/*===================================================================*/ /* NRDF D1810 Data No.19 */ /*===================================================================*/ /* Bibliography */ /*===================================================================*/ \\BIB,19; 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,19; 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(ALPHA,N)X; PHQ=ENGY-SPEC'26'; /* '26' Neutron energy spectrum */ THK-TGT=17010MG/CM**2; INC-ENGY-LAB-RANGE=100MEV/A; /*===================================================================*/ /* Descriptive Parameters */ /*===================================================================*/ \\DATA,19; 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%'27'; /* '27' 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 6.23212 6.92028 6.35145E-03 0 6.92028 7.68573 5.16859E-03 0 7.68573 8.53507 4.86533E-03 0 8.53507 9.47412 3.76108E-03 0 9.47412 10.50794 3.23316E-03 0 10.50794 11.6399 2.89648E-03 0 11.6399 12.8710 3.12752E-03 0 12.8710 14.3101 2.62196E-03 0 14.3101 15.8760 2.44063E-03 0 15.8760 17.5635 2.76232E-03 0 17.5635 19.5384 2.67076E-03 0 19.5384 21.6602 2.80254E-03 0 21.6602 24.1524 2.46256E-03 0 24.1524 26.8168 2.60440E-03 0 26.8168 29.9555 2.30380E-03 0 29.9555 33.2857 2.45238E-03 0 33.2857 37.2158 2.06000E-03 0 37.2158 41.3384 2.17999E-03 0 41.3384 46.2046 1.70401E-03 0 46.2046 51.2244 1.80898E-03 0 51.2244 57.1361 1.91484E-03 0 57.1361 64.1716 1.53525E-03 0 64.1716 71.3328 1.49888E-03 0 71.3328 79.8185 1.42877E-03 0 79.8185 89.9923 1.11737E-03 0 89.9923 100.1182 1.15092E-03 0 100.1182 112.164 1.04233E-03 0 112.164 126.679 5.55554E-04 0 126.679 140.580 4.74328E-04 0 140.580 157.101 3.64028E-04 0 157.101 177.004 2.21741E-04 0 177.004 201.371 1.08117E-04 0 201.371 223.506 6.62756E-05 0 223.506 249.994 3.39453E-05 0 249.994 282.203 1.82471E-05 7.5 4.88065 5.40350 6.88185E-03 7.5 5.40350 5.98537 6.02040E-03 7.5 5.98537 6.63198 5.44013E-03 7.5 6.63198 7.34870 4.37038E-03 7.5 7.34870 8.14092 3.92751E-03 7.5 8.14092 9.01378 3.30810E-03 7.5 9.01378 9.97087 2.83580E-03 7.5 9.97087 11.0898 2.49868E-03 7.5 11.0898 12.3204 2.24017E-03 7.5 12.3204 13.6650 2.11028E-03 7.5 13.6650 15.1227 2.25758E-03 7.5 15.1227 16.8289 1.95074E-03 7.5 16.8289 18.6766 1.96439E-03 7.5 18.6766 20.6545 2.20530E-03 7.5 20.6545 22.9684 2.02361E-03 7.5 22.9684 25.4316 2.08284E-03 7.5 25.4316 28.3201 1.81865E-03 7.5 28.3201 31.3698 2.00683E-03 7.5 31.3698 34.9501 1.67121E-03 7.5 34.9501 38.6849 1.82354E-03 7.5 38.6849 43.0669 1.69006E-03 7.5 43.0669 48.2591 1.36076E-03 7.5 48.2591 53.6368 1.59057E-03 7.5 53.6368 59.9975 1.16616E-03 7.5 59.9975 66.4298 1.31883E-03 7.5 66.4298 73.9986 1.26252E-03 7.5 73.9986 83.0008 9.86065E-04 7.5 83.0008 91.8850 1.01349E-03 7.5 91.8850 102.3587 8.16735E-04 7.5 102.3587 114.848 6.54705E-04 7.5 114.848 129.941 3.47682E-04 7.5 129.941 144.439 2.91850E-04 7.5 144.439 161.724 1.81671E-04 7.5 161.724 182.626 1.10287E-04 7.5 182.626 208.332 3.02626E-05 7.5 208.332 231.794 1.34060E-05 7.5 231.794 260.012 1.00069E-05 15 4.54520 5.03847 7.83723E-03 15 5.03847 5.57520 6.98980E-03 15 5.57520 6.20288 5.85432E-03 15 6.20288 6.88601 4.48956E-03 15 6.88601 7.62244 4.05062E-03 15 7.62244 8.48422 3.08510E-03 15 8.48422 9.41017 2.82190E-03 15 9.41017 10.49719 2.22618E-03 15 10.49719 11.6587 2.01233E-03 15 11.6587 13.0257 1.76973E-03 15 13.0257 14.4743 1.81644E-03 15 14.4743 16.1809 1.55702E-03 15 16.1809 17.9674 1.78152E-03 15 17.9674 20.0704 1.55147E-03 15 20.0704 22.2328 1.73007E-03 15 22.2328 24.7696 1.59819E-03 15 24.7696 27.7738 1.21827E-03 15 27.7738 30.8140 1.33947E-03 15 30.8140 34.3923 1.20192E-03 15 34.3923 38.6462 9.11058E-04 15 38.6462 42.8392 9.63475E-04 15 42.8392 47.7727 8.37972E-04 15 47.7727 53.6368 7.88790E-04 15 53.6368 60.6894 5.41407E-04 15 60.6894 67.4224 6.21558E-04 15 67.4224 75.3901 6.02453E-04 15 75.3901 84.9279 4.63700E-04 15 84.9279 96.4986 2.84306E-04 15 96.4986 106.896 3.25505E-04 15 106.896 119.182 2.23864E-04 15 119.182 133.876 1.52847E-04 15 133.876 151.698 1.09538E-04 15 151.698 173.684 6.48503E-05 15 173.684 201.371 2.93141E-05 15 201.371 224.126 2.41152E-05 15 224.126 251.493 1.01865E-05 30 3.83239 4.24637 9.70915E-03 30 4.24637 4.69640 8.87966E-03 30 4.69640 5.20189 7.19567E-03 30 5.20189 5.77020 5.69411E-03 30 5.77020 6.38209 5.36564E-03 30 6.38209 7.06499 3.89178E-03 30 7.06499 7.82652 3.24019E-03 30 7.82652 8.67508 2.53167E-03 30 8.67508 9.61906 2.21792E-03 30 9.61906 10.6671 1.91379E-03 30 10.6671 11.8275 1.64988E-03 30 11.8275 13.1077 1.54493E-03 30 13.1077 14.5139 1.40116E-03 30 14.5139 16.0504 1.49675E-03 30 16.0504 17.8471 1.36897E-03 30 17.8471 19.8138 1.30824E-03 30 19.8138 21.9501 1.35364E-03 30 21.9501 24.4565 1.07268E-03 30 24.4565 27.1775 9.63885E-04 30 27.1775 30.0984 9.81694E-04 30 30.0984 33.5260 7.92258E-04 30 33.5260 37.1878 7.87817E-04 30 37.1878 41.4985 5.94222E-04 30 41.4985 46.0698 5.55048E-04 30 46.0698 51.4629 4.17607E-04 30 51.4629 57.1194 4.38696E-04 30 57.1194 63.7970 2.97580E-04 30 63.7970 70.6883 2.68570E-04 30 70.6883 78.8102 2.22537E-04 30 78.8102 88.4882 1.46263E-04 30 88.4882 98.3558 1.09168E-04 30 98.3558 110.074 7.44351E-05 30 110.074 124.168 3.50351E-05 30 124.168 138.248 2.95108E-05 30 138.248 155.074 1.60560E-05 60 3.60681 4.00398 9.92441E-03 60 4.00398 4.44686 8.36581E-03 60 4.44686 4.93946 6.56592E-03 60 4.93946 5.48593 4.77116E-03 60 5.48593 6.09009 3.97689E-03 60 6.09009 6.75518 3.01705E-03 60 6.75518 7.48322 2.25420E-03 60 7.48322 8.27488 2.01327E-03 60 8.27488 9.19982 1.41460E-03 60 9.19982 10.20586 1.21074E-03 60 10.20586 11.2893 1.09829E-03 60 11.2893 12.5563 8.24970E-04 60 12.5563 13.9164 8.04658E-04 60 13.9164 15.5120 7.05237E-04 60 15.5120 17.2159 7.03151E-04 60 17.2159 19.2196 5.65885E-04 60 19.2196 21.3418 5.65451E-04 60 21.3418 23.8408 4.01021E-04 60 23.8408 26.4557 3.65973E-04 60 26.4557 29.5328 2.87463E-04 60 29.5328 32.6965 2.62141E-04 60 32.6965 36.4081 2.05495E-04 60 36.4081 40.8045 1.25695E-04 60 40.8045 45.2557 1.12200E-04 60 45.2557 50.4986 7.47893E-05 60 50.4986 56.7383 4.76821E-05 60 56.7383 62.8980 3.91071E-05 60 62.8980 70.1587 2.18982E-05 60 70.1587 78.8102 1.07048E-05 90 3.60681 4.00398 9.14206E-03 90 4.00398 4.44686 7.63637E-03 90 4.44686 4.93946 6.27560E-03 90 4.93946 5.48593 4.43849E-03 90 5.48593 6.09009 3.83011E-03 90 6.09009 6.75518 2.82693E-03 90 6.75518 7.48322 2.07700E-03 90 7.48322 8.27488 1.80166E-03 90 8.27488 9.19982 1.19742E-03 90 9.19982 10.20586 9.52419E-04 90 10.20586 11.2893 8.22576E-04 90 11.2893 12.5563 5.99627E-04 90 12.5563 13.9164 5.14744E-04 90 13.9164 15.5120 4.27334E-04 90 15.5120 17.2159 4.24412E-04 90 17.2159 19.2196 3.18316E-04 90 19.2196 21.3418 2.73623E-04 90 21.3418 23.8408 2.16086E-04 90 23.8408 26.4557 1.80182E-04 90 26.4557 29.5328 1.30002E-04 90 29.5328 32.6965 1.18777E-04 90 32.6965 36.4081 8.63657E-05 90 36.4081 40.8045 5.36952E-05 90 40.8045 45.2557 3.31162E-05 90 45.2557 50.4986 2.70545E-05 90 50.4986 56.7383 9.49861E-06 90 56.7383 62.8980 1.15885E-05 \END; /*===================================================================*/ |