|
| /*===================================================================*/
/* NRDF D1810 Data No.25 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,25;
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,25;
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
RCT=C(12C,N)X;
PHQ=ENGY-SPEC'28';
/* '28' Neutron energy spectrum */
THK-TGT=3540MG/CM**2;
INC-ENGY-LAB-RANGE=100MEV/A;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,25;
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=100MEV/A;
DELTA-DN/DOMEGA/DE=14%'29';
/* '29' 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 8.36415 9.26266 5.07720E-03
0 9.26266 10.26097 5.31844E-03
0 10.26097 11.3677 5.21545E-03
0 11.3677 12.5912 4.77150E-03
0 12.5912 13.9391 5.61055E-03
0 13.9391 15.4174 6.08172E-03
0 15.4174 17.0879 7.34749E-03
0 17.0879 18.9120 8.53290E-03
0 18.9120 20.9685 7.70489E-03
0 20.9685 23.1980 9.02873E-03
0 23.1980 25.6997 8.93420E-03
0 25.6997 28.5091 8.77760E-03
0 28.5091 31.5168 9.20043E-03
0 31.5168 34.8638 9.04131E-03
0 34.8638 38.5842 9.88984E-03
0 38.5842 42.7125 1.01127E-02
0 42.7125 47.2831 9.57329E-03
0 47.2831 52.3289 9.30840E-03
0 52.3289 57.8782 9.58272E-03
0 57.8782 64.3920 9.18734E-03
0 64.3920 71.5927 8.34550E-03
0 71.5927 79.5108 7.38656E-03
0 79.5108 88.1602 5.74576E-03
0 88.1602 97.5302 4.37342E-03
0 97.5302 108.569 2.30803E-03
0 108.569 120.533 1.34989E-03
0 120.533 133.340 9.29828E-04
0 133.340 148.471 4.96246E-04
0 148.471 164.605 2.64556E-04
0 164.605 183.786 1.29179E-04
0 183.786 204.109 1.30263E-04
0 204.109 228.419 2.74633E-05
7.5 7.72952 8.54526 2.81015E-03
7.5 8.54526 9.45027 2.80085E-03
7.5 9.45027 10.45227 3.48616E-03
7.5 10.45227 11.5588 3.20660E-03
7.5 11.5588 12.7767 3.65534E-03
7.5 12.7767 14.1555 3.99276E-03
7.5 14.1555 15.6696 4.32074E-03
7.5 15.6696 17.3233 4.84281E-03
7.5 17.3233 19.1866 4.69145E-03
7.5 19.1866 21.2088 5.58226E-03
7.5 21.2088 23.4782 5.64342E-03
7.5 23.4782 26.0274 5.71031E-03
7.5 26.0274 28.8928 5.42751E-03
7.5 28.8928 31.9642 6.10989E-03
7.5 31.9642 35.3860 6.41981E-03
7.5 35.3860 39.1943 6.15109E-03
7.5 39.1943 43.4259 6.25437E-03
7.5 43.4259 48.1177 5.88283E-03
7.5 48.1177 53.3051 5.51580E-03
7.5 53.3051 59.0196 5.43980E-03
7.5 59.0196 65.2855 5.44980E-03
7.5 65.2855 72.6468 4.54674E-03
7.5 72.6468 80.7530 3.38711E-03
7.5 80.7530 89.6212 2.74891E-03
7.5 89.6212 99.2437 2.00469E-03
7.5 99.2437 110.600 1.27727E-03
7.5 110.600 122.933 7.27189E-04
7.5 122.933 136.162 4.83699E-04
7.5 136.162 151.829 2.92337E-04
7.5 151.829 168.577 1.94407E-04
7.5 168.577 188.545 1.03291E-04
7.5 188.545 209.772 3.45638E-05
15 5.53410 6.12235 3.99669E-03
15 6.12235 6.77378 3.37582E-03
15 6.77378 7.49330 3.29227E-03
15 7.49330 8.28552 3.93045E-03
15 8.28552 9.18235 3.61267E-03
15 9.18235 10.16733 3.60999E-03
15 10.16733 11.2429 3.71305E-03
15 11.2429 12.4547 3.52402E-03
15 12.4547 13.7694 3.59614E-03
15 13.7694 15.2443 3.80719E-03
15 15.2443 16.9002 4.04999E-03
15 16.9002 18.7602 4.06120E-03
15 18.7602 20.7519 4.38087E-03
15 20.7519 22.9684 4.32190E-03
15 22.9684 25.4316 4.42540E-03
15 25.4316 28.1640 4.02987E-03
15 28.1640 31.1875 4.09739E-03
15 31.1875 34.5222 3.87743E-03
15 34.5222 38.1855 3.81534E-03
15 38.1855 42.4787 3.43068E-03
15 42.4787 47.2147 2.97295E-03
15 47.2147 52.4092 2.64719E-03
15 52.4092 58.0661 2.60636E-03
15 58.0661 64.7249 2.06298E-03
15 64.7249 71.9851 1.82169E-03
15 71.9851 79.8185 1.59296E-03
15 79.8185 89.0689 1.11329E-03
15 89.0689 99.0268 6.19789E-04
15 99.0268 109.577 6.08846E-04
15 109.577 122.024 3.87001E-04
15 122.024 135.093 2.31036E-04
15 135.093 150.556 1.82046E-04
15 150.556 166.572 1.32950E-04
15 166.572 185.547 6.55360E-05
15 185.547 208.332 3.03342E-05
30 3.52606 3.90520 1.36621E-03
30 3.90520 4.32443 1.56095E-03
30 4.32443 4.78668 1.83450E-03
30 4.78668 5.29407 1.96173E-03
30 5.29407 5.86754 1.93129E-03
30 5.86754 6.49443 2.28457E-03
30 6.49443 7.20153 1.79981E-03
30 7.20153 7.96944 1.91268E-03
30 7.96944 8.83188 1.79093E-03
30 8.83188 9.80096 1.69919E-03
30 9.80096 10.8416 1.52488E-03
30 10.8416 12.0012 1.57039E-03
30 12.0012 13.2922 1.49815E-03
30 13.2922 14.7273 1.39213E-03
30 14.7273 16.3193 1.39921E-03
30 16.3193 18.0807 1.36628E-03
30 18.0807 20.0228 1.26267E-03
30 20.0228 22.1552 1.32115E-03
30 22.1552 24.6520 1.14543E-03
30 24.6520 27.4031 1.05063E-03
30 27.4031 30.4160 9.68146E-04
30 30.4160 33.6902 9.68750E-04
30 33.6902 37.5348 8.61049E-04
30 37.5348 41.7133 7.45218E-04
30 41.7133 46.2046 7.27895E-04
30 46.2046 51.4840 5.74150E-04
30 51.4840 57.1361 5.43071E-04
30 57.1361 63.8069 4.27660E-04
30 63.8069 70.9032 3.62500E-04
30 70.9032 79.3067 2.56504E-04
30 79.3067 88.1602 2.39557E-04
30 88.1602 98.6673 1.49586E-04
30 98.6673 109.577 1.16528E-04
30 109.577 122.528 7.27469E-05
30 122.528 135.686 6.09023E-05
30 135.686 151.261 4.41546E-05
30 151.261 169.936 2.02298E-05
30 169.936 188.545 1.13170E-05
60 3.72789 4.12383 1.08411E-03
60 4.12383 4.56659 1.04938E-03
60 4.56659 5.06166 1.00516E-03
60 5.06166 5.61474 9.07980E-04
60 5.61474 6.23212 9.39274E-04
60 6.23212 6.92028 8.01668E-04
60 6.92028 7.68573 7.33224E-04
60 7.68573 8.53507 6.77448E-04
60 8.53507 9.47412 5.94236E-04
60 9.47412 10.50794 5.73484E-04
60 10.50794 11.6399 4.74811E-04
60 11.6399 12.8710 4.90496E-04
60 12.8710 14.3101 4.41972E-04
60 14.3101 15.8760 4.33115E-04
60 15.8760 17.5635 4.40955E-04
60 17.5635 19.5384 3.64976E-04
60 19.5384 21.6602 3.61670E-04
60 21.6602 24.1524 2.86737E-04
60 24.1524 26.8168 2.69223E-04
60 26.8168 29.9555 2.11164E-04
60 29.9555 33.2857 1.94989E-04
60 33.2857 37.2158 1.43861E-04
60 37.2158 41.3384 1.30648E-04
60 41.3384 46.2046 1.07369E-04
60 46.2046 51.2244 8.11167E-05
60 51.2244 57.1361 6.48859E-05
60 57.1361 64.1716 4.46994E-05
60 64.1716 71.3328 4.69212E-05
60 71.3328 79.8185 2.94741E-05
60 79.8185 89.9923 1.92086E-05
60 89.9923 100.1182 1.58661E-05
60 100.1182 112.164 1.33516E-05
60 112.164 126.679 9.18751E-06
90 3.61320 4.00678 5.49987E-04
90 4.00678 4.43039 5.49515E-04
90 4.43039 4.90272 5.17943E-04
90 4.90272 5.42926 4.54460E-04
90 5.42926 6.01539 4.41775E-04
90 6.01539 6.66692 3.92620E-04
90 6.66692 7.38958 3.47702E-04
90 7.38958 8.18875 3.04967E-04
90 8.18875 9.06945 2.65339E-04
90 9.06945 10.03561 2.54817E-04
90 10.03561 11.1660 2.45132E-04
90 11.1660 12.4097 1.69438E-04
90 12.4097 13.7694 1.72327E-04
90 13.7694 15.2443 1.72862E-04
90 15.2443 16.9721 1.41362E-04
90 16.9721 18.8442 1.16225E-04
90 18.8442 20.8499 1.26696E-04
90 20.8499 23.1980 9.37378E-05
90 23.1980 25.6997 8.42290E-05
90 25.6997 28.6361 5.87413E-05
90 28.6361 31.7393 4.74308E-05
90 31.7393 35.3860 3.76134E-05
90 35.3860 39.1943 3.47388E-05
90 39.1943 43.6677 2.05121E-05
90 43.6677 48.9751 9.26149E-06
90 48.9751 54.4800 9.67819E-06
90 54.4800 61.0008 7.15679E-06
90 61.0008 67.6054 4.36296E-06
90 67.6054 75.3901 2.66005E-06
\END;
/*===================================================================*/
|