|
| /*===================================================================*/
/* NRDF D1810 Data No.43 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,43;
97, 103, 109, 115, 121[128;
D#=D1810;
TITLE=/ Measurements of secondary neutrons produced from thick
targets bombarded by high-energy helium and carbon ions /;
PURPOSE=/ To present the angular and energy distributions of
neutrons produced from thick C, Al, Cu, and Pb targets
bombarded by 100 and 180 MeV/nucleon He and 100, 180, and
400 MeV/nucleon C ions. /;
ATH=(T.KUROSAWA'1', N.NAKAO'2', T.NAKAMURA'1', Y.UWAMINO'3',
T.SHIBATA'2', N.NAKANISHI'3', A.FUKUMURA'4', K.MURAKAMI'4');
INST-ATH=(2JPNTOH'1', 2JPNKEK'2', 2JPNIPC'3', 2JPNIRS'4');
/* '1' Cyclotron and Radioisotope Center */
/* '2' Tanashi branch */
REF=NSE;
VLP=132(1999)30;
RCTS=(C(ALPHA,N)X, 27AL(ALPHA,N)X, CU(ALPHA,N)X, PB(ALPHA,N)X,
C(12C,N)X, 27AL(12C,N)X, CU(12C,N)X, PB(12C,N)X);
PHQS=(ENGY-SPEC'5', N-MLT'6');
/* '5' Neutron energy spectrum */
/* '6' Neutron Yield above 5 MeV integrated for a hemisphere from 0
deg to 90 deg. */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,43;
97, 103, 109, 115, 121[128;
/* 2004-01-27 : Compiled+Checked, Sr + On */
/* 2009-08-23 : Altered, Nf. 122-129 corrected */
ENR=NAT;
CHM=ELM;
PHYS-FORM=SLD;
BAC=X;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=SYN'7';
/* '7' HIMAC heavy-ion synchrotron */
INST-ACC=2JPNIRS;
BEAM-INTNSTY=XMA'8';
/* '8' The beam intensities were maintained at 100,000 - 1,000,000
particles per pulse */
POL-PRJ=0%;
DET-PARTCL=N;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(SCT'9',SCT'10',TOF'11',EDE'12');
/* '9' Plastic scintillator (NE102A) was used as the delta-E
counter and the beam pick-up counter (the output pulses of this
scintillator were used as start signals for the TOF and to
count the absolute number of projectile incident). */
/* '10' Liquid scintillator (NE213) was used as the E counter. */
/* '11' To measure the energy of neutron */
/* '12' To eliminate charged particles */
ERS-DET=XKEV'13';
/* '13' Energy resolutions are represented as a function of
neutron energy in Fig. 4 in the reference. */
CALB-DET=/ After the experimental run, 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. [Ref: R. A. Cecil et al.,
Nucl. Instrum. Methods 161, 439 (1979).] /;
ANL=(INCASC'14',X'15');
/* '14' HIC calculation [H. W. Bertini, et al. ORNL-TM-4134, Oak
Ridge National Laboratory (1974)] */
/* '15' Phenomenological hybrid analysis by the moving source
model [G. Mantzouranis et al., Z. Phys. A276(1976)145] */
/* 2007-10-24 : Altered, On. Extended for angular range */
/* 2007-10-25 : Altered, On. Superseded by data with new analysis
RCT=PB(12C,N)X;
PHQ=ENGY-SPEC'34';
/* '34' Neutron energy spectrum */
THK-TGT=5670MG/CM**2;
INC-ENGY-LAB-RANGE=100MEV/A;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,43;
97, 103, 109, 115, 121[128;
SYS-ERR=(<3%'16',<10%'17',[8%'18');
/* '16' Uncertainty in the number of accepted beam particles
incident to target (less than 3%.) */
/* '17' Uncertainty in solid angle (less than 10%) */
/* '18' Uncertainty in calculated detection efficiencies (about
9%) */
STATIST-ERR=X%'19';
/* '19' The statistical uncertainties vary from 2 to 5% for the
low- to medium-energy (5- to 50-MeV) region of the spectra and
increase to about 30% at the highest energies. */
INC-ENGY-LAB=100MEV/A;
DELTA-DN/DOMEGA/DE=14%'35';
/* '35' Total normalization uncertainty */
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTL ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE
(DEG) (MEV) (MEV) (1/SR/MEV/PARTCL)
0 3.21065 3.54958 1.17430E-02
0 3.54958 3.92625 1.46866E-02
0 3.92625 4.34403 1.48054E-02
0 4.34403 4.80662 1.46502E-02
0 4.80662 5.31736 1.21784E-02
0 5.31736 5.87907 1.07628E-02
0 5.87907 6.50799 1.07237E-02
0 6.50799 7.19626 8.78668E-03
0 7.19626 7.96339 8.32740E-03
0 7.96339 8.81755 6.45870E-03
0 8.81755 9.76758 5.23654E-03
0 9.76758 10.8221 5.32937E-03
0 10.8221 11.9899 4.56740E-03
0 11.9899 13.2790 4.80230E-03
0 13.2790 14.6963 4.19264E-03
0 14.6963 16.2471 4.51533E-03
0 16.2471 17.9964 4.26675E-03
0 17.9964 19.9001 4.73230E-03
0 19.9001 22.0405 4.46528E-03
0 22.0405 24.4503 4.37725E-03
0 24.4503 27.0491 3.97647E-03
0 27.0491 29.9555 3.91584E-03
0 29.9555 33.2057 3.73923E-03
0 33.2057 36.8385 3.78722E-03
0 36.8385 40.8955 3.78170E-03
0 40.8955 45.4203 3.82759E-03
0 45.4203 50.4573 3.40010E-03
0 50.4573 56.0501 3.15235E-03
0 56.0501 62.2394 3.20448E-03
0 62.2394 69.0592 2.97839E-03
0 69.0592 76.5329 2.83036E-03
0 76.5329 84.6669 2.45472E-03
0 84.6669 94.2397 1.64095E-03
0 94.2397 104.6793 1.18265E-03
0 104.6793 115.951 7.76623E-04
0 115.951 129.278 3.40620E-04
0 129.278 143.653 2.48773E-04
0 143.653 158.924 1.06239E-04
0 158.924 177.004 1.13332E-04
0 177.004 196.074 3.36513E-05
0 196.074 218.767 2.14510E-05
7.5 4.20705 4.65552 7.98202E-03
7.5 4.65552 5.15115 7.88561E-03
7.5 5.15115 5.69718 8.02894E-03
7.5 5.69718 6.30906 7.98234E-03
7.5 6.30906 6.98020 6.06721E-03
7.5 6.98020 7.72952 5.20975E-03
7.5 7.72952 8.54526 4.89542E-03
7.5 8.54526 9.45027 4.07835E-03
7.5 9.45027 10.45227 3.58801E-03
7.5 10.45227 11.5588 3.14570E-03
7.5 11.5588 12.7767 2.77496E-03
7.5 12.7767 14.1555 2.72513E-03
7.5 14.1555 15.6696 2.57806E-03
7.5 15.6696 17.3233 2.97696E-03
7.5 17.3233 19.1866 2.77591E-03
7.5 19.1866 21.2088 3.09416E-03
7.5 21.2088 23.4782 2.94220E-03
7.5 23.4782 26.0274 3.03801E-03
7.5 26.0274 28.8928 2.42633E-03
7.5 28.8928 31.9642 2.91288E-03
7.5 31.9642 35.3860 2.77511E-03
7.5 35.3860 39.1943 2.58497E-03
7.5 39.1943 43.4259 2.44106E-03
7.5 43.4259 48.1177 2.18948E-03
7.5 48.1177 53.3051 2.27081E-03
7.5 53.3051 59.0196 1.98114E-03
7.5 59.0196 65.2855 2.01194E-03
7.5 65.2855 72.6468 1.79645E-03
7.5 72.6468 80.7530 1.34070E-03
7.5 80.7530 89.6212 1.09001E-03
7.5 89.6212 99.2437 8.50003E-04
7.5 99.2437 110.600 5.44783E-04
7.5 110.600 122.933 3.03934E-04
7.5 122.933 136.162 2.73456E-04
7.5 136.162 151.829 1.27141E-04
7.5 151.829 168.577 5.84571E-05
7.5 168.577 188.545 5.46639E-05
7.5 188.545 209.772 1.68124E-05
15 3.34237 3.69866 1.28384E-02
15 3.69866 4.08989 1.16215E-02
15 4.08989 4.52705 1.16124E-02
15 4.52705 5.00397 1.04331E-02
15 5.00397 5.53410 9.91645E-03
15 5.53410 6.12235 9.25348E-03
15 6.12235 6.77378 7.93730E-03
15 6.77378 7.49330 6.74890E-03
15 7.49330 8.28552 5.83451E-03
15 8.28552 9.18235 4.82830E-03
15 9.18235 10.16733 4.03092E-03
15 10.16733 11.2429 3.85970E-03
15 11.2429 12.4547 3.37280E-03
15 12.4547 13.7694 3.15908E-03
15 13.7694 15.2443 2.92206E-03
15 15.2443 16.9002 2.66048E-03
15 16.9002 18.7602 2.61755E-03
15 18.7602 20.7519 2.88902E-03
15 20.7519 22.9684 2.51078E-03
15 22.9684 25.4316 2.29205E-03
15 25.4316 28.1640 2.37403E-03
15 28.1640 31.1875 2.37319E-03
15 31.1875 34.5222 1.99394E-03
15 34.5222 38.1855 2.20624E-03
15 38.1855 42.4787 1.60399E-03
15 42.4787 47.2147 1.46557E-03
15 47.2147 52.4092 1.34459E-03
15 52.4092 58.0661 1.24485E-03
15 58.0661 64.7249 9.58531E-04
15 64.7249 71.9851 8.14670E-04
15 71.9851 79.8185 7.86266E-04
15 79.8185 89.0689 5.78024E-04
15 89.0689 99.0268 4.28749E-04
15 99.0268 109.577 3.41737E-04
15 109.577 122.024 1.51981E-04
15 122.024 135.093 1.36645E-04
15 135.093 150.556 7.77545E-05
15 150.556 166.572 7.30479E-05
15 166.572 185.547 6.87426E-05
15 185.547 208.332 2.46336E-05
30 3.84292 4.25208 4.48560E-03
30 4.25208 4.70234 5.92045E-03
30 4.70234 5.21219 5.63237E-03
30 5.21219 5.77188 5.16235E-03
30 5.77188 6.38321 5.22612E-03
30 6.38321 7.07160 4.00561E-03
30 7.07160 7.81823 3.38291E-03
30 7.81823 8.65547 2.96277E-03
30 8.65547 9.59476 2.52324E-03
30 9.59476 10.6490 2.19831E-03
30 10.6490 11.7769 1.74765E-03
30 11.7769 13.0306 1.59541E-03
30 13.0306 14.4221 1.38484E-03
30 14.4221 15.9632 1.26866E-03
30 15.9632 17.6652 1.26582E-03
30 17.6652 19.5384 1.25849E-03
30 19.5384 21.7299 1.08449E-03
30 21.7299 24.1524 1.01529E-03
30 24.1524 26.8168 8.71466E-04
30 26.8168 29.7293 7.25835E-04
30 29.7293 32.8885 7.79812E-04
30 32.8885 36.5902 6.46968E-04
30 36.5902 40.6041 5.32561E-04
30 40.6041 44.9087 5.37045E-04
30 44.9087 49.9556 4.30379E-04
30 49.9556 55.3438 3.92008E-04
30 55.3438 61.6842 2.78935E-04
30 61.6842 68.4071 2.61248E-04
30 68.4071 76.3405 2.10820E-04
30 76.3405 84.6669 1.49843E-04
30 84.6669 94.5072 1.11436E-04
30 94.5072 104.6793 7.30224E-05
30 104.6793 116.695 5.54229E-05
30 116.695 131.059 2.75159E-05
60 3.72789 4.12383 5.26147E-03
60 4.12383 4.56659 5.48097E-03
60 4.56659 5.06166 4.77781E-03
60 5.06166 5.61474 4.28491E-03
60 5.61474 6.23212 3.94678E-03
60 6.23212 6.92028 3.06853E-03
60 6.92028 7.68573 2.51445E-03
60 7.68573 8.53507 1.97234E-03
60 8.53507 9.47412 1.62667E-03
60 9.47412 10.50794 1.36353E-03
60 10.50794 11.6399 1.06829E-03
60 11.6399 12.8710 9.28680E-04
60 12.8710 14.3101 7.49183E-04
60 14.3101 15.8760 6.35920E-04
60 15.8760 17.5635 5.78384E-04
60 17.5635 19.5384 4.89255E-04
60 19.5384 21.6602 4.98219E-04
60 21.6602 24.1524 3.54495E-04
60 24.1524 26.8168 3.30194E-04
60 26.8168 29.9555 2.57108E-04
60 29.9555 33.2857 2.54672E-04
60 33.2857 37.2158 1.87204E-04
60 37.2158 41.3384 1.77269E-04
60 41.3384 46.2046 1.12852E-04
60 46.2046 51.2244 9.89422E-05
60 51.2244 57.1361 7.35771E-05
60 57.1361 64.1716 5.81598E-05
60 64.1716 71.3328 5.04054E-05
60 71.3328 79.8185 3.87849E-05
60 79.8185 89.9923 2.29955E-05
60 89.9923 100.1182 2.58609E-05
60 100.1182 112.164 1.77910E-05
60 112.164 126.679 1.27209E-05
90 3.72789 4.12383 4.29137E-03
90 4.12383 4.56659 4.25283E-03
90 4.56659 5.06166 3.61426E-03
90 5.06166 5.61474 3.03244E-03
90 5.61474 6.23212 2.83073E-03
90 6.23212 6.92028 2.06551E-03
90 6.92028 7.68573 1.53772E-03
90 7.68573 8.53507 1.29739E-03
90 8.53507 9.47412 9.65819E-04
90 9.47412 10.50794 7.90499E-04
90 10.50794 11.6399 5.94610E-04
90 11.6399 12.8710 4.66328E-04
90 12.8710 14.3101 3.68290E-04
90 14.3101 15.8760 3.15183E-04
90 15.8760 17.5635 2.71479E-04
90 17.5635 19.5384 2.06619E-04
90 19.5384 21.6602 1.97539E-04
90 21.6602 24.1524 1.33417E-04
90 24.1524 26.8168 1.15525E-04
90 26.8168 29.9555 7.37010E-05
90 29.9555 33.2857 7.95463E-05
90 33.2857 37.2158 3.89244E-05
90 37.2158 41.3384 3.82860E-05
90 41.3384 46.2046 2.48087E-05
90 46.2046 51.2244 1.77568E-05
90 51.2244 57.1361 1.41926E-05
\END;
/*===================================================================*/
|