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| /*===================================================================*/
/* NRDF D1738 Data No.9 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,9;
D#=D1738;
TITLE=/ Sub-barrier fusion of deformed nuclei in 60Ni+154Sm and
32S+182W Reactions /;
ATH=(S.MITSUOKA'1', H.IKEZOE'1', K.NISHIO'1', J.LU'1');
INST-ATH=(2JPNJAE'1');
REF=PR/C;
VLP=62(2000)054603;
RCTS=(182W(32S,FISSN), 154SM(60NI,FISSN), 182W(32S,3*N)211TH,
182W(32S,2*N)212TH, 182W(32S,4*N)210TH, 182W(32S,X)210AC,
182W(32S,X)211AC, 182W(32S,X)208AC, 182W(32S,X)209AC,
182W(32S,X)209RA, 182W(32S,X)210RA, 182W(32S,X)207RA,
182W(32S,X)208RA, 182W(32S,X)208FR, 182W(32S,X)209FR,
182W(32S,X)206FR, 182W(32S,X)207FR, 154SM(60NI,3*N)211TH,
154SM(60NI,2*N)212TH, 154SM(60NI,4*N)210TH, 154SM(60NI,X)210AC,
154SM(60NI,X)211AC, 154SM(60NI,X)208AC, 154SM(60NI,X)209AC,
154SM(60NI,X)209RA, 154SM(60NI,X)210RA, 154SM(60NI,X)207RA,
154SM(60NI,X)208RA, 154SM(60NI,X)208FR, 154SM(60NI,X)209FR,
154SM(60NI,X)206FR, 154SM(60NI,X)207FR);
PHQS=(ANGL-DSTRN'2', FISSN-XSECTN, EXC-FUNCT'3');
/* '2' for fission fragments */
/* '3' for fusion-evapolation cross section */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,9;
/* 2002-02-08 : Converted, Mt + On. Data converted to EXFOR E1738
/* 2003-06-13 : Altered, On */
PHYS-FORM=SLD;
BAC=AL;
THK-BAC=XMG/CM**2'4';
/* '4' 0.7 micro-meter */
POL-TGT=0%;
ALGN-TGT=0%;
ACC=VDGT;
INST-ACC=2JPNJAE;
BEAM-INTNSTY=XMA'5';
/* '5' 30+-20 particle-nA */
POL-PRJ=0%;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG,IC'6',SSD'7',TOF'8');
/* '6' To detect fusion-fission products */
/* '7' To monitor Rutherford scattering */
/* '8' To obtain information on fusion-evaporation residue */
SOLID-ANGL=20MSR;
ERS-DET=80KEV'9';
/* '9' for position sensitive strip detector working on 5.486MeV
alpha particles from an 241Am source */
MONTR-RCT=/ , Rutherford scattering was monitored at forward angle of
theta(lab)=45deg by small-area solid-state detector for
the normalization of the cross section measurements. /;
EFCN-DET=/ Total efficiency is typically 25% for xn channel and 18%
for alpha+xn channel in 60Ni+154Sm system. /;
/* Experimental Method:
- Time-of-flight (To obtain information on fusion-evaporation
residue)
/* 2006-09-05 : Altered, At. Re-digitized */
RCT=(182W(32S,X)207RA+182W(32S,X)208RA);
PHQ=EXC-FUNCT'51';
/* '51' for fusion-evapolation cross section */
ENR=94.5%;
CHM=ELM;
THK-TGT=0.4MG/CM**2;
DET-PARTCL=(ALPHA'54',ALPHA'53',ALPHA'55',ALPHA'52');
/* '55' Alpha from 203Rn */
/* '54' Alpha from 204Rn */
/* '53' Alpha from 207Ra */
/* '52' Alpha from 208Ra */
ANL=STATIST-MODEL'56';
/* '56' HIVAP, See [W.Reisdorf and M.Schadel,
Z.Phys.A343(1992)47]. */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,9;
SYS-ERR=40%'57';
/* '57' Uncertainty in estimations of recoil mass separator
transmission and angular distribution of evaporation residue
CMPD=(214TH,214TH);
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-CM SIGMA DELTA-SIGMA
(MEV) (MB) (MB)
1.244E+02 1.799E-05 +1.297E-05-1.103E-05
1.271E+02 5.339E-05 +2.469E-05-2.556E-05
1.292E+02 6.485E-06 +6.674E-06-UNKNOWN
1.314E+02 4.426E-05 +2.597E-05-2.932E-05
1.335E+02 6.482E-05 +4.674E-05-3.976E-05
1.357E+02 1.280E-04 +5.918E-05-5.946E-05
1.379E+02 4.009E-04 +1.697E-04-1.680E-04
1.401E+02 2.209E-04 +1.021E-04-9.936E-05
1.421E+02 2.603E-04 +1.309E-04-1.131E-04
1.443E+02 3.068E-04 +1.299E-04-1.237E-04
1.486E+02 4.598E-05 +3.104E-05-2.868E-05
\END;
/*===================================================================*/
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