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 /* NRDF D1841 Data No.52                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,52;
 D#=D1841;
 TITLE=/Shell and odd-even effects on alpha-particle energy spectra
        from the (p,alpha) reaction on nuclei around neutron number 50/;
 PURPOSE=/To clarify the shell and odd-even effects on the (p,alpha)
          reaction/;
 ATH=(I.KUMABE'1', Y.MITO'1', M.HYAKUTAKE'1', N.KOORI'1', H.SAKAI'1',
      Y.WATANABE'1');
 INST-ATH=(2JPNKYU'1');
      /* '1' Department of Nuclear Engineering */
 REF=PR/C;
 VLP=35(1987)467;
 RCTS=(92MO(P,ALPHA)X, 94MO(P,ALPHA)X, 93NB(P,ALPHA)X,
       106PD(P,ALPHA)X, AG(P,ALPHA)X, 90ZR(P,ALPHA)X, 96MO(P,ALPHA)X,
       98MO(P,ALPHA)X, 100MO(P,ALPHA)X);
 PHQS=(ENGY-SPEC, ENGY-SPEC'2');
 /* '2' Angular integrated energy spectrum */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,52;
 /* 2003-11-11 : Converted, Data converted from EXFOR E1303.
    Numerical data are exchanged with author's one. Many data tables
    are added. */
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=SELF;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=VDGT;
 INST-ACC=2JPNKYU;
 BEAM-INTNSTY=20[300NA'3';
 /* '3' Smaller beam currents were used at forward angles in order
        to reduce the dead time for the detector system. */
 POL-PRJ=0%;
 DET-PARTCL=ALPHA;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=SBD'4';
 /* '4' To analyze and detect alpha-particle. Used as Delta E-E
        counter. Silicon surface barrier detectors having thickness of
        15 and 300 micro-meter. The energy scale for alpha-particles
        was calibrated using the position of the alpha-particle peaks
        leading to the ground states of the residual nucleus for high
        energy calibration points. Low energy calibration points were
        obtained using the positions of the alpha-particle peaks
        leading to low lying states of 13N in the 16O(p,alpha)13N
        reaction on the oxygen impurities on the targets. */
 /* Experimental Method:
    - Particle identification by 'E/Delta E' measurement (To identify
      alpha-particles from other reaction products)
 RCT=235U(P,FISSN)103RU;
 ENR=>99.0%;
 INC-ENGY-LAB-RANGE=9[18MEV;
 DET-PARTCL=GAMMA'142';
 /* '142' Delayed gamma from 103Ru */
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 /* Descriptive Parameters                                            */
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 \\DATA,52;
 TOT-ERR=X%'143';
 /* '143' The errors cited originate from the consideration of
          gamma-counting statistics and the half-life fitting for the
          decay of the photopeak area. */
 ENGY-GAMMA=497.1KEV'144';
 INTNSTY-GAMMA=0.895'144';
 HALF-LIFE=39.25DAY'144';
 /* '144' Delayed gamma from 103Ru */
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-LAB SIGMA DELTA-SIGMA
 (MEV) (MB) (MB)
 9.0 0.19 +-0.02
 10.2 1.58 +-0.10
 11.4 4.09 +-0.22
 12.0 5.63 +-0.16
 12.5 10.01 +-0.80
 13.6 14.59 +-0.54
 14.6 22.63 +-0.84
 15.6 30.14 +-0.80
 18.0 47.16 +-1.87
 \END;
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