/*===================================================================*/
 /* NRDF D1876 Data No.3                                              */
 /*===================================================================*/
 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,3;
 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,3;
 /* 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,2*N)111IN;
 ENR=NAT;
 PHYS-FORM=SLD'15';
 /* '15' Rolled foils */
 THK-TGT=7[10MG/CM**2;
 ACC=CYC'16';
 /* '16' 160 cm variable energy cyclotron */
 INST-ACC=2JPNINS;
 DET-PARTCL=GAMMA'17';
 /* '17' Delayed gamma from 111In (ground state) */
 DET-SYS=NAI'18';
 /* '18' To detect the sum peak of the 170 and 240 keV gamma rays
 /* Experimental Method:
    - Chemical separation
 /* Authors assumed that the 10 min isomer of 111In decays only to the
    2.8 day isomer. */
 /* The disintegration rate of 111In was determined by means of
    gamma-gamma coincidence method. */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,3;
 TOT-ERR=X%'4';
 /* '4' Uncertainties in beta- and gamma-ray counting fluctuations,
        decay curve analyses and adopted nuclear data (half-lives,
        branching ratios) */
 ENGY-GAMMA=(170.KEV'19',240.KEV'19');
 HALF-LIFE=2.8DAY'19';
 /* '19' Delayed gamma from 111In (ground state) */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 INC-ENGY-CM
 (MEV) (B) (MB)
 13.6 0.006 +-0.005
 15.4 0.10 X
 17.1 0.30 +-0.08
 18.6 0.52 X
 20.0 0.69 +-0.07
 21.2 0.81 X
 22.5 0.88 X
 24.0 1.03 +-0.09
 25.3 1.10 X
 25.5 0.97 X
 26.6 0.95 X
 28.1 0.90 +-0.08
 29.1 0.78 X
 30.2 0.61 X
 31.1 0.53 X
 31.9 0.48 +-0.07
 32.9 0.36 +-0.06
 33.6 0.32 X
 34.4 0.27 +-0.04
 35.2 0.24 X
 36.1 0.19 X
 37.0 0.15 +-0.02
 38.1 0.12 X
 \END;
 /*===================================================================*/