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| /*===================================================================*/
/* NRDF D1738 Data No.15 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,15;
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,15;
/* 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)208AC+154SM(60NI,X)209AC);
PHQ=EXC-FUNCT'94';
/* '94' for fusion-evapolation cross section */
ENR=98.6%;
CHM=X'95';
/* '95' Oxide */
THK-TGT=0.35MG/CM**2;
DET-PARTCL=(ALPHA'99',ALPHA'97',ALPHA'98',ALPHA'96');
/* '99' Alpha from 204Fr */
/* '98' Alpha from 205Fr */
/* '97' Alpha from 208Ac */
/* '96' Alpha from 209Ac */
ANL=STATIST-MODEL'100';
/* '100' HIVAP, See [W.Reisdorf and M.Schadel,
Z.Phys.A343(1992)47]. */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,15;
SYS-ERR=40%'101';
/* '101' 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)
1.753E+02 X 1.422E-06 +X-X
1.820E+02 X 2.254E-06 +X-X
1.842E+02 X 2.512E-06 +X-X
1.881E+02 X 4.090E-06 +X-X
1.940E+02 X 8.973E-06 +X-X
2.001E+02 9.733E-06 X +6.116E-06-6.256E-06
2.032E+02 1.145E-05 X +6.212E-06-5.940E-06
2.091E+02 3.771E-05 X +2.890E-05-2.595E-05
2.141E+02 2.078E-05 X +1.494E-05-1.430E-05
\END;
/*===================================================================*/
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