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 /* NRDF D1809 Data No.19                                             */
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 /* Bibliography                                                      */
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 \\BIB,19;
 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,19;
 /* 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=PB(ALPHA,P)X;
 THK-TGT=17010MG/CM**2;
 DET-PARTCL=P;
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 /* Descriptive Parameters                                            */
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 \\DATA,19;
 INC-ENGY-LAB=100MEV/A;
 SYS-ERR=(<3%'126',<1%'127',<1%'128');
 /* '126' Uncertainty in the number of accepted beam particles
          incident on the target is estimated to be less than 3%. */
 /* '127' Uncertainty in the solid angle for the thickest carbon
          target, which has the maximum uncertainty, is less than 1%.
 /* '128' 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%'129';
 /* '129' 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%'130';
 /* '130' 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'131'
 (MEV) (MEV) (1/SR/MEV/PARTCL)
   23.198    25.700   1.4252e-06
   25.700    28.636   2.8535e-05
   28.636    31.739   0.00020911
   31.739    35.386   0.00039305
   35.386    39.194   0.00053085
   39.194    43.668   0.00060994
   43.668    48.975   0.00054853
   48.975    54.480   0.00067215
   54.480    61.001   0.00061814
   61.001    67.605   0.00067361
   67.605    75.390   0.00067225
   75.390    84.667   0.00051829
   84.667    93.841   0.00051314
   93.841    104.68   0.00039607
   104.68    117.64   0.00020584
   117.64    133.34   0.00011375
   133.34    148.47   9.4846e-05
   148.47    166.57   6.6334e-05
   166.57    188.54   3.4562e-05
   188.54    215.70   1.1556e-05
   215.70    240.61   6.1193e-06
   240.61    270.72   2.6638e-06
   270.72    307.81   5.2880e-07
   307.81    354.53   3.8161e-08
 \END;
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