DARPE: Search Results
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 /* NRDF D1810 Data No.67                                             */
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 /* Bibliography                                                      */
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 \\BIB,67;
       97, 103, 109, 115, 121[128;
 D#=D1810;
 TITLE=/ Measurements of secondary neutrons produced from thick
         targets bombarded by high-energy helium and carbon ions /;
 PURPOSE=/ To present the angular and energy distributions of
           neutrons produced from thick C, Al, Cu, and Pb targets
           bombarded by 100 and 180 MeV/nucleon He and 100, 180, and
           400 MeV/nucleon C ions. /;
 ATH=(T.KUROSAWA'1', N.NAKAO'2', T.NAKAMURA'1', Y.UWAMINO'3',
      T.SHIBATA'2', N.NAKANISHI'3', A.FUKUMURA'4', K.MURAKAMI'4');
 INST-ATH=(2JPNTOH'1', 2JPNKEK'2', 2JPNIPC'3', 2JPNIRS'4');
      /* '1' Cyclotron and Radioisotope Center */
      /* '2' Tanashi branch */
 REF=NSE;
 VLP=132(1999)30;
 RCTS=(C(ALPHA,N)X, 27AL(ALPHA,N)X, CU(ALPHA,N)X, PB(ALPHA,N)X,
       C(12C,N)X, 27AL(12C,N)X, CU(12C,N)X, PB(12C,N)X);
 PHQS=(ENGY-SPEC'5', N-MLT'6');
 /* '5' Neutron energy spectrum */
 /* '6' Neutron Yield above 5 MeV integrated for a hemisphere from 0
    deg to 90 deg. */
 /*===================================================================*/
 /* Experimental Conditions                                           */
 /*===================================================================*/
 \\EXP,67;
       97, 103, 109, 115, 121[128;
 /* 2004-01-27 : Compiled+Checked, Sr + On */
 /* 2009-08-23 : Altered, Nf. 122-129 corrected */
 ENR=NAT;
 CHM=ELM;
 PHYS-FORM=SLD;
 BAC=X;
 POL-TGT=0%;
 ALGN-TGT=0%;
 ACC=SYN'7';
 /* '7' HIMAC heavy-ion synchrotron */
 INST-ACC=2JPNIRS;
 BEAM-INTNSTY=XMA'8';
 /* '8' 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'9',SCT'10',TOF'11',EDE'12');
 /* '9' Plastic scintillator (NE102A) was used as the delta-E
        counter and the beam pick-up counter (the output pulses of this
        scintillator were used as start signals for the TOF and to
        count the absolute number of projectile incident). */
 /* '10' Liquid scintillator (NE213) was used as the E counter. */
 /* '11' To measure the energy of neutron */
 /* '12' To eliminate charged particles */
 ERS-DET=XKEV'13';
 /* '13' Energy resolutions are represented as a function of
         neutron energy in Fig. 4 in the reference. */
 CALB-DET=/ After the experimental run, 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. [Ref: R. A. Cecil et al.,
            Nucl. Instrum. Methods 161, 439 (1979).] /;
 ANL=(INCASC'14',X'15');
 /* '14' HIC calculation [H. W. Bertini, et al. ORNL-TM-4134, Oak
         Ridge National Laboratory (1974)] */
 /* '15' Phenomenological hybrid analysis by the moving source
         model [G. Mantzouranis et al., Z. Phys. A276(1976)145] */
 /* 2007-10-24 : Altered, On. Extended for angular range */
 /* 2007-10-25 : Altered, On. Superseded by data with new analysis
 /* Related references 
    - R.A.Cecil et al., PR/C, 21(1980)2471.
    Reference with which data agree (Data in this reference agree with
    present results in the lower-energy region below about 100 MeV.)
 RCT=PB(ALPHA,N)X;
 PHQ=ENGY-SPEC'42';
 /* '42' Neutron energy spectrum */
 THK-TGT=56700MG/CM**2;
 INC-ENGY-LAB-RANGE=180MEV/A;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,67;
        97, 103, 109, 115, 121[128;
 SYS-ERR=(<3%'16',<10%'17',[8%'18');
 /* '16' Uncertainty in the number of accepted beam particles
         incident to target (less than 3%.) */
 /* '17' Uncertainty in solid angle (less than 10%) */
 /* '18' Uncertainty in calculated detection efficiencies (about
         9%) */
 STATIST-ERR=X%'19';
 /* '19' The statistical uncertainties vary from 2 to 5% for the
         low- to medium-energy (5- to 50-MeV) region of the spectra and
         increase to about 30% at the highest energies. */
 INC-ENGY-LAB=180MEV/A;
 DELTA-DN/DOMEGA/DE=14%'43';
 /* '43' Total normalization uncertainty */
 /*===================================================================*/
 /* Data Table                                                        */
 /*===================================================================*/
 \DATA;
 THTL ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE
 (DEG) (MEV) (MEV) (1/SR/MEV/PARTCL)
 0 17.024 18.820 0.0029884
 0 18.820 20.811 0.0032852
 0 20.811 23.011 0.0028940
 0 23.011 25.435 0.0033109
 0 25.435 28.155 0.0029995
 0 28.155 31.142 0.0027045
 0 31.142 34.482 0.0031431
 0 34.482 38.125 0.0031506
 0 38.125 42.179 0.0029906
 0 42.179 46.681 0.0028993
 0 46.681 51.674 0.0026047
 0 51.674 57.197 0.0028990
 0 57.197 63.287 0.0028497
 0 63.287 69.974 0.0027476
 0 69.974 77.553 0.0031942
 0 77.553 85.849 0.0033607
 0 85.849 95.246 0.0034594
 0 95.246 105.47 0.0038156
 0 105.47 117.03 0.0037593
 0 117.03 129.49 0.0033400
 0 129.49 143.49 0.0036179
 0 143.49 159.24 0.0033066
 0 159.24 176.96 0.0027791
 0 176.96 195.72 0.0021696
 0 195.72 216.55 0.0015589
 0 216.55 239.64 0.00070185
 0 239.64 265.17 0.00036818
 0 265.17 293.27 0.00023175
 0 293.27 326.84 0.00010324
 0 326.84 364.19 3.2258e-05
 7.5 11.233 12.432 0.0037396
 7.5 12.432 13.762 0.0035668
 7.5 13.762 15.234 0.0034727
 7.5 15.234 16.858 0.0032625
 7.5 16.858 18.643 0.0031853
 7.5 18.643 20.641 0.0035740
 7.5 20.641 22.824 0.0035072
 7.5 22.824 25.256 0.0030741
 7.5 25.256 27.962 0.0034044
 7.5 27.962 30.967 0.0028534
 7.5 30.967 34.299 0.0032013
 7.5 34.299 37.982 0.0029352
 7.5 37.982 42.039 0.0025828
 7.5 42.039 46.489 0.0027969
 7.5 46.489 51.524 0.0025130
 7.5 51.524 57.023 0.0028288
 7.5 57.023 63.235 0.0028089
 7.5 63.235 69.975 0.0027910
 7.5 69.975 77.557 0.0029095
 7.5 77.557 86.098 0.0029571
 7.5 86.098 95.258 0.0027987
 7.5 95.258 105.49 0.0029376
 7.5 105.49 116.93 0.0026896
 7.5 116.93 129.68 0.0026390
 7.5 129.68 143.91 0.0022150
 7.5 143.91 159.73 0.0020759
 7.5 159.73 177.30 0.0015636
 7.5 177.30 196.73 0.0011397
 7.5 196.73 218.11 0.00051715
 7.5 218.11 241.50 0.00032893
 7.5 241.50 269.40 0.00020493
 7.5 269.40 300.14 5.3542e-05
 7.5 300.14 333.67 4.8535e-05
 7.5 333.67 369.80 1.2738e-05
 7.5 369.80 413.38 1.1250e-05
 15 5.7130 6.3204 0.012567
 15 6.3204 6.9950 0.0091779
 15 6.9950 7.7428 0.0081739
 15 7.7428 8.5701 0.0063282
 15 8.5701 9.4821 0.0056166
 15 9.4821 10.484 0.0046002
 15 10.484 11.603 0.0039012
 15 11.603 12.826 0.0034846
 15 12.826 14.184 0.0029723
 15 14.184 15.694 0.0030726
 15 15.694 17.367 0.0028028
 15 17.367 19.218 0.0029975
 15 19.218 21.258 0.0031870
 15 21.258 23.498 0.0030698
 15 23.498 26.032 0.0026304
 15 26.032 28.806 0.0025442
 15 28.806 31.938 0.0025843
 15 31.938 35.347 0.0026472
 15 35.347 39.184 0.0023132
 15 39.184 43.324 0.0022612
 15 43.324 47.955 0.0021153
 15 47.955 53.138 0.0022725
 15 53.138 58.938 0.0018738
 15 58.938 65.424 0.0020483
 15 65.424 72.673 0.0019265
 15 72.673 80.764 0.0018556
 15 80.764 89.775 0.0015738
 15 89.775 99.787 0.0015304
 15 99.787 110.87 0.0013171
 15 110.87 123.09 0.0012542
 15 123.09 136.47 0.00095222
 15 136.47 151.02 0.00078672
 15 151.02 168.25 0.00051561
 15 168.25 187.03 0.00031444
 15 187.03 207.28 0.00029037
 15 207.28 231.42 0.00014671
 15 231.42 257.44 7.1710e-05
 15 257.44 284.99 4.5545e-05
 15 284.99 317.96 1.7194e-05
 30 7.0840 7.8396 0.0085111
 30 7.8396 8.6750 0.0069438
 30 8.6750 9.5956 0.0059143
 30 9.5956 10.606 0.0050604
 30 10.606 11.736 0.0040192
 30 11.736 12.997 0.0037149
 30 12.997 14.372 0.0035079
 30 14.372 15.898 0.0031397
 30 15.898 17.589 0.0029403
 30 17.589 19.458 0.0031599
 30 19.458 21.519 0.0031297
 30 21.519 23.855 0.0027522
 30 23.855 26.424 0.0025840
 30 26.424 29.236 0.0024846
 30 29.236 32.412 0.0023541
 30 32.412 35.868 0.0021230
 30 35.868 39.758 0.0019919
 30 39.758 43.954 0.0016961
 30 43.954 48.647 0.0014892
 30 48.647 53.899 0.0014327
 30 53.899 59.776 0.0013626
 30 59.776 66.347 0.0011652
 30 66.347 73.690 0.0010626
 30 73.690 81.885 0.00084524
 30 81.885 91.013 0.00080562
 30 91.013 101.15 0.00068027
 30 101.15 112.38 0.00050714
 30 112.38 124.75 0.00039059
 30 124.75 138.30 0.00028368
 30 138.30 153.04 0.00019868
 30 153.04 170.48 0.00014309
 30 170.48 189.51 0.00010015
 30 189.51 210.02 6.0791e-05
 30 210.02 234.48 4.0966e-05
 30 234.48 260.84 1.7558e-05
 30 260.84 288.77 1.3913e-05
 60 3.3106 3.6606 0.0047891
 60 3.6606 4.0464 0.0062033
 60 4.0464 4.4792 0.0094183
 60 4.4792 4.9547 0.010830
 60 4.9547 5.4863 0.0098544
 60 5.4863 6.0666 0.0093356
 60 6.0666 6.7121 0.0079062
 60 6.7121 7.4288 0.0059859
 60 7.4288 8.2232 0.0048551
 60 8.2232 9.1016 0.0040701
 60 9.1016 10.069 0.0033083
 60 10.069 11.131 0.0029471
 60 11.131 12.331 0.0023219
 60 12.331 13.643 0.0021445
 60 13.643 15.123 0.0018617
 60 15.123 16.729 0.0016375
 60 16.729 18.534 0.0014993
 60 18.534 20.563 0.0014469
 60 20.563 22.744 0.0014515
 60 22.744 25.175 0.0012176
 60 25.175 27.885 0.0011312
 60 27.885 30.900 0.0010259
 60 30.900 34.252 0.00085912
 60 34.252 37.968 0.00073758
 60 37.968 42.075 0.00068558
 60 42.075 46.598 0.00058537
 60 46.598 51.554 0.00054219
 60 51.554 57.371 0.00040600
 60 57.371 63.770 0.00034042
 60 63.770 70.760 0.00031820
 60 70.760 78.329 0.00027596
 60 78.329 87.243 0.00019478
 60 87.243 96.895 0.00014087
 60 96.895 107.21 0.00011339
 60 107.21 119.38 7.7000e-05
 60 119.38 132.33 5.3331e-05
 60 132.33 147.68 2.8598e-05
 60 147.68 163.88 2.0239e-05
 90 3.2311 3.5726 0.011851
 90 3.5726 3.9493 0.016338
 90 3.9493 4.3716 0.012364
 90 4.3716 4.8355 0.011940
 90 4.8355 5.3542 0.0099642
 90 5.3542 5.9204 0.0084435
 90 5.9204 6.5502 0.0074921
 90 6.5502 7.2495 0.0055135
 90 7.2495 8.0246 0.0045156
 90 8.0246 8.8812 0.0034548
 90 8.8812 9.8251 0.0027010
 90 9.8251 10.861 0.0022758
 90 10.861 12.031 0.0018908
 90 12.031 13.311 0.0015734
 90 13.311 14.753 0.0012797
 90 14.753 16.320 0.0010924
 90 16.320 18.079 0.0010392
 90 18.079 20.057 0.00094352
 90 20.057 22.181 0.00078708
 90 22.181 24.550 0.00070237
 90 24.550 27.190 0.00059880
 90 27.190 30.127 0.00049445
 90 30.127 33.390 0.00043862
 90 33.390 37.007 0.00037306
 90 37.007 41.004 0.00031454
 90 41.004 45.404 0.00024697
 90 45.404 50.223 0.00018859
 90 50.223 55.878 0.00013077
 90 55.878 62.094 0.00010746
 90 62.094 68.881 6.8943e-05
 90 68.881 76.227 6.4792e-05
 90 76.227 84.870 4.1245e-05
 90 84.870 94.223 2.9066e-05
 90 94.223 104.21 1.7787e-05
 90 104.21 115.99 1.1513e-05
 \END;
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