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 /* NRDF D1749 Data No.4                                              */
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 /* Bibliography                                                      */
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 \\BIB,4;
 D#=D1749;
 TITLE=/ Effects of nuclear deformation on fusion probability in the
         reactions of 82Se+natCe and 76Ge+150Nd near the Coulomb
         barrier /;
 PURPOSE=/ To test the supposition that the 76Ge+150Nd system
           exhibits larger fusion probability than the system
           consisting of spherical colliding nuclei whose Z1Z2 value is
           close to that of 76Ge+150Nd /;
 ATH=(K.NISHIO'1', H.IKEZOE'1', S.MITSUOKA'1', K.SATOU'1',
      S.C.JEONG'2');
 INST-ATH=(2JPNJAE'1', 2JPNKEK'2');
      /* '1' Advanced Science Research Center */
      /* '2' Institute of Particle and Nuclear Studies */
 REF=PR/C;
 VLP=63(2001)044610;
 RCTS=(CE(82SE,X)214TH, CE(82SE,X)219U, CE(82SE,X)215TH,
       CE(82SE,X)213AC, CE(82SE,X)220U, CE(82SE,X)216TH,
       CE(82SE,X)221U, CE(82SE,X)217TH, CE(82SE,X)218PA,
       CE(82SE,X)214AC, CE(82SE,X)219PA, CE(82SE,X)215AC,
       CE(82SE,X)220PA, CE(82SE,X)216AC);
 PHQS=XSECTN;
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 /* Experimental Conditions                                           */
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 \\EXP,4;
 /* 2002-02-10 : Converted, Data converted to EXFOR E1749. */
 /* 2003-06-13 : Altered */
 PHQ=XSECTN;
 ENR=NAT'3';
 /* '3' Abundance of 140Ce and 142Ce are 88.5 and 11.1%. */
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.425MG/CM**2;
 BAC=AL;
 THK-BAC=XMG/CM**2'4';
 /* '4' 1.5 micro-meter thick aluminium foil */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT'5';
 /* '5' JAERI-tandem booster accelerator */
 INST-ACC=2JPNJAE;
 INC-ENGY-CM=215.0[253.0MEV;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(MAG'6',PS-SSD'7',SBD'8',TOF'9');
 /* '6' JAERI recoil mass separater (JAERI-RMS) */
 /* '7' Double sided position-sensitive strip detector (DPSD).
        Energy calibration of the DPSD was made using known alpha
        transition energy from 216Th(7.921MeV) which were produced in
        the present reactions. */
 /* '8' To monitor the beams, set at 45 deg direction in the target
        chamber to determine the absolute values of the evaporation
        residue cross sections. */
 /* '9' Two-dimensional spectrum of the energy versus TOF signal
        was used to distinguish evaporation residue (ER) implantation
        events from the subsequent alpha decays, which generate no TOF
        signal */
 ERS-DET=70KEV'10';
 /* '10' typical value for DPSD */
 EFCN-DET=/ Estimated transport efficiency of evaporation residue to
            the focal plane detectors through the JAERI-RMS is
            estimated. The values are 0.22-0.33 for alpha-xn channels
            and 0.29-0.40 for xn channel. /;
 ANL=STATIST-MODEL'11';
 /* '11' HIVAP, See [W.Reisdorf and M.Schadel, ZP/A343(1992)47].
 /* Experimental Method:
    - Time-of-flight (Two-dimensional spectrum of the energy versus
      TOF signal was used to distinguish evaporation residue (ER)
      implantation events from the subsequent alpha decays, which
      generate no TOF signal)
 RCT=(CE(82SE,X)221U+CE(82SE,X)217TH);
 DET-PARTCL=(ALPHA'23',ALPHA'22');
 /* '23' Alpha from 213Ra */
 /* '22' Alpha from 217Th */
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 /* Descriptive Parameters                                            */
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 \\DATA,4;
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-CM XSECTN XSECTN'24' DELTA-XSECTN'24'
 (MEV) (NB) (NB) (NB)
 215.0 17.3 X +18.0-13.2
 220.0 11.2 X +11.6-8.5
 223.0 X 4.7 +X-X
 228.0 8.4 X +11.0-7.3
 230.0 10.0 X +10.4-7.7
 233.0 25.6 X +33.5-22.2
 238.0 21.6 X +28.2-18.7
 243.0 X 12.5 +X-X
 245.0 X 2.9 +X-X
 253.0 X 8.2 +X-X
 \END;
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