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| /*===================================================================*/
/* NRDF D1810 Data No.91 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,91;
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,91;
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'50';
/* '50' Neutron energy spectrum */
THK-TGT=17010MG/CM**2;
INC-ENGY-LAB-RANGE=180MEV/A;
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,91;
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=180MEV/A;
DELTA-DN/DOMEGA/DE=14%'51';
/* '51' 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 6.20075 6.86249 1.55188E-02
0 6.86249 7.60878 1.29163E-02
0 7.60878 8.41914 1.07355E-02
0 8.41914 9.32908 8.44849E-03
0 9.32908 10.35147 8.27881E-03
0 10.35147 11.4490 6.67716E-03
0 11.4490 12.6720 5.45542E-03
0 12.6720 14.0333 5.48295E-03
0 14.0333 15.5463 5.48488E-03
0 15.5463 17.2246 5.48010E-03
0 17.2246 19.0812 4.82237E-03
0 19.0812 21.1282 4.34407E-03
0 21.1282 23.3753 4.80767E-03
0 23.3753 26.0064 4.44325E-03
0 26.0064 28.9051 3.86863E-03
0 28.9051 32.0794 3.75877E-03
0 32.0794 35.5290 4.59725E-03
0 35.5290 39.5794 3.70953E-03
0 39.5794 43.9818 3.81580E-03
0 43.9818 48.7141 4.34338E-03
0 48.7141 54.2774 4.13330E-03
0 54.2774 60.2342 4.56331E-03
0 60.2342 67.2662 4.15699E-03
0 67.2662 74.7490 5.32252E-03
0 74.7490 83.6136 5.27639E-03
0 83.6136 92.9572 5.96433E-03
0 92.9572 104.0524 5.51731E-03
0 104.0524 115.581 6.73255E-03
0 115.581 129.278 5.40306E-03
0 129.278 143.208 6.23308E-03
0 143.208 159.716 6.18416E-03
0 159.716 179.539 4.30379E-03
0 179.539 199.326 5.19338E-03
0 199.326 222.971 3.59216E-03
0 222.971 251.665 1.89169E-03
0 251.665 279.396 1.34721E-03
0 279.396 312.733 6.72475E-04
0 312.733 353.523 4.06611E-04
0 353.523 404.544 1.59990E-04
0 404.544 452.072 1.12707E-04
0 452.072 510.628 3.82027E-05
0 510.628 584.642 1.95904E-05
7.5 5.68396 6.28330 1.66164E-02
7.5 6.28330 6.95870 1.34459E-02
7.5 6.95870 7.69278 1.16869E-02
7.5 7.69278 8.51715 1.13472E-02
7.5 8.51715 9.44344 8.99232E-03
7.5 9.44344 10.44040 8.90827E-03
7.5 10.44040 11.5526 6.38942E-03
7.5 11.5526 12.7929 5.81978E-03
7.5 12.7929 14.1743 5.55121E-03
7.5 14.1743 15.7111 5.11820E-03
7.5 15.7111 17.4171 4.64210E-03
7.5 17.4171 19.3061 4.63479E-03
7.5 19.3061 21.3908 4.47087E-03
7.5 21.3908 23.6815 4.18636E-03
7.5 23.6815 26.1856 4.34245E-03
7.5 26.1856 29.1157 3.89590E-03
7.5 29.1157 32.3261 3.95898E-03
7.5 32.3261 35.8176 4.32692E-03
7.5 35.8176 39.9200 4.33474E-03
7.5 39.9200 44.3822 4.30712E-03
7.5 44.3822 49.1828 4.73475E-03
7.5 49.1828 54.8312 4.33993E-03
7.5 54.8312 60.8849 5.33150E-03
7.5 60.8849 68.0387 3.77501E-03
7.5 68.0387 75.6597 3.99076E-03
7.5 75.6597 84.6991 3.82112E-03
7.5 84.6991 94.2397 4.27054E-03
7.5 94.2397 105.585 3.50224E-03
7.5 105.585 117.393 4.26206E-03
7.5 117.393 131.445 3.32061E-03
7.5 131.445 145.763 3.59691E-03
7.5 145.763 162.766 2.84199E-03
7.5 162.766 183.232 2.24433E-03
7.5 183.232 203.714 1.22691E-03
7.5 203.714 228.260 8.52001E-04
7.5 228.260 258.150 4.32196E-04
7.5 258.150 287.144 3.06095E-04
7.5 287.144 322.143 1.60439E-04
7.5 322.143 365.182 2.79320E-05
15 4.15956 4.59874 1.90330E-02
15 4.59874 5.09178 1.78238E-02
15 5.09178 5.64565 1.43287E-02
15 5.64565 6.24152 1.42335E-02
15 6.24152 6.90606 1.18439E-02
15 6.90606 7.64675 1.07885E-02
15 7.64675 8.47134 8.34900E-03
15 8.47134 9.38799 7.08693E-03
15 9.38799 10.40456 6.73438E-03
15 10.40456 11.5292 5.85931E-03
15 11.5292 12.7688 5.46116E-03
15 12.7688 14.1290 4.93535E-03
15 14.1290 15.7208 4.39307E-03
15 15.7208 17.4731 3.71219E-03
15 17.4731 19.3900 4.13303E-03
15 19.3900 21.4707 3.95685E-03
15 21.4707 23.9099 3.62022E-03
15 23.9099 26.5558 3.07266E-03
15 26.5558 29.3936 3.08723E-03
15 29.3936 32.7205 2.60040E-03
15 32.7205 36.2708 3.41283E-03
15 36.2708 40.4458 2.58510E-03
15 40.4458 44.8677 3.14169E-03
15 44.8677 50.0778 2.39984E-03
15 50.0778 55.5346 2.55327E-03
15 55.5346 61.9666 2.38616E-03
15 61.9666 68.5933 2.38862E-03
15 68.5933 76.3895 2.35494E-03
15 76.3895 85.6602 1.91245E-03
15 85.6602 95.0913 2.08211E-03
15 95.0913 106.265 1.78120E-03
15 106.265 119.664 1.28993E-03
15 119.664 133.010 1.20381E-03
15 133.010 148.907 8.88474E-04
15 148.907 168.103 7.35023E-04
15 168.103 186.538 5.35274E-04
15 186.538 208.527 3.54240E-04
15 208.527 235.147 2.20243E-04
15 235.147 267.959 7.71124E-05
15 267.959 298.002 6.21612E-05
15 298.002 334.285 3.76129E-05
15 334.285 378.936 1.62920E-05
30 3.15968 3.49290 9.38090E-03
30 3.49290 3.86499 1.44697E-02
30 3.86499 4.28053 1.50854E-02
30 4.28053 4.74423 1.84272E-02
30 4.74423 5.26114 1.63623E-02
30 5.26114 5.83629 1.46993E-02
30 5.83629 6.47517 1.44477E-02
30 6.47517 7.18271 1.16343E-02
30 7.18271 7.96361 9.26220E-03
30 7.96361 8.82169 8.06505E-03
30 8.82169 9.75918 7.62468E-03
30 9.75918 10.8555 6.00056E-03
30 10.8555 12.0556 5.67089E-03
30 12.0556 13.3589 4.61587E-03
30 13.3589 14.8873 4.04094E-03
30 14.8873 16.5458 3.61513E-03
30 16.5458 18.3248 3.61861E-03
30 18.3248 20.4104 3.09359E-03
30 20.4104 22.6356 3.01555E-03
30 22.6356 25.2510 2.63108E-03
30 25.2510 28.0190 2.49124E-03
30 28.0190 31.2770 2.20400E-03
30 31.2770 34.6843 2.17751E-03
30 34.6843 38.6929 1.78000E-03
30 38.6929 42.8132 1.82494E-03
30 42.8132 47.6469 1.63220E-03
30 47.6469 53.3734 1.31497E-03
30 53.3734 59.1731 1.51518E-03
30 59.1731 66.0085 1.29569E-03
30 66.0085 74.1513 1.07991E-03
30 74.1513 82.1996 1.00258E-03
30 82.1996 91.7020 8.23486E-04
30 91.7020 103.0500 7.32895E-04
30 103.0500 116.784 4.66504E-04
30 116.784 129.994 4.48905E-04
30 129.994 145.763 3.54334E-04
30 145.763 164.852 2.46312E-04
30 164.852 188.353 1.46699E-04
30 188.353 209.818 1.37328E-04
30 209.818 235.644 1.03209E-04
30 235.644 267.244 6.54112E-05
30 267.244 306.718 2.71585E-05
30 306.718 357.337 1.49930E-05
60 2.89289 3.20202 5.60073E-03
60 3.20202 3.54084 9.69473E-03
60 3.54084 3.93644 1.28385E-02
60 3.93644 4.37092 1.26064E-02
60 4.37092 4.84492 1.24361E-02
60 4.84492 5.35791 1.20163E-02
60 5.35791 5.95725 9.86449E-03
60 5.95725 6.60465 9.31089E-03
60 6.60465 7.36416 6.81336E-03
60 7.36416 8.18225 5.76548E-03
60 8.18225 9.05085 5.28010E-03
60 9.05085 10.06641 4.04815E-03
60 10.06641 11.1348 3.58822E-03
60 11.1348 12.3840 2.92770E-03
60 12.3840 13.8578 2.19143E-03
60 13.8578 15.4023 2.06536E-03
60 15.4023 17.2228 1.65424E-03
60 17.2228 19.0972 1.68918E-03
60 19.0972 21.2989 1.51684E-03
60 21.2989 23.9099 1.27644E-03
60 23.9099 26.5558 1.24313E-03
60 26.5558 29.6743 1.00082E-03
60 29.6743 33.3868 8.38095E-04
60 33.3868 37.0514 8.46073E-04
60 37.0514 41.3689 7.38798E-04
60 41.3689 46.5081 5.84150E-04
60 46.5081 52.6975 3.68303E-04
60 52.6975 58.6144 4.43890E-04
60 58.6144 65.6249 3.60329E-04
60 65.6249 74.0267 2.72950E-04
60 74.0267 84.2312 1.60684E-04
60 84.2312 93.4094 1.82659E-04
60 93.4094 104.2629 1.21937E-04
60 104.2629 117.251 9.75175E-05
60 117.251 133.010 6.59537E-05
60 133.010 152.453 2.86435E-05
60 152.453 176.930 1.44524E-05
60 176.930 197.030 1.39868E-05
90 3.01072 3.34685 4.78982E-03
90 3.34685 3.71871 7.99600E-03
90 3.71871 4.12876 9.59095E-03
90 4.12876 4.57801 1.04110E-02
90 4.57801 5.06714 1.05865E-02
90 5.06714 5.63938 8.69189E-03
90 5.63938 6.26247 8.13835E-03
90 6.26247 6.93450 7.59884E-03
90 6.93450 7.72112 5.08922E-03
90 7.72112 8.56677 4.82126E-03
90 8.56677 9.56003 3.45949E-03
90 9.56003 10.6220 3.20609E-03
90 10.6220 11.8723 2.37102E-03
90 11.8723 13.1979 2.12950E-03
90 13.1979 14.7606 1.48253E-03
90 14.7606 16.3972 1.39579E-03
90 16.3972 18.3248 1.08317E-03
90 18.3248 20.3079 9.73081E-04
90 20.3079 22.6356 9.39209E-04
90 22.6356 25.3936 7.05923E-04
90 25.3936 28.1863 6.87006E-04
90 28.1863 31.4746 5.59682E-04
90 31.4746 35.3860 3.86887E-04
90 35.3860 39.2434 3.69528E-04
90 39.2434 43.7836 3.30492E-04
90 43.7836 49.1828 2.38907E-04
90 49.1828 55.6784 1.41974E-04
90 55.6784 61.8817 1.45229E-04
90 61.8817 69.2237 1.07810E-04
90 69.2237 78.0139 8.79603E-05
90 78.0139 88.6777 3.76562E-05
90 88.6777 98.2588 4.35893E-05
90 98.2588 109.577 3.53820E-05
90 109.577 123.108 2.09747E-05
90 123.108 139.507 1.22877E-05
\END;
/*===================================================================*/
|