/*===================================================================*/
 /* NRDF D1979 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1979;
 TITLE=/ Measurements of evaporation residue cross sections for the
         fusion reactions 86Kr+134Ba and 86Kr+138Ba /;
 PURPOSE=/ To investigate the effect of the shell structure of the
           interacting nuclei on fusion process /;
 ATH=(K.SATOU'1', H.IKEZOE'2', S.MITSUOKA'2', K.NISHIO'2', C.J.LIN'3',
      S.C.JEONG'4');
 INST-ATH=(2JPNJAE'1', 2JPNJAE'2', 3CPRAEP'3', 2JPNKEK'4');
      /* '1' Quantum Beam Science Directorate */
      /* '2' Advanced Science Research Center */
      /* '4' Institute of Particle and Nuclear Studies */
 REF=PR/C;
 VLP=73(2006)034609;
 RCTS=(138BA(86KR,N)223U, 138BA(86KR,X)219TH, 138BA(86KR,X)215RA,
       138BA(86KR,2*N)222U, 138BA(86KR,X)218TH, 138BA(86KR,X)214RA,
       138BA(86KR,X)222PA, 138BA(86KR,X)218AC, 138BA(86KR,3*N)221U,
       138BA(86KR,X)217TH, 134BA(86KR,N)219U, 134BA(86KR,X)215TH,
       134BA(86KR,2*N)218U, 134BA(86KR,X)214TH, 134BA(86KR,X)218PA,
       134BA(86KR,X)214AC);
 PHQS=XSECTN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2006-10-04 : Compiled, Tt + On */
 PHQ=XSECTN;
 CHM=ELM;
 PHYS-FORM=SLD;
 THK-TGT=0.40[0.45MG/CM**2;
 BAC=AL;
 THK-BAC=XMG/CM**2'5';
 /* '5' 1.3 micro-meter */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNJAE'6';
 /* '6' JAERI-tandem booster accelerator */
 BEAM-INTNSTY=15PNA;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SBD'7',MAG'8',error'9',MCPLT'10',TOF'11');
 /* '7' To detect elastically scattered Kr beams to determine
        absolute value of evaporation residue cross sections */
 /* '8' Recoil mass separator to separate evaporation residues
        (JAERI-RMS) */
 /* '9' To measure energies and positions of incoming particle and
        its subsequent alpha decays */
 /* '10' To obtain time-of-flight signals of incoming particles */
 /* '11' To distinguish incoming particles from subsequent
         alpha-decay */
 ANL=STATIST-MODEL'12';
 /* '12' Statistical model code HIVAP */
 RCT=(138BA(86KR,2*N)222U+138BA(86KR,X)218TH+138BA(86KR,X)214RA);
 ENR=99.7%;
 DET-PARTCL=(ALPHA'15',218TH,214RA,222U);
 /* '15' Alpha from 214Ra */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 SYS-ERR=40%'13';
 /* '13' Total systematic error. Uncertainty in transport
         efficiency in JAERI-RMS and charge distribution of evaporation
         residues */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-CM SIGMA DELTA-SIGMA
 (MEV) (NB) (NB)
 209.3 5 +11-5
 211.3 6 +12-6
 217.3 14 +18-12
 218.6 4 +9-4
 221.1 13 +12-8
 222.9 22 +22-15
 225.3 19 +38-19
 226.6 23 +47-23
 229.4 250 +170-140
 232.3 140 +120-90
 233.1 110 +140-90
 237.4 180 +130-100
 \END;
 /*===================================================================*/