]>
Commit | Line | Data |
---|---|---|
f5ab1a71 | 1 | c 1 2 3 4 5 6 7 8 |
2 | c---------|---------|---------|---------|---------|---------|---------|---------| | |
3 | *-- Author : R.Lednicky 20/01/95 | |
4 | SUBROUTINE fsiw | |
5 | C======================================================================= | |
6 | C Calculates final state interaction (FSI) weights | |
7 | C WEIF = weight due to particle - (effective) nucleus FSI (p-N) | |
8 | C WEI = weight due to p-p-N FSI | |
9 | C WEIN = weight due to p-p FSI; note that WEIN=WEI if I3C=0; | |
10 | C note that if I3C=1 the calculation of | |
11 | C WEIN can be skipped by putting J=0 | |
12 | C....................................................................... | |
13 | C Correlation Functions: | |
14 | C CF(p-p-N) = sum(WEI)/sum(WEIF) | |
15 | C CF(p-p) = sum(WEIN)/sum(1); here the nucleus is completely | |
16 | C inactive | |
17 | C CF(p-p-"N") = sum(WEIN*WEIF')/sum(WEIF'), where WEIN and WEIF' | |
18 | C are not correlated (calculated at different emission | |
19 | C points, e.g., for different events); | |
20 | C thus here the nucleus affects one-particle | |
21 | C spectra but not the correlation | |
22 | C....................................................................... | |
23 | C User must supply data file <fn> on unit NUNIT (e.g. =11) specifying | |
24 | C LL : particle pair | |
25 | C NS : approximation used to calculate Bethe-Salpeter amplitude | |
26 | C ITEST: test switch | |
27 | C If ITEST=1 then also following parameters are required | |
28 | C ICH : 1(0) Coulomb interaction between the two particles ON (OFF) | |
29 | C IQS : 1(0) quantum statistics for the two particles ON (OFF) | |
30 | C ISI : 1(0) strong interaction between the two particles ON (OFF) | |
31 | C I3C : 1(0) Coulomb interaction with residual nucleus ON (OFF) | |
32 | C This data file can contain other information useful for the user. | |
33 | C It is read by subroutines READINT4 and READREA8(4) (or READ_FILE). | |
34 | C---------------------------------------------------------------------- | |
35 | C- LL 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 | |
36 | C- part. 1: n p n alfa pi+ pi0 pi+ n p pi+ pi+ pi+ pi- K+ K+ K+ K- | |
37 | C- part. 2: n p p alfa pi- pi0 pi+ d d K- K+ p p K- K+ p p | |
38 | C NS=1 y/n: + + + + + - - - - - - - - - - - - | |
39 | C---------------------------------------------------------------------- | |
40 | C- LL 18 19 20 21 22 23 24 25 26 27 28 | |
41 | C- part. 1: d d t t K0 K0 d p p p n | |
42 | C- part. 2: d alfa t alfa K0 K0b t t alfa lambda lambda | |
43 | C NS=1 y/n: - - - - - - - - - + + | |
44 | C---------------------------------------------------------------------- | |
45 | C NS=1 Square well potential, | |
46 | C NS=3 not used | |
47 | C NS=4 scattered wave approximated by the spherical wave, | |
48 | C NS=2 same as NS=4 but the approx. of equal emission times in PRF | |
49 | C not required (t=0 approx. used in all other cases). | |
50 | C Note: if NS=2,4, the B-S amplitude diverges at zero distance r* in | |
51 | C the two-particle c.m.s.; user can specify a cutoff AA in | |
52 | C SUBROUTINE FSIINI, for example: | |
53 | C IF(NS.EQ.2.OR.NS.EQ.4)AA=5.D0 !! in 1/GeV --> AA=1. fm | |
54 | C--------------------------------------------------------------------- | |
55 | C ITEST=1 any values of parameters ICH, IQS, ISI, I3C are allowed | |
56 | C and should be given in data file <fn> | |
57 | C ITEST=0 physical values of these parameters are put automatically | |
58 | C in FSIINI (their values are not required in data file) | |
59 | C===================================================================== | |
60 | C At the beginning of calculation user should call FSIINI, | |
61 | C which reads LL, NS, ITEST (and eventually ICH, IQS, ISI, I3C) | |
62 | C and initializes various parameters. | |
63 | C In particular the constants in | |
64 | C COMMON/FSI_CONS/PI,PI2,SPI,DR,W | |
65 | C may be useful for the user: | |
66 | C W=1/.1973D0 ! from fm to 1/GeV | |
67 | C PI=4*DATAN(1.D0) | |
68 | C PI2=2*PI | |
69 | C SPI=DSQRT(PI) | |
70 | C DR=180.D0/PI ! from radian to degree | |
71 | C _______________________________________________________ | |
72 | C !! |Important note: all real quantities are assumed REAL*8 | !! | |
73 | C ------------------------------------------------------- | |
74 | C For each event user should fill in the following information | |
75 | C in COMMONs (all COMMONs in FSI calculation start with FSI_): | |
76 | C ................................................................... | |
77 | C COMMON/FSI_POC/AMN,AM1,AM2,CN,C1,C2,AC1,AC2 | |
78 | C Only | |
79 | C AMN = mass of the effective nucleus [GeV/c**2] | |
80 | C CN = charge of the effective nucleus [elem. charge units] | |
81 | C are required | |
82 | C ................................................................... | |
83 | C COMMON/FSI_MOM/P1X,P1Y,P1Z,E1,P1, !part. momenta in the rest frame | |
84 | C 1 P2X,P2Y,P2Z,E2,P2 !of effective nucleus (NRF) | |
85 | C Only the components | |
86 | C PiX,PiY,PiZ [GeV/c] | |
87 | C in NRF are required. | |
88 | C To make the corresponding Lorentz transformation user can use the | |
89 | C subroutines LTRAN and LTRANB | |
90 | C ................................................................... | |
91 | C COMMON/FSI_COOR/X1,Y1,Z1,T1,R1, ! 4-coord. of emission | |
92 | C 1 X2,Y2,Z2,T2,R2 ! points in NRF | |
93 | C The componets | |
94 | C Xi,Yi,Zi [fm] | |
95 | C and emission times | |
96 | C Ti [fm/c] | |
97 | C should be given in NRF with the origin assumed at the center | |
98 | C of the effective nucleus. If the effect of residual nucleus is | |
99 | C not calculated within FSIW, the NRF can be any fixed frame. | |
100 | C----------------------------------------------------------------------- | |
101 | C Before calling FSIW the user must call | |
102 | C CALL LTRAN12 | |
103 | C Besides Lorentz transformation to pair rest frame: | |
104 | C (p1-p2)/2 --> k* it also transforms 4-coordinates of | |
105 | C emission points from fm to 1/GeV and calculates Ei,Pi and Ri. | |
106 | C Note that |k*|=AK in COMMON/FSI_PRF/ | |
107 | C----------------------------------------------------------------------- | |
108 | C After making some additional filtering using k* (say k* < k*max) | |
109 | C or direction of vector k*, | |
110 | C user can finally call FSIW to calculate the FSI weights | |
111 | C to be used to construct the correlation function | |
112 | C======================================================================= | |
113 | ||
114 | IMPLICIT REAL*8 (A-H,O-Z) | |
115 | COMMON/FSI_JR/JRAT | |
116 | COMMON/FSI_POC/AMN,AM1,AM2,CN,C1,C2,AC1,AC2 | |
117 | COMMON/FSI_MOM/P1X,P1Y,P1Z,E1,P1, ! particle momenta in NRF | |
118 | 1 P2X,P2Y,P2Z,E2,P2 | |
119 | COMMON/FSI_PRF/PPX,PPY,PPZ,AK,AKS, ! k*=(p1-p2)/2 and x1-x2 | |
120 | 1 X,Y,Z,T,RP,RPS ! in pair rest frame (PRF) | |
121 | COMMON/FSI_COOR/X1,Y1,Z1,T1,R1, !4-coord. of emis. points in NRF | |
122 | 1 X2,Y2,Z2,T2,R2 | |
123 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
124 | COMMON/FSI_FFPN/FF12,FF21 | |
125 | COMPLEX*16 FF12,FF21 | |
126 | COMMON/LEDWEIGHT/WEIF,WEI,WEIN,ITEST,IRANPOS | |
127 | ||
128 | C------------------------------------------------------------------ | |
129 | c write(*,*)'in fsiw C1 C2 CN',C1,C2,CN | |
130 | ||
131 | C==> AC1,2 = "relativistic" Bohr radii for particle-nucleus systems | |
132 | ||
133 | C1N=C1*CN | |
134 | IF(C1N.NE.0.D0)AC1=137.036D0/(C1N*E1) !m1-->E1 | |
135 | C2N=C2*CN | |
136 | IF(C2N.NE.0.D0)AC2=137.036D0/(C2N*E2) !m2-->E2 | |
137 | ||
138 | C----------------------------------------------------------- | |
139 | CALL FSIPN !(WEIF) !weight due to particle-nucleus FSI | |
140 | JRAT=0 | |
141 | CALL FSIWF !(WEI) !weight due to particle-particle-nucleus FSI | |
142 | WEIN=WEI | |
143 | IF(I3C*J.NE.0) THEN | |
144 | FF12=DCMPLX(1.D0,0.D0) | |
145 | FF21=DCMPLX(1.D0,0.D0) | |
146 | JRAT=1 | |
147 | CALL VZ !(WEIN) ! weight due to particle-particle FSI | |
148 | ENDIF | |
149 | RETURN | |
150 | END | |
151 | C======================================================================= | |
152 | ||
153 | SUBROUTINE LTRAN(P0,P,PS) | |
154 | C==>calculating particle 4-momentum PS={PSX,PSY,PSZ,ES} | |
155 | C in rest frame of a system 0 with 4-momentum P0={P0X,P0Y,P0Z,E0} | |
156 | C from its 4-momentum P={PX,PY,PZ,E} | |
157 | ||
158 | IMPLICIT REAL*8 (A-H,O-Z) | |
159 | DIMENSION P0(4),P(4),PS(4) | |
160 | C----------------------------------------------------------------------- | |
161 | P0S=P0(1)**2+P0(2)**2+P0(3)**2 | |
162 | AM0=DSQRT(P0(4)**2-P0S) | |
163 | EPM=P0(4)+AM0 | |
164 | PP0=P(1)*P0(1)+P(2)*P0(2)+P(3)*P0(3) | |
165 | H=(PP0/EPM-P(4))/AM0 | |
166 | PS(1)=P(1)+P0(1)*H | |
167 | PS(2)=P(2)+P0(2)*H | |
168 | PS(3)=P(3)+P0(3)*H | |
169 | PS(4)=(P0(4)*P(4)-PP0)/AM0 | |
170 | RETURN | |
171 | END | |
172 | ||
173 | SUBROUTINE LTRANB(P0,PS,P) | |
174 | C==>calculating particle 4-momentum P={PX,PY,PZ,E} | |
175 | C from its 4-momentum PS={PSX,PSY,PSZ,ES} | |
176 | C in rest frame of a system 0 with 4-momentum P0={P0X,P0Y,P0Z,E0} | |
177 | ||
178 | IMPLICIT REAL*8 (A-H,O-Z) | |
179 | DIMENSION P0(4),P(4),PS(4) | |
180 | C----------------------------------------------------------------------- | |
181 | P0S=P0(1)**2+P0(2)**2+P0(3)**2 | |
182 | AM0=DSQRT(P0(4)**2-P0S) | |
183 | EPM=P0(4)+AM0 | |
184 | PSP0=PS(1)*P0(1)+PS(2)*P0(2)+PS(3)*P0(3) | |
185 | HS=(PSP0/EPM+PS(4))/AM0 | |
186 | P(1)=PS(1)+P0(1)*HS | |
187 | P(2)=PS(2)+P0(2)*HS | |
188 | P(3)=PS(3)+P0(3)*HS | |
189 | P(4)=(P0(4)*PS(4)+PSP0)/AM0 | |
190 | RETURN | |
191 | END | |
192 | ||
193 | FUNCTION GND(X,J) | |
194 | C--- GND = k*COTG(DELTA), X=k^2 | |
195 | C--- J=1(2) corresp. to nd(pd), S=1/2, | |
196 | C--- J=3(4) corresp. to nd(pd), S=3/2 | |
197 | IMPLICIT REAL*8 (A-H,O-Z) | |
198 | COMMON/FSI_AAND/AAND(20,4) | |
199 | XX=X | |
200 | GND=1/AAND(1,J)+.5D0*AAND(2,J)*X | |
201 | DO 1 I=4,4 | |
202 | XX=XX*X | |
203 | 1 GND=GND+AAND(I,J)*XX | |
204 | GND=GND/(1+AAND(3,J)*X) | |
205 | RETURN | |
206 | END | |
207 | ||
208 | FUNCTION GDD(X,J) | |
209 | C--- GDD = k*COTG(DELTA), X=k^2 | |
210 | C--- J=1,2,3 corresp. to S=0,1,2 | |
211 | IMPLICIT REAL*8 (A-H,O-Z) | |
212 | COMMON/FSI_AADD/AADD(20,3) | |
213 | COMMON/FSI_C/C(10),AM,AMS,DM | |
214 | COMMON/FSI_CONS/PI,PI2,SPI,DR,W | |
215 | COMPLEX*16 C | |
216 | E=X/2/AM | |
217 | ER=DSQRT(E) | |
218 | IF(J.EQ.1)THEN | |
219 | GDD=ER*(AADD(1,1)*DEXP(-E/AADD(2,1))-AADD(3,1)) | |
220 | GDD=GDD/DR ! from degree to radian | |
221 | TAND=DTAN(GDD) | |
222 | IF(TAND.EQ.0.D0)TAND=1.D-10 | |
223 | GDD=DSQRT(X)/TAND | |
224 | END IF | |
225 | IF(J.EQ.2)THEN | |
226 | GDD=1.D10 | |
227 | END IF | |
228 | IF(J.EQ.3)THEN | |
229 | GDD=ER*(AADD(1,3)+AADD(2,3)*E) | |
230 | GDD=GDD/DR ! from degree to radian | |
231 | TAND=DTAN(GDD) | |
232 | IF(TAND.EQ.0.D0)TAND=1.D-10 | |
233 | GDD=DSQRT(X)/TAND | |
234 | END IF | |
235 | RETURN | |
236 | END | |
237 | ||
238 | ||
239 | SUBROUTINE CKKB ! calculates KK-b scattering amplitude, | |
240 | ! saturated by S*(980) and delta(982) resonances | |
241 | IMPLICIT REAL*8 (A-H,O-Z) | |
242 | COMMON/FSI_PRF/PPX,PPY,PPZ,AK,AKS, | |
243 | 1 X,Y,Z,T,RP,RPS | |
244 | COMMON/FSI_AAKK/AAKK(9) | |
245 | COMMON/FSI_C/C(10),AM,AMS,DM | |
246 | COMPLEX*16 C | |
247 | S4=AKS+AAKK(1) | |
248 | S=4*S4 | |
249 | AKPIPI=DSQRT(S4-AAKK(2)) | |
250 | EETA2=(S+AAKK(3)-AAKK(2))**2/4/S | |
251 | AKPIETA=DSQRT(EETA2-AAKK(3)) | |
252 | C(1)=AAKK(6)/2/DCMPLX(AAKK(4)-S, | |
253 | ,-AK*AAKK(6)-AKPIPI*AAKK(7)) | |
254 | C(1)=C(1)+AAKK(8)/2/DCMPLX(AAKK(5)-S, | |
255 | ,-AK*AAKK(8)-AKPIETA*AAKK(9)) | |
256 | RETURN | |
257 | END | |
258 | ||
259 | SUBROUTINE VZ !(WEI) | |
260 | C==> Calculates the weight WEI due to FSI | |
261 | IMPLICIT REAL*8 (A-H,O-Z) | |
262 | COMMON/FSI_JR/JRAT | |
263 | COMMON/FSI_PRF/PPX,PPY,PPZ,AK,AKS, | |
264 | 1 X,Y,Z,T,RP,RPS | |
265 | COMMON/FSI_SPIN/RHO(10) | |
266 | COMMON/FSI_ETA/ETA | |
267 | COMMON/FSI_AA/AA | |
268 | COMMON/FSI_FFF/F12,F21 | |
269 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
270 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
271 | COMMON/FSI_FD/FD(10),RD(10) | |
272 | COMMON/FSI_RR/F(10) | |
273 | COMMON/FSI_C/C(10),AM,AMS,DM | |
274 | COMMON/FSI_COULPH/EIDC | |
275 | COMMON/LEDWEIGHT/WEIF,WEI,WEIN,ITEST,IRANPOS | |
276 | COMPLEX*16 F,C,G,PSI12,PSI21 | |
277 | COMPLEX*16 F12,F21 | |
278 | COMPLEX*16 EIDC | |
279 | COMPLEX*8 Z8,CGAMMA | |
280 | COMMON/FSI_FFPN/FF12,FF21 | |
281 | COMPLEX*16 FF12,FF21 | |
282 | c--mlv------------------------------------------------------ | |
283 | c write(*,*)'------- WE are in VZ-----------' | |
284 | c write(*,*)'JRAT=', JRAT | |
285 | c write(*,*)'AK=', AK,'RP=',RP | |
286 | c write(*,*)'X Y Z', X,Y,Z | |
287 | c write(*,*)'PPX PPY PPZ',PPX,PPY,PPZ | |
288 | c write(*,*)'ETA',ETA | |
289 | c write(*,*)'MSPIN',MSPIN | |
290 | c write(*,*)'ISI',ISI | |
291 | c write(*,*)'RP RPS',RP,RPS | |
292 | c write(*,*)'AA- BEFORE FIRT------',AA | |
293 | c write(*,*)'IQS',IQS | |
294 | c write(*,*)'ICH',ICH | |
295 | c write(*,*)'MSPIN',MSPIN | |
296 | c write(*,*)'C',(C(I),I=1,MSPIN) | |
297 | c write(*,*)'ACHR',ACHR | |
298 | c write(*,*)'F12',F12,'F21',F21,'FF12',FF12,'FF21',FF21 | |
299 | ||
300 | c--mlv------------------------------------------------------ | |
301 | WEI=0.D0 | |
302 | IF(JRAT.EQ.1)GOTO 11 | |
303 | RHOS=AK*RP | |
304 | HS=X*PPX+Y*PPY+Z*PPZ | |
305 | c write(*,*)'rhos',rhos,'hs',hs | |
306 | IF(RHOS.LT.15.D0.AND.RHOS+DABS(HS).LT.20.D0)GOTO 2 | |
307 | C---Calc. EIDC=exp(i*Coul.Ph.); | |
308 | C-- used in calc. of hypergeom. f-s in SEQA, FAS at k*R > 15, 20 | |
309 | c write(*,*)'1111' | |
310 | Z8=CMPLX(1.,SNGL(ETA)) | |
311 | Z8=CGAMMA(Z8) | |
312 | EIDC=Z8/CABS(Z8) | |
313 | c write(*,*)'1111 z8 eidc',z8,eidc | |
314 | ||
315 | 2 CALL FF(RHOS,HS) | |
316 | 11 MSP=MSPIN | |
317 | ||
318 | c write(*,*)'before go to 4', wei | |
319 | ||
320 | IF(ISI.EQ.0)GOTO 4 ! the strong interaction ON (OFF) if ISI=1(0) | |
321 | IF(RP.LT.AA)GOTO 4 | |
322 | IF(JRAT.NE.1) CALL FIRT | |
323 | IF(IQS.EQ.0)GOTO 5 ! the quantum statistics ON (OFF) if IQS=1(0) | |
324 | JSIGN=-1 | |
325 | DO 1 JJ=1,MSP | |
326 | JSIGN=-JSIGN | |
327 | G=F(JJ)*C(JJ) | |
328 | IF(ICH.EQ.1)G=G*ACHR | |
329 | PSI12=FF12*(F12+G) | |
330 | PSI21=FF21*(F21+G) | |
331 | G=PSI12+JSIGN*PSI21 | |
332 | 1 WEI=WEI+RHO(JJ)*(DREAL(G)**2+DIMAG(G)**2) | |
333 | ||
334 | c WRITE(*,*)'WEI111=',WEI | |
335 | ||
336 | GOTO 8 | |
337 | 5 DO 6 JJ=1,MSP | |
338 | G=F(JJ)*C(JJ) | |
339 | IF(ICH.EQ.1)G=G*ACHR | |
340 | CW WRITE(6,38)'JJ ',JJ,'F ',DREAL(F(JJ)),DIMAG(F(JJ)) | |
341 | CW WRITE(6,38)'JJ ',JJ,'C ',DREAL(C(JJ)),DIMAG(C(JJ)) | |
342 | CW WRITE(6,38)'JJ ',JJ,'G ',DREAL(G),DIMAG(G) | |
343 | CW WRITE(6,38)'JJ ',JJ,'F12+G ',DREAL(F12+G),DIMAG(F12+G) | |
344 | CW WRITE(6,38)'JJ ',JJ,'F21+G ',DREAL(F21+G),DIMAG(F21+G) | |
345 | 38 FORMAT(A7,I3,A7,2E11.4) | |
346 | PSI12=FF12*(F12+G) | |
347 | 6 WEI=WEI+RHO(JJ)*(DREAL(PSI12)**2+DIMAG(PSI12)**2) | |
348 | RETURN | |
349 | ||
350 | c write(*,*)'before 4 wei',wei | |
351 | 4 PSI12=FF12*F12 | |
352 | IF(IQS.EQ.0)GOTO 50 ! the quantum statistics ON (OFF) if IQS=1(0) | |
353 | PSI21=FF21*F21 | |
354 | JSIGN=-1 | |
355 | DO 3 JJ=1,MSP | |
356 | JSIGN=-JSIGN | |
357 | G=PSI12+JSIGN*PSI21 | |
358 | c write(*,*)'msp jsign psi12 psi21',msp,jsign,psi12,psi21 | |
359 | 3 WEI=WEI+RHO(JJ)*(DREAL(G)**2+DIMAG(G)**2) | |
360 | c write(*,*)'wei rho(1)G dreal(G) dimag(G)',wei,rho(1),G, | |
361 | c + dreal(G),dimag(G) | |
362 | GOTO 8 | |
363 | ||
364 | 50 WEI=DREAL(PSI12)**2+DIMAG(PSI12)**2 | |
365 | c write(*,*)'WEI ---in VZ 50 before returne', WEI | |
366 | RETURN | |
367 | 8 WEI=WEI/2 | |
368 | c write(*,*)'WEI ---in VZ 8 before returne and END', WEI | |
369 | RETURN | |
370 | END | |
371 | ||
372 | SUBROUTINE FIRT | |
373 | C---CALC. THE F(JJ) | |
374 | C-- F(JJ)*C(JJ)= DEVIATION OF THE BETHE-SALPETER AMPL. FROM PLANE WAVE | |
375 | IMPLICIT REAL*8 (A-H,O-Z) | |
376 | COMMON/FSI_PRF/PPX,PPY,PPZ,AK,AKS, | |
377 | 1 X,Y,Z,T,RP,RPS | |
378 | COMMON/FSI_SHH/SH,CHH | |
379 | COMMON/FSI_BP/B,P | |
380 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
381 | COMMON/FSI_C/C(10),AM,AMS,DM | |
382 | COMMON/FSI_SW/RB(10),EB(10),BK(10),CDK(10),SDK(10), | |
383 | 1 SBKRB(10),SDKK(10) | |
384 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
385 | COMMON/FSI_RR/F(10) | |
386 | EQUIVALENCE(RSS,RP),(TSS,T) | |
387 | COMPLEX*16 F,C,CH1 | |
388 | MSP=MSPIN | |
389 | DO 10 JJ=1,MSP | |
390 | IF(JJ.GT.1)GOTO 3 | |
391 | XRA=2*RSS/AC | |
392 | IF(AK.NE.0.D0)GOTO2 | |
393 | SHK=1.D0 | |
394 | SH=.0D0 | |
395 | SHH=SH | |
396 | CHH=1/RSS | |
397 | GOTO3 | |
398 | 2 H=AK*RSS | |
399 | CALL GST(XRA,H) | |
400 | SH=SH/RSS | |
401 | CHH=CHH/RSS | |
402 | SHH=SH | |
403 | IF(ICH.EQ.1) SHH=ACH*SH | |
404 | 3 IF(NS.EQ.2)GOTO1 | |
405 | C---F= ASYMPTOTIC FORMULA (T= 0 APPROX.); NS= 4 | |
406 | 6 F(JJ)=DCMPLX(CHH,SHH) | |
407 | IF(NS.NE.1)GOTO 10 | |
408 | C---F INSIDE THE SQUARE-WELL (T= 0 APPROX.); NS= 1 | |
409 | IF(RSS.GE.RB(JJ)) GOTO 10 | |
410 | IF(AK.NE.0.D0.AND.JJ.EQ.1)SHK=SH/AK | |
411 | H=BK(JJ)*RSS | |
412 | CALL GST(XRA,H) | |
413 | SKR=B*BK(JJ) | |
414 | F(JJ)=DCMPLX(CDK(JJ),SDK(JJ))*SKR | |
415 | CH1=(SDKK(JJ)*SKR-SHK*SBKRB(JJ))/C(JJ) | |
416 | F(JJ)=(F(JJ)+CH1)/SBKRB(JJ) | |
417 | GOTO 10 | |
418 | 1 CONTINUE | |
419 | C---F= ASYMPTOTIC FORMULA (T= 0 NOT REQUIRED); NS= 2 | |
420 | IF(JJ.GT.1)GOTO 8 | |
421 | IF(TSS.EQ.0.D0)GOTO6 | |
422 | TSSA=DABS(TSS) | |
423 | IF(DM.NE.0.D0)GOTO 11 | |
424 | H=AM*.5D0/TSSA | |
425 | IF(AK.NE.0.D0)GOTO4 | |
426 | HM=H*RPS | |
427 | IF(HM.GE.3.D15)GOTO6 | |
428 | ||
429 | FS1=DFRSIN(HM) | |
430 | FC1=DFRCOS(HM) | |
431 | ||
432 | FC2=FC1 | |
433 | FS2=FS1 | |
434 | GOTO5 | |
435 | 4 CONTINUE | |
436 | H1=AK*TSSA/AM | |
437 | HM=H*(RSS-H1)**2 | |
438 | HP=H*(RSS+H1)**2 | |
439 | IF(HP.GE.3.D15)GOTO6 | |
440 | ||
441 | FS1=DFRSIN(HM) | |
442 | FC1=DFRCOS(HM) | |
443 | FS2=DFRSIN(HP) | |
444 | FC2=DFRCOS(HP) | |
445 | ||
446 | GOTO 5 | |
447 | 11 CONTINUE | |
448 | FS1=0.D0 | |
449 | FS2=0.D0 | |
450 | FC1=0.D0 | |
451 | FC2=0.D0 | |
452 | DO 13 I=1,2 | |
453 | IF(I.EQ.1)TSSH=TSSA*(1+DM) | |
454 | IF(I.EQ.2)TSSH=TSSA*(1-DM) | |
455 | H=AM*.5D0/TSSH | |
456 | IF(AK.NE.0.D0)GOTO 12 | |
457 | HM=H*RPS | |
458 | IF(HM.GE.3.D15)GOTO6 | |
459 | ||
460 | FS1=FS1+DFRSIN(HM)/2 | |
461 | FC1=FC1+DFRCOS(HM)/2 | |
462 | ||
463 | IF(I.EQ.1)GOTO 13 | |
464 | FC2=FC1 | |
465 | FS2=FS1 | |
466 | GOTO 13 | |
467 | 12 CONTINUE | |
468 | H1=AK*TSSH/AM | |
469 | HM=H*(RSS-H1)**2 | |
470 | HP=H*(RSS+H1)**2 | |
471 | IF(HP.GE.3.D15)GOTO6 | |
472 | ||
473 | FS1=FS1+DFRSIN(HM)/2 | |
474 | FC1=FC1+DFRCOS(HM)/2 | |
475 | FS2=FS2+DFRSIN(HP)/2 | |
476 | FC2=FC2+DFRCOS(HP)/2 | |
477 | ||
478 | 13 CONTINUE | |
479 | 5 C12=FC1+FS2 | |
480 | S12=FS1+FC2 | |
481 | A12=FS1-FC2 | |
482 | A21=FS2-FC1 | |
483 | A2=.5D0*(CHH*(A12+A21)+SH*(A12-A21))+SHH | |
484 | A1=.5D0*(CHH*(C12+S12)+SH*(C12-S12)) | |
485 | F(JJ)=.3989422D0*DCMPLX(A1,A2) | |
486 | GOTO 10 | |
487 | 8 F(JJ)=F(1) | |
488 | 10 CONTINUE | |
489 | RETURN | |
490 | END | |
491 | ||
492 | FUNCTION EXF(X) | |
493 | IMPLICIT REAL*8 (A-H,O-Z) | |
494 | IF(X.LT.-15.D0) GO TO 1 | |
495 | EXF=DEXP(X) | |
496 | RETURN | |
497 | 1 EXF=.0D0 | |
498 | RETURN | |
499 | END | |
500 | ||
501 | SUBROUTINE SEQ(X,H) | |
502 | C---CALC. FUNCTIONS B, P (EQS. (17) OF G-K-L-L); | |
503 | C-- NEEDED TO CALC. THE CONFLUENT HYPERGEOMETRIC FUNCTION GST. | |
504 | IMPLICIT REAL*8 (A-H,O-Z) | |
505 | COMMON/FSI_BP/B,P | |
506 | DIMENSION BH(3),PH(3) | |
507 | DATA ERR/1.D-7/ | |
508 | BH(1)=1.D0 | |
509 | PH(1)=1.D0 | |
510 | PH(2)=.0D0 | |
511 | BH(2)=.5D0*X | |
512 | B=1+BH(2) | |
513 | P=1.D0 | |
514 | HS=H*H | |
515 | J=0 | |
516 | 2 J=J+1 | |
517 | BH(3)=(X*BH(2)-HS*BH(1))/((J+1)*(J+2)) | |
518 | PH(3)=(X*PH(2)-HS*PH(1)-(2*J+1)*X*BH(2))/(J*(J+1)) | |
519 | B=B+BH(3) | |
520 | P=P+PH(3) | |
521 | Z=DABS(BH(2))+DABS(BH(3))+DABS(PH(2))+DABS(PH(3)) | |
522 | IF(Z.LT.ERR)RETURN | |
523 | BH(1)=BH(2) | |
524 | BH(2)=BH(3) | |
525 | PH(1)=PH(2) | |
526 | PH(2)=PH(3) | |
527 | GOTO 2 | |
528 | END | |
529 | ||
530 | SUBROUTINE SEQA(X,H) | |
531 | C---CALC. FUNCTIONS CHH=REAL(GST), SH=IMAG(GST)/ACH, B=SH/H | |
532 | C-- IN THE ASYMPTOTIC REGION H=K*R >> 1. | |
533 | IMPLICIT REAL*8 (A-H,O-Z) | |
534 | COMMON/FSI_BP/B,P | |
535 | COMMON/FSI_SHH/SH,CHH | |
536 | COMMON/FSI_ETA/ETA | |
537 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
538 | COMMON/FSI_COULPH/EIDC | |
539 | COMPLEX*16 EIDC,GST | |
540 | ARG=H-ETA*DLOG(2*H) | |
541 | GST=DCMPLX(DCOS(ARG),DSIN(ARG)) | |
542 | GST=ACHR*EIDC*GST | |
543 | CHH=DREAL(GST) | |
544 | SH=DIMAG(GST)/ACH | |
545 | B=SH/H | |
546 | RETURN | |
547 | END | |
548 | ||
549 | SUBROUTINE FF(RHO,H) | |
550 | C---Calc. F12, F21; | |
551 | C-- F12= FF0* plane wave, FF0=F*ACHR, | |
552 | C---F is the confluent hypergeometric function, | |
553 | C-- ACHR=sqrt(ACH), where ACH is the Coulomb factor | |
554 | IMPLICIT REAL*8 (A-H,O-Z) | |
555 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
556 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
557 | COMMON/FSI_ETA/ETA | |
558 | COMMON/FSI_FFF/F12,F21 | |
559 | COMPLEX*16 FF0,F12,F21 | |
560 | C=DCOS(H) | |
561 | S=DSIN(H) | |
562 | F12=DCMPLX(C,-S) | |
563 | F21=DCMPLX(C,S) | |
564 | IF(ICH.EQ.0)RETURN | |
565 | RHOP=RHO+H | |
566 | RHOM=RHO-H | |
567 | F12=FF0(RHO,H)*F12 | |
568 | F21=FF0(RHO,-H)*F21 | |
569 | RETURN | |
570 | END | |
571 | ||
572 | FUNCTION FAS(RKS) | |
573 | C-- FAS=F*ACHR | |
574 | C---F is the confluent hypergeometric function at k*r >> 1 | |
575 | C-- ACHR=sqrt(ACH), where ACH is the Coulomb factor | |
576 | IMPLICIT REAL*8 (A-H,O-Z) | |
577 | COMPLEX*16 FAS,EIDC,ZZ1 | |
578 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
579 | COMMON/FSI_ETA/ETA | |
580 | COMMON/FSI_COULPH/EIDC | |
581 | D1=DLOG(RKS)*ETA | |
582 | D2=ETA*ETA/RKS | |
583 | ZZ1=DCMPLX(DCOS(D1),DSIN(D1))/EIDC | |
584 | FAS=DCMPLX(1.D0,-D2)*ZZ1 | |
585 | FAS=FAS-DCMPLX(DCOS(RKS),DSIN(RKS))*ETA/RKS/ZZ1 | |
586 | RETURN | |
587 | END | |
588 | ||
589 | FUNCTION FF0(RHO,H) | |
590 | C-- FF0=F*ACHR | |
591 | C-- F is the confluent hypergeometric function | |
592 | C-- (Eq. (15) of G-K-L-L), F= 1 at r* << AC | |
593 | C-- ACHR=sqrt(ACH), where ACH is the Coulomb factor | |
594 | IMPLICIT REAL*8 (A-H,O-Z) | |
595 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
596 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
597 | COMMON/FSI_ETA/ETA | |
598 | COMPLEX*16 ALF,ALF1,Z,S,A,FF0,FAS | |
599 | DATA ERR/1.D-5/ | |
600 | S=DCMPLX(1.D0,0.D0) | |
601 | FF0=S | |
602 | RHOP=RHO+H | |
603 | CC GOTO 5 ! rejects the approx. calcul. of hyperg. f-ion F | |
604 | IF(RHOP.LT.20.D0)GOTO5 | |
605 | FF0=FAS(RHOP) ! approx. calc. | |
606 | RETURN | |
607 | 5 ALF=DCMPLX(.0D0,-ETA) | |
608 | ALF1=ALF-1 | |
609 | Z=DCMPLX(.0D0,RHOP) | |
610 | J=0 | |
611 | 3 J=J+1 | |
612 | A=(ALF1+J)/(J*J) | |
613 | S=S*A*Z | |
614 | FF0=FF0+S | |
615 | ZR=DABS(DREAL(S)) | |
616 | ZI=DABS(DIMAG(S)) | |
617 | IF((ZR+ZI).GT.ERR)GOTO3 | |
618 | FF0=FF0*ACHR | |
619 | RETURN | |
620 | END | |
621 | ||
622 | FUNCTION HC(XA) | |
623 | C---HC = h-function of Landau-Lifshitz: h(x)=Re[psi(1-i/x)]+ln(x) | |
624 | C-- psi(x) is the digamma function (the logarithmic derivative of | |
625 | C-- the gamma function) | |
626 | IMPLICIT REAL*8 (A-H,O-Z) | |
627 | DIMENSION BN(15) | |
628 | DATA BN/.8333333333D-1,.8333333333D-2,.396825396825D-2, | |
629 | 1 .4166666667D-2,.7575757576D-2,.2109279609D-1, | |
630 | 2 .8333333333D-1,.4432598039D0 ,.305395433D1, | |
631 | 3 .2645621212D2, .2814601449D3, .3607510546D4, | |
632 | 4 .5482758333D5, .9749368235D6, .200526958D8/ | |
633 | X=DABS(XA) | |
634 | IF(X.LT..33D0) GOTO 1 | |
635 | CC IF(X.GE.3.5D0) GO TO 2 | |
636 | S=.0D0 | |
637 | N=0 | |
638 | 3 N=N+1 | |
639 | DS=1.D0/N/((N*X)**2+1) | |
640 | S=S+DS | |
641 | IF(DS.GT.0.1D-12) GOTO 3 | |
642 | C---Provides 7 digit accuracy | |
643 | HC=S-.5772156649D0+DLOG(X) | |
644 | RETURN | |
645 | CC 2 HC=1.2D0/X**2+DLOG(X)-.5772156649 D0 | |
646 | CC RETURN | |
647 | 1 X2=X*X | |
648 | XP=X2 | |
649 | HC=0.D0 | |
650 | IMA=9 | |
651 | IF(X.LT.0.1D0)IMA=3 | |
652 | DO 4 I=1,IMA | |
653 | HC=HC+XP*BN(I) | |
654 | 4 XP=X2*XP | |
655 | RETURN | |
656 | END | |
657 | ||
658 | FUNCTION ACP(X) | |
659 | C--- ACP = COULOMB PENETRATION FACTOR | |
660 | IMPLICIT REAL*8 (A-H,O-Z) | |
661 | IF(X.LT.0.05D0.AND.X.GE.0.D0) GO TO 1 | |
662 | Y=6.2831853D0/X | |
663 | ACP=Y/(EXF(Y)-1) | |
664 | RETURN | |
665 | 1 ACP=1.D-6 | |
666 | RETURN | |
667 | END | |
668 | ||
669 | SUBROUTINE GST(X,H) | |
670 | C---CALC. THE CONFL. HYPERGEOM. F-N = CHH+i*SH | |
671 | C-- AND THE COULOMB F-S B, P (CALLS SEQ OR SEQA). | |
672 | IMPLICIT REAL*8 (A-H,O-Z) | |
673 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
674 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
675 | COMMON/FSI_SHH/SH,CHH | |
676 | COMMON/FSI_BP/B,P | |
677 | 1 IF(ICH.EQ.1)GOTO 2 | |
678 | 3 SH=DSIN(H) | |
679 | CHH=DCOS(H) | |
680 | B=1.D0 | |
681 | IF(H.NE.0.D0)B=SH/H | |
682 | P=CHH | |
683 | RETURN | |
684 | 2 CONTINUE | |
685 | IF(H.GT.15.D0)GOTO4 ! comment out if you want to reject | |
686 | ! the approximate calculation of hyperg. f-ion G | |
687 | CALL SEQ(X,H) ! exact calculation | |
688 | SH=H*B | |
689 | CHH=P+B*X*(DLOG(DABS(X))+HPR) | |
690 | RETURN | |
691 | 4 CALL SEQA(X,H) | |
692 | RETURN | |
693 | END | |
694 | ||
695 | FUNCTION FF1(RHO,H) | |
696 | C---FF1=FF0; used for particle-nucleus system | |
697 | C-- FF0=F12*ACHR | |
698 | C-- F12 is the confluent hypergeometric function | |
699 | C-- (Eq. (15) of G-K-L-L), F12= 1 at r* << AC | |
700 | C-- ACHR=sqrt(ACH), where ACH is the Coulomb factor | |
701 | IMPLICIT REAL*8 (A-H,O-Z) | |
702 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
703 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
704 | COMMON/FSI_ETA/ETA | |
705 | COMMON/FSI_COULPH/EIDC | |
706 | COMMON/FSI_ICH1/ICH1 | |
707 | COMPLEX*16 FF0,FF1 | |
708 | COMPLEX*16 EIDC | |
709 | COMPLEX*8 Z8,CGAMMA | |
710 | FF1=DCMPLX(1.D0,0.D0) | |
711 | IF(ICH1.EQ.0)GOTO 2 | |
712 | IF(RHO.LT.15.D0.AND.RHO+H.LT.20.D0)GOTO 2 | |
713 | C---Calc. EIDC=exp(i*Coul.Ph.); | |
714 | C-- used in calc. of hypergeom. f-s in SEQA, FAS at k*R > 15, 20 | |
715 | ||
716 | Z8=CMPLX(1.,SNGL(ETA)) | |
717 | Z8=CGAMMA(Z8) | |
718 | ||
719 | EIDC=Z8/CABS(Z8) | |
720 | ||
721 | 2 FF1=FF0(RHO,H) | |
722 | RETURN | |
723 | END | |
724 | ||
725 | FUNCTION G(AK) | |
726 | C---Used to calculate SW scattering amplitude for alpa-alpha system | |
727 | C-- and for sear.f (square well potential search) | |
728 | C---NOTE THAT SCATT. AMPL.= 1/CMPLX(G(AK),-AK*ACH) | |
729 | IMPLICIT REAL*8 (A-H,O-Z) | |
730 | COMMON/FSI_SW/RB(10),EB(10),BK(10),CDK(10),SDK(10), | |
731 | 1 SBKRB(10),SDKK(10) | |
732 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
733 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,JJ,MSPIN | |
734 | COMMON/FSI_BP/B,P/FSI_DERIV/BPR,PPR/FSI_SHH/SH,CHH | |
735 | COMMON/FSI_DAK/DAK,HAC,IFUN | |
736 | HAC=.0D0 | |
737 | IF(ICH.EQ.0)GOTO 1 | |
738 | XH=AC*AK | |
739 | HCP=HC(XH) | |
740 | HPR=HCP+.1544313298D0 | |
741 | ACH=ACP(XH) | |
742 | HAC=2*HCP/AC | |
743 | 1 AKS=AK**2 | |
744 | BK(JJ)=DSQRT(AKS+EB(JJ)**2) ! kappa=kp | |
745 | X=2*RB(JJ)/AC | |
746 | H=BK(JJ)*RB(JJ) ! kp*d | |
747 | CALL GST(X,H) | |
748 | BRHO=B ! B(kp,d) | |
749 | SBKRB(JJ)=SH ! kp*d*B(kp,d) | |
750 | CALL DERIW(X,H) | |
751 | BRHOP=BPR ! B'(kp,d)= dB(kp,r)/dln(r) at r=d | |
752 | H=AK*RB(JJ) | |
753 | CALL GST(X,H) | |
754 | CDK(JJ)=CHH ! ReG(k,d) | |
755 | BRHOS=B ! B(k,d) | |
756 | PRHOS=P ! P(k,d) | |
757 | SDK(JJ)=SH | |
758 | IF(ICH.EQ.0)GOTO 2 | |
759 | SDK(JJ)=ACH*SH ! ImG(k,d) | |
760 | IF(AK.EQ.0.D0.AND.AC.LT.0.D0)SDK(JJ)=3.14159*X*B | |
761 | 2 SDKK(JJ)=RB(JJ) | |
762 | IF(AK.NE.0.D0)SDKK(JJ)=SH/AK ! d*B(k,d) | |
763 | CALL DERIW(X,H) ! PPR=P'(k,d)= dP(k,r)/dln(r) at r=d | |
764 | ZZ=PPR-PRHOS | |
765 | IF(ICH.EQ.1)ZZ=ZZ+X*(BRHOS+BPR*(DLOG(DABS(X))+HPR)) | |
766 | C ZZ= P'(k,d)-P(k,d)+x*{B(k,d)+B'(k,d)*[ln!x!+2*C-1+h(k*ac)]} | |
767 | GG=(BRHOP*CDK(JJ)-BRHO*ZZ)/RB(JJ) | |
768 | C GG= [B'(kp,d)*ReG(k,d)-B(kp,d)*ZZ]/d | |
769 | G=GG/(BRHO*BPR-BRHOP*BRHOS) | |
770 | C G= GG/[B(kp,d)*B'(k,d)-B'(kp,d)*B(k,d)] | |
771 | RETURN | |
772 | END | |
773 | ||
774 | SUBROUTINE DERIW(X,H) | |
775 | C---CALLED BY F-N G(AK) | |
776 | IMPLICIT REAL*8 (A-H,O-Z) | |
777 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
778 | COMMON/FSI_BP/B,P/FSI_DERIV/BPR,PPR | |
779 | HH=.1D-3 | |
780 | CALL GST(X,H-HH) | |
781 | Q1=P | |
782 | B1=B | |
783 | CALL GST(X,H+HH) | |
784 | HHH=HH+HH | |
785 | BPR=H*(B-B1)/HHH | |
786 | PPR=H*(P-Q1)/HHH | |
787 | IF(ICH.EQ.0)RETURN | |
788 | CALL GST(X-HH,H) | |
789 | Q1=P | |
790 | B1=B | |
791 | CALL GST(X+HH,H) | |
792 | BPR=BPR+X*(B-B1)/HHH | |
793 | PPR=PPR+X*(P-Q1)/HHH | |
794 | RETURN | |
795 | END | |
796 | ||
797 | c-------------#include "gen/pilot.h" | |
798 | FUNCTION DFRSIN(X) | |
148aadde | 799 | IMPLICIT DOUBLE PRECISION (A-H,O-Z) |
f5ab1a71 | 800 | |
801 | DIMENSION A(0:16),B(0:15),C1(0:25),C2(0:28) | |
f5ab1a71 | 802 | PARAMETER (Z1 = 1, R8 = Z1/8, R32 = Z1/32) |
f5ab1a71 | 803 | DATA C0 /1.25331 41373 15500 3D0/ |
f5ab1a71 | 804 | DATA NA,NB,NC1,NC2 /16,15,25,28/ |
f5ab1a71 | 805 | DATA A( 0) / 0.76435 13866 41860 002D0/ |
806 | DATA A( 1) /-0.43135 54754 76601 793D0/ | |
807 | DATA A( 2) / 0.43288 19997 97266 531D0/ | |
808 | DATA A( 3) /-0.26973 31033 83871 110D0/ | |
809 | DATA A( 4) / 0.08416 04532 08769 354D0/ | |
810 | DATA A( 5) /-0.01546 52448 44613 820D0/ | |
811 | DATA A( 6) / 0.00187 85542 34398 220D0/ | |
812 | DATA A( 7) /-0.00016 26497 76188 875D0/ | |
813 | DATA A( 8) / 0.00001 05739 76563 833D0/ | |
814 | DATA A( 9) /-0.00000 05360 93398 892D0/ | |
815 | DATA A(10) / 0.00000 00218 16584 549D0/ | |
816 | DATA A(11) /-0.00000 00007 29016 212D0/ | |
817 | DATA A(12) / 0.00000 00000 20373 325D0/ | |
818 | DATA A(13) /-0.00000 00000 00483 440D0/ | |
819 | DATA A(14) / 0.00000 00000 00009 865D0/ | |
820 | DATA A(15) /-0.00000 00000 00000 175D0/ | |
821 | DATA A(16) / 0.00000 00000 00000 003D0/ | |
822 | ||
823 | DATA B( 0) / 0.63041 40431 45705 392D0/ | |
824 | DATA B( 1) /-0.42344 51140 57053 335D0/ | |
825 | DATA B( 2) / 0.37617 17264 33436 566D0/ | |
826 | DATA B( 3) /-0.16249 48915 45095 674D0/ | |
827 | DATA B( 4) / 0.03822 25577 86330 087D0/ | |
828 | DATA B( 5) /-0.00564 56347 71321 909D0/ | |
829 | DATA B( 6) / 0.00057 45495 19768 974D0/ | |
830 | DATA B( 7) /-0.00004 28707 15321 020D0/ | |
831 | DATA B( 8) / 0.00000 24512 07499 233D0/ | |
832 | DATA B( 9) /-0.00000 01109 88418 409D0/ | |
833 | DATA B(10) / 0.00000 00040 82497 317D0/ | |
834 | DATA B(11) /-0.00000 00001 24498 302D0/ | |
835 | DATA B(12) / 0.00000 00000 03200 484D0/ | |
836 | DATA B(13) /-0.00000 00000 00070 324D0/ | |
837 | DATA B(14) / 0.00000 00000 00001 336D0/ | |
838 | DATA B(15) /-0.00000 00000 00000 022D0/ | |
839 | ||
840 | DATA C1( 0) / 0.99056 04793 73497 549D0/ | |
841 | DATA C1( 1) /-0.01218 35098 31478 997D0/ | |
842 | DATA C1( 2) /-0.00248 27428 23113 060D0/ | |
843 | DATA C1( 3) / 0.00026 60949 52647 247D0/ | |
844 | DATA C1( 4) /-0.00000 10790 68987 406D0/ | |
845 | DATA C1( 5) /-0.00000 48836 81753 933D0/ | |
846 | DATA C1( 6) / 0.00000 09990 55266 368D0/ | |
847 | DATA C1( 7) /-0.00000 00750 92717 372D0/ | |
848 | DATA C1( 8) /-0.00000 00190 79487 573D0/ | |
849 | DATA C1( 9) / 0.00000 00090 90797 293D0/ | |
850 | DATA C1(10) /-0.00000 00019 66236 033D0/ | |
851 | DATA C1(11) / 0.00000 00001 64772 911D0/ | |
852 | DATA C1(12) / 0.00000 00000 63079 714D0/ | |
853 | DATA C1(13) /-0.00000 00000 36432 219D0/ | |
854 | DATA C1(14) / 0.00000 00000 10536 930D0/ | |
855 | DATA C1(15) /-0.00000 00000 01716 438D0/ | |
856 | DATA C1(16) /-0.00000 00000 00107 124D0/ | |
857 | DATA C1(17) / 0.00000 00000 00204 099D0/ | |
858 | DATA C1(18) /-0.00000 00000 00090 064D0/ | |
859 | DATA C1(19) / 0.00000 00000 00025 506D0/ | |
860 | DATA C1(20) /-0.00000 00000 00004 036D0/ | |
861 | DATA C1(21) /-0.00000 00000 00000 570D0/ | |
862 | DATA C1(22) / 0.00000 00000 00000 762D0/ | |
863 | DATA C1(23) /-0.00000 00000 00000 363D0/ | |
864 | DATA C1(24) / 0.00000 00000 00000 118D0/ | |
865 | DATA C1(25) /-0.00000 00000 00000 025D0/ | |
866 | ||
867 | DATA C2( 0) / 0.04655 77987 37516 4561D0/ | |
868 | DATA C2( 1) / 0.04499 21302 01239 4140D0/ | |
869 | DATA C2( 2) /-0.00175 42871 39651 4532D0/ | |
870 | DATA C2( 3) /-0.00014 65340 02581 0678D0/ | |
871 | DATA C2( 4) / 0.00003 91330 40863 0159D0/ | |
872 | DATA C2( 5) /-0.00000 34932 28659 7731D0/ | |
873 | DATA C2( 6) /-0.00000 03153 53003 2345D0/ | |
874 | DATA C2( 7) / 0.00000 01876 58200 8529D0/ | |
875 | DATA C2( 8) /-0.00000 00377 55280 4930D0/ | |
876 | DATA C2( 9) / 0.00000 00026 65516 5010D0/ | |
877 | DATA C2(10) / 0.00000 00010 88144 8122D0/ | |
878 | DATA C2(11) /-0.00000 00005 35500 7671D0/ | |
879 | DATA C2(12) / 0.00000 00001 31576 5447D0/ | |
880 | DATA C2(13) /-0.00000 00000 15286 0881D0/ | |
881 | DATA C2(14) /-0.00000 00000 03394 7646D0/ | |
882 | DATA C2(15) / 0.00000 00000 02702 0267D0/ | |
883 | DATA C2(16) /-0.00000 00000 00946 3142D0/ | |
884 | DATA C2(17) / 0.00000 00000 00207 1565D0/ | |
885 | DATA C2(18) /-0.00000 00000 00012 6931D0/ | |
886 | DATA C2(19) /-0.00000 00000 00013 9756D0/ | |
887 | DATA C2(20) / 0.00000 00000 00008 5929D0/ | |
888 | DATA C2(21) /-0.00000 00000 00003 1070D0/ | |
889 | DATA C2(22) / 0.00000 00000 00000 7515D0/ | |
890 | DATA C2(23) /-0.00000 00000 00000 0648D0/ | |
891 | DATA C2(24) /-0.00000 00000 00000 0522D0/ | |
892 | DATA C2(25) / 0.00000 00000 00000 0386D0/ | |
893 | DATA C2(26) /-0.00000 00000 00000 0165D0/ | |
894 | DATA C2(27) / 0.00000 00000 00000 0050D0/ | |
895 | DATA C2(28) /-0.00000 00000 00000 0009D0/ | |
896 | ||
897 | V=ABS(X) | |
898 | IF(V .LT. 8) THEN | |
899 | Y=R8*V | |
900 | H=2*Y**2-1 | |
901 | ALFA=H+H | |
902 | B1=0 | |
903 | B2=0 | |
904 | DO 4 I = NB,0,-1 | |
905 | B0=B(I)+ALFA*B1-B2 | |
906 | B2=B1 | |
907 | 4 B1=B0 | |
908 | H=SQRT(V)*Y*(B0-B2) | |
909 | ELSE | |
910 | R=1/V | |
911 | H=10*R-1 | |
912 | ALFA=H+H | |
913 | B1=0 | |
914 | B2=0 | |
915 | DO 5 I = NC1,0,-1 | |
916 | B0=C1(I)+ALFA*B1-B2 | |
917 | B2=B1 | |
918 | 5 B1=B0 | |
919 | S=B0-H*B2 | |
920 | B1=0 | |
921 | B2=0 | |
922 | DO 6 I = NC2,0,-1 | |
923 | B0=C2(I)+ALFA*B1-B2 | |
924 | B2=B1 | |
925 | 6 B1=B0 | |
926 | H=C0-SQRT(R)*(S*COS(V)+(B0-H*B2)*SIN(V)) | |
927 | END IF | |
928 | IF(X .LT. 0) H=-H | |
929 | GO TO 9 | |
930 | ||
931 | ENTRY DFRCOS(X) | |
932 | ||
933 | V=ABS(X) | |
934 | IF(V .LT. 8) THEN | |
935 | H=R32*V**2-1 | |
936 | ALFA=H+H | |
937 | B1=0 | |
938 | B2=0 | |
939 | DO 1 I = NA,0,-1 | |
940 | B0=A(I)+ALFA*B1-B2 | |
941 | B2=B1 | |
942 | 1 B1=B0 | |
943 | H=SQRT(V)*(B0-H*B2) | |
944 | ELSE | |
945 | R=1/V | |
946 | H=10*R-1 | |
947 | ALFA=H+H | |
948 | B1=0 | |
949 | B2=0 | |
950 | DO 2 I = NC1,0,-1 | |
951 | B0=C1(I)+ALFA*B1-B2 | |
952 | B2=B1 | |
953 | 2 B1=B0 | |
954 | S=B0-H*B2 | |
955 | B1=0 | |
956 | B2=0 | |
957 | DO 3 I = NC2,0,-1 | |
958 | B0=C2(I)+ALFA*B1-B2 | |
959 | B2=B1 | |
960 | 3 B1=B0 | |
961 | H=C0-SQRT(R)*((B0-H*B2)*COS(V)-S*SIN(V)) | |
962 | END IF | |
963 | IF(X .LT. 0) H=-H | |
964 | 9 DFRSIN=H | |
965 | RETURN | |
966 | END | |
967 | ||
968 | c--#include "gen/pilot.h" | |
148aadde | 969 | FUNCTION CGAMMA(Z) |
f5ab1a71 | 970 | |
971 | COMPLEX*8 CGAMMA | |
972 | COMPLEX*8 Z,U,V,F,H,S | |
973 | CHARACTER NAME*(*) | |
974 | CHARACTER*80 ERRTXT | |
975 | PARAMETER (NAME = 'CGAMMA') | |
f5ab1a71 | 976 | DIMENSION C(0:15) |
f5ab1a71 | 977 | PARAMETER (Z1 = 1, HF = Z1/2) |
978 | ||
979 | c--#if defined(CERNLIB_QF2C) | |
980 | c--#include "gen/gcmpfun.inc" | |
981 | c--#endif | |
982 | ||
983 | DATA PI /3.14159 26535 89793 24D0/ | |
984 | DATA C1 /2.50662 82746 31000 50D0/ | |
985 | ||
986 | DATA C( 0) / 41.62443 69164 39068D0/ | |
987 | DATA C( 1) /-51.22424 10223 74774D0/ | |
988 | DATA C( 2) / 11.33875 58134 88977D0/ | |
989 | DATA C( 3) / -0.74773 26877 72388D0/ | |
990 | DATA C( 4) / 0.00878 28774 93061D0/ | |
991 | DATA C( 5) / -0.00000 18990 30264D0/ | |
992 | DATA C( 6) / 0.00000 00019 46335D0/ | |
993 | DATA C( 7) / -0.00000 00001 99345D0/ | |
994 | DATA C( 8) / 0.00000 00000 08433D0/ | |
995 | DATA C( 9) / 0.00000 00000 01486D0/ | |
996 | DATA C(10) / -0.00000 00000 00806D0/ | |
997 | DATA C(11) / 0.00000 00000 00293D0/ | |
998 | DATA C(12) / -0.00000 00000 00102D0/ | |
999 | DATA C(13) / 0.00000 00000 00037D0/ | |
1000 | DATA C(14) / -0.00000 00000 00014D0/ | |
1001 | DATA C(15) / 0.00000 00000 00006D0/ | |
1002 | ||
1003 | c----#if !defined(CERNLIB_QF2C) | |
1004 | c----#include "gen/gcmpfun.inc" | |
1005 | c----#endif | |
1006 | ||
1007 | COMPLEX*8 GREAL,GIMAG,XARG,YARG | |
1008 | ||
1009 | COMPLEX*8 ZARG,GCONJG,GCMPLX | |
1010 | GREAL( ZARG)=REAL( ZARG) | |
1011 | GIMAG( ZARG)=AIMAG(ZARG) | |
1012 | GCONJG(ZARG)=CONJG(ZARG) | |
1013 | c-- GCMPLX(XARG,YARG)= CMPLX(XARG,YARG) | |
1014 | ||
1015 | U=Z | |
1016 | X=U | |
1017 | IF(GIMAG(U) .EQ. 0 .AND. -ABS(X) .EQ. INT(X)) THEN | |
1018 | F=0 | |
1019 | H=0 | |
1020 | WRITE(ERRTXT,101) X | |
1021 | c- CALL MTLPRT(NAME,'C305.1',ERRTXT) | |
1022 | ELSE | |
1023 | IF(X .GE. 1) THEN | |
1024 | F=1 | |
1025 | V=U | |
1026 | ELSEIF(X .GE. 0) THEN | |
1027 | F=1/U | |
1028 | V=1+U | |
1029 | ELSE | |
1030 | F=1 | |
1031 | V=1-U | |
1032 | END IF | |
1033 | H=1 | |
1034 | S=C(0) | |
1035 | DO 1 K = 1,15 | |
1036 | H=((V-K)/(V+(K-1)))*H | |
1037 | 1 S=S+C(K)*H | |
1038 | H=V+(4+HF) | |
1039 | H=C1*EXP((V-HF)*LOG(H)-H)*S | |
1040 | IF(X .LT. 0) H=PI/(SIN(PI*U)*H) | |
1041 | ENDIF | |
1042 | ||
1043 | c----#if !defined(CERNLIB_DOUBLE) | |
1044 | CGAMMA=F*H | |
1045 | c----#endif | |
1046 | ||
1047 | RETURN | |
1048 | 101 FORMAT('ARGUMENT EQUALS NON-POSITIVE INTEGER = ',1P,E15.1) | |
1049 | END | |
1050 | ||
1051 | ||
1052 | SUBROUTINE FSIPN !(WEIF) | |
1053 | C calculating particle-nucleus Coulomb Wave functions FFij | |
1054 | IMPLICIT REAL*8 (A-H,O-Z) | |
1055 | COMMON/FSI_POC/AMN,AM1,AM2,CN,C1,C2,AC1,AC2 | |
1056 | COMMON/FSI_MOM/P1X,P1Y,P1Z,E1,P1, !part. momenta in NRF | |
1057 | 1 P2X,P2Y,P2Z,E2,P2 | |
1058 | COMMON/FSI_COOR/X1,Y1,Z1,T1,R1, ! 4-coord. of emis. points in NRF | |
1059 | 1 X2,Y2,Z2,T2,R2 | |
1060 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
1061 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
1062 | COMMON/FSI_ICH1/ICH1 | |
1063 | COMMON/FSI_ETA/ETA | |
1064 | COMMON/LEDWEIGHT/WEIF,WEI,WEIN,ITEST,IRANPOS | |
1065 | COMMON/FSI_FFPN/FF12,FF21 | |
1066 | COMPLEX*16 FF1,FF12,FF21 | |
1067 | FF12=DCMPLX(1.D0,0.D0) | |
1068 | FF21=DCMPLX(1.D0,0.D0) | |
1069 | IF(I3C.EQ.0)RETURN | |
1070 | ICH1=IDINT(C1) | |
1071 | IF(ICH1.EQ.0)GOTO 11 | |
1072 | XH=AC1*P1 | |
1073 | ACH=ACP(XH) | |
1074 | ACHR=DSQRT(ACH) | |
1075 | ETA=0.D0 | |
1076 | IF(XH.NE.0.D0)ETA=1/XH | |
1077 | RHOS=P1*R1 | |
1078 | HS=X1*P1X+Y1*P1Y+Z1*P1Z | |
1079 | FF12=FF12*FF1(RHOS,HS) | |
1080 | IF(IQS.EQ.0)GOTO 11 | |
1081 | RHOS=P1*R2 | |
1082 | HS=X2*P1X+Y2*P1Y+Z2*P1Z | |
1083 | FF21=FF21*FF1(RHOS,HS) | |
1084 | 11 ICH1=IDINT(C2) | |
1085 | IF(ICH1.EQ.0)GOTO 10 | |
1086 | XH=AC2*P2 | |
1087 | ACH=ACP(XH) | |
1088 | ACHR=DSQRT(ACH) | |
1089 | ETA=0.D0 | |
1090 | IF(XH.NE.0.D0)ETA=1/XH | |
1091 | RHOS=P2*R2 | |
1092 | HS=X2*P2X+Y2*P2Y+Z2*P2Z | |
1093 | FF12=FF12*FF1(RHOS,HS) | |
1094 | CW WRITE(6,41)'AC2 ',AC2,'ACH ',ACH,'ETA ',ETA,'RHOS ',RHOS,'HS ',HS | |
1095 | 41 FORMAT(5(A5,E11.4)) | |
1096 | CW WRITE(6,40)'FF12 ',DREAL(FF12),DIMAG(FF12) | |
1097 | IF(IQS.EQ.0)GOTO 10 | |
1098 | RHOS=P2*R1 | |
1099 | HS=X1*P2X+Y1*P2Y+Z1*P2Z | |
1100 | FF21=FF21*FF1(RHOS,HS) | |
1101 | CW WRITE(6,41)'AC1 ',AC1,'ACH ',ACH,'ETA ',ETA,'RHOS ',RHOS,'HS ',HS | |
1102 | CW WRITE(6,40)'FF21 ',DREAL(FF21),DIMAG(FF21) | |
1103 | 40 FORMAT(A7,2E12.4) | |
1104 | 10 CONTINUE | |
1105 | ||
1106 | C WEIF = the weight due to the Coulomb particle-nucleus interaction | |
1107 | WEIF=DREAL(FF12)**2+DIMAG(FF12)**2 | |
1108 | IF(IQS.EQ.1)WEIF=0.5D0*(WEIF+DREAL(FF21)**2+DIMAG(FF21)**2) | |
1109 | RETURN | |
1110 | END | |
1111 | ||
1112 | C======================================================= | |
1113 | C | |
1114 | SUBROUTINE FSIWF !(WEI) | |
1115 | C==> Prepares necessary quantities and call VZ(WEI) to calculate | |
1116 | C the weight due to FSI | |
1117 | IMPLICIT REAL*8 (A-H,O-Z) | |
1118 | COMMON/FSI_CVK/V,CVK | |
1119 | COMMON/FSI_MOM/P1X,P1Y,P1Z,E1,P1, !part. momenta in NRF | |
1120 | 1 P2X,P2Y,P2Z,E2,P2 | |
1121 | COMMON/FSI_PRF/PPX,PPY,PPZ,AK,AKS, | |
1122 | 1 X,Y,Z,T,RP,RPS | |
1123 | COMMON/FSI_COOR/X1,Y1,Z1,T1,R1, ! 4-coord. of emis. points in NRF | |
1124 | 1 X2,Y2,Z2,T2,R2 | |
1125 | COMMON/FSI_POC/AMN,AM1,AM2,CN,C1,C2,AC1,AC2 | |
1126 | COMMON/FSI_SPIN/RHO(10) | |
1127 | COMMON/FSI_BP/B,P | |
1128 | COMMON/FSI_ETA/ETA | |
1129 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
1130 | COMMON/FSI_SW/RB(10),EB(10),BK(10),CDK(10),SDK(10), | |
1131 | 1 SBKRB(10),SDKK(10) | |
1132 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
1133 | COMMON/FSI_RR/F(10) | |
1134 | COMMON/FSI_FD/FD(10),RD(10) | |
1135 | COMMON/FSI_C/C(10),AM,AMS,DM | |
1136 | COMPLEX*16 C,F | |
1137 | COMMON/FSI_AA/AA | |
1138 | COMMON/FSI_SHH/SH,CHH | |
1139 | COMMON/FSI_AAPI/AAPI(20,2)/FSI_AAND/AAND(20,4) | |
1140 | COMMON/FSI_AAPIN/AAPIN(20,2) | |
1141 | COMMON/FSI_P12/P12X,P12Y,P12Z,E12,P12,AM12,EPM | |
1142 | COMMON/LEDWEIGHT/WEIF,WEI,WEIN,ITEST,IRANPOS | |
1143 | ||
1144 | ||
1145 | cmlv | |
1146 | IF(IRANPOS.EQ.0)THEN | |
1147 | C==>calculating relative 4-coordinates of the particles in PRF | |
1148 | C- {T,X,Y,Z} from the relative coordinates {TS,XS,YS,ZS} in NRF | |
1149 | XS=X1-X2 | |
1150 | YS=Y1-Y2 | |
1151 | ZS=Z1-Z2 | |
1152 | TS=T1-T2 | |
1153 | RS12=XS*P12X+YS*P12Y+ZS*P12Z | |
1154 | H1=(RS12/EPM-TS)/AM12 | |
1155 | X=XS+P12X*H1 | |
1156 | Y=YS+P12Y*H1 | |
1157 | Z=ZS+P12Z*H1 | |
1158 | T=(E12*TS-RS12)/AM12 | |
1159 | RPS=X*X+Y*Y+Z*Z | |
1160 | RP=DSQRT(RPS) | |
1161 | c WRITE(6,38)'RP ',RP,'X ',X,Y,Z,T | |
1162 | c FORMAT(A7,E11.4,A7,4E11.4) | |
1163 | ENDIF | |
1164 | ||
1165 | CVK=(P12X*PPX+P12Y*PPY+P12Z*PPZ)/(P12*AK) | |
1166 | V=P12/E12 | |
1167 | ||
1168 | IF(ICH.EQ.0)GOTO 21 | |
1169 | XH=AC*AK | |
1170 | ACH=ACP(XH) | |
1171 | ACHR=DSQRT(ACH) | |
1172 | ETA=0.D0 | |
1173 | IF(XH.NE.0.D0)ETA=1/XH | |
1174 | C---HCP, HPR needed (e.g. in GST) if ICH=1 | |
1175 | HCP=HC(XH) | |
1176 | HPR=HCP+.1544313298D0 | |
1177 | 21 CONTINUE | |
1178 | MSP=MSPIN | |
1179 | DO 30 JJ=1,MSP | |
1180 | ISPIN=JJ | |
1181 | IF(NS.NE.1)GOTO22 | |
1182 | C---Calc. quantities for the square well potential; | |
1183 | C-- for LL > 5 the square well potential is not possible or available | |
1184 | IF(LL.EQ.4)GOTO 22 | |
1185 | BK(JJ)=DSQRT(EB(JJ)**2+AKS) | |
1186 | XRA=2*RB(JJ)/AC | |
1187 | HRA=BK(JJ)*RB(JJ) | |
1188 | CALL SEQ(XRA,HRA) | |
1189 | SBKRB(JJ)=HRA*B | |
1190 | HRA=AK*RB(JJ) | |
1191 | CALL GST(XRA,HRA) | |
1192 | SDK(JJ)=SH | |
1193 | CDK(JJ)=CHH | |
1194 | SDKK(JJ)=RB(JJ) | |
1195 | IF(AK.NE.0.D0)SDKK(JJ)=SH/AK | |
1196 | IF(ICH.EQ.1)SDK(JJ)=ACH*SDK(JJ) | |
1197 | 22 CONTINUE | |
1198 | C----------------------------------------------------------------------- | |
1199 | C---Calc. the strong s-wave scattering amplitude = C(JJ) | |
1200 | C-- divided by Coulomb penetration factor squared (if ICH=1) | |
1201 | IF(NS.NE.1)GOTO 230 | |
1202 | IF(LL.NE.4)GOTO 230 ! SW scat. amplitude used for alfa-alfa only | |
1203 | GAK=G(AK) | |
1204 | AKACH=AK | |
1205 | IF(ICH.EQ.1)AKACH=AK*ACH | |
1206 | C(JJ)=1/DCMPLX(GAK,-AKACH) ! amplitude for the SW-potential | |
1207 | GOTO 30 | |
1208 | 230 IF(LL.EQ.5.OR.LL.EQ.6.OR.LL.EQ.7)GOTO20 ! pipi | |
1209 | IF(LL.EQ.12.OR.LL.EQ.13)GOTO20 ! piN | |
1210 | IF(LL.EQ.8.OR.LL.EQ.9.OR.LL.EQ.18)GOTO20 ! Nd, dd | |
1211 | IF(LL.EQ.14.OR.LL.EQ.17.OR.LL.EQ.23)GOTO27 ! K+K-, K-p, K0K0-b | |
1212 | A1=RD(JJ)*FD(JJ)*AKS | |
1213 | A2=1+.5D0*A1 | |
1214 | IF(ICH.EQ.1)A2=A2-2*HCP*FD(JJ)/AC | |
1215 | AKF=AK*FD(JJ) | |
1216 | IF(ICH.EQ.1)AKF=AKF*ACH | |
1217 | C(JJ)=FD(JJ)/DCMPLX(A2,-AKF) | |
1218 | GOTO30 | |
1219 | 20 CONTINUE | |
1220 | C---Calc. scatt. ampl. C(JJ) for pipi, piN and Nd, dd | |
1221 | JH=LL-7+2*JJ-2 | |
1222 | IF(LL.EQ.8.OR.LL.EQ.9)GPI2=GND(AKS,JH) | |
1223 | IF(LL.EQ.18)GPI2=GDD(AKS,JJ) | |
1224 | IF(LL.EQ.5.OR.LL.EQ.6.OR.LL.EQ.7)GPI2=GPIPI(AKS,2) | |
1225 | IF(LL.EQ.12.OR.LL.EQ.13)GPI2=GPIN(AKS,2) | |
1226 | C(JJ)=1.D0/DCMPLX(GPI2,-AK) !pi+pi+, nd, pd, pi+p, dd | |
1227 | IF(LL.NE.5.AND.LL.NE.6.AND.LL.NE.13)GOTO27 | |
1228 | IF(LL.EQ.5.OR.LL.EQ.6)GPI1=GPIPI(AKS,1) | |
1229 | IF(LL.EQ.13)GPI1=GPIN(AKS,1) | |
1230 | IF(LL.EQ.5.OR.LL.EQ.13) | |
1231 | c C(JJ)=.6667D0/DCMPLX(GPI1,-AK)+.3333D0*C(JJ) !pi+pi-,pi-p | |
1232 | IF(LL.EQ.6)C(JJ)=.3333D0/DCMPLX(GPI1,-AK)+.6667D0*C(JJ) !pi0pi0 | |
1233 | 27 CONTINUE | |
1234 | C---Calc. K+K-, K0K0-b or K-p s-wave scatt. ampl. | |
1235 | IF(LL.EQ.14.OR.LL.EQ.23)CALL CKKB | |
1236 | IF(LL.EQ.17)C(JJ)=DCMPLX(3.29D0,3.55D0) | |
1237 | C---Calc. pi+pi-, pi+pi+, pd, pi+p, pi-p, K+K- or K-p s-wave scatt. ampl. | |
1238 | C-- divided by Coulomb penetration factor squared (if ICH=1) | |
1239 | IF(ICH.EQ.0)GOTO 30 | |
1240 | AAK=ACH*AK | |
1241 | HCP2=2*HCP/AC | |
1242 | C(JJ)=1/(1/C(JJ)-HCP2+DCMPLX(0.D0,AK-AAK)) | |
1243 | c write(*,*)'c(jj)',c(jj) | |
1244 | 30 CONTINUE | |
1245 | C*********************************************************************** | |
1246 | c write(*,*)'before call vz in fsiwf wei',wei | |
1247 | CALL VZ !(WEI) | |
1248 | RETURN | |
1249 | END |