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 /* NRDF D1877 Data No.2                                              */
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 /* Bibliography                                                      */
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 \\BIB,2;
 D#=D1877;
 TITLE=/ Excitation functions for proton-induced reactions of 140Ce and
        142Ce up to Ep=15 MeV /;
 ATH=(M.FURUKAWA'1');
 INST-ATH=(2JPNTOK'1');
      /* '1' Department of Chemistry, Faculty of Science */
 REF=NP/A'2';
 VLP=90(1967)253'2';
 /* '2' Misprinted as Vol.67 at the top of the first page */
 RCTS=(140CE(P,N)140PR, 140CE(P,2*N)139PR, 142CE(P,N)142PR);
 PHQS=XSECTN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2004-02-26 : Compiled, Kc + On */
 PHQ=XSECTN;
 /* Additional results shown but not compiled
    - Total reaction cross section (The sum of measured cross
      sections for 140Ce is compared with the calculation on the basis
      of the continuum theory [M.M. Shapiro, Phys. Rev. 90(1953)171].)
 ENR=NAT;
 CHM=X'3';
 /* '3' Ceric oxide or cerous fluoride */
 PHYS-FORM=SLD;
 THK-TGT=[5MG/CM**2;
 BAC=AL'4';
 /* '4' Deposited on aluminium foil */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=CYC;
 INST-ACC=2JPNINS;
 BEAM-INTNSTY=[0.5UA;
 POL-PRJ=0%;
 ANT-COINC=NO;
 ANL=STATIST-MODEL;
 /* Experimental Method:
    - Activation (Irradiated between 0.5 min and 2 h)
    - Energy degradation by foils (Degraded by aluminium placed
      between targets. The stopping power was taken from the
      compilation of Sternheimer [R.M. Sternheimer, Phys. Rev.
      115(1959)137].)
 RCT=140CE(P,2*N)139PR;
 DET-PARTCL=GAMMA'8';
 /* '8' Delayed gamma from 139Pr. Conversion electron emission is
        taken into account for given abundance. */
 COINC=NO;
 DET-SYS=NAI'9';
 /* '9' To detect 166 keV decay gamma from 139Ce */
 /* Experimental Method:
    - Chemical separation
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 /* Descriptive Parameters                                            */
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 \\DATA,2;
 TOT-ERR=X%'10';
 /* '10' Uncertainties in target thickness, beam currents and
         disintegration rates of residual nuclei */
 RSD=139PR;
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 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-LAB XSECTN DELTA-XSECTN
 (MEV) (MB) (MB)
 13.28 91 +-15
 14.04 281 +-42
 14.58 447 +-67
 \END;
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