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| /*===================================================================*/
/* 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;
/*===================================================================*/
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