|
| /*===================================================================*/
/* NRDF D1759 Data No.7 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,7;
D#=D1759;
TITLE=/ Measurements of secondary neutrons produced from thick
targets bombarded by high energy neon ions /;
PURPOSE=/ To perform a systematic study to measure the angular and
energy distributions of neutrons produced from thick C, Al,
Cu, and Pb targets bombarded by 100, 180 and 400 MeV/nucleon
Ne ions. /;
ATH=(T.KUROSAWA'1', N.NAKAO'2', T.NAKAMURA'1', Y.UWAMINO'3',
T.SHIBATA'2', A.FUKUMURA'4', K.MURAKAMI'4');
INST-ATH=(2JPNTOH'1', 2JPNKEK'2', 2JPNIPC'3', 2JPNIRS'4');
/* '1' Cyclotron and Radioisotope Center */
REF=NST;
VLP=36(1999)41;
RCTS=(C(20NE,N)X, 27AL(20NE,N)X, CU(20NE,N)X, PB(20NE,N)X);
PHQS=(ENGY-SPEC, N-MLT'5');
/* '5' Thick target differential multiplicity of neutron with
respect to angle integrated over partial angular range */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,7;
/* 2002-02-24 : Compiled+Checked, R.Suzuki + sK */
/* 2004-04-23 : Altered, N.Otuka. MLT in SF6 replaced by PY */
/* 2008-01-30 : Altered, N.Otuka. EDE added under METHOD */
/* 2009-08-23 : Altered, Nf. 014-017 corrected */
RTY=HEAVY-ION-RCT;
ENR=NAT'6';
/* '6' The enrichments of targets are not given in the reference.
But compiler asked T.Kurosawa. */
CHM=ELM;
PHYS-FORM=SLD;
BAC=X;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=SYN'7';
/* '7' Heavy Ion Medical Accelerator in Chiba (HIMAC) */
INST-ACC=2JPNIRS'8';
/* '8' The mass numbers of projectiles are not given in the
reference. But compiler asked NIRS staff. */
BEAM-INTNSTY=XMA'9';
/* '9' The beam intensities were kept to be 100,000-1,000,000
particles per pulse. */
POL-PRJ=0%;
DET-PARTCL=N;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(SCT'10',SCT'11',TOF'12',EDE'13');
/* '10' Plastic scintillator (NE102A) was used as the delta-E
counter and the beam pick-up counter. Liquid scintillator
(NE213) was used as the E counter. */
/* '11' Liquid scintillator */
/* '12' To measure the energy of neutron */
/* '13' To eliminate charged particles */
ERS-DET=XKEV'14';
/* '14' The neutron energy resolutions is represented as a
function of neutron energy at Fig. 2 in reference. */
CALB-DET=/ 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. for all energy ranges.
Reference: R. A. Cecil, B. D. Anderson, and R. Madey, Nucl.
Instrum. Methods 161, 439 (1979). /;
/* 2007-10-25 : Altered, N.Otuka. Superseded by data with new
analysis */
RCT=CU(20NE,N)X;
PHQ=ENGY-SPEC;
THK-TGT=8930MG/CM**2;
INC-ENGY-LAB-RANGE=180MEV/A;
ANL=(INCASC'32',X'33');
/* '32' HIC calculation [Bertini, H. W.: ORNL-TM-4134, (1974).]
/* '33' Phenomenological Hybrid analysis by the moving source
model */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,7;
SYS-ERR=(3%'15',10%'16',8%'17',14%'18');
/* '15' Notmalization uncertainty due to number of accepted beam
particles incident on target */
/* '16' Normalization uncertainty due to solid angle uncertainty
/* '17' Normalization uncertainty due to additional uncertainty
in the efficiencies at neutron energies near threshold (8% in
Table 2, but 7% in text) */
/* '18' Total normalization uncertainty */
STATIST-ERR=X%'19';
/* '19' The statistical uncertainties vary in a range of 2 to 5 %
for the low- to medium-energy (5-50 MeV) region of the spectra
and increase to about 30% at the highest energies. */
INC-ENGY-LAB=180MEV/A;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTL ENGY-EMT-LAB DN/DOMEGA/DE
(DEG) (MEV) (1/SR/MEV/PARTCL)
0 6.76117 6.46035E-03
0 7.4755 5.84845E-03
0 8.26889 5.52496E-03
0 9.14864 4.52660E-03
0 10.1219 4.68625E-03
0 11.1953 4.23227E-03
0 12.3952 4.65017E-03
0 13.7326 4.62158E-03
0 15.198 4.01206E-03
0 16.8259 4.89000E-03
0 18.6254 5.23493E-03
0 20.6142 5.48292E-03
0 22.8486 5.07583E-03
0 25.3011 4.81946E-03
0 27.9877 5.46340E-03
0 30.9826 5.45227E-03
0 34.3182 5.41635E-03
0 38.0279 6.29602E-03
0 42.1458 6.36636E-03
0 46.7053 6.76696E-03
0 51.737 7.15189E-03
0 57.2664 8.90062E-03
0 63.5551 8.24199E-03
0 70.6919 8.82130E-03
0 78.5217 9.95520E-03
0 87.0474 1.15806E-02
0 96.7154 1.08312E-02
0 107.625 1.12178E-02
0 119.386 1.14279E-02
0 132.666 1.01860E-02
0 147.545 1.11041E-02
0 164.37 7.68286E-03
0 183.21 6.82823E-03
0 204.52 4.25879E-03
0 228.327 2.82542E-03
0 255.202 1.33904E-03
0 285.054 7.67613E-04
0 318.561 3.08468E-04
0 355.36 1.98426E-04
0 396.143 1.29146E-04
0 445.991 5.27857E-05
0 500.661 2.58346E-05
0 561.231 1.11203E-05
7.5 3.66684 6.34587E-03
7.5 4.055 6.71766E-03
7.5 4.48796 6.93192E-03
7.5 4.97054 6.50532E-03
7.5 5.50044 7.24245E-03
7.5 6.08041 6.80336E-03
7.5 6.73004 5.82951E-03
7.5 7.45634 4.85947E-03
7.5 8.25639 4.35488E-03
7.5 9.13362 3.83935E-03
7.5 10.1085 3.42347E-03
7.5 11.1872 3.92810E-03
7.5 12.3807 3.83516E-03
7.5 13.7225 3.44297E-03
7.5 15.198 3.53037E-03
7.5 16.8178 3.93364E-03
7.5 18.6267 3.86909E-03
7.5 20.6455 3.90730E-03
7.5 22.8961 4.02342E-03
7.5 25.4016 3.85699E-03
7.5 28.185 3.46213E-03
7.5 31.2688 4.03715E-03
7.5 34.6733 4.29103E-03
7.5 38.4153 4.13092E-03
7.5 42.5053 4.66180E-03
7.5 47.1377 4.25060E-03
7.5 52.3661 4.54207E-03
7.5 58.0478 5.32135E-03
7.5 64.474 4.82206E-03
7.5 71.7023 5.21423E-03
7.5 79.4645 5.73977E-03
7.5 88.1865 5.40663E-03
7.5 97.9026 5.53500E-03
7.5 108.811 4.73213E-03
7.5 120.928 5.13749E-03
7.5 134.492 3.75729E-03
7.5 149.474 3.57964E-03
7.5 166.147 2.65335E-03
7.5 186.067 1.41336E-03
7.5 208.15 9.52048E-04
7.5 232.853 3.34010E-04
7.5 259.865 2.15311E-04
7.5 289.617 7.99924E-05
7.5 325.683 3.01408E-05
7.5 364.845 1.62060E-05
7.5 407.646 1.07400E-05
15 3.18483 3.80172E-03
15 3.52516 4.94898E-03
15 3.90117 6.16492E-03
15 4.31525 6.65135E-03
15 4.77721 6.23439E-03
15 5.29093 6.31268E-03
15 5.86278 5.84636E-03
15 6.49634 5.23279E-03
15 7.19839 4.59040E-03
15 7.97157 4.06849E-03
15 8.82186 3.84297E-03
15 9.77267 3.19878E-03
15 10.8357 3.16557E-03
15 12.0231 2.90102E-03
15 13.3483 3.00734E-03
15 14.8247 3.24009E-03
15 16.4662 3.14066E-03
15 18.2858 3.09598E-03
15 20.2955 3.17825E-03
15 22.5047 3.13961E-03
15 24.9194 3.10233E-03
15 27.6533 2.86681E-03
15 30.7368 2.67095E-03
15 34.0845 2.99323E-03
15 37.865 3.00594E-03
15 42.1089 2.83377E-03
15 46.6547 2.85075E-03
15 51.7458 2.56177E-03
15 57.3954 2.83638E-03
15 63.7068 2.60520E-03
15 70.6774 2.77504E-03
15 78.4252 2.63512E-03
15 87.5862 2.27641E-03
15 97.7322 2.51391E-03
15 109.05 1.79944E-03
15 121.448 1.89028E-03
15 135.109 1.34029E-03
15 151.413 9.96699E-04
15 169.18 9.23045E-04
15 188.647 5.98848E-04
15 212.079 2.74233E-04
15 237.303 2.36141E-04
15 264.542 1.28565E-04
15 297.514 5.85678E-05
15 338.197 1.87612E-05
15 381.672 1.07344E-05
30 3.52516 6.64912E-03
30 3.90117 6.49405E-03
30 4.31525 7.26274E-03
30 4.77721 7.03625E-03
30 5.29093 6.18222E-03
30 5.86278 6.13389E-03
30 6.49634 5.49034E-03
30 7.19839 4.62264E-03
30 7.97157 4.31186E-03
30 8.82186 3.92409E-03
30 9.77267 3.32593E-03
30 10.8357 3.02827E-03
30 12.0231 2.85517E-03
30 13.3483 2.68157E-03
30 14.8247 2.72118E-03
30 16.4662 2.47837E-03
30 18.2858 2.56961E-03
30 20.2955 2.30755E-03
30 22.5047 2.29411E-03
30 24.9194 2.24955E-03
30 27.6533 2.06218E-03
30 30.7368 1.98089E-03
30 34.0845 1.91572E-03
30 37.865 1.70627E-03
30 42.1089 1.55591E-03
30 46.6547 1.53636E-03
30 51.7458 1.27478E-03
30 57.3954 1.37141E-03
30 63.7068 1.07819E-03
30 70.6774 1.02336E-03
30 78.4252 9.00307E-04
30 87.5862 7.04996E-04
30 97.7322 6.93802E-04
30 109.05 4.63871E-04
30 121.448 4.37636E-04
30 135.109 3.53724E-04
30 151.413 2.50905E-04
30 169.18 2.15929E-04
30 188.647 1.46507E-04
30 212.079 7.09067E-05
30 237.303 5.44284E-05
30 264.542 3.36115E-05
30 297.514 1.56242E-05
60 3.24033 3.07329E-03
60 3.58957 4.73718E-03
60 3.97363 5.09079E-03
60 4.40311 4.82468E-03
60 4.88323 4.83202E-03
60 5.41952 4.17111E-03
60 6.01785 4.06671E-03
60 6.68417 3.41180E-03
60 7.42453 2.81883E-03
60 8.24469 2.45921E-03
60 9.14959 2.10300E-03
60 10.1432 1.79896E-03
60 11.2276 1.72409E-03
60 12.4533 1.47402E-03
60 13.8328 1.23421E-03
60 15.3267 1.29388E-03
60 17.0087 1.13638E-03
60 18.8904 1.22651E-03
60 21.0102 1.01286E-03
60 23.3795 1.01549E-03
60 26.0462 7.61690E-04
60 29.0191 8.03940E-04
60 32.3557 6.78965E-04
60 36.0566 6.79156E-04
60 40.1872 5.31217E-04
60 44.7295 4.66688E-04
60 49.7512 4.17153E-04
60 55.6972 3.05641E-04
60 62.2144 3.24131E-04
60 69.3933 2.60985E-04
60 77.9487 1.65133E-04
60 87.2484 1.66380E-04
60 97.3944 1.20609E-04
60 109.533 7.44009E-05
60 122.501 6.47774E-05
60 136.358 5.20843E-05
60 152.913 3.03247E-05
60 172.979 1.16628E-05
90 3.13101 3.95194E-03
90 3.46966 4.67891E-03
90 3.84152 4.44468E-03
90 4.24916 4.06843E-03
90 4.70357 3.77868E-03
90 5.20967 3.08122E-03
90 5.77261 3.13728E-03
90 6.39743 2.42299E-03
90 7.08924 2.01757E-03
90 7.85279 1.75615E-03
90 8.69205 1.57587E-03
90 9.64443 1.28219E-03
90 10.7226 1.06761E-03
90 11.9045 8.96089E-04
90 13.1907 8.13864E-04
90 14.6433 7.53844E-04
90 16.2754 6.36903E-04
90 18.0326 6.27635E-04
90 20.0041 5.85699E-04
90 22.199 4.87131E-04
90 24.6581 3.86785E-04
90 27.387 3.46619E-04
90 30.4339 2.84398E-04
90 33.7958 2.77956E-04
90 37.526 2.34265E-04
90 41.9254 1.67061E-04
90 46.7817 1.49667E-04
90 52.1736 1.08437E-04
90 58.0478 1.11154E-04
90 64.474 7.69175E-05
90 72.0754 5.39750E-05
90 80.2746 4.50249E-05
90 89.1405 3.90519E-05
90 99.6467 2.44245E-05
90 112.249 1.19200E-05
90 125.748 1.46769E-05
90 140.217 1.11205E-05
\END;
/*===================================================================*/
|