/*===================================================================*/
 /* NRDF D1813 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1813;
 TITLE=/Fragment mass distribution of the 239Pu(d,pf) reaction via the
        superdeformed beta-vibrational resonance/;
 PURPOSE=/The authors are interested in resonance fission through the
          beta-vibrational state built on the SD. Then the purpose of
          this experiment is to confirm the enhancement of
          near-symmetric fission by measurement of the mass distribution
          of fission fragments by gating on this resonance./;
 ATH=(K.NISHIO'1', H.IKEZOE'1', Y.NAGAME'1', S.MITSUOKA'1',
      I.NISHINAKA'1', L.DUAN'2', K.SATOU'1', S.GOTO'3', M.ASAI'1',
      H.HABA'1', K.TSUKADA'1', N.SHINOHARA'1', S.ICHIKAWA'1',
      T.OHSAWA'4');
 INST-ATH=(2JPNJAE'1', 3CPRIMP'2', 2JPNNII'3', 2JPNKNK'4');
      /* '1' Advanced Science Research Center */
      /* '3' Department of Chemistry, Faculty of Science */
      /* '4' Department of Electrical & Electronic Engineering, School
            of Science & Engineering */
 REF=PR/C;
 VLP=67(2003)014604;
 RCTS=239PU(D,P,FISSN)A-RESD, 239PU(D,P,FISSN);
 PHQS=(A-DSTRN, MASS'5');
 /* '5' The average value of the heavy fragment mass */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2004-07-26 : Compiled */
 RTY=(FISSN,FISSN,FISSN);
 CHM=PU.O2(NO3)2;
 PHYS-FORM=SLD;
 THK-TGT=0.035MG/CM**2;
 BAC=X'6';
 /* '6' Nickel foil */
 THK-BAC=0.09MG/CM**2;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT'7';
 /* '7' JAERI-tandem accelerator */
 INST-ACC=2JPNJAE;
 INC-ENGY-LAB=13.5MEV;
 BEAM-INTNSTY=5NA;
 POL-PRJ=0%;
 DET-PARTCL=(P,X'8');
 /* '8' Fission Fragments */
 COINC=(P,X'9');
 /* '9' Fission Fragments */
 ANT-COINC=NO;
 DET-SYS=(SI'10',SBD'11');
 /* '10' Used as DeltaE-E telescope to distinguish and detect
         proton. Solid angle is 45 msr. Its resolution is 55 keV. 198Pt
         target was also used to produce elastically scattered
         deuterons and to calibrate the proton detectors. */
 /* '11' Silicon PIN diodes to determine mass of the fission
         fragment. Solid angle is 1.25 sr. The energy calibration of
         the silicon PIN diodes was made by using the Schmitt formula.
 RCT=239PU(D,P,FISSN)A-RESD;
 PHQ=A-DSTRN;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 INC-ENGY-LAB=13.5MEV;
 EMT-1=P;
 INTRM=240PU;
 THTL-1=135DEG;
 EXC-ENGY-INTRM=4.78[5.30MEV;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 A-MIN A-MAX YLD'14' DELTA-YLD'14,15'
 (AMU) (AMU) (%) (%)
   1.195E+02  1.245E+02  2.597E-01  +2.598E-01-2.597E-01
   1.245E+02  1.295E+02  1.558E+00  +6.370E-01-6.358E-01
   1.295E+02  1.345E+02  2.727E+00  +8.420E-01-8.410E-01
   1.345E+02  1.395E+02  6.753E+00  +1.325E+00-1.324E+00
   1.395E+02  1.445E+02  3.896E+00  +1.006E+00-1.006E+00
   1.445E+02  1.495E+02  2.597E+00  +8.220E-01-8.210E-01
   1.495E+02  1.545E+02  1.429E+00  +6.090E-01-6.096E-01
   1.545E+02  1.595E+02  5.195E-01  +3.673E-01-3.673E-01
   1.595E+02  1.645E+02  1.299E-01  +1.836E-01-1.837E-01
   1.645E+02  1.695E+02  1.299E-01  +1.836E-01-1.837E-01
   1.695E+02  1.745E+02  0.000E+00  +0.000E+00-0.000E+00
 \END;
 /*===================================================================*/