program= LPOTT input= in/in.sample Mon Feb 24 17:18:55 PST 1992 cat in/tfoldc>tape3 cat in/gth>tape2 cat in/denomt>tape4 for it do run LPOTT $it & wait done Run Time STOP Real 8.6 User 2.6 System 0.1 pion scattering via lpott(vaxversion) on 32,1/86 ok tape6 1 10 50.0000 16 22 .20E+05 3-2.00-3.00 no of grid points= 16 1.5500 1.5500 .0000 1.5500 1.5500 .0000 3.0000 7.0000 6 12 0 101705003 0 0 0 0 0 0 0 0 0 0 nifty( 1)= 0 pi+ 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)= 0 no spin ms nifty( 7)= 5 abs-old,sp nifty( 8)= 0 no del/fld nifty( 9)= 0 no pauli nifty(10)= 3 exact coul 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)= 0 rhog,rho2g nifty(17)= 0 kmt nifty(18)= 0 full amps nifty(19)= 0 use nif-16 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 ********** amass= 12.0000********** tpi epilab ecm(sqrts) kcm plab 50.0000 189.5780 11447.9310 126.1716 128.2880 relativistic calculation energy momentum 50.0000 126.1716 ----- angular momentum = 0----- OPT POTEN VALUES FOR KP=K0= 126.172AND L=1 K REV VC RABS(N0 FLIP) RABS(FLIP)IMV IMVABS(NOFLIP),IMABS(FLIP) .6722E+00 .3648E-07 .3016E-07 -.380E-08 .000E+00 .2362E-08 -.166E-06 .000E+00 .3596E+01 .1331E-06 .1612E-06 .142E-08 .000E+00 .1854E-07 -.176E-06 .000E+00 .9087E+01 -.4757E-06 .4058E-06 .112E-07 .000E+00 .1239E-06 -.233E-06 .000E+00 .1758E+02 -.9389E-06 .7749E-06 .262E-07 .000E+00 .2398E-06 -.403E-06 .000E+00 .2980E+02 -.1548E-05 .1271E-05 .476E-07 .000E+00 .3958E-06 -.662E-06 .000E+00 .4690E+02 -.2335E-05 .1854E-05 .764E-07 .000E+00 .5902E-06 -.999E-06 .000E+00 .7072E+02 -.3211E-05 .2374E-05 .113E-06 .000E+00 .7934E-06 -.139E-05 .000E+00 .1043E+03 -.3981E-05 .2455E-05 .157E-06 .000E+00 .9271E-06 -.172E-05 .000E+00 .1527E+03 -.4131E-05 .1599E-05 .196E-06 .000E+00 .8488E-06 -.180E-05 .000E+00 .2251E+03 -.2793E-05 .2622E-06 .202E-06 .000E+00 .4893E-06 -.137E-05 .000E+00 .3394E+03 -.3556E-06 .4633E-07 .126E-06 .000E+00 .3824E-07 -.521E-06 .000E+00 .5342E+03 .6527E-07 .4541E-08 .899E-08 .000E+00 -.1508E-09 -.657E-08 .000E+00 .9055E+03 .7703E-09 .6988E-09 -.526E-09 .000E+00 .0000E+00 .870E-09 .000E+00 .1752E+04 .1648E-09 .1648E-09 .144E-14 .000E+00 .0000E+00 -.191E-14 .000E+00 .4427E+04 .1367E-10 .1367E-10 .750E-67 .000E+00 .0000E+00 -.913E-67 .000E+00 .2368E+05 .2390E-12 .2390E-12 .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 126.172 .73876E-10 -.73876E-10 .18842E-13 .00000E+00 .11807E-05 -.19043E-05 .00000E+00 .00000E+00 .17822E-06 -.18137E-05 .00000E+00 .00000E+00 .13846E-07 -.30500E-06 .00000E+00 .00000E+00 .70217E-09 -.24856E-07 .00000E+00 .00000E+00 .26092E-10 -.12949E-08 .00000E+00 .00000E+00 .76016E-12 -.48953E-10 .00000E+00 .00000E+00 .18148E-13 -.14434E-11 .00000E+00 .00000E+00 .36621E-15 -.34766E-13 .00000E+00 .00000E+00 .63907E-17 -.70631E-15 .00000E+00 .00000E+00 .98218E-19 -.12392E-16 .00000E+00 .00000E+00 OPT POTEN VALUES FOR KP=K0= 126.172AND L=1 K REV VC RABS(N0 FLIP) RABS(FLIP)IMV IMVABS(NOFLIP),IMABS(FLIP) .1262E+03 -.4173E-05 .2161E-05 .178E-06 .000E+00 .9211E-06 -.181E-05 .000E+00 determinant from matrix inversion= .5038391E+00 unnormalized r matrix(re,im,re,-im) .4467984E-05 -.1712296E-05 .4467984E-05 .1712296E-05 normalized r(k,k..k)= -.2086486E+00 .7996182E-01 t(k,k,k)= -.1881360E+00 .1171202E+00 eta= .8532 delta= -13.0841 now with exact coulomb after matching t(k,k,k)= -.6078032E-01 .7819965E-01 eta= .8523 delta= -4.0999 coulomb phase modified nuclear amplitude t(k,k.k) = -.5534315E-01 .8213750E-01 born approximation normalized r(k,k..k)= -.1896564E+00 .7239389E-01 t(k,k,k)= -.2068978E+00 .7897515E-01 eta= .9382 delta= -13.0851 now with exact coulomb after matching t(k,k,k)= -.6683928E-01 .3587068E-01 eta= .9378 delta= -4.0974 ----- angular momentum = 1----- determinant from matrix inversion= .5702570E+00 unnormalized r matrix(re,im,re,-im) -.4986588E-05 -.1249645E-05 -.4986588E-05 .1249645E-05 normalized r(k,k..k)= .2328666E+00 .5835665E-01 t(k,k,k)= .2163216E+00 .1077481E+00 eta= .8959 delta= 14.4381 now with exact coulomb after matching t(k,k,k)= .2902845E+00 .1579686E+00 eta= .8972 delta= 20.1607 coulomb phase modified nuclear amplitude t(k,k.k) = .2820602E+00 .1722241E+00 born approximation normalized r(k,k..k)= .1948961E+00 .4301320E-01 t(k,k,k)= .2126140E+00 .4692349E-01 eta= 1.0010 delta= 12.5696 now with exact coulomb after matching t(k,k,k)= .2986540E+00 .9840049E-01 eta= 1.0010 delta= 18.3184 ----- angular momentum = 2----- determinant from matrix inversion= .6402674E+00 unnormalized r matrix(re,im,re,-im) -.7301225E-06 -.2374145E-06 -.7301225E-06 .2374145E-06 normalized r(k,k..k)= .3409570E-01 .1108692E-01 t(k,k,k)= .3634273E-01 .1318774E-01 eta= .9763 delta= 2.1347 now with exact coulomb after matching t(k,k,k)= .1090716E+00 .2432659E-01 eta= .9760 delta= 6.4573 coulomb phase modified nuclear amplitude t(k,k.k) = .1057904E+00 .3601103E-01 born approximation normalized r(k,k..k)= .2407947E-01 .8729616E-02 t(k,k,k)= .2626851E-01 .9523218E-02 eta= .9824 delta= 1.5328 now with exact coulomb after matching t(k,k,k)= .9954237E-01 .1912843E-01 eta= .9821 delta= 5.8476 ----- angular momentum = 3----- determinant from matrix inversion= .8309314E+00 unnormalized r matrix(re,im,re,-im) .3785412E-06 -.1541076E-07 .3785412E-06 .1541076E-07 normalized r(k,k..k)= -.1767734E-01 .7196608E-03 t(k,k,k)= -.1925064E-01 .1124575E-02 eta= .9985 delta= -1.1049 now with exact coulomb after matching t(k,k,k)= .1307836E-01 .9303211E-03 eta= .9985 delta= .7506 coulomb phase modified nuclear amplitude t(k,k.k) = .1279850E-01 .2847353E-02 born approximation normalized r(k,k..k)= -.1821172E-01 .7477144E-03 t(k,k,k)= -.1986733E-01 .8156885E-03 eta= .9992 delta= -1.1396 now with exact coulomb after matching t(k,k,k)= .1247847E-01 .5795272E-03 eta= .9992 delta= .7156 ----- angular momentum = 4----- born approximation normalized r(k,k..k)= -.7622181E-02 -.5938993E-04 t(k,k,k)= -.8315107E-02 -.6478902E-04 eta= 1.0003 delta= -.4763 now with exact coulomb after matching t(k,k,k)= .2500015E-03 -.1291479E-03 eta= 1.0003 delta= .0143 t(k,k,k)= -.8315611E-02 -.1406005E-05 eta= 1.0001 delta= -.4764 now with exact coulomb after matching t(k,k,k)= .2484677E-03 -.6800965E-04 eta= 1.0001 delta= .0142 coulomb phase modified nuclear amplitude t(k,k.k) = .2565682E-03 -.2311358E-04 ----- angular momentum = 5----- born approximation normalized r(k,k..k)= -.1507966E-02 -.2905409E-04 t(k,k,k)= -.1645054E-02 -.3169537E-04 eta= 1.0001 delta= -.0942 now with exact coulomb after matching t(k,k,k)= -.1538401E-03 -.3197077E-04 eta= 1.0001 delta= -.0088 t(k,k,k)= -.1645146E-02 -.2921540E-04 eta= 1.0001 delta= -.0943 now with exact coulomb after matching t(k,k,k)= -.1539324E-03 -.2966458E-04 eta= 1.0001 delta= -.0088 coulomb phase modified nuclear amplitude t(k,k.k) = -.1449184E-03 -.5978153E-04 ----- angular momentum = 6----- born approximation normalized r(k,k..k)= -.1912151E-03 -.4396017E-05 t(k,k,k)= -.2085983E-03 -.4795655E-05 eta= 1.0000 delta= -.0120 now with exact coulomb after matching t(k,k,k)= -.2772747E-04 -.4397744E-05 eta= 1.0000 delta= -.0016 t(k,k,k)= -.2086001E-03 -.4755789E-05 eta= 1.0000 delta= -.0120 now with exact coulomb after matching t(k,k,k)= -.2772914E-04 -.4361509E-05 eta= 1.0000 delta= -.0016 coulomb phase modified nuclear amplitude t(k,k.k) = -.2610388E-04 -.1032064E-04 ----- angular momentum = 7----- born approximation normalized r(k,k..k)= -.1734574E-04 -.4137386E-06 t(k,k,k)= -.1892263E-04 -.4513512E-06 eta= 1.0000 delta= -.0011 now with exact coulomb after matching t(k,k,k)= -.2770784E-05 -.4046630E-06 eta= 1.0000 delta= -.0002 t(k,k,k)= -.1892265E-04 -.4510231E-06 eta= 1.0000 delta= -.0011 now with exact coulomb after matching t(k,k,k)= -.2770798E-05 -.4043691E-06 eta= 1.0000 delta= -.0002 coulomb phase modified nuclear amplitude t(k,k.k) = -.2598076E-05 -.1044432E-05 ----- angular momentum = 8----- born approximation normalized r(k,k..k)= -.1196749E-05 -.2835023E-07 t(k,k,k)= -.1305545E-05 -.3092752E-07 eta= 1.0000 delta= -.0001 now with exact coulomb after matching t(k,k,k)= -.1964694E-06 -.2743099E-07 eta= 1.0000 delta= .0000 t(k,k,k)= -.1305545E-05 -.3092596E-07 eta= 1.0000 delta= -.0001 now with exact coulomb after matching t(k,k,k)= -.1964695E-06 -.2742960E-07 eta= 1.0000 delta= .0000 coulomb phase modified nuclear amplitude t(k,k.k) = -.1834224E-06 -.7555695E-07 ----- angular momentum = 9----- born approximation normalized r(k,k..k)= -.6536049E-07 -.1525927E-08 t(k,k,k)= -.7130235E-07 -.1664648E-08 eta= 1.0000 delta= .0000 now with exact coulomb after matching t(k,k,k)= -.1079664E-07 -.1465314E-08 eta= 1.0000 delta= .0000 t(k,k,k)= -.7130235E-07 -.1664643E-08 eta= 1.0000 delta= .0000 now with exact coulomb after matching t(k,k,k)= -.1079664E-07 -.1465310E-08 eta= 1.0000 delta= .0000 coulomb phase modified nuclear amplitude t(k,k.k) = -.1003550E-07 -.4243032E-08 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 .0 1.000 .435E+15 .435E+15 .000E+00 .0 1.000 .450E+15 .450E+15 2.205 1.248 .6418E+02 3.0 .999 .501E+05 .504E+05 -.436E+02 3.0 .999 .518E+05 .521E+05 2.198 1.245 .6384E+02 6.0 .995 .253E+04 .257E+04 -.174E+03 5.9 .995 .261E+04 .266E+04 2.179 1.238 .6282E+02 9.0 .988 .337E+03 .349E+03 -.392E+03 8.9 .988 .349E+03 .361E+03 2.148 1.225 .6116E+02 12.0 .978 .574E+02 .587E+02 -.696E+03 11.8 .979 .593E+02 .606E+02 2.105 1.208 .5889E+02 15.0 .966 .112E+02 .833E+01 -.108E+04 14.8 .967 .116E+02 .861E+01 2.049 1.186 .5608E+02 18.0 .951 .681E+01 .207E+01 -.156E+04 17.7 .953 .703E+01 .214E+01 1.983 1.160 .5279E+02 21.0 .934 .999E+01 .446E+01 -.211E+04 20.7 .936 .103E+02 .460E+01 1.907 1.130 .4911E+02 24.0 .914 .134E+02 .766E+01 -.275E+04 23.6 .916 .138E+02 .790E+01 1.821 1.095 .4513E+02 27.0 .891 .156E+02 .994E+01 -.347E+04 26.6 .894 .161E+02 .102E+02 1.726 1.057 .4094E+02 30.0 .866 .165E+02 .111E+02 -.427E+04 29.5 .870 .170E+02 .114E+02 1.623 1.015 .3664E+02 33.0 .839 .164E+02 .113E+02 -.514E+04 32.5 .844 .168E+02 .116E+02 1.514 .970 .3231E+02 36.0 .809 .154E+02 .108E+02 -.608E+04 35.4 .815 .158E+02 .111E+02 1.399 .922 .2806E+02 39.0 .777 .140E+02 .979E+01 -.710E+04 38.4 .784 .143E+02 .100E+02 1.279 .872 .2395E+02 42.0 .743 .122E+02 .851E+01 -.818E+04 41.4 .751 .125E+02 .873E+01 1.156 .819 .2008E+02 45.0 .707 .103E+02 .710E+01 -.933E+04 44.3 .715 .106E+02 .727E+01 1.031 .765 .1648E+02 48.0 .669 .848E+01 .568E+01 -.105E+05 47.3 .678 .867E+01 .581E+01 .904 .710 .1322E+02 51.0 .629 .673E+01 .434E+01 -.118E+05 50.3 .639 .687E+01 .443E+01 .778 .654 .1033E+02 54.0 .588 .516E+01 .315E+01 -.131E+05 53.2 .599 .526E+01 .321E+01 .653 .597 .7826E+01 57.0 .545 .382E+01 .214E+01 -.145E+05 56.2 .556 .389E+01 .218E+01 .529 .540 .5721E+01 60.0 .500 .274E+01 .135E+01 -.159E+05 59.2 .512 .279E+01 .137E+01 .409 .484 .4011E+01 63.0 .454 .193E+01 .786E+00 -.174E+05 62.2 .467 .196E+01 .798E+00 .292 .427 .2682E+01 66.0 .407 .138E+01 .446E+00 -.189E+05 65.1 .421 .140E+01 .453E+00 .180 .372 .1710E+01 69.0 .358 .108E+01 .319E+00 -.204E+05 68.1 .373 .109E+01 .323E+00 .073 .318 .1065E+01 72.0 .309 .101E+01 .386E+00 -.220E+05 71.1 .324 .102E+01 .390E+00 -.028 .265 .7109E+00 75.0 .259 .113E+01 .622E+00 -.236E+05 74.1 .274 .114E+01 .628E+00 -.123 .214 .6095E+00 78.0 .208 .142E+01 .100E+01 -.252E+05 77.1 .224 .143E+01 .101E+01 -.212 .165 .7196E+00 81.0 .156 .185E+01 .149E+01 -.269E+05 80.1 .173 .186E+01 .150E+01 -.294 .117 .1001E+01 84.0 .105 .237E+01 .207E+01 -.285E+05 83.0 .121 .238E+01 .208E+01 -.369 .072 .1413E+01 87.0 .052 .296E+01 .270E+01 -.302E+05 86.0 .069 .297E+01 .271E+01 -.437 .029 .1920E+01 90.0 .000 .359E+01 .337E+01 -.318E+05 89.0 .017 .359E+01 .337E+01 -.499 -.012 .2488E+01 93.0 -.052 .423E+01 .404E+01 -.335E+05 92.0 -.036 .423E+01 .404E+01 -.553 -.051 .3088E+01 96.0 -.105 .487E+01 .471E+01 -.352E+05 95.0 -.088 .485E+01 .469E+01 -.602 -.087 .3695E+01 99.0 -.156 .547E+01 .535E+01 -.368E+05 98.1 -.140 .545E+01 .532E+01 -.644 -.121 .4289E+01 102.0 -.208 .604E+01 .595E+01 -.385E+05 101.1 -.192 .600E+01 .591E+01 -.680 -.153 .4851E+01 105.0 -.259 .655E+01 .650E+01 -.401E+05 104.1 -.243 .650E+01 .645E+01 -.710 -.182 .5372E+01 108.0 -.309 .701E+01 .701E+01 -.417E+05 107.1 -.294 .694E+01 .694E+01 -.735 -.209 .5841E+01 111.0 -.358 .741E+01 .745E+01 -.432E+05 110.1 -.344 .732E+01 .736E+01 -.755 -.234 .6254E+01 114.0 -.407 .774E+01 .783E+01 -.448E+05 113.1 -.393 .764E+01 .773E+01 -.771 -.257 .6609E+01 117.0 -.454 .801E+01 .816E+01 -.463E+05 116.1 -.441 .789E+01 .804E+01 -.783 -.278 .6905E+01 120.0 -.500 .823E+01 .843E+01 -.478E+05 119.2 -.487 .809E+01 .830E+01 -.791 -.297 .7144E+01 123.0 -.545 .838E+01 .865E+01 -.492E+05 122.2 -.533 .823E+01 .850E+01 -.796 -.314 .7330E+01 126.0 -.588 .849E+01 .883E+01 -.506E+05 125.2 -.577 .833E+01 .866E+01 -.799 -.330 .7468E+01 129.0 -.629 .856E+01 .895E+01 -.519E+05 128.2 -.619 .838E+01 .877E+01 -.799 -.344 .7561E+01 132.0 -.669 .858E+01 .904E+01 -.531E+05 131.3 -.660 .839E+01 .884E+01 -.797 -.356 .7616E+01 135.0 -.707 .858E+01 .910E+01 -.544E+05 134.3 -.699 .838E+01 .889E+01 -.793 -.367 .7638E+01 138.0 -.743 .854E+01 .913E+01 -.555E+05 137.4 -.736 .834E+01 .891E+01 -.788 -.377 .7633E+01 141.0 -.777 .849E+01 .914E+01 -.566E+05 140.4 -.770 .827E+01 .890E+01 -.782 -.386 .7606E+01 144.0 -.809 .842E+01 .912E+01 -.576E+05 143.4 -.803 .820E+01 .888E+01 -.776 -.393 .7563E+01 147.0 -.839 .834E+01 .910E+01 -.585E+05 146.5 -.834 .811E+01 .884E+01 -.769 -.400 .7507E+01 150.0 -.866 .826E+01 .906E+01 -.594E+05 149.5 -.862 .802E+01 .880E+01 -.761 -.406 .7443E+01 153.0 -.891 .817E+01 .901E+01 -.602E+05 152.6 -.887 .793E+01 .875E+01 -.754 -.411 .7375E+01 156.0 -.914 .808E+01 .897E+01 -.609E+05 155.6 -.911 .784E+01 .870E+01 -.747 -.415 .7306E+01 159.0 -.934 .800E+01 .892E+01 -.616E+05 158.7 -.931 .776E+01 .865E+01 -.741 -.418 .7239E+01 162.0 -.951 .793E+01 .887E+01 -.621E+05 161.7 -.949 .768E+01 .860E+01 -.735 -.421 .7176E+01 165.0 -.966 .786E+01 .883E+01 -.626E+05 164.7 -.965 .761E+01 .855E+01 -.730 -.424 .7120E+01 168.0 -.978 .780E+01 .880E+01 -.630E+05 167.8 -.977 .755E+01 .851E+01 -.725 -.425 .7071E+01 171.0 -.988 .775E+01 .877E+01 -.633E+05 170.8 -.987 .750E+01 .848E+01 -.722 -.427 .7032E+01 174.0 -.995 .772E+01 .874E+01 -.635E+05 173.9 -.994 .747E+01 .846E+01 -.719 -.428 .7004E+01 177.0 -.999 .770E+01 .873E+01 -.636E+05 176.9 -.999 .745E+01 .844E+01 -.718 -.428 .6987E+01 180.0 -1.000 .769E+01 .873E+01 -.637E+05 180.0 -1.000 .744E+01 .844E+01 -.717 -.429 .6981E+01 total cross-section = 208.784 elast , inel cross-section = 123.292 85.492 cross-sections in millibarns --------- energy(kinetic),gamcoul= 50.0 .642E-01 born approx total = 167.246 elastic sigma= 109.072 SIG(TH) 50.0 6 12 0 101705003 0 0 0 0 0 0 0 0 0 0 .10E+04+++ . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1.550 1.550 .000 1.550 1.550 .000 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .32E+03. + . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .10E+03. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . + . . . . . . . . . . . . . . . . . . . . .32E+02. . . . . . . . . . . . . . . . . . . . . . . . . . . . . ++++ . . . . . . + . ++ . . . . . .10E+02. . .+. . . . .+. . . . . . . . . . . . . . . . . . . . . . . . + . + . . .++++++++++ . . + . . . +++++ .++++++++++ . . + . . ++ . . . . . + . . ++ . . . . . . .+ . . . .32E+01. . +. + . . . . . + +. . . . . . . + . . . . . . .+ + . . . . . . . . . . . . . . + + . . . . .10E+01. . . . . . . . . . . .+++. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .32E+00. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .10E+00. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .32E-01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .10E-01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . SIG(TH) 50.0 6 12 0 101705003 0 0 0 0 0 0 0 0 0 0 .10E+03++++. . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1.550 1.550 .000 1.550 1.550 .000 . . . . . . . . . . . . . . . + . . . . . . . . . . . . . . . . . . . . .32E+02. . . . . . . . . . . . . . . . . . . . . . . . . . . . . ++++ . . . . . . + . ++ . . . . . .10E+02. . .+. . 000 .+. . . . . . . . . . . . . . . . . . . . . . . . 0 + 0. 00 + . . 0++++++++++0000000000 . + 0 . 0 . . +++++ .++++++++++ . . 0+ . . ++ . . . . . + . . ++ . . . . 0 . 0 . .+ . . . .32E+01. . +. + . . . . . 0 + +. . . . . . . + . . . . . 0 . 0.+ +0 . . . . . . . 0 . . . . . . 0 + + . . . . .10E+01. . . . . . . . . . . .+++0 . . . . . . . . . . . . . . . . . . . . . . . . . . .0 . . . . . . . 0 . . . . . . . . . . . . . . 0 0 . . . . .32E+00. . . 0 . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .10E+00. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .32E-01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .10E-01. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .32E-02. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . .10E-02. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . eof in main