|
| /*===================================================================*/
/* NRDF D1810 Data No.85 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,85;
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,85;
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(12C,N)X;
PHQ=ENGY-SPEC'48';
/* '48' Neutron energy spectrum */
THK-TGT=13395MG/CM**2;
INC-ENGY-LAB-RANGE=180MEV/A;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,85;
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=180MEV/A;
DELTA-DN/DOMEGA/DE=14%'49';
/* '49' 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 8.38677 9.29133 5.28382E-03
0 9.29133 10.30734 5.28993E-03
0 10.30734 11.3977 4.66465E-03
0 11.3977 12.6122 4.26557E-03
0 12.6122 13.9635 4.12843E-03
0 13.9635 15.4650 3.84053E-03
0 15.4650 17.1296 4.07549E-03
0 17.1296 18.9703 3.78342E-03
0 18.9703 20.9987 3.89310E-03
0 20.9987 23.2245 4.50983E-03
0 23.2245 25.8290 3.72076E-03
0 25.8290 28.6969 3.65286E-03
0 28.6969 31.8353 4.14522E-03
0 31.8353 35.2440 3.99451E-03
0 35.2440 39.2434 4.76013E-03
0 39.2434 43.5868 4.55109E-03
0 43.5868 48.2522 4.94721E-03
0 48.2522 53.7321 5.48075E-03
0 53.7321 59.5940 5.83038E-03
0 59.5940 66.5072 6.25282E-03
0 66.5072 73.8552 7.67379E-03
0 73.8552 82.5496 6.88665E-03
0 82.5496 91.7020 9.37928E-03
0 91.7020 102.5544 8.24853E-03
0 102.5544 113.814 9.75710E-03
0 113.814 127.167 7.37301E-03
0 127.167 140.723 9.58377E-03
0 140.723 156.758 8.41926E-03
0 156.758 175.966 6.76396E-03
0 175.966 195.091 7.54317E-03
0 195.091 217.882 6.02634E-03
0 217.882 245.449 3.99774E-03
0 245.449 271.996 3.27678E-03
0 271.996 303.784 2.23425E-03
0 303.784 342.495 1.00297E-03
0 342.495 390.626 4.79709E-04
0 390.626 435.170 3.90329E-04
0 435.170 489.653 1.55945E-04
7.5 7.89462 8.75258 5.48993E-03
7.5 8.75258 9.67887 6.02677E-03
7.5 9.67887 10.7145 5.04995E-03
7.5 10.7145 11.8723 4.44719E-03
7.5 11.8723 13.1661 3.89158E-03
7.5 13.1661 14.6106 4.31319E-03
7.5 14.6106 16.2215 4.38851E-03
7.5 16.2215 18.0145 4.88887E-03
7.5 18.0145 20.0052 4.26144E-03
7.5 20.0052 22.2087 4.46140E-03
7.5 22.2087 24.6376 4.23031E-03
7.5 24.6376 27.3013 4.31112E-03
7.5 27.3013 30.2041 4.41383E-03
7.5 30.2041 33.6049 4.39071E-03
7.5 33.6049 37.3156 5.06722E-03
7.5 37.3156 41.3279 5.61794E-03
7.5 41.3279 46.0411 5.00802E-03
7.5 46.0411 51.1284 5.44680E-03
7.5 51.1284 56.5460 5.54023E-03
7.5 56.5460 62.9038 5.72262E-03
7.5 62.9038 69.6258 6.10494E-03
7.5 69.6258 77.5340 5.49578E-03
7.5 77.5340 85.8069 6.02925E-03
7.5 85.8069 95.5502 6.48840E-03
7.5 95.5502 107.154 5.17096E-03
7.5 107.154 119.250 5.73135E-03
7.5 119.250 133.671 4.85739E-03
7.5 133.671 148.393 4.57702E-03
7.5 148.393 165.912 3.91277E-03
7.5 165.912 187.051 2.45564E-03
7.5 187.051 208.264 2.02560E-03
7.5 208.264 233.761 1.06411E-03
7.5 233.761 264.920 4.60504E-04
7.5 264.920 295.265 3.69685E-04
7.5 295.265 332.050 1.81454E-04
7.5 332.050 377.529 2.47058E-05
15 6.23671 6.90438 6.94774E-03
15 6.90438 7.65067 6.26621E-03
15 7.65067 8.48422 5.53625E-03
15 8.48422 9.41465 5.00360E-03
15 9.41465 10.45160 4.05950E-03
15 10.45160 11.6050 4.71505E-03
15 11.6050 12.8846 3.92522E-03
15 12.8846 14.2996 3.39597E-03
15 14.2996 15.8574 3.02919E-03
15 15.8574 17.5635 3.69805E-03
15 17.5635 19.4200 3.50637E-03
15 19.4200 21.5909 2.89884E-03
15 21.5909 23.9545 2.89997E-03
15 23.9545 26.5037 3.18982E-03
15 26.5037 29.4897 3.20044E-03
15 29.4897 32.7019 3.02224E-03
15 32.7019 36.4802 2.93155E-03
15 36.4802 40.5267 3.33567E-03
15 40.5267 45.3038 2.96718E-03
15 45.3038 50.3852 3.01923E-03
15 50.3852 56.4000 2.77232E-03
15 56.4000 62.7317 2.92958E-03
15 62.7317 70.2359 2.38612E-03
15 70.2359 78.0139 2.98968E-03
15 78.0139 87.2238 2.55106E-03
15 87.2238 96.5519 2.55572E-03
15 96.5519 107.552 2.42363E-03
15 107.552 120.674 1.79992E-03
15 120.674 133.671 2.06511E-03
15 133.671 149.062 1.58388E-03
15 149.062 167.522 1.27024E-03
15 167.522 190.001 6.56950E-04
15 190.001 211.787 6.60877E-04
15 211.787 238.033 4.28585E-04
15 238.033 270.197 1.95899E-04
15 270.197 299.473 1.51698E-04
15 299.473 334.610 4.04074E-05
15 334.610 377.529 2.01527E-05
30 3.11085 3.45023 4.33180E-03
30 3.45023 3.81537 6.54773E-03
30 3.81537 4.22262 7.13160E-03
30 4.22262 4.67669 8.30259E-03
30 4.67669 5.18217 8.28129E-03
30 5.18217 5.74411 7.81035E-03
30 5.74411 6.36753 7.24534E-03
30 6.36753 7.05693 6.55711E-03
30 7.05693 7.81677 5.62208E-03
30 7.81677 8.65055 5.41077E-03
30 8.65055 9.62578 4.32162E-03
30 9.62578 10.6989 3.90107E-03
30 10.6989 11.8723 3.50246E-03
30 11.8723 13.1449 3.44992E-03
30 13.1449 14.6355 3.03551E-03
30 14.6355 16.2506 2.92255E-03
30 16.2506 17.9804 3.12857E-03
30 17.9804 20.0052 2.73747E-03
30 20.0052 22.1620 2.63170E-03
30 22.1620 24.6924 2.27799E-03
30 24.6924 27.3654 2.37375E-03
30 27.3654 30.5049 2.00695E-03
30 30.5049 33.7812 2.15616E-03
30 33.7812 37.6268 2.05182E-03
30 37.6268 42.1846 1.64293E-03
30 42.1846 46.9066 1.78802E-03
30 46.9066 52.4923 1.38210E-03
30 52.4923 58.1409 1.50071E-03
30 58.1409 64.7869 1.42686E-03
30 64.7869 72.6891 1.07779E-03
30 72.6891 80.4841 1.19959E-03
30 80.4841 89.6682 9.67537E-04
30 89.6682 100.6094 8.77157E-04
30 100.6094 113.814 5.60409E-04
30 113.814 126.476 6.32545E-04
30 126.476 141.544 4.52198E-04
30 141.544 159.716 3.96226E-04
30 159.716 181.987 1.99301E-04
30 181.987 202.234 2.32411E-04
30 202.234 226.474 1.62861E-04
30 226.474 255.957 8.24644E-05
30 255.957 292.515 5.21407E-05
30 292.515 338.951 2.90530E-05
30 338.951 377.529 1.76675E-05
60 2.77842 3.08744 2.49059E-03
60 3.08744 3.42939 3.54876E-03
60 3.42939 3.80596 5.18314E-03
60 3.80596 4.21836 5.28867E-03
60 4.21836 4.66706 6.08453E-03
60 4.66706 5.19169 5.23598E-03
60 5.19169 5.76248 4.54718E-03
60 5.76248 6.37750 4.79582E-03
60 6.37750 7.09703 3.59367E-03
60 7.09703 7.86964 3.39817E-03
60 7.86964 8.77622 2.63488E-03
60 8.77622 9.74440 2.36763E-03
60 9.74440 10.8830 1.83644E-03
60 10.8830 12.0888 1.84637E-03
60 12.0888 13.5082 1.51245E-03
60 13.5082 14.9927 1.37030E-03
60 14.9927 16.7383 1.19005E-03
60 16.7383 18.5314 1.32947E-03
60 18.5314 20.6321 1.14079E-03
60 20.6321 23.1163 9.32938E-04
60 23.1163 25.6264 1.02360E-03
60 25.6264 28.5755 8.60554E-04
60 28.5755 32.0742 6.73782E-04
60 32.0742 35.5151 7.42617E-04
60 35.5151 39.5539 6.07870E-04
60 39.5539 44.3408 5.37953E-04
60 44.3408 50.0778 3.86929E-04
60 50.0778 55.5346 4.51996E-04
60 55.5346 61.9666 3.65171E-04
60 61.9666 69.6293 3.03943E-04
60 69.6293 78.8720 2.35175E-04
60 78.8720 90.1826 1.30275E-04
60 90.1826 100.4335 1.45828E-04
60 100.4335 112.649 9.78790E-05
60 112.649 127.400 6.49138E-05
60 127.400 145.491 4.15127E-05
60 145.491 168.103 1.35711E-05
60 168.103 186.538 1.31272E-05
60 186.538 208.527 1.26552E-05
90 2.72297 3.01072 1.51324E-03
90 3.01072 3.34685 2.17843E-03
90 3.34685 3.71871 3.31022E-03
90 3.71871 4.12876 3.84958E-03
90 4.12876 4.57801 4.05251E-03
90 4.57801 5.06714 4.36755E-03
90 5.06714 5.63938 3.58801E-03
90 5.63938 6.26247 3.35451E-03
90 6.26247 6.93450 3.14780E-03
90 6.93450 7.72112 2.33097E-03
90 7.72112 8.56677 2.12295E-03
90 8.56677 9.56003 1.65649E-03
90 9.56003 10.6220 1.52652E-03
90 10.6220 11.8723 1.14288E-03
90 11.8723 13.1979 1.06921E-03
90 13.1979 14.7606 7.92111E-04
90 14.7606 16.3972 8.11969E-04
90 16.3972 18.3248 6.88594E-04
90 18.3248 20.3079 6.49655E-04
90 20.3079 22.6356 6.10679E-04
90 22.6356 25.3936 4.94865E-04
90 25.3936 28.1863 4.84152E-04
90 28.1863 31.4746 4.09175E-04
90 31.4746 35.3860 2.78329E-04
90 35.3860 39.2434 2.71304E-04
90 39.2434 43.7836 2.12751E-04
90 43.7836 49.1828 1.83224E-04
90 49.1828 55.6784 1.25229E-04
90 55.6784 61.8817 1.19421E-04
90 61.8817 69.2237 8.48558E-05
90 69.2237 78.0139 5.60925E-05
90 78.0139 88.6777 3.10007E-05
90 88.6777 98.2588 2.42099E-05
90 98.2588 109.577 1.76160E-05
90 109.577 123.108 1.41853E-05
\END;
/*===================================================================*/
|