DARPE: Search Results
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 /* NRDF D1810 Data No.49                                             */
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 /* Bibliography                                                      */
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 \\BIB,49;
       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,49;
       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 disagree (Data in this reference disagree
    with present results in the lower-energy region below about 100
    MeV.)
 RCT=C(ALPHA,N)X;
 PHQ=ENGY-SPEC'36';
 /* '36' Neutron energy spectrum */
 THK-TGT=28320MG/CM**2;
 INC-ENGY-LAB-RANGE=180MEV/A;
 /*===================================================================*/
 /* Descriptive Parameters                                            */
 /*===================================================================*/
 \\DATA,49;
        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%'37';
 /* '37' 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 0.0031086
 0 18.820 20.811 0.0031683
 0 20.811 23.011 0.0039451
 0 23.011 25.435 0.0041428
 0 25.435 28.155 0.0041450
 0 28.155 31.142 0.0041941
 0 31.142 34.482 0.0043913
 0 34.482 38.125 0.0049974
 0 38.125 42.179 0.0050944
 0 42.179 46.681 0.0052153
 0 46.681 51.674 0.0058324
 0 51.674 57.197 0.0062259
 0 57.197 63.287 0.0070265
 0 63.287 69.974 0.0072046
 0 69.974 77.553 0.0082539
 0 77.553 85.849 0.0085963
 0 85.849 95.246 0.010285
 0 95.246 105.47 0.010897
 0 105.47 117.03 0.011149
 0 117.03 129.49 0.011085
 0 129.49 143.49 0.010785
 0 143.49 159.24 0.010644
 0 159.24 176.96 0.0077182
 0 176.96 195.72 0.0066243
 0 195.72 216.55 0.0037731
 0 216.55 239.64 0.0021296
 0 239.64 265.17 0.0011100
 0 265.17 293.27 0.00050663
 0 293.27 326.84 0.00018375
 0 326.84 364.19 3.3123e-05
 0 364.19 405.51 2.5557e-05
 7.5 11.543 12.773 0.0027583
 7.5 12.773 14.134 0.0028532
 7.5 14.134 15.639 0.0026901
 7.5 15.639 17.296 0.0031017
 7.5 17.296 19.154 0.0030345
 7.5 19.154 21.191 0.0030752
 7.5 21.191 23.466 0.0033807
 7.5 23.466 25.942 0.0031996
 7.5 25.942 28.689 0.0034696
 7.5 28.689 31.731 0.0037160
 7.5 31.731 35.091 0.0041176
 7.5 35.091 38.791 0.0047203
 7.5 38.791 42.985 0.0046256
 7.5 42.985 47.594 0.0046189
 7.5 47.594 52.631 0.0048087
 7.5 52.631 58.320 0.0048264
 7.5 58.320 64.500 0.0054427
 7.5 64.500 71.456 0.0061478
 7.5 71.456 79.298 0.0056116
 7.5 79.298 87.734 0.0062081
 7.5 87.734 97.177 0.0062811
 7.5 97.177 107.75 0.0065779
 7.5 107.75 119.58 0.0060921
 7.5 119.58 132.82 0.0057158
 7.5 132.82 147.62 0.0052369
 7.5 147.62 164.13 0.0044310
 7.5 164.13 182.52 0.0030349
 7.5 182.52 202.92 0.0022240
 7.5 202.92 225.47 0.0012658
 7.5 225.47 250.24 0.00072809
 7.5 250.24 277.24 0.00041203
 7.5 277.24 309.57 0.00012746
 7.5 309.57 345.01 5.6418e-05
 7.5 345.01 383.40 2.0901e-05
 7.5 383.40 424.31 1.2507e-05
 15 5.7217 6.3305 0.0032424
 15 6.3305 7.0068 0.0029140
 15 7.0068 7.7566 0.0023113
 15 7.7566 8.5860 0.0025012
 15 8.5860 9.5008 0.0023568
 15 9.5008 10.505 0.0024807
 15 10.505 11.629 0.0018535
 15 11.629 12.855 0.0020012
 15 12.855 14.219 0.0021897
 15 14.219 15.734 0.0021505
 15 15.734 17.414 0.0024793
 15 17.414 19.272 0.0022724
 15 19.272 21.321 0.0027771
 15 21.321 23.572 0.0028487
 15 23.572 26.118 0.0026604
 15 26.118 28.906 0.0030058
 15 28.906 32.055 0.0026575
 15 32.055 35.484 0.0032583
 15 35.484 39.345 0.0027465
 15 39.345 43.511 0.0029641
 15 43.511 48.174 0.0030060
 15 48.174 53.394 0.0032546
 15 53.394 59.238 0.0033274
 15 59.238 65.777 0.0031813
 15 65.777 73.089 0.0031925
 15 73.089 81.254 0.0031075
 15 81.254 90.354 0.0029348
 15 90.354 100.47 0.0029876
 15 100.47 111.68 0.0028086
 15 111.68 124.04 0.0024461
 15 124.04 137.60 0.0019530
 15 137.60 152.35 0.0018761
 15 152.35 169.82 0.0014171
 15 169.82 188.90 0.00098633
 15 188.90 209.50 0.00083356
 15 209.50 234.09 0.00050776
 15 234.09 260.64 0.00028849
 15 260.64 288.79 0.00018192
 15 288.79 322.54 9.1485e-05
 15 322.54 358.06 4.2479e-05
 15 358.06 400.99 2.8439e-05
 30 6.4331 7.1198 0.0032188
 30 7.1198 7.8812 0.0025401
 30 7.8812 8.7235 0.0024268
 30 8.7235 9.6521 0.0023838
 30 9.6521 10.672 0.0022269
 30 10.672 11.812 0.0021446
 30 11.812 13.057 0.0022912
 30 13.057 14.441 0.0022001
 30 14.441 15.978 0.0022841
 30 15.978 17.683 0.0022148
 30 17.683 19.568 0.0024481
 30 19.568 21.646 0.0025877
 30 21.646 23.929 0.0024837
 30 23.929 26.511 0.0024708
 30 26.511 29.338 0.0024491
 30 29.338 32.531 0.0023389
 30 32.531 36.007 0.0023277
 30 36.007 39.921 0.0022504
 30 39.921 44.143 0.0022286
 30 44.143 48.869 0.0019892
 30 48.869 54.159 0.0018937
 30 54.159 60.080 0.0017186
 30 60.080 66.705 0.0017670
 30 66.705 74.112 0.0015429
 30 74.112 82.382 0.0014362
 30 82.382 91.599 0.0012313
 30 91.599 101.85 0.0010939
 30 101.85 113.20 0.00082880
 30 113.20 125.71 0.00074355
 30 125.71 139.44 0.00049565
 30 139.44 154.38 0.00043435
 30 154.38 172.08 0.00030246
 30 172.08 191.41 0.00020185
 30 191.41 212.27 0.00012452
 30 212.27 237.18 7.9663e-05
 30 237.18 264.08 3.0734e-05
 30 264.08 292.62 2.5434e-05
 60 3.1803 3.5154 0.0011208
 60 3.5154 3.8922 0.0017530
 60 3.8922 4.3081 0.0017618
 60 4.3081 4.7655 0.0024298
 60 4.7655 5.2773 0.0024231
 60 5.2773 5.8370 0.0022788
 60 5.8370 6.4603 0.0025088
 60 6.4603 7.1538 0.0023245
 60 7.1538 7.9240 0.0017086
 60 7.9240 8.7774 0.0018323
 60 8.7774 9.7208 0.0016154
 60 9.7208 10.759 0.0015502
 60 10.759 11.898 0.0014627
 60 11.898 13.183 0.0014154
 60 13.183 14.586 0.0014085
 60 14.586 16.166 0.0013172
 60 16.166 17.878 0.0013129
 60 17.878 19.796 0.0013456
 60 19.796 21.947 0.0013287
 60 21.947 24.360 0.0012319
 60 24.360 26.934 0.0010985
 60 26.934 29.791 0.0010599
 60 29.791 32.956 0.00098954
 60 32.956 36.453 0.00088901
 60 36.453 40.305 0.00086120
 60 40.305 44.818 0.00068519
 60 44.818 49.815 0.00061101
 60 49.815 55.325 0.00054459
 60 55.325 61.363 0.00047283
 60 61.363 67.937 0.00041953
 60 67.937 75.672 0.00032314
 60 75.672 84.103 0.00025184
 60 84.103 93.199 0.00021510
 60 93.199 103.94 0.00014731
 60 103.94 115.51 0.00010821
 60 115.51 127.78 7.8702e-05
 60 127.78 142.26 4.8454e-05
 60 142.26 157.49 2.6098e-05
 60 157.49 175.53 1.7556e-05
 60 175.53 194.26 1.1488e-05
 90 3.3090 3.6633 0.0022662
 90 3.6633 4.0547 0.0021487
 90 4.0547 4.4856 0.0024049
 90 4.4856 4.9578 0.0023964
 90 4.9578 5.4849 0.0019365
 90 5.4849 6.0726 0.0018908
 90 6.0726 6.7275 0.0017758
 90 6.7275 7.4371 0.0012177
 90 7.4371 8.2210 0.0013099
 90 8.2210 9.1104 0.0011165
 90 9.1104 10.092 0.0010686
 90 10.092 11.172 0.00093913
 90 11.172 12.354 0.00092484
 90 12.354 13.686 0.00078701
 90 13.686 15.137 0.00080661
 90 15.137 16.767 0.00068201
 90 16.767 18.602 0.00061312
 90 18.602 20.580 0.00062180
 90 20.580 22.792 0.00058336
 90 22.792 25.263 0.00051991
 90 25.263 28.024 0.00041225
 90 28.024 31.103 0.00037263
 90 31.103 34.534 0.00033968
 90 34.534 38.347 0.00026943
 90 38.347 42.574 0.00019135
 90 42.574 47.243 0.00016513
 90 47.243 52.375 0.00012468
 90 52.375 57.983 9.9964e-05
 90 57.983 64.576 7.8768e-05
 90 64.576 71.802 5.0524e-05
 90 71.802 79.653 3.5075e-05
 90 79.653 88.096 3.4891e-05
 90 88.096 98.030 2.0081e-05
 90 98.030 108.68 1.2276e-05
 \END;
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