DARPE: Search Results
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 /* NRDF D1738 Data No.16                                             */
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 /* Bibliography                                                      */
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 \\BIB,16;
 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 */
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 /* Experimental Conditions                                           */
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 \\EXP,16;
 /* 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)209RA+154SM(60NI,X)210RA);
 PHQ=EXC-FUNCT'102';
 /* '102' for fusion-evapolation cross section */
 ENR=98.6%;
 CHM=X'103';
 /* '103' Oxide */
 THK-TGT=0.35MG/CM**2;
 DET-PARTCL=(ALPHA'106',ALPHA'105',ALPHA'107',ALPHA'104');
 /* '107' Alpha from 205Rn */
 /* '106' Alpha from 206Rn */
 /* '105' Alpha from 209Ra */
 /* '104' Alpha from 210Ra */
 ANL=STATIST-MODEL'108';
 /* '108' HIVAP, See [W.Reisdorf and M.Schadel,
          Z.Phys.A343(1992)47]. */
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 /* Descriptive Parameters                                            */
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 \\DATA,16;
 SYS-ERR=40%'109';
 /* '109' Uncertainty in estimations of recoil mass separator
          transmission and angular distribution of evaporation residue
 CMPD=(214TH,214TH);
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-CM SIGMA XSECTN-MAX DELTA-SIGMA
 (MEV) (MB) (MB) (MB)
 1.753E+02 X 1.438E-06 +X-X
 1.821E+02 X 2.274E-06 +X-X
 1.839E+02 2.841E-06 X +3.172E-06-UNKNOWN
 1.880E+02 9.475E-06 X +7.661E-06-7.785E-06
 1.940E+02 2.116E-05 X +1.698E-05-1.714E-05
 2.000E+02 6.343E-05 X +3.657E-05-3.007E-05
 2.030E+02 7.449E-05 X +3.387E-05-3.316E-05
 2.091E+02 1.129E-04 X +6.080E-05-5.978E-05
 2.140E+02 4.600E-05 X +2.849E-05-2.594E-05
 \END;
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