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| /*===================================================================*/
/* NRDF D0805 Data No.11 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,11;
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,11;
/* 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,11;
INC-ENGY-LAB=64.8MEV;
EXC-ENGY=2.906MEV;
J-PTY=4+;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTC DSIGMA/DOMEGA DELTA-DSIGMA/DOMEGA
(DEG) (UB/SR) (UB/SR)
1.2323E+01 7.427E+02 +-2.369E+02
1.6323E+01 1.051E+03 +-1.199E+02
2.0319E+01 1.351E+03 +-1.672E+02
2.4627E+01 1.521E+03 +-1.880E+02
2.8451E+01 1.502E+03 +-1.856E+02
3.2266E+01 1.223E+03 +-1.767E+02
3.6394E+01 8.731E+02 +-1.171E+02
4.0512E+01 5.021E+02 +-6.735E+01
4.4314E+01 3.104E+02 +-4.162E+01
4.8604E+01 2.352E+02 +-3.155E+01
5.2574E+01 1.720E+02 +-2.484E+01
5.6382E+01 1.199E+02 +-1.975E+01
\END;
/*===================================================================*/
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