/*===================================================================*/ /* NRDF D1198 Data No.3 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,3; D#=D1198; TITLE=/ High energy component of giant octupole resonance in medium and heavy mass nuclei /; ATH=(T.YAMAGATA'1', S.KISHIMOTO'1', K.YUASA'1', K.IWAMOTO'1', B.SAEKI'1', M.TANAKA'2', T.FUKUDA'3', I.MIURA'4', M.INOUE'4', H.OGATA'4'); INST-ATH=(2JPNKON'1', 2JPNKTJ'2', 2JPNOSA'3', 2JPNRCN'4'); /* '1' Department of Physics */ /* '3' Department of Physics */ REF=PR/C; VLP=23(1981)937; RCTS=(90ZR(3HE,3HE)90ZR, 118SN(3HE,3HE)118SN, 120SN(3HE,3HE)120SN, 208PB(3HE,3HE)208PB); PHQS=ANGL-DSTRN; /*===================================================================*/ /* Experimental Conditions */ /*===================================================================*/ \\EXP,3; /* 2007-01-31 : Converted, N.Otuka. Converted to EXFOR E1198 */ /* 2007-02-08 : Altered, Mh. Re-digitized */ RTY=INEL-SCATT; PHQ=ANGL-DSTRN; ENR=X%'5'; /* '5' Enriched target */ CHM=ELM; PHYS-FORM=SLD; BAC=SELF; ACC=CYC'6'; /* '6' Isochronous cyclotron, AVF cyclotron */ INST-ACC=2JPNRCN; POL-PRJ=0%; DET-PARTCL=3HE; COINC=NO; ANT-COINC=NO; DET-SYS=(CNTR-TLSCP'7',SI'7'); /* '7' To detect scattered particles */ ERS-DET=150[300KEV; ANL=DWBA'8'; /* '8' Code DWUCK4 */ RCT=90ZR(3HE,3HE)90ZR; THK-TGT=4.0MG/CM**2; INC-ENGY-LAB-RANGE=140MEV; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,3; STATIST-ERR=X%'9'; /* '9' Statistical errors are considerably smaller than uncertainty due to the choice of the shape of continua */ INC-ENGY-LAB=140MEV; /*===================================================================*/ /* Data Table */ /*===================================================================*/ \DATA; THTC DSIGMA/DOMEGA/DE (DEG) (MB/SR/MEV) 9.572E+00 1.327E+01 1.042E+01 8.538E+00 1.193E+01 3.894E+00 1.363E+01 2.950E+00 1.513E+01 2.353E+00 1.646E+01 1.747E+00 1.872E+01 1.111E+00 2.001E+01 8.976E-01 2.144E+01 7.491E-01 2.262E+01 6.132E-01 2.415E+01 5.535E-01 2.558E+01 4.413E-01 2.742E+01 4.143E-01 \END; /*===================================================================*/ |