]>
Commit | Line | Data |
---|---|---|
ff4431bb | 1 | |
2 | SUBROUTINE FSIINI | |
f5ab1a71 | 3 | C---Note: |
4 | C-- ICH= 0 (1) if the Coulomb interaction is absent (present); | |
5 | C-- ISPIN= JJ= 1,2,..,MSPIN denote increasing values of the pair | |
6 | C-- total spin S. | |
7 | C-- To calculate the CF of two particles (with masses m1, m2 and | |
8 | C-- charges C1, C2) the following information is required: | |
9 | C-- AM= twice the reduced mass= 2*m1*m2/(m1+m2) in GeV/c^2, | |
10 | C-- DM= (m1-m2)/(m1+m2), required if NS=2; | |
11 | C-- AC= Bohr radius= 2*137.036*0.1973/(C1*C2*AMH) in fm; | |
12 | C-- AC > 1.D9 if C1*C2= 0, AC < 0 if C1*C2 < 0; | |
13 | C-- MSPIN= MSPINH(LL)= number of the values of the total pair spin S; | |
14 | C-- FD= FDH(LL,JJ), RD= RDH(LL,JJ)= scattering length and effective | |
15 | C-- radius for each value of the total pair spin S, JJ= 1,..,MSPIN; ; | |
16 | C-- the corresponding square well parameters EB= EBH(LL,JJ), RB= | |
ff4431bb | 17 | C-- RBH(LL,JJ) (required if NS=1) may be calculated by SEAR; |
f5ab1a71 | 18 | C-- if the effective range approximation is not valid (as is the case, |
19 | C-- e.g., for two-pion system) a code for calculation of the scattering | |
20 | C-- amplitude should be supplemented; | |
21 | C-- RHO= RHOH(LL,JJ), SF= SFH(LL,JJ), SE= SEH(LL) are spin factors; | |
22 | C-- RHO= the probability that the spins j1 and j2 of the two particles | |
23 | C-- will combine in a total spin S; | |
24 | C-- RHO= (2*S+1)/[(2j1+1)*(2j2+1)] for unpolarized particles; | |
25 | C-- RHO= (1-P1*P2)/4 and (3+P1*P2)/4 correspond to S=0 and 1 in the | |
26 | C-- case of spin-1/2 particles with polarizations P1 and P2; | |
27 | C----------------------------------------------------------------------- | |
28 | IMPLICIT REAL*8 (A-H,O-Z) | |
29 | COMMON/FSI_POC/AMN,AM1,AM2,CN,C1,C2,AC1,AC2 | |
30 | COMMON/FSI_PRF/PPX,PPY,PPZ,AK,AKS, | |
31 | 1 X,Y,Z,T,RP,RPS | |
32 | COMMON/FSI_SPIN/RHO(10) | |
33 | COMMON/FSI_ACH/HPR,AC,ACH,ACHR,ISPIN,MSPIN | |
34 | COMMON/FSI_NS/LL,NS,ICH,ISI,IQS,I3C,I3S | |
35 | COMMON/FSI_FD/FD(10),RD(10) | |
36 | COMMON/FSI_C/C(10),AM,AMS,DM | |
37 | COMMON/FSI_CONS/PI,PI2,SPI,DR,W | |
ff4431bb | 38 | COMPLEX*16 C |
f5ab1a71 | 39 | COMMON/FSI_AA/AA |
40 | COMMON/FSI_AAPI/AAPI(20,2)/FSI_AAND/AAND(20,4) | |
f5ab1a71 | 41 | COMMON/FSI_SW/RB(10),EB(10),BK(10),CDK(10),SDK(10), |
42 | 1 SBKRB(10),SDKK(10) | |
f5ab1a71 | 43 | |
ff4431bb | 44 | COMMON/LEDWEIGHT/WEIF,WEI,WEIN,ITEST,IRANPOS |
f5ab1a71 | 45 | |
46 | DIMENSION FDH(30,10),RDH(30,10),EBH(30,10),RBH(30,10) | |
47 | DIMENSION RHOH(30,10) | |
48 | DIMENSION AM1H(30),AM2H(30),C1H(30),C2H(30),MSPINH(30) | |
49 | C============= declarations pour l'appel de READ_FILE()============ | |
50 | CHARACTER*10 KEY | |
51 | CHARACTER*8 CH8 | |
52 | INTEGER*4 INT4 | |
53 | REAL*8 REAL8 | |
54 | INTEGER*4 IERR | |
55 | C | |
56 | C--- mass of the first and second particle | |
ff4431bb | 57 | DATA AM1H/.9395656D0,.9382723D0,.9395656D0,3.7294D0,.13957D0, |
58 | C .13498D0,.13957D0, .9395656D0, .9382723D0, | |
f5ab1a71 | 59 | C 4*.13957D0,4*.493677D0, |
ff4431bb | 60 | C 2*1.875613D0,2*2.808D0,2*.497672D0, |
61 | C 1.875613D0,2*.9382723D0, 4*0.D0/ | |
62 | DATA AM2H/.9395656D0,.9382723D0,.9382723D0,3.7294D0,.13957D0, | |
63 | C .13498D0,.13957D0, 2*1.875613D0, | |
64 | C 2*.493677D0,2*.9382723D0, | |
65 | C 2*.493677D0,2*.9382723D0, | |
66 | C 1.875613D0,3.7294D0,2.808D0,3.7294D0, | |
67 | C 2*.497672D0,2*2.808D0,3.7294D0, 4*0.D0/ | |
f5ab1a71 | 68 | C--- charge of the first and second particle |
69 | DATA C1H/0.D0,1.D0,0.D0,2.D0, 1.D0,0.D0,1.D0,0.D0,1.D0, | |
70 | C 3*1.D0,-1.D0,3*1.D0,-1.D0, | |
ff4431bb | 71 | C 4*1.D0,2*0.D0,3*1.D0, 4*0.D0/ |
f5ab1a71 | 72 | DATA C2H/0.D0,1.D0,1.D0,2.D0,-1.D0,0.D0,3*1.D0, |
73 | C -1.D0,3*1.D0,-1.D0,3*1.D0, | |
ff4431bb | 74 | C 1.D0,2.D0,1.D0,2.D0,2*0.D0,2*1.D0,2.D0, 4*0.D0/ |
f5ab1a71 | 75 | C---MSPIN vs (LL) |
ff4431bb | 76 | DATA MSPINH/3*2,4*1,2*2,8*1,3,1,2,1,2*1,2*2,1, 4*0/ |
f5ab1a71 | 77 | C---Spin factors RHO vs (LL,ISPIN) |
78 | DATA RHOH/3*.25D0, 4*1.D0, 2*.3333D0, 8*1.D0, | |
ff4431bb | 79 | C .1111D0,1.D0,.25D0,1.D0,2*1.D0, |
80 | 1 .3333D0,.25D0,1.D0, 4*0.D0, | |
81 | C 3*.75D0, 4*0.D0, 2*.6667D0, 8*0.D0, | |
82 | C .3333D0,.0D0,.75D0,.0D0,2*0.D0, | |
83 | 2 .6667D0,.75D0,0.D0, 4*0.D0, | |
84 | C 17*.0D0,.5556D0,3*0.D0, 5*0.D0,4*0.D0,210*0.D0/ | |
f5ab1a71 | 85 | C---Scattering length FD and effective radius RD in fm vs (LL,ISPIN) |
86 | DATA FDH/17.0D0,7.8D0,23.7D0,2230.1218D0,.225D0,.081D0,-.063D0, | |
ff4431bb | 87 | C -.65D0,-2.73D0, |
88 | C .137D0,-.071D0,-.148D0,.112D0,2*1.D-6,-.360D0, | |
89 | 1 2*1.D-6,1.344D0,6*1.D-6,-5.628D0, 4*0.D0, | |
90 | C -10.8D0,2*-5.4D0,4*0.D0,-6.35D0,-11.88D0,8*0.D0,9*0.D0,4*0.D0, | |
91 | C 240*0.D0/ | |
f5ab1a71 | 92 | DATA RDH/2.7D0,2.8D0,2.7D0,1.12139906D0,-44.36D0,64.0D0,784.9D0, |
ff4431bb | 93 | c--------|---------|---------|---------|---------|---------|---------|---------- |
94 | C 477.9D0, 2.27D0, 9*0.D0,-69.973D0, 6*0.D0,3.529D0, 4*0.D0, | |
95 | C 3*1.7D0,4*0.D0,2.0D0,2.63D0, 17*0.D0, 4*0.D0, 240*0.D0/ | |
f5ab1a71 | 96 | C---Corresponding square well parameters RB (width in fm) and |
97 | C-- EB =SQRT(-AM*U) (in GeV/c); U is the well height | |
98 | DATA RBH/2.545739D0, 2.779789D0, 2.585795D0, 5.023544D0, | |
ff4431bb | 99 | C .124673D0, .3925180D0,.09D0, 2.D0, 4.058058D0, 17*0.D0, 4*0.D0, |
100 | C 3*2.003144D0, | |
101 | C 4*0.D0, 2.D0, 4.132163D0, 17*0.D0, 4*0.D0, 240*0.D0/ | |
f5ab1a71 | 102 | DATA EBH/.1149517D0, .1046257D0, .1148757D0, .1186010D0, |
ff4431bb | 103 | C .7947389D0,2.281208D0,8.7D0,.4D0,.1561219D0,17*0.D0,4*0.D0, |
104 | C 3*.1847221D0, | |
105 | C 4*0.D0, .4D0, .1150687D0, 17*0.D0, 4*0.D0, 240*0.D0/ | |
f5ab1a71 | 106 | C=======< constants >======================== |
107 | W=1/.1973D0 ! from fm to 1/GeV | |
108 | PI=4*DATAN(1.D0) | |
109 | PI2=2*PI | |
110 | SPI=DSQRT(PI) | |
111 | DR=180.D0/PI ! from radian to degree | |
f5ab1a71 | 112 | AC1=1.D10 |
113 | AC2=1.D10 | |
f5ab1a71 | 114 | |
115 | C---setting particle masses and charges | |
116 | AM1=AM1H(LL) | |
117 | AM2=AM2H(LL) | |
118 | C1=C1H(LL) | |
119 | C2=C2H(LL) | |
120 | ||
121 | C-- Switches: | |
122 | C ISI=1(0) the strong interaction between the two particles ON (OFF) | |
123 | C IQS=1(0) the quantum statistics ON (OFF); | |
124 | C should be OFF for nonidentical particles | |
125 | C I3C=1(0) the Coulomb interaction with the nucleus ON (OFF) | |
126 | C I3S=1(0) the strong interaction with the nucleus ON (OFF) | |
127 | C ICH=1(0) if C1*C2 is different from 0 (is equal to 0) | |
128 | C- to switch off the Coulomb force between the two particles | |
129 | C put ICH=0 and substitute the strong amplitude parameters by | |
130 | C the ones not affected by Coulomb interaction | |
131 | ||
ff4431bb | 132 | IF(ITEST.EQ.0)THEN |
133 | ||
f5ab1a71 | 134 | ICH=0 |
135 | IF(C1*C2.NE.0.D0) ICH=1 | |
136 | IQS=0 | |
137 | IF(C1+AM1.EQ.C2+AM2) IQS=1 | |
138 | I3S=0 ! only this option is available | |
139 | ISI=1 | |
ff4431bb | 140 | I3C=1 |
141 | ||
f5ab1a71 | 142 | ENDIF |
f5ab1a71 | 143 | |
ff4431bb | 144 | c23456 |
145 | write(*,*)'FSIINI ITEST ich iqs i3s isi i3c',ITEST, | |
146 | + ICH,IQS,I3S,ISI,I3C | |
147 | ||
f5ab1a71 | 148 | C================================================================== |
149 | C---fm to 1/GeV | |
150 | DO 3 J1=1,30 | |
151 | DO 3 J2=1,10 | |
152 | FDH(J1,J2)=FDH(J1,J2)*W | |
153 | RDH(J1,J2)=RDH(J1,J2)*W | |
154 | 3 RBH(J1,J2)=RBH(J1,J2)*W | |
155 | C---calcul. twice the reduced mass (AM), the relative mass difference | |
156 | C-- (DM) and the Bohr radius (AC) | |
157 | AM=2*AM1*AM2/(AM1+AM2) | |
158 | AMS=AM*AM | |
159 | DM=(AM1-AM2)/(AM1+AM2) | |
160 | AC=1.D10 | |
161 | C12=C1*C2 | |
162 | IF(C12.NE.0.D0)AC=2*137.036D0/(C12*AM) | |
163 | C---Setting spin factors | |
164 | MSPIN=MSPINH(LL) | |
165 | MSP=MSPIN | |
166 | DO 91 ISPIN=1,10 | |
167 | 91 RHO(ISPIN)=RHOH(LL,ISPIN) | |
168 | C---Integration limit AA in the spherical wave approximation | |
169 | AA=0.D0 | |
170 | cc IF(NS.EQ.2.OR.NS.EQ.4)AA=.5D0 !!in 1/GeV --> 0.1 fm | |
171 | IF(NS.EQ.2.OR.NS.EQ.4)AA=6.D0 !!in 1/GeV --> 1.2 fm | |
172 | C---Setting scatt. length (FD), eff. radius (RD) and, if possible, | |
173 | C-- also the corresp. square well parameters (EB, RB) | |
174 | DO 55 JJ=1,MSP | |
175 | ISPIN=JJ | |
176 | FD(JJ)=FDH(LL,JJ) | |
177 | RD(JJ)=RDH(LL,JJ) | |
178 | EB(JJ)=EBH(LL,JJ) | |
179 | RB(JJ)=RBH(LL,JJ) | |
ff4431bb | 180 | IF(LL.NE.8.AND.LL.NE.9)GOTO25 |
f5ab1a71 | 181 | C---Resets FD and RD for a nucleon-deuteron system (LL=8,9) |
ff4431bb | 182 | JH=LL-7+2*JJ-2 |
183 | FD(JJ)=AAND(1,JH) | |
184 | RD(JJ)=AAND(2,JH)-2*AAND(3,JH)/AAND(1,JH) | |
f5ab1a71 | 185 | C---Resets FD and RD for a pion-pion system (LL=5,6,7) |
ff4431bb | 186 | 25 IF(LL.GT.7.OR.LL.LT.5)GOTO 24 |
187 | IF(LL.EQ.7)FD(JJ)=AAPI(1,2)/AM | |
188 | IF(LL.EQ.5)FD(JJ)=(.6667D0*AAPI(1,1)+.3333D0*AAPI(1,2))/AM | |
189 | IF(LL.EQ.6)FD(JJ)=(.3333D0*AAPI(1,1)+.6667D0*AAPI(1,2))/AM | |
190 | AKS=0.D0 | |
191 | DAKS=1.D-5 | |
192 | AKSH=AKS+DAKS | |
193 | AKH=DSQRT(AKSH) | |
194 | GPI1H=GPIPI(AKSH,1) | |
195 | GPI2H=GPIPI(AKSH,2) | |
196 | H=1/FD(JJ) | |
197 | IF(LL.EQ.7)C(JJ)=1/DCMPLX(GPI2H,-AKH) | |
198 | IF(LL.EQ.5) | |
199 | +C(JJ)=.6667D0/DCMPLX(GPI1H,-AKH)+.3333D0/DCMPLX(GPI2H,-AKH) | |
200 | IF(LL.EQ.6) | |
201 | +C(JJ)=.3333D0/DCMPLX(GPI1H,-AKH)+.6667D0/DCMPLX(GPI2H,-AKH) | |
202 | HH=DREAL(1/C(JJ)) | |
203 | RD(JJ)=2*(HH-H)/DAKS | |
204 | 24 CONTINUE | |
f5ab1a71 | 205 | C---Calculation continues for any system (any LL) |
206 | 55 CONTINUE | |
f5ab1a71 | 207 | END |
ff4431bb | 208 | C======================================================= |
209 | ||
210 | ||
211 | ||
212 | ||
213 | ||
214 | ||
215 | ||
216 | ||
217 | ||
f5ab1a71 | 218 | |
219 | ||
220 | ||
ff4431bb | 221 | FUNCTION GPIPIold(X,J) |
f5ab1a71 | 222 | C--- GPIPI = k*COTG(DELTA), X=k^2 |
223 | C-- J=1(2) corresponds to isospin=0(2) | |
224 | IMPLICIT REAL*8 (A-H,O-Z) | |
225 | c-- Include 'common_fsi_aapi.inc' | |
226 | c-- Include 'common_fsi_c.inc' | |
227 | COMMON/FSI_AAPI/AAPI(20,2) | |
228 | COMMON/FSI_C/HELP(20),AM,AMS,DM | |
229 | OM=DSQRT(X+AMS) | |
230 | XX=X/AMS | |
231 | GPIPI=OM/AAPI(1,J) | |
232 | GPIPI=GPIPI*(1+(AAPI(3,J)-AAPI(1,J)**2)*XX+AAPI(4,J)*XX*XX) | |
233 | GPIPI=GPIPI/(1+(AAPI(3,J)+AAPI(2,J)/AAPI(1,J))*XX) | |
234 | ||
235 | END | |
236 | ||
237 | FUNCTION GPIN(X,J) | |
238 | C--- GPIN = k*COTG(DELTA), X=k^2 | |
239 | C-- J=1(2) corresponds to piN isospin=1/2(3/2) | |
240 | IMPLICIT REAL*8 (A-H,O-Z) | |
241 | c-- Include 'common_fsi_aapin.inc' | |
242 | COMMON/FSI_AAPIN/AAPIN(20,2) | |
243 | GPIN=1/AAPIN(1,J)+.5D0*AAPIN(2,J)*X | |
244 | ||
245 | END |