|
| /*===================================================================*/
/* NRDF D1750 Data No.16 */
/*===================================================================*/
/* Bibliography */
/*===================================================================*/
\\BIB,16;
D#=D1750;
TITLE=/ Measurements of double differential neutron production cross
sections by 135 MeV/nucleon He, C, Ne and 95 MeV/nucleon Ar
ions /;
PURPOSE=/ To performe a series of systematic studies to measure the
double-differential neutron production cross sections by
heavy ions for energies from about 100 to 800 MeV/nucleon.
ATH=(H.SATO'1', T.KUROSAWA'2', H.IWASE'1', T.NAKAMURA'1', Y.UWAMINO'3',
N.NAKAO'4');
INST-ATH=(2JPNTOH'1', 2JPNETL'2', 2JPNIPC'3', 2JPNKEK'4');
/* '1' Cyclotron and Radioisotope Center */
REF=PR/C;
VLP=64(2001)034607;
RCTS=(C(4HE,N)X, 27AL(4HE,N)X, CU(4HE,N)X, PB(4HE,N)X, C(12C,N)X,
27AL(12C,N)X, CU(12C,N)X, PB(12C,N)X, C(20NE,N)X, 27AL(20NE,N)X,
CU(20NE,N)X, PB(20NE,N)X, C(40AR,N)X, 27AL(40AR,N)X,
CU(40AR,N)X, PB(40AR,N)X, H(4HE,N)X);
PHQS=(ENGY-SPEC, ANGL-DSTRN, XSECTN'5');
/* '5' The neutron production cross section integrated over
energies above 20 MeV, and also over partial angular range. */
/*===================================================================*/
/* Experimental Conditions */
/*===================================================================*/
\\EXP,16;
/* 2002-02-01 : Compiled+Checked, Sr + On */
/* 2009-08-23 : Altered, Nf. 021-052 corrected */
RTY=HEAVY-ION-RCT;
ENR=NAT'6';
/* '6' The enrichments of targets are not given in the reference.
But compiler asked T.Kurosawa. */
BAC=X;
POL-TGT=0%;
ALGN-TGT=0%;
ACC=CYC;
INST-ACC=2JPNIPC;
POL-PRJ=0%;
DET-PARTCL=N;
COINC=NO;
ANT-COINC=NO;
DET-SYS=(MAG,SCT'7',SCT'8',TOF,EDE);
/* '7' Used as Delta-E counter */
/* '8' Used as E counter, calibrated with a 60Co gamma-ray source
ERS-DET=XKEV'9';
/* '9' The energy resolutions of the measured neutron spectra are
about 3% for neutrons having energies near 100 MeV. */
EFCN-DET=/ The neutron detection efficiencies were calculated with the
Monte Carlo code of Cecil et al. for all energy ranges.
References is R. A. Cecil, B. D. Anderson, and R. Madey,
Nucl. Instrum. Methods 161, 439 (1979). /;
/* 2003-04-16 : Altered, On. SF7 modified */
RCT=PB(40AR,N)X;
PHQ=ENGY-SPEC;
CHM=ELM;
PHYS-FORM=SLD;
THK-TGT=340.2MG/CM**2;
INC-ENGY-LAB-RANGE=95MEV/A;
ANL=(MONTE-MTHD'55',MONTE-MTHD'56');
/* '55' Intranuclear-cascade and evaporation model (HIC), See
H.W.Bertini et al., ORNL-TM-4134(1974). */
/* '56' Quantum molecular dynamics model (QMD), See J.Aichelin,
PL/C 202(1991)233. */
/*===================================================================*/
/* Descriptive Parameters */
/*===================================================================*/
\\DATA,16;
INC-ENGY-LAB=95MEV/A;
STATIST-ERR=X%'57';
/* '57' The statistical uncertainties vary from 2 to 5% for the
low- to medium-energy (about 10-100 MeV) region of the spectra
and increase to about 30% at the highest energies. */
NORM=/ The total normalization uncertainty is within 17%. /;
/*===================================================================*/
/* Data Table */
/*===================================================================*/
\DATA;
THTL ENGY-EMT-LAB DSIGMA/DOMEGA/DE
(DEG) (MEV) (MB/SR/MEV)
0 10.0981 0.36818E+03
0 10.6280 0.42053E+03
0 11.1830 0.43531E+03
0 11.7650 0.46224E+03
0 12.3935 0.48457E+03
0 13.0510 0.50570E+03
0 13.7400 0.51735E+03
0 14.4855 0.52186E+03
0 15.2645 0.52299E+03
0 16.0800 0.52908E+03
0 16.9290 0.54009E+03
0 17.8135 0.52992E+03
0 18.7700 0.52954E+03
0 19.7635 0.54034E+03
0 20.7960 0.55096E+03
0 21.9125 0.57266E+03
0 23.1225 0.58666E+03
0 24.3775 0.59133E+03
0 25.6795 0.60140E+03
0 27.0905 0.61212E+03
0 28.5480 0.64598E+03
0 30.0525 0.70711E+03
0 31.6810 0.76193E+03
0 33.4485 0.81892E+03
0 35.2670 0.89042E+03
0 37.1370 0.96483E+03
0 39.1630 0.10354E+04
0 41.3630 0.11174E+04
0 43.6145 0.12352E+04
0 45.9155 0.13783E+04
0 48.4080 0.15253E+04
0 51.1155 0.16238E+04
0 54.0630 0.17503E+04
0 57.0625 0.19776E+04
0 60.1095 0.22471E+04
0 63.4155 0.25072E+04
0 67.0120 0.27295E+04
0 70.9350 0.29369E+04
0 74.8940 0.30941E+04
0 78.8760 0.31441E+04
0 83.1985 0.31241E+04
0 87.9035 0.30918E+04
0 93.0395 0.29812E+04
0 98.6610 0.25349E+04
0 104.2800 0.20189E+04
0 109.8600 0.16458E+04
0 115.9250 0.12557E+04
0 122.5450 0.89005E+03
0 129.7850 0.57919E+03
0 137.7350 0.37701E+03
0 145.5400 0.25004E+03
0 153.1300 0.17090E+03
0 161.3800 0.11462E+03
0 170.3700 0.74112E+02
0 180.2050 0.46712E+02
0 191.0050 0.29862E+02
0 202.9050 0.18517E+02
0 216.0800 0.11066E+02
0 230.7350 0.64425E+01
0 244.8600 0.35427E+01
0 258.2600 0.20512E+01
0 272.9400 0.12082E+01
0 289.0850 0.63329E+00
0 306.9250 0.33983E+00
0 326.7400 0.24135E+00
0 348.8700 0.14258E+00
30 10.0981 0.25324E+03
30 10.6280 0.27904E+03
30 11.1830 0.27549E+03
30 11.7650 0.28035E+03
30 12.3935 0.28276E+03
30 13.0510 0.27526E+03
30 13.7400 0.26864E+03
30 14.4855 0.26262E+03
30 15.2645 0.25265E+03
30 16.0800 0.24602E+03
30 16.9290 0.23657E+03
30 17.8135 0.22249E+03
30 18.7700 0.21652E+03
30 19.7635 0.20907E+03
30 20.7960 0.20158E+03
30 21.9125 0.19821E+03
30 23.1225 0.19464E+03
30 24.3775 0.18846E+03
30 25.6795 0.18237E+03
30 27.0905 0.17883E+03
30 28.5480 0.18060E+03
30 30.0525 0.18696E+03
30 31.6810 0.18893E+03
30 33.4485 0.18814E+03
30 35.2670 0.18941E+03
30 37.1370 0.18780E+03
30 39.1630 0.18411E+03
30 41.3630 0.18057E+03
30 43.6145 0.17839E+03
30 45.9155 0.17779E+03
30 48.4080 0.17495E+03
30 51.1155 0.16382E+03
30 54.0630 0.15003E+03
30 57.0625 0.14701E+03
30 60.1095 0.14785E+03
30 63.4155 0.14079E+03
30 67.0120 0.13065E+03
30 70.9350 0.12237E+03
30 74.8940 0.11484E+03
30 78.8760 0.10558E+03
30 83.1985 0.94614E+02
30 87.9035 0.84145E+02
30 93.0395 0.73520E+02
30 98.6610 0.59966E+02
30 104.2800 0.46961E+02
30 109.8600 0.40291E+02
30 115.9250 0.33771E+02
30 122.5450 0.27480E+02
30 129.7850 0.21409E+02
30 137.7350 0.16628E+02
30 145.5400 0.13246E+02
30 153.1300 0.10252E+02
30 161.3800 0.75341E+01
30 170.3700 0.54172E+01
30 180.2050 0.39378E+01
30 191.0050 0.28311E+01
30 202.9050 0.19704E+01
30 216.0800 0.10980E+01
30 230.7350 0.64006E+00
30 244.8600 0.49579E+00
30 258.2600 0.32210E+00
30 272.9400 0.18717E+00
50 10.0981 0.16632E+03
50 10.6280 0.17817E+03
50 11.1830 0.17257E+03
50 11.7650 0.17452E+03
50 12.3935 0.17437E+03
50 13.0510 0.16818E+03
50 13.7400 0.16258E+03
50 14.4855 0.15465E+03
50 15.2645 0.14395E+03
50 16.0800 0.13620E+03
50 16.9290 0.12823E+03
50 17.8135 0.11809E+03
50 18.7700 0.11185E+03
50 19.7635 0.10701E+03
50 20.7960 0.10269E+03
50 21.9125 0.99101E+02
50 23.1225 0.95890E+02
50 24.3775 0.89719E+02
50 25.6795 0.84947E+02
50 27.0905 0.82294E+02
50 28.5480 0.80692E+02
50 30.0525 0.81879E+02
50 31.6810 0.81240E+02
50 33.4485 0.78832E+02
50 35.2670 0.76401E+02
50 37.1370 0.74892E+02
50 39.1630 0.72021E+02
50 41.3630 0.68134E+02
50 43.6145 0.65435E+02
50 45.9155 0.62729E+02
50 48.4080 0.60063E+02
50 51.1155 0.54603E+02
50 54.0630 0.48426E+02
50 57.0625 0.45706E+02
50 60.1095 0.43460E+02
50 63.4155 0.40638E+02
50 67.0120 0.37485E+02
50 70.9350 0.34612E+02
50 74.8940 0.31354E+02
50 78.8760 0.27507E+02
50 83.1985 0.24073E+02
50 87.9035 0.20994E+02
50 93.0395 0.17764E+02
50 98.6610 0.13785E+02
50 104.2800 0.10628E+02
50 109.8600 0.88039E+01
50 115.9250 0.71002E+01
50 122.5450 0.55880E+01
50 129.7850 0.41874E+01
50 137.7350 0.31617E+01
50 145.5400 0.25295E+01
50 153.1300 0.19496E+01
50 161.3800 0.12913E+01
50 170.3700 0.86702E+00
50 180.2050 0.69226E+00
50 191.0050 0.48596E+00
50 202.9050 0.25252E+00
50 216.0800 0.13227E+00
50 230.7350 0.12830E+00
80 10.0981 0.10258E+03
80 10.6280 0.10621E+03
80 11.1830 0.10021E+03
80 11.7650 0.98743E+02
80 12.3935 0.96266E+02
80 13.0510 0.90887E+02
80 13.7400 0.84995E+02
80 14.4855 0.78588E+02
80 15.2645 0.73765E+02
80 16.0800 0.69077E+02
80 16.9290 0.61317E+02
80 17.8135 0.55512E+02
80 18.7700 0.52232E+02
80 19.7635 0.48836E+02
80 20.7960 0.46133E+02
80 21.9125 0.43172E+02
80 23.1225 0.40037E+02
80 24.3775 0.38019E+02
80 25.6795 0.36013E+02
80 27.0905 0.33242E+02
80 28.5480 0.31814E+02
80 30.0525 0.30540E+02
80 31.6810 0.28909E+02
80 33.4485 0.28035E+02
80 35.2670 0.26999E+02
80 37.1370 0.25057E+02
80 39.1630 0.22890E+02
80 41.3630 0.21216E+02
80 43.6145 0.19874E+02
80 45.9155 0.18617E+02
80 48.4080 0.17026E+02
80 51.1155 0.14639E+02
80 54.0630 0.12666E+02
80 57.0625 0.11747E+02
80 60.1095 0.10518E+02
80 63.4155 0.90784E+01
80 67.0120 0.78007E+01
80 70.9350 0.67316E+01
80 74.8940 0.57741E+01
80 78.8760 0.47536E+01
80 83.1985 0.40167E+01
80 87.9035 0.32787E+01
80 93.0395 0.26538E+01
80 98.6610 0.19285E+01
80 104.2800 0.12093E+01
80 109.8600 0.87046E+00
80 115.9250 0.74645E+00
80 122.5450 0.62450E+00
80 129.7850 0.42842E+00
80 137.7350 0.27841E+00
80 145.5400 0.18297E+00
80 153.1300 0.14954E+00
110 10.0981 0.74898E+02
110 10.6280 0.77548E+02
110 11.1830 0.72495E+02
110 11.7650 0.70829E+02
110 12.3935 0.68478E+02
110 13.0510 0.62703E+02
110 13.7400 0.57023E+02
110 14.4855 0.51502E+02
110 15.2645 0.46133E+02
110 16.0800 0.42104E+02
110 16.9290 0.38507E+02
110 17.8135 0.33864E+02
110 18.7700 0.29897E+02
110 19.7635 0.27547E+02
110 20.7960 0.25474E+02
110 21.9125 0.23090E+02
110 23.1225 0.20372E+02
110 24.3775 0.18186E+02
110 25.6795 0.16592E+02
110 27.0905 0.15043E+02
110 28.5480 0.13689E+02
110 30.0525 0.13044E+02
110 31.6810 0.12109E+02
110 33.4485 0.10701E+02
110 35.2670 0.95623E+01
110 37.1370 0.86189E+01
110 39.1630 0.75785E+01
110 41.3630 0.66539E+01
110 43.6145 0.60186E+01
110 45.9155 0.54433E+01
110 48.4080 0.47321E+01
110 51.1155 0.37108E+01
110 54.0630 0.28029E+01
110 57.0625 0.23806E+01
110 60.1095 0.21112E+01
110 63.4155 0.17375E+01
110 67.0120 0.13117E+01
110 70.9350 0.10521E+01
110 74.8940 0.85811E+00
110 78.8760 0.64543E+00
110 83.1985 0.50682E+00
110 87.9035 0.36841E+00
110 93.0395 0.22626E+00
\END;
/*===================================================================*/
|