/*===================================================================*/
 /* NRDF D1738 Data No.6                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,6;
 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,6;
 /* 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)210AC+182W(32S,X)211AC);
 PHQ=EXC-FUNCT'30';
 /* '30' for fusion-evapolation cross section */
 ENR=94.5%;
 CHM=ELM;
 THK-TGT=0.4MG/CM**2;
 DET-PARTCL=(ALPHA'34',ALPHA'31',ALPHA'32',ALPHA'33');
 /* '34' Alpha from 206Fr */
 /* '33' Alpha from 207Fr */
 /* '32' Alpha from 210Ac */
 /* '31' Alpha from 211Ac */
 ANL=STATIST-MODEL'35';
 /* '35' HIVAP, See [W.Reisdorf and M.Schadel,
         Z.Phys.A343(1992)47]. */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,6;
 SYS-ERR=40%'36';
 /* '36' 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 5.204E-05 +NEGLIGIBLE-NEGLIGIBLE
 1.270E+02 7.029E-05 +NEGLIGIBLE-NEGLIGIBLE
 1.292E+02 1.002E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.315E+02 1.724E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.334E+02 2.088E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.356E+02 4.463E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.379E+02 5.124E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.400E+02 3.158E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.420E+02 3.166E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.443E+02 1.826E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.486E+02 1.771E-05 +1.110E-05-9.173E-06
 1.573E+02 5.786E-07 +1.596E-06-UNKNOWN
 \END;
 /*===================================================================*/