|
| /*===================================================================*/
/* NRDF D1810 Data No.7 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,7;
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,7;
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(ALPHA,N)X;
PHQ=ENGY-SPEC'22';
/* '22' Neutron energy spectrum */
THK-TGT=10800MG/CM**2;
INC-ENGY-LAB-RANGE=100MEV/A;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,7;
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%'23';
/* '23' 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 6.63198 7.34870 4.54255E-03
0 7.34870 8.14092 4.52491E-03
0 8.14092 9.01378 4.20368E-03
0 9.01378 9.97087 3.73182E-03
0 9.97087 11.0898 3.75597E-03
0 11.0898 12.3204 3.52608E-03
0 12.3204 13.6650 3.48190E-03
0 13.6650 15.1227 3.75819E-03
0 15.1227 16.8289 3.46308E-03
0 16.8289 18.6766 3.53505E-03
0 18.6766 20.6545 4.11538E-03
0 20.6545 22.9684 3.67266E-03
0 22.9684 25.4316 4.09973E-03
0 25.4316 28.3201 3.69637E-03
0 28.3201 31.3698 4.24043E-03
0 31.3698 34.9501 3.62699E-03
0 34.9501 38.6849 4.18106E-03
0 38.6849 43.0669 4.18085E-03
0 43.0669 48.2591 3.28632E-03
0 48.2591 53.6368 3.71196E-03
0 53.6368 59.9975 3.29580E-03
0 59.9975 66.4298 3.37998E-03
0 66.4298 73.9986 3.34651E-03
0 73.9986 83.0008 2.57680E-03
0 83.0008 91.8850 2.83779E-03
0 91.8850 102.3587 2.55641E-03
0 102.3587 114.848 2.03903E-03
0 114.848 129.941 1.19734E-03
0 129.941 144.439 9.88940E-04
0 144.439 161.724 7.19418E-04
0 161.724 182.626 4.46449E-04
0 182.626 208.332 1.53216E-04
0 208.332 231.794 8.59421E-05
0 231.794 260.012 4.48179E-05
0 260.012 294.532 2.35236E-05
7.5 6.23212 6.92028 3.92410E-03
7.5 6.92028 7.68573 3.81519E-03
7.5 7.68573 8.53507 3.47152E-03
7.5 8.53507 9.47412 3.14523E-03
7.5 9.47412 10.50794 2.77499E-03
7.5 10.50794 11.6399 2.64346E-03
7.5 11.6399 12.8710 2.77844E-03
7.5 12.8710 14.3101 2.75743E-03
7.5 14.3101 15.8760 2.76189E-03
7.5 15.8760 17.5635 2.91470E-03
7.5 17.5635 19.5384 2.65057E-03
7.5 19.5384 21.6602 3.19390E-03
7.5 21.6602 24.1524 2.96234E-03
7.5 24.1524 26.8168 3.06393E-03
7.5 26.8168 29.9555 2.81908E-03
7.5 29.9555 33.2857 3.24775E-03
7.5 33.2857 37.2158 2.84732E-03
7.5 37.2158 41.3384 3.11707E-03
7.5 41.3384 46.2046 2.89810E-03
7.5 46.2046 51.2244 3.08162E-03
7.5 51.2244 57.1361 3.07132E-03
7.5 57.1361 64.1716 2.52809E-03
7.5 64.1716 71.3328 2.67536E-03
7.5 71.3328 79.8185 2.45365E-03
7.5 79.8185 89.9923 1.84769E-03
7.5 89.9923 100.1182 1.97719E-03
7.5 100.1182 112.164 1.47576E-03
7.5 112.164 126.679 8.12191E-04
7.5 126.679 140.580 7.37243E-04
7.5 140.580 157.101 4.39289E-04
7.5 157.101 177.004 2.73492E-04
7.5 177.004 201.371 9.65297E-05
7.5 201.371 223.506 5.15419E-05
7.5 223.506 249.994 2.86991E-05
15 6.61047 7.36427 3.32676E-03
15 7.36427 8.18135 3.16721E-03
15 8.18135 9.05657 3.02522E-03
15 9.05657 10.08097 2.63218E-03
15 10.08097 11.1719 2.45088E-03
15 11.1719 12.4512 2.05555E-03
15 12.4512 13.8018 2.23270E-03
15 13.8018 15.3867 2.08990E-03
15 15.3867 17.0388 2.31034E-03
15 17.0388 18.9749 2.38754E-03
15 18.9749 21.2648 2.20642E-03
15 21.2648 23.6312 2.34899E-03
15 23.6312 26.4220 1.77602E-03
15 26.4220 29.2339 2.03567E-03
15 29.2339 32.5282 2.04250E-03
15 32.5282 36.4245 1.95049E-03
15 36.4245 41.0819 1.48828E-03
15 41.0819 45.6995 1.70275E-03
15 45.6995 51.1648 1.51216E-03
15 51.1648 57.7056 1.10738E-03
15 57.7056 63.9187 1.24324E-03
15 63.9187 71.2334 1.15846E-03
15 71.2334 79.9373 1.00137E-03
15 79.9373 90.4237 8.13449E-04
15 90.4237 103.2415 4.77858E-04
15 103.2415 114.848 4.84491E-04
15 114.848 128.671 3.47263E-04
15 128.671 145.354 2.48152E-04
15 145.354 165.811 1.39334E-04
15 165.811 191.384 6.94294E-05
15 191.384 212.246 6.15594E-05
15 212.246 237.153 2.72660E-05
15 237.153 267.350 1.62855E-05
30 3.40050 3.76933 3.76673E-03
30 3.76933 4.17278 3.01927E-03
30 4.17278 4.62786 2.99801E-03
30 4.62786 5.12203 2.69864E-03
30 5.12203 5.67690 2.60107E-03
30 5.67690 6.30044 2.37996E-03
30 6.30044 6.96979 2.21155E-03
30 6.96979 7.71563 1.91234E-03
30 7.71563 8.54560 1.71210E-03
30 8.54560 9.46785 1.57035E-03
30 9.46785 10.49047 1.42010E-03
30 10.49047 11.6212 1.39173E-03
30 11.6212 12.8669 1.28367E-03
30 12.8669 14.2335 1.32841E-03
30 14.2335 15.8318 1.26964E-03
30 15.8318 17.5905 1.25363E-03
30 17.5905 19.5133 1.23244E-03
30 19.5133 21.5994 1.29479E-03
30 21.5994 24.0434 1.13701E-03
30 24.0434 26.6929 9.72968E-04
30 26.6929 29.5328 1.05465E-03
30 29.5328 32.8599 8.55551E-04
30 32.8599 36.4081 9.21399E-04
30 36.4081 40.5771 7.18014E-04
30 40.5771 44.9894 6.58936E-04
30 44.9894 50.1833 5.14117E-04
30 50.1833 55.6184 5.36254E-04
30 55.6184 62.0185 4.00379E-04
30 62.0185 68.6057 3.81430E-04
30 68.6057 76.3471 2.97148E-04
30 76.3471 85.5411 2.05572E-04
30 85.5411 94.8823 1.60821E-04
30 94.8823 105.934 1.25023E-04
30 105.934 119.166 6.13010E-05
30 119.166 132.323 4.28146E-05
30 132.323 147.968 2.74836E-05
30 147.968 166.820 1.47872E-05
30 166.820 184.885 1.19255E-05
60 3.60681 4.00398 2.46755E-03
60 4.00398 4.44686 2.28928E-03
60 4.44686 4.93946 1.99965E-03
60 4.93946 5.48593 1.67479E-03
60 5.48593 6.09009 1.47568E-03
60 6.09009 6.75518 1.29407E-03
60 6.75518 7.48322 1.04878E-03
60 7.48322 8.27488 9.82384E-04
60 8.27488 9.19982 7.85605E-04
60 9.19982 10.20586 6.14724E-04
60 10.20586 11.2893 6.14729E-04
60 11.2893 12.5563 5.02973E-04
60 12.5563 13.9164 5.28379E-04
60 13.9164 15.5120 4.59790E-04
60 15.5120 17.2159 4.65869E-04
60 17.2159 19.2196 4.17785E-04
60 19.2196 21.3418 4.24634E-04
60 21.3418 23.8408 3.26162E-04
60 23.8408 26.4557 2.74641E-04
60 26.4557 29.5328 2.31899E-04
60 29.5328 32.6965 2.05687E-04
60 32.6965 36.4081 1.70277E-04
60 36.4081 40.8045 1.16030E-04
60 40.8045 45.2557 1.04544E-04
60 45.2557 50.4986 7.12920E-05
60 50.4986 56.7383 4.38560E-05
60 56.7383 62.8980 3.79395E-05
60 62.8980 70.1587 2.42554E-05
60 70.1587 78.8102 1.31760E-05
90 3.31156 3.67782 1.89432E-03
90 3.67782 4.06604 1.47637E-03
90 4.06604 4.49513 1.51286E-03
90 4.49513 4.99602 1.18641E-03
90 4.99602 5.55224 9.26762E-04
90 5.55224 6.16771 8.55073E-04
90 6.16771 6.84591 7.29981E-04
90 6.84591 7.58918 5.98935E-04
90 7.58918 8.39820 5.67345E-04
90 8.39820 9.34465 4.10631E-04
90 9.34465 10.37521 3.64780E-04
90 10.37521 11.4868 2.93429E-04
90 11.4868 12.7883 2.55755E-04
90 12.7883 14.1874 2.48695E-04
90 14.1874 15.8318 2.04875E-04
90 15.8318 17.5905 2.16194E-04
90 17.5905 19.6627 1.42227E-04
90 19.6627 21.8616 1.54942E-04
90 21.8616 24.4565 1.00516E-04
90 24.4565 27.1775 9.39177E-05
90 27.1775 30.3875 6.53834E-05
90 30.3875 33.6958 6.34598E-05
90 33.6958 37.5874 4.33143E-05
90 37.5874 42.2107 2.29173E-05
90 42.2107 46.9066 1.57713E-05
90 46.9066 52.4558 1.03948E-05
\END;
/*===================================================================*/
|