/*===================================================================*/ /* NRDF D1736 Data No.2 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,2; D#=D1736; TITLE=/ Inclusive reaction 40Ca(p,px) at an incident energy of 392 MeV /; ATH=(A.A.COWLEY'1', G.F.STEYN'2', Y.WATANABE'3', T.NORO'4', K.TAMURA'4', M.KAWABATA'4', K.HATANAKA'4', H.SAKAGUCHI'5', H.TAKEDA'5', M.ITOH'5'); INST-ATH=(3SAFSTL'1', 3SAFNAC'2', 2JPNKYU'3', 2JPNRCN'4', 2JPNKTO'5'); /* '1' Department of Physics */ /* '3' Department of Advanced Energy Engineering Science */ /* '5' Department of Physics */ REF=PR/C; VLP=62(2000)064604; RCTS=40CA(P,P)X; PHQS=ENGY-SPEC; /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,2; /* 2001-11-06 : Converted, Am + On. Data converted to EXFOR E1736. RTY=INCL; PHQ=ENGY-SPEC; ENR=NAT'6'; /* '6' 96.9% */ CHM=ELM; PHYS-FORM=SLD; THK-TGT=(12.8+-0.2MG/CM**2,16.0+-0.2MG/CM**2); BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=CYC; INST-ACC=2JPNRCN; INC-ENGY-LAB=392MEV; POL-PRJ=0%; DET-PARTCL=P; COINC=NO; ANT-COINC=NO; DET-SYS=MAG'7'; /* '7' Large acceptance spectormeter (LAS) */ SOLID-ANGL=XMSR'8'; /* '8' The horizontal acceptance angle is +-60mrad. */ ANL=DWBA'9'; /* '9' The semiclassical distorted wave model based on DWBA. */ /* 2006-09-05 : Altered, At. Re-digitized */ RCT=40CA(P,P)X; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,2; INC-ENGY-LAB=392MEV; THTL=40DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; ENGY-EMT-LAB DSIGMA/DOMEGA/DE DELTA-DSIGMA/DOMEGA/DE (MEV) (UB/SR/MEV) (UB/SR/MEV) 5.040E+01 5.595E+02 +-NEGLIGIBLE 5.609E+01 5.139E+02 +-NEGLIGIBLE 6.081E+01 5.139E+02 +-NEGLIGIBLE 6.553E+01 5.052E+02 +-NEGLIGIBLE 7.094E+01 5.269E+02 +-NEGLIGIBLE 7.549E+01 4.967E+02 +-NEGLIGIBLE 8.073E+01 5.139E+02 +-NEGLIGIBLE 8.598E+01 4.802E+02 +-NEGLIGIBLE 9.069E+01 4.721E+02 +-NEGLIGIBLE 9.594E+01 4.884E+02 +-NEGLIGIBLE 1.012E+02 5.052E+02 +-NEGLIGIBLE 1.054E+02 4.967E+02 +-NEGLIGIBLE 1.106E+02 4.743E+02 +-NEGLIGIBLE 1.153E+02 4.967E+02 +-NEGLIGIBLE 1.206E+02 4.802E+02 +-NEGLIGIBLE 1.258E+02 4.564E+02 +-NEGLIGIBLE 1.305E+02 4.884E+02 +-NEGLIGIBLE 1.353E+02 5.037E+02 +-NEGLIGIBLE 1.405E+02 5.139E+02 +-NEGLIGIBLE 1.457E+02 5.227E+02 +-NEGLIGIBLE 1.507E+02 5.269E+02 +-NEGLIGIBLE 1.554E+02 5.113E+02 +-NEGLIGIBLE 1.609E+02 5.052E+02 +-NEGLIGIBLE 1.657E+02 5.052E+02 +-NEGLIGIBLE 1.699E+02 5.052E+02 +-NEGLIGIBLE 1.756E+02 5.052E+02 +-NEGLIGIBLE 1.803E+02 4.967E+02 +-NEGLIGIBLE 1.856E+02 4.884E+02 +-NEGLIGIBLE 1.908E+02 4.887E+02 +-NEGLIGIBLE 1.950E+02 4.642E+02 +-NEGLIGIBLE 1.982E+02 4.487E+02 +-NEGLIGIBLE 2.013E+02 4.802E+02 +-NEGLIGIBLE 2.060E+02 4.802E+02 +-NEGLIGIBLE 2.113E+02 4.802E+02 +-NEGLIGIBLE 2.160E+02 4.802E+02 +-NEGLIGIBLE 2.207E+02 4.815E+02 +-NEGLIGIBLE 2.254E+02 4.815E+02 +-NEGLIGIBLE 2.307E+02 4.564E+02 +-NEGLIGIBLE 2.352E+02 4.400E+02 +-NEGLIGIBLE 2.406E+02 4.122E+02 +-NEGLIGIBLE 2.453E+02 3.984E+02 +-NEGLIGIBLE 2.506E+02 3.787E+02 +-NEGLIGIBLE 2.553E+02 3.479E+02 +-NEGLIGIBLE 2.606E+02 3.251E+02 +-NEGLIGIBLE 2.658E+02 2.986E+02 +-NEGLIGIBLE 2.705E+02 2.790E+02 +-NEGLIGIBLE 2.753E+02 2.562E+02 +-NEGLIGIBLE 2.805E+02 2.315E+02 +-NEGLIGIBLE 2.852E+02 2.056E+02 +-NEGLIGIBLE 2.903E+02 1.841E+02 +-NEGLIGIBLE 2.952E+02 1.515E+02 +-NEGLIGIBLE 3.009E+02 1.369E+02 +-NEGLIGIBLE 3.057E+02 1.246E+02 +-NEGLIGIBLE 3.109E+02 1.043E+02 +-NEGLIGIBLE 3.151E+02 9.585E+01 +-NEGLIGIBLE 3.203E+02 7.688E+01 +-NEGLIGIBLE 3.250E+02 7.063E+01 +-NEGLIGIBLE 3.303E+02 5.961E+01 +-NEGLIGIBLE 3.355E+02 4.781E+01 +-NEGLIGIBLE 3.402E+02 3.835E+01 +-NEGLIGIBLE 3.450E+02 2.875E+01 +-2.781E+00 3.507E+02 2.596E+01 +-2.512E+00 3.544E+02 1.535E+01 +-1.718E+00 3.602E+02 9.874E+00 +-1.245E+00 3.654E+02 1.004E+01 +-1.266E+00 3.701E+02 6.572E+00 +-1.025E+00 3.754E+02 3.951E+00 +-7.818E-01 3.801E+02 2.585E+00 +-6.145E-01 \END; /*===================================================================*/ |