program= LPOTT input= in/in.he3.hadj Thu Aug 15 16:46:26 PDT 1991 cat in/tfoldc>tape3 cat in/gth>tape2 cat in/denomt>tape4 for it do run LPOTT $it & wait done Run Time STOP Real 19.0 User 8.7 System 0.4 pion scattering via lpott(vaxversion) on 32,1/86 ok tape6 1 9 200.0000 16 22 .20E+05 3-2.00-4.00 no of grid points= 16 .6540 .4560 .8210 .6750 .3660 .8360 2.1600 6.0000 2 3 3 101733001 0 0 0 0 0 3 0 0 1 0 nifty( 1)= 3 pi cex nifty( 2)= 1 *5=be shift nifty( 3)= 0 no w.f. nifty( 4)= 1 nlsp-g(p) nifty( 5)= 7 e3b, aay nifty( 6)= 3 spin,ms nifty( 7)= 3 vabs-old nifty( 8)= 0 no del/fld nifty( 9)= 0 no pauli nifty(10)= 1 +fc+phase nifty(11)= 0 pi0,pi-,k+ shift nifty(12)= 0 pi+,ko shift nifty(13)= 0 pi-channel shift nifty(14)= 0 pi+channel shift nifty(15)= 0 not used shift nifty(16)= 3 he/d nifty(17)= 0 kmt nifty(18)= 0 full amps nifty(19)= 1 hadjm's ff nifty(20)= 0 no t10 plt nes,nwaves,b0r,b0i,c0r,c0i= 59 14 .00000 .00000 .00000 .00000 nes,nwaves,b0r,b0i,c0r,c0i= 59 14 -.04000 .04000 .00000 .08000 .4277 .2079 .6740 .4556 .1340 .6989 pi-plus, pi-minus and then cex(pi- to pi0) 3 calcs ********** amass= 3.0000********** tpi epilab ecm(sqrts) kcm plab 200.0000 339.5780 3139.1188 277.5801 309.5661 relativistic calculation energy momentum 200.0000 277.5801 ----- angular momentum = 0----- OPT POTEN VALUES FOR KP=K0= 277.580AND L=1 K REV VC RABS(N0 FLIP) RABS(FLIP)IMV IMVABS(NOFLIP),IMABS(FLIP) .1479E+01 .9205E-08 .0000E+00 -.164E-08 .000E+00 .1034E-06 -.499E-07 .000E+00 .7912E+01 .5200E-07 .0000E+00 -.742E-09 .000E+00 .3011E-06 -.563E-07 .000E+00 .1999E+02 .1497E-06 .0000E+00 .935E-09 .000E+00 .8261E-06 -.896E-07 .000E+00 .3868E+02 .2829E-06 .0000E+00 .350E-08 .000E+00 .1532E-05 -.156E-06 .000E+00 .6556E+02 .4496E-06 .0000E+00 .706E-08 .000E+00 .2442E-05 -.241E-06 .000E+00 .1032E+03 .6085E-06 .0000E+00 .116E-07 .000E+00 .3410E-05 -.325E-06 .000E+00 .1556E+03 .6755E-06 .0000E+00 .168E-07 .000E+00 .4119E-05 -.369E-06 .000E+00 .2294E+03 .5526E-06 .0000E+00 .211E-07 .000E+00 .4153E-05 -.336E-06 .000E+00 .3359E+03 .1391E-06 .0000E+00 .213E-07 .000E+00 .3270E-05 -.225E-06 .000E+00 .4952E+03 -.3405E-06 .0000E+00 .140E-07 .000E+00 .1667E-05 -.923E-07 .000E+00 .7467E+03 -.2211E-06 .0000E+00 .333E-08 .000E+00 .2036E-06 -.139E-07 .000E+00 .1175E+04 .1515E-07 .0000E+00 .485E-10 .000E+00 -.5552E-08 -.136E-09 .000E+00 .1992E+04 .3996E-10 .0000E+00 .452E-16 .000E+00 .8916E-16 -.892E-16 .000E+00 .3854E+04 -.1857E-13 .0000E+00 .259E-42 .000E+00 .3595E-42 -.360E-42 .000E+00 .9739E+04 .1060E-32 .0000E+00 .000E+00 .000E+00 .0000E+00 .000E+00 .000E+00 .5210E+05 .7683E-71 .0000E+00 .000E+00 .000E+00 .0000E+00 .000E+00 .000E+00 TRUE 2N ANNIHILATION PARAMS FOR K(=KP=K0): IMB,REB,IMC,REC/ THEN, RE, IM VABS(L) FLIP+NOFLIP 277.580 .80077E-10 -.80077E-10 .99041E-14 .00000E+00 .75875E-07 -.28556E-06 .00000E+00 .00000E+00 .22003E-07 -.28809E-06 .00000E+00 .00000E+00 .39446E-08 -.90736E-07 .00000E+00 .00000E+00 .51036E-09 -.16902E-07 .00000E+00 .00000E+00 .51602E-10 -.22359E-08 .00000E+00 .00000E+00 .42798E-11 -.22937E-09 .00000E+00 .00000E+00 .30082E-12 -.19219E-10 .00000E+00 .00000E+00 .18343E-13 -.13612E-11 .00000E+00 .00000E+00 .98762E-15 -.83490E-13 .00000E+00 .00000E+00 OPT POTEN VALUES FOR KP=K0= 277.580AND L=1 K REV VC RABS(N0 FLIP) RABS(FLIP)IMV IMVABS(NOFLIP),IMABS(FLIP) .2776E+03 .3784E-06 .0000E+00 .220E-07 .000E+00 .3816E-05 -.288E-06 .000E+00 determinant from matrix inversion= .5375282E+00 unnormalized r matrix(re,im,re,-im) .1776123E-05 -.2752220E-05 .1776123E-05 .2752220E-05 normalized r(k,k..k)= -.2760355E+00 .4277353E+00 t(k,k,k)= -.1958047E+00 .4872416E+00 eta= .3924 delta= -43.1360 coulomb phase modified nuclear amplitude t(k,k.k) = -.1874988E+00 .4904977E+00 born approximation normalized r(k,k..k)= -.1069329E+00 .4917003E+00 t(k,k,k)= -.1603994E+00 .7375505E+00 eta= .5733 delta= -72.9859 determinant from matrix inversion= .5375282E+00 unnormalized r matrix(re,im,re,-im) .1776123E-05 -.2752220E-05 .1776123E-05 .2752220E-05 normalized r(k,k..k)= -.2760355E+00 .4277353E+00 t(k,k,k)= -.1958047E+00 .4872416E+00 eta= .3924 delta= -43.1360 coulomb phase modified nuclear amplitude t(k,k.k) = -.1874988E+00 .4904977E+00 born approximation normalized r(k,k..k)= -.1069329E+00 .4917003E+00 t(k,k,k)= -.1603994E+00 .7375505E+00 eta= .5733 delta= -72.9859 ----- angular momentum = 1----- determinant from matrix inversion= .5244084E+00 unnormalized r matrix(re,im,re,-im) .1273819E-05 -.3707490E-05 .1273819E-05 .3707490E-05 normalized r(k,k..k)= -.1979702E+00 .5761982E+00 t(k,k,k)= -.1176716E+00 .5631226E+00 eta= .2671 delta= -59.1052 coulomb phase modified nuclear amplitude t(k,k.k) = -.1246712E+00 .5616144E+00 born approximation normalized r(k,k..k)= -.5880749E-01 .5931293E+00 t(k,k,k)= -.8821124E-01 .8896939E+00 eta= .7991 delta= -83.6227 determinant from matrix inversion= .5722496E+00 unnormalized r matrix(re,im,re,-im) .7639640E-06 -.2790874E-05 .7639640E-06 .2790874E-05 normalized r(k,k..k)= -.1187312E+00 .4337428E+00 t(k,k,k)= -.8604893E-01 .4609131E+00 eta= .1890 delta= -32.7853 coulomb phase modified nuclear amplitude t(k,k.k) = -.9177884E-01 .4598064E+00 born approximation normalized r(k,k..k)= -.5725622E-01 .4413792E+00 t(k,k,k)= -.8588433E-01 .6620687E+00 eta= .3668 delta= -76.0399 ----- angular momentum = 2----- determinant from matrix inversion= .5519908E+00 unnormalized r matrix(re,im,re,-im) .4662895E-06 -.1882022E-05 .4662895E-06 .1882022E-05 normalized r(k,k..k)= -.7246822E-01 .2924939E+00 t(k,k,k)= -.6486624E-01 .3430899E+00 eta= .3396 delta= -11.2300 coulomb phase modified nuclear amplitude t(k,k.k) = -.7416128E-01 .3412014E+00 born approximation normalized r(k,k..k)= -.9697346E-03 .2869856E+00 t(k,k,k)= -.1454602E-02 .4304783E+00 eta= .1391 delta= -.5993 determinant from matrix inversion= .6136558E+00 unnormalized r matrix(re,im,re,-im) .3197069E-06 -.1569611E-05 .3197069E-06 .1569611E-05 normalized r(k,k..k)= -.4968714E-01 .2439405E+00 t(k,k,k)= -.4808877E-01 .2960754E+00 eta= .4190 delta= -6.6344 coulomb phase modified nuclear amplitude t(k,k.k) = -.5611300E-01 .2946599E+00 born approximation normalized r(k,k..k)= -.5823595E-02 .2424686E+00 t(k,k,k)= -.8735393E-02 .3637030E+00 eta= .2732 delta= -1.8336 ----- angular momentum = 3----- determinant from matrix inversion= .6034347E+00 unnormalized r matrix(re,im,re,-im) .3162553E-07 -.6414571E-06 .3162553E-07 .6414571E-06 normalized r(k,k..k)= -.4915070E-02 .9969183E-01 t(k,k,k)= -.6096356E-02 .1360088E+00 eta= .7281 delta= -.4798 coulomb phase modified nuclear amplitude t(k,k.k) = -.1112036E-01 .1356904E+00 born approximation normalized r(k,k..k)= .6945927E-02 .9437795E-01 t(k,k,k)= .1041889E-01 .1415669E+00 eta= .7172 delta= .8325 determinant from matrix inversion= .6497910E+00 unnormalized r matrix(re,im,re,-im) .2303172E-07 -.5756752E-06 .2303172E-07 .5756752E-06 normalized r(k,k..k)= -.3579467E-02 .8946836E-01 t(k,k,k)= -.4523512E-02 .1231965E+00 eta= .7537 delta= -.3439 coulomb phase modified nuclear amplitude t(k,k.k) = -.9074929E-02 .1229451E+00 born approximation normalized r(k,k..k)= .5553819E-02 .8614576E-01 t(k,k,k)= .8330728E-02 .1292186E+00 eta= .7417 delta= .6436 ----- angular momentum = 4----- determinant from matrix inversion= .6901416E+00 unnormalized r matrix(re,im,re,-im) -.1387700E-07 -.1792553E-06 -.1387700E-07 .1792553E-06 normalized r(k,k..k)= .2156690E-02 .2785891E-01 t(k,k,k)= .3062034E-02 .4066216E-01 eta= .9187 delta= .1910 coulomb phase modified nuclear amplitude t(k,k.k) = .1256762E-02 .4075792E-01 born approximation normalized r(k,k..k)= .3304934E-02 .2695200E-01 t(k,k,k)= .4957401E-02 .4042800E-01 eta= .9192 delta= .3090 determinant from matrix inversion= .7164116E+00 unnormalized r matrix(re,im,re,-im) -.1365313E-07 -.1737658E-06 -.1365313E-07 .1737658E-06 normalized r(k,k..k)= .2121896E-02 .2700576E-01 t(k,k,k)= .3017642E-02 .3944967E-01 eta= .9211 delta= .1877 coulomb phase modified nuclear amplitude t(k,k.k) = .1266154E-02 .3954465E-01 born approximation normalized r(k,k..k)= .3155189E-02 .2630253E-01 t(k,k,k)= .4732784E-02 .3945379E-01 eta= .9211 delta= .2944 ----- angular momentum = 5----- determinant from matrix inversion= .7675416E+00 unnormalized r matrix(re,im,re,-im) -.6502919E-08 -.4627700E-07 -.6502919E-08 .4627700E-07 normalized r(k,k..k)= .1010649E-02 .7192124E-02 t(k,k,k)= .1494399E-02 .1071265E-01 eta= .9786 delta= .0875 coulomb phase modified nuclear amplitude t(k,k.k) = .9546977E-03 .1077417E-01 born approximation normalized r(k,k..k)= .1112078E-02 .7093290E-02 t(k,k,k)= .1668117E-02 .1063993E-01 eta= .9787 delta= .0977 determinant from matrix inversion= .7838471E+00 unnormalized r matrix(re,im,re,-im) -.6944455E-08 -.4792782E-07 -.6944455E-08 .4792782E-07 normalized r(k,k..k)= .1079270E-02 .7448685E-02 t(k,k,k)= .1595053E-02 .1109213E-01 eta= .9778 delta= .0935 coulomb phase modified nuclear amplitude t(k,k.k) = .1036173E-02 .1115822E-01 born approximation normalized r(k,k..k)= .1182520E-02 .7360644E-02 t(k,k,k)= .1773779E-02 .1104097E-01 eta= .9779 delta= .1039 ----- angular momentum = 6----- born approximation normalized r(k,k..k)= .3405154E-03 .2049216E-02 t(k,k,k)= .5107731E-03 .3073824E-02 eta= .9939 delta= .0294 t(k,k,k)= .5086861E-03 .3067711E-02 eta= .9939 delta= .0293 coulomb phase modified nuclear amplitude t(k,k.k) = .3388718E-03 .3091081E-02 born approximation normalized r(k,k..k)= .3968636E-03 .2106948E-02 t(k,k,k)= .5952954E-03 .3160423E-02 eta= .9937 delta= .0343 t(k,k,k)= .5927947E-03 .3154012E-02 eta= .9937 delta= .0342 coulomb phase modified nuclear amplitude t(k,k.k) = .4180971E-03 .3181885E-02 ----- angular momentum = 7----- born approximation normalized r(k,k..k)= .1094706E-03 .6913031E-03 t(k,k,k)= .1642059E-03 .1036955E-02 eta= .9979 delta= .0094 t(k,k,k)= .1639791E-03 .1036256E-02 eta= .9979 delta= .0094 coulomb phase modified nuclear amplitude t(k,k.k) = .1022384E-03 .1044157E-02 born approximation normalized r(k,k..k)= .1234103E-03 .7163309E-03 t(k,k,k)= .1851154E-03 .1074496E-02 eta= .9979 delta= .0106 t(k,k,k)= .1848505E-03 .1073750E-02 eta= .9979 delta= .0106 coulomb phase modified nuclear amplitude t(k,k.k) = .1208496E-03 .1082822E-02 ----- angular momentum = 8----- born approximation normalized r(k,k..k)= .4109411E-04 -.3541141E-04 t(k,k,k)= .6164117E-04 -.5311712E-04 eta= 1.0001 delta= .0035 t(k,k,k)= .6164553E-04 -.5311647E-04 eta= 1.0001 delta= .0035 coulomb phase modified nuclear amplitude t(k,k.k) = .6486817E-04 -.4912892E-04 born approximation normalized r(k,k..k)= .5048286E-04 .2095489E-04 t(k,k,k)= .7572428E-04 .3143233E-04 eta= .9999 delta= .0043 t(k,k,k)= .7572111E-04 .3143550E-04 eta= .9999 delta= .0043 coulomb phase modified nuclear amplitude t(k,k.k) = .7359117E-04 .3614163E-04 th-c.m. cos(cm) dsig/dw-cm ds/dw(b.a.) t th-lab cos(lab) ds/dw ds/dw(b.a.) ref(th)-cm imf signuc noflip noflip-b polar flip flip-b .0 1.000 .472E+13 .472E+13 .000E+00 .0 1.000 .587E+13 .587E+13 -.643 3.652 .1375E+03 .137E+03 .472E+13 -.174E-04 .000E+00 .000E+00 3.0 .999 .764E+03 .773E+03 -.211E+03 2.7 .999 .950E+03 .961E+03 -.642 3.634 .1362E+03 .136E+03 .773E+03 -.929E-03 .155E-02 .347E-02 6.0 .995 .183E+03 .251E+03 -.844E+03 5.4 .996 .227E+03 .311E+03 -.638 3.580 .1322E+03 .132E+03 .251E+03 -.185E-02 .612E-02 .138E-01 9.0 .988 .140E+03 .216E+03 -.190E+04 8.1 .990 .174E+03 .268E+03 -.632 3.492 .1260E+03 .126E+03 .216E+03 -.275E-02 .135E-01 .305E-01 12.0 .978 .124E+03 .200E+03 -.337E+04 10.8 .982 .154E+03 .248E+03 -.623 3.373 .1177E+03 .118E+03 .200E+03 -.363E-02 .235E-01 .533E-01 15.0 .966 .111E+03 .184E+03 -.525E+04 13.5 .973 .138E+03 .228E+03 -.611 3.226 .1078E+03 .108E+03 .184E+03 -.446E-02 .357E-01 .813E-01 18.0 .951 .992E+02 .168E+03 -.754E+04 16.2 .960 .122E+03 .207E+03 -.597 3.054 .9689E+02 .968E+02 .168E+03 -.524E-02 .494E-01 .114E+00 21.0 .934 .870E+02 .150E+03 -.102E+05 18.9 .946 .107E+03 .185E+03 -.579 2.863 .8541E+02 .853E+02 .150E+03 -.595E-02 .643E-01 .149E+00 24.0 .914 .749E+02 .133E+03 -.133E+05 21.6 .930 .917E+02 .162E+03 -.559 2.658 .7385E+02 .738E+02 .132E+03 -.657E-02 .796E-01 .187E+00 27.0 .891 .634E+02 .115E+03 -.168E+05 24.3 .911 .773E+02 .140E+03 -.537 2.442 .6263E+02 .625E+02 .115E+03 -.705E-02 .946E-01 .225E+00 30.0 .866 .527E+02 .984E+02 -.206E+05 27.0 .891 .639E+02 .119E+03 -.512 2.222 .5210E+02 .520E+02 .982E+02 -.737E-02 .109E+00 .263E+00 33.0 .839 .429E+02 .828E+02 -.249E+05 29.7 .868 .518E+02 .999E+02 -.485 2.000 .4249E+02 .424E+02 .825E+02 -.746E-02 .121E+00 .298E+00 36.0 .809 .343E+02 .686E+02 -.294E+05 32.5 .844 .411E+02 .823E+02 -.456 1.782 .3398E+02 .338E+02 .683E+02 -.724E-02 .132E+00 .331E+00 39.0 .777 .269E+02 .560E+02 -.343E+05 35.2 .817 .320E+02 .667E+02 -.426 1.571 .2662E+02 .265E+02 .556E+02 -.661E-02 .141E+00 .360E+00 42.0 .743 .206E+02 .450E+02 -.396E+05 38.0 .788 .244E+02 .532E+02 -.394 1.368 .2041E+02 .203E+02 .446E+02 -.538E-02 .146E+00 .384E+00 45.0 .707 .155E+02 .356E+02 -.451E+05 40.7 .758 .182E+02 .418E+02 -.362 1.177 .1531E+02 .152E+02 .352E+02 -.330E-02 .150E+00 .403E+00 48.0 .669 .113E+02 .277E+02 -.510E+05 43.5 .725 .132E+02 .322E+02 -.329 .999 .1121E+02 .111E+02 .272E+02 .449E-04 .150E+00 .417E+00 51.0 .629 .808E+01 .211E+02 -.571E+05 46.3 .691 .934E+01 .245E+02 -.296 .835 .7993E+01 .785E+01 .207E+02 .532E-02 .148E+00 .424E+00 54.0 .588 .560E+01 .159E+02 -.635E+05 49.1 .655 .642E+01 .182E+02 -.264 .685 .5536E+01 .539E+01 .154E+02 .136E-01 .144E+00 .427E+00 57.0 .545 .376E+01 .117E+02 -.702E+05 51.9 .617 .427E+01 .133E+02 -.233 .550 .3707E+01 .357E+01 .113E+02 .270E-01 .138E+00 .424E+00 60.0 .500 .242E+01 .842E+01 -.771E+05 54.7 .578 .273E+01 .948E+01 -.203 .430 .2388E+01 .226E+01 .800E+01 .489E-01 .130E+00 .417E+00 63.0 .454 .150E+01 .593E+01 -.841E+05 57.5 .537 .167E+01 .661E+01 -.174 .323 .1470E+01 .135E+01 .552E+01 .864E-01 .121E+00 .406E+00 66.0 .407 .879E+00 .407E+01 -.914E+05 60.4 .494 .971E+00 .449E+01 -.148 .230 .8589E+00 .747E+00 .368E+01 .153E+00 .112E+00 .391E+00 69.0 .358 .490E+00 .272E+01 -.989E+05 63.3 .450 .536E+00 .298E+01 -.123 .150 .4761E+00 .375E+00 .235E+01 .276E+00 .101E+00 .373E+00 72.0 .309 .267E+00 .178E+01 -.106E+06 66.1 .405 .289E+00 .192E+01 -.100 .081 .2569E+00 .166E+00 .142E+01 .496E+00 .911E-01 .353E+00 75.0 .259 .157E+00 .114E+01 -.114E+06 69.0 .358 .168E+00 .123E+01 -.080 .023 .1500E+00 .691E-01 .812E+00 .806E+00 .810E-01 .332E+00 78.0 .208 .120E+00 .747E+00 -.122E+06 71.9 .310 .128E+00 .792E+00 -.062 -.025 .1158E+00 .446E-01 .438E+00 .973E+00 .712E-01 .310E+00 81.0 .156 .127E+00 .523E+00 -.130E+06 74.8 .261 .134E+00 .548E+00 -.046 -.064 .1244E+00 .625E-01 .236E+00 .828E+00 .619E-01 .287E+00 84.0 .105 .157E+00 .419E+00 -.138E+06 77.8 .212 .162E+00 .435E+00 -.033 -.095 .1548E+00 .101E+00 .156E+00 .600E+00 .533E-01 .264E+00 87.0 .052 .194E+00 .398E+00 -.146E+06 80.7 .161 .198E+00 .408E+00 -.021 -.119 .1924E+00 .147E+00 .157E+00 .429E+00 .455E-01 .241E+00 90.0 .000 .229E+00 .429E+00 -.154E+06 83.7 .110 .232E+00 .435E+00 -.012 -.137 .2283E+00 .190E+00 .209E+00 .318E+00 .386E-01 .220E+00 93.0 -.052 .258E+00 .490E+00 -.162E+06 86.7 .058 .258E+00 .491E+00 -.005 -.150 .2573E+00 .225E+00 .291E+00 .245E+00 .324E-01 .199E+00 96.0 -.105 .278E+00 .564E+00 -.170E+06 89.7 .005 .275E+00 .559E+00 .000 -.158 .2776E+00 .250E+00 .385E+00 .196E+00 .271E-01 .179E+00 99.0 -.156 .289E+00 .642E+00 -.178E+06 92.7 -.047 .283E+00 .629E+00 .003 -.163 .2888E+00 .266E+00 .481E+00 .161E+00 .225E-01 .161E+00 102.0 -.208 .292E+00 .717E+00 -.186E+06 95.8 -.100 .282E+00 .694E+00 .005 -.165 .2921E+00 .273E+00 .573E+00 .136E+00 .187E-01 .144E+00 105.0 -.259 .289E+00 .785E+00 -.194E+06 98.8 -.153 .276E+00 .751E+00 .006 -.165 .2889E+00 .273E+00 .656E+00 .116E+00 .155E-01 .129E+00 108.0 -.309 .281E+00 .843E+00 -.202E+06 101.9 -.206 .266E+00 .797E+00 .005 -.164 .2810E+00 .268E+00 .729E+00 .101E+00 .128E-01 .114E+00 111.0 -.358 .270E+00 .891E+00 -.209E+06 105.0 -.258 .252E+00 .833E+00 .003 -.161 .2699E+00 .259E+00 .790E+00 .895E-01 .106E-01 .101E+00 114.0 -.407 .257E+00 .929E+00 -.217E+06 108.1 -.310 .237E+00 .859E+00 .001 -.157 .2569E+00 .248E+00 .840E+00 .801E-01 .883E-02 .897E-01 117.0 -.454 .243E+00 .957E+00 -.224E+06 111.2 -.362 .222E+00 .875E+00 -.003 -.153 .2429E+00 .236E+00 .878E+00 .725E-01 .734E-02 .790E-01 120.0 -.500 .229E+00 .976E+00 -.231E+06 114.4 -.412 .207E+00 .883E+00 -.007 -.149 .2287E+00 .223E+00 .906E+00 .666E-01 .611E-02 .692E-01 123.0 -.545 .215E+00 .985E+00 -.238E+06 117.5 -.462 .192E+00 .882E+00 -.011 -.144 .2147E+00 .210E+00 .925E+00 .620E-01 .509E-02 .604E-01 126.0 -.588 .201E+00 .986E+00 -.245E+06 120.7 -.510 .178E+00 .874E+00 -.016 -.139 .2012E+00 .197E+00 .934E+00 .585E-01 .424E-02 .524E-01 129.0 -.629 .189E+00 .979E+00 -.251E+06 123.9 -.558 .166E+00 .859E+00 -.021 -.134 .1885E+00 .185E+00 .934E+00 .560E-01 .353E-02 .452E-01 132.0 -.669 .177E+00 .966E+00 -.257E+06 127.1 -.603 .154E+00 .840E+00 -.026 -.129 .1766E+00 .174E+00 .928E+00 .542E-01 .293E-02 .386E-01 135.0 -.707 .166E+00 .948E+00 -.263E+06 130.3 -.647 .143E+00 .816E+00 -.031 -.124 .1658E+00 .163E+00 .915E+00 .530E-01 .242E-02 .328E-01 138.0 -.743 .157E+00 .925E+00 -.269E+06 133.6 -.689 .134E+00 .789E+00 -.036 -.119 .1563E+00 .154E+00 .897E+00 .521E-01 .199E-02 .276E-01 141.0 -.777 .148E+00 .900E+00 -.274E+06 136.8 -.729 .126E+00 .761E+00 -.041 -.114 .1481E+00 .146E+00 .876E+00 .512E-01 .164E-02 .231E-01 144.0 -.809 .142E+00 .873E+00 -.279E+06 140.1 -.767 .119E+00 .733E+00 -.046 -.109 .1413E+00 .140E+00 .854E+00 .501E-01 .134E-02 .190E-01 147.0 -.839 .136E+00 .846E+00 -.283E+06 143.4 -.802 .114E+00 .705E+00 -.050 -.105 .1360E+00 .135E+00 .830E+00 .485E-01 .109E-02 .155E-01 150.0 -.866 .133E+00 .820E+00 -.288E+06 146.7 -.835 .110E+00 .679E+00 -.055 -.101 .1322E+00 .131E+00 .808E+00 .464E-01 .879E-03 .125E-01 153.0 -.891 .130E+00 .797E+00 -.291E+06 150.0 -.866 .107E+00 .656E+00 -.058 -.097 .1297E+00 .129E+00 .787E+00 .437E-01 .703E-03 .990E-02 156.0 -.914 .129E+00 .777E+00 -.295E+06 153.3 -.893 .105E+00 .635E+00 -.062 -.095 .1284E+00 .128E+00 .769E+00 .403E-01 .554E-03 .767E-02 159.0 -.934 .129E+00 .759E+00 -.298E+06 156.6 -.918 .105E+00 .618E+00 -.065 -.093 .1282E+00 .128E+00 .754E+00 .364E-01 .427E-03 .577E-02 162.0 -.951 .129E+00 .745E+00 -.301E+06 159.9 -.939 .105E+00 .604E+00 -.067 -.091 .1287E+00 .128E+00 .741E+00 .319E-01 .318E-03 .419E-02 165.0 -.966 .130E+00 .735E+00 -.303E+06 163.3 -.958 .105E+00 .593E+00 -.070 -.090 .1297E+00 .129E+00 .732E+00 .271E-01 .225E-03 .288E-02 168.0 -.978 .131E+00 .727E+00 -.305E+06 166.6 -.973 .106E+00 .585E+00 -.071 -.089 .1309E+00 .131E+00 .725E+00 .219E-01 .147E-03 .183E-02 171.0 -.988 .133E+00 .721E+00 -.306E+06 169.9 -.985 .106E+00 .579E+00 -.073 -.089 .1322E+00 .132E+00 .720E+00 .166E-01 .842E-04 .103E-02 174.0 -.995 .134E+00 .718E+00 -.307E+06 173.3 -.993 .107E+00 .575E+00 -.074 -.089 .1333E+00 .133E+00 .717E+00 .111E-01 .380E-04 .455E-03 177.0 -.999 .134E+00 .716E+00 -.308E+06 176.6 -.998 .108E+00 .573E+00 -.074 -.089 .1340E+00 .134E+00 .716E+00 .557E-02 .959E-05 .114E-03 180.0 -1.000 .135E+00 .715E+00 -.308E+06 180.0 -1.000 .108E+00 .572E+00 -.074 -.089 .1343E+00 .134E+00 .715E+00 .104E-03 .373E-15 .439E-14 total cross-section = 326.819 elast , inel cross-section = 116.787 210.032 cross-sections in millibarns --------- energy(kinetic),gamcoul= 200.0 .147E-01 born approx total = 424.654 elastic sigma= 227.461 SIG(TH) 200.0 2 3 0 101733001 0 0 0 0 0 3 0 0 1 0 .10E+04+ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .428 .208 .674 .456 .134 .699 . . . . . . . .+ . . . . . . . . . . . . . . . . . . . . . . . . . . . .32E+03. . . . . . . . . . . . . . . . . . . . . . + . . . . . . . . . . . . . 000++ . . . . . . .10E+03. . 0+. . . . . . . . . . . . . . . . . . . . . . . . . . . . . ++ . . . . . . . + . . . . . . . +. . . . . . . + . . . . . . .+ . . . . . .32E+02. . + . . . . . . . + . . . . . . . . . . . . . . + . . . . . . . + . . . . . . . . . . . . .10E+02. . . . . . . . + . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . + . . . . . . . . . . . . . . + . . . . . . . . . . . . .32E+01. . +. . . . . . . . . . . . . . + . . . . . . . . . . . . . .+ . . . . . . .0 . . . . .10E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . + . . . . . . . 0 . . . . . . . . . . . . . . + . . . . . . . . . . . .32E+00. . . 0 . . . . . . . + . ++++++ . . . . . . ++0 0+++ . . . . . +0 .+++ . . . . . 0+ +0. . ++++ . . . . . + . . 0+++++++++++++ .10E+00. . . . . . . . . . . . . + 0 . . . . . . . . . . . . . . . . . . . . . . . . . . 0 . . . . . . . 0 . . . . . . . . . . . . . . 0 . . . . .32E-01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .10E-01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . SIG(TH) 200.0 2 3 0 101733001 0 0 0 0 0 3 0 0 1 0 .10E+02+++++++++++++++++ . . . . . . . . . . . . . . . . . . . . . . .428 .208 .674 .456 .134 .699 . . . . . . . . . + . . . . . . . . . . . . . . + . . . . . . . . . . . . .32E+01. . +. . . . . . . . . . . . . . + . . . . . . . . . . . . . .+ . . . . . . . . . . . .10E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . + . . . . . . . . . . . . . . . . . . . . . + . . . . . . . . . . . .32E+00. . . . . . . . . . + . ++++++ . . . . . . ++ +++ . . . . . +. .+++ . . . . 000 . + + . . ++++ . . . .0000 0000 + . . +++++++++++++ .10E+00. . . . . 0 . . . . . 00. + . . . . . . . . . . . . . . . . . . 0. . 0 . . . . . 0 . . 00 . . . . . 0 . . 0 . . . . . 0 . . 0 . . . . . . . 00 . . . .32E-01. 0 . . .0 . . . . . . . 0 . . . . 0 . . . 0 . . . . . . . 0 . . . . . . . 0 . . . . 0 . . . 0 . . . .10E-01. . . . . . . . . . . . . . . . . . .0. . . . . . . . . . . . . . . . 0 . . . . . . . 0. . . . 0 . . . 0 . . . . . . .0 . . . . . . . 0 . . .32E-02. . . . . 0 . . . . . . . 0 . . . . . . . 0 . . . . . . . 0 . . .0 . . . . 0 . . . . . . . 0 . . .10E-02. . . . . . . . . . . . . . . . . . . . . . . . .0. . . . . . . . . . . 0 . . . . . . .0 . . . . . . . . . . . . . . 0 . . . . . . . 0 . .32E-03. . . . . . 0 . . . . . . . . . . . . . . 0 . . . . . . . . . . . . . . 0 . . . . . . . . .10E-030 . . . . . . . . . . . . . . . . . . . . . . . . . . . .0000 POLAR 200.0 2 3 0 101733001 0 0 0 0 0 3 0 0 1 0 .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .428 .208 .674 .456 .134 .699 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . + . . . . . . . . . . . . . . . . . . . . . . . . . . . . + + . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . + . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . + . . . . . . . +. . . . . . . . . . . . . . . . . . . . . + . . . .15E+01. . . + . . . . . . . .+ . . . . . . . + . . . . . . + . ++ . . . . . .+ . +++ . . . . . + . ++++++++++++++ . .15E+01. . ++++. . . . +++++++++ ---------------- . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 200.0000 339.5780 3139.1188 277.5801 309.5661 relativistic calculation energy momentum 200.0000 277.5801 ----- angular momentum = 0----- OPT POTEN VALUES FOR KP=K0= 277.580AND L=1 K REV VC RABS(N0 FLIP) RABS(FLIP)IMV IMVABS(NOFLIP),IMABS(FLIP) .1479E+01 .3165E-08 .0000E+00 -.164E-08 .000E+00 .9882E-07 -.499E-07 .000E+00 .7912E+01 .2170E-07 .0000E+00 -.742E-09 .000E+00 .2878E-06 -.563E-07 .000E+00 .1999E+02 .6865E-07 .0000E+00 .935E-09 .000E+00 .7594E-06 -.896E-07 .000E+00 .3868E+02 .1292E-06 .0000E+00 .350E-08 .000E+00 .1409E-05 -.156E-06 .000E+00 .6556E+02 .2058E-06 .0000E+00 .706E-08 .000E+00 .2236E-05 -.241E-06 .000E+00 .1032E+03 .2791E-06 .0000E+00 .116E-07 .000E+00 .3092E-05 -.325E-06 .000E+00 .1556E+03 .3030E-06 .0000E+00 .168E-07 .000E+00 .3670E-05 -.369E-06 .000E+00 .2294E+03 .2288E-06 .0000E+00 .211E-07 .000E+00 .3617E-05 -.336E-06 .000E+00 .3359E+03 -.2266E-07 .0000E+00 .213E-07 .000E+00 .2790E-05 -.225E-06 .000E+00 .4952E+03 -.3188E-06 .0000E+00 .140E-07 .000E+00 .1423E-05 -.923E-07 .000E+00 .7467E+03 -.1834E-06 .0000E+00 .333E-08 .000E+00 .1663E-06 -.139E-07 .000E+00 .1175E+04 .1818E-07 .0000E+00 .485E-10 .000E+00 -.6518E-08 -.136E-09 .000E+00 .1992E+04 -.1243E-10 .0000E+00 .452E-16 .000E+00 .8916E-16 -.892E-16 .000E+00 .3854E+04 .3632E-14 .0000E+00 .259E-42 .000E+00 .3595E-42 -.360E-42 .000E+00 .9739E+04 .9597E-34 .0000E+00 .000E+00 .000E+00 .0000E+00 .000E+00 .000E+00 .5210E+05 -.3014E-71 .0000E+00 .000E+00 .000E+00 .0000E+00 .000E+00 .000E+00 TRUE 2N ANNIHILATION PARAMS FOR K(=KP=K0): IMB,REB,IMC,REC/ THEN, RE, IM VABS(L) FLIP+NOFLIP 277.580 .80077E-10 -.80077E-10 .99041E-14 .00000E+00 .75875E-07 -.28556E-06 .00000E+00 .00000E+00 .22003E-07 -.28809E-06 .00000E+00 .00000E+00 .39446E-08 -.90736E-07 .00000E+00 .00000E+00 .51036E-09 -.16902E-07 .00000E+00 .00000E+00 .51602E-10 -.22359E-08 .00000E+00 .00000E+00 .42798E-11 -.22937E-09 .00000E+00 .00000E+00 .30082E-12 -.19219E-10 .00000E+00 .00000E+00 .18343E-13 -.13612E-11 .00000E+00 .00000E+00 .98762E-15 -.83490E-13 .00000E+00 .00000E+00 OPT POTEN VALUES FOR KP=K0= 277.580AND L=1 K REV VC RABS(N0 FLIP) RABS(FLIP)IMV IMVABS(NOFLIP),IMABS(FLIP) .2776E+03 .1241E-06 .0000E+00 .220E-07 .000E+00 .3287E-05 -.288E-06 .000E+00 determinant from matrix inversion= .6508987E+00 unnormalized r matrix(re,im,re,-im) .9563384E-06 -.2235482E-05 .9563384E-06 .2235482E-05 normalized r(k,k..k)= -.1486290E+00 .3474267E+00 t(k,k,k)= -.1213199E+00 .4001492E+00 eta= .3143 delta= -25.2722 coulomb phase modified nuclear amplitude t(k,k.k) = -.1281005E+00 .3980303E+00 born approximation normalized r(k,k..k)= -.4564154E-01 .3701574E+00 t(k,k,k)= -.6846231E-01 .5552360E+00 eta= .1759 delta= -64.4484 determinant from matrix inversion= .6508987E+00 unnormalized r matrix(re,im,re,-im) .9563384E-06 -.2235482E-05 .9563384E-06 .2235482E-05 normalized r(k,k..k)= -.1486290E+00 .3474267E+00 t(k,k,k)= -.1213199E+00 .4001492E+00 eta= .3143 delta= -25.2722 coulomb phase modified nuclear amplitude t(k,k.k) = -.1281005E+00 .3980303E+00 born approximation normalized r(k,k..k)= -.4564154E-01 .3701574E+00 t(k,k,k)= -.6846231E-01 .5552360E+00 eta= .1759 delta= -64.4484 ----- angular momentum = 1----- determinant from matrix inversion= .6136903E+00 unnormalized r matrix(re,im,re,-im) .7463726E-06 -.3308168E-05 .7463726E-06 .3308168E-05 normalized r(k,k..k)= -.1159972E+00 .5141377E+00 t(k,k,k)= -.7545130E-01 .5151174E+00 eta= .1539 delta= -50.6649 coulomb phase modified nuclear amplitude t(k,k.k) = -.6903425E-01 .5160166E+00 born approximation normalized r(k,k..k)= -.1928634E-01 .5109231E+00 t(k,k,k)= -.2892950E-01 .7663847E+00 eta= .5359 delta= -86.9010 determinant from matrix inversion= .6973396E+00 unnormalized r matrix(re,im,re,-im) .4452902E-06 -.1440638E-05 .4452902E-06 .1440638E-05 normalized r(k,k..k)= -.6920462E-01 .2238962E+00 t(k,k,k)= -.6907976E-01 .2783120E+00 eta= .4644 delta= -8.6537 coulomb phase modified nuclear amplitude t(k,k.k) = -.6561051E-01 .2791502E+00 born approximation normalized r(k,k..k)= -.4739446E-01 .2269984E+00 t(k,k,k)= -.7109169E-01 .3404976E+00 eta= .3493 delta= -12.0115 ----- angular momentum = 2----- determinant from matrix inversion= .6294839E+00 unnormalized r matrix(re,im,re,-im) .2527612E-06 -.1654784E-05 .2527612E-06 .1654784E-05 normalized r(k,k..k)= -.3928279E-01 .2571777E+00 t(k,k,k)= -.3724573E-01 .3080150E+00 eta= .3911 delta= -5.4896 coulomb phase modified nuclear amplitude t(k,k.k) = -.2886571E-01 .3089131E+00 born approximation normalized r(k,k..k)= .1367982E-01 .2465605E+00 t(k,k,k)= .2051973E-01 .3698407E+00 eta= .2635 delta= 4.4795 determinant from matrix inversion= .7519010E+00 unnormalized r matrix(re,im,re,-im) .1614228E-06 -.8006455E-06 .1614228E-06 .8006455E-06 normalized r(k,k..k)= -.2508747E-01 .1244320E+00 t(k,k,k)= -.2974853E-01 .1666569E+00 eta= .6693 delta= -2.5499 coulomb phase modified nuclear amplitude t(k,k.k) = -.2521083E-01 .1674035E+00 born approximation normalized r(k,k..k)= -.1258159E-01 .1247456E+00 t(k,k,k)= -.1887239E-01 .1871184E+00 eta= .6269 delta= -1.7259 ----- angular momentum = 3----- determinant from matrix inversion= .6734654E+00 unnormalized r matrix(re,im,re,-im) -.1680736E-07 -.5386489E-06 -.1680736E-07 .5386489E-06 normalized r(k,k..k)= .2612109E-02 .8371393E-01 t(k,k,k)= .3336190E-02 .1158789E+00 eta= .7683 delta= .2488 coulomb phase modified nuclear amplitude t(k,k.k) = .7617890E-02 .1156764E+00 born approximation normalized r(k,k..k)= .1084338E-01 .7875909E-01 t(k,k,k)= .1626507E-01 .1181386E+00 eta= .7644 delta= 1.2195 determinant from matrix inversion= .7873596E+00 unnormalized r matrix(re,im,re,-im) .1614261E-07 -.2771703E-06 .1614261E-07 .2771703E-06 normalized r(k,k..k)= -.2508798E-02 .4307633E-01 t(k,k,k)= -.3458774E-02 .6195441E-01 eta= .8761 delta= -.2262 coulomb phase modified nuclear amplitude t(k,k.k) = -.1165989E-02 .6203993E-01 born approximation normalized r(k,k..k)= -.1365974E-03 .4243280E-01 t(k,k,k)= -.2048961E-03 .6364920E-01 eta= .8727 delta= -.0135 ----- angular momentum = 4----- determinant from matrix inversion= .7525667E+00 unnormalized r matrix(re,im,re,-im) -.2248086E-07 -.1443499E-06 -.2248086E-07 .1443499E-06 normalized r(k,k..k)= .3493855E-02 .2243409E-01 t(k,k,k)= .5013262E-02 .3292990E-01 eta= .9342 delta= .3075 coulomb phase modified nuclear amplitude t(k,k.k) = .6467882E-02 .3267533E-01 born approximation normalized r(k,k..k)= .4207490E-02 .2168920E-01 t(k,k,k)= .6311235E-02 .3253380E-01 eta= .9350 delta= .3868 determinant from matrix inversion= .8328800E+00 unnormalized r matrix(re,im,re,-im) -.3081949E-08 -.8220348E-07 -.3081949E-08 .8220348E-07 normalized r(k,k..k)= .4789801E-03 .1277563E-01 t(k,k,k)= .7004581E-03 .1892203E-01 eta= .9622 delta= .0417 coulomb phase modified nuclear amplitude t(k,k.k) = .1538448E-02 .1887239E-01 born approximation normalized r(k,k..k)= .7296726E-03 .1263817E-01 t(k,k,k)= .1094509E-02 .1895725E-01 eta= .9621 delta= .0652 ----- angular momentum = 5----- determinant from matrix inversion= .8206640E+00 unnormalized r matrix(re,im,re,-im) -.7871213E-08 -.3716659E-07 -.7871213E-08 .3716659E-07 normalized r(k,k..k)= .1223302E-02 .5776233E-02 t(k,k,k)= .1813934E-02 .8616795E-02 eta= .9828 delta= .1058 coulomb phase modified nuclear amplitude t(k,k.k) = .2244244E-02 .8514863E-02 born approximation normalized r(k,k..k)= .1279061E-02 .5700784E-02 t(k,k,k)= .1918592E-02 .8551176E-02 eta= .9829 delta= .1118 determinant from matrix inversion= .8743594E+00 unnormalized r matrix(re,im,re,-im) -.1990495E-08 -.2380439E-07 -.1990495E-08 .2380439E-07 normalized r(k,k..k)= .3093521E-03 .3699550E-02 t(k,k,k)= .4606137E-03 .5529013E-02 eta= .9889 delta= .0267 coulomb phase modified nuclear amplitude t(k,k.k) = .7376108E-03 .5498916E-02 born approximation normalized r(k,k..k)= .3338780E-03 .3682869E-02 t(k,k,k)= .5008170E-03 .5524303E-02 eta= .9890 delta= .0290 ----- angular momentum = 6----- born approximation normalized r(k,k..k)= .3047728E-03 .1876719E-02 t(k,k,k)= .4571592E-03 .2815079E-02 eta= .9944 delta= .0263 t(k,k,k)= .4554481E-03 .2809944E-02 eta= .9944 delta= .0262 coulomb phase modified nuclear amplitude t(k,k.k) = .6095937E-03 .2780578E-02 born approximation normalized r(k,k..k)= .7471844E-04 .1298349E-02 t(k,k,k)= .1120777E-03 .1947523E-02 eta= .9961 delta= .0064 t(k,k,k)= .1117872E-03 .1945006E-02 eta= .9961 delta= .0064 coulomb phase modified nuclear amplitude t(k,k.k) = .2187939E-03 .1935891E-02 ----- angular momentum = 7----- born approximation normalized r(k,k..k)= .3813617E-04 .8164090E-03 t(k,k,k)= .5720426E-04 .1224614E-02 eta= .9976 delta= .0033 t(k,k,k)= .5711097E-04 .1223617E-02 eta= .9976 delta= .0033 coulomb phase modified nuclear amplitude t(k,k.k) = .1295734E-03 .1218076E-02 born approximation normalized r(k,k..k)= -.1904919E-04 .7349388E-03 t(k,k,k)= -.2857378E-04 .1102408E-02 eta= .9978 delta= -.0016 t(k,k,k)= -.2853183E-04 .1101599E-02 eta= .9978 delta= -.0016 coulomb phase modified nuclear amplitude t(k,k.k) = .3684541E-04 .1101352E-02 ----- angular momentum = 8----- born approximation normalized r(k,k..k)= .1000330E-04 .2525654E-03 t(k,k,k)= .1500495E-04 .3788481E-03 eta= .9992 delta= .0009 t(k,k,k)= .1499737E-04 .3787526E-03 eta= .9992 delta= .0009 coulomb phase modified nuclear amplitude t(k,k.k) = .3881950E-04 .3770563E-03 born approximation normalized r(k,k..k)= -.1051001E-04 .2353374E-03 t(k,k,k)= -.1576502E-04 .3530061E-03 eta= .9993 delta= -.0009 t(k,k,k)= -.1575760E-04 .3529232E-03 eta= .9993 delta= -.0009 coulomb phase modified nuclear amplitude t(k,k.k) = .6498970E-05 .3532151E-03 th-c.m. cos(cm) dsig/dw-cm ds/dw(b.a.) t th-lab cos(lab) ds/dw ds/dw(b.a.) ref(th)-cm imf signuc noflip noflip-b polar flip flip-b .0 1.000 .472E+13 .472E+13 .000E+00 .0 1.000 .587E+13 .587E+13 -.269 2.838 .8125E+02 .813E+02 .472E+13 .114E-03 .000E+00 .000E+00 3.0 .999 .581E+03 .649E+03 -.211E+03 2.7 .999 .722E+03 .807E+03 -.270 2.824 .8051E+02 .805E+02 .649E+03 .612E-02 .196E-01 .328E-01 6.0 .995 .966E+02 .145E+03 -.844E+03 5.4 .996 .120E+03 .180E+03 -.271 2.784 .7832E+02 .782E+02 .145E+03 .123E-01 .770E-01 .129E+00 9.0 .988 .746E+02 .118E+03 -.190E+04 8.1 .990 .926E+02 .146E+03 -.272 2.719 .7481E+02 .746E+02 .118E+03 .186E-01 .168E+00 .282E+00 12.0 .978 .686E+02 .109E+03 -.337E+04 10.8 .982 .849E+02 .135E+03 -.274 2.630 .7018E+02 .699E+02 .108E+03 .252E-01 .285E+00 .483E+00 15.0 .966 .633E+02 .101E+03 -.525E+04 13.5 .973 .782E+02 .125E+03 -.276 2.520 .6469E+02 .643E+02 .100E+03 .320E-01 .420E+00 .717E+00 18.0 .951 .575E+02 .923E+02 -.754E+04 16.2 .960 .709E+02 .114E+03 -.277 2.393 .5859E+02 .580E+02 .914E+02 .392E-01 .564E+00 .972E+00 21.0 .934 .514E+02 .834E+02 -.102E+05 18.9 .946 .631E+02 .102E+03 -.279 2.251 .5217E+02 .515E+02 .822E+02 .469E-01 .706E+00 .123E+01 24.0 .914 .451E+02 .742E+02 -.133E+05 21.6 .930 .552E+02 .908E+02 -.279 2.099 .4569E+02 .449E+02 .728E+02 .551E-01 .838E+00 .148E+01 27.0 .891 .389E+02 .652E+02 -.168E+05 24.3 .911 .474E+02 .794E+02 -.278 1.940 .3937E+02 .384E+02 .635E+02 .641E-01 .953E+00 .171E+01 30.0 .866 .330E+02 .565E+02 -.206E+05 27.0 .891 .400E+02 .684E+02 -.275 1.777 .3338E+02 .323E+02 .546E+02 .739E-01 .105E+01 .191E+01 33.0 .839 .276E+02 .483E+02 -.249E+05 29.7 .868 .333E+02 .582E+02 -.271 1.613 .2787E+02 .268E+02 .462E+02 .847E-01 .111E+01 .208E+01 36.0 .809 .227E+02 .408E+02 -.294E+05 32.5 .844 .272E+02 .489E+02 -.265 1.451 .2290E+02 .218E+02 .386E+02 .969E-01 .115E+01 .220E+01 39.0 .777 .184E+02 .340E+02 -.343E+05 35.2 .817 .219E+02 .405E+02 -.258 1.293 .1853E+02 .174E+02 .317E+02 .111E+00 .116E+01 .227E+01 42.0 .743 .146E+02 .280E+02 -.396E+05 38.0 .788 .173E+02 .331E+02 -.248 1.140 .1476E+02 .136E+02 .257E+02 .126E+00 .115E+01 .231E+01 45.0 .707 .115E+02 .228E+02 -.451E+05 40.7 .758 .135E+02 .267E+02 -.237 .994 .1156E+02 .105E+02 .205E+02 .145E+00 .111E+01 .230E+01 48.0 .669 .883E+01 .183E+02 -.510E+05 43.5 .725 .103E+02 .213E+02 -.225 .857 .8904E+01 .785E+01 .160E+02 .166E+00 .105E+01 .226E+01 51.0 .629 .668E+01 .145E+02 -.571E+05 46.3 .691 .772E+01 .168E+02 -.211 .729 .6739E+01 .575E+01 .123E+02 .192E+00 .986E+00 .219E+01 54.0 .588 .496E+01 .114E+02 -.635E+05 49.1 .655 .569E+01 .130E+02 -.196 .609 .5008E+01 .410E+01 .926E+01 .224E+00 .908E+00 .209E+01 57.0 .545 .361E+01 .878E+01 -.702E+05 51.9 .617 .411E+01 .998E+01 -.181 .500 .3652E+01 .283E+01 .680E+01 .263E+00 .824E+00 .198E+01 60.0 .500 .259E+01 .671E+01 -.771E+05 54.7 .578 .291E+01 .756E+01 -.165 .401 .2615E+01 .188E+01 .486E+01 .311E+00 .737E+00 .185E+01 63.0 .454 .182E+01 .508E+01 -.841E+05 57.5 .537 .203E+01 .567E+01 -.149 .311 .1841E+01 .119E+01 .336E+01 .372E+00 .652E+00 .171E+01 66.0 .407 .126E+01 .381E+01 -.914E+05 60.4 .494 .140E+01 .421E+01 -.133 .231 .1281E+01 .711E+00 .223E+01 .446E+00 .569E+00 .157E+01 69.0 .358 .875E+00 .285E+01 -.989E+05 63.3 .450 .957E+00 .311E+01 -.117 .161 .8879E+00 .397E+00 .141E+01 .533E+00 .491E+00 .143E+01 72.0 .309 .614E+00 .213E+01 -.106E+06 66.1 .405 .665E+00 .231E+01 -.102 .100 .6239E+00 .204E+00 .836E+00 .623E+00 .420E+00 .129E+01 75.0 .259 .447E+00 .161E+01 -.114E+06 69.0 .358 .479E+00 .173E+01 -.088 .047 .4547E+00 .100E+00 .453E+00 .698E+00 .355E+00 .116E+01 78.0 .208 .348E+00 .125E+01 -.122E+06 71.9 .310 .369E+00 .133E+01 -.075 .003 .3531E+00 .563E-01 .216E+00 .727E+00 .297E+00 .104E+01 81.0 .156 .293E+00 .101E+01 -.130E+06 74.8 .261 .307E+00 .106E+01 -.063 -.034 .2971E+00 .511E-01 .887E-01 .692E+00 .246E+00 .918E+00 84.0 .105 .267E+00 .848E+00 -.138E+06 77.8 .212 .277E+00 .879E+00 -.052 -.064 .2703E+00 .681E-01 .384E-01 .603E+00 .202E+00 .809E+00 87.0 .052 .259E+00 .751E+00 -.146E+06 80.7 .161 .265E+00 .769E+00 -.042 -.088 .2606E+00 .958E-01 .409E-01 .489E+00 .165E+00 .710E+00 90.0 .000 .258E+00 .697E+00 -.154E+06 83.7 .110 .262E+00 .706E+00 -.033 -.107 .2599E+00 .127E+00 .774E-01 .377E+00 .133E+00 .620E+00 93.0 -.052 .262E+00 .672E+00 -.162E+06 86.7 .058 .262E+00 .674E+00 -.026 -.122 .2627E+00 .156E+00 .134E+00 .280E+00 .107E+00 .539E+00 96.0 -.105 .265E+00 .667E+00 -.170E+06 89.7 .005 .263E+00 .660E+00 -.020 -.133 .2659E+00 .180E+00 .200E+00 .202E+00 .856E-01 .466E+00 99.0 -.156 .267E+00 .673E+00 -.178E+06 92.7 -.047 .262E+00 .659E+00 -.015 -.141 .2677E+00 .200E+00 .270E+00 .139E+00 .681E-01 .403E+00 102.0 -.208 .267E+00 .685E+00 -.186E+06 95.8 -.100 .258E+00 .663E+00 -.011 -.146 .2674E+00 .213E+00 .338E+00 .902E-01 .541E-01 .346E+00 105.0 -.259 .264E+00 .699E+00 -.194E+06 98.8 -.153 .253E+00 .669E+00 -.008 -.149 .2646E+00 .222E+00 .402E+00 .510E-01 .429E-01 .297E+00 108.0 -.309 .259E+00 .714E+00 -.202E+06 101.9 -.206 .245E+00 .675E+00 -.006 -.150 .2595E+00 .226E+00 .459E+00 .195E-01 .340E-01 .254E+00 111.0 -.358 .252E+00 .726E+00 -.209E+06 105.0 -.258 .236E+00 .679E+00 -.005 -.150 .2522E+00 .225E+00 .509E+00 -.622E-02 .270E-01 .217E+00 114.0 -.407 .243E+00 .735E+00 -.217E+06 108.1 -.310 .225E+00 .680E+00 -.005 -.149 .2430E+00 .221E+00 .550E+00 -.275E-01 .216E-01 .185E+00 117.0 -.454 .232E+00 .741E+00 -.224E+06 111.2 -.362 .212E+00 .677E+00 -.005 -.146 .2322E+00 .215E+00 .584E+00 -.452E-01 .174E-01 .157E+00 120.0 -.500 .220E+00 .742E+00 -.231E+06 114.4 -.412 .199E+00 .671E+00 -.006 -.143 .2203E+00 .206E+00 .609E+00 -.600E-01 .141E-01 .133E+00 123.0 -.545 .207E+00 .738E+00 -.238E+06 117.5 -.462 .186E+00 .661E+00 -.008 -.140 .2076E+00 .196E+00 .626E+00 -.722E-01 .116E-01 .113E+00 126.0 -.588 .194E+00 .731E+00 -.245E+06 120.7 -.510 .172E+00 .648E+00 -.009 -.136 .1945E+00 .185E+00 .636E+00 -.821E-01 .956E-02 .947E-01 129.0 -.629 .181E+00 .720E+00 -.251E+06 123.9 -.558 .159E+00 .632E+00 -.012 -.131 .1815E+00 .174E+00 .641E+00 -.898E-01 .796E-02 .794E-01 132.0 -.669 .169E+00 .707E+00 -.257E+06 127.1 -.603 .147E+00 .614E+00 -.014 -.127 .1689E+00 .162E+00 .640E+00 -.954E-01 .667E-02 .662E-01 135.0 -.707 .157E+00 .691E+00 -.263E+06 130.3 -.647 .135E+00 .595E+00 -.017 -.122 .1571E+00 .152E+00 .636E+00 -.987E-01 .562E-02 .549E-01 138.0 -.743 .146E+00 .674E+00 -.269E+06 133.6 -.689 .125E+00 .575E+00 -.020 -.117 .1463E+00 .142E+00 .629E+00 -.999E-01 .473E-02 .452E-01 141.0 -.777 .137E+00 .656E+00 -.274E+06 136.8 -.729 .116E+00 .555E+00 -.022 -.113 .1367E+00 .133E+00 .620E+00 -.990E-01 .396E-02 .369E-01 144.0 -.809 .128E+00 .639E+00 -.279E+06 140.1 -.767 .108E+00 .537E+00 -.025 -.109 .1284E+00 .125E+00 .609E+00 -.961E-01 .330E-02 .298E-01 147.0 -.839 .121E+00 .622E+00 -.283E+06 143.4 -.802 .101E+00 .519E+00 -.028 -.105 .1212E+00 .118E+00 .599E+00 -.916E-01 .272E-02 .237E-01 150.0 -.866 .115E+00 .606E+00 -.288E+06 146.7 -.835 .951E-01 .502E+00 -.031 -.102 .1152E+00 .113E+00 .588E+00 -.857E-01 .221E-02 .186E-01 153.0 -.891 .110E+00 .592E+00 -.291E+06 150.0 -.866 .904E-01 .487E+00 -.033 -.099 .1101E+00 .108E+00 .577E+00 -.787E-01 .176E-02 .144E-01 156.0 -.914 .106E+00 .578E+00 -.295E+06 153.3 -.893 .865E-01 .473E+00 -.035 -.096 .1060E+00 .105E+00 .567E+00 -.709E-01 .137E-02 .108E-01 159.0 -.934 .102E+00 .565E+00 -.298E+06 156.6 -.918 .833E-01 .460E+00 -.037 -.094 .1026E+00 .102E+00 .558E+00 -.626E-01 .103E-02 .795E-02 162.0 -.951 .996E-01 .554E+00 -.301E+06 159.9 -.939 .807E-01 .449E+00 -.039 -.092 .9987E-01 .991E-01 .549E+00 -.540E-01 .742E-03 .561E-02 165.0 -.966 .974E-01 .545E+00 -.303E+06 163.3 -.958 .786E-01 .440E+00 -.041 -.090 .9764E-01 .971E-01 .541E+00 -.452E-01 .507E-03 .376E-02 168.0 -.978 .956E-01 .537E+00 -.305E+06 166.6 -.973 .769E-01 .432E+00 -.042 -.088 .9588E-01 .956E-01 .534E+00 -.363E-01 .319E-03 .233E-02 171.0 -.988 .943E-01 .530E+00 -.306E+06 169.9 -.985 .757E-01 .426E+00 -.043 -.087 .9453E-01 .944E-01 .529E+00 -.273E-01 .177E-03 .128E-02 174.0 -.995 .933E-01 .526E+00 -.307E+06 173.3 -.993 .748E-01 .421E+00 -.044 -.086 .9357E-01 .935E-01 .525E+00 -.182E-01 .780E-04 .558E-03 177.0 -.999 .927E-01 .523E+00 -.308E+06 176.6 -.998 .742E-01 .418E+00 -.044 -.086 .9300E-01 .930E-01 .523E+00 -.910E-02 .194E-04 .138E-03 180.0 -1.000 .926E-01 .522E+00 -.308E+06 180.0 -1.000 .741E-01 .418E+00 -.044 -.086 .9281E-01 .928E-01 .522E+00 -.170E-03 .748E-15 .532E-14 total cross-section = 253.401 elast , inel cross-section = 77.367 176.034 cross-sections in millibarns --------- energy(kinetic),gamcoul= 200.0 -.147E-01 born approx total = 314.249 elastic sigma= 137.768 SIG(TH) 200.0 2 3 0 101733001 0 0 0 0 0 3 0 0 1 0 .10E+04+ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .428 .208 .674 .456 .134 .699 . . . . . . . . . . . . . . .+ . . . . . . . . . . . . . . . . . . . . .32E+03. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .10E+03. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . + . . . . . . 000++ . . . . . . . ++ . . . . . . . + . . . . . . . ++. . . . . . .32E+02. + . . . . . . .+ . . . . . . . + . . . . . . . + . . . . . . . 0 . . . . . . . + . . . . . .10E+02. . . . . . . .+. . . . . . . . . . . . . . . . . . . . . . . . . + . . . . . . . 0 . . . . . . . + . . . . . . . + . . . . . . . 0 . . . . . .32E+01. . +. . . . . . . 0. . . . . . . + . . . . . . 0+ . . . . . . . . . . . . . . + . . . . .10E+01. . . . . . . . . . .0. . . . . . . . . . . . . . . . . . . . . . . + . . . . . . . 0 . . . . . . . + . . . . . . . . . . . . . . 0 + . . . . .32E+00. . . + . . . . . . . ++ .+++++ . . . . . . ++ 0+++++ . . . . . 0 . 000 00+++ . . . . . .0 . 0++ . . . . . 0 . +++ . . .10E+00. . . . . . . . . . . . .0. . . . . . . . . . . .+++++. . . . . . . 0. . . +++++++ . . . . . . . . . . 0 0 . . . . . . . 0 . . . . . . . . . . . .32E-01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .10E-01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . SIG(TH) 200.0 2 3 0 101733001 0 0 0 0 0 3 0 0 1 0 .10E+02++++++++++++++++. . . . . . . . . . . . . . . . . . . . . . . .428 .208 .674 .456 .134 .699 . . + . . . . . . . . . . . . . . + . . . . . . . + . . . . . . . . . . . . .32E+01. . +. . . . . . . . . . . . . . + . . . . . . .+ . . . . . . . . . . . . . . + . . . . .10E+01. . . . . 0000000 . . . . . . . . . . . . . . . . . . . . . . . 00. 00 . + . . . . . 0 . 00 . . . . . 0 . .00 + . . . . . . . 0 . . . . . 0 . . 0+ . . . . .32E+00. . . 0+ . . . . . 0 . . 0++ .+++++ . . . . . . 0 ++ +++++ . . . . . 0 . .+++ . . . 0 . . 0. . ++ . . . . . 0 . +++ . . .10E+00. . . . . . . . . . . . . . . .0. . . . . . . . .+++++. . . . . . . . 0 . . +++++++ . 0 . . . 0 . . . . . . . . . . . . . . 0 . . . . . . . 0 . . . .32E-01. . . . 0 . . . . . . . 0 . . . . . . . 0 . . . .0 . . . . . . . . . . 0. . . . . . . 0 . . .10E-01. . . . . . . . . . . . . . . . . . . . .0. . . . . . . . . . . . . . . 0 . . . . . . . 0 . . . . . . . 0 . . . . . . . 00 . . . . . . . 0 . . .32E-02. . . . . 0 . . . . . . . 0. . . . . . . 0 . . . . . . . . . . . . . .0 . . . . . . . 0 . .10E-02. . . . . . . . . . . . . . . . . . . . . . . . . . .0. . . . . . . . . . . . . . . . . 0 . . . . . . . . . . . . . . 0 . . . . . . . . .32E-03. . . . . . 0 . . . . . . . . . . . . . . . . . . . . . . . . . . . . 0 . . . . . . . . .10E-030 . . . . . . . . . . . . . . . . . . . . . . . . . . . . 000 POLAR 200.0 2 3 0 101733001 0 0 0 0 0 3 0 0 1 0 .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .428 .208 .674 .456 .134 .699 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . + . . . . . . . + + . . . . . . . . . . . . . . + + . . . . . . . . . . . .15E+01. . . . . . . . . . . .+. . . . . . . . . . . . . . . . . . . . . . +. . . . . . . + . . . . . . . + . . . . . .+ . . . . . . + . . . . .15E+01. . +. .+ . . . . . + . . . . . . . + . . + . . . . . +++ . . + . . . . .+++ . . + . . . . ++++ . . + . . . .15E+01+++++++ . . . + . . . . . . . -- . . ----- . . . . ---- .----- . . . . . . -------- . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 3 t(k,k,k)= -.4200096E-01 .6538432E-01 -.4200096E-01 .6538432E-01 t(k,k,k)= -.3934126E-01 .3224251E-01 -.1850380E-01 .1277433E+00 t(k,k,k)= -.3202880E-01 .2283129E-01 -.2185113E-01 .8998392E-01 t(k,k,k)= -.1324994E-01 .1415205E-01 -.5592465E-02 .4306646E-01 t(k,k,k)= -.3684819E-02 .5715251E-02 -.1925411E-03 .1461749E-01 t(k,k,k)= -.9118466E-03 .1597568E-02 .2111155E-03 .4001730E-02 t(k,k,k)= -.1914293E-03 .2195583E-03 .1409287E-03 .8810511E-03 t(k,k,k)= -.1932872E-04 -.1229797E-03 .5939996E-04 -.1310274E-04 t(k,k,k)= .1841919E-04 -.3013585E-03 .4744135E-04 -.2242048E-03 th-c.m. cos(cm) dsig/dw-cm ds/dw(b.a.) t th-lab cos(lab) ds/dw ds/dw(b.a.) ref(th)-cm imf signuc noflip noflip-b polar flip flip-b .0 1.000 .401E+01 .779E+01 .000E+00 .0 1.000 .499E+01 .969E+01 -.264 .576 .4013E+01 .401E+01 .779E+01 -.880E-03 .000E+00 .000E+00 3.0 .999 .398E+01 .773E+01 -.211E+03 2.7 .999 .494E+01 .962E+01 -.263 .572 .3976E+01 .397E+01 .773E+01 -.472E-01 .555E-02 .762E-02 6.0 .995 .387E+01 .756E+01 -.844E+03 5.4 .996 .480E+01 .939E+01 -.260 .563 .3865E+01 .384E+01 .753E+01 -.945E-01 .217E-01 .298E-01 9.0 .988 .369E+01 .727E+01 -.190E+04 8.1 .990 .457E+01 .902E+01 -.254 .547 .3687E+01 .364E+01 .720E+01 -.142E+00 .470E-01 .648E-01 12.0 .978 .345E+01 .688E+01 -.337E+04 10.8 .982 .427E+01 .853E+01 -.247 .526 .3450E+01 .337E+01 .678E+01 -.190E+00 .791E-01 .110E+00 15.0 .966 .317E+01 .642E+01 -.525E+04 13.5 .973 .391E+01 .793E+01 -.237 .499 .3166E+01 .305E+01 .626E+01 -.238E+00 .115E+00 .161E+00 18.0 .951 .285E+01 .589E+01 -.754E+04 16.2 .960 .351E+01 .726E+01 -.226 .468 .2849E+01 .270E+01 .568E+01 -.287E+00 .152E+00 .215E+00 21.0 .934 .251E+01 .532E+01 -.102E+05 18.9 .946 .309E+01 .653E+01 -.213 .433 .2513E+01 .232E+01 .505E+01 -.337E+00 .188E+00 .267E+00 24.0 .914 .217E+01 .473E+01 -.133E+05 21.6 .930 .266E+01 .578E+01 -.199 .395 .2173E+01 .195E+01 .441E+01 -.388E+00 .219E+00 .315E+00 27.0 .891 .184E+01 .414E+01 -.168E+05 24.3 .911 .224E+01 .504E+01 -.183 .355 .1842E+01 .160E+01 .378E+01 -.441E+00 .244E+00 .355E+00 30.0 .866 .153E+01 .357E+01 -.206E+05 27.0 .891 .186E+01 .433E+01 -.168 .314 .1532E+01 .127E+01 .318E+01 -.493E+00 .262E+00 .387E+00 33.0 .839 .125E+01 .303E+01 -.249E+05 29.7 .868 .151E+01 .366E+01 -.151 .274 .1252E+01 .979E+00 .263E+01 -.546E+00 .272E+00 .408E+00 36.0 .809 .101E+01 .254E+01 -.294E+05 32.5 .844 .121E+01 .305E+01 -.135 .234 .1006E+01 .731E+00 .213E+01 -.598E+00 .275E+00 .419E+00 39.0 .777 .798E+00 .211E+01 -.343E+05 35.2 .817 .950E+00 .251E+01 -.119 .197 .7976E+00 .527E+00 .169E+01 -.645E+00 .270E+00 .420E+00 42.0 .743 .626E+00 .173E+01 -.396E+05 38.0 .788 .740E+00 .205E+01 -.103 .161 .6257E+00 .366E+00 .132E+01 -.685E+00 .259E+00 .413E+00 45.0 .707 .488E+00 .141E+01 -.451E+05 40.7 .758 .573E+00 .165E+01 -.088 .129 .4878E+00 .244E+00 .101E+01 -.711E+00 .244E+00 .397E+00 48.0 .669 .380E+00 .114E+01 -.510E+05 43.5 .725 .442E+00 .132E+01 -.074 .100 .3796E+00 .155E+00 .761E+00 -.718E+00 .225E+00 .376E+00 51.0 .629 .296E+00 .914E+00 -.571E+05 46.3 .691 .343E+00 .106E+01 -.060 .075 .2963E+00 .926E-01 .564E+00 -.700E+00 .204E+00 .350E+00 54.0 .588 .233E+00 .733E+00 -.635E+05 49.1 .655 .267E+00 .841E+00 -.048 .054 .2330E+00 .516E-01 .412E+00 -.652E+00 .181E+00 .322E+00 57.0 .545 .185E+00 .588E+00 -.702E+05 51.9 .617 .210E+00 .668E+00 -.037 .035 .1851E+00 .260E-01 .296E+00 -.574E+00 .159E+00 .291E+00 60.0 .500 .149E+00 .471E+00 -.771E+05 54.7 .578 .168E+00 .531E+00 -.027 .021 .1488E+00 .114E-01 .211E+00 -.468E+00 .137E+00 .261E+00 63.0 .454 .121E+00 .379E+00 -.841E+05 57.5 .537 .135E+00 .423E+00 -.018 .009 .1211E+00 .396E-02 .148E+00 -.341E+00 .117E+00 .231E+00 66.0 .407 .995E-01 .305E+00 -.914E+05 60.4 .494 .110E+00 .337E+00 -.010 -.001 .9955E-01 .107E-02 .103E+00 -.201E+00 .985E-01 .202E+00 69.0 .358 .826E-01 .247E+00 -.989E+05 63.3 .450 .903E-01 .270E+00 -.004 -.008 .8258E-01 .787E-03 .710E-01 -.566E-01 .818E-01 .176E+00 72.0 .309 .690E-01 .200E+00 -.106E+06 66.1 .405 .747E-01 .217E+00 .002 -.013 .6897E-01 .181E-02 .492E-01 .844E-01 .672E-01 .151E+00 75.0 .259 .578E-01 .163E+00 -.114E+06 69.0 .358 .620E-01 .175E+00 .006 -.017 .5784E-01 .332E-02 .348E-01 .216E+00 .545E-01 .129E+00 78.0 .208 .486E-01 .135E+00 -.122E+06 71.9 .310 .515E-01 .143E+00 .009 -.020 .4861E-01 .479E-02 .257E-01 .335E+00 .438E-01 .109E+00 81.0 .156 .408E-01 .112E+00 -.130E+06 74.8 .261 .428E-01 .117E+00 .012 -.021 .4083E-01 .595E-02 .204E-01 .438E+00 .349E-01 .914E-01 84.0 .105 .342E-01 .938E-01 -.138E+06 77.8 .212 .354E-01 .972E-01 .014 -.022 .3417E-01 .666E-02 .176E-01 .525E+00 .275E-01 .762E-01 87.0 .052 .284E-01 .796E-01 -.146E+06 80.7 .161 .291E-01 .816E-01 .015 -.022 .2840E-01 .688E-02 .164E-01 .597E+00 .215E-01 .631E-01 90.0 .000 .234E-01 .682E-01 -.154E+06 83.7 .110 .237E-01 .692E-01 .015 -.021 .2336E-01 .665E-02 .163E-01 .657E+00 .167E-01 .520E-01 93.0 -.052 .189E-01 .591E-01 -.162E+06 86.7 .058 .190E-01 .592E-01 .015 -.020 .1895E-01 .605E-02 .166E-01 .706E+00 .129E-01 .425E-01 96.0 -.105 .151E-01 .515E-01 -.170E+06 89.7 .005 .150E-01 .510E-01 .014 -.018 .1510E-01 .520E-02 .170E-01 .747E+00 .990E-02 .346E-01 99.0 -.156 .118E-01 .452E-01 -.178E+06 92.7 -.047 .115E-01 .443E-01 .013 -.016 .1179E-01 .422E-02 .173E-01 .782E+00 .757E-02 .279E-01 102.0 -.208 .900E-02 .399E-01 -.186E+06 95.8 -.100 .871E-02 .386E-01 .011 -.014 .8999E-02 .322E-02 .175E-01 .809E+00 .578E-02 .224E-01 105.0 -.259 .672E-02 .353E-01 -.194E+06 98.8 -.153 .643E-02 .338E-01 .010 -.012 .6720E-02 .231E-02 .174E-01 .825E+00 .441E-02 .179E-01 108.0 -.309 .492E-02 .315E-01 -.202E+06 101.9 -.206 .465E-02 .297E-01 .008 -.010 .4919E-02 .154E-02 .172E-01 .823E+00 .338E-02 .142E-01 111.0 -.358 .355E-02 .282E-01 -.209E+06 105.0 -.258 .332E-02 .263E-01 .006 -.008 .3553E-02 .939E-03 .170E-01 .790E+00 .261E-02 .112E-01 114.0 -.407 .256E-02 .254E-01 -.217E+06 108.1 -.310 .237E-02 .235E-01 .004 -.006 .2565E-02 .520E-03 .166E-01 .706E+00 .204E-02 .880E-02 117.0 -.454 .189E-02 .231E-01 -.224E+06 111.2 -.362 .173E-02 .212E-01 .002 -.005 .1893E-02 .267E-03 .163E-01 .550E+00 .163E-02 .688E-02 120.0 -.500 .148E-02 .212E-01 -.231E+06 114.4 -.412 .134E-02 .192E-01 -.001 -.004 .1477E-02 .158E-03 .159E-01 .316E+00 .132E-02 .535E-02 123.0 -.545 .126E-02 .197E-01 -.238E+06 117.5 -.462 .113E-02 .176E-01 -.003 -.003 .1263E-02 .171E-03 .155E-01 .411E-01 .109E-02 .416E-02 126.0 -.588 .121E-02 .183E-01 -.245E+06 120.7 -.510 .107E-02 .162E-01 -.005 -.003 .1206E-02 .284E-03 .151E-01 -.200E+00 .922E-03 .322E-02 129.0 -.629 .127E-02 .171E-01 -.251E+06 123.9 -.558 .111E-02 .150E-01 -.007 -.002 .1269E-02 .478E-03 .146E-01 -.353E+00 .791E-03 .248E-02 132.0 -.669 .142E-02 .159E-01 -.257E+06 127.1 -.603 .124E-02 .138E-01 -.008 -.002 .1422E-02 .736E-03 .140E-01 -.419E+00 .687E-03 .191E-02 135.0 -.707 .164E-02 .147E-01 -.263E+06 130.3 -.647 .141E-02 .127E-01 -.010 -.001 .1642E-02 .104E-02 .133E-01 -.428E+00 .599E-03 .146E-02 138.0 -.743 .191E-02 .136E-01 -.269E+06 133.6 -.689 .163E-02 .116E-01 -.012 -.001 .1908E-02 .139E-02 .125E-01 -.410E+00 .521E-03 .111E-02 141.0 -.777 .221E-02 .124E-01 -.274E+06 136.8 -.729 .187E-02 .105E-01 -.013 -.001 .2205E-02 .176E-02 .116E-01 -.378E+00 .450E-03 .836E-03 144.0 -.809 .252E-02 .113E-01 -.279E+06 140.1 -.767 .212E-02 .950E-02 -.015 .000 .2520E-02 .214E-02 .107E-01 -.339E+00 .384E-03 .619E-03 147.0 -.839 .284E-02 .103E-01 -.283E+06 143.4 -.802 .237E-02 .858E-02 -.016 .000 .2839E-02 .252E-02 .985E-02 -.297E+00 .321E-03 .449E-03 150.0 -.866 .315E-02 .940E-02 -.288E+06 146.7 -.835 .260E-02 .778E-02 -.017 .001 .3147E-02 .289E-02 .909E-02 -.252E+00 .262E-03 .318E-03 153.0 -.891 .343E-02 .867E-02 -.291E+06 150.0 -.866 .282E-02 .713E-02 -.018 .001 .3433E-02 .322E-02 .845E-02 -.206E+00 .209E-03 .217E-03 156.0 -.914 .369E-02 .811E-02 -.295E+06 153.3 -.893 .301E-02 .663E-02 -.019 .001 .3686E-02 .352E-02 .796E-02 -.160E+00 .161E-03 .143E-03 159.0 -.934 .390E-02 .773E-02 -.298E+06 156.6 -.918 .317E-02 .629E-02 -.019 .001 .3900E-02 .378E-02 .764E-02 -.117E+00 .120E-03 .896E-04 162.0 -.951 .408E-02 .752E-02 -.301E+06 159.9 -.939 .330E-02 .609E-02 -.020 .000 .4076E-02 .399E-02 .746E-02 -.795E-01 .853E-04 .533E-04 165.0 -.966 .422E-02 .745E-02 -.303E+06 163.3 -.958 .340E-02 .601E-02 -.020 .000 .4218E-02 .416E-02 .742E-02 -.480E-01 .575E-04 .298E-04 168.0 -.978 .433E-02 .748E-02 -.305E+06 166.6 -.973 .349E-02 .602E-02 -.021 -.001 .4332E-02 .430E-02 .746E-02 -.244E-01 .358E-04 .154E-04 171.0 -.988 .442E-02 .758E-02 -.306E+06 169.9 -.985 .355E-02 .608E-02 -.021 -.001 .4423E-02 .440E-02 .757E-02 -.906E-02 .197E-04 .708E-05 174.0 -.995 .449E-02 .769E-02 -.307E+06 173.3 -.993 .360E-02 .616E-02 -.021 -.002 .4491E-02 .448E-02 .768E-02 -.124E-02 .861E-05 .267E-05 177.0 -.999 .453E-02 .777E-02 -.308E+06 176.6 -.998 .363E-02 .622E-02 -.021 -.002 .4534E-02 .453E-02 .777E-02 .898E-03 .213E-05 .600E-06 180.0 -1.000 .455E-02 .780E-02 -.308E+06 180.0 -1.000 .364E-02 .624E-02 -.021 -.002 .4549E-02 .455E-02 .780E-02 .264E-04 .823E-16 .224E-16 total cross-section = 51.425 elast , inel cross-section = 3.685 47.740 cross-sections in millibarns --------- energy(kinetic),gamcoul= 200.0 -.147E-01 born approx total = 78.069 elastic sigma= 8.748 SIG(TH) 200.0 2 3 0 101733001 0 0 0 0 0 3 0 0 1 0 .10E+03. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .428 .208 .674 .456 .134 .699 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .32E+02. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .10E+02. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . +++ . . . . . . .32E+01. +++ . . . . . . . 0+ . . . . . . . ++ . . . . . . . 0+. . . . . . . 0+ . . . . . . 0+ . . . . . .10E+01. . . . . . + . . . . . . . . . . . . . . . . . . . . . . . . . .0 . . . . . . . 0+ . . . . . . . + . . . . . . . 0 + . . . . . . . . . . . . .32E+00. . 0 + . . . . . . . + . . . . . . . 0 + . . . . . . . +. . . . . . . 0 + . . . . . . . . . . . .10E+00. . . . . . . . . . .+. . . . . . . . . . . . . . . . . . . . . . 0 . ++ . . . . . . . + . . . . . . . + . . . . . . 0 . + . . . . . . . + . . . . .32E-01. . . + . . . . . . . +. . . . . . 0. + . . . . . . .+ . . . . . . . + . . . . . . . . . . .10E-01. . . . . . . . . . 0 . . . . . .+. . . . . . . . . . . . . . . . . . + . . . . . . 0. . . . . . . 00 00 + . . . . . . 0 . 0 + . . . . . .0 . 0 . . ++++++++ .32E-02. . . 0 . 0 + . .++0 . . . . . . ++ . . . . . 0 + . ++0. . . . . 0 . +. + 0 . . . . . . 0 + + 0 . . . . . . .+ ++ 0 . . .10E-02. . . . . . . . . . . 00. . . . . . .00000+000. . . . . . . . SIG(TH) 200.0 2 3 0 101733001 0 0 0 0 0 3 0 0 1 0 .10E+02. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .428 .208 .674 .456 .134 .699 . . . . . . . . . . . . . . . . . . . . . . . . . . . . +++ . . . . . . .32E+01. +++ . . . . . . . + . . . . . . . ++ . . . . . . . +. . . . . . . + . . . . . . .+ . . . . . .10E+01. . . . . . + . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . + . . . . . . . + . . . . . . . + . . . . . . . . . . . . .32E+00. . + . . . . . . 0000 + . . . . . . 00. 000 + . . . . . . 0 . 00+. . . . . . 0 . 0+ . . . . . . 0 . . . . .10E+00. . .0. . . . . . . .+. . . . . . . . . . . . . . . . . . . . . . . ++ . . . . . 0 . . 0+ . . . . . . . 0+ . . . . . 0 . . 0+ . . . . . . . 0+ . . . . .32E-01. . . 0+ . . . . . . . 0+. . . . . 0 . . + . . . . . . 0.+ . . . . . . 0 + . . . . . . .0 . . . .10E-01. . . . . . . . . . . . . . . . .+. . . . . . . . . . . . . . . . . . 0 + . . . . . . . 0 . . . . . . . 0+ . . . .0 . . . + . . . . . . . 0 . . ++++++++ .32E-02. . . . 0+ . .++ . . . . . 0 . ++ . . . . . + . ++ . . . . . . 0+. + . . . . . . 0+ + . . . . . . 0+ ++ . . .10E-02. . . . . . . . . . . . . . . . . . . . .0+ . . . . . . . . . . . . . . 0 . . . . . . . 00 . . . . . . . 0 . . . . . . . 0 . . . . . . . 00 . . .32E-03. . . . . 0. . . . . . . 0 . . . . . . . . . . . . . .0 . . . . . . . 0 . . . . . . . . .10E-030 . . . . . . . . . . . . . . . . . . . . . . . . . .00000000 POLAR 200.0 2 3 0 101733001 0 0 0 0 0 3 0 0 1 0 .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .428 .208 .674 .456 .134 .699 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . +++ . . . .15E+01. . . . + + . . . . . . . + . . . . . . .+ + . . . . . . + . . . . . . +. . . . . . . . +. . . .15E+01. . . . . . . . . . . . . . + . . . . . . . . . . . . . . . . . . . . . . . . . . + . . . . . . . . . . . . . . + . . . . . . . . + . . .15E+01. . . . . . . . . . + . . . . . . . . . . . . . . . . . . . . . + . . . . . . . . . . . .15E+01. . . . .+ . ++ - . . . . . --- . .- . . - . . . -- . . - . . . . . - . . - . . . . . - . . - . . - . . - .- . .15E+01. - . . . . . . . - . . . . - . . . . . . -. . . - . .- . . - - . . . - . . . . -- . . . -. . . . -- . . .15E+01. . . . . - . . . . - . . . . . . . . . . . . . . . . . . . . . . . . . . . . .- -. . . . . . . - . . . . . . . - - . . . . . . . - - . . . . . .15E+01. . -- . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .15E+01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . eof in main