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 /* NRDF D1626 Data No.8                                              */
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 /* Bibliography                                                      */
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 \\BIB,8;
 D#=D1626;
 TITLE=/ Binary decay fragment cross sections and prescission charge
         multiplicity in 84Kr+27Al at 10.6MeV/nucleon /;
 PURPOSE=/ To suggest the mechanizm of a binary decay in thelighter
           mass system /;
 ATH=(K.YUASA-NAKAGAWA'1', J.KASAGI'1', T.NAKAGAWA'2', K.YOSHIDA'2',
      Y.FUTAMI'3', S.M.LEE'3', K.FURUTAKA'4', K.MATSUDA'4',
      W.Q.SHEN'5');
 INST-ATH=(2JPNTOH'1', 2JPNIPC'2', 2JPNTSU'3', 2JPNTIT'4',
           3CPRNRS'5');
      /* '1' Laboratory of Nuclear Science */
      /* '3' Institute of Physics */
      /* '4' Department of Physics */
 REF=PR/C;
 VLP=53(1996)997;
 RCTS=(27AL(84KR,P)X, 27AL(84KR,ALPHA)X, 27AL(84KR,FISSN));
 PHQS=(ENGY-SPEC'6', XSECTN);
 /* '6' Light charged particles multiplicity in coincidence with
    heavy fragments */
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 /* Experimental Conditions                                           */
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 \\EXP,8;
 /* 2003-08-21 : Converted, Am + On. Data converted to EXFOR E1626
 /* 2007-04-06 : Altered, On. REL-REF corrected */
 /* 2007-05-10 : Altered, On. TITLE corrected */
 /* Related references 
    - T.Mizota et al., NIM/A, 305(1991)125.
    (Details of the experiment and some of the results of the cross
    section measurement)
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.6MG/CM**2;
 BAC=SELF;
 ACC=CYC;
 INST-ACC=2JPNIPC'7';
 /* '7' RIKEN Accelerator Research Facility */
 INC-ENGY-LAB=10.6MEV/A;
 ANT-COINC=NO;
 DET-SYS=(X'8',SSD'9',SCT'10',TOF);
 /* '8' Channel plate detector used as ToF counter for heavy
        fragments. Placed at 10 deg away from the beam axis and flight
        path was 35 cm. */
 /* '9' To detect heavy fragments (Solid angle is about 4 msr) */
 /* '10' Phoswich detector consisted of a thin plastic
         scintillator (NE102A, 100 or 200 micro-meter in thickness) and
         a thick (180 mm) BaF2 crystal. To detect light charged
         particles (Z=1 and 2). Solid angle is 3 pi. Calibration was
         done by using elastically scattered protons and alpha
         particles at the energy ranges of 10-20 and 15-30 MeV,
         respectively. */
 /* 2006-10-26 : Altered, On. Re-digitized */
 RCT=27AL(84KR,ALPHA)X;
 PHQ=ENGY-SPEC'39';
 /* '39' Light charged particles multiplicity in coincidence with
         heavy fragments */
 DET-PARTCL=(ALPHA,X'40');
 /* '40' Fission fragments, 40