|
| /*===================================================================*/
/* NRDF D1759 Data No.9 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,9;
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,9;
/* 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=19470MG/CM**2;
INC-ENGY-LAB-RANGE=400MEV/A;
ANL=(INCASC'36',X'37');
/* '36' HIC calculation [Bertini, H. W.: ORNL-TM-4134, (1974).]
/* '37' Phenomenological Hybrid analysis by the moving source
model */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,9;
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 1.41714E-02
0 6.84031 1.31338E-02
0 7.57574 9.21191E-03
0 8.39159 6.59296E-03
0 9.29441 7.22091E-03
0 10.2902 7.89308E-03
0 11.3842 6.82931E-03
0 12.6024 8.18749E-03
0 13.9533 7.23231E-03
0 15.4523 5.94927E-03
0 17.1063 7.89911E-03
0 18.9305 7.49367E-03
0 20.9757 7.35057E-03
0 23.2696 7.40201E-03
0 25.776 7.05254E-03
0 28.5057 7.34101E-03
0 31.5324 7.86423E-03
0 34.8812 8.35805E-03
0 38.576 7.69887E-03
0 42.7816 9.10103E-03
0 47.5631 1.02334E-02
0 52.8459 1.19102E-02
0 58.6529 1.31293E-02
0 64.9957 1.65201E-02
0 72.1921 2.05812E-02
0 80.3241 2.04622E-02
0 89.1423 2.57642E-02
0 99.1253 3.15706E-02
0 110.355 3.85892E-02
0 122.352 5.56864E-02
0 135.82 7.18438E-02
0 150.781 0.106331
0 167.541 0.118436
0 186.072 0.154107
0 206.728 0.168382
0 231.468 0.155379
0 258.981 0.193780
0 289.894 0.153975
0 323.87 0.162728
0 361.548 0.109763
0 407.611 4.59882E-02
0 458.125 2.27669E-02
0 514.062 7.56965E-03
0 583.901 1.71009E-03
0 659.651 9.71251E-04
0 742.467 4.75642E-04
0 848.082 1.52118E-04
0 958.382 1.19093E-04
0 1072.81 8.29858E-05
7.5 5.04587 1.26696E-02
7.5 5.58422 1.01183E-02
7.5 6.17863 9.85296E-03
7.5 6.84031 7.43948E-03
7.5 7.57574 1.01114E-02
7.5 8.39159 9.00219E-03
7.5 9.29441 7.65026E-03
7.5 10.2902 6.21082E-03
7.5 11.3842 7.59880E-03
7.5 12.6024 7.57396E-03
7.5 13.9533 8.95498E-03
7.5 15.4523 6.98959E-03
7.5 17.1063 6.71069E-03
7.5 18.9305 7.98886E-03
7.5 20.9757 8.16064E-03
7.5 23.2696 7.57853E-03
7.5 25.776 7.40124E-03
7.5 28.5057 6.08792E-03
7.5 31.5324 7.05495E-03
7.5 34.8812 8.48605E-03
7.5 38.576 8.63203E-03
7.5 42.7816 1.02289E-02
7.5 47.5631 9.55418E-03
7.5 52.8459 1.15855E-02
7.5 58.6529 1.11914E-02
7.5 64.9957 1.18748E-02
7.5 72.1921 1.20664E-02
7.5 80.3241 1.26356E-02
7.5 89.1423 1.38229E-02
7.5 99.1253 1.25266E-02
7.5 110.355 1.38900E-02
7.5 122.352 1.62195E-02
7.5 135.82 1.51330E-02
7.5 150.781 1.64623E-02
7.5 167.541 1.50390E-02
7.5 186.072 1.87145E-02
7.5 206.728 1.86832E-02
7.5 231.468 1.70527E-02
7.5 258.981 1.89152E-02
7.5 289.894 1.38483E-02
7.5 323.87 1.53844E-02
7.5 361.548 1.06858E-02
7.5 407.611 5.53219E-03
7.5 458.125 4.95006E-03
7.5 514.062 2.40049E-03
7.5 583.901 9.11119E-04
7.5 659.651 7.88901E-04
7.5 742.467 4.16316E-04
7.5 848.082 1.41577E-04
7.5 958.382 7.55729E-05
7.5 1072.81 3.61100E-05
15 3.31207 1.47389E-02
15 3.66601 1.67312E-02
15 4.05584 1.23345E-02
15 4.48426 1.09576E-02
15 4.95878 1.26323E-02
15 5.48313 9.64614E-03
15 6.07005 9.20516E-03
15 6.72561 7.56947E-03
15 7.44649 8.19943E-03
15 8.24985 6.62529E-03
15 9.14152 1.01770E-02
15 10.1317 8.29578E-03
15 11.2253 9.57452E-03
15 12.4322 8.58062E-03
15 13.7862 7.68086E-03
15 15.2681 6.62171E-03
15 16.8853 6.94754E-03
15 18.6817 8.31849E-03
15 20.6732 8.67047E-03
15 22.876 7.96703E-03
15 25.3052 6.41813E-03
15 28.068 6.08809E-03
15 31.2058 5.60353E-03
15 34.6677 6.41770E-03
15 38.4666 5.30331E-03
15 42.6069 5.49237E-03
15 47.2919 4.20748E-03
15 52.5692 4.75996E-03
15 58.2699 5.17912E-03
15 64.6934 4.16935E-03
15 71.8807 4.57137E-03
15 79.9855 4.36510E-03
15 89.0466 4.31336E-03
15 99.2595 4.51118E-03
15 110.647 4.60277E-03
15 123.451 4.22104E-03
15 137.651 3.91502E-03
15 153.528 4.54867E-03
15 170.97 5.23327E-03
15 190.266 4.67608E-03
15 213.413 4.21862E-03
15 238.797 4.24270E-03
15 266.841 4.06661E-03
15 300.944 2.35671E-03
15 338.087 2.38263E-03
15 378.82 1.63748E-03
15 429.043 7.59564E-04
15 482.724 5.36197E-04
15 540.241 2.63023E-04
15 611.793 1.06972E-04
15 703.489 1.00045E-04
15 799.646 1.33366E-05
30 3.33312 8.20215E-03
30 3.69054 1.08200E-02
30 4.08956 8.70951E-03
30 4.53467 9.74697E-03
30 5.03052 9.94599E-03
30 5.58193 8.46323E-03
30 6.19359 9.16304E-03
30 6.86988 6.68301E-03
30 7.61472 7.03997E-03
30 8.43096 6.39736E-03
30 9.35573 5.31518E-03
30 10.4001 4.71683E-03
30 11.5389 5.44559E-03
30 12.8273 4.73886E-03
30 14.2777 4.72060E-03
30 15.8423 5.00695E-03
30 17.6018 4.97072E-03
30 19.5648 5.74941E-03
30 21.7694 5.31375E-03
30 24.2214 5.87115E-03
30 26.9665 4.86038E-03
30 30.0028 5.65662E-03
30 33.3811 4.93273E-03
30 37.084 5.41077E-03
30 41.1623 5.20211E-03
30 45.9711 4.14921E-03
30 51.2186 4.86738E-03
30 56.9686 4.55050E-03
30 63.7813 3.65994E-03
30 71.1411 4.21405E-03
30 79.1124 3.99814E-03
30 88.5728 3.84452E-03
30 99.9385 3.02913E-03
30 112.13 3.66073E-03
30 125.216 3.52415E-03
30 140.923 3.49411E-03
30 160.058 2.59988E-03
30 180.197 3.15916E-03
30 201.292 3.06511E-03
30 226.793 2.73415E-03
30 258.169 2.18327E-03
30 297.635 1.05645E-03
30 338.087 1.13427E-03
30 378.82 8.39797E-04
30 429.043 4.95043E-04
30 492.542 2.89420E-04
30 575.534 1.49344E-04
30 689.1 4.88134E-05
30 799.646 3.28890E-05
60 3.01313 9.07779E-03
60 3.33312 1.22931E-02
60 3.69054 1.71509E-02
60 4.08956 1.14304E-02
60 4.53467 1.04126E-02
60 5.03052 9.95571E-03
60 5.58193 8.24266E-03
60 6.19359 7.95195E-03
60 6.86988 6.57453E-03
60 7.61472 6.40735E-03
60 8.43096 6.05322E-03
60 9.35573 5.19367E-03
60 10.4001 4.60528E-03
60 11.5389 4.81389E-03
60 12.8273 4.11570E-03
60 14.2777 4.22023E-03
60 15.8423 4.80835E-03
60 17.6018 4.31378E-03
60 19.5648 4.87227E-03
60 21.7694 4.31425E-03
60 24.2214 4.29967E-03
60 26.9665 3.29543E-03
60 30.0028 3.56089E-03
60 33.3811 2.94178E-03
60 37.084 2.93602E-03
60 41.1623 2.68333E-03
60 45.9711 1.98841E-03
60 51.2186 2.21805E-03
60 56.9686 1.87740E-03
60 63.7813 1.41536E-03
60 71.1411 1.40425E-03
60 79.1124 1.31687E-03
60 88.5728 1.02586E-03
60 99.9385 7.24431E-04
60 112.13 7.32085E-04
60 125.216 5.75891E-04
60 140.923 4.53048E-04
60 160.058 2.62065E-04
60 180.197 3.16628E-04
60 201.292 1.99829E-04
60 226.793 1.42945E-04
60 258.169 1.15030E-04
60 297.635 3.07050E-05
60 338.087 2.05782E-05
60 378.82 1.91490E-05
90 3.01313 4.12932E-03
90 3.33312 5.09470E-03
90 3.69054 7.15183E-03
90 4.08956 6.08080E-03
90 4.53467 5.63534E-03
90 5.03052 4.61322E-03
90 5.58193 4.75655E-03
90 6.19359 3.27328E-03
90 6.86988 3.02978E-03
90 7.61472 2.83579E-03
90 8.43096 3.00164E-03
90 9.35573 2.26626E-03
90 10.4001 2.15333E-03
90 11.5389 2.08108E-03
90 12.8273 1.87414E-03
90 14.2777 1.72171E-03
90 15.8423 1.85200E-03
90 17.6018 1.74461E-03
90 19.5648 1.89569E-03
90 21.7694 1.72556E-03
90 24.2214 1.71554E-03
90 26.9665 1.21297E-03
90 30.0028 1.22152E-03
90 33.3811 9.13122E-04
90 37.084 9.53150E-04
90 41.1623 7.52659E-04
90 45.9711 5.61138E-04
90 51.2186 5.14738E-04
90 56.9686 3.90493E-04
90 63.7813 2.69888E-04
90 71.1411 3.09596E-04
90 79.1124 2.14858E-04
90 88.5728 1.44986E-04
90 99.9385 9.00162E-05
90 112.13 7.99515E-05
90 125.216 5.48729E-05
90 140.923 3.96768E-05
90 160.058 2.35713E-05
90 180.197 2.92701E-05
90 201.292 2.63896E-05
90 226.793 2.47768E-05
90 258.169 1.74007E-05
90 297.635 1.32462E-05
\END;
/*===================================================================*/
|