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 /* NRDF D1809 Data No.51                                             */
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 /* Bibliography                                                      */
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 \\BIB,51;
 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,51;
 /* 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=27AL(ALPHA,T)X;
 THK-TGT=10800MG/CM**2;
 DET-PARTCL=T;
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 /* Descriptive Parameters                                            */
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 \\DATA,51;
 INC-ENGY-LAB=100MEV/A;
 SYS-ERR=(<3%'320',<1%'321',<1%'322');
 /* '320' Uncertainty in the number of accepted beam particles
          incident on the target is estimated to be less than 3%. */
 /* '321' Uncertainty in the solid angle for the thickest carbon
          target, which has the maximum uncertainty, is less than 1%.
 /* '322' 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%'323';
 /* '323' 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=T;
 THTL=15DEG;
 DELTA-DN/DOMEGA/DE=<4%'324';
 /* '324' Total normalization uncertainty */
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 /* Data Table                                                        */
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 \DATA;
 ENGY-EMT-LAB-MIN'325' ENGY-EMT-LAB-MAX DN/DOMEGA/DE'326'
 (MEV) (MEV) (1/SR/MEV/PARTCL)
   X         41.405   1.0880e-05
   41.405    46.160   3.2860e-05
   46.160    51.116   0.00011443
   51.116    56.925   0.00021578
   56.925    63.794   0.00019999
   63.794    70.894   0.00023546
   70.894    79.266   0.00020077
   79.266    87.702   0.00023787
   87.702    97.585   0.00024526
   97.585    109.27   0.00023708
   109.27    123.25   0.00019385
   123.25    137.10   0.00021302
   137.10    153.49   0.00018285
   153.49    173.12   0.00011696
   173.12    191.76   0.00011483
   191.76    213.70   8.3208e-05
   213.70    239.81   5.3701e-05
   239.81    271.27   4.3593e-05
   271.27    309.72   1.7832e-05
   309.72    344.55   2.5741e-06
 \END;
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