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 /*===================================================================*/
 /* NRDF D1756 Data No.10                                             */
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 /* Bibliography                                                      */
 /*===================================================================*/
 \\BIB,10;
 D#=D1756;
 TITLE=/ Neutron yields from thick C, Al, Cu, and Pb targets
         bombarded by 400 MeV/nucleon Ar, Fe, Xe and 800 MeV/nucleon Si
         ions /;
 PURPOSE=/ To perform a systematic study to measure the double
           differential neutron yields from thick targets of C, Al, Cu,
           and Pb bombarded by various heavy ions having energies of
           100 to 800 MeV/nucleon using HIMAC. /;
 ATH=(T.KUROSAWA'1', T.NAKAO'2', T.NAKAMURA'1', H.IWASE'1', H.SATO'1',
      Y.UWAMINO'3', A.FUKUMURA'4');
 INST-ATH=(2JPNTOH'1', 2JPNKEK'2', 2JPNIPC'3', 2JPNIRS'4');
      /* '1' Cyclotron and Radioisotope Center */
 REF=PR/C;
 VLP=62(2000)044615;
 RCTS=(C(40AR,N)X, 27AL(40AR,N)X, CU(40AR,N)X, PB(40AR,N)X,
       C(56FE,N)X, 27AL(56FE,N)X, CU(56FE,N)X, PB(56FE,N)X,
       C(132XE,N)X, 27AL(132XE,N)X, CU(132XE,N)X, PB(132XE,N)X,
       C(28SI,N)X, CU(28SI,N)X);
 PHQS=(ENGY-SPEC'5', ANGL-DSTRN'6', N-MLT'7');
 /* '5' Neutron energy spectrum */
 /* '6' Neutron yield */
 /* '7' Thick target differential multiplicity of neutron with
    respect to angle integrated over partial angular range */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,10;
 /* 2002-02-28 : Compiled+Checked, R.Suzuki + sK */
 /* 2004-04-23 : Altered, N.Otuka. MLT in SF6 replaced by PY */
 /* 2008-01-30 : Altered, N.Otuka. EDE addded under METHOD */
 RTY=HEAVY-ION-RCT;
 ENR=NAT'8';
 /* '8' (The enrichments of targets are not given in the reference.
        But compiler asked T.Kurosawa.) */
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN'9';
 /* '9' Heavy Ion Medical Accelerator in Chiba (HIMAC) */
 INST-ACC=2JPNIRS'10';
 /* '10' The mass numbers of projectile nuclei are not given in
        the reference. But compiler asked NIRS staff. */
 BEAM-INTNSTY=XMA'11';
 /* '11' The beam intensities were maintained at 100,000-1,000,000
         particles per pulse. */
 POL-PRJ=0%;
 DET-PARTCL=N;
 COINC=NO;
 ANT-COINC=NO;
 DET-SYS=(SCT'12',SCT'13',TOF'14',EDE'15');
 /* '12' Plastic scintillator (NE102A) was used as the delta-E
         counter and the beam pick-up counter. */
 /* '13' Liquid scintillator (NE213) was used as the E counter. */
 /* '14' To measure the energy of neutron */
 /* '15' To eliminate charged particles */
 ERS-DET=XKEV'16';
 /* '16' The energy resolutions of measured neutron spectra are at
         maximum about 20% for about 2000 MeV neutrons of highest
         energy at 0 degree and 7.5 degree, about 20% for about 1000
         MeV neutrons of highest energy at 15 degree and 30 degree, and
         about 40% for about 600 MeV neutrons of highest energy at 60
         degree and 90 degree, which were produced by 800 MeV/nucleon
         Si ions. */
 CALB-DET=/ Each E counter was calibrated with a 60Co Gamma-ray source.
 EFCN-DET=/ The neutron detection efficiencies were calculated with the
            Monte Carlo code of Cecil et al. for all energy ranges.
            Reference is R. A. Cecil, B. D. Anderson, and R. Madey,
            Nucl. Instrum. Methods 161, 439 (1979). /;
 /* 2007-10-25 : Altered, N.Otuka. Superseded by data with new
    analysis */
 RCT=27AL(132XE,N)X;
 PHQ=ENGY-SPEC'45';
 /* '45' Neutron energy spectrum */
 THK-TGT=5400MG/CM**2;
 INC-ENGY-LAB-RANGE=400MEV/A;
 ANL=(INCASC'46',X'47');
 /* '46' HIC calculation [H.W.Bertini, et al. Oak Ridge National
         Laboratory Report No. ORNL-TM-4134, 1974 (unpublished).] */
 /* '47' Phenomenological hybrid analysis by the moving source
         model. */
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,10;
 STATIST-ERR=X%'17';
 /* '17' The statistical uncertainties vary in a range of 2 to 5 %
         for the low- to medium-energy (5-400 MeV) region of the
         spectra and increase to about 30% at the highest energies. */
 NORM=/ The total normalization uncertainty is 15%. /;
 INC-ENGY-LAB=400MEV/A;
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTL ENGY-EMT-LAB DN/DOMEGA/DE
 (DEG) (MEV) (1/SR/MEV/PARTCL)
 0 10.218 0.019811
 0 11.309 0.022612
 0 12.5185 0.017247
 0 13.856 0.019274
 0 15.33 0.026078
 0 16.977 0.026114
 0 18.8115 0.027609
 0 20.8185 0.028058
 0 23.045 0.027438
 0 25.5015 0.033251
 0 28.2115 0.030041
 0 31.2505 0.042362
 0 34.66 0.041143
 0 38.388 0.053475
 0 42.4515 0.066774
 0 46.9625 0.071258
 0 51.961 0.091613
 0 57.485 0.10990
 0 63.57 0.11238
 0 70.498 0.099663
 0 78.3755 0.10098
 0 87.062 0.13073
 0 96.586 0.15967
 0 106.95 0.19501
 0 118.7 0.20864
 0 131.96 0.22739
 0 146.255 0.26694
 0 162.415 0.29813
 0 180.54 0.38475
 0 201.07 0.42634
 0 224.115 0.54202
 0 250.265 0.52141
 0 279.6 0.65488
 0 312.89 0.53056
 0 350.1 0.45421
 0 392.205 0.21549
 0 438.86 0.091512
 0 491.19 0.023211
 0 548.145 0.011243
 0 610.685 0.0029550
 0 688.1 0.0010523
 0 771.345 0.00046696
 0 861.43 0.00018828
 7.5 8.4726 0.011382
 7.5 9.36855 0.011609
 7.5 10.3695 0.011647
 7.5 11.4845 0.013839
 7.5 12.705 0.014254
 7.5 14.06 0.014873
 7.5 15.5565 0.014582
 7.5 17.2085 0.016402
 7.5 19.0625 0.019887
 7.5 21.145 0.016438
 7.5 23.4265 0.020859
 7.5 25.919 0.019447
 7.5 28.692 0.026207
 7.5 31.772 0.021434
 7.5 35.185 0.026433
 7.5 38.957 0.024921
 7.5 43.1115 0.028502
 7.5 47.8385 0.031289
 7.5 53.208 0.034759
 7.5 59.1205 0.036511
 7.5 65.59 0.038234
 7.5 72.6135 0.048335
 7.5 80.5505 0.049334
 7.5 89.4725 0.058258
 7.5 99.588 0.062811
 7.5 110.985 0.067525
 7.5 123.18 0.081308
 7.5 136.895 0.075872
 7.5 152.165 0.094950
 7.5 169.305 0.093241
 7.5 188.3 0.12124
 7.5 209.535 0.11378
 7.5 232.87 0.12681
 7.5 258.72 0.13091
 7.5 289.805 0.10152
 7.5 324.01 0.11458
 7.5 361.995 0.071247
 7.5 408.505 0.030814
 7.5 459.59 0.019153
 7.5 516.28 0.0072973
 7.5 587.24 0.0028833
 7.5 664.41 0.0015691
 15 4.51345 0.019287
 15 4.997 0.024707
 15 5.5307 0.023602
 15 6.1176 0.018366
 15 6.77155 0.020291
 15 7.49755 0.020885
 15 8.3041 0.018748
 15 9.1956 0.016786
 15 10.1808 0.013718
 15 11.287 0.017368
 15 12.5005 0.018452
 15 13.829 0.013950
 15 15.308 0.020569
 15 16.9525 0.017840
 15 18.7785 0.023358
 15 20.801 0.013710
 15 23.0345 0.018821
 15 25.492 0.025807
 15 28.2835 0.021667
 15 31.4485 0.023767
 15 34.9255 0.025594
 15 38.7185 0.022828
 15 43.0155 0.022670
 15 47.861 0.021383
 15 53.1005 0.025768
 15 59.0115 0.026120
 15 65.632 0.023460
 15 73.1055 0.026148
 15 81.469 0.027702
 15 90.905 0.026152
 15 101.438 0.032723
 15 113.29 0.026105
 15 126.44 0.029829
 15 141.155 0.027253
 15 157.335 0.031122
 15 175.24 0.029336
 15 196.72 0.029223
 15 220.275 0.028385
 15 246.295 0.027188
 15 277.925 0.025472
 15 312.345 0.027715
 15 350.04 0.023433
 15 396.43 0.013474
 15 445.905 0.016614
 15 498.755 0.014305
 15 564.24 0.012433
 15 647.695 0.0060535
 15 734.685 0.0071384
 30 3.43305 0.012861
 30 3.79805 0.015754
 30 4.20315 0.013437
 30 4.6519 0.013078
 30 5.1477 0.011765
 30 5.69355 0.012642
 30 6.30255 0.010635
 30 6.9799 0.010552
 30 7.73385 0.0087349
 30 8.56935 0.0089660
 30 9.49525 0.0082070
 30 10.5152 0.0072812
 30 11.637 0.0077243
 30 12.8915 0.0076164
 30 14.295 0.0069748
 30 15.8635 0.0060519
 30 17.6145 0.0074367
 30 19.5665 0.0072090
 30 21.738 0.0068990
 30 24.1475 0.0069909
 30 26.8115 0.0066748
 30 29.7435 0.0065954
 30 32.952 0.0072178
 30 36.5905 0.0066771
 30 40.7015 0.0060676
 30 45.1735 0.0065387
 30 50.2365 0.0061937
 30 55.9355 0.0059568
 30 62.0585 0.0063176
 30 68.941 0.0058154
 30 76.608 0.0066031
 30 85.2135 0.0058637
 30 94.766 0.0062951
 30 105.45 0.0053833
 30 117.23 0.0060225
 30 130.31 0.0059934
 30 145.895 0.0051550
 30 163.11 0.0061176
 30 182.27 0.0048220
 30 203.11 0.0053803
 30 225.9 0.0051688
 30 253.285 0.0035918
 30 282.73 0.0034578
 30 314.5 0.0031332
 30 352.95 0.0023569
 30 400.405 0.0012396
 30 451.17 0.0011847
 30 505.61 0.00072619
 30 573.36 0.00038949
 30 660.195 0.00012724
 30 751.24 7.8146e-05
 30 846.045 3.9489e-05
 60 3.38705 0.010623
 60 3.74945 0.015013
 60 4.14955 0.012949
 60 4.591 0.012375
 60 5.086 0.011446
 60 5.64135 0.0094563
 60 6.2489 0.0092859
 60 6.91155 0.0079744
 60 7.64705 0.0081291
 60 8.4618 0.0059234
 60 9.36195 0.0065069
 60 10.353 0.0053732
 60 11.4785 0.0055079
 60 12.754 0.0048809
 60 14.1575 0.0044345
 60 15.693 0.0051433
 60 17.433 0.0047902
 60 19.397 0.0047626
 60 21.5305 0.0044238
 60 23.941 0.0040527
 60 26.647 0.0035986
 60 29.5455 0.0037646
 60 32.7915 0.0033955
 60 36.391 0.0034710
 60 40.408 0.0028221
 60 44.839 0.0031661
 60 49.7545 0.0029299
 60 55.5515 0.0022176
 60 61.952 0.0025381
 60 69.062 0.0020775
 60 76.814 0.0021918
 60 85.304 0.0019950
 60 95.3625 0.0016797
 60 106.235 0.0016339
 60 118.02 0.0015582
 60 132.03 0.0012780
 60 148.91 0.00099370
 60 167.08 0.00095228
 60 186.68 0.00091935
 60 210.355 0.00066804
 60 239.45 0.00044017
 60 270.37 0.00043188
 60 303.19 0.00033646
 60 343.485 0.00023367
 60 394.095 0.00013039
 60 445.96 0.00013342
 60 498.25 0.00012086
 60 562.895 5.2981e-05
 90 3.4441 0.0054356
 90 3.8127 0.0049027
 90 4.2204 0.0067962
 90 4.6786 0.0063632
 90 5.1822 0.0059428
 90 5.73465 0.0053908
 90 6.35105 0.0051649
 90 7.03815 0.0039097
 90 7.803 0.0039067
 90 8.65295 0.0032385
 90 9.59505 0.0029108
 90 10.6365 0.0024316
 90 11.7825 0.0020810
 90 13.0375 0.0020751
 90 14.459 0.0019428
 90 16.063 0.0017199
 90 17.811 0.0020585
 90 19.7885 0.0018964
 90 22.014 0.0016932
 90 24.4145 0.0015653
 90 27.114 0.0012154
 90 30.126 0.0014045
 90 33.51 0.0010341
 90 37.276 0.0010475
 90 41.495 0.00080550
 90 46.1665 0.00086677
 90 51.372 0.00066683
 90 57.088 0.00058038
 90 63.3975 0.00047121
 90 70.8585 0.00035935
 90 79.027 0.00035462
 90 88.015 0.00026258
 90 98.718 0.00014707
 90 110.345 0.00012397
 90 123.03 0.00010234
 90 138.21 7.0033e-05
 90 154.435 5.6583e-05
 90 171.8 3.0598e-05
 90 192.585 2.3390e-05
 90 217.845 2.1724e-05
 90 244.39 1.1399e-05
 \END;
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