/*===================================================================*/
 /* NRDF D1738 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 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,2;
 /* 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,FISSN);
 RTY=FISSN;
 PHQ=FISSN-XSECTN;
 ENR=94.5%;
 CHM=ELM;
 THK-TGT=0.4MG/CM**2;
 DET-PARTCL=X'13';
 /* '13' Fission fragments */
 ANL=CC'14';
 /* '14' Coupled Channel Calculation (CCDEF, See.
         J.Fernandez-Niello, C.H.Dasso, S.Landowne, Comput.Phys.Commum.
         54(1989)409. */
 /* Analysis:
    - Integration of angular distribution
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 CMPD=214TH;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-CM SIGMA DELTA-SIGMA
 (MEV) (MB) (MB)
 1.228E+02 2.199E-01 +-4.304E-02
 1.249E+02 2.166E+00 +-3.918E-01
 1.269E+02 8.612E+00 +-1.430E+00
 1.288E+02 1.781E+01 +-2.782E+00
 1.313E+02 3.960E+01 +-6.569E+00
 1.339E+02 7.346E+01 +-1.147E+01
 1.354E+02 1.019E+02 +-1.377E+01
 1.393E+02 1.695E+02 +-2.815E+01
 1.411E+02 1.823E+02 +-2.747E+01
 1.445E+02 2.623E+02 +-4.749E+01
 1.494E+02 3.986E+02 +-6.012E+01
 1.531E+02 4.870E+02 +-1.024E+02
 1.627E+02 7.014E+02 +-9.499E+01
 1.654E+02 6.069E+02 +-1.008E+02
 1.701E+02 7.975E+02 +-1.677E+02
 1.784E+02 6.907E+02 +-8.243E+01
 1.880E+02 9.594E+02 +-9.905E+01
 \END;
 /*===================================================================*/