/*===================================================================*/ /* NRDF D1664 Data No.11 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,11; D#=D1664; TITLE=/GAMOW-TELLER STRENGTH OF 90NB IN THE CONTINUUM STUDIED VIA MULTIPOLE DECOMPOSITION ANALYSIS OF THE 90ZR(P,N) REACTION AT 295 MEV/; ATH=(T.WAKASA'1,4',H.SAKAI'1',H.OKAMURA'1',S.FUJITA'1,5',S.ISHIDA'1,6', N.SAKAMOTO'1,6',T.UESAKA'1',Y.SATOU'1',M.B.GREENFIELD'2', K.HATANAKA'3'); INST-ATH=(2JPNTOK'1',2JPNICU'2',2JPNRCN'3'); /*@34@*/ /*@35@*/ /*@36@*/ REF=PR/C; VLP=55(1997)2909; RCTS=(90ZR(P,N)90NB); PHQS=(POL-TRNSF,DSIGMA/DOMEGA/DE,ANGL-DSTRN,EXC-ENGY); /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,11; /* 2006-02-27 N.OTUKA 2JPNJPN -> 2JPNICU in BIB,1[11 */ RCT=90ZR(P,N)90NB; RTY=(POL-RCT); ENR=X; CHM=ELM; PHYS-FORM=SLD; THK-TGT=112MG/CM**2; BAC=SELF; POL-TGT=0%; ALGN-TGT=0%; ACC=(CYC); INST-ACC=2JPNRCN; INC-ENGY-LAB=(295MEV); DELTA-INC-ENGY-LAB=1000KEV; POL-PRJ=73%; DET-PARTCL=(N); COINC=NO; ANT-COINC=NO; DET-SYS=(NPOL2'21');/*@31@*/ SOLID-ANGL=XMSR; ERS-DET=1900KEV; MONTR-RCT=/1H(P(POL),P)1H/; ANL=(DWIA,X'22');/*@32@*/ PHQ=(ANGL-DSTRN,DSIGMA/DOMEGA/DE); PHQ=(EXC-ENGY,DSIGMA/DOMEGA/DE); /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,11; INC-ENGY-LAB=295MEV; EMT-1=N; RSD=90NB; THTL-1=12.3DEG; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; EXC-ENGY DSIGMA/DOMEGA/DE (MEV) (MB/SR/MEV) -5.496E+00 2.251E-01 -3.038E+00 1.931E-01 -2.081E+00 1.361E-01 -9.954E-01 2.334E-01 3.870E-01 2.740E-01 1.304E+00 5.722E-01 2.211E+00 6.799E-01 3.523E+00 5.455E-01 5.318E+00 4.624E-01 5.743E+00 5.549E-01 7.012E+00 6.985E-01 8.455E+00 7.545E-01 8.699E+00 8.316E-01 1.081E+01 9.594E-01 1.182E+01 8.354E-01 1.380E+01 8.603E-01 1.243E+01 1.072E+00 1.442E+01 1.220E+00 1.520E+01 1.199E+00 1.605E+01 1.312E+00 1.696E+01 1.554E+00 1.780E+01 1.461E+00 1.966E+01 1.584E+00 2.026E+01 1.589E+00 2.128E+01 1.470E+00 2.279E+01 1.773E+00 2.261E+01 1.644E+00 2.435E+01 1.695E+00 2.605E+01 1.972E+00 2.676E+01 1.848E+00 2.826E+01 1.843E+00 2.934E+01 1.919E+00 3.090E+01 1.944E+00 3.259E+01 2.021E+00 3.469E+01 2.030E+00 3.530E+01 2.184E+00 3.710E+01 2.230E+00 3.825E+01 2.353E+00 3.974E+01 2.208E+00 4.070E+01 2.254E+00 4.149E+01 2.331E+00 4.256E+01 2.238E+00 4.394E+01 2.181E+00 4.610E+01 2.159E+00 4.723E+01 2.102E+00 4.849E+01 2.107E+00 4.963E+01 2.101E+00 5.052E+01 1.905E+00 5.203E+01 2.049E+00 5.347E+01 1.986E+00 5.448E+01 1.919E+00 5.586E+01 1.877E+00 5.652E+01 1.805E+00 5.922E+01 1.840E+00 5.975E+01 1.731E+00 6.071E+01 1.659E+00 6.161E+01 1.725E+00 6.215E+01 1.782E+00 6.275E+01 1.725E+00 6.347E+01 1.699E+00 6.425E+01 1.642E+00 6.466E+01 1.606E+00 6.550E+01 1.543E+00 6.670E+01 1.569E+00 6.736E+01 1.486E+00 6.855E+01 1.434E+00 \END; /*===================================================================*/ |