|
| /*===================================================================*/
/* NRDF D1759 Data No.11 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,11;
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,11;
/* 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=CU(20NE,N)X;
PHQ=ENGY-SPEC;
THK-TGT=26790MG/CM**2;
INC-ENGY-LAB-RANGE=400MEV/A;
ANL=(INCASC'40',X'41');
/* '40' HIC calculation [Bertini, H. W.: ORNL-TM-4134, (1974).]
/* '41' Phenomenological Hybrid analysis by the moving source
model */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,11;
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 1.54585E-02
0 7.96798 1.23258E-02
0 8.82567 1.31953E-02
0 9.77323 1.20523E-02
0 10.8164 1.11929E-02
0 11.9804 9.96781E-03
0 13.2745 1.04164E-02
0 14.6861 9.67714E-03
0 16.2476 9.93908E-03
0 18.0028 1.12165E-02
0 19.9326 9.95206E-03
0 22.0512 7.86242E-03
0 24.4171 9.90681E-03
0 27.0579 9.76526E-03
0 30.0028 1.03301E-02
0 33.2823 8.41763E-03
0 36.9275 8.34172E-03
0 40.9686 8.74466E-03
0 45.4342 9.06746E-03
0 50.3475 8.54282E-03
0 55.725 1.06099E-02
0 61.8257 1.09057E-02
0 68.7244 1.27912E-02
0 76.239 1.40546E-02
0 84.7622 1.47510E-02
0 94.3804 1.65733E-02
0 104.748 2.15201E-02
0 116.452 2.43899E-02
0 129.555 3.22082E-02
0 144.36 3.53888E-02
0 160.918 4.94055E-02
0 179.613 5.03275E-02
0 200.455 6.42536E-02
0 223.916 5.92957E-02
0 249.893 7.11809E-02
0 278.923 5.77397E-02
0 310.654 6.56944E-02
0 345.606 4.79036E-02
0 388.008 2.27101E-02
0 434.115 1.34012E-02
0 484.634 4.96170E-03
0 546.93 1.19481E-03
0 613.595 8.07476E-04
0 685.215 4.10738E-04
0 774.691 1.91817E-04
0 890.173 7.31412E-05
0 1012.32 2.82077E-05
7.5 6.17863 1.99281E-02
7.5 6.84031 1.69914E-02
7.5 7.57574 1.39576E-02
7.5 8.39159 1.42974E-02
7.5 9.29441 1.30876E-02
7.5 10.2902 1.07078E-02
7.5 11.3842 1.10944E-02
7.5 12.6024 1.03308E-02
7.5 13.9533 9.76228E-03
7.5 15.4523 9.46814E-03
7.5 17.1063 9.84846E-03
7.5 18.9305 1.09335E-02
7.5 20.9757 9.87495E-03
7.5 23.2696 9.96953E-03
7.5 25.776 8.30616E-03
7.5 28.5057 9.90802E-03
7.5 31.5324 7.82028E-03
7.5 34.8812 8.04601E-03
7.5 38.576 1.01503E-02
7.5 42.7816 9.18812E-03
7.5 47.5631 9.75045E-03
7.5 52.8459 9.88572E-03
7.5 58.6529 9.86904E-03
7.5 64.9957 1.06652E-02
7.5 72.1921 9.86156E-03
7.5 80.3241 1.01742E-02
7.5 89.1423 1.26082E-02
7.5 99.1253 1.08454E-02
7.5 110.355 9.83258E-03
7.5 122.352 1.22224E-02
7.5 135.82 1.10588E-02
7.5 150.781 1.26324E-02
7.5 167.541 1.09739E-02
7.5 186.072 1.37920E-02
7.5 206.728 1.32257E-02
7.5 231.468 1.08144E-02
7.5 258.981 1.28878E-02
7.5 289.894 9.59807E-03
7.5 323.87 1.00312E-02
7.5 361.548 6.85629E-03
7.5 407.611 3.90107E-03
7.5 458.125 2.86847E-03
7.5 514.062 1.38513E-03
7.5 583.901 5.71957E-04
7.5 659.651 3.90919E-04
7.5 742.467 2.12189E-04
7.5 848.082 1.18443E-04
7.5 958.382 4.27979E-05
15 4.03261 3.68621E-02
15 4.46226 3.49068E-02
15 4.93324 2.95021E-02
15 5.45345 2.52159E-02
15 6.03543 2.47761E-02
15 6.68524 2.20638E-02
15 7.39944 1.94209E-02
15 8.19496 1.45711E-02
15 9.07751 1.44025E-02
15 10.057 1.15982E-02
15 11.1381 1.19040E-02
15 12.3303 1.09652E-02
15 13.6672 1.21483E-02
15 15.1666 1.07185E-02
15 16.8043 1.22621E-02
15 18.5873 1.02613E-02
15 20.5633 9.04757E-03
15 22.7478 8.81463E-03
15 25.1557 8.93043E-03
15 27.893 7.20331E-03
15 31.0003 7.40938E-03
15 34.4265 6.90578E-03
15 38.1838 6.30950E-03
15 42.2764 5.98330E-03
15 46.904 5.38240E-03
15 52.1129 4.87276E-03
15 57.7353 5.01247E-03
15 64.0652 4.88034E-03
15 71.1411 4.58222E-03
15 79.1124 3.94449E-03
15 88.0145 4.67551E-03
15 98.0359 3.74670E-03
15 109.196 3.98347E-03
15 121.725 3.25830E-03
15 135.599 3.96663E-03
15 151.084 2.94116E-03
15 168.064 4.14050E-03
15 186.809 3.61838E-03
15 209.241 2.88192E-03
15 233.778 3.34805E-03
15 260.802 2.83524E-03
15 293.548 1.75042E-03
15 329.078 1.75323E-03
15 367.861 1.29685E-03
15 415.421 7.24994E-04
15 465.966 6.82383E-04
15 519.732 3.62971E-04
15 586.069 2.53422E-04
15 670.163 4.96216E-05
30 3.33312 2.40442E-02
30 3.69054 3.92265E-02
30 4.08956 2.84638E-02
30 4.53467 2.89284E-02
30 5.03052 2.61749E-02
30 5.58193 2.04070E-02
30 6.19359 2.13452E-02
30 6.86988 1.68755E-02
30 7.61472 1.61300E-02
30 8.43096 1.35013E-02
30 9.35573 1.03677E-02
30 10.4001 9.62991E-03
30 11.5389 9.29393E-03
30 12.8273 7.48450E-03
30 14.2777 7.12063E-03
30 15.8423 7.20302E-03
30 17.6018 6.47971E-03
30 19.5648 7.04848E-03
30 21.7694 6.59759E-03
30 24.2214 6.90514E-03
30 26.9665 5.55782E-03
30 30.0028 6.47168E-03
30 33.3811 5.35160E-03
30 37.084 5.50176E-03
30 41.1623 5.31121E-03
30 45.9711 4.14973E-03
30 51.2186 4.60163E-03
30 56.9686 4.33596E-03
30 63.7813 3.30777E-03
30 71.1411 3.63993E-03
30 79.1124 3.43989E-03
30 88.5728 3.06245E-03
30 99.9385 2.42317E-03
30 112.13 2.82084E-03
30 125.216 2.72064E-03
30 140.923 2.46834E-03
30 160.058 1.76844E-03
30 180.197 2.07141E-03
30 201.292 2.15447E-03
30 226.793 1.82331E-03
30 258.169 1.50917E-03
30 297.635 8.16115E-04
30 338.087 9.62022E-04
30 378.82 6.57962E-04
30 429.043 4.72027E-04
30 492.542 3.68727E-04
30 575.534 2.14025E-04
30 689.1 7.00543E-05
60 3.01313 2.82636E-02
60 3.33312 3.80746E-02
60 3.69054 4.75634E-02
60 4.08956 3.57267E-02
60 4.53467 2.80684E-02
60 5.03052 2.47748E-02
60 5.58193 2.10391E-02
60 6.19359 1.84110E-02
60 6.86988 1.49331E-02
60 7.61472 1.25413E-02
60 8.43096 1.14301E-02
60 9.35573 8.60355E-03
60 10.4001 7.55361E-03
60 11.5389 7.26705E-03
60 12.8273 6.17856E-03
60 14.2777 5.43067E-03
60 15.8423 5.96552E-03
60 17.6018 5.36812E-03
60 19.5648 5.83459E-03
60 21.7694 4.66002E-03
60 24.2214 4.54995E-03
60 26.9665 3.53317E-03
60 30.0028 3.86762E-03
60 33.3811 3.04100E-03
60 37.084 2.86196E-03
60 41.1623 2.53487E-03
60 45.9711 2.10845E-03
60 51.2186 1.98665E-03
60 56.9686 1.62786E-03
60 63.7813 1.15837E-03
60 71.1411 1.32316E-03
60 79.1124 1.07965E-03
60 88.5728 9.09275E-04
60 99.9385 6.37562E-04
60 112.13 6.82499E-04
60 125.216 5.15545E-04
60 140.923 3.73097E-04
60 160.058 2.62836E-04
60 180.197 2.64734E-04
60 201.292 1.80218E-04
60 226.793 1.44088E-04
60 258.169 6.61464E-05
60 297.635 3.93742E-05
60 338.087 2.34884E-05
90 3.33312 2.23572E-02
90 3.69054 2.65447E-02
90 4.08956 2.36071E-02
90 4.53467 1.96854E-02
90 5.03052 1.58633E-02
90 5.58193 1.44572E-02
90 6.19359 1.16475E-02
90 6.86988 1.01472E-02
90 7.61472 8.52379E-03
90 8.43096 7.69894E-03
90 9.35573 5.52656E-03
90 10.4001 4.75740E-03
90 11.5389 4.53074E-03
90 12.8273 3.77010E-03
90 14.2777 3.49412E-03
90 15.8423 3.44100E-03
90 17.6018 3.06493E-03
90 19.5648 3.53722E-03
90 21.7694 2.82763E-03
90 24.2214 2.69074E-03
90 26.9665 1.91356E-03
90 30.0028 2.10273E-03
90 33.3811 1.48800E-03
90 37.084 1.51396E-03
90 41.1623 1.20367E-03
90 45.9711 8.95144E-04
90 51.2186 8.27482E-04
90 56.9686 6.64191E-04
90 63.7813 4.81778E-04
90 71.1411 4.14904E-04
90 79.1124 3.42357E-04
90 88.5728 2.56771E-04
90 99.9385 1.62835E-04
90 112.13 1.65476E-04
90 125.216 1.13595E-04
90 140.923 7.92378E-05
90 160.058 4.58969E-05
90 180.197 5.98465E-05
90 201.292 3.95267E-05
90 226.793 3.21628E-05
90 258.169 3.25786E-05
\END;
/*===================================================================*/
|