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 /* NRDF D1740 Data No.5                                              */
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 /* Bibliography                                                      */
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 \\BIB,5;
 D#=D1740;
 TITLE=/ Fusion of deformed nuclei in the reactions of 76Ge+150Nd and
         28Si+198Pt at the Coulomb barrier region /;
 ATH=(K.NISHIO'1', H.IKEZOE'1', S.MITSUOKA'1', J.LU'2');
 INST-ATH=(2JPNJAE'1', 3CPRIMP'2');
      /* '1' Advanced Science Research Center */
 REF=PR/C;
 VLP=62(2000)014602;
 RCTS=(198PT(28SI,3*N)223U, 198PT(28SI,X)219TH, 198PT(28SI,X)215RA,
       198PT(28SI,4*N)222U, 198PT(28SI,X)218TH, 198PT(28SI,X)214RA,
       198PT(28SI,5*N)221U, 198PT(28SI,X)217TH, 198PT(28SI,6*N)220U,
       198PT(28SI,X)216TH, 198PT(28SI,X)220PA, 198PT(28SI,X)216AC,
       198PT(28SI,X)219PA, 198PT(28SI,X)215AC, 198PT(28SI,X)222PA,
       198PT(28SI,X)221TH, 150ND(76GE,3*N)223U, 150ND(76GE,X)219TH,
       150ND(76GE,X)215RA, 150ND(76GE,4*N)222U, 150ND(76GE,X)218TH,
       150ND(76GE,X)214RA, 150ND(76GE,5*N)221U, 150ND(76GE,X)217TH,
       150ND(76GE,6*N)220U, 150ND(76GE,X)216TH, 150ND(76GE,X)220PA,
       150ND(76GE,X)216AC, 150ND(76GE,X)219PA, 150ND(76GE,X)215AC,
       150ND(76GE,X)222PA, 150ND(76GE,X)221TH, 198PT(28SI,FISSN));
 PHQS=XSECTN;
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 /* Experimental Conditions                                           */
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 \\EXP,5;
 /* 2002-10-30 : Compiled, Am + On. */
 /* 2003-06-13 : Altered, On */
 PHQ=XSECTN;
 PHYS-FORM=SLD;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT'3';
 /* '3' Jaeri-tandem */
 INST-ACC=2JPNJAE;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 MONTR-RCT=/ , Elastic scattering is monitored in order to normalize
             the evaporation regidue cross section. /;
 RCT=(198PT(28SI,X)220PA+198PT(28SI,X)216AC);
 RTY=X'47';
 /* '47' Evapolation */
 ENR=98%;
 CHM=ELM;
 THK-TGT=0.46MG/CM**2;
 BAC=AL;
 THK-BAC=XMG/CM**2'48';
 /* '48' 0.8 micro-meter */
 INC-ENGY-LAB=140.0[179.0MEV;
 DET-PARTCL=(ALPHA'50',ALPHA'49');
 /* '50' Alpha from 212Fr */
 /* '49' Alpha from 216Ac */
 DET-SYS=(MAG'51',PS-SSD'52',SBD'53',TOF'54',EDE);
 /* '51' Recoil mass separator (JAERI-RMS) to separate evaporation
         residues [H.Ikezoe et al., Nucl. Instrum. Meth. A376(1996)420]
 /* '52' Double sided position sensitive detector (DPSD) to obtain
         ToF signal */
 /* '53' To monitor elastic scattering */
 /* '54' To separate evaporation residue implant events from the
         subsequent alpha decays and to estimate mass number of
         incoming particles */
 ERS-DET=75KEV'55';
 /* '55' FWHM */
 CALB-DET=/ DPSD was calibrated using known alpha line from
            214Ra(7.137MeV), 215Ra(8.700MeV) and 216Th(7.921MeV) which
            are produced in the present reactions. /;
 ANL=STATIST-MODEL'56';
 /* '56' HIVAP, See [W.Reisdorf and M.Schadel,
         Z.Phys.A343(1992)47]. */
 /* Experimental Method:
    - Time-of-flight (To separate evaporation residue implant events
      from the subsequent alpha decays and to estimate mass number of
      incoming particles)
    - Particle identification by 'E/Delta E' measurement
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 /* Descriptive Parameters                                            */
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 \\DATA,5;
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 /* Data Table                                                        */
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 \DATA;
 INC-ENGY-CM XSECTN DELTA-XSECTN INC-ENGY-LAB'57'
 (MEV) (NB) (NB) (MEV)
 135.0 25.0 +32.0-24.0 156.9
 137.5 32.0 +24.0-20.0 159.7
 140.0 21.0 +27.0-18.0 162.6
 142.5 18.0 +23.0-15.0 165.4
 145.0 68.0 +45.0-40.0 168.2
 147.5 42.0 +37.0-27.0 171.0
 150.0 143.0 +83.0-83.0 173.9
 152.5 135.0 +73.0-73.0 176.7
 155.0 210.0 +120.0-120.0 179.0
 \END;
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