|
| /*===================================================================*/
/* NRDF D1810 Data No.1 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,1;
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,1;
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(ALPHA,N)X;
PHQ=ENGY-SPEC'20';
/* '20' Neutron energy spectrum */
THK-TGT=8850MG/CM**2;
INC-ENGY-LAB-RANGE=100MEV/A;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,1;
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%'21';
/* '21' 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 8.26267 9.15704 2.92386E-03
0 9.15704 10.13922 2.73874E-03
0 10.13922 11.2118 2.91945E-03
0 11.2118 12.4202 2.73323E-03
0 12.4202 13.7312 3.06968E-03
0 13.7312 15.2020 3.34458E-03
0 15.2020 16.8531 3.75812E-03
0 16.8531 18.7077 3.93503E-03
0 18.7077 20.6936 4.10179E-03
0 20.6936 22.9037 4.66164E-03
0 22.9037 25.3597 4.65505E-03
0 25.3597 28.0841 4.73346E-03
0 28.0841 31.0985 5.24885E-03
0 31.0985 34.4233 4.98519E-03
0 34.4233 38.0754 5.40164E-03
0 38.0754 42.3555 4.99590E-03
0 42.3555 47.0766 5.04214E-03
0 47.0766 52.2549 4.80090E-03
0 52.2549 57.8935 5.01173E-03
0 57.8935 64.5306 4.48506E-03
0 64.5306 71.7667 4.20574E-03
0 71.7667 79.5735 3.91135E-03
0 79.5735 88.7916 3.14961E-03
0 88.7916 98.7141 2.30106E-03
0 98.7141 109.226 2.11058E-03
0 109.226 121.626 1.14231E-03
0 121.626 134.643 7.68517E-04
0 134.643 150.044 4.06464E-04
0 150.044 165.992 2.25198E-04
0 165.992 184.885 1.05235E-04
0 184.885 207.565 4.84168E-05
0 207.565 230.914 5.44924E-05
0 230.914 258.987 1.76873E-05
7.5 7.17845 7.94939 2.65124E-03
7.5 7.94939 8.81878 2.47130E-03
7.5 8.81878 9.76097 2.34549E-03
7.5 9.76097 10.8177 2.39700E-03
7.5 10.8177 12.0036 2.24522E-03
7.5 12.0036 13.2719 2.41389E-03
7.5 13.2719 14.6815 2.68985E-03
7.5 14.6815 16.2457 3.08997E-03
7.5 16.2457 17.9776 2.92837E-03
7.5 17.9776 19.8901 3.19823E-03
7.5 19.8901 21.9946 3.54354E-03
7.5 21.9946 24.4565 3.43820E-03
7.5 24.4565 27.1775 3.48568E-03
7.5 27.1775 30.1703 3.51837E-03
7.5 30.1703 33.4417 3.41752E-03
7.5 33.4417 36.9905 3.68173E-03
7.5 36.9905 41.1493 3.35474E-03
7.5 41.1493 45.6600 3.08674E-03
7.5 45.6600 50.4986 3.21349E-03
7.5 50.4986 56.1741 2.79290E-03
7.5 56.1741 62.2366 2.87948E-03
7.5 62.2366 69.3754 2.52053E-03
7.5 69.3754 76.9515 2.44708E-03
7.5 76.9515 85.9010 1.94984E-03
7.5 85.9010 95.3058 1.86112E-03
7.5 95.3058 106.438 1.21359E-03
7.5 106.438 117.965 9.81363E-04
7.5 117.965 131.612 6.94787E-04
7.5 131.612 147.968 3.62393E-04
7.5 147.968 164.764 2.28855E-04
7.5 164.764 184.885 8.23673E-05
7.5 184.885 204.921 6.10395E-05
7.5 204.921 228.805 4.74585E-05
7.5 228.805 257.705 1.16220E-05
15 6.38209 7.06499 2.57959E-03
15 7.06499 7.82652 2.55457E-03
15 7.82652 8.67508 2.52981E-03
15 8.67508 9.61906 2.32513E-03
15 9.61906 10.6671 2.29466E-03
15 10.6671 11.8275 2.28478E-03
15 11.8275 13.1077 2.26670E-03
15 13.1077 14.5139 2.47450E-03
15 14.5139 16.0504 2.78865E-03
15 16.0504 17.8471 2.75453E-03
15 17.8471 19.8138 2.83274E-03
15 19.8138 21.9501 2.97232E-03
15 21.9501 24.4565 2.73592E-03
15 24.4565 27.1775 2.41847E-03
15 27.1775 30.0984 2.62119E-03
15 30.0984 33.5260 2.35282E-03
15 33.5260 37.1878 2.53526E-03
15 37.1878 41.4985 1.99526E-03
15 41.4985 46.0698 2.03577E-03
15 46.0698 51.4629 1.71876E-03
15 51.4629 57.1194 1.74968E-03
15 57.1194 63.7970 1.30711E-03
15 63.7970 70.6883 1.29046E-03
15 70.6883 78.8102 1.05828E-03
15 78.8102 88.4882 7.19625E-04
15 88.4882 98.3558 6.37462E-04
15 98.3558 110.074 4.09635E-04
15 110.074 124.168 1.89144E-04
15 124.168 138.248 1.41891E-04
15 138.248 155.074 7.81245E-05
15 155.074 175.474 4.43213E-05
15 175.474 195.149 2.75394E-05
15 195.149 218.724 1.08093E-05
30 3.46535 3.83239 3.09253E-03
30 3.83239 4.24637 2.06337E-03
30 4.24637 4.69640 2.41089E-03
30 4.69640 5.20189 2.20260E-03
30 5.20189 5.77020 1.83293E-03
30 5.77020 6.38209 1.90921E-03
30 6.38209 7.06499 1.76968E-03
30 7.06499 7.82652 1.62586E-03
30 7.82652 8.67508 1.56214E-03
30 8.67508 9.61906 1.47290E-03
30 9.61906 10.6671 1.32956E-03
30 10.6671 11.8275 1.40934E-03
30 11.8275 13.1077 1.32554E-03
30 13.1077 14.5139 1.23221E-03
30 14.5139 16.0504 1.46728E-03
30 16.0504 17.8471 1.32512E-03
30 17.8471 19.8138 1.34723E-03
30 19.8138 21.9501 1.48800E-03
30 21.9501 24.4565 1.21392E-03
30 24.4565 27.1775 1.15558E-03
30 27.1775 30.0984 1.18561E-03
30 30.0984 33.5260 9.89662E-04
30 33.5260 37.1878 1.04014E-03
30 37.1878 41.4985 7.90311E-04
30 41.4985 46.0698 7.84812E-04
30 46.0698 51.4629 5.85788E-04
30 51.4629 57.1194 6.14163E-04
30 57.1194 63.7970 4.27037E-04
30 63.7970 70.6883 4.03972E-04
30 70.6883 78.8102 3.27185E-04
30 78.8102 88.4882 1.97429E-04
30 88.4882 98.3558 1.58461E-04
30 98.3558 110.074 1.19906E-04
30 110.074 124.168 5.66187E-05
30 124.168 138.248 4.96905E-05
30 138.248 155.074 2.72681E-05
60 3.67782 4.06604 1.59596E-03
60 4.06604 4.49513 1.62583E-03
60 4.49513 4.99602 1.36190E-03
60 4.99602 5.55224 1.15570E-03
60 5.55224 6.16771 1.17289E-03
60 6.16771 6.84591 8.69483E-04
60 6.84591 7.58918 7.95884E-04
60 7.58918 8.39820 7.86267E-04
60 8.39820 9.34465 6.49610E-04
60 9.34465 10.37521 5.57775E-04
60 10.37521 11.4868 5.94733E-04
60 11.4868 12.7883 4.87728E-04
60 12.7883 14.1874 5.20525E-04
60 14.1874 15.8318 4.56968E-04
60 15.8318 17.5905 5.26309E-04
60 17.5905 19.6627 4.11946E-04
60 19.6627 21.8616 4.21589E-04
60 21.8616 24.4565 2.92922E-04
60 24.4565 27.1775 2.71242E-04
60 27.1775 30.3875 2.20137E-04
60 30.3875 33.6958 2.15536E-04
60 33.6958 37.5874 1.73539E-04
60 37.5874 42.2107 1.13314E-04
60 42.2107 46.9066 9.51821E-05
60 46.9066 52.4558 6.21652E-05
60 52.4558 59.0853 4.55456E-05
60 59.0853 65.6558 3.22369E-05
60 65.6558 73.4329 2.06770E-05
90 3.57209 3.96344 1.28752E-03
90 3.96344 4.39936 8.76945E-04
90 4.39936 4.88379 7.20857E-04
90 4.88379 5.42086 6.03282E-04
90 5.42086 6.01393 6.20177E-04
90 6.01393 6.66625 4.70806E-04
90 6.66625 7.37950 4.47320E-04
90 7.37950 8.21428 3.73502E-04
90 8.21428 9.12870 3.39514E-04
90 9.12870 10.12264 2.87364E-04
90 10.12264 11.1925 2.59279E-04
90 11.1925 12.4427 2.48418E-04
90 12.4427 13.7838 2.08561E-04
90 13.7838 15.3559 1.57552E-04
90 15.3559 17.0331 1.89178E-04
90 17.0331 19.0038 1.52788E-04
90 19.0038 21.0889 1.51344E-04
90 21.0889 23.5418 1.02538E-04
90 23.5418 26.1055 9.58734E-05
90 26.1055 29.1192 6.59631E-05
90 29.1192 32.2138 6.56677E-05
90 32.2138 35.8396 3.87156E-05
90 35.8396 40.1282 2.39216E-05
90 40.1282 44.4636 1.94961E-05
90 44.4636 49.5619 9.37170E-06
\END;
/*===================================================================*/
|