|
| /*===================================================================*/
/* NRDF D1759 Data No.10 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,10;
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,10;
/* 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=21600MG/CM**2;
INC-ENGY-LAB-RANGE=400MEV/A;
ANL=(INCASC'38',X'39');
/* '38' HIC calculation [Bertini, H. W.: ORNL-TM-4134, (1974).]
/* '39' Phenomenological Hybrid analysis by the moving source
model */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,10;
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=400MEV/A;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTL ENGY-EMT-LAB DN/DOMEGA/DE
(DEG) (MEV) (1/SR/MEV/PARTCL)
0 6.17863 8.20007E-03
0 6.84031 7.69420E-03
0 7.57574 7.65106E-03
0 8.39159 7.37152E-03
0 9.29441 6.73587E-03
0 10.2902 7.06672E-03
0 11.3842 7.06282E-03
0 12.6024 5.59128E-03
0 13.9533 6.10378E-03
0 15.4523 6.95107E-03
0 17.1063 6.86538E-03
0 18.9305 6.74539E-03
0 20.9757 6.25021E-03
0 23.2696 6.29142E-03
0 25.776 5.13394E-03
0 28.5057 5.66800E-03
0 31.5324 5.50029E-03
0 34.8812 5.88344E-03
0 38.576 6.46882E-03
0 42.7816 6.16621E-03
0 47.5631 5.92018E-03
0 52.8459 6.58204E-03
0 58.6529 7.39163E-03
0 64.9957 9.25070E-03
0 72.1921 1.03291E-02
0 80.3241 1.06981E-02
0 89.1423 1.46111E-02
0 99.1253 1.42311E-02
0 110.355 1.70356E-02
0 122.352 2.06367E-02
0 135.82 2.12314E-02
0 150.781 2.75106E-02
0 167.541 2.56558E-02
0 186.072 3.27023E-02
0 206.728 3.21918E-02
0 231.468 2.81866E-02
0 258.981 3.13302E-02
0 289.894 2.43701E-02
0 323.87 2.41786E-02
0 361.548 1.72105E-02
0 407.611 7.07589E-03
0 458.125 3.80803E-03
0 514.062 1.46148E-03
0 583.901 4.01508E-04
0 659.651 2.72621E-04
0 742.467 6.34997E-05
0 848.082 2.45391E-05
7.5 6.49685 8.80132E-03
7.5 7.19391 8.22274E-03
7.5 7.96798 7.09561E-03
7.5 8.82567 6.15247E-03
7.5 9.77323 7.03765E-03
7.5 10.8164 5.28771E-03
7.5 11.9804 6.02526E-03
7.5 13.2745 6.40594E-03
7.5 14.6861 5.75932E-03
7.5 16.2476 6.58941E-03
7.5 18.0028 6.56428E-03
7.5 19.9326 7.25611E-03
7.5 22.0512 6.35802E-03
7.5 24.4171 5.86882E-03
7.5 27.0579 5.87522E-03
7.5 30.0028 5.54801E-03
7.5 33.2823 5.58130E-03
7.5 36.9275 5.47385E-03
7.5 40.9686 5.31850E-03
7.5 45.4342 5.08385E-03
7.5 50.3475 5.36516E-03
7.5 55.725 6.19813E-03
7.5 61.8257 6.13184E-03
7.5 68.7244 5.18911E-03
7.5 76.239 5.93224E-03
7.5 84.7622 5.44053E-03
7.5 94.3804 5.38618E-03
7.5 104.748 6.53196E-03
7.5 116.452 5.92899E-03
7.5 129.555 6.37005E-03
7.5 144.36 5.38786E-03
7.5 160.918 6.55497E-03
7.5 179.613 5.69964E-03
7.5 200.455 6.24679E-03
7.5 223.916 5.30655E-03
7.5 249.893 6.01721E-03
7.5 278.923 3.96346E-03
7.5 310.654 4.15544E-03
7.5 345.606 3.39848E-03
7.5 388.008 1.49831E-03
7.5 434.115 1.18986E-03
7.5 484.634 4.81418E-04
7.5 546.93 2.83977E-04
7.5 613.595 1.83921E-04
7.5 685.215 1.05249E-04
7.5 774.691 4.36905E-05
7.5 890.173 2.22127E-05
15 9.14152 7.07495E-03
15 10.1317 5.74285E-03
15 11.2253 6.60176E-03
15 12.4322 7.12997E-03
15 13.7862 6.44800E-03
15 15.2681 6.18280E-03
15 16.8853 6.30261E-03
15 18.6817 7.36092E-03
15 20.6732 6.30438E-03
15 22.876 5.97373E-03
15 25.3052 4.62141E-03
15 28.068 4.62241E-03
15 31.2058 3.58113E-03
15 34.6677 4.09345E-03
15 38.4666 3.13231E-03
15 42.6069 3.58752E-03
15 47.2919 3.17413E-03
15 52.5692 2.68107E-03
15 58.2699 2.95834E-03
15 64.6934 2.99034E-03
15 71.8807 2.88750E-03
15 79.9855 2.73390E-03
15 89.0466 2.92385E-03
15 99.2595 2.47787E-03
15 110.647 2.64881E-03
15 123.451 2.41451E-03
15 137.651 2.86122E-03
15 153.528 2.51171E-03
15 170.97 2.69611E-03
15 190.266 2.68648E-03
15 213.413 2.03132E-03
15 238.797 2.35194E-03
15 266.841 1.82094E-03
15 300.944 1.33380E-03
15 338.087 1.15759E-03
15 378.82 8.89652E-04
15 429.043 4.36162E-04
15 482.724 2.94556E-04
15 540.241 1.80353E-04
15 611.793 8.06222E-05
15 703.489 4.02138E-05
15 799.646 2.14431E-05
30 3.01313 1.13124E-02
30 3.33312 1.54307E-02
30 3.69054 1.94000E-02
30 4.08956 1.60714E-02
30 4.53467 1.46917E-02
30 5.03052 1.28381E-02
30 5.58193 1.20972E-02
30 6.19359 1.11975E-02
30 6.86988 8.98677E-03
30 7.61472 8.56774E-03
30 8.43096 7.61518E-03
30 9.35573 6.62932E-03
30 10.4001 5.86033E-03
30 11.5389 6.28208E-03
30 12.8273 5.43457E-03
30 14.2777 5.57845E-03
30 15.8423 5.77840E-03
30 17.6018 5.33900E-03
30 19.5648 5.79247E-03
30 21.7694 5.00846E-03
30 24.2214 5.13558E-03
30 26.9665 4.00057E-03
30 30.0028 4.44762E-03
30 33.3811 3.67732E-03
30 37.084 3.87240E-03
30 41.1623 3.59379E-03
30 45.9711 2.78335E-03
30 51.2186 2.91158E-03
30 56.9686 2.67536E-03
30 63.7813 2.13988E-03
30 71.1411 2.36354E-03
30 79.1124 2.29624E-03
30 88.5728 2.04815E-03
30 99.9385 1.70585E-03
30 112.13 1.86102E-03
30 125.216 1.68277E-03
30 140.923 1.55066E-03
30 160.058 1.13836E-03
30 180.197 1.34316E-03
30 201.292 1.21407E-03
30 226.793 1.02643E-03
30 258.169 8.38536E-04
30 297.635 4.17322E-04
30 338.087 4.58143E-04
30 378.82 2.83453E-04
30 429.043 1.88501E-04
30 492.542 1.10441E-04
30 575.534 5.96920E-05
30 689.1 1.20426E-05
60 3.01313 2.34098E-02
60 3.33312 2.56577E-02
60 3.69054 2.77639E-02
60 4.08956 1.72581E-02
60 4.53467 1.66233E-02
60 5.03052 1.14220E-02
60 5.58193 1.17453E-02
60 6.19359 1.00526E-02
60 6.86988 8.35943E-03
60 7.61472 7.21628E-03
60 8.43096 6.74117E-03
60 9.35573 5.25426E-03
60 10.4001 4.90880E-03
60 11.5389 5.03498E-03
60 12.8273 4.31974E-03
60 14.2777 4.37689E-03
60 15.8423 4.96086E-03
60 17.6018 4.27941E-03
60 19.5648 4.71976E-03
60 21.7694 3.69319E-03
60 24.2214 3.64668E-03
60 26.9665 2.85567E-03
60 30.0028 3.11531E-03
60 33.3811 2.59529E-03
60 37.084 2.53878E-03
60 41.1623 2.17765E-03
60 45.9711 1.60416E-03
60 51.2186 1.74234E-03
60 56.9686 1.53707E-03
60 63.7813 1.15067E-03
60 71.1411 1.16109E-03
60 79.1124 9.87423E-04
60 88.5728 8.44158E-04
60 99.9385 6.11636E-04
60 112.13 6.16422E-04
60 125.216 4.47639E-04
60 140.923 3.69270E-04
60 160.058 2.26917E-04
60 180.197 2.46470E-04
60 201.292 1.63482E-04
60 226.793 1.10254E-04
60 258.169 6.83213E-05
60 297.635 2.14641E-05
60 338.087 2.34745E-05
60 378.82 1.11206E-05
90 2.9835 1.75428E-02
90 3.30506 1.87436E-02
90 3.65788 2.00601E-02
90 4.05147 1.36013E-02
90 4.4902 1.12892E-02
90 4.97855 9.24622E-03
90 5.5211 8.23927E-03
90 6.12246 6.53295E-03
90 6.78688 5.54620E-03
90 7.51788 4.88868E-03
90 8.31811 4.51354E-03
90 9.22379 3.52252E-03
90 10.2454 3.42008E-03
90 11.358 2.94793E-03
90 12.6152 2.67760E-03
90 14.0286 2.45670E-03
90 15.5512 2.78949E-03
90 17.2606 2.49514E-03
90 19.1647 2.61834E-03
90 21.2993 2.08798E-03
90 23.6692 1.99782E-03
90 26.3169 1.52723E-03
90 29.2396 1.54404E-03
90 32.484 1.27959E-03
90 36.3119 9.56933E-04
90 40.5387 9.18457E-04
90 45.2328 6.25468E-04
90 50.3475 5.86409E-04
90 55.9429 4.81314E-04
90 62.5608 3.29802E-04
90 69.6972 2.95799E-04
90 77.4102 2.21742E-04
90 86.5436 1.67569E-04
90 97.488 9.22509E-05
90 109.196 9.46253E-05
90 121.725 7.79434E-05
90 136.712 4.15548E-05
90 154.897 2.44411E-05
90 173.958 1.49663E-05
\END;
/*===================================================================*/
|