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 /* NRDF D1829 Data No.26                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,26;
 D#=D1829;
 TITLE=/Measurement and calculation of radioactivities of spallation
        products by high-energy heavy ions/;
 ATH=(H.YASHIMA'1', Y.UWAMINO'2', H.IWASE'1', H.SUGITA'1',
      T.NAKAMURA'1', S.ITO'2', A.FUKUMURA'3');
 INST-ATH=(2JPNTOH'1', 2JPNIPC'2', 2JPNIRS'3');
      /* '1' Cyclotron and Radioisotope Center */
 REF=RCA;
 VLP=91(2003)689;
 RCTS=(CU(40AR,X)X, CU(20NE,X)X, CU(12C,X)X, CU(ALPHA,X)X, CU(P,X)X,
       27AL(40AR,X)X, 27AL(20NE,X)X, 27AL(12C,X)X, 27AL(ALPHA,X)X,
       27AL(P,X)X, 12C(40AR,X)X, 12C(20NE,X)X, 12C(12C,X)X,
       12C(ALPHA,X)X, 12C(P,X)X, CU(P,X)60CU, CU(P,X)58CO, CU(P,X)54MN,
       CU(P,X)48CR, CU(ALPHA,X)41AR, CU(ALPHA,X)39CL, CU(12C,X)41AR,
       CU(12C,X)39CL, CU(20NE,X)41AR, CU(20NE,X)39CL);
 PHQS=(XSECTN'4', XSECTN'5');
 /* '4' Independent yield */
 /* '5' Cummulative yield */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,26;
 /* 2004-04-08 : Compiled */
 /* Additional result not compiled:
    - Spatial distribution of residual radioactivities in Cu target
      assembly
 ENR=NAT;
 CHM=ELM'6';
 /* '6' Chemical purities are 99.9% / 99.4% / 99.8% for copper,
        aluminium and carbon target, respectively. */
 PHYS-FORM=SLD;
 THK-TGT=XMG/CM**2'7';
 /* '7' HxWxT (mm) = 90x100x0.1 / 90x100x0.1 / 50x50x0.2 for
        cupper, aluminium and carbon target, respectively. */
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN;
 INST-ACC=2JPNIRS'8';
 /* '8' HIMAC facility */
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(HPGE'9',IC'10');
 /* '9' To measure gamma-ray spectra from samples */
 /* '10' To monitor beam current during irradiation */
 /* Experimental Method:
    - Activation
    - Beam current integrated
    - Stacked target irradiation (Samples put on the front of surface
      were used for measurements of the reaction cross section and the
      mass-yield distributions or produced nuclides, while samples
      inserted between the Cu plates were used for measurements of the
      spatial distribution of the residual activities of produced
      nuclides in copper and of the energy dependence of the cross
      section.)
 /* Comment to data: Decay data of 11C are not shown in reference, but
    obtained by private communication */
 RCT=27AL(ALPHA,X)X;
 PHQ=XSECTN'161';
 /* '161' Cummulative yield */
 INC-ENGY-LAB=230MEV/A;
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 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,26;
 INC-ENGY-LAB=230MEV/A;
 TOT-ERR=2[40%;
 SYS-ERR=(0.5[7.2%'162',1[6%'163');
 /* '162' Error of peak efficiency */
 /* '163' Error of beam intensity */
 STATIST-ERR=1[40%'164';
 /* '164' Error of total counts of gamma-ray peak area */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 Z A XSECTN DELTA-XSECTN'165' FLAG'166'
 (NODIM) (NODIM) (MB) (MB) (NODIM)
  11  24  25.8 +-0.61  4
 \END;
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