|
| /*===================================================================*/
/* NRDF D1759 Data No.5 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,5;
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,5;
/* 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=C(20NE,N)X;
PHQ=ENGY-SPEC;
THK-TGT=7080MG/CM**2;
INC-ENGY-LAB-RANGE=180MEV/A;
ANL=(INCASC'28',X'29');
/* '28' HIC calculation [Bertini, H. W.: ORNL-TM-4134, (1974).]
/* '29' Phenomenological Hybrid analysis by the moving source
model */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,5;
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 9.93341 3.75327E-03
0 10.9971 3.80217E-03
0 12.1746 3.58326E-03
0 13.4782 4.39047E-03
0 14.9446 4.03387E-03
0 16.5583 5.20834E-03
0 18.3313 5.46007E-03
0 20.3128 6.69861E-03
0 22.5262 7.09809E-03
0 24.9962 7.75945E-03
0 27.7491 7.85441E-03
0 30.8109 8.32838E-03
0 34.2075 9.37480E-03
0 37.9627 1.08259E-02
0 42.0966 1.14219E-02
0 46.6227 1.30149E-02
0 51.7587 1.35718E-02
0 57.5671 1.55275E-02
0 63.8939 1.81885E-02
0 71.0681 1.81073E-02
0 79.1603 2.03356E-02
0 87.8773 2.32688E-02
0 97.7066 2.24848E-02
0 108.697 2.69365E-02
0 121.092 2.35888E-02
0 134.924 2.44979E-02
0 150.496 2.01521E-02
0 167.797 1.74497E-02
0 187.187 1.08346E-02
0 208.55 6.78431E-03
0 232.276 3.41580E-03
0 260.876 1.19373E-03
0 292.418 6.21313E-04
0 327.529 2.40878E-04
0 365.407 1.91815E-04
0 406.485 6.14867E-05
7.5 7.06572 2.92571E-03
7.5 7.82114 2.96669E-03
7.5 8.65698 2.81221E-03
7.5 9.59661 3.12448E-03
7.5 10.6297 3.36683E-03
7.5 11.7637 3.37718E-03
7.5 13.0296 3.32082E-03
7.5 14.4417 3.67841E-03
7.5 16.0153 3.78436E-03
7.5 17.7659 4.63219E-03
7.5 19.709 4.22402E-03
7.5 21.8595 4.79118E-03
7.5 24.2309 4.86755E-03
7.5 26.8335 5.59781E-03
7.5 29.788 5.72922E-03
7.5 33.1324 6.08907E-03
7.5 36.7897 6.31529E-03
7.5 40.7561 6.94615E-03
7.5 45.2307 6.93260E-03
7.5 50.2493 7.67507E-03
7.5 55.9211 7.17101E-03
7.5 62.2862 8.00814E-03
7.5 69.0648 9.26585E-03
7.5 76.641 8.41343E-03
7.5 85.0142 9.75867E-03
7.5 94.33 9.69511E-03
7.5 105.36 8.49385E-03
7.5 117.595 9.27700E-03
7.5 131.275 6.89184E-03
7.5 146.298 6.88507E-03
7.5 162.905 4.61752E-03
7.5 182.803 2.52140E-03
7.5 204.585 1.85746E-03
7.5 228.593 8.09579E-04
7.5 257.692 3.17408E-04
7.5 289.262 1.54014E-04
7.5 323.698 6.26856E-05
7.5 365.874 2.85348E-05
7.5 410.617 2.19537E-05
15 3.18483 2.34077E-03
15 3.52516 3.29261E-03
15 3.90117 3.46648E-03
15 4.31525 3.88040E-03
15 4.77721 3.68193E-03
15 5.29093 3.90601E-03
15 5.86278 4.00669E-03
15 6.49634 3.66822E-03
15 7.19839 3.44695E-03
15 7.97157 3.44273E-03
15 8.82186 3.48778E-03
15 9.77267 3.26303E-03
15 10.8357 3.30790E-03
15 12.0231 3.56603E-03
15 13.3483 3.73476E-03
15 14.8247 3.94343E-03
15 16.4662 3.97383E-03
15 18.2858 4.72557E-03
15 20.2955 4.72881E-03
15 22.5047 4.74940E-03
15 24.9194 5.15502E-03
15 27.6533 4.54152E-03
15 30.7368 5.37630E-03
15 34.0845 5.20548E-03
15 37.865 4.72844E-03
15 42.1089 5.20953E-03
15 46.6547 5.02019E-03
15 51.7458 4.29618E-03
15 57.3954 5.33193E-03
15 63.7068 4.56255E-03
15 70.6774 4.55529E-03
15 78.4252 4.01956E-03
15 87.5862 3.63800E-03
15 97.7322 3.80440E-03
15 109.05 2.89317E-03
15 121.448 2.66933E-03
15 135.109 2.17159E-03
15 151.413 1.49331E-03
15 169.18 1.37641E-03
15 188.647 9.21647E-04
15 212.079 4.20427E-04
15 237.303 2.99227E-04
15 264.542 1.64252E-04
15 297.514 7.02441E-05
15 338.197 2.48299E-05
15 381.672 1.57181E-05
30 6.65029 3.78120E-03
30 7.36455 3.74956E-03
30 8.16075 3.70680E-03
30 9.04705 3.80568E-03
30 10.032 3.68028E-03
30 11.1239 3.62744E-03
30 12.3305 3.84009E-03
30 13.6586 3.80726E-03
30 15.1135 3.94162E-03
30 16.7611 3.70506E-03
30 18.6213 3.78039E-03
30 20.6493 4.03520E-03
30 22.9439 3.49956E-03
30 25.5271 3.28762E-03
30 28.3151 3.48054E-03
30 31.4518 2.98115E-03
30 34.9541 2.96957E-03
30 38.8922 2.55913E-03
30 43.2789 2.62018E-03
30 48.1993 1.98481E-03
30 53.6546 2.04886E-03
30 59.7426 1.67060E-03
30 66.4387 1.67760E-03
30 73.8456 1.48343E-03
30 82.6244 1.06949E-03
30 92.2611 1.11763E-03
30 102.9 9.50477E-04
30 115.615 6.62404E-04
30 129.486 6.03320E-04
30 144.695 4.49471E-04
30 163 2.87033E-04
30 182.691 2.20558E-04
30 203.923 1.52496E-04
30 229.56 8.65672E-05
30 261.062 3.56137E-05
30 294.555 2.91649E-05
30 330.125 1.38720E-05
60 3.24033 1.35579E-03
60 3.58957 2.09013E-03
60 3.97363 1.87011E-03
60 4.40311 2.17152E-03
60 4.88323 2.05550E-03
60 5.41952 1.75513E-03
60 6.01785 1.94132E-03
60 6.68417 1.52536E-03
60 7.42453 1.49265E-03
60 8.24469 1.28202E-03
60 9.14959 1.31973E-03
60 10.1432 1.15677E-03
60 11.2276 1.20173E-03
60 12.4533 1.06075E-03
60 13.8328 1.01351E-03
60 15.3267 1.11023E-03
60 17.0087 9.65749E-04
60 18.8904 1.09872E-03
60 21.0102 1.04869E-03
60 23.3795 9.97604E-04
60 26.0462 7.91200E-04
60 29.0191 8.12825E-04
60 32.3557 6.68202E-04
60 36.0566 6.81081E-04
60 40.1872 5.34380E-04
60 44.7295 4.97581E-04
60 49.7512 4.22445E-04
60 55.6972 3.43395E-04
60 62.2144 3.26058E-04
60 69.3933 2.85233E-04
60 77.9487 1.63084E-04
60 87.2484 1.58912E-04
60 97.3944 1.32992E-04
60 109.533 7.43877E-05
60 122.501 5.58501E-05
60 136.358 4.38391E-05
60 152.913 2.62762E-05
60 172.979 1.05960E-05
90 2.86029 1.07843E-03
90 3.16685 1.64119E-03
90 3.51144 1.82018E-03
90 3.89024 1.54874E-03
90 4.30589 1.51843E-03
90 4.76977 1.40463E-03
90 5.28695 1.19247E-03
90 5.86278 1.28347E-03
90 6.50272 1.05693E-03
90 7.21222 9.21364E-04
90 7.99637 8.56070E-04
90 8.85949 7.92340E-04
90 9.80476 7.82381E-04
90 10.8751 6.29734E-04
90 12.0832 6.22243E-04
90 13.3996 6.05840E-04
90 14.8882 5.51218E-04
90 16.563 5.53874E-04
90 18.3685 5.19756E-04
90 20.3976 3.97976E-04
90 22.6601 3.89372E-04
90 25.1995 3.22192E-04
90 28.0226 2.74045E-04
90 31.1812 2.42216E-04
90 34.6733 2.08287E-04
90 38.5571 1.51634E-04
90 42.8127 1.34858E-04
90 47.498 1.20784E-04
90 53.0215 7.73997E-05
90 59.0481 7.16957E-05
90 65.6518 5.93728E-05
90 73.4773 3.60008E-05
90 81.934 3.32967E-05
90 91.0979 2.41592E-05
90 101.982 1.80363E-05
\END;
/*===================================================================*/
|