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 /* NRDF D1775 Data No.15                                             */
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 /* Bibliography                                                      */
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 \\BIB,15;
 D#=D1775;
 TITLE=/ Effects of neutron number and nuclear deformation on
         complete fusion of 60,64Ni+154Sm near the Coulomb barrier /;
 PURPOSE=/ To study the effects of heavy projectile neutron number on
           complete fusiion with a well-deformed target /;
 ATH=(S.MITSUOKA'1', H.IKEZOE'1', K.NISHIO'1', K.SATOU'1', J.LU'1');
 INST-ATH=(2JPNJAE'1');
      /* '1' Advanced Science Research Center */
 REF=PR/C;
 VLP=65(2002)054608;
 RCTS=(154SM(64NI,2*N)216TH, 154SM(64NI,3*N)215TH,
       154SM(64NI,4*N)214TH, 154SM(64NI,5*N)213TH,
       154SM(64NI,6*N)212TH, 154SM(64NI,7*N)211TH, 154SM(64NI,X)215AC,
       154SM(64NI,X)214AC, 154SM(64NI,X)213AC, 154SM(64NI,X)212AC,
       154SM(64NI,X)211AC, 154SM(64NI,X)210AC, 154SM(64NI,X)214RA,
       154SM(64NI,X)213RA, 154SM(64NI,X)212RA, 154SM(64NI,X)211RA,
       154SM(64NI,X)210RA, 154SM(64NI,X)209RA, 154SM(64NI,N)X,
       154SM(64NI,FUSN), 154SM(60NI,FUSN));
 PHQS=(EXC-FUNCT'2', EXC-FUNCT'3', EXC-FUNCT'4', EXC-FUNCT'5',
       EXC-FUNCT'6', EXC-FUNCT'7', EXC-FUNCT'8', EXC-FUNCT'9',
       EXC-FUNCT'10', EXC-FUNCT'11', EXC-FUNCT'12', EXC-FUNCT'13',
       XSECTN'14', X'15');
 /* '2' Evapolation Residue cross section for 2n channel */
 /* '3' Evapolation Residue cross section for 3n channel */
 /* '4' Evapolation Residue cross section for 4n and 5n channel */
 /* '5' Evapolation Residue cross section for 6n and 7n channel */
 /* '6' Evapolation Residue cross section for p+2n channel */
 /* '7' Evapolation Residue cross section for p+3n channel */
 /* '8' Evapolation Residue cross section for p+4n and p+5n channel
 /* '9' Evapolation Residue cross section for p+6n and p+7n channel
 /* '10' Evapolation Residue cross section for 2p+2n channel */
 /* '11' Evapolation Residue cross section for 2p+3n channel */
 /* '12' Evapolation Residue cross section for 2p+4n and 2p+5n
    channel */
 /* '13' Evapolation Residue cross section for alpha+4n and alpha+5n
    channel */
 /* '14' summation of 2n to 7n evaporate cross sections */
 /* '15' Fusion Probability */
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 /* Experimental Conditions                                           */
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 \\EXP,15;
 /* 2003-03-10 : Compiled */
 ENR=98.6%;
 CHM=X'16';
 /* '16' Oxide */
 PHYS-FORM=SLD;
 THK-TGT=0.35MG/CM**2;
 BAC=AL;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT'17';
 /* '17' Jaeri tandem-booster facility */
 INST-ACC=2JPNJAE;
 BEAM-INTNSTY=10[35NA;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'18',SI'19',TOF);
 /* '18' JAERI recoil mass separator (RMS) [H.Ikezoe et al., Nucl.
         Instrum. Methods Phys. Res. A376(1996)420]. */
 /* '19' The alpha peaks from the decay chain of 216Th-212Ra-208Rn
         and 5.486MeV alpha peak from an 241Am source were used for the
         energy calibration of PSSD. */
 SOLID-ANGL=20.0MSR;
 ERS-DET=70KEV'20';
 /* '20' Typical energy resolution of the individual front strips
         (FWHM) */
 EFCN-DET=/ The total efficiency of the present system was typically
            18% and 10% for xn and alpha+xn channels, respectively. /;
 /* Experimental Method:
    - Time-of-flight
 RCT=154SM(60NI,FUSN);
 RTY=FUSN;
 PHQ=X'137';
 /* '137' Fusion Probability */
 INC-ENGY-LAB=(172MEV/A, 175MEV/A, 179MEV/A, 183MEV/A, 187MEV/A,
               190MEV/A, 194MEV/A, 200MEV/A, 205MEV/A, 210MEV/A,
               215MEV/A, 224MEV/A);
 DET-PARTCL=ALPHA;
 ANL=(CC'138',STATIST-MODEL'139');
 /* '138' CCDEF [J.Fernandez-Niello et al, Comput. Phys. Commun.
          54(1989)409]. */
 /* '139' HIVAP [W.Reisdorf and M.Schadel, Z. Phys.
          A343(1992)47]. */
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 /* Descriptive Parameters                                            */
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 \\DATA,15;
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 /* Data Table                                                        */
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 \DATA;
 DATA1'140' DATA2'141' DATA2'142' DELTA-DATA2'142'
 (MEV) (NODIM) (NODIM) (NODIM)
 -17.8 X 3.3e-05 +-X
 -10.8 2.3e-03 X +-4.8e-04
 -8.8 1.3e-03 X +-8.4e-04
 -4.8 2.0e-02 X +-6.0e-03
 1.2 1.2e-01 X +-3.7e-02
 7.2 2.7e-01 X +-5.7e-02
 10.2 3.7e-01 X +-8.9e-02
 14.2 6.0e-01 X +-1.3e-01
 16.2 1.0e+00 X +-2.9e-01
 21.2 9.8e-01 X +-2.8e-01
 \END;
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