|
| /*===================================================================*/
/* NRDF D1759 Data No.6 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,6;
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,6;
/* 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=27AL(20NE,N)X;
PHQ=ENGY-SPEC;
THK-TGT=8100MG/CM**2;
INC-ENGY-LAB-RANGE=180MEV/A;
ANL=(INCASC'30',X'31');
/* '30' HIC calculation [Bertini, H. W.: ORNL-TM-4134, (1974).]
/* '31' Phenomenological Hybrid analysis by the moving source
model */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,6;
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 9.66544 3.29714E-03
0 10.7017 4.53515E-03
0 11.8532 3.68375E-03
0 13.1265 4.32988E-03
0 14.5341 4.63041E-03
0 16.1155 4.34906E-03
0 17.8514 5.23848E-03
0 19.7527 5.33487E-03
0 21.8718 5.79282E-03
0 24.2309 6.37214E-03
0 26.8531 6.35845E-03
0 29.7615 7.03774E-03
0 32.9785 7.88331E-03
0 36.5241 8.21306E-03
0 40.4142 9.54247E-03
0 44.8297 9.17896E-03
0 49.8285 9.71095E-03
0 55.297 1.14593E-02
0 61.2317 1.27642E-02
0 67.9339 1.33313E-02
0 75.4614 1.57391E-02
0 83.9862 1.54014E-02
0 93.5768 1.58588E-02
0 103.823 1.91705E-02
0 115.32 1.77945E-02
0 128.084 1.89341E-02
0 142.368 1.63774E-02
0 158.139 1.55886E-02
0 175.686 1.09715E-02
0 196.647 6.07386E-03
0 219.883 4.19234E-03
0 245.88 1.63742E-03
0 274.315 7.86836E-04
0 305.65 4.73353E-04
0 343.665 1.92082E-04
0 384.984 1.01191E-04
0 430.209 4.78215E-05
0 485.882 1.78915E-05
7.5 6.38293 3.39975E-03
7.5 7.06572 2.98659E-03
7.5 7.82114 3.83243E-03
7.5 8.65698 2.95497E-03
7.5 9.59661 3.32436E-03
7.5 10.6297 3.00989E-03
7.5 11.7637 3.49405E-03
7.5 13.0296 3.31812E-03
7.5 14.4417 3.41547E-03
7.5 16.0153 3.86827E-03
7.5 17.7659 3.83052E-03
7.5 19.709 3.98718E-03
7.5 21.8595 4.32314E-03
7.5 24.2309 4.53330E-03
7.5 26.8335 4.85858E-03
7.5 29.788 4.87858E-03
7.5 33.1324 4.82983E-03
7.5 36.7897 4.98935E-03
7.5 40.7561 5.65557E-03
7.5 45.2307 5.68957E-03
7.5 50.2493 6.11115E-03
7.5 55.9211 5.98289E-03
7.5 62.2862 5.96965E-03
7.5 69.0648 6.96243E-03
7.5 76.641 6.06434E-03
7.5 85.0142 7.21307E-03
7.5 94.33 7.17186E-03
7.5 105.36 6.71329E-03
7.5 117.595 7.05530E-03
7.5 131.275 5.32686E-03
7.5 146.298 5.18273E-03
7.5 162.905 3.79953E-03
7.5 182.803 1.96753E-03
7.5 204.585 1.30153E-03
7.5 228.593 7.49516E-04
7.5 257.692 2.52531E-04
7.5 289.262 1.55989E-04
7.5 323.698 8.27852E-05
7.5 365.874 1.69480E-05
15 3.44183 4.32639E-03
15 3.80994 4.73239E-03
15 4.22145 5.25818E-03
15 4.67462 5.11650E-03
15 5.17142 5.35565E-03
15 5.72344 5.13553E-03
15 6.33392 4.82269E-03
15 7.00905 4.13762E-03
15 7.7676 3.96816E-03
15 8.6011 3.84575E-03
15 9.51534 3.65582E-03
15 10.5353 3.69913E-03
15 11.6721 3.65619E-03
15 12.9378 3.56328E-03
15 14.3443 3.42058E-03
15 15.9038 3.60501E-03
15 17.6276 3.89493E-03
15 19.5258 4.34901E-03
15 21.606 4.30107E-03
15 23.9634 4.59532E-03
15 26.6267 3.78343E-03
15 29.5329 4.61753E-03
15 32.825 4.28140E-03
15 36.5363 3.93338E-03
15 40.5482 4.64412E-03
15 45.0709 3.84083E-03
15 50.132 3.99598E-03
15 55.8384 3.72404E-03
15 62.2144 4.15826E-03
15 69.3933 3.51195E-03
15 77.3861 3.35150E-03
15 86.3518 2.91136E-03
15 96.2673 3.13214E-03
15 107.31 2.22146E-03
15 119.386 2.19210E-03
15 132.666 1.69119E-03
15 148.482 1.26028E-03
15 165.678 1.17934E-03
15 184.47 8.05856E-04
15 207.022 4.36356E-04
15 231.221 3.04989E-04
15 257.255 1.82105E-04
15 288.639 9.06504E-05
15 327.163 2.42738E-05
15 368.105 1.50991E-05
15 411.613 1.06380E-05
30 3.60939 2.02531E-03
30 3.99559 2.26099E-03
30 4.42283 3.08461E-03
30 4.89538 3.46910E-03
30 5.4264 3.57867E-03
30 6.01006 4.12353E-03
30 6.65029 3.76424E-03
30 7.36455 3.74672E-03
30 8.16075 3.52248E-03
30 9.04705 3.15470E-03
30 10.032 2.94164E-03
30 11.1239 2.94959E-03
30 12.3305 2.79696E-03
30 13.6586 2.84428E-03
30 15.1135 2.92873E-03
30 16.7611 2.83456E-03
30 18.6213 2.66333E-03
30 20.6493 2.90085E-03
30 22.9439 2.55404E-03
30 25.5271 2.39468E-03
30 28.3151 2.51262E-03
30 31.4518 2.19836E-03
30 34.9541 2.24755E-03
30 38.8922 1.80615E-03
30 43.2789 1.93007E-03
30 48.1993 1.49977E-03
30 53.6546 1.55609E-03
30 59.7426 1.28326E-03
30 66.4387 1.32017E-03
30 73.8456 1.09063E-03
30 82.6244 8.27412E-04
30 92.2611 8.56652E-04
30 102.9 7.55547E-04
30 115.615 5.00740E-04
30 129.486 4.78038E-04
30 144.695 3.61992E-04
30 163 2.20209E-04
30 182.691 2.12022E-04
30 203.923 1.28319E-04
30 229.56 7.12626E-05
30 261.062 2.64087E-05
30 294.555 2.02730E-05
30 330.125 1.09889E-05
60 2.9233 1.44746E-03
60 3.24033 2.21474E-03
60 3.58957 2.97606E-03
60 3.97363 3.23552E-03
60 4.40311 3.36148E-03
60 4.88323 3.01108E-03
60 5.41952 2.56241E-03
60 6.01785 2.67730E-03
60 6.68417 2.16276E-03
60 7.42453 1.94130E-03
60 8.24469 1.65255E-03
60 9.14959 1.71029E-03
60 10.1432 1.35592E-03
60 11.2276 1.30455E-03
60 12.4533 1.19740E-03
60 13.8328 1.07278E-03
60 15.3267 1.18915E-03
60 17.0087 1.03544E-03
60 18.8904 1.10630E-03
60 21.0102 9.92569E-04
60 23.3795 1.00038E-03
60 26.0462 8.14008E-04
60 29.0191 7.53956E-04
60 32.3557 6.82158E-04
60 36.0566 6.30148E-04
60 40.1872 5.19467E-04
60 44.7295 4.79764E-04
60 49.7512 4.16919E-04
60 55.6972 3.19005E-04
60 62.2144 2.91639E-04
60 69.3933 2.82648E-04
60 77.9487 1.66081E-04
60 87.2484 1.73450E-04
60 97.3944 1.28739E-04
60 109.533 7.31208E-05
60 122.501 7.05114E-05
60 136.358 3.92579E-05
60 152.913 2.73873E-05
60 172.979 1.45636E-05
60 193.993 1.27780E-05
90 2.86029 1.79374E-03
90 3.16685 2.58586E-03
90 3.51144 2.77624E-03
90 3.89024 2.61232E-03
90 4.30589 2.45682E-03
90 4.76977 2.09391E-03
90 5.28695 1.87519E-03
90 5.86278 1.83282E-03
90 6.50272 1.43154E-03
90 7.21222 1.31547E-03
90 7.99637 1.11640E-03
90 8.85949 9.63064E-04
90 9.80476 9.40997E-04
90 10.8751 7.44209E-04
90 12.0832 6.88787E-04
90 13.3996 7.78867E-04
90 14.8882 5.83780E-04
90 16.563 5.98462E-04
90 18.3685 5.53301E-04
90 20.3976 4.39745E-04
90 22.6601 4.42857E-04
90 25.1995 3.70542E-04
90 28.0226 3.07534E-04
90 31.1812 2.32926E-04
90 34.6733 2.50559E-04
90 38.5571 1.61938E-04
90 42.8127 1.65836E-04
90 47.498 1.36813E-04
90 53.0215 9.28363E-05
90 59.0481 9.25164E-05
90 65.6518 7.68699E-05
90 73.4773 3.98437E-05
90 81.934 3.82052E-05
90 91.0979 3.16409E-05
90 101.982 1.71337E-05
90 115.072 1.45683E-05
90 129.133 1.20865E-05
90 144.255 1.16732E-05
\END;
/*===================================================================*/
|