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 /* NRDF D1809 Data No.14                                             */
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 /* Bibliography                                                      */
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 \\BIB,14;
 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,14;
 /* 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,14;
 INC-ENGY-LAB=100MEV/A;
 SYS-ERR=(<3%'96',<1%'97',<1%'98');
 /* '96' Uncertainty in the number of accepted beam particles
         incident on the target is estimated to be less than 3%. */
 /* '97' Uncertainty in the solid angle for the thickest carbon
         target, which has the maximum uncertainty, is less than 1%. */
 /* '98' 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%'99';
 /* '99' 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=7.5DEG;
 DELTA-DN/DOMEGA/DE=<4%'100';
 /* '100' 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'101'
 (MEV) (MEV) (1/SR/MEV/PARTCL)
   22.968    25.432   2.5209e-05
   25.432    28.320   0.00014722
   28.320    31.370   0.00059726
   31.370    34.950   0.00069086
   34.950    38.685   0.00086177
   38.685    43.067   0.00089102
   43.067    48.259   0.00082429
   48.259    53.637   0.00096695
   53.637    59.998   0.00082151
   59.998    66.430   0.00086985
   66.430    73.999   0.00077914
   73.999    83.001   0.00053635
   83.001    91.885   0.00049794
   91.885    102.36   0.00034880
   102.36    114.85   0.00024512
   114.85    129.94   0.00011831
   129.94    144.44   8.9557e-05
   144.44    161.72   5.7804e-05
   161.72    182.63   2.6557e-05
   182.63    208.33   8.2350e-06
   208.33    231.79   4.4911e-06
   231.79    260.01   1.6004e-06
   260.01    294.53   3.8156e-07
 \END;
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