|
| /*===================================================================*/
/* NRDF D1759 Data No.12 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,12;
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,12;
/* 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=34020MG/CM**2;
INC-ENGY-LAB-RANGE=400MEV/A;
ANL=(INCASC'42',X'43');
/* '42' HIC calculation [Bertini, H. W.: ORNL-TM-4134, (1974).]
/* '43' Phenomenological Hybrid analysis by the moving source
model */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,12;
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 7.19391 2.87174E-02
0 7.96798 2.60803E-02
0 8.82567 2.23458E-02
0 9.77323 1.88522E-02
0 10.8164 1.81652E-02
0 11.9804 1.57352E-02
0 13.2745 1.39884E-02
0 14.6861 1.43627E-02
0 16.2476 1.45691E-02
0 18.0028 1.29341E-02
0 19.9326 1.26330E-02
0 22.0512 1.20277E-02
0 24.4171 9.94900E-03
0 27.0579 8.50689E-03
0 30.0028 8.86933E-03
0 33.2823 8.47106E-03
0 36.9275 7.45554E-03
0 40.9686 6.83474E-03
0 45.4342 7.27156E-03
0 50.3475 6.44488E-03
0 55.725 8.05770E-03
0 61.8257 7.03999E-03
0 68.7244 8.60090E-03
0 76.239 9.45042E-03
0 84.7622 8.95433E-03
0 94.3804 9.35820E-03
0 104.748 1.23265E-02
0 116.452 1.23993E-02
0 129.555 1.44133E-02
0 144.36 1.48359E-02
0 160.918 1.73135E-02
0 179.613 1.58412E-02
0 200.455 1.96392E-02
0 223.916 1.72361E-02
0 249.893 1.85490E-02
0 278.923 1.52168E-02
0 310.654 1.61607E-02
0 345.606 1.19037E-02
0 388.008 5.68940E-03
0 434.115 3.66549E-03
0 484.634 1.32026E-03
0 546.93 4.55262E-04
0 613.595 2.35884E-04
0 685.215 9.56146E-05
0 774.691 5.60345E-05
7.5 6.84031 2.81459E-02
7.5 7.57574 2.43099E-02
7.5 8.39159 2.24429E-02
7.5 9.29441 1.88596E-02
7.5 10.2902 1.59600E-02
7.5 11.3842 1.57086E-02
7.5 12.6024 1.33170E-02
7.5 13.9533 1.39418E-02
7.5 15.4523 1.27287E-02
7.5 17.1063 1.25428E-02
7.5 18.9305 1.17993E-02
7.5 20.9757 1.10703E-02
7.5 23.2696 9.31585E-03
7.5 25.776 8.83957E-03
7.5 28.5057 7.77234E-03
7.5 31.5324 6.84139E-03
7.5 34.8812 7.33724E-03
7.5 38.576 7.20464E-03
7.5 42.7816 6.28768E-03
7.5 47.5631 5.51047E-03
7.5 52.8459 5.13970E-03
7.5 58.6529 5.19460E-03
7.5 64.9957 5.40642E-03
7.5 72.1921 5.19989E-03
7.5 80.3241 5.04455E-03
7.5 89.1423 5.55862E-03
7.5 99.1253 4.64054E-03
7.5 110.355 4.59416E-03
7.5 122.352 5.04153E-03
7.5 135.82 4.14847E-03
7.5 150.781 4.81678E-03
7.5 167.541 4.24654E-03
7.5 186.072 5.37497E-03
7.5 206.728 4.77996E-03
7.5 231.468 3.95284E-03
7.5 258.981 3.92098E-03
7.5 289.894 2.99041E-03
7.5 323.87 2.71040E-03
7.5 361.548 1.81046E-03
7.5 407.611 7.69900E-04
7.5 458.125 6.69473E-04
7.5 514.062 3.78821E-04
7.5 583.901 1.19761E-04
7.5 659.651 7.16859E-05
7.5 742.467 4.03518E-05
15 4.03261 6.99416E-02
15 4.46226 6.44416E-02
15 4.93324 5.00996E-02
15 5.45345 4.47285E-02
15 6.03543 3.96268E-02
15 6.68524 3.17954E-02
15 7.39944 3.19226E-02
15 8.19496 2.38381E-02
15 9.07751 2.15999E-02
15 10.057 1.91914E-02
15 11.1381 1.62532E-02
15 12.3303 1.48157E-02
15 13.6672 1.47919E-02
15 15.1666 1.27008E-02
15 16.8043 1.24685E-02
15 18.5873 1.32599E-02
15 20.5633 9.87778E-03
15 22.7478 9.55059E-03
15 25.1557 8.50307E-03
15 27.893 6.91119E-03
15 31.0003 6.53127E-03
15 34.4265 6.07206E-03
15 38.1838 4.98960E-03
15 42.2764 4.94499E-03
15 46.904 3.87719E-03
15 52.1129 3.74296E-03
15 57.7353 3.55500E-03
15 64.0652 3.38259E-03
15 71.1411 3.51563E-03
15 79.1124 2.86772E-03
15 88.0145 2.74859E-03
15 98.0359 2.54060E-03
15 109.196 2.71484E-03
15 121.725 2.13497E-03
15 135.599 2.55765E-03
15 151.084 2.04120E-03
15 168.064 2.45939E-03
15 186.809 2.09587E-03
15 209.241 1.66399E-03
15 233.778 1.71678E-03
15 260.802 1.70561E-03
15 293.548 1.00535E-03
15 329.078 8.30424E-04
15 367.861 6.76733E-04
15 415.421 3.30669E-04
15 465.966 2.73318E-04
15 519.732 1.41153E-04
15 586.069 1.07024E-04
15 670.163 3.32966E-05
30 4.53467 4.61346E-02
30 5.03052 4.00423E-02
30 5.58193 3.61400E-02
30 6.19359 3.08979E-02
30 6.86988 2.59714E-02
30 7.61472 2.27003E-02
30 8.43096 2.04154E-02
30 9.35573 1.59546E-02
30 10.4001 1.36945E-02
30 11.5389 1.30676E-02
30 12.8273 1.05856E-02
30 14.2777 9.99910E-03
30 15.8423 9.91884E-03
30 17.6018 9.01722E-03
30 19.5648 9.00513E-03
30 21.7694 7.10511E-03
30 24.2214 6.48788E-03
30 26.9665 4.83592E-03
30 30.0028 5.12527E-03
30 33.3811 4.01906E-03
30 37.084 4.04625E-03
30 41.1623 3.57789E-03
30 45.9711 2.57185E-03
30 51.2186 2.74401E-03
30 56.9686 2.48533E-03
30 63.7813 1.81445E-03
30 71.1411 2.05905E-03
30 79.1124 1.76421E-03
30 88.5728 1.59399E-03
30 99.9385 1.16712E-03
30 112.13 1.18068E-03
30 125.216 1.12182E-03
30 140.923 9.98409E-04
30 160.058 7.11390E-04
30 180.197 8.24525E-04
30 201.292 7.35377E-04
30 226.793 6.05602E-04
30 258.169 4.61307E-04
30 297.635 2.41160E-04
30 338.087 2.53549E-04
30 378.82 1.71723E-04
30 429.043 1.11965E-04
30 492.542 7.16683E-05
30 575.534 3.38939E-05
30 689.1 1.00941E-05
60 3.01313 8.94061E-02
60 3.33312 9.79787E-02
60 3.69054 1.00084E-01
60 4.08956 5.84335E-02
60 4.53467 5.50754E-02
60 5.03052 3.94246E-02
60 5.58193 3.74503E-02
60 6.19359 3.00675E-02
60 6.86988 2.46753E-02
60 7.61472 2.08792E-02
60 8.43096 1.88931E-02
60 9.35573 1.38111E-02
60 10.4001 1.19819E-02
60 11.5389 1.15336E-02
60 12.8273 8.86923E-03
60 14.2777 8.63861E-03
60 15.8423 8.75757E-03
60 17.6018 7.32713E-03
60 19.5648 7.43222E-03
60 21.7694 5.69047E-03
60 24.2214 4.91330E-03
60 26.9665 3.80353E-03
60 30.0028 4.05940E-03
60 33.3811 2.99390E-03
60 37.084 2.98205E-03
60 41.1623 2.49518E-03
60 45.9711 1.76763E-03
60 51.2186 1.73469E-03
60 56.9686 1.46746E-03
60 63.7813 1.07313E-03
60 71.1411 1.09366E-03
60 79.1124 9.13498E-04
60 88.5728 7.79775E-04
60 99.9385 5.42084E-04
60 112.13 5.22013E-04
60 125.216 3.86217E-04
60 140.923 3.26468E-04
60 160.058 1.88407E-04
60 180.197 1.74486E-04
60 201.292 1.39589E-04
60 226.793 1.01934E-04
60 258.169 6.13611E-05
60 297.635 2.61358E-05
60 338.087 2.44372E-05
60 378.82 1.68543E-05
60 429.043 1.12928E-05
60 492.542 1.01495E-05
90 3.01313 4.92038E-02
90 3.33312 5.13899E-02
90 3.69054 5.20277E-02
90 4.08956 3.37431E-02
90 4.53467 2.81880E-02
90 5.03052 2.27897E-02
90 5.58193 1.97227E-02
90 6.19359 1.58913E-02
90 6.86988 1.36308E-02
90 7.61472 1.09215E-02
90 8.43096 9.80888E-03
90 9.35573 7.36136E-03
90 10.4001 6.51354E-03
90 11.5389 5.54614E-03
90 12.8273 4.66898E-03
90 14.2777 4.18494E-03
90 15.8423 3.90153E-03
90 17.6018 3.51734E-03
90 19.5648 3.44195E-03
90 21.7694 2.61966E-03
90 24.2214 2.38230E-03
90 26.9665 1.76476E-03
90 30.0028 1.75871E-03
90 33.3811 1.18533E-03
90 37.084 1.13921E-03
90 41.1623 9.26608E-04
90 45.9711 6.86262E-04
90 51.2186 6.52388E-04
90 56.9686 5.47345E-04
90 63.7813 3.40150E-04
90 71.1411 3.26301E-04
90 79.1124 2.24997E-04
90 88.5728 1.84625E-04
90 99.9385 1.03341E-04
90 112.13 1.08702E-04
90 125.216 7.29394E-05
90 140.923 5.57873E-05
90 160.058 2.83809E-05
90 180.197 2.56149E-05
90 201.292 1.83957E-05
\END;
/*===================================================================*/
|