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 /* NRDF D1809 Data No.1                                              */
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 /* Bibliography                                                      */
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 \\BIB,1;
 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,1;
 /* 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=12C(ALPHA,P)X;
 THK-TGT=8850MG/CM**2;
 DET-PARTCL=P;
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 /* Descriptive Parameters                                            */
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 \\DATA,1;
 INC-ENGY-LAB=100MEV/A;
 SYS-ERR=(<3%'14',<1%'15',<1%'16');
 /* '14' Uncertainty in the number of accepted beam particles
         incident on the target is estimated to be less than 3%. */
 /* '15' Uncertainty in the solid angle for the thickest carbon
         target, which has the maximum uncertainty, is less than 1%. */
 /* '16' 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%'17';
 /* '17' 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%'18';
 /* '18' 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'19'
 (MEV) (MEV) (1/SR/MEV/PARTCL)
   28.636    31.739   0.00098559
   31.739    35.386   0.0021321
   35.386    39.194   0.0028856
   39.194    43.668   0.0031680
   43.668    48.975   0.0029538
   48.975    54.480   0.0033945
   54.480    61.001   0.0030331
   61.001    67.605   0.0035588
   67.605    75.390   0.0033417
   75.390    84.667   0.0025631
   84.667    93.841   0.0025051
   93.841    104.68   0.0018373
   104.68    117.64   0.00094644
   117.64    133.34   0.00049025
   133.34    148.47   0.00038412
   148.47    166.57   0.00027273
   166.57    188.54   0.00013048
   188.54    215.70   4.1913e-05
   215.70    240.61   2.1961e-05
   240.61    270.72   8.2100e-06
   270.72    307.81   2.0550e-06
   307.81    354.53   1.4500e-07
 \END;
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