/*===================================================================*/
 /* NRDF D1738 Data No.8                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,8;
 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,8;
 /* 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)209RA+182W(32S,X)210RA);
 PHQ=EXC-FUNCT'44';
 /* '44' for fusion-evapolation cross section */
 ENR=94.5%;
 CHM=ELM;
 THK-TGT=0.4MG/CM**2;
 DET-PARTCL=(ALPHA'47',ALPHA'48',ALPHA'45',ALPHA'46');
 /* '48' Alpha from 205Rn */
 /* '47' Alpha from 206Rn */
 /* '46' Alpha from 209Ra */
 /* '45' Alpha from 210Ra */
 ANL=STATIST-MODEL'49';
 /* '49' HIVAP, See [W.Reisdorf and M.Schadel,
         Z.Phys.A343(1992)47]. */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,8;
 SYS-ERR=40%'50';
 /* '50' 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 1.771E-05 +6.766E-06-5.891E-06
 1.271E+02 3.609E-06 +2.579E-06-2.313E-06
 1.292E+02 1.150E-05 +6.206E-06-5.317E-06
 1.335E+02 2.257E-05 +1.410E-05-1.225E-05
 1.358E+02 1.078E-04 +3.337E-05-2.092E-05
 1.379E+02 2.116E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.400E+02 2.357E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.421E+02 3.171E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.444E+02 6.746E-04 +NEGLIGIBLE-NEGLIGIBLE
 1.486E+02 5.292E-04 +NEGLIGIBLE-NEGLIGIBLE
 \END;
 /*===================================================================*/