|
| /*===================================================================*/
/* NRDF D1810 Data No.31 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,31;
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,31;
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=27AL(12C,N)X;
PHQ=ENGY-SPEC'30';
/* '30' Neutron energy spectrum */
THK-TGT=5400MG/CM**2;
INC-ENGY-LAB-RANGE=100MEV/A;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,31;
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%'31';
/* '31' 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 7.59075 8.40391 4.88705E-03
0 8.40391 9.30903 4.56131E-03
0 9.30903 10.31506 4.15819E-03
0 10.31506 11.4309 3.87233E-03
0 11.4309 12.6649 4.52922E-03
0 12.6649 14.0250 4.61446E-03
0 14.0250 15.5175 5.21347E-03
0 15.5175 17.2050 4.86726E-03
0 17.2050 19.0485 5.62986E-03
0 19.0485 21.1282 6.03737E-03
0 21.1282 23.3842 6.10591E-03
0 23.3842 25.9175 6.29196E-03
0 25.9175 28.7640 5.50137E-03
0 28.7640 31.8140 6.45224E-03
0 31.8140 35.2107 6.96200E-03
0 35.2107 38.9893 6.34265E-03
0 38.9893 43.1861 6.33667E-03
0 43.1861 47.8370 6.07599E-03
0 47.8370 52.9766 5.70572E-03
0 52.9766 58.6353 5.86632E-03
0 58.6353 64.8365 6.00151E-03
0 64.8365 72.1167 5.44114E-03
0 72.1167 80.1282 4.96602E-03
0 80.1282 88.8860 3.57801E-03
0 88.8860 98.3810 2.72598E-03
0 98.3810 109.577 1.83193E-03
0 109.577 121.724 9.13245E-04
0 121.724 134.739 6.45055E-04
0 134.739 150.135 3.33944E-04
0 150.135 166.572 2.09409E-04
0 166.572 186.141 1.10626E-04
0 186.141 206.908 6.84683E-05
0 206.908 231.794 1.44260E-05
7.5 5.97338 6.60409 3.58622E-03
7.5 6.60409 7.30804 3.22512E-03
7.5 7.30804 8.09365 3.01749E-03
7.5 8.09365 8.94770 2.76160E-03
7.5 8.94770 9.89381 2.73110E-03
7.5 9.89381 10.9398 2.86747E-03
7.5 10.9398 12.0927 3.35208E-03
7.5 12.0927 13.3990 3.02897E-03
7.5 13.3990 14.8364 2.99992E-03
7.5 14.8364 16.4102 3.54893E-03
7.5 16.4102 18.1868 3.65843E-03
7.5 18.1868 20.1220 3.54066E-03
7.5 20.1220 22.2997 4.06808E-03
7.5 22.2997 24.6520 3.92522E-03
7.5 24.6520 27.2844 4.25080E-03
7.5 27.2844 30.2305 4.08241E-03
7.5 30.2305 33.5275 4.30420E-03
7.5 33.5275 37.2158 4.24849E-03
7.5 37.2158 41.3384 4.45828E-03
7.5 41.3384 45.9409 4.08352E-03
7.5 45.9409 51.0695 4.07184E-03
7.5 51.0695 56.7705 3.72319E-03
7.5 56.7705 63.0869 3.35472E-03
7.5 63.0869 70.0556 3.27169E-03
7.5 70.0556 77.7028 2.68230E-03
7.5 77.7028 86.0377 2.26871E-03
7.5 86.0377 95.8627 1.78106E-03
7.5 95.8627 106.596 1.11341E-03
7.5 106.596 118.207 7.75423E-04
7.5 118.207 131.964 5.54397E-04
7.5 131.964 146.837 3.11141E-04
7.5 146.837 162.675 2.18007E-04
7.5 162.675 181.479 9.23461E-05
7.5 181.479 201.371 2.84391E-05
7.5 201.371 225.124 2.64279E-05
7.5 225.124 249.994 1.14077E-05
15 7.49330 8.28552 3.40226E-03
15 8.28552 9.18235 3.30951E-03
15 9.18235 10.16733 3.08331E-03
15 10.16733 11.2429 3.42505E-03
15 11.2429 12.4547 3.27807E-03
15 12.4547 13.7694 3.06609E-03
15 13.7694 15.2443 3.22898E-03
15 15.2443 16.9002 3.53004E-03
15 16.9002 18.7602 3.28651E-03
15 18.7602 20.7519 3.22557E-03
15 20.7519 22.9684 3.16393E-03
15 22.9684 25.4316 3.09789E-03
15 25.4316 28.1640 3.19720E-03
15 28.1640 31.1875 2.94762E-03
15 31.1875 34.5222 2.91744E-03
15 34.5222 38.1855 2.97880E-03
15 38.1855 42.4787 2.37984E-03
15 42.4787 47.2147 2.37531E-03
15 47.2147 52.4092 2.16360E-03
15 52.4092 58.0661 1.92419E-03
15 58.0661 64.7249 1.55701E-03
15 64.7249 71.9851 1.37009E-03
15 71.9851 79.8185 1.12372E-03
15 79.8185 89.0689 9.17767E-04
15 89.0689 99.0268 6.26004E-04
15 99.0268 109.577 4.57778E-04
15 109.577 122.024 2.90067E-04
15 122.024 135.093 2.62569E-04
15 135.093 150.556 9.90369E-05
15 150.556 166.572 1.38220E-04
15 166.572 185.547 7.54428E-05
15 185.547 208.332 3.13073E-05
15 208.332 231.794 2.04696E-05
30 3.66505 4.05640 1.48043E-03
30 4.05640 4.48796 1.89975E-03
30 4.48796 4.96242 2.33854E-03
30 4.96242 5.49881 2.16309E-03
30 5.49881 6.08640 2.22820E-03
30 6.08640 6.74981 2.06915E-03
30 6.74981 7.47236 1.95500E-03
30 7.47236 8.28552 1.77142E-03
30 8.28552 9.16342 1.69149E-03
30 9.16342 10.14515 1.73016E-03
30 10.14515 11.2429 1.56082E-03
30 11.2429 12.4697 1.50849E-03
30 12.4697 13.8398 1.24251E-03
30 13.8398 15.3676 1.35910E-03
30 15.3676 17.0685 1.33230E-03
30 17.0685 18.9573 1.17469E-03
30 18.9573 21.0481 1.08027E-03
30 21.0481 23.3530 1.02842E-03
30 23.3530 25.8810 9.80730E-04
30 25.8810 28.6361 9.19682E-04
30 28.6361 31.8639 8.95467E-04
30 31.8639 35.3860 8.15059E-04
30 35.3860 39.1943 7.78792E-04
30 39.1943 43.6677 5.77550E-04
30 43.6677 48.4959 5.42932E-04
30 48.4959 53.6368 5.56506E-04
30 53.6368 59.6688 4.21777E-04
30 59.6688 66.0449 3.98073E-04
30 66.0449 73.5437 2.63933E-04
30 73.5437 81.3853 2.15092E-04
30 81.3853 90.6164 1.68354E-04
30 90.6164 101.6032 1.10296E-04
30 101.6032 113.047 8.67362E-05
30 113.047 126.679 5.51477E-05
30 126.679 140.580 3.67801E-05
30 140.580 157.101 1.89714E-05
60 3.36107 3.72789 1.44930E-03
60 3.72789 4.12383 1.37274E-03
60 4.12383 4.56659 1.42991E-03
60 4.56659 5.06166 1.32434E-03
60 5.06166 5.61474 1.17660E-03
60 5.61474 6.23212 1.23696E-03
60 6.23212 6.92028 1.03564E-03
60 6.92028 7.68573 9.55460E-04
60 7.68573 8.53507 7.52373E-04
60 8.53507 9.47412 6.91100E-04
60 9.47412 10.50794 6.27577E-04
60 10.50794 11.6399 5.38211E-04
60 11.6399 12.8710 5.11268E-04
60 12.8710 14.3101 4.62705E-04
60 14.3101 15.8760 4.20375E-04
60 15.8760 17.5635 4.22716E-04
60 17.5635 19.5384 3.44701E-04
60 19.5384 21.6602 3.57342E-04
60 21.6602 24.1524 2.83769E-04
60 24.1524 26.8168 2.76911E-04
60 26.8168 29.9555 2.08909E-04
60 29.9555 33.2857 2.09512E-04
60 33.2857 37.2158 1.55930E-04
60 37.2158 41.3384 1.20948E-04
60 41.3384 46.2046 9.42226E-05
60 46.2046 51.2244 8.85539E-05
60 51.2244 57.1361 6.46602E-05
60 57.1361 64.1716 4.64743E-05
60 64.1716 71.3328 3.96316E-05
60 71.3328 79.8185 2.49056E-05
60 79.8185 89.9923 2.39190E-05
60 89.9923 100.1182 1.41811E-05
90 3.61320 4.00678 9.47044E-04
90 4.00678 4.43039 8.96360E-04
90 4.43039 4.90272 8.54403E-04
90 4.90272 5.42926 7.72206E-04
90 5.42926 6.01539 7.42660E-04
90 6.01539 6.66692 5.94046E-04
90 6.66692 7.38958 5.17195E-04
90 7.38958 8.18875 4.15608E-04
90 8.18875 9.06945 3.61991E-04
90 9.06945 10.03561 3.42849E-04
90 10.03561 11.1660 2.60821E-04
90 11.1660 12.4097 2.83729E-04
90 12.4097 13.7694 2.02055E-04
90 13.7694 15.2443 1.81261E-04
90 15.2443 16.9721 1.64971E-04
90 16.9721 18.8442 1.49061E-04
90 18.8442 20.8499 1.52888E-04
90 20.8499 23.1980 8.96741E-05
90 23.1980 25.6997 9.46764E-05
90 25.6997 28.6361 7.81690E-05
90 28.6361 31.7393 5.93154E-05
90 31.7393 35.3860 4.60943E-05
90 35.3860 39.1943 3.24965E-05
90 39.1943 43.6677 2.56062E-05
90 43.6677 48.9751 9.93435E-06
90 48.9751 54.4800 1.34092E-05
90 54.4800 61.0008 6.39728E-06
90 61.0008 67.6054 6.68563E-06
90 67.6054 75.3901 6.73696E-06
\END;
/*===================================================================*/
|