5 * Revision 1.1.1.2 1996/10/30 08:30:53 cernlib
8 * Revision 1.1.1.1 1996/04/12 15:29:48 plothow
12 #include "pdf/pilot.h"
13 SUBROUTINE SMRSPI(X,SCALE,MODE,UPV,DNV,SEA,STR,CHM,BOT,GLU)
14 C***************************************************************C
16 C PION DISTRIBUTION FUNCTIONS EXTRACTED FROM DRELL-YAN AND C
17 C PROMPT PHOTON PION BEAM DATA, USING (NUCLEAR TARGET C
18 C CORRECTED) HMRS(B) DISTRIBUTIONS FOR THE NUCLEON. C
19 C MAIN UNCERTAINTY IS IN SEA, HENCE FOLLOWING THREE SETS... C
20 C MODE=2 IS THE "BEST FIT" SET. C
22 C MODE 1 CORRESPONDS TO A 10% MOMENTUM SEA (0.11213) C
23 C MODE 2 CORRESPONDS TO A 15% MOMENTUM SEA (0.16119) C
24 C MODE 3 CORRESPONDS TO A 20% MOMENTUM SEA (0.23785) C
26 C (NUMBER IN BRACKETS IS LAST ENTRY IN FIRST ROW OF GRID) C
30 C REFERENCE: A.D. MARTIN. R.G. ROBERTS. W.J. STIRLING C
31 C AND P.J. SUTTON, PREPRINT RAL-91-058 (1991). C
34 C FOR THESE SETS.... C
35 C * LAMBDA(MSBAR,NF=4) = 190 MEV C
36 C * UV=DV, STR=USEA=DSEA, BTM=0 C
38 C NOTE THAT X TIMES THE PARTON DISTRIBUTION FUNCTION C
39 C IS RETURNED I.E. G(X) = GLU/X ETC, AND THAT "SEA" C
40 C IS THE QUARK SEA / 6 I.E. UBAR(X)=DBAR(X) C
41 C = SEA/X FOR A PION. IF IN DOUBT, CHECK THE C
42 C MOMENTUM SUM RULE! NOTE ALSO THAT SCALE=Q IN GEV C
46 C THE RANGE OF APPLICABILITY IS CURRENTLY: C
47 C 10**-5 < X < 1 AND 5 < Q**2 < 1.31 * 10**6 C
48 C HIGHER Q**2 VALUES CAN BE SUPPLIED ON REQUEST C
49 C - PROBLEMS, COMMENTS ETC TO WJS@UK.AC.DUR.HEP C
52 C***************************************************************C
53 #include "pdf/impdp.inc"
54 IF(MODE.EQ.1) CALL SMRSP31(X,SCALE,UPV,DNV,SEA,STR,CHM,BOT,GLU)
55 IF(MODE.EQ.2) CALL SMRSP32(X,SCALE,UPV,DNV,SEA,STR,CHM,BOT,GLU)
56 IF(MODE.EQ.3) CALL SMRSP33(X,SCALE,UPV,DNV,SEA,STR,CHM,BOT,GLU)