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21886bb6 | 1 | #include "pdf/pilot.h" |
2 | C...SaSgam version 2 - parton distributions of the photon | |
3 | C...by Gerhard A. Schuler and Torbjorn Sjostrand | |
4 | C...For further information see Z. Phys. C68 (1995) 607 | |
5 | C...and CERN-TH/96-04 and LU TP 96-2. | |
6 | C...Program last changed on 18 January 1996. | |
7 | ||
8 | C!!!Note that one further call parameter - IP2 - has been added | |
9 | C!!!to the SASGAM argument list compared with version 1. | |
10 | ||
11 | C...The user should only need to call the SASGAM routine, | |
12 | C...which in turn calls the auxiliary routines SASVMD, SASANO, | |
13 | C...SASBEH and SASDIR. The package is self-contained. | |
14 | ||
15 | C...One particular aspect of these parametrizations is that F2 for | |
16 | C...the photon is not obtained just as the charge-squared-weighted | |
17 | C...sum of quark distributions, but differ in the treatment of | |
18 | C...heavy flavours (in F2 the DIS relation W2 = Q2*(1-x)/x restricts | |
19 | C...the kinematics range of heavy-flavour production, but the same | |
20 | C...kinematics is not relevant e.g. for jet production) and, for the | |
21 | C...'MSbar' fits, in the addition of a Cgamma term related to the | |
22 | C...separation of direct processes. Schematically: | |
23 | C...PDF = VMD (rho, omega, phi) + anomalous (d, u, s, c, b). | |
24 | C...F2 = VMD (rho, omega, phi) + anomalous (d, u, s) + | |
25 | C... Bethe-Heitler (c, b) (+ Cgamma (d, u, s)). | |
26 | C...The J/psi and Upsilon states have not been included in the VMD sum, | |
27 | C...but low c and b masses in the other components should compensate | |
28 | C...for this in a duality sense. | |
29 | ||
30 | C...The calling sequence is the following: | |
31 | C CALL SASGAM2(ISET,X,Q2,P2,IP2,F2GM,XPDFGM) | |
32 | C...with the following declaration statement: | |
33 | C DIMENSION XPDFGM(-6:6) | |
34 | C...and, optionally, further information in: | |
35 | C COMMON/SASCOM/XPVMD(-6:6),XPANL(-6:6),XPANH(-6:6),XPBEH(-6:6), | |
36 | C &XPDIR(-6:6) | |
37 | C COMMON/SASVAL/VXPVMD(-6:6),VXPANL(-6:6),VXPANH(-6:6),VXPDGM(-6:6) | |
38 | C...Input: ISET = 1 : SaS set 1D ('DIS', Q0 = 0.6 GeV) | |
39 | C = 2 : SaS set 1M ('MSbar', Q0 = 0.6 GeV) | |
40 | C = 3 : SaS set 2D ('DIS', Q0 = 2 GeV) | |
41 | C = 4 : SaS set 2M ('MSbar', Q0 = 2 GeV) | |
42 | C X : x value. | |
43 | C Q2 : Q2 value. | |
44 | C P2 : P2 value; should be = 0. for an on-shell photon. | |
45 | C IP2 : scheme used to evaluate off-shell anomalous component. | |
46 | C = 0 : recommended default, see = 7. | |
47 | C = 1 : dipole dampening by integration; very time-consuming. | |
48 | C = 2 : P_0^2 = max( Q_0^2, P^2 ) | |
49 | C = 3 : P'_0^2 = Q_0^2 + P^2. | |
50 | C = 4 : P_{eff} that preserves momentum sum. | |
51 | C = 5 : P_{int} that preserves momentum and average | |
52 | C evolution range. | |
53 | C = 6 : P_{eff}, matched to P_0 in P2 -> Q2 limit. | |
54 | C = 7 : P_{eff}, matched to P_0 in P2 -> Q2 limit. | |
55 | C...Output: F2GM : F2 value of the photon (including factors of alpha_em). | |
56 | C XPFDGM : x times parton distribution functions of the photon, | |
57 | C with elements 0 = g, 1 = d, 2 = u, 3 = s, 4 = c, 5 = b, | |
58 | C 6 = t (always empty!), - for antiquarks (result is same). | |
59 | C...The breakdown by component is stored in the commonblock SASCOM, | |
60 | C with elements as above. | |
61 | C XPVMD : rho, omega, phi VMD part only of output. | |
62 | C XPANL : d, u, s anomalous part only of output. | |
63 | C XPANH : c, b anomalous part only of output. | |
64 | C XPBEH : c, b Bethe-Heitler part only of output. | |
65 | C XPDIR : Cgamma (direct contribution) part only of output. | |
66 | C...The above arrays do not distinguish valence and sea contributions, | |
67 | C...although this information is available internally. The additional | |
68 | C...commonblock SASVAL provides the valence part only of the above | |
69 | C...distributions. Array names VXPVMD, VXPANL and VXPANH correspond | |
70 | C...to XPVMD, XPANL and XPANH, while XPBEH and XPDIR are valence only | |
71 | C...and therefore not given doubly. VXPDGM gives the sum of valence | |
72 | C...parts, and so matches XPDFGM. The difference, i.e. XPVMD-VXPVMD | |
73 | C...and so on, gives the sea part only. | |
74 | ||
75 | SUBROUTINE SASGAM2(ISET,X,Q2,P2,IP2,F2GM,XPDFGM) | |
76 | C...Purpose: to construct the F2 and parton distributions of the photon | |
77 | C...by summing homogeneous (VMD) and inhomogeneous (anomalous) terms. | |
78 | C...For F2, c and b are included by the Bethe-Heitler formula; | |
79 | C...in the 'MSbar' scheme additionally a Cgamma term is added. | |
80 | DIMENSION XPDFGM(-6:6) | |
81 | COMMON/SASCOM/XPVMD(-6:6),XPANL(-6:6),XPANH(-6:6),XPBEH(-6:6), | |
82 | &XPDIR(-6:6) | |
83 | COMMON/SASVAL/VXPVMD(-6:6),VXPANL(-6:6),VXPANH(-6:6),VXPDGM(-6:6) | |
84 | SAVE /SASCOM/,/SASVAL/ | |
85 | ||
86 | C...Temporary array. | |
87 | DIMENSION XPGA(-6:6), VXPGA(-6:6) | |
88 | C...Charm and bottom masses (low to compensate for J/psi etc.). | |
89 | DATA PMC/1.3/, PMB/4.6/ | |
90 | C...alpha_em and alpha_em/(2*pi). | |
91 | DATA AEM/0.007297/, AEM2PI/0.0011614/ | |
92 | C...Lambda value for 4 flavours. | |
93 | DATA ALAM/0.20/ | |
94 | C...Mixture u/(u+d), = 0.5 for incoherent and = 0.8 for coherent sum. | |
95 | DATA FRACU/0.8/ | |
96 | C...VMD couplings f_V**2/(4*pi). | |
97 | DATA FRHO/2.20/, FOMEGA/23.6/, FPHI/18.4/ | |
98 | C...Masses for rho (=omega) and phi. | |
99 | DATA PMRHO/0.770/, PMPHI/1.020/ | |
100 | C...Number of points in integration for IP2=1. | |
101 | DATA NSTEP/100/ | |
102 | ||
103 | C...Reset output. | |
104 | F2GM=0. | |
105 | DO 100 KFL=-6,6 | |
106 | XPDFGM(KFL)=0. | |
107 | XPVMD(KFL)=0. | |
108 | XPANL(KFL)=0. | |
109 | XPANH(KFL)=0. | |
110 | XPBEH(KFL)=0. | |
111 | XPDIR(KFL)=0. | |
112 | VXPVMD(KFL)=0. | |
113 | VXPANL(KFL)=0. | |
114 | VXPANH(KFL)=0. | |
115 | VXPDGM(KFL)=0. | |
116 | 100 CONTINUE | |
117 | ||
118 | C...Check that input sensible. | |
119 | IF(ISET.LE.0.OR.ISET.GE.5) THEN | |
120 | WRITE(*,*) ' FATAL ERROR: SaSgam called for unknown set' | |
121 | WRITE(*,*) ' ISET = ',ISET | |
122 | STOP | |
123 | ENDIF | |
124 | IF(X.LE.0..OR.X.GT.1.) THEN | |
125 | WRITE(*,*) ' FATAL ERROR: SaSgam called for unphysical x' | |
126 | WRITE(*,*) ' X = ',X | |
127 | STOP | |
128 | ENDIF | |
129 | ||
130 | C...Set Q0 cut-off parameter as function of set used. | |
131 | IF(ISET.LE.2) THEN | |
132 | Q0=0.6 | |
133 | ELSE | |
134 | Q0=2. | |
135 | ENDIF | |
136 | Q02=Q0**2 | |
137 | ||
138 | C...Scale choice for off-shell photon; common factors. | |
139 | Q2A=Q2 | |
140 | FACNOR=1. | |
141 | IF(IP2.EQ.1) THEN | |
142 | P2MX=P2+Q02 | |
143 | Q2A=Q2+P2*Q02/MAX(Q02,Q2) | |
144 | FACNOR=LOG(Q2/Q02)/NSTEP | |
145 | ELSEIF(IP2.EQ.2) THEN | |
146 | P2MX=MAX(P2,Q02) | |
147 | ELSEIF(IP2.EQ.3) THEN | |
148 | P2MX=P2+Q02 | |
149 | Q2A=Q2+P2*Q02/MAX(Q02,Q2) | |
150 | ELSEIF(IP2.EQ.4) THEN | |
151 | P2MX=Q2*(Q02+P2)/(Q2+P2)*EXP(P2*(Q2-Q02)/ | |
152 | & ((Q2+P2)*(Q02+P2))) | |
153 | ELSEIF(IP2.EQ.5) THEN | |
154 | P2MXA=Q2*(Q02+P2)/(Q2+P2)*EXP(P2*(Q2-Q02)/ | |
155 | & ((Q2+P2)*(Q02+P2))) | |
156 | P2MX=Q0*SQRT(P2MXA) | |
157 | FACNOR=LOG(Q2/P2MXA)/LOG(Q2/P2MX) | |
158 | ELSEIF(IP2.EQ.6) THEN | |
159 | P2MX=Q2*(Q02+P2)/(Q2+P2)*EXP(P2*(Q2-Q02)/ | |
160 | & ((Q2+P2)*(Q02+P2))) | |
161 | P2MX=MAX(0.,1.-P2/Q2)*P2MX+MIN(1.,P2/Q2)*MAX(P2,Q02) | |
162 | ELSE | |
163 | P2MXA=Q2*(Q02+P2)/(Q2+P2)*EXP(P2*(Q2-Q02)/ | |
164 | & ((Q2+P2)*(Q02+P2))) | |
165 | P2MX=Q0*SQRT(P2MXA) | |
166 | P2MXB=P2MX | |
167 | P2MX=MAX(0.,1.-P2/Q2)*P2MX+MIN(1.,P2/Q2)*MAX(P2,Q02) | |
168 | P2MXB=MAX(0.,1.-P2/Q2)*P2MXB+MIN(1.,P2/Q2)*P2MXA | |
169 | FACNOR=LOG(Q2/P2MXA)/LOG(Q2/P2MXB) | |
170 | ENDIF | |
171 | ||
172 | C...Call VMD parametrization for d quark and use to give rho, omega, | |
173 | C...phi. Note dipole dampening for off-shell photon. | |
174 | CALL SASVMD(ISET,1,X,Q2A,P2MX,ALAM,XPGA,VXPGA) | |
175 | XFVAL=VXPGA(1) | |
176 | XPGA(1)=XPGA(2) | |
177 | XPGA(-1)=XPGA(-2) | |
178 | FACUD=AEM*(1./FRHO+1./FOMEGA)*(PMRHO**2/(PMRHO**2+P2))**2 | |
179 | FACS=AEM*(1./FPHI)*(PMPHI**2/(PMPHI**2+P2))**2 | |
180 | DO 110 KFL=-5,5 | |
181 | XPVMD(KFL)=(FACUD+FACS)*XPGA(KFL) | |
182 | 110 CONTINUE | |
183 | XPVMD(1)=XPVMD(1)+(1.-FRACU)*FACUD*XFVAL | |
184 | XPVMD(2)=XPVMD(2)+FRACU*FACUD*XFVAL | |
185 | XPVMD(3)=XPVMD(3)+FACS*XFVAL | |
186 | XPVMD(-1)=XPVMD(-1)+(1.-FRACU)*FACUD*XFVAL | |
187 | XPVMD(-2)=XPVMD(-2)+FRACU*FACUD*XFVAL | |
188 | XPVMD(-3)=XPVMD(-3)+FACS*XFVAL | |
189 | VXPVMD(1)=(1.-FRACU)*FACUD*XFVAL | |
190 | VXPVMD(2)=FRACU*FACUD*XFVAL | |
191 | VXPVMD(3)=FACS*XFVAL | |
192 | VXPVMD(-1)=(1.-FRACU)*FACUD*XFVAL | |
193 | VXPVMD(-2)=FRACU*FACUD*XFVAL | |
194 | VXPVMD(-3)=FACS*XFVAL | |
195 | ||
196 | IF(IP2.NE.1) THEN | |
197 | C...Anomalous parametrizations for different strategies | |
198 | C...for off-shell photons; except full integration. | |
199 | ||
200 | C...Call anomalous parametrization for d + u + s. | |
201 | CALL SASANO(-3,X,Q2A,P2MX,ALAM,XPGA,VXPGA) | |
202 | DO 120 KFL=-5,5 | |
203 | XPANL(KFL)=FACNOR*XPGA(KFL) | |
204 | VXPANL(KFL)=FACNOR*VXPGA(KFL) | |
205 | 120 CONTINUE | |
206 | ||
207 | C...Call anomalous parametrization for c and b. | |
208 | CALL SASANO(4,X,Q2A,P2MX,ALAM,XPGA,VXPGA) | |
209 | DO 130 KFL=-5,5 | |
210 | XPANH(KFL)=FACNOR*XPGA(KFL) | |
211 | VXPANH(KFL)=FACNOR*VXPGA(KFL) | |
212 | 130 CONTINUE | |
213 | CALL SASANO(5,X,Q2A,P2MX,ALAM,XPGA,VXPGA) | |
214 | DO 140 KFL=-5,5 | |
215 | XPANH(KFL)=XPANH(KFL)+FACNOR*XPGA(KFL) | |
216 | VXPANH(KFL)=VXPANH(KFL)+FACNOR*VXPGA(KFL) | |
217 | 140 CONTINUE | |
218 | ||
219 | ELSE | |
220 | C...Special option: loop over flavours and integrate over k2. | |
221 | DO 170 KF=1,5 | |
222 | DO 160 ISTEP=1,NSTEP | |
223 | Q2STEP=Q02*(Q2/Q02)**((ISTEP-0.5)/NSTEP) | |
224 | IF((KF.EQ.4.AND.Q2STEP.LT.PMC**2).OR. | |
225 | & (KF.EQ.5.AND.Q2STEP.LT.PMB**2)) GOTO 160 | |
226 | CALL SASVMD(0,KF,X,Q2,Q2STEP,ALAM,XPGA,VXPGA) | |
227 | FACQ=AEM2PI*(Q2STEP/(Q2STEP+P2))**2*FACNOR | |
228 | IF(MOD(KF,2).EQ.0) FACQ=FACQ*(8./9.) | |
229 | IF(MOD(KF,2).EQ.1) FACQ=FACQ*(2./9.) | |
230 | DO 150 KFL=-5,5 | |
231 | IF(KF.LE.3) XPANL(KFL)=XPANL(KFL)+FACQ*XPGA(KFL) | |
232 | IF(KF.GE.4) XPANH(KFL)=XPANH(KFL)+FACQ*XPGA(KFL) | |
233 | IF(KF.LE.3) VXPANL(KFL)=VXPANL(KFL)+FACQ*VXPGA(KFL) | |
234 | IF(KF.GE.4) VXPANH(KFL)=VXPANH(KFL)+FACQ*VXPGA(KFL) | |
235 | 150 CONTINUE | |
236 | 160 CONTINUE | |
237 | 170 CONTINUE | |
238 | ENDIF | |
239 | ||
240 | C...Call Bethe-Heitler term expression for charm and bottom. | |
241 | CALL SASBEH(4,X,Q2,P2,PMC**2,XPBH) | |
242 | XPBEH(4)=XPBH | |
243 | XPBEH(-4)=XPBH | |
244 | CALL SASBEH(5,X,Q2,P2,PMB**2,XPBH) | |
245 | XPBEH(5)=XPBH | |
246 | XPBEH(-5)=XPBH | |
247 | ||
248 | C...For MSbar subtraction call C^gamma term expression for d, u, s. | |
249 | IF(ISET.EQ.2.OR.ISET.EQ.4) THEN | |
250 | CALL SASDIR(X,Q2,P2,Q02,XPGA) | |
251 | DO 180 KFL=-5,5 | |
252 | XPDIR(KFL)=XPGA(KFL) | |
253 | 180 CONTINUE | |
254 | ENDIF | |
255 | ||
256 | C...Store result in output array. | |
257 | DO 190 KFL=-5,5 | |
258 | CHSQ=1./9. | |
259 | IF(IABS(KFL).EQ.2.OR.IABS(KFL).EQ.4) CHSQ=4./9. | |
260 | XPF2=XPVMD(KFL)+XPANL(KFL)+XPBEH(KFL)+XPDIR(KFL) | |
261 | IF(KFL.NE.0) F2GM=F2GM+CHSQ*XPF2 | |
262 | XPDFGM(KFL)=XPVMD(KFL)+XPANL(KFL)+XPANH(KFL) | |
263 | VXPDGM(KFL)=VXPVMD(KFL)+VXPANL(KFL)+VXPANH(KFL) | |
264 | 190 CONTINUE | |
265 | ||
266 | RETURN | |
267 | END |