/*===================================================================*/
 /* NRDF D1876 Data No.2                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,2;
 D#=D1876;
 TITLE=/ Excitation functions for the reactions induced by alpha
         particles on 109Ag /;
 ATH=(S.FUKUSHIMA'1', S.KUME'1', H.OKAMURA'1', K.OTOZAI'1',
      K.SAKAMOTO'1', Y.YOSHIZAWA'1', S.HAYASHI'2');
 INST-ATH=(2JPNOSA'1', 2JPNJPN'2');
      /* '1' Faculty of Science */
      /* '2' Osaka Public Health Institute, Osaka */
 REF=NP;
 VLP=69(1965)273;
 RCTS=(109AG(ALPHA,N)112IN, 109AG(ALPHA,2*N)111IN,
       109AG(ALPHA,3*N)110IN);
 PHQS=XSECTN;
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,2;
 /* 2004-02-25 : Compiled+Checked, Kc + On */
 /* 2010-06-04 : Altered, Tsubakihara. 002-006 DATA,ERR-T: MB -> B
 PHQ=XSECTN;
 CHM=ELM;
 POL-TGT=0%;
 ALGN-TGT=0%;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 ANL=STATIST-MODEL'3';
 /* '3' Using level density expressions based on the Fermi gas
        model */
 /* Experimental Method:
    - Stacked target irradiation (Stacks consisted of the 109Ag foils
      and aluminium foils or of the natural silver foils only.)
    - Energy degradation by foils (Energy degradation by aluminium
      foils)
 /* Analysis:
    - Decay curve analysis (Initial activities were computed by the
      least-squares method using know half-lives.)
 RCT=109AG(ALPHA,N)112IN;
 ENR=99.8%;
 PHYS-FORM=SLD;
 THK-TGT=8MG/CM**2;
 BAC=X'10';
 /* '10' Electro-deposited onto iron foils */
 ACC=CYC'11';
 /* '11' 110 cm cyclotron */
 INST-ACC=2JPNOSA;
 DET-PARTCL=BETA'12';
 /* '12' Beta from 112In (metastable state). Beta rays higher than
         0.3 MeV were counted. The half-life of the longer-lived isomer
         was obtained as the weighted mean value of the published data.
 DET-SYS=X'13';
 /* '13' Anthracene crystal */
 /* Disintegration rate of 112In was determined from the annihilation
    radiation measurement with NaI(Tl) crystal which was calibrated
    with a 22Na standard source. The position branching was taken to be
    21.6%. */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,2;
 TOT-ERR=X%'4';
 /* '4' Uncertainties in beta- and gamma-ray counting fluctuations,
        decay curve analyses and adopted nuclear data (half-lives,
        branching ratios) */
 HALF-LIFE=20.8MIN'14';
 /* '14' Beta from 112In (metastable state) (Beta rays higher than
         0.3 MeV were counted. The half-life of the longer-lived isomer
         was obtained as the weighted mean value of the published
         data.) */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-CM
 (MEV) (B) (MB)
 9.7 0.0005 +-0.0002
 11.5 0.014 +-0.004
 13.8 0.18 +-0.04
 15.2 0.26 +-0.06
 17.5 0.30 +-0.07
 19.5 0.21 +-0.05
 \END;
 /*===================================================================*/