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 /* NRDF D1809 Data No.15                                             */
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 /* Bibliography                                                      */
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 \\BIB,15;
 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,15;
 /* 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,15;
 INC-ENGY-LAB=100MEV/A;
 SYS-ERR=(<3%'102',<1%'103',<1%'104');
 /* '102' Uncertainty in the number of accepted beam particles
          incident on the target is estimated to be less than 3%. */
 /* '103' Uncertainty in the solid angle for the thickest carbon
          target, which has the maximum uncertainty, is less than 1%.
 /* '104' 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%'105';
 /* '105' 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=15DEG;
 DELTA-DN/DOMEGA/DE=<4%'106';
 /* '106' 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'107'
 (MEV) (MEV) (1/SR/MEV/PARTCL)
   24.770    27.774   1.3911e-05
   27.774    30.814   0.00010547
   30.814    34.392   0.00032409
   34.392    38.646   0.00033713
   38.646    42.839   0.00039674
   42.839    47.773   0.00041147
   47.773    53.637   0.00039202
   53.637    60.689   0.00029832
   60.689    67.422   0.00033940
   67.422    75.390   0.00030929
   75.390    84.928   0.00025476
   84.928    96.499   0.00014665
   96.499    106.90   0.00014520
   106.90    119.18   0.00010197
   119.18    133.88   6.6234e-05
   133.88    151.70   4.1891e-05
   151.70    173.68   2.5569e-05
   173.68    201.37   1.1465e-05
   201.37    224.13   1.0772e-05
   224.13    251.49   4.3021e-06
   251.49    284.97   2.2326e-06
   284.97    326.79   7.3030e-07
   326.79    380.42   1.4982e-07
 \END;
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