // = chm-cbar | |
767 | f[11][n][m] = 0.; // = bot-bbar | |
768 | } | |
769 | if (nExtraFlavours>0) | |
770 | data_file >> f[12][n][m]; // = photon | |
771 | else | |
772 | f[12][n][m] = 0.; // photon | |
773 | if (data_file.eof()) { | |
774 | if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " | |
775 | "failed to read in data file"); | |
776 | else cout << " Error from MSTWpdf::init: failed to read in data file" | |
777 | << endl; | |
778 | isSet = false; | |
779 | return; | |
780 | } | |
781 | } | |
782 | ||
783 | // Check that ALL the file contents have been read in. | |
784 | data_file >> dtemp; | |
785 | if (!data_file.eof()) { | |
786 | if (infoPtr != 0) infoPtr->errorMsg("Error from MSTWpdf::init: " | |
787 | "failed to read in data file"); | |
788 | else cout << " Error from MSTWpdf::init: failed to read in data file" | |
789 | << endl; | |
790 | isSet = false; | |
791 | return; | |
792 | } | |
793 | ||
794 | // Close the datafile. | |
795 | data_file.close(); | |
796 | ||
797 | // PDFs are identically zero at x = 1. | |
798 | for (i=1;i<=np;i++) | |
799 | for (m=1;m<=nq;m++) | |
800 | f[i][nx][m]=0.0; | |
801 | ||
802 | // Set up the new array in log10(x) and log10(qsq). | |
803 | for (i=1;i<=nx;i++) | |
804 | xx[i]=log10(xxInit[i]); | |
805 | for (m=1;m<=nq;m++) | |
806 | qq[m]=log10(qq[m]); | |
807 | ||
808 | // Now calculate the derivatives used for bicubic interpolation. | |
809 | for (i=1;i<=np;i++) { | |
810 | ||
811 | // Start by calculating the first x derivatives | |
812 | // along the first x value: | |
813 | for (m=1;m<=nq;m++) { | |
814 | f1[i][1][m]=polderivative1(xx[1],xx[2],xx[3],f[i][1][m],f[i][2][m], | |
815 | f[i][3][m]); | |
816 | // Then along the rest (up to the last): | |
817 | for (k=2;k<nx;k++) | |
818 | f1[i][k][m]=polderivative2(xx[k-1],xx[k],xx[k+1],f[i][k-1][m], | |
819 | f[i][k][m],f[i][k+1][m]); | |
820 | // Then for the last column: | |
821 | f1[i][nx][m]=polderivative3(xx[nx-2],xx[nx-1],xx[nx],f[i][nx-2][m], | |
822 | f[i][nx-1][m],f[i][nx][m]); | |
823 | } | |
824 | ||
825 | // Then calculate the qq derivatives. At NNLO there are | |
826 | // discontinuities in the PDFs at mc2 and mb2, so calculate | |
827 | // the derivatives at q^2 = mc2, mc2+eps, mb2, mb2+eps in | |
828 | // the same way as at the endpoints qsqmin and qsqmax. | |
829 | for (m=1;m<=nq;m++) { | |
830 | if (m==1 || m==nqc0+1 || m==nqb0+1) { | |
831 | for (k=1;k<=nx;k++) | |
832 | f2[i][k][m]=polderivative1(qq[m],qq[m+1],qq[m+2], | |
833 | f[i][k][m],f[i][k][m+1],f[i][k][m+2]); | |
834 | } | |
835 | else if (m==nq || m==nqc0 || m==nqb0) { | |
836 | for (k=1;k<=nx;k++) | |
837 | f2[i][k][m]=polderivative3(qq[m-2],qq[m-1],qq[m], | |
838 | f[i][k][m-2],f[i][k][m-1],f[i][k][m]); | |
839 | } | |
840 | else { | |
841 | // The rest: | |
842 | for (k=1;k<=nx;k++) | |
843 | f2[i][k][m]=polderivative2(qq[m-1],qq[m],qq[m+1], | |
844 | f[i][k][m-1],f[i][k][m],f[i][k][m+1]); | |
845 | } | |
846 | } | |
847 | ||
848 | // Now, calculate the cross derivatives. | |
849 | // Calculate these as the average between (d/dx)(d/dy) and (d/dy)(d/dx). | |
850 | ||
851 | // First calculate (d/dx)(d/dy). | |
852 | // Start by calculating the first x derivatives | |
853 | // along the first x value: | |
854 | for (m=1;m<=nq;m++) | |
855 | f12[i][1][m]=polderivative1(xx[1],xx[2],xx[3],f2[i][1][m], | |
856 | f2[i][2][m],f2[i][3][m]); | |
857 | // Then along the rest (up to the last): | |
858 | for (k=2;k<nx;k++) { | |
859 | for (m=1;m<=nq;m++) | |
860 | f12[i][k][m]=polderivative2(xx[k-1],xx[k],xx[k+1],f2[i][k-1][m], | |
861 | f2[i][k][m],f2[i][k+1][m]); | |
862 | } | |
863 | // Then for the last column: | |
864 | for (m=1;m<=nq;m++) | |
865 | f12[i][nx][m]=polderivative3(xx[nx-2],xx[nx-1],xx[nx], | |
866 | f2[i][nx-2][m],f2[i][nx-1][m],f2[i][nx][m]); | |
867 | ||
868 | // Now calculate (d/dy)(d/dx). | |
869 | for (m=1;m<=nq;m++) { | |
870 | if (m==1 || m==nqc0+1 || m==nqb0+1) { | |
871 | for (k=1;k<=nx;k++) | |
872 | f21[i][k][m]=polderivative1(qq[m],qq[m+1],qq[m+2], | |
873 | f1[i][k][m],f1[i][k][m+1],f1[i][k][m+2]); | |
874 | } | |
875 | else if (m==nq || m==nqc0 || m==nqb0) { | |
876 | for (k=1;k<=nx;k++) | |
877 | f21[i][k][m]=polderivative3(qq[m-2],qq[m-1],qq[m], | |
878 | f1[i][k][m-2],f1[i][k][m-1],f1[i][k][m]); | |
879 | } | |
880 | else { | |
881 | // The rest: | |
882 | for (k=1;k<=nx;k++) | |
883 | f21[i][k][m]=polderivative2(qq[m-1],qq[m],qq[m+1], | |
884 | f1[i][k][m-1],f1[i][k][m],f1[i][k][m+1]); | |
885 | } | |
886 | } | |
887 | ||
888 | // Now take the average of (d/dx)(d/dy) and (d/dy)(d/dx). | |
889 | for (k=1;k<=nx;k++) { | |
890 | for (m=1;m<=nq;m++) { | |
891 | f12[i][k][m] = 0.5*(f12[i][k][m]+f21[i][k][m]); | |
892 | } | |
893 | } | |
894 | ||
895 | // Now calculate the coefficients c_ij. | |
896 | for (n=1;n<=nx-1;n++) { | |
897 | for (m=1;m<=nq-1;m++) { | |
898 | d1=xx[n+1]-xx[n]; | |
899 | d2=qq[m+1]-qq[m]; | |
900 | d1d2=d1*d2; | |
901 | ||
902 | y[1]=f[i][n][m]; | |
903 | y[2]=f[i][n+1][m]; | |
904 | y[3]=f[i][n+1][m+1]; | |
905 | y[4]=f[i][n][m+1]; | |
906 | ||
907 | y1[1]=f1[i][n][m]; | |
908 | y1[2]=f1[i][n+1][m]; | |
909 | y1[3]=f1[i][n+1][m+1]; | |
910 | y1[4]=f1[i][n][m+1]; | |
911 | ||
912 | y2[1]=f2[i][n][m]; | |
913 | y2[2]=f2[i][n+1][m]; | |
914 | y2[3]=f2[i][n+1][m+1]; | |
915 | y2[4]=f2[i][n][m+1]; | |
916 | ||
917 | y12[1]=f12[i][n][m]; | |
918 | y12[2]=f12[i][n+1][m]; | |
919 | y12[3]=f12[i][n+1][m+1]; | |
920 | y12[4]=f12[i][n][m+1]; | |
921 | ||
922 | for (k=1;k<=4;k++) { | |
923 | x[k-1]=y[k]; | |
924 | x[k+3]=y1[k]*d1; | |
925 | x[k+7]=y2[k]*d2; | |
926 | x[k+11]=y12[k]*d1d2; | |
927 | } | |
928 | ||
929 | for (l=0;l<=15;l++) { | |
930 | xxd=0.0; | |
931 | for (k=0;k<=15;k++) xxd+= wt[l][k]*x[k]; | |
932 | cl[l]=xxd; | |
933 | } | |
934 | ||
935 | l=0; | |
936 | for (k=1;k<=4;k++) | |
937 | for (j=1;j<=4;j++) c[i][n][m][k][j]=cl[l++]; | |
938 | } //m | |
939 | } //n | |
940 | } // i | |
941 | ||
942 | } | |
943 | ||
944 | //-------------------------------------------------------------------------- | |
945 | ||
946 | // Update PDF values. | |
947 | ||
948 | void MSTWpdf::xfUpdate(int , double x, double Q2) { | |
949 | ||
950 | // Update using MSTW routine. | |
951 | double q = sqrtpos(Q2); | |
952 | // Quarks: | |
953 | double dn = parton(1,x,q); | |
954 | double up = parton(2,x,q); | |
955 | double str = parton(3,x,q); | |
956 | double chm = parton(4,x,q); | |
957 | double bot = parton(5,x,q); | |
958 | // Valence quarks: | |
959 | double dnv = parton(7,x,q); | |
960 | double upv = parton(8,x,q); | |
961 | double sv = parton(9,x,q); | |
962 | double cv = parton(10,x,q); | |
963 | double bv = parton(11,x,q); | |
964 | // Antiquarks = quarks - valence quarks: | |
965 | double dsea = dn - dnv; | |
966 | double usea = up - upv; | |
967 | double sbar = str - sv; | |
968 | double cbar = chm - cv; | |
969 | double bbar = bot - bv; | |
970 | // Gluon: | |
971 | double glu = parton(0,x,q); | |
972 | // Photon (= zero unless considering QED contributions): | |
973 | double phot = parton(13,x,q); | |
974 | ||
975 | // Transfer to Pythia notation. | |
976 | xg = glu; | |
977 | xu = up; | |
978 | xd = dn; | |
979 | xubar = usea; | |
980 | xdbar = dsea; | |
981 | xs = str; | |
982 | xsbar = sbar; | |
983 | xc = 0.5 * (chm + cbar); | |
984 | xb = 0.5 * (bot + bbar); | |
985 | xgamma = phot; | |
986 | ||
987 | // Subdivision of valence and sea. | |
988 | xuVal = upv; | |
989 | xuSea = xubar; | |
990 | xdVal = dnv; | |
991 | xdSea = xdbar; | |
992 | ||
993 | // idSav = 9 to indicate that all flavours reset. | |
994 | idSav = 9; | |
995 | ||
996 | } | |
997 | ||
998 | //-------------------------------------------------------------------------- | |
999 | ||
1000 | // Returns the PDF value for parton of flavour 'f' at x,q. | |
1001 | ||
1002 | double MSTWpdf::parton(int f,double x,double q) { | |
1003 | ||
1004 | double qsq; | |
1005 | int ip; | |
1006 | int interpolate(1); | |
1007 | double parton_pdf=0,parton_pdf1=0,anom; | |
1008 | double xxx,qqq; | |
1009 | ||
1010 | qsq=q*q; | |
1011 | ||
1012 | // If mc2 < qsq < mc2+eps, then qsq = mc2+eps. | |
1013 | if (qsq>pow(10.,qq[nqc0]) && qsq<pow(10.,qq[nqc0+1])) { | |
1014 | qsq = pow(10.,qq[nqc0+1]); | |
1015 | } | |
1016 | ||
1017 | // If mb2 < qsq < mb2+eps, then qsq = mb2+eps. | |
1018 | if (qsq>pow(10.,qq[nqb0]) && qsq<pow(10.,qq[nqb0+1])) { | |
1019 | qsq = pow(10.,qq[nqb0+1]); | |
1020 | } | |
1021 | ||
1022 | if (x<xmin) { | |
1023 | interpolate=0; | |
1024 | if (x<=0.) return 0.; | |
1025 | } | |
1026 | else if (x>xmax) return 0.; | |
1027 | ||
1028 | if (qsq<qsqmin) { | |
1029 | interpolate=-1; | |
1030 | if (q<=0.) return 0.; | |
1031 | } | |
1032 | else if (qsq>qsqmax) { | |
1033 | interpolate=0; | |
1034 | } | |
1035 | ||
1036 | if (f==0) ip=1; | |
1037 | else if (f>=1 && f<=5) ip=f+1; | |
1038 | else if (f<=-1 && f>=-5) ip=-f+1; | |
1039 | else if (f>=7 && f<=11) ip=f; | |
1040 | else if (f==13) ip=12; | |
1041 | else if (abs(f)==6 || f==12) return 0.; | |
1042 | else return 0.; | |
1043 | ||
1044 | // Interpolation in log10(x), log10(qsq): | |
1045 | xxx=log10(x); | |
1046 | qqq=log10(qsq); | |
1047 | ||
1048 | if (interpolate==1) { // do usual interpolation | |
1049 | parton_pdf=parton_interpolate(ip,xxx,qqq); | |
1050 | if (f<=-1 && f>=-5) // antiquark = quark - valence | |
1051 | parton_pdf -= parton_interpolate(ip+5,xxx,qqq); | |
1052 | } | |
1053 | else if (interpolate==-1) { // extrapolate to low Q^2 | |
1054 | ||
1055 | if (x<xmin) { // extrapolate to low x | |
1056 | parton_pdf = parton_extrapolate(ip,xxx,log10(qsqmin)); | |
1057 | parton_pdf1 = parton_extrapolate(ip,xxx,log10(1.01*qsqmin)); | |
1058 | if (f<=-1 && f>=-5) { // antiquark = quark - valence | |
1059 | parton_pdf -= parton_extrapolate(ip+5,xxx,log10(qsqmin)); | |
1060 | parton_pdf1 -= parton_extrapolate(ip+5,xxx,log10(1.01*qsqmin)); | |
1061 | } | |
1062 | } | |
1063 | else { // do usual interpolation | |
1064 | parton_pdf = parton_interpolate(ip,xxx,log10(qsqmin)); | |
1065 | parton_pdf1 = parton_interpolate(ip,xxx,log10(1.01*qsqmin)); | |
1066 | if (f<=-1 && f>=-5) { // antiquark = quark - valence | |
1067 | parton_pdf -= parton_interpolate(ip+5,xxx,log10(qsqmin)); | |
1068 | parton_pdf1 -= parton_interpolate(ip+5,xxx,log10(1.01*qsqmin)); | |
1069 | } | |
1070 | } | |
1071 | // Calculate the anomalous dimension, dlog(xf)/dlog(qsq), | |
1072 | // evaluated at qsqmin. Then extrapolate the PDFs to low | |
1073 | // qsq < qsqmin by interpolating the anomalous dimenion between | |
1074 | // the value at qsqmin and a value of 1 for qsq << qsqmin. | |
1075 | // If value of PDF at qsqmin is very small, just set | |
1076 | // anomalous dimension to 1 to prevent rounding errors. | |
1077 | if (fabs(parton_pdf) >= 1.e-5) | |
1078 | anom = max(-2.5, (parton_pdf1-parton_pdf)/parton_pdf/0.01); | |
1079 | else anom = 1.; | |
1080 | parton_pdf = parton_pdf*pow(qsq/qsqmin,anom*qsq/qsqmin+1.-qsq/qsqmin); | |
1081 | ||
1082 | } | |
1083 | else { // extrapolate outside PDF grid to low x or high Q^2 | |
1084 | parton_pdf = parton_extrapolate(ip,xxx,qqq); | |
1085 | if (f<=-1 && f>=-5) // antiquark = quark - valence | |
1086 | parton_pdf -= parton_extrapolate(ip+5,xxx,qqq); | |
1087 | } | |
1088 | ||
1089 | return parton_pdf; | |
1090 | } | |
1091 | ||
1092 | //-------------------------------------------------------------------------- | |
1093 | ||
1094 | // Interpolate PDF value inside data grid. | |
1095 | ||
1096 | double MSTWpdf::parton_interpolate(int ip, double xxx, double qqq) { | |
1097 | ||
1098 | double g, t, u; | |
1099 | int n, m, l; | |
1100 | ||
1101 | n=locate(xx,nx,xxx); // 0: below xmin, nx: above xmax | |
1102 | m=locate(qq,nq,qqq); // 0: below qsqmin, nq: above qsqmax | |
1103 | ||
1104 | t=(xxx-xx[n])/(xx[n+1]-xx[n]); | |
1105 | u=(qqq-qq[m])/(qq[m+1]-qq[m]); | |
1106 | ||
1107 | // Assume PDF proportional to (1-x)^p as x -> 1. | |
1108 | if (n==nx-1) { | |
1109 | double g0=((c[ip][n][m][1][4]*u+c[ip][n][m][1][3])*u | |
1110 | +c[ip][n][m][1][2])*u+c[ip][n][m][1][1]; // value at xx[n] | |
1111 | double g1=((c[ip][n-1][m][1][4]*u+c[ip][n-1][m][1][3])*u | |
1112 | +c[ip][n-1][m][1][2])*u+c[ip][n-1][m][1][1]; // value at xx[n-1] | |
1113 | double p = 1.0; | |
1114 | if (g0>0.0&&g1>0.0) p = log(g1/g0)/log((xx[n+1]-xx[n-1])/(xx[n+1]-xx[n])); | |
1115 | if (p<=1.0) p=1.0; | |
1116 | g=g0*pow((xx[n+1]-xxx)/(xx[n+1]-xx[n]),p); | |
1117 | } | |
1118 | ||
1119 | // Usual interpolation. | |
1120 | else { | |
1121 | g=0.0; | |
1122 | for (l=4;l>=1;l--) { | |
1123 | g=t*g+((c[ip][n][m][l][4]*u+c[ip][n][m][l][3])*u | |
1124 | +c[ip][n][m][l][2])*u+c[ip][n][m][l][1]; | |
1125 | } | |
1126 | } | |
1127 | ||
1128 | return g; | |
1129 | } | |
1130 | ||
1131 | //-------------------------------------------------------------------------- | |
1132 | ||
1133 | // Extrapolate PDF value outside data grid. | |
1134 | ||
1135 | ||
1136 | double MSTWpdf::parton_extrapolate(int ip, double xxx, double qqq) { | |
1137 | ||
1138 | double parton_pdf=0.; | |
1139 | int n,m; | |
1140 | ||
1141 | n=locate(xx,nx,xxx); // 0: below xmin, nx: above xmax | |
1142 | m=locate(qq,nq,qqq); // 0: below qsqmin, nq: above qsqmax | |
1143 | ||
1144 | if (n==0&&(m>0&&m<nq)) { // if extrapolation in small x only | |
1145 | ||
1146 | double f0,f1; | |
1147 | f0=parton_interpolate(ip,xx[1],qqq); | |
1148 | f1=parton_interpolate(ip,xx[2],qqq); | |
1149 | if ( f0>1e-3 && f1>1e-3 ) { // if values are positive, keep them so | |
1150 | f0=log(f0); | |
1151 | f1=log(f1); | |
1152 | parton_pdf=exp(f0+(f1-f0)/(xx[2]-xx[1])*(xxx-xx[1])); | |
1153 | } else // otherwise just extrapolate in the value | |
1154 | parton_pdf=f0+(f1-f0)/(xx[2]-xx[1])*(xxx-xx[1]); | |
1155 | ||
1156 | } if (n>0&&m==nq) { // if extrapolation into large q only | |
1157 | ||
1158 | double f0,f1; | |
1159 | f0=parton_interpolate(ip,xxx,qq[nq]); | |
1160 | f1=parton_interpolate(ip,xxx,qq[nq-1]); | |
1161 | if ( f0>1e-3 && f1>1e-3 ) { // if values are positive, keep them so | |
1162 | f0=log(f0); | |
1163 | f1=log(f1); | |
1164 | parton_pdf=exp(f0+(f0-f1)/(qq[nq]-qq[nq-1])*(qqq-qq[nq])); | |
1165 | } else // otherwise just extrapolate in the value | |
1166 | parton_pdf=f0+(f0-f1)/(qq[nq]-qq[nq-1])*(qqq-qq[nq]); | |
1167 | ||
1168 | } if (n==0&&m==nq) { // if extrapolation into large q AND small x | |
1169 | ||
1170 | double f0,f1; | |
1171 | f0=parton_extrapolate(ip,xx[1],qqq); | |
1172 | f1=parton_extrapolate(ip,xx[2],qqq); | |
1173 | if ( f0>1e-3 && f1>1e-3 ) { // if values are positive, keep them so | |
1174 | f0=log(f0); | |
1175 | f1=log(f1); | |
1176 | parton_pdf=exp(f0+(f1-f0)/(xx[2]-xx[1])*(xxx-xx[1])); | |
1177 | } else // otherwise just extrapolate in the value | |
1178 | parton_pdf=f0+(f1-f0)/(xx[2]-xx[1])*(xxx-xx[1]); | |
1179 | ||
1180 | } | |
1181 | ||
1182 | return parton_pdf; | |
1183 | } | |
1184 | ||
1185 | //-------------------------------------------------------------------------- | |
1186 | ||
1187 | // Returns an integer j such that x lies inbetween xloc[j] and xloc[j+1]. | |
1188 | // unit offset of increasing ordered array xloc assumed. | |
1189 | // n is the length of the array (xloc[n] highest element). | |
1190 | ||
1191 | int MSTWpdf::locate(double xloc[],int n,double x) { | |
1192 | int ju,jm,jl(0),j; | |
1193 | ju=n+1; | |
1194 | ||
1195 | while (ju-jl>1) { | |
1196 | jm=(ju+jl)/2; // compute a mid point. | |
1197 | if ( x>= xloc[jm]) | |
1198 | jl=jm; | |
1199 | else ju=jm; | |
1200 | } | |
1201 | if (x==xloc[1]) j=1; | |
1202 | else if (x==xloc[n]) j=n-1; | |
1203 | else j=jl; | |
1204 | ||
1205 | return j; | |
1206 | } | |
1207 | ||
1208 | //-------------------------------------------------------------------------- | |
1209 | ||
1210 | // Returns the estimate of the derivative at x1 obtained by a polynomial | |
1211 | // interpolation using the three points (x_i,y_i). | |
1212 | ||
1213 | double MSTWpdf::polderivative1(double x1, double x2, double x3, double y1, | |
1214 | double y2, double y3) { | |
1215 | ||
1216 | return (x3*x3*(y1-y2)+2.0*x1*(x3*(-y1+y2)+x2*(y1-y3))+x2*x2*(-y1+y3) | |
1217 | +x1*x1*(-y2+y3))/((x1-x2)*(x1-x3)*(x2-x3)); | |
1218 | ||
1219 | } | |
1220 | ||
1221 | //-------------------------------------------------------------------------- | |
1222 | ||
1223 | // Returns the estimate of the derivative at x2 obtained by a polynomial | |
1224 | // interpolation using the three points (x_i,y_i). | |
1225 | ||
1226 | double MSTWpdf::polderivative2(double x1, double x2, double x3, double y1, | |
1227 | double y2, double y3) { | |
1228 | ||
1229 | return (x3*x3*(y1-y2)-2.0*x2*(x3*(y1-y2)+x1*(y2-y3))+x2*x2*(y1-y3) | |
1230 | +x1*x1*(y2-y3))/((x1-x2)*(x1-x3)*(x2-x3)); | |
1231 | ||
1232 | } | |
1233 | ||
1234 | //-------------------------------------------------------------------------- | |
1235 | ||
1236 | // Returns the estimate of the derivative at x3 obtained by a polynomial | |
1237 | // interpolation using the three points (x_i,y_i). | |
1238 | ||
1239 | double MSTWpdf::polderivative3(double x1, double x2, double x3, double y1, | |
1240 | double y2, double y3) { | |
1241 | ||
1242 | return (x3*x3*(-y1+y2)+2.0*x2*x3*(y1-y3)+x1*x1*(y2-y3)+x2*x2*(-y1+y3) | |
1243 | +2.0*x1*x3*(-y2+y3))/((x1-x2)*(x1-x3)*(x2-x3)); | |
1244 | ||
1245 | } | |
1246 | ||
1247 | //========================================================================== | |
1248 | ||
1249 | // The CTEQ6pdf class. | |
1250 | // Code for handling CTEQ6L, CTEQ6L1, CTEQ66.00, CT09MC1, CT09MC2, (CT09MCS?). | |
1251 | ||
1252 | // Constants: could be changed here if desired, but normally should not. | |
1253 | // These are of technical nature, as described for each. | |
1254 | ||
1255 | // Stay away from xMin, xMax, Qmin, Qmax limits. | |
1256 | const double CTEQ6pdf::EPSILON = 1e-6; | |
1257 | ||
1258 | // Assumed approximate power of small-x behaviour for interpolation. | |
1259 | const double CTEQ6pdf::XPOWER = 0.3; | |
1260 | ||
1261 | //-------------------------------------------------------------------------- | |
1262 | ||
1263 | // Initialize PDF: read in data grid from file. | |
1264 | ||
1265 | void CTEQ6pdf::init(int iFitIn, string xmlPath, Info* infoPtr) { | |
1266 | ||
1267 | // Choice of fit among possibilities. | |
1268 | iFit = iFitIn; | |
1269 | ||
1270 | // Select which data file to read for current fit. | |
1271 | if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; | |
1272 | string fileName = " "; | |
1273 | if (iFit == 1) fileName = "cteq6l.tbl"; | |
1274 | if (iFit == 2) fileName = "cteq6l1.tbl"; | |
1275 | if (iFit == 3) fileName = "ctq66.00.pds"; | |
1276 | if (iFit == 4) fileName = "ct09mc1.pds"; | |
1277 | if (iFit == 5) fileName = "ct09mc2.pds"; | |
1278 | if (iFit == 6) fileName = "ct09mcs.pds"; | |
1279 | bool isPdsGrid = (iFit > 2); | |
1280 | ||
1281 | // Open data file. | |
1282 | ifstream pdfgrid( (xmlPath + fileName).c_str() ); | |
1283 | if (!pdfgrid.good()) { | |
1284 | if (infoPtr != 0) infoPtr->errorMsg("Error from CTEQ6pdf::init: " | |
1285 | "did not find parametrization file ", fileName); | |
1286 | else cout << " Error from CTEQ6pdf::init: " | |
1287 | << "did not find parametrization file " << fileName << endl; | |
1288 | isSet = false; | |
1289 | return; | |
1290 | } | |
1291 | ||
1292 | // Read in common information. | |
1293 | int iDum; | |
1294 | double orderTmp, nQTmp, qTmp, rDum; | |
1295 | string line; | |
1296 | getline( pdfgrid, line); | |
1297 | getline( pdfgrid, line); | |
1298 | getline( pdfgrid, line); | |
1299 | istringstream is1(line); | |
1300 | is1 >> orderTmp >> nQTmp >> lambda >> mQ[1] >> mQ[2] >> mQ[3] | |
1301 | >> mQ[4] >> mQ[5] >> mQ[6]; | |
1302 | order = int(orderTmp + 0.5); | |
1303 | nQuark = int(nQTmp + 0.5); | |
1304 | getline( pdfgrid, line); | |
1305 | ||
1306 | // Read in information for the .pds grid format. | |
1307 | if (isPdsGrid) { | |
1308 | getline( pdfgrid, line); | |
1309 | istringstream is2(line); | |
1310 | is2 >> iDum >> iDum >> iDum >> nfMx >> mxVal >> iDum; | |
1311 | if (mxVal > 4) mxVal = 3; | |
1312 | getline( pdfgrid, line); | |
1313 | getline( pdfgrid, line); | |
1314 | istringstream is3(line); | |
1315 | is3 >> nX >> nT >> iDum >> nG >> iDum; | |
1316 | for (int i = 0; i < nG + 2; ++i) getline( pdfgrid, line); | |
1317 | getline( pdfgrid, line); | |
1318 | istringstream is4(line); | |
1319 | is4 >> qIni >> qMax; | |
1320 | for (int iT = 0; iT <= nT; ++iT) { | |
1321 | getline( pdfgrid, line); | |
1322 | istringstream is5(line); | |
1323 | is5 >> qTmp; | |
1324 | tv[iT] = log( log( qTmp/lambda)); | |
1325 | } | |
1326 | getline( pdfgrid, line); | |
1327 | getline( pdfgrid, line); | |
1328 | istringstream is6(line); | |
1329 | is6 >> xMin >> rDum; | |
1330 | int nPackX = 6; | |
1331 | xv[0] = 0.; | |
1332 | for (int iXrng = 0; iXrng < int( (nX + nPackX - 1) / nPackX); ++iXrng) { | |
1333 | getline( pdfgrid, line); | |
1334 | istringstream is7(line); | |
1335 | for (int iX = nPackX * iXrng + 1; iX <= nPackX * (iXrng + 1); ++iX) | |
1336 | if (iX <= nX) is7 >> xv[iX]; | |
1337 | } | |
1338 | } | |
1339 | ||
1340 | // Read in information for the .tbl grid format. | |
1341 | else { | |
1342 | mxVal = 2; | |
1343 | getline( pdfgrid, line); | |
1344 | istringstream is2(line); | |
1345 | is2 >> nX >> nT >> nfMx; | |
1346 | getline( pdfgrid, line); | |
1347 | getline( pdfgrid, line); | |
1348 | istringstream is3(line); | |
1349 | is3 >> qIni >> qMax; | |
1350 | int nPackT = 6; | |
1351 | for (int iTrng = 0; iTrng < int( (nT + nPackT) / nPackT); ++iTrng) { | |
1352 | getline( pdfgrid, line); | |
1353 | istringstream is4(line); | |
1354 | for (int iT = nPackT * iTrng; iT < nPackT * (iTrng + 1); ++iT) | |
1355 | if (iT <= nT) { | |
1356 | is4 >> qTmp; | |
1357 | tv[iT] = log( log( qTmp / lambda) ); | |
1358 | } | |
1359 | } | |
1360 | getline( pdfgrid, line); | |
1361 | getline( pdfgrid, line); | |
1362 | istringstream is5(line); | |
1363 | is5 >> xMin; | |
1364 | int nPackX = 6; | |
1365 | for (int iXrng = 0; iXrng < int( (nX + nPackX) / nPackX); ++iXrng) { | |
1366 | getline( pdfgrid, line); | |
1367 | istringstream is6(line); | |
1368 | for (int iX = nPackX * iXrng; iX < nPackX * (iXrng + 1); ++iX) | |
1369 | if (iX <= nX) is6 >> xv[iX]; | |
1370 | } | |
1371 | } | |
1372 | ||
1373 | // Read in the grid proper. | |
1374 | getline( pdfgrid, line); | |
1375 | int nBlk = (nX + 1) * (nT + 1); | |
1376 | int nPts = nBlk * (nfMx + 1 + mxVal); | |
1377 | int nPack = (isPdsGrid) ? 6 : 5; | |
1378 | for (int iRng = 0; iRng < int( (nPts + nPack - 1) / nPack); ++iRng) { | |
1379 | getline( pdfgrid, line); | |
1380 | istringstream is8(line); | |
1381 | for (int i = nPack * iRng + 1; i <= nPack * (iRng + 1); ++i) | |
1382 | if (i <= nPts) is8 >> upd[i]; | |
1383 | } | |
1384 | ||
1385 | // Initialize x grid mapped to x^0.3. | |
1386 | xvpow[0] = 0.; | |
1387 | for (int iX = 1; iX <= nX; ++iX) xvpow[iX] = pow(xv[iX], XPOWER); | |
1388 | ||
1389 | // Set x and Q borders with some margin. | |
1390 | xMinEps = xMin * (1. + EPSILON); | |
1391 | xMaxEps = 1. - EPSILON; | |
1392 | qMinEps = qIni * (1. + EPSILON); | |
1393 | qMaxEps = qMax * (1. - EPSILON); | |
1394 | ||
1395 | // Initialize (x, Q) values of previous call. | |
1396 | xLast = 0.; | |
1397 | qLast = 0.; | |
1398 | ||
1399 | } | |
1400 | ||
1401 | //-------------------------------------------------------------------------- | |
1402 | ||
1403 | // Update PDF values. | |
1404 | ||
1405 | void CTEQ6pdf::xfUpdate(int , double x, double Q2) { | |
1406 | ||
1407 | // Update using CTEQ6 routine, within allowed (x, q) range. | |
1408 | double xEps = max( xMinEps, x); | |
1409 | double qEps = max( qMinEps, min( qMaxEps, sqrtpos(Q2) ) ); | |
1410 | ||
1411 | // Gluon: | |
1412 | double glu = xEps * parton6( 0, xEps, qEps); | |
1413 | // Sea quarks (note wrong order u, d): | |
1414 | double bot = xEps * parton6( 5, xEps, qEps); | |
1415 | double chm = xEps * parton6( 4, xEps, qEps); | |
1416 | double str = xEps * parton6( 3, xEps, qEps); | |
1417 | double usea = xEps * parton6(-1, xEps, qEps); | |
1418 | double dsea = xEps * parton6(-2, xEps, qEps); | |
1419 | // Valence quarks: | |
1420 | double upv = xEps * parton6( 1, xEps, qEps) - usea; | |
1421 | double dnv = xEps * parton6( 2, xEps, qEps) - dsea; | |
1422 | ||
1423 | // Transfer to Pythia notation. | |
1424 | xg = glu; | |
1425 | xu = upv + usea; | |
1426 | xd = dnv + dsea; | |
1427 | xubar = usea; | |
1428 | xdbar = dsea; | |
1429 | xs = str; | |
1430 | xsbar = str; | |
1431 | xc = chm; | |
1432 | xb = bot; | |
1433 | xgamma = 0.; | |
1434 | ||
1435 | // Subdivision of valence and sea. | |
1436 | xuVal = upv; | |
1437 | xuSea = usea; | |
1438 | xdVal = dnv; | |
1439 | xdSea = dsea; | |
1440 | ||
1441 | // idSav = 9 to indicate that all flavours reset. | |
1442 | idSav = 9; | |
1443 | ||
1444 | } | |
1445 | ||
1446 | //-------------------------------------------------------------------------- | |
1447 | ||
1448 | // Returns the PDF value for parton of flavour iParton at x, q. | |
1449 | ||
1450 | double CTEQ6pdf::parton6(int iParton, double x, double q) { | |
1451 | ||
1452 | // Put zero for large x. Parton table and interpolation variables. | |
1453 | if (x > xMaxEps) return 0.; | |
1454 | int iP = (iParton > mxVal) ? -iParton : iParton; | |
1455 | double ss = pow( x, XPOWER); | |
1456 | double tt = log( log(q / lambda) ); | |
1457 | ||
1458 | // Find location in grid.Skip if same as in latest call. | |
1459 | if (x != xLast || q != qLast) { | |
1460 | ||
1461 | // Binary search in x grid. | |
1462 | iGridX = 0; | |
1463 | iGridLX = -1; | |
1464 | int ju = nX + 1; | |
1465 | int jm = 0; | |
1466 | while (ju - iGridLX > 1 && jm >= 0) { | |
1467 | jm = (ju + iGridLX) / 2; | |
1468 | if (x >= xv[jm]) iGridLX = jm; | |
1469 | else ju = jm; | |
1470 | } | |
1471 | ||
1472 | // Separate acceptable from unacceptable grid points. | |
1473 | if (iGridLX <= -1) return 0.; | |
1474 | else if (iGridLX == 0) iGridX = 0; | |
1475 | else if (iGridLX <= nX - 2) iGridX = iGridLX - 1; | |
1476 | else if (iGridLX == nX - 1) iGridX = iGridLX - 2; | |
1477 | else return 0.; | |
1478 | ||
1479 | // Expressions for interpolation in x Grid. | |
1480 | if (iGridLX > 1 && iGridLX < nX - 1) { | |
1481 | double svec1 = xvpow[iGridX]; | |
1482 | double svec2 = xvpow[iGridX+1]; | |
1483 | double svec3 = xvpow[iGridX+2]; | |
1484 | double svec4 = xvpow[iGridX+3]; | |
1485 | double s12 = svec1 - svec2; | |
1486 | double s13 = svec1 - svec3; | |
1487 | xConst[8] = svec2 - svec3; | |
1488 | double s24 = svec2 - svec4; | |
1489 | double s34 = svec3 - svec4; | |
1490 | xConst[6] = ss - svec2; | |
1491 | xConst[7] = ss - svec3; | |
1492 | xConst[0] = s13 / xConst[8]; | |
1493 | xConst[1] = s12 / xConst[8]; | |
1494 | xConst[2] = s34 / xConst[8]; | |
1495 | xConst[3] = s24 / xConst[8]; | |
1496 | double s1213 = s12 + s13; | |
1497 | double s2434 = s24 + s34; | |
1498 | double sdet = s12 * s34 - s1213 * s2434; | |
1499 | double tmp = xConst[6] * xConst[7] / sdet; | |
1500 | xConst[4] = (s34 * xConst[6] - s2434 * xConst[7]) * tmp / s12; | |
1501 | xConst[5] = (s1213 * xConst[6] - s12 * xConst[7]) * tmp / s34; | |
1502 | } | |
1503 | ||
1504 | // Binary search in Q grid. | |
1505 | iGridQ = 0; | |
1506 | iGridLQ = -1; | |
1507 | ju = nT + 1; | |
1508 | jm = 0; | |
1509 | while (ju - iGridLQ > 1 && jm >= 0) { | |
1510 | jm = (ju + iGridLQ) / 2; | |
1511 | if (tt >= tv[jm]) iGridLQ = jm; | |
1512 | else ju = jm; | |
1513 | } | |
1514 | if (iGridLQ == 0) iGridQ = 0; | |
1515 | else if (iGridLQ <= nT - 2) iGridQ = iGridLQ - 1; | |
1516 | else iGridQ = nT - 3; | |
1517 | ||
1518 | // Expressions for interpolation in Q Grid. | |
1519 | if (iGridLQ > 0 && iGridLQ < nT - 1) { | |
1520 | double tvec1 = tv[iGridQ]; | |
1521 | double tvec2 = tv[iGridQ+1]; | |
1522 | double tvec3 = tv[iGridQ+2]; | |
1523 | double tvec4 = tv[iGridQ+3]; | |
1524 | double t12 = tvec1 - tvec2; | |
1525 | double t13 = tvec1 - tvec3; | |
1526 | tConst[8] = tvec2 - tvec3; | |
1527 | double t24 = tvec2 - tvec4; | |
1528 | double t34 = tvec3 - tvec4; | |
1529 | tConst[6] = tt - tvec2; | |
1530 | tConst[7] = tt - tvec3; | |
1531 | double tmp1 = t12 + t13; | |
1532 | double tmp2 = t24 + t34; | |
1533 | double tdet = t12 * t34 - tmp1 * tmp2; | |
1534 | tConst[0] = t13 / tConst[8]; | |
1535 | tConst[1] = t12 / tConst[8]; | |
1536 | tConst[2] = t34 / tConst[8]; | |
1537 | tConst[3] = t24 / tConst[8]; | |
1538 | tConst[4] = (t34 * tConst[6] - tmp2 * tConst[7]) / t12 | |
1539 | * tConst[6] * tConst[7] / tdet; | |
1540 | tConst[5] = (tmp1 * tConst[6] - t12 * tConst[7]) / t34 | |
1541 | * tConst[6] * tConst[7] / tdet; | |
1542 | } | |
1543 | ||
1544 | // Save x and q values so do not have to redo same again. | |
1545 | xLast = x; | |
1546 | qLast = q; | |
1547 | } | |
1548 | ||
1549 | // Jump to here if x and q are the same as for the last call. | |
1550 | int jtmp = ( (iP + nfMx) * (nT + 1) + (iGridQ - 1) ) * (nX + 1) + iGridX + 1; | |
1551 | ||
1552 | // Interpolate in x space for four different q values. | |
1553 | for(int it = 1; it <= 4; ++it) { | |
1554 | int j1 = jtmp + it * (nX + 1); | |
1555 | if (iGridX == 0) { | |
1556 | double fij[5]; | |
1557 | fij[1] = 0.; | |
1558 | fij[2] = upd[j1+1] * pow2(xv[1]); | |
1559 | fij[3] = upd[j1+2] * pow2(xv[2]); | |
1560 | fij[4] = upd[j1+3] * pow2(xv[3]); | |
1561 | double fX = polint4F( &xvpow[0], &fij[1], ss); | |
1562 | fVec[it] = (x > 0.) ? fX / pow2(x) : 0.; | |
1563 | } else if (iGridLX==nX-1) { | |
1564 | fVec[it] = polint4F( &xvpow[nX-3], &upd[j1], ss); | |
1565 | } else { | |
1566 | double sf2 = upd[j1+1]; | |
1567 | double sf3 = upd[j1+2]; | |
1568 | double g1 = sf2 * xConst[0] - sf3 * xConst[1]; | |
1569 | double g4 = -sf2 * xConst[2] + sf3 * xConst[3]; | |
1570 | fVec[it] = (xConst[4] * (upd[j1] - g1) + xConst[5] * (upd[j1+3] - g4) | |
1571 | + sf2 * xConst[7] - sf3 * xConst[6]) / xConst[8]; | |
1572 | } | |
1573 | } | |
1574 | ||
1575 | // Interpolate in q space for x-interpolated values found above. | |
1576 | double ff; | |
1577 | if( iGridLQ <= 0 ) { | |
1578 | ff = polint4F( &tv[0], &fVec[1], tt); | |
1579 | } else if (iGridLQ >= nT - 1) { | |
1580 | ff=polint4F( &tv[nT-3], &fVec[1], tt); | |
1581 | } else { | |
1582 | double tf2 = fVec[2]; | |
1583 | double tf3 = fVec[3]; | |
1584 | double g1 = tf2 * tConst[0] - tf3 * tConst[1]; | |
1585 | double g4 = -tf2 * tConst[2] + tf3 * tConst[3]; | |
1586 | ff = (tConst[4] * (fVec[1] - g1) + tConst[5] * (fVec[4] - g4) | |
1587 | + tf2 * tConst[7] - tf3 * tConst[6]) / tConst[8]; | |
1588 | } | |
1589 | ||
1590 | // Done. | |
1591 | return ff; | |
1592 | } | |
1593 | ||
1594 | //-------------------------------------------------------------------------- | |
1595 | ||
1596 | // The POLINT4 routine is based on the POLINT routine from "Numerical Recipes", | |
1597 | // but assuming N=4, and ignoring the error estimation. | |
1598 | // Suggested by Z. Sullivan. | |
1599 | ||
1600 | double CTEQ6pdf::polint4F(double xa[],double ya[],double x) { | |
1601 | ||
1602 | double y, h1, h2, h3, h4, w, den, d1, c1, d2, c2, d3, c3, cd1, cc1, | |
1603 | cd2, cc2, dd1, dc1; | |
1604 | ||
1605 | h1 = xa[0] - x; | |
1606 | h2 = xa[1] - x; | |
1607 | h3 = xa[2] - x; | |
1608 | h4 = xa[3] - x; | |
1609 | ||
1610 | w = ya[1] - ya[0]; | |
1611 | den = w / (h1 - h2); | |
1612 | d1 = h2 * den; | |
1613 | c1 = h1 * den; | |
1614 | ||
1615 | w = ya[2] - ya[1]; | |
1616 | den = w / (h2 - h3); | |
1617 | d2 = h3 * den; | |
1618 | c2 = h2 * den; | |
1619 | ||
1620 | w = ya[3] - ya[2]; | |
1621 | den = w / (h3 - h4); | |
1622 | d3 = h4 * den; | |
1623 | c3 = h3 * den; | |
1624 | ||
1625 | w = c2 - d1; | |
1626 | den = w / (h1 - h3); | |
1627 | cd1 = h3 * den; | |
1628 | cc1 = h1 * den; | |
1629 | ||
1630 | w = c3 - d2; | |
1631 | den = w / (h2 - h4); | |
1632 | cd2 = h4 * den; | |
1633 | cc2 = h2 * den; | |
1634 | ||
1635 | w = cc2 - cd1; | |
1636 | den = w / (h1 - h4); | |
1637 | dd1 = h4 * den; | |
1638 | dc1 = h1 * den; | |
1639 | ||
1640 | if (h3 + h4 < 0.) y = ya[3] + d3 + cd2 + dd1; | |
1641 | else if (h2 + h3 < 0.) y = ya[2] + d2 + cd1 + dc1; | |
1642 | else if (h1 + h2 < 0.) y = ya[1] + c2 + cd1 + dc1; | |
1643 | else y = ya[0] + c1 + cc1 + dc1; | |
1644 | ||
1645 | return y; | |
1646 | ||
1647 | } | |
1648 | ||
1649 | //========================================================================== | |
1650 | ||
1651 | // SA Unresolved proton: equivalent photon spectrum from | |
1652 | // V.M. Budnev, I.F. Ginzburg, G.V. Meledin and V.G. Serbo, | |
1653 | // Phys. Rept. 15 (1974/1975) 181. | |
1654 | ||
1655 | // Constants: | |
1656 | const double ProtonPoint::ALPHAEM = 0.00729735; | |
1657 | const double ProtonPoint::Q2MAX = 2.0; | |
1658 | const double ProtonPoint::Q20 = 0.71; | |
1659 | const double ProtonPoint::A = 7.16; | |
1660 | const double ProtonPoint::B = -3.96; | |
1661 | const double ProtonPoint::C = 0.028; | |
1662 | ||
1663 | //-------------------------------------------------------------------------- | |
1664 | ||
1665 | // Gives a generic Q2-independent equivalent photon spectrum. | |
1666 | ||
1667 | void ProtonPoint::xfUpdate(int , double x, double /*Q2*/ ) { | |
1668 | ||
1669 | // Photon spectrum | |
1670 | double tmpQ2Min = 0.88 * pow2(x); | |
1671 | double phiMax = phiFunc(x, Q2MAX / Q20); | |
1672 | double phiMin = phiFunc(x, tmpQ2Min / Q20); | |
1673 | ||
1674 | double fgm = 0; | |
1675 | if (phiMax < phiMin && m_infoPtr != 0) { | |
1676 | m_infoPtr->errorMsg("Error from ProtonPoint::xfUpdate: " | |
1677 | "phiMax - phiMin < 0!"); | |
1678 | } else { | |
1679 | // Corresponds to: x*f(x) | |
1680 | fgm = (ALPHAEM / M_PI) * (1 - x) * (phiMax - phiMin); | |
1681 | } | |
1682 | ||
1683 | // Update values | |
1684 | xg = 0.; | |
1685 | xu = 0.; | |
1686 | xd = 0.; | |
1687 | xubar = 0.; | |
1688 | xdbar = 0.; | |
1689 | xs = 0.; | |
1690 | xsbar = 0.; | |
1691 | xc = 0.; | |
1692 | xb = 0.; | |
1693 | xgamma = fgm; | |
1694 | ||
1695 | // Subdivision of valence and sea. | |
1696 | xuVal = 0.; | |
1697 | xuSea = 0; | |
1698 | xdVal = 0.; | |
1699 | xdSea = 0; | |
1700 | ||
1701 | // idSav = 9 to indicate that all flavours reset. | |
1702 | idSav = 9; | |
1703 | ||
1704 | } | |
1705 | ||
1706 | //-------------------------------------------------------------------------- | |
1707 | ||
1708 | // Function related to Q2 integration. | |
1709 | ||
1710 | double ProtonPoint::phiFunc(double x, double Q) { | |
1711 | ||
1712 | double tmpV = 1. + Q; | |
1713 | double tmpSum1 = 0; | |
1714 | double tmpSum2 = 0; | |
1715 | for (int k=1; k<4; ++k) { | |
1716 | tmpSum1 += 1. / (k * pow(tmpV, k)); | |
1717 | tmpSum2 += pow(B, k) / (k * pow(tmpV, k)); | |
1718 | } | |
1719 | ||
1720 | double tmpY = pow2(x) / (1 - x); | |
1721 | double funVal = (1 + A * tmpY) * (-1.*log(tmpV / Q) + tmpSum1) | |
1722 | + (1 - B) * tmpY / (4 * Q * pow(tmpV, 3)) | |
1723 | + C * (1 + tmpY/4.)* (log((tmpV - B)/tmpV) + tmpSum2); | |
1724 | ||
1725 | return funVal; | |
1726 | ||
1727 | } | |
1728 | ||
1729 | //========================================================================== | |
1730 | ||
1731 | // Gives the GRV 1992 pi+ (leading order) parton distribution function set | |
1732 | // in parametrized form. Authors: Glueck, Reya and Vogt. | |
1733 | // Ref: M. Glueck, E. Reya and A. Vogt, Z. Phys. C53 (1992) 651. | |
1734 | // Allowed variable range: 0.25 GeV^2 < Q^2 < 10^8 GeV^2 and 10^-5 < x < 1. | |
1735 | ||
1736 | void GRVpiL::xfUpdate(int , double x, double Q2) { | |
1737 | ||
1738 | // Common expressions. Constrain Q2 for which parametrization is valid. | |
1739 | double mu2 = 0.25; | |
1740 | double lam2 = 0.232 * 0.232; | |
1741 | double s = (Q2 > mu2) ? log( log(Q2/lam2) / log(mu2/lam2) ) : 0.; | |
1742 | double s2 = s * s; | |
1743 | double x1 = 1. - x; | |
1744 | double xL = -log(x); | |
1745 | double xS = sqrt(x); | |
1746 | ||
1747 | // uv, dbarv. | |
1748 | double uv = (0.519 + 0.180 * s - 0.011 * s2) * pow(x, 0.499 - 0.027 * s) | |
1749 | * (1. + (0.381 - 0.419 * s) * xS) * pow(x1, 0.367 + 0.563 * s); | |
1750 | ||
1751 | // g. | |
1752 | double gl = ( pow(x, 0.482 + 0.341 * sqrt(s)) | |
1753 | * ( (0.678 + 0.877 * s - 0.175 * s2) + (0.338 - 1.597 * s) * xS | |
1754 | + (-0.233 * s + 0.406 * s2) * x) + pow(s, 0.599) | |
1755 | * exp(-(0.618 + 2.070 * s) + sqrt(3.676 * pow(s, 1.263) * xL) ) ) | |
1756 | * pow(x1, 0.390 + 1.053 * s); | |
1757 | ||
1758 | // sea: u, d, s. | |
1759 | double ub = pow(s, 0.55) * (1. - 0.748 * xS + (0.313 + 0.935 * s) * x) | |
1760 | * pow(x1, 3.359) * exp(-(4.433 + 1.301 * s) + sqrt((9.30 - 0.887 * s) | |
1761 | * pow(s, 0.56) * xL) ) / pow(xL, 2.538 - 0.763 * s); | |
1762 | ||
1763 | // c. | |
1764 | double chm = (s < 0.888) ? 0. : pow(s - 0.888, 1.02) * (1. + 1.008 * x) | |
1765 | * pow(x1, 1.208 + 0.771 * s) * exp(-(4.40 + 1.493 * s) | |
1766 | + sqrt( (2.032 + 1.901 * s) * pow(s, 0.39) * xL) ); | |
1767 | ||
1768 | // b. | |
1769 | double bot = (s < 1.351) ? 0. : pow(s - 1.351, 1.03) | |
1770 | * pow(x1, 0.697 + 0.855 * s) * exp(-(4.51 + 1.490 * s) | |
1771 | + sqrt( (3.056 + 1.694 * s) * pow(s, 0.39) * xL) ); | |
1772 | ||
1773 | // Update values. | |
1774 | xg = gl; | |
1775 | xu = uv + ub; | |
1776 | xd = ub; | |
1777 | xubar = ub; | |
1778 | xdbar = uv + ub; | |
1779 | xs = ub; | |
1780 | xsbar = ub; | |
1781 | xc = chm; | |
1782 | xb = bot; | |
1783 | ||
1784 | // Subdivision of valence and sea. | |
1785 | xuVal = uv; | |
1786 | xuSea = ub; | |
1787 | xdVal = uv; | |
1788 | xdSea = ub; | |
1789 | ||
1790 | // idSav = 9 to indicate that all flavours reset. | |
1791 | idSav = 9; | |
1792 | ||
1793 | } | |
1794 | ||
1795 | //========================================================================== | |
1796 | ||
1797 | // Pomeron PDF: simple Q2-independent parametrizations N x^a (1 - x)^b. | |
1798 | ||
1799 | //-------------------------------------------------------------------------- | |
1800 | ||
1801 | // Calculate normalization factors once and for all. | |
1802 | ||
1803 | void PomFix::init() { | |
1804 | ||
1805 | normGluon = GammaReal(PomGluonA + PomGluonB + 2.) | |
1806 | / (GammaReal(PomGluonA + 1.) * GammaReal(PomGluonB + 1.)); | |
1807 | normQuark = GammaReal(PomQuarkA + PomQuarkB + 2.) | |
1808 | / (GammaReal(PomQuarkA + 1.) * GammaReal(PomQuarkB + 1.)); | |
1809 | ||
1810 | } | |
1811 | ||
1812 | //-------------------------------------------------------------------------- | |
1813 | ||
1814 | // Gives a generic Q2-independent Pomeron PDF. | |
1815 | ||
1816 | void PomFix::xfUpdate(int , double x, double) { | |
1817 | ||
1818 | // Gluon and quark distributions. | |
1819 | double gl = normGluon * pow(x, PomGluonA) * pow( (1. - x), PomGluonB); | |
1820 | double qu = normQuark * pow(x, PomQuarkA) * pow( (1. - x), PomQuarkB); | |
1821 | ||
1822 | // Update values | |
1823 | xg = (1. - PomQuarkFrac) * gl; | |
1824 | xu = (PomQuarkFrac / (4. + 2. * PomStrangeSupp) ) * qu; | |
1825 | xd = xu; | |
1826 | xubar = xu; | |
1827 | xdbar = xu; | |
1828 | xs = PomStrangeSupp * xu; | |
1829 | xsbar = xs; | |
1830 | xc = 0.; | |
1831 | xb = 0.; | |
1832 | ||
1833 | // Subdivision of valence and sea. | |
1834 | xuVal = 0.; | |
1835 | xuSea = xu; | |
1836 | xdVal = 0.; | |
1837 | xdSea = xd; | |
1838 | ||
1839 | // idSav = 9 to indicate that all flavours reset. | |
1840 | idSav = 9; | |
1841 | ||
1842 | } | |
1843 | ||
1844 | //========================================================================== | |
1845 | ||
1846 | // Pomeron PDF: the H1 2006 Fit A and Fit B Q2-dependent parametrizations. | |
1847 | ||
1848 | //-------------------------------------------------------------------------- | |
1849 | ||
1850 | void PomH1FitAB::init( int iFit, string xmlPath, Info* infoPtr) { | |
1851 | ||
1852 | // Open files from which grids should be read in. | |
1853 | if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; | |
1854 | string dataFile = "pomH1FitBlo.data"; | |
1855 | if (iFit == 1) dataFile = "pomH1FitA.data"; | |
1856 | if (iFit == 2) dataFile = "pomH1FitB.data"; | |
1857 | ifstream is( (xmlPath + dataFile).c_str() ); | |
1858 | if (!is.good()) { | |
1859 | if (infoPtr != 0) infoPtr->errorMsg("Error from PomH1FitAB::init: " | |
1860 | "the H1 Pomeron parametrization file was not found"); | |
1861 | else cout << " Error from PomH1FitAB::init: " | |
1862 | << "the H1 Pomeron parametrization file was not found" << endl; | |
1863 | isSet = false; | |
1864 | return; | |
1865 | } | |
1866 | ||
1867 | // Lower and upper bounds. Bin widths for logarithmic spacing. | |
1868 | nx = 100; | |
1869 | xlow = 0.001; | |
1870 | xupp = 0.99; | |
1871 | dx = log(xupp / xlow) / (nx - 1.); | |
1872 | nQ2 = 30; | |
1873 | Q2low = 1.0; | |
1874 | Q2upp = 30000.; | |
1875 | dQ2 = log(Q2upp / Q2low) / (nQ2 - 1.); | |
1876 | ||
1877 | // Read in quark data grid. | |
1878 | for (int i = 0; i < nx; ++i) | |
1879 | for (int j = 0; j < nQ2; ++j) | |
1880 | is >> quarkGrid[i][j]; | |
1881 | ||
1882 | // Read in gluon data grid. | |
1883 | for (int i = 0; i < nx; ++i) | |
1884 | for (int j = 0; j < nQ2; ++j) | |
1885 | is >> gluonGrid[i][j]; | |
1886 | ||
1887 | // Check for errors during read-in of file. | |
1888 | if (!is) { | |
1889 | if (infoPtr != 0) infoPtr->errorMsg("Error from PomH1FitAB::init: " | |
1890 | "the H1 Pomeron parametrization files could not be read"); | |
1891 | else cout << " Error from PomH1FitAB::init: " | |
1892 | << "the H1 Pomeron parametrization files could not be read" << endl; | |
1893 | isSet = false; | |
1894 | return; | |
1895 | } | |
1896 | ||
1897 | // Done. | |
1898 | isSet = true; | |
1899 | return; | |
1900 | } | |
1901 | ||
1902 | //-------------------------------------------------------------------------- | |
1903 | ||
1904 | void PomH1FitAB::xfUpdate(int , double x, double Q2) { | |
1905 | ||
1906 | // Retrict input to validity range. | |
1907 | double xt = min( xupp, max( xlow, x) ); | |
1908 | double Q2t = min( Q2upp, max( Q2low, Q2) ); | |
1909 | ||
1910 | // Lower grid point and distance above it. | |
1911 | double dlx = log( xt / xlow) / dx; | |
1912 | int i = min( nx - 2, int(dlx) ); | |
1913 | dlx -= i; | |
1914 | double dlQ2 = log( Q2t / Q2low) / dQ2; | |
1915 | int j = min( nQ2 - 2, int(dlQ2) ); | |
1916 | dlQ2 -= j; | |
1917 | ||
1918 | // Interpolate to derive quark PDF. | |
1919 | double qu = (1. - dlx) * (1. - dlQ2) * quarkGrid[i][j] | |
1920 | + dlx * (1. - dlQ2) * quarkGrid[i + 1][j] | |
1921 | + (1. - dlx) * dlQ2 * quarkGrid[i][j + 1] | |
1922 | + dlx * dlQ2 * quarkGrid[i + 1][j + 1]; | |
1923 | ||
1924 | // Interpolate to derive gluon PDF. | |
1925 | double gl = (1. - dlx) * (1. - dlQ2) * gluonGrid[i][j] | |
1926 | + dlx * (1. - dlQ2) * gluonGrid[i + 1][j] | |
1927 | + (1. - dlx) * dlQ2 * gluonGrid[i][j + 1] | |
1928 | + dlx * dlQ2 * gluonGrid[i + 1][j + 1]; | |
1929 | ||
1930 | // Update values. | |
1931 | xg = rescale * gl; | |
1932 | xu = rescale * qu; | |
1933 | xd = xu; | |
1934 | xubar = xu; | |
1935 | xdbar = xu; | |
1936 | xs = xu; | |
1937 | xsbar = xu; | |
1938 | xc = 0.; | |
1939 | xb = 0.; | |
1940 | ||
1941 | // Subdivision of valence and sea. | |
1942 | xuVal = 0.; | |
1943 | xuSea = xu; | |
1944 | xdVal = 0.; | |
1945 | xdSea = xu; | |
1946 | ||
1947 | // idSav = 9 to indicate that all flavours reset. | |
1948 | idSav = 9; | |
1949 | ||
1950 | } | |
1951 | ||
1952 | //========================================================================== | |
1953 | ||
1954 | // Pomeron PDF: the H1 2007 Jets Q2-dependent parametrization. | |
1955 | ||
1956 | //-------------------------------------------------------------------------- | |
1957 | ||
1958 | void PomH1Jets::init( string xmlPath, Info* infoPtr) { | |
1959 | ||
1960 | // Open files from which grids should be read in. | |
1961 | if (xmlPath[ xmlPath.length() - 1 ] != '/') xmlPath += "/"; | |
1962 | ifstream isg( (xmlPath + "pomH1JetsGluon.data").c_str() ); | |
1963 | ifstream isq( (xmlPath + "pomH1JetsSinglet.data").c_str() ); | |
1964 | ifstream isc( (xmlPath + "pomH1JetsCharm.data").c_str() ); | |
1965 | if (!isg.good() || !isq.good() || !isc.good()) { | |
1966 | if (infoPtr != 0) infoPtr->errorMsg("Error from PomH1Jets::init: " | |
1967 | "the H1 Pomeron parametrization files were not found"); | |
1968 | else cout << " Error from PomH1Jets::init: " | |
1969 | << "the H1 Pomeron parametrization files were not found" << endl; | |
1970 | isSet = false; | |
1971 | return; | |
1972 | } | |
1973 | ||
1974 | // Read in x and Q grids. Do interpolation logarithmically in Q2. | |
1975 | for (int i = 0; i < 100; ++i) { | |
1976 | isg >> setw(13) >> xGrid[i]; | |
1977 | } | |
1978 | for (int j = 0; j < 88; ++j) { | |
1979 | isg >> setw(13) >> Q2Grid[j]; | |
1980 | Q2Grid[j] = log( Q2Grid[j] ); | |
1981 | } | |
1982 | ||
1983 | // Read in gluon data grid. | |
1984 | for (int j = 0; j < 88; ++j) { | |
1985 | for (int i = 0; i < 100; ++i) { | |
1986 | isg >> setw(13) >> gluonGrid[i][j]; | |
1987 | } | |
1988 | } | |
1989 | ||
1990 | // Identical x and Q2 grid for singlet, so skip ahead. | |
1991 | double dummy; | |
1992 | for (int i = 0; i < 188; ++i) isq >> setw(13) >> dummy; | |
1993 | ||
1994 | // Read in singlet data grid. | |
1995 | for (int j = 0; j < 88; ++j) { | |
1996 | for (int i = 0; i < 100; ++i) { | |
1997 | isq >> setw(13) >> singletGrid[i][j]; | |
1998 | } | |
1999 | } | |
2000 | ||
2001 | // Identical x and Q2 grid for charm, so skip ahead. | |
2002 | for (int i = 0; i < 188; ++i) isc >> setw(13) >> dummy; | |
2003 | ||
2004 | // Read in charm data grid. | |
2005 | for (int j = 0; j < 88; ++j) { | |
2006 | for (int i = 0; i < 100; ++i) { | |
2007 | isc >> setw(13) >> charmGrid[i][j]; | |
2008 | } | |
2009 | } | |
2010 | ||
2011 | // Check for errors during read-in of files. | |
2012 | if (!isg || !isq || !isc) { | |
2013 | if (infoPtr != 0) infoPtr->errorMsg("Error from PomH1Jets::init: " | |
2014 | "the H1 Pomeron parametrization files could not be read"); | |
2015 | else cout << " Error from PomH1Jets::init: " | |
2016 | << "the H1 Pomeron parametrization files could not be read" << endl; | |
2017 | isSet = false; | |
2018 | return; | |
2019 | } | |
2020 | ||
2021 | // Done. | |
2022 | isSet = true; | |
2023 | return; | |
2024 | } | |
2025 | ||
2026 | //-------------------------------------------------------------------------- | |
2027 | ||
2028 | void PomH1Jets::xfUpdate(int , double x, double Q2) { | |
2029 | ||
2030 | // Find position in x array. | |
2031 | double xLog = log(x); | |
2032 | int i = 0; | |
2033 | double dx = 0.; | |
2034 | if (xLog <= xGrid[0]); | |
2035 | else if (xLog >= xGrid[99]) { | |
2036 | i = 98; | |
2037 | dx = 1.; | |
2038 | } else { | |
2039 | while (xLog > xGrid[i]) ++i; | |
2040 | --i; | |
2041 | dx = (xLog - xGrid[i]) / (xGrid[i + 1] - xGrid[i]); | |
2042 | } | |
2043 | ||
2044 | // Find position in y array. | |
2045 | double Q2Log = log(Q2); | |
2046 | int j = 0; | |
2047 | double dQ2 = 0.; | |
2048 | if (Q2Log <= Q2Grid[0]); | |
2049 | else if (Q2Log >= Q2Grid[87]) { | |
2050 | j = 86; | |
2051 | dQ2 = 1.; | |
2052 | } else { | |
2053 | while (Q2Log > Q2Grid[j]) ++j; | |
2054 | --j; | |
2055 | dQ2 = (Q2Log - Q2Grid[j]) / (Q2Grid[j + 1] - Q2Grid[j]); | |
2056 | } | |
2057 | ||
2058 | // Interpolate to derive gluon PDF. | |
2059 | double gl = (1. - dx) * (1. - dQ2) * gluonGrid[i][j] | |
2060 | + dx * (1. - dQ2) * gluonGrid[i + 1][j] | |
2061 | + (1. - dx) * dQ2 * gluonGrid[i][j + 1] | |
2062 | + dx * dQ2 * gluonGrid[i + 1][j + 1]; | |
2063 | ||
2064 | // Interpolate to derive singlet PDF. (Sum of u, d, s, ubar, dbar, sbar.) | |
2065 | double sn = (1. - dx) * (1. - dQ2) * singletGrid[i][j] | |
2066 | + dx * (1. - dQ2) * singletGrid[i + 1][j] | |
2067 | + (1. - dx) * dQ2 * singletGrid[i][j + 1] | |
2068 | + dx * dQ2 * singletGrid[i + 1][j + 1]; | |
2069 | ||
2070 | // Interpolate to derive charm PDF. (Charge-square times c and cbar.) | |
2071 | double ch = (1. - dx) * (1. - dQ2) * charmGrid[i][j] | |
2072 | + dx * (1. - dQ2) * charmGrid[i + 1][j] | |
2073 | + (1. - dx) * dQ2 * charmGrid[i][j + 1] | |
2074 | + dx * dQ2 * charmGrid[i + 1][j + 1]; | |
2075 | ||
2076 | // Update values. | |
2077 | xg = rescale * gl; | |
2078 | xu = rescale * sn / 6.; | |
2079 | xd = xu; | |
2080 | xubar = xu; | |
2081 | xdbar = xu; | |
2082 | xs = xu; | |
2083 | xsbar = xu; | |
2084 | xc = rescale * ch * 9./8.; | |
2085 | xb = 0.; | |
2086 | ||
2087 | // Subdivision of valence and sea. | |
2088 | xuVal = 0.; | |
2089 | xuSea = xu; | |
2090 | xdVal = 0.; | |
2091 | xdSea = xd; | |
2092 | ||
2093 | // idSav = 9 to indicate that all flavours reset. | |
2094 | idSav = 9; | |
2095 | ||
2096 | } | |
2097 | ||
2098 | //========================================================================== | |
2099 | ||
2100 | // Gives electron (or muon, or tau) parton distribution. | |
2101 | ||
2102 | // Constants: alphaEM(0), m_e, m_mu, m_tau. | |
2103 | const double Lepton::ALPHAEM = 0.00729735; | |
2104 | const double Lepton::ME = 0.0005109989; | |
2105 | const double Lepton::MMU = 0.10566; | |
2106 | const double Lepton::MTAU = 1.77699; | |
2107 | ||
2108 | void Lepton::xfUpdate(int id, double x, double Q2) { | |
2109 | ||
2110 | // Squared mass of lepton species: electron, muon, tau. | |
2111 | if (!isInit) { | |
2112 | double mLep = ME; | |
2113 | if (abs(id) == 13) mLep = MMU; | |
2114 | if (abs(id) == 15) mLep = MTAU; | |
2115 | m2Lep = pow2( mLep ); | |
2116 | isInit = true; | |
2117 | } | |
2118 | ||
2119 | // Electron inside electron, see R. Kleiss et al., in Z physics at | |
2120 | // LEP 1, CERN 89-08, p. 34 | |
2121 | double xLog = log(max(1e-10,x)); | |
2122 | double xMinusLog = log( max(1e-10, 1. - x) ); | |
2123 | double Q2Log = log( max(3., Q2/m2Lep) ); | |
2124 | double beta = (ALPHAEM / M_PI) * (Q2Log - 1.); | |
2125 | double delta = 1. + (ALPHAEM / M_PI) * (1.5 * Q2Log + 1.289868) | |
2126 | + pow2(ALPHAEM / M_PI) * (-2.164868 * Q2Log*Q2Log | |
2127 | + 9.840808 * Q2Log - 10.130464); | |
2128 | double fPrel = beta * pow(1. - x, beta - 1.) * sqrtpos( delta ) | |
2129 | - 0.5 * beta * (1. + x) + 0.125 * beta*beta * ( (1. + x) | |
2130 | * (-4. * xMinusLog + 3. * xLog) - 4. * xLog / (1. - x) - 5. - x); | |
2131 | ||
2132 | // Zero distribution for very large x and rescale it for intermediate. | |
2133 | if (x > 1. - 1e-10) fPrel = 0.; | |
2134 | else if (x > 1. - 1e-7) fPrel *= pow(1000.,beta) / (pow(1000.,beta) - 1.); | |
2135 | xlepton = x * fPrel; | |
2136 | ||
2137 | // Photon inside electron (one possible scheme - primitive). | |
2138 | xgamma = (0.5 * ALPHAEM / M_PI) * Q2Log * (1. + pow2(1. - x)); | |
2139 | ||
2140 | // idSav = 9 to indicate that all flavours reset. | |
2141 | idSav = 9; | |
2142 | ||
2143 | } | |
2144 | ||
2145 | //========================================================================== | |
2146 | ||
2147 | } // end namespace Pythia8 |