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 /*===================================================================*/
 /* NRDF D2026 Data No.10                                             */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,10;
 D#=D2026;
 TITLE=/ Rare gas isotope yields in Bremsstrahlung-induced nuclear
         reactions of 41K, 87Rb, 127I, 133Cs, and 139La /;
 ATH=(Y.OURA'2', A.YAZAWA'1', M.YOSHIDA'1', S.R.SARKAR'2', K.SAKAMOTO'1,
     2', S.SHIBATA'3', I.FUJIWARA'4', M.FURUKAWA'5');
 INST-ATH=(2JPNKNZ'1', 2JPNKNZ'2', 2JPNINS'3', 2JPNJPN'4',
           2JPNNAG'5');
      /* '1' Department of Chemistry */
      /* '2' Division of Physical Sciences, Graduate School of Natural
              Science and Technology */
      /* '4' School of Economics, Otemon Gakuin Univ., Ibaragi */
      /* '5' Department of Chemistry */
 REF=RCA;
 VLP=68(1995)27;
 RCTS=(41K(GAMMA,PIP)41AR, 87RB(GAMMA,PIP)87KR, 133CS(GAMMA,PIP)133XE,
       127I(GAMMA,PIN)127XE, 127I(GAMMA,PIN,2*N)125XE,
       127I(GAMMA,PIN,4*N)123XE, 127I(GAMMA,PIN,5*N)122XE,
       127I(GAMMA,PIN,6*N)121XE, 133CS(GAMMA,X)131XE,
       133CS(GAMMA,X)129XE, 133CS(GAMMA,X)127XE, 133CS(GAMMA,X)125XE,
       133CS(GAMMA,X)123XE, 133CS(GAMMA,X)122XE, 133CS(GAMMA,X)121XE,
       139LA(GAMMA,X)129XE, 139LA(GAMMA,X)127XE, 139LA(GAMMA,X)125XE,
       139LA(GAMMA,X)123XE, 139LA(GAMMA,X)122XE, 139LA(GAMMA,X)121XE);
 PHQS=XSECTN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,10;
 /* 2007-02-17 : Compiled, N.Otuka */
 /* Related references 
    - S.R.Sarkar et al., RCA, 55(1991)139.
    (Correction for isobaric precursor decays)
 PHQ=XSECTN;
 PHYS-FORM=SLD;
 THK-TGT=([640MG/CM**2,[860MG/CM**2);
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=(LINAC'6',SYN'7');
 /* '6' 300 MeV electron linac for E(max) <250 MeV */
 /* '7' 1.3 GeV electron synchrotron for E(max) >250 MeV */
 INST-ACC=(2JPNTOH'8',2JPNINS);
 /* '8' Laboratory of Nuclear Science */
 POL-PRJ=0%;
 ION-SOURCE=/ Bremsstrahlung (By internal target of Pt with 0.5 mm
              (Sendai) or 0.05 mm (Tokyo) thickness) /;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=HPGE'9';
 /* '9' To perform gamma-ray measurement */
 ANL=X'10';
 /* '10' Cascade-evaporation code PICA */
 /* Experimental Method:
    - Activation (Irradiated for 5-10 min (Sendai) and 60-240 min
      (Tokyo))
    - Gamma ray spectrometry (Measured over 3 months)
 /* Authors give yield with unit of [micro-barn/equivalent quantum]. */
 /* Correction of isobaric precursor decays by iterative non-linear
    squares fit for cumulative yields */
 /* Related references 
    - S.R.Sarkar et al., RCA, 55(1991)113.
    (Compared with present data). See also EXFOR K2027.116.
 RCT=133CS(GAMMA,X)129XE;
 CHM=X'50';
 /* '50' CsCl */
 INC-ENGY-LAB-RANGE=80[1000MEV;
 DET-PARTCL=GAMMA'51';
 /* '51' Delayed gamma from 129Xe (metastable state) */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,10;
 ENGY-GAMMA=196.6KEV'52';
 INTNSTY-GAMMA=0.0459'52';
 HALF-LIFE=8.89DAY'52';
 /* '52' Delayed gamma from 129Xe (metastable state) */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-LAB-MAX SIGMA'53' DELTA-SIGMA'53,53'
 (MEV) (UB) (UB)
 1000 1.71 +-0.49
 900 1.64 +-0.22
 850 2.78 +-0.22
 800 1.12 +-0.6
 650 2.46 +-0.28
 600 1.17 +-0.86
 500 1.1 +-0.63
 450 1.73 +-0.28
 400 1.05 +-0.69
 365 0.96 +-0.53
 320 1.31 +-0.29
 320 1.54 +-0.4
 320 1.13 +-0.15
 315 0.7 +-0.15
 275 0.76 +-0.38
 250 0.8 +-0.26
 250 1.07 +-0.3
 180 0.76 +-0.05
 150 0.46 +-0.22
 90 0.23 +-0.08
 80 0.2 +-0.02
 \END;
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