|
| /*===================================================================*/
/* NRDF D1759 Data No.8 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,8;
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,8;
/* 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=PB(20NE,N)X;
PHQ=ENGY-SPEC;
THK-TGT=11340MG/CM**2;
INC-ENGY-LAB-RANGE=180MEV/A;
ANL=(INCASC'34',X'35');
/* '34' HIC calculation [Bertini, H. W.: ORNL-TM-4134, (1974).]
/* '35' Phenomenological Hybrid analysis by the moving source
model */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,8;
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 8.26889 8.55806E-03
0 9.14864 7.96100E-03
0 10.1219 6.92935E-03
0 11.1953 6.93686E-03
0 12.3952 6.90412E-03
0 13.7326 6.59588E-03
0 15.198 5.67446E-03
0 16.8259 5.40419E-03
0 18.6254 5.64356E-03
0 20.6142 5.13683E-03
0 22.8486 4.55733E-03
0 25.3011 4.99371E-03
0 27.9877 5.16281E-03
0 30.9826 4.57342E-03
0 34.3182 4.82907E-03
0 38.0279 5.06416E-03
0 42.1458 4.96004E-03
0 46.7053 4.80381E-03
0 51.737 5.54163E-03
0 57.2664 5.74801E-03
0 63.5551 5.81886E-03
0 70.6919 6.58542E-03
0 78.5217 5.99465E-03
0 87.0474 7.28793E-03
0 96.7154 7.21297E-03
0 107.625 7.11263E-03
0 119.386 7.84955E-03
0 132.666 6.44857E-03
0 147.545 7.49834E-03
0 164.37 5.29562E-03
0 183.21 4.45580E-03
0 204.52 2.93101E-03
0 228.327 2.13447E-03
0 255.202 1.08057E-03
0 285.054 4.55712E-04
0 318.561 1.86300E-04
0 355.36 1.47127E-04
0 396.143 2.75868E-05
0 445.991 1.19019E-05
7.5 6.08041 1.35197E-02
7.5 6.73004 9.61777E-03
7.5 7.45634 9.52608E-03
7.5 8.25639 8.20771E-03
7.5 9.13362 7.40709E-03
7.5 10.1085 6.26748E-03
7.5 11.1872 5.36831E-03
7.5 12.3807 5.12482E-03
7.5 13.7225 4.57694E-03
7.5 15.198 4.51288E-03
7.5 16.8178 4.40260E-03
7.5 18.6267 4.12749E-03
7.5 20.6455 4.89714E-03
7.5 22.8961 3.79772E-03
7.5 25.4016 4.24925E-03
7.5 28.185 3.72550E-03
7.5 31.2688 3.57236E-03
7.5 34.6733 3.77226E-03
7.5 38.4153 3.86629E-03
7.5 42.5053 4.27432E-03
7.5 47.1377 3.52779E-03
7.5 52.3661 3.85965E-03
7.5 58.0478 4.09987E-03
7.5 64.474 3.59519E-03
7.5 71.7023 3.66555E-03
7.5 79.4645 3.94629E-03
7.5 88.1865 3.53980E-03
7.5 97.9026 4.00333E-03
7.5 108.811 3.47828E-03
7.5 120.928 3.57728E-03
7.5 134.492 2.86714E-03
7.5 149.474 2.68124E-03
7.5 166.147 1.86114E-03
7.5 186.067 1.05271E-03
7.5 208.15 6.38508E-04
7.5 232.853 2.57466E-04
7.5 259.865 1.55390E-04
7.5 289.617 1.14356E-04
7.5 325.683 1.51609E-05
15 3.52516 1.20627E-02
15 3.90117 1.25891E-02
15 4.31525 1.37983E-02
15 4.77721 1.32347E-02
15 5.29093 1.22037E-02
15 5.86278 1.21826E-02
15 6.49634 1.08647E-02
15 7.19839 8.47027E-03
15 7.97157 7.71319E-03
15 8.82186 6.78841E-03
15 9.77267 5.44748E-03
15 10.8357 4.94695E-03
15 12.0231 4.32351E-03
15 13.3483 3.99179E-03
15 14.8247 3.91261E-03
15 16.4662 3.60391E-03
15 18.2858 3.58727E-03
15 20.2955 3.59632E-03
15 22.5047 3.19482E-03
15 24.9194 3.25966E-03
15 27.6533 2.90550E-03
15 30.7368 2.85141E-03
15 34.0845 3.06166E-03
15 37.865 2.75893E-03
15 42.1089 2.32642E-03
15 46.6547 2.62550E-03
15 51.7458 2.29265E-03
15 57.3954 2.39570E-03
15 63.7068 2.19793E-03
15 70.6774 2.24951E-03
15 78.4252 2.22976E-03
15 87.5862 1.84198E-03
15 97.7322 1.89734E-03
15 109.05 1.31101E-03
15 121.448 1.44767E-03
15 135.109 1.09988E-03
15 151.413 7.31154E-04
15 169.18 7.17331E-04
15 188.647 3.84001E-04
15 212.079 1.95549E-04
15 237.303 1.37143E-04
15 264.542 9.57261E-05
15 297.514 2.83453E-05
30 3.18483 9.62631E-03
30 3.52516 1.35647E-02
30 3.90117 1.49277E-02
30 4.31525 1.60749E-02
30 4.77721 1.44664E-02
30 5.29093 1.30130E-02
30 5.86278 1.26384E-02
30 6.49634 1.04091E-02
30 7.19839 8.63153E-03
30 7.97157 8.05042E-03
30 8.82186 7.04875E-03
30 9.77267 5.79319E-03
30 10.8357 5.01111E-03
30 12.0231 4.41761E-03
30 13.3483 3.81525E-03
30 14.8247 3.55093E-03
30 16.4662 3.22950E-03
30 18.2858 3.22361E-03
30 20.2955 2.89462E-03
30 22.5047 2.80103E-03
30 24.9194 2.45835E-03
30 27.6533 2.17201E-03
30 30.7368 2.14938E-03
30 34.0845 1.96981E-03
30 37.865 1.70662E-03
30 42.1089 1.47560E-03
30 46.6547 1.51638E-03
30 51.7458 1.24156E-03
30 57.3954 1.25394E-03
30 63.7068 1.01000E-03
30 70.6774 9.92018E-04
30 78.4252 8.06628E-04
30 87.5862 6.31686E-04
30 97.7322 6.01248E-04
30 109.05 4.19814E-04
30 121.448 3.87820E-04
30 135.109 2.77297E-04
30 151.413 1.82939E-04
30 169.18 1.76920E-04
30 188.647 1.15261E-04
30 212.079 5.65327E-05
30 237.303 3.84836E-05
30 264.542 3.18160E-05
30 297.514 1.06052E-05
60 3.46966 9.59820E-03
60 3.84152 1.09800E-02
60 4.24916 1.15454E-02
60 4.70357 1.16329E-02
60 5.20967 9.97567E-03
60 5.77261 9.52177E-03
60 6.39743 7.79835E-03
60 7.08924 6.52126E-03
60 7.85279 5.56957E-03
60 8.69205 4.86978E-03
60 9.64443 4.03368E-03
60 10.7226 2.99486E-03
60 11.9045 2.66365E-03
60 13.1907 2.39576E-03
60 14.6433 2.02386E-03
60 16.2754 1.75291E-03
60 18.0326 1.76405E-03
60 20.0041 1.51497E-03
60 22.199 1.41998E-03
60 24.6581 1.16164E-03
60 27.387 1.05465E-03
60 30.4339 8.26133E-04
60 33.7958 8.74359E-04
60 37.526 7.35460E-04
60 41.9254 5.34010E-04
60 46.7817 5.44694E-04
60 52.1736 3.96818E-04
60 58.0478 3.70140E-04
60 64.474 3.31350E-04
60 72.0754 2.22480E-04
60 80.2746 2.06297E-04
60 89.1405 1.55138E-04
60 99.6467 1.39551E-04
60 112.249 7.35776E-05
60 125.748 6.62266E-05
60 140.217 4.04492E-05
60 157.562 3.01430E-05
60 178.67 1.29178E-05
90 3.13101 1.01186E-02
90 3.46966 1.20612E-02
90 3.84152 1.12495E-02
90 4.24916 1.00623E-02
90 4.70357 9.38698E-03
90 5.20967 7.61681E-03
90 5.77261 7.28066E-03
90 6.39743 5.78120E-03
90 7.08924 4.71822E-03
90 7.85279 4.05296E-03
90 8.69205 3.54210E-03
90 9.64443 2.70937E-03
90 10.7226 2.18783E-03
90 11.9045 1.84276E-03
90 13.1907 1.58743E-03
90 14.6433 1.35034E-03
90 16.2754 1.14922E-03
90 18.0326 9.92650E-04
90 20.0041 7.90041E-04
90 22.199 6.71198E-04
90 24.6581 5.52946E-04
90 27.387 4.83349E-04
90 30.4339 3.89022E-04
90 33.7958 3.67176E-04
90 37.526 3.15392E-04
90 41.9254 2.16955E-04
90 46.7817 1.81078E-04
90 52.1736 1.33444E-04
90 58.0478 1.30677E-04
90 64.474 9.95788E-05
90 72.0754 6.90756E-05
90 80.2746 6.99943E-05
90 89.1405 4.62150E-05
90 99.6467 3.68189E-05
90 112.249 2.19884E-05
90 125.748 1.94267E-05
90 140.217 1.02868E-05
\END;
/*===================================================================*/
|