/*===================================================================*/ /* NRDF D0805 Data No.10 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,10; D#=D805; TITLE=/ Fragmentation of low-lying hexadecapole states in even 74-82Se and a RPA calculation /; ATH=(K.OGINO'1', Y.KADOTA'1', H.HAGA'1', S.MATSUKI'2', T.HIGO'2', T.SHIBA'2', N.SAKAMOTO'3', Y.OKUMA'4', T.YANABU'5'); INST-ATH=(2JPNKTO'1', 2JPNKTO'2', 2JPNJPN'3', 2JPNRCN'4', 2JPNKNZ'5'); /* '1' Department of Nuclear Engineering */ /* '2' Institute for Chemical Research */ /* '3' Department of Physics, Nara Women's University */ /* '5' Department of Education */ REF=PL/B; VLP=130(1983)147; RCTS=78SE(P,P)78SE; PHQS=ANGL-DSTRN; /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,10; /* 2007-08-25 : Converted, N.Otuka. Converted to EXFOR E0805 */ RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=98.58%; CHM=ELM; PHYS-FORM=SLD; THK-TGT=0.5MG/CM**2; BAC=AU; POL-TGT=0%; ALGN-TGT=0%; ACC=CYC'6'; /* '6' Isochronous cyclotron, AVF cyclotron */ INST-ACC=2JPNRCN; INC-ENGY-LAB-RANGE=64.8MEV; POL-PRJ=0%; DET-PARTCL=P; COINC=NO; ANT-COINC=NO; DET-SYS=MAG'7'; /* '7' To analyze momenta of scattered protons (RAIDEN) */ ERS-DET=[20KEV; ANL=(DWBA'8',CC'9'); /* '8' DWUCK-4 */ /* '9' ECIS */ /* 2007-11-20 : Altered, T.Ashizawa. Re-digitized */ RCT=78SE(P,P)78SE; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,10; INC-ENGY-LAB=64.8MEV; EXC-ENGY=2.678MEV; J-PTY=4+; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA (DEG) (UB/SR) (UB/SR) 1.2205E+01 3.417E+02 +-1.369E+02 1.6018E+01 3.804E+02 +-9.201E+01 2.0150E+01 4.498E+02 +-8.759E+01 2.4276E+01 4.602E+02 +-1.028E+02 2.8399E+01 4.488E+02 +-5.743E+01 3.2352E+01 3.359E+02 +-4.293E+01 3.6135E+01 1.929E+02 +-2.187E+01 4.0392E+01 1.081E+02 +-1.983E+01 4.4330E+01 5.848E+01 +-1.917E+01 4.8454E+01 5.703E+01 +-1.582E+01 5.2412E+01 4.813E+01 +-9.373E+00 5.6357E+01 3.044E+01 +-7.907E+00 \END; /*===================================================================*/ |