|
| /*===================================================================*/
/* NRDF D1810 Data No.13 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,13;
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,13;
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=CU(ALPHA,N)X;
PHQ=ENGY-SPEC'24';
/* '24' Neutron energy spectrum */
THK-TGT=13395MG/CM**2;
INC-ENGY-LAB-RANGE=100MEV/A;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,13;
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%'25';
/* '25' 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 8.53507 9.47412 3.75093E-03
0 9.47412 10.50794 3.26340E-03
0 10.50794 11.6399 3.46100E-03
0 11.6399 12.8710 3.32510E-03
0 12.8710 14.3101 2.99462E-03
0 14.3101 15.8760 2.75152E-03
0 15.8760 17.5635 3.34795E-03
0 17.5635 19.5384 3.12137E-03
0 19.5384 21.6602 3.23948E-03
0 21.6602 24.1524 3.06608E-03
0 24.1524 26.8168 3.13221E-03
0 26.8168 29.9555 2.81200E-03
0 29.9555 33.2857 3.06219E-03
0 33.2857 37.2158 2.79055E-03
0 37.2158 41.3384 2.87071E-03
0 41.3384 46.2046 2.42483E-03
0 46.2046 51.2244 2.58193E-03
0 51.2244 57.1361 2.57531E-03
0 57.1361 64.1716 2.16498E-03
0 64.1716 71.3328 2.32198E-03
0 71.3328 79.8185 2.14263E-03
0 79.8185 89.9923 1.61191E-03
0 89.9923 100.1182 1.86775E-03
0 100.1182 112.164 1.45938E-03
0 112.164 126.679 9.37230E-04
0 126.679 140.580 7.92236E-04
0 140.580 157.101 5.61322E-04
0 157.101 177.004 3.70586E-04
0 177.004 201.371 1.41052E-04
0 201.371 223.506 1.04109E-04
0 223.506 249.994 5.12452E-05
0 249.994 282.203 1.97111E-05
7.5 6.63198 7.34870 3.93011E-03
7.5 7.34870 8.14092 3.41873E-03
7.5 8.14092 9.01378 3.39171E-03
7.5 9.01378 9.97087 2.95807E-03
7.5 9.97087 11.0898 2.63566E-03
7.5 11.0898 12.3204 2.45909E-03
7.5 12.3204 13.6650 2.17750E-03
7.5 13.6650 15.1227 2.33444E-03
7.5 15.1227 16.8289 2.28684E-03
7.5 16.8289 18.6766 2.22206E-03
7.5 18.6766 20.6545 2.41918E-03
7.5 20.6545 22.9684 2.29382E-03
7.5 22.9684 25.4316 2.60618E-03
7.5 25.4316 28.3201 2.19701E-03
7.5 28.3201 31.3698 2.49630E-03
7.5 31.3698 34.9501 2.00067E-03
7.5 34.9501 38.6849 2.36541E-03
7.5 38.6849 43.0669 2.22913E-03
7.5 43.0669 48.2591 1.87007E-03
7.5 48.2591 53.6368 2.08767E-03
7.5 53.6368 59.9975 1.80289E-03
7.5 59.9975 66.4298 2.08498E-03
7.5 66.4298 73.9986 1.97800E-03
7.5 73.9986 83.0008 1.44534E-03
7.5 83.0008 91.8850 1.51234E-03
7.5 91.8850 102.3587 1.32173E-03
7.5 102.3587 114.848 1.02359E-03
7.5 114.848 129.941 5.89848E-04
7.5 129.941 144.439 4.65150E-04
7.5 144.439 161.724 2.80970E-04
7.5 161.724 182.626 1.66236E-04
7.5 182.626 208.332 5.15648E-05
7.5 208.332 231.794 4.05914E-05
7.5 231.794 260.012 1.17065E-05
15 7.62244 8.48422 2.87688E-03
15 8.48422 9.41017 2.78256E-03
15 9.41017 10.49719 2.16802E-03
15 10.49719 11.6587 2.08606E-03
15 11.6587 13.0257 1.80196E-03
15 13.0257 14.4743 1.96285E-03
15 14.4743 16.1809 1.70240E-03
15 16.1809 17.9674 1.92641E-03
15 17.9674 20.0704 1.72597E-03
15 20.0704 22.2328 1.88266E-03
15 22.2328 24.7696 1.78972E-03
15 24.7696 27.7738 1.42321E-03
15 27.7738 30.8140 1.59242E-03
15 30.8140 34.3923 1.44650E-03
15 34.3923 38.6462 1.11616E-03
15 38.6462 42.8392 1.25944E-03
15 42.8392 47.7727 1.12942E-03
15 47.7727 53.6368 1.06387E-03
15 53.6368 60.6894 7.82871E-04
15 60.6894 67.4224 8.49330E-04
15 67.4224 75.3901 7.94769E-04
15 75.3901 84.9279 6.68108E-04
15 84.9279 96.4986 4.16970E-04
15 96.4986 106.896 4.53174E-04
15 106.896 119.182 3.03527E-04
15 119.182 133.876 2.12977E-04
15 133.876 151.698 1.50071E-04
15 151.698 173.684 9.31588E-05
15 173.684 201.371 3.75307E-05
15 201.371 224.126 3.61311E-05
15 224.126 251.493 1.46034E-05
30 3.83239 4.24637 5.82869E-03
30 4.24637 4.69640 5.86908E-03
30 4.69640 5.20189 4.64343E-03
30 5.20189 5.77020 3.91416E-03
30 5.77020 6.38209 4.00532E-03
30 6.38209 7.06499 3.01470E-03
30 7.06499 7.82652 2.63335E-03
30 7.82652 8.67508 2.42022E-03
30 8.67508 9.61906 1.96751E-03
30 9.61906 10.6671 1.71458E-03
30 10.6671 11.8275 1.63125E-03
30 11.8275 13.1077 1.46477E-03
30 13.1077 14.5139 1.43637E-03
30 14.5139 16.0504 1.42819E-03
30 16.0504 17.8471 1.22892E-03
30 17.8471 19.8138 1.22802E-03
30 19.8138 21.9501 1.30286E-03
30 21.9501 24.4565 1.05450E-03
30 24.4565 27.1775 1.01372E-03
30 27.1775 30.0984 9.86479E-04
30 30.0984 33.5260 8.47478E-04
30 33.5260 37.1878 8.70968E-04
30 37.1878 41.4985 6.88067E-04
30 41.4985 46.0698 6.15648E-04
30 46.0698 51.4629 4.99147E-04
30 51.4629 57.1194 4.67644E-04
30 57.1194 63.7970 3.38213E-04
30 63.7970 70.6883 3.22174E-04
30 70.6883 78.8102 2.54667E-04
30 78.8102 88.4882 1.55413E-04
30 88.4882 98.3558 1.32899E-04
30 98.3558 110.074 1.04733E-04
30 110.074 124.168 4.76818E-05
30 124.168 138.248 3.54306E-05
30 138.248 155.074 2.41500E-05
30 155.074 175.474 1.16378E-05
60 3.67782 4.06604 4.87249E-03
60 4.06604 4.49513 4.97658E-03
60 4.49513 4.99602 3.90081E-03
60 4.99602 5.55224 2.96493E-03
60 5.55224 6.16771 2.55244E-03
60 6.16771 6.84591 2.07472E-03
60 6.84591 7.58918 1.62595E-03
60 7.58918 8.39820 1.57497E-03
60 8.39820 9.34465 1.13345E-03
60 9.34465 10.37521 9.41170E-04
60 10.37521 11.4868 8.40934E-04
60 11.4868 12.7883 6.48278E-04
60 12.7883 14.1874 6.78389E-04
60 14.1874 15.8318 5.70786E-04
60 15.8318 17.5905 5.77425E-04
60 17.5905 19.6627 4.96526E-04
60 19.6627 21.8616 4.57071E-04
60 21.8616 24.4565 3.29281E-04
60 24.4565 27.1775 3.08356E-04
60 27.1775 30.3875 2.28530E-04
60 30.3875 33.6958 2.25222E-04
60 33.6958 37.5874 1.82322E-04
60 37.5874 42.2107 1.10048E-04
60 42.2107 46.9066 9.17037E-05
60 46.9066 52.4558 5.85741E-05
60 52.4558 59.0853 3.56914E-05
60 59.0853 65.6558 2.63487E-05
60 65.6558 73.4329 2.02794E-05
90 3.60681 4.00398 4.82589E-03
90 4.00398 4.44686 4.29170E-03
90 4.44686 4.93946 3.50020E-03
90 4.93946 5.48593 2.75074E-03
90 5.48593 6.09009 2.55959E-03
90 6.09009 6.75518 1.95271E-03
90 6.75518 7.48322 1.53183E-03
90 7.48322 8.27488 1.28481E-03
90 8.27488 9.19982 9.09090E-04
90 9.19982 10.20586 7.83797E-04
90 10.20586 11.2893 6.84004E-04
90 11.2893 12.5563 5.15962E-04
90 12.5563 13.9164 4.18170E-04
90 13.9164 15.5120 3.53229E-04
90 15.5120 17.2159 3.77925E-04
90 17.2159 19.2196 2.69066E-04
90 19.2196 21.3418 2.44141E-04
90 21.3418 23.8408 1.94379E-04
90 23.8408 26.4557 1.71342E-04
90 26.4557 29.5328 9.81420E-05
90 29.5328 32.6965 9.79702E-05
90 32.6965 36.4081 7.62490E-05
90 36.4081 40.8045 4.66717E-05
90 40.8045 45.2557 3.19556E-05
90 45.2557 50.4986 2.08051E-05
90 50.4986 56.7383 1.05461E-05
\END;
/*===================================================================*/
|