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| /*===================================================================*/
/* NRDF D1738 Data No.14 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,14;
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,14;
/* 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=(154SM(60NI,X)210AC+154SM(60NI,X)211AC);
PHQ=EXC-FUNCT'86';
/* '86' for fusion-evapolation cross section */
ENR=98.6%;
CHM=X'87';
/* '87' Oxide */
THK-TGT=0.35MG/CM**2;
DET-PARTCL=(ALPHA'90',ALPHA'88',ALPHA'89',ALPHA'91');
/* '91' Alpha from 206Fr */
/* '90' Alpha from 207Fr */
/* '89' Alpha from 210Ac */
/* '88' Alpha from 211Ac */
ANL=STATIST-MODEL'92';
/* '92' HIVAP, See [W.Reisdorf and M.Schadel,
Z.Phys.A343(1992)47]. */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,14;
SYS-ERR=40%'93';
/* '93' Uncertainty in estimations of recoil mass separator
transmission and angular distribution of evaporation residue
CMPD=(214TH,214TH);
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
INC-ENGY-CM SIGMA XSECTN-MAX DELTA-SIGMA
(MEV) (MB) (MB) (MB)
1.754E+02 X 1.427E-06 +X-X
1.820E+02 X 2.314E-06 +X-X
1.841E+02 5.042E-06 X +4.061E-06-4.088E-06
1.880E+02 3.303E-05 X +1.911E-05-1.703E-05
1.941E+02 3.778E-05 X +2.348E-05-2.416E-05
2.001E+02 4.544E-05 X +2.276E-05-1.983E-05
2.031E+02 1.476E-05 X +7.922E-06-7.417E-06
2.091E+02 1.256E-05 X +1.338E-05-UNKNOWN
2.140E+02 1.399E-05 X +1.195E-05-1.134E-05
\END;
/*===================================================================*/
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