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 /* NRDF D1809 Data No.13                                             */
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 /* Bibliography                                                      */
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 \\BIB,13;
 D#=D1809;
 TITLE=/Spectral measurements of neutrons, protons, deuterons and
        tritons produced by 100 MeV/nucleon He bombardment/;
 PURPOSE=/To present the angular-energy distributions of neutrons,
          protons, deuterons and tritons produced from thick carbon,
          aluminum, copper and lead targets bombarded by 100 MeV/nucleon
          helium ion. /;
 ATH=(T.KUROSAWA'1', T.NAKAMURA'1', N.NAKAO'2', T.SHIBATA'3',
      Y.UWAMINO'4', A.FUKUMURA'5');
 INST-ATH=(2JPNTOH'1', 2JPNKEK'2', 2JPNKEK'3', 2JPNIPC'4', 2JPNIRS'5');
      /* '1' Cyclotron and Radioisotope Center */
      /* '2' Tanashi Branch */
 REF=NIM/A;
 VLP=430(1999)400;
 RCTS=(12C(ALPHA,P)X, 27AL(ALPHA,P)X, CU(ALPHA,P)X, PB(ALPHA,P)X,
       12C(ALPHA,D)X, 27AL(ALPHA,D)X, CU(ALPHA,D)X, PB(ALPHA,D)X,
       12C(ALPHA,T)X, 27AL(ALPHA,T)X, CU(ALPHA,T)X, PB(ALPHA,T)X);
 PHQS=ENGY-SPEC'6';
 /* '6' Double differential thick target yield */
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 /* Experimental Conditions                                           */
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 \\EXP,13;
 /* 2003-09-13 : Compiled */
 PHQ=ENGY-SPEC'7';
 /* '7' Double differential thick target yield */
 ENR=X%;
 CHM=ELM;
 PHYS-FORM=SLD;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN'8';
 /* '8' Heavy Ion Medical Accelerator in Chiba (HIMAC) */
 INST-ACC=2JPNIRS;
 INC-ENGY-LAB=100MEV/A;
 POL-PRJ=0%;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'9',SCT'10',TOF'11',EDE'12');
 /* '9' Plastic scintillator (NE102A) was used as the delta-E
        counter, ToF start signal detector, and incident projectile
        counter */
 /* '10' Liquid scintillator (NE213) was used as the E counter */
 /* '11' To measure the energy of outgoing neutrons, protons,
         deuterons and tritons */
 /* '12' To eliminate charged particles */
 ANL=MONTE-MTHD'13';
 /* '13' LAHET Monte Carlo Code System, LCS [R.E. Prael, H.
         Lichtenstein, LA-UR-89-3014, Los Alamos National Laboratory,
         1989.] */
 /* Experimental Method:
    - Time-of-flight (To measure the energy of outgoing neutrons,
      protons, deuterons and tritons)
    - Particle identification by 'E/Delta E' measurement (To
      eliminate charged particles)
 RCT=CU(ALPHA,P)X;
 THK-TGT=13395MG/CM**2;
 DET-PARTCL=P;
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 /* Descriptive Parameters                                            */
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 \\DATA,13;
 INC-ENGY-LAB=100MEV/A;
 SYS-ERR=(<3%'90',<1%'91',<1%'92');
 /* '90' Uncertainty in the number of accepted beam particles
         incident on the target is estimated to be less than 3%. */
 /* '91' Uncertainty in the solid angle for the thickest carbon
         target, which has the maximum uncertainty, is less than 1%. */
 /* '92' Uncertainty of charged particle detection efficiency is
         estimated to be 1%, considering a small fraction of the slant
         incidence of a particle onto the detector. */
 STATIST-ERR=X%'93';
 /* '93' The statistical uncertainties vary from 2-5% in the low
         to medium energy (5-50 MeV) region of the spectra and increase
         to about 30% at the highest energies. */
 EMT=P;
 THTL=0DEG;
 DELTA-DN/DOMEGA/DE=<4%'94';
 /* '94' Total normalization uncertainty */
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 /* Data Table                                                        */
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 \DATA;
 ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE'95'
 (MEV) (MEV) (1/SR/MEV/PARTCL)
   24.152    26.817   2.0427e-05
   26.817    29.955   0.00010004
   29.955    33.286   0.00074989
   33.286    37.216   0.00091929
   37.216    41.338   0.0011455
   41.338    46.205   0.0011044
   46.205    51.224   0.0012969
   51.224    57.136   0.0013615
   57.136    64.172   0.0011584
   64.172    71.333   0.0013106
   71.333    79.818   0.0011947
   79.818    89.992   0.00086322
   89.992    100.12   0.00081252
   100.12    112.16   0.00047858
   112.16    126.68   0.00025107
   126.68    140.58   0.00020322
   140.58    157.10   0.00013987
   157.10    177.00   8.3874e-05
   177.00    201.37   3.0582e-05
   201.37    223.51   1.8535e-05
   223.51    249.99   8.3768e-06
   249.99    282.20   2.6646e-06
   282.20    322.14   6.2893e-07
 \END;
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