/* 2005-02-24 FILE IS GENERATED BY HENDEL */ \\BIB,1[9; D#=D1858; TITLE=/Measurement of neutrons from thick Fe target bombarded by 210 MeV protons/; ATH=(S.YONAI'1', T.KUROSAWA'2', H.IWASE'1', H.YASHIMA'1', Y.UWAMINO'3', T.NAKAMURA'1'); INST-ATH=(2JPNTOH'1', 2JPNAIS'2', 2JPNIPC'3'); /* '1' Cyclotron and Radioisotope Center (CYRIC) */ REF=NIM/A; VLP=515(2003)733; RCTS=FE(P,N)X; PHQS=(ENGY-SPEC, ANGL-DSTRN, N-MLT); \\EXP,1[9; /* 2003-12-16 : Compiled */ ENR=NAT; CHM=ELM; PHYS-FORM=SLD'4'; /* '4' Covered with aluminium foil to absorb secondary electorons emitting from the target */ THK-TGT=XMG/CM**2'5'; /* '5' 24 mm diameter by 55 mm thickness, which can stop the incident protons completely */ POL-TGT=0%; ALGN-TGT=0%; ACC=CYC'6'; /* '6' Ring Cyclotron */ INST-ACC=2JPNIPC; INC-ENGY-LAB=210MEV; POL-PRJ=0%; DET-PARTCL=N; COINC=NO; ANT-COINC=NO; DET-SYS=(SCT'7',SCT'8',EDE'9',TOF'10'); /* '7' NE213 liquid scintillator used as E-counter and ToF start signal for neutron energy measurement. Calibration was performed to convert light output into MeV electron equivalent using 60Co and 241Am-Be gamma-ray sources. */ /* '8' NE102A liquid scintillator used as Delta E counter */ /* '9' To eliminate charged particles */ /* '10' To measure emitted neutron energy (Chopper trigger signal from the cyclotron was used as the stop signal for ToF measurement). Energy resolution of ToF experiment is shown in Fig.6 as a function of neutron energy. */ /* Experimental Method: - Particle identification by 'E/Delta E' measurement (To eliminate charged particles) - Time-of-flight (To measure emitted neutron energy (Chopper trigger signal from the cyclotron was used as the stop signal for ToF measurement). Energy resolution of ToF experiment is shown in Fig.6 as a function of neutron energy.) - Beam current integrated */ \\EXP,1; RCT=FE(P,N)X; PHQ=ENGY-SPEC; ANL=INCASC'11'; /* '11' MCNPX [L.S.Waters(Ed.) MCNPX User's Manual Version 2.4.0, LA-CP-02-408, LANL, 2002] and NMTC/JAM [K.Niita et al., Nucl. Instr. Meth. B184(2001)406]. */ \\DATA,1; INC-ENGY-LAB=210MEV; SYS-ERR=(<5%'12',<2%'13',<5%'14',<18%'15',X%'16'); /* '12' Maximum normalization uncertainty in the beam current measured with a current integrator */ /* '13' Maximum uncertainty in the solid angle dominated by the uncertainty in the flight path length of neutron */ /* '14' Maximum uncertainty in neutron energy correction factor in terms of absorption and scattering between target and detector */ /* '15' Maximum uncertainty in total normalization */ /* '16' Uncertainty in the calculated detection efficiency is from 4% to 6% in the energy region below 38.3 MeV, and within 10% in the energy region above 38.3 MeV. */ EMT=N; THTL=0DEG; \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE DELTA-DN/DOMEGA/DE'17' (MEV) (MEV) (1/SR/MEV/PARTCL) (1/SR/MEV/PARTCL) 4.693 5.241 1.85E-03 +-2.87E-05 5.241 5.852 1.67E-03 +-2.38E-05 5.852 6.536 1.39E-03 +-1.97E-05 6.536 7.299 1.34E-03 +-1.80E-05 7.299 8.151 1.01E-03 +-1.51E-05 8.151 9.103 1.01E-03 +-1.43E-05 9.103 10.17 8.91E-04 +-1.27E-05 10.17 11.35 7.85E-04 +-1.14E-05 11.35 12.68 6.37E-04 +-9.85E-06 12.68 14.16 5.55E-04 +-8.97E-06 14.16 15.81 5.23E-04 +-8.39E-06 15.81 17.66 4.96E-04 +-7.82E-06 17.66 19.72 4.91E-04 +-7.40E-06 19.72 22.02 4.94E-04 +-6.95E-06 22.02 24.59 5.05E-04 +-6.52E-06 24.59 27.46 4.88E-04 +-6.01E-06 27.46 30.67 4.69E-04 +-5.58E-06 30.67 34.25 4.73E-04 +-5.32E-06 34.25 38.25 4.71E-04 +-5.10E-06 38.25 42.72 4.56E-04 +-2.10E-06 42.72 47.7 4.44E-04 +-1.90E-06 47.7 53.27 4.19E-04 +-1.67E-06 53.27 59.49 4.29E-04 +-1.56E-06 59.49 66.44 4.15E-04 +-1.43E-06 66.44 74.2 3.99E-04 +-1.33E-06 74.2 82.86 4.08E-04 +-1.30E-06 82.86 92.54 3.89E-04 +-1.24E-06 92.54 103.3 3.86E-04 +-1.21E-06 103.3 115.4 3.61E-04 +-1.16E-06 115.4 128.9 3.74E-04 +-1.17E-06 128.9 143.9 3.38E-04 +-1.10E-06 143.9 160.7 3.10E-04 +-1.05E-06 160.7 179.5 2.70E-04 +-9.74E-07 179.5 200.5 1.79E-04 +-7.92E-07 200.5 223.9 2.82E-05 +-3.12E-07 \END; /* Data (Fig. 8, p739 in reference) received by e-mail from S.Yonai (2003.12.8) */ /* '17' Statistical error */ \\EXP,2; RCT=FE(P,N)X; PHQ=ENGY-SPEC; ANL=INCASC'18'; /* '18' MCNPX [L.S.Waters(Ed.) MCNPX User's Manual Version 2.4.0, LA-CP-02-408, LANL, 2002] and NMTC/JAM [K.Niita et al., Nucl. Instr. Meth. B184(2001)406]. */ \\DATA,2; INC-ENGY-LAB=210MEV; SYS-ERR=(<5%'19',<2%'20',<5%'21',<18%'22',X%'23'); /* '19' Maximum normalization uncertainty in the beam current measured with a current integrator */ /* '20' Maximum uncertainty in the solid angle dominated by the uncertainty in the flight path length of neutron */ /* '21' Maximum uncertainty in neutron energy correction factor in terms of absorption and scattering between target and detector */ /* '22' Maximum uncertainty in total normalization */ /* '23' Uncertainty in the calculated detection efficiency is from 4% to 6% in the energy region below 38.3 MeV, and within 10% in the energy region above 38.3 MeV. */ EMT=N; THTL=7.5DEG; \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE DELTA-DN/DOMEGA/DE'24' (MEV) (MEV) (1/SR/MEV/PARTCL) (1/SR/MEV/PARTCL) 4.693 5.241 1.28E-03 +-2.12E-05 5.241 5.852 1.28E-03 +-1.86E-05 5.852 6.536 1.12E-03 +-1.58E-05 6.536 7.299 1.11E-03 +-1.46E-05 7.299 8.151 8.40E-04 +-1.22E-05 8.151 9.103 8.50E-04 +-1.17E-05 9.103 10.17 7.60E-04 +-1.04E-05 10.17 11.35 6.78E-04 +-9.42E-06 11.35 12.68 5.43E-04 +-8.09E-06 12.68 14.16 4.68E-04 +-7.33E-06 14.16 15.81 4.42E-04 +-6.86E-06 15.81 17.66 4.15E-04 +-6.37E-06 17.66 19.72 4.08E-04 +-6.00E-06 19.72 22.02 4.17E-04 +-5.68E-06 22.02 24.59 4.30E-04 +-5.35E-06 24.59 27.46 4.18E-04 +-4.95E-06 27.46 30.67 4.03E-04 +-4.61E-06 30.67 34.25 4.06E-04 +-4.39E-06 34.25 38.25 4.03E-04 +-4.20E-06 38.25 42.72 3.77E-04 +-1.70E-06 42.72 47.7 3.75E-04 +-1.55E-06 47.7 53.27 3.52E-04 +-1.36E-06 53.27 59.49 3.58E-04 +-1.27E-06 59.49 66.44 3.46E-04 +-1.16E-06 66.44 74.2 3.33E-04 +-1.08E-06 74.2 82.86 3.40E-04 +-1.06E-06 82.86 92.54 3.28E-04 +-1.01E-06 92.54 103.3 3.25E-04 +-9.89E-07 103.3 115.4 3.00E-04 +-9.38E-07 115.4 128.9 3.08E-04 +-9.45E-07 128.9 143.9 2.73E-04 +-8.84E-07 143.9 160.7 2.45E-04 +-8.30E-07 160.7 179.5 1.95E-04 +-7.36E-07 179.5 200.5 8.58E-05 +-4.83E-07 200.5 223.9 5.94E-06 +-1.25E-07 \END; /* Data (Fig. 8, p739 in reference) received by e-mail from S.Yonai (2003.12.8) */ /* '24' Statistical error */ \\EXP,3; RCT=FE(P,N)X; PHQ=ENGY-SPEC; ANL=INCASC'25'; /* '25' MCNPX [L.S.Waters(Ed.) MCNPX User's Manual Version 2.4.0, LA-CP-02-408, LANL, 2002] and NMTC/JAM [K.Niita et al., Nucl. Instr. Meth. B184(2001)406]. */ \\DATA,3; INC-ENGY-LAB=210MEV; SYS-ERR=(<5%'26',<2%'27',<5%'28',<18%'29',X%'30'); /* '26' Maximum normalization uncertainty in the beam current measured with a current integrator */ /* '27' Maximum uncertainty in the solid angle dominated by the uncertainty in the flight path length of neutron */ /* '28' Maximum uncertainty in neutron energy correction factor in terms of absorption and scattering between target and detector */ /* '29' Maximum uncertainty in total normalization */ /* '30' Uncertainty in the calculated detection efficiency is from 4% to 6% in the energy region below 38.3 MeV, and within 10% in the energy region above 38.3 MeV. */ EMT=N; THTL=15DEG; \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE DELTA-DN/DOMEGA/DE'31' (MEV) (MEV) (1/SR/MEV/PARTCL) (1/SR/MEV/PARTCL) 4.693 5.241 1.21E-03 +-2.04E-05 5.241 5.852 1.20E-03 +-1.79E-05 5.852 6.536 1.05E-03 +-1.51E-05 6.536 7.299 1.04E-03 +-1.40E-05 7.299 8.151 7.89E-04 +-1.17E-05 8.151 9.103 7.85E-04 +-1.11E-05 9.103 10.17 7.05E-04 +-9.94E-06 10.17 11.35 6.17E-04 +-8.89E-06 11.35 12.68 4.86E-04 +-7.58E-06 12.68 14.16 4.34E-04 +-6.99E-06 14.16 15.81 4.10E-04 +-6.55E-06 15.81 17.66 3.85E-04 +-6.08E-06 17.66 19.72 3.81E-04 +-5.75E-06 19.72 22.02 3.82E-04 +-5.39E-06 22.02 24.59 3.95E-04 +-5.08E-06 24.59 27.46 3.80E-04 +-4.68E-06 27.46 30.67 3.69E-04 +-4.37E-06 30.67 34.25 3.73E-04 +-4.17E-06 34.25 38.25 3.67E-04 +-3.97E-06 38.25 42.72 3.45E-04 +-1.62E-06 42.72 47.7 3.41E-04 +-1.47E-06 47.7 53.27 3.22E-04 +-1.29E-06 53.27 59.49 3.24E-04 +-1.20E-06 59.49 66.44 3.15E-04 +-1.10E-06 66.44 74.2 3.03E-04 +-1.02E-06 74.2 82.86 3.10E-04 +-1.00E-06 82.86 92.54 2.94E-04 +-9.52E-07 92.54 103.3 2.90E-04 +-9.28E-07 103.3 115.4 2.67E-04 +-8.78E-07 115.4 128.9 2.66E-04 +-8.72E-07 128.9 143.9 2.22E-04 +-7.91E-07 143.9 160.7 1.80E-04 +-7.06E-07 160.7 179.5 1.12E-04 +-5.53E-07 179.5 200.5 3.88E-05 +-3.23E-07 200.5 223.9 3.02E-06 +-8.88E-08 \END; /* Data (Fig. 8, p739 in reference) received by e-mail from S.Yonai (2003.12.8) */ /* '31' Statistical error */ \\EXP,4; RCT=FE(P,N)X; PHQ=ENGY-SPEC; ANL=INCASC'32'; /* '32' MCNPX [L.S.Waters(Ed.) MCNPX User's Manual Version 2.4.0, LA-CP-02-408, LANL, 2002] and NMTC/JAM [K.Niita et al., Nucl. Instr. Meth. B184(2001)406]. */ \\DATA,4; INC-ENGY-LAB=210MEV; SYS-ERR=(<5%'33',<2%'34',<5%'35',<18%'36',X%'37'); /* '33' Maximum normalization uncertainty in the beam current measured with a current integrator */ /* '34' Maximum uncertainty in the solid angle dominated by the uncertainty in the flight path length of neutron */ /* '35' Maximum uncertainty in neutron energy correction factor in terms of absorption and scattering between target and detector */ /* '36' Maximum uncertainty in total normalization */ /* '37' Uncertainty in the calculated detection efficiency is from 4% to 6% in the energy region below 38.3 MeV, and within 10% in the energy region above 38.3 MeV. */ EMT=N; THTL=30DEG; \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE DELTA-DN/DOMEGA/DE'38' (MEV) (MEV) (1/SR/MEV/PARTCL) (1/SR/MEV/PARTCL) 4.693 5.241 1.52E-03 +-2.98E-05 5.241 5.852 1.51E-03 +-2.60E-05 5.852 6.536 1.29E-03 +-2.18E-05 6.536 7.299 1.29E-03 +-2.02E-05 7.299 8.151 9.55E-04 +-1.67E-05 8.151 9.103 9.32E-04 +-1.57E-05 9.103 10.17 8.10E-04 +-1.39E-05 10.17 11.35 6.72E-04 +-1.21E-05 11.35 12.68 5.47E-04 +-1.05E-05 12.68 14.16 4.94E-04 +-9.70E-06 14.16 15.81 4.46E-04 +-8.89E-06 15.81 17.66 4.17E-04 +-8.23E-06 17.66 19.72 4.07E-04 +-7.72E-06 19.72 22.02 4.03E-04 +-7.20E-06 22.02 24.59 4.08E-04 +-6.72E-06 24.59 27.46 3.97E-04 +-6.23E-06 27.46 30.67 3.74E-04 +-5.73E-06 30.67 34.25 3.70E-04 +-5.41E-06 34.25 38.25 3.64E-04 +-5.15E-06 38.25 42.72 3.43E-04 +-2.09E-06 42.72 47.7 3.33E-04 +-1.89E-06 47.7 53.27 3.06E-04 +-1.64E-06 53.27 59.49 2.98E-04 +-1.50E-06 59.49 66.44 2.82E-04 +-1.36E-06 66.44 74.2 2.67E-04 +-1.25E-06 74.2 82.86 2.66E-04 +-1.21E-06 82.86 92.54 2.47E-04 +-1.14E-06 92.54 103.3 2.34E-04 +-1.08E-06 103.3 115.4 2.02E-04 +-9.95E-07 115.4 128.9 1.86E-04 +-9.49E-07 128.9 143.9 1.39E-04 +-8.14E-07 143.9 160.7 9.46E-05 +-6.65E-07 160.7 179.5 4.96E-05 +-4.78E-07 179.5 200.5 1.52E-05 +-2.63E-07 200.5 223.9 1.09E-06 +-6.94E-08 \END; /* Data (Fig. 9, p740 in reference) received by e-mail from S.Yonai (2003.12.8) */ /* '38' Statistical error */ \\EXP,5; RCT=FE(P,N)X; PHQ=ENGY-SPEC; ANL=INCASC'39'; /* '39' MCNPX [L.S.Waters(Ed.) MCNPX User's Manual Version 2.4.0, LA-CP-02-408, LANL, 2002] and NMTC/JAM [K.Niita et al., Nucl. Instr. Meth. B184(2001)406]. */ \\DATA,5; INC-ENGY-LAB=210MEV; SYS-ERR=(<5%'40',<2%'41',<5%'42',<18%'43',X%'44'); /* '40' Maximum normalization uncertainty in the beam current measured with a current integrator */ /* '41' Maximum uncertainty in the solid angle dominated by the uncertainty in the flight path length of neutron */ /* '42' Maximum uncertainty in neutron energy correction factor in terms of absorption and scattering between target and detector */ /* '43' Maximum uncertainty in total normalization */ /* '44' Uncertainty in the calculated detection efficiency is from 4% to 6% in the energy region below 38.3 MeV, and within 10% in the energy region above 38.3 MeV. */ EMT=N; THTL=60DEG; \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE DELTA-DN/DOMEGA/DE'45' (MEV) (MEV) (1/SR/MEV/PARTCL) (1/SR/MEV/PARTCL) 4.693 5.241 1.56E-03 +-1.08E-05 5.241 5.852 1.45E-03 +-9.13E-06 5.852 6.536 1.20E-03 +-7.53E-06 6.536 7.299 1.16E-03 +-6.86E-06 7.299 8.151 8.18E-04 +-5.54E-06 8.151 9.103 7.76E-04 +-5.14E-06 9.103 10.17 6.35E-04 +-4.39E-06 10.17 11.35 5.03E-04 +-3.73E-06 11.35 12.68 4.39E-04 +-3.35E-06 12.68 14.16 3.81E-04 +-3.05E-06 14.16 15.81 3.40E-04 +-2.77E-06 15.81 17.66 3.03E-04 +-2.51E-06 17.66 19.72 2.78E-04 +-2.28E-06 19.72 22.02 2.69E-04 +-2.11E-06 22.02 24.59 2.59E-04 +-1.92E-06 24.59 27.46 2.39E-04 +-1.73E-06 27.46 30.67 2.18E-04 +-1.56E-06 30.67 34.25 2.05E-04 +-1.44E-06 34.25 38.25 1.89E-04 +-1.33E-06 38.25 42.72 1.48E-04 +-1.76E-06 42.72 47.7 1.42E-04 +-1.58E-06 47.7 53.27 1.19E-04 +-1.30E-06 53.27 59.49 1.08E-04 +-1.15E-06 59.49 66.44 9.26E-05 +-9.91E-07 66.44 74.2 7.80E-05 +-8.61E-07 74.2 82.86 6.68E-05 +-7.73E-07 82.86 92.54 5.17E-05 +-6.61E-07 92.54 103.3 3.85E-05 +-5.60E-07 103.3 115.4 2.53E-05 +-4.47E-07 115.4 128.9 1.61E-05 +-3.55E-07 128.9 143.9 7.80E-06 +-2.45E-07 143.9 160.7 3.07E-06 +-1.52E-07 160.7 179.5 9.19E-07 +-8.27E-08 179.5 200.5 2.75E-07 +-4.53E-08 \END; /* Data (Fig. 9, p740 in reference) received by e-mail from S.Yonai (2003.12.8) */ /* '45' Statistical error */ \\EXP,6; RCT=FE(P,N)X; PHQ=ENGY-SPEC; ANL=INCASC'46'; /* '46' MCNPX [L.S.Waters(Ed.) MCNPX User's Manual Version 2.4.0, LA-CP-02-408, LANL, 2002] and NMTC/JAM [K.Niita et al., Nucl. Instr. Meth. B184(2001)406]. */ \\DATA,6; INC-ENGY-LAB=210MEV; SYS-ERR=(<5%'47',<2%'48',<5%'49',<18%'50',X%'51'); /* '47' Maximum normalization uncertainty in the beam current measured with a current integrator */ /* '48' Maximum uncertainty in the solid angle dominated by the uncertainty in the flight path length of neutron */ /* '49' Maximum uncertainty in neutron energy correction factor in terms of absorption and scattering between target and detector */ /* '50' Maximum uncertainty in total normalization */ /* '51' Uncertainty in the calculated detection efficiency is from 4% to 6% in the energy region below 38.3 MeV, and within 10% in the energy region above 38.3 MeV. */ EMT=N; THTL=90DEG; \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE DELTA-DN/DOMEGA/DE'52' (MEV) (MEV) (1/SR/MEV/PARTCL) (1/SR/MEV/PARTCL) 4.693 5.241 1.48E-03 +-2.15E-05 5.241 5.852 1.31E-03 +-1.76E-05 5.852 6.536 1.06E-03 +-1.43E-05 6.536 7.299 9.65E-04 +-1.27E-05 7.299 8.151 6.60E-04 +-1.01E-05 8.151 9.103 6.00E-04 +-9.21E-06 9.103 10.17 4.72E-04 +-7.73E-06 10.17 11.35 3.80E-04 +-6.63E-06 11.35 12.68 3.17E-04 +-5.84E-06 12.68 14.16 2.68E-04 +-5.24E-06 14.16 15.81 2.48E-04 +-4.86E-06 15.81 17.66 1.97E-04 +-4.16E-06 17.66 19.72 1.73E-04 +-3.70E-06 19.72 22.02 1.57E-04 +-3.30E-06 22.02 24.59 1.42E-04 +-2.90E-06 24.59 27.46 1.23E-04 +-2.54E-06 27.46 30.67 1.05E-04 +-2.21E-06 30.67 34.25 9.04E-05 +-1.95E-06 34.25 38.25 7.67E-05 +-1.73E-06 38.25 42.72 5.97E-05 +-6.33E-07 42.72 47.7 4.80E-05 +-5.19E-07 47.7 53.27 3.54E-05 +-4.03E-07 53.27 59.49 2.70E-05 +-3.26E-07 59.49 66.44 1.89E-05 +-2.55E-07 66.44 74.2 1.33E-05 +-2.03E-07 74.2 82.86 8.98E-06 +-1.62E-07 82.86 92.54 5.45E-06 +-1.23E-07 92.54 103.3 3.19E-06 +-9.37E-08 103.3 115.4 1.60E-06 +-6.67E-08 115.4 128.9 7.81E-07 +-4.74E-08 128.9 143.9 3.20E-07 +-3.27E-08 143.9 160.7 1.48E-07 +-2.32E-08 160.7 179.5 7.86E-08 +-1.86E-08 \END; /* Data (Fig. 10, p741 in reference) received by e-mail from S.Yonai (2003.12.8) */ /* '52' Statistical error */ \\EXP,7; RCT=FE(P,N)X; PHQ=ENGY-SPEC; ANL=INCASC'53'; /* '53' MCNPX [L.S.Waters(Ed.) MCNPX User's Manual Version 2.4.0, LA-CP-02-408, LANL, 2002] and NMTC/JAM [K.Niita et al., Nucl. Instr. Meth. B184(2001)406]. */ \\DATA,7; INC-ENGY-LAB=210MEV; SYS-ERR=(<5%'54',<2%'55',<5%'56',<18%'57',X%'58'); /* '54' Maximum normalization uncertainty in the beam current measured with a current integrator */ /* '55' Maximum uncertainty in the solid angle dominated by the uncertainty in the flight path length of neutron */ /* '56' Maximum uncertainty in neutron energy correction factor in terms of absorption and scattering between target and detector */ /* '57' Maximum uncertainty in total normalization */ /* '58' Uncertainty in the calculated detection efficiency is from 4% to 6% in the energy region below 38.3 MeV, and within 10% in the energy region above 38.3 MeV. */ EMT=N; THTL=110DEG; \DATA; ENGY-EMT-LAB-MIN ENGY-EMT-LAB-MAX DN/DOMEGA/DE DELTA-DN/DOMEGA/DE'59' (MEV) (MEV) (1/SR/MEV/PARTCL) (1/SR/MEV/PARTCL) 4.693 5.241 1.31E-03 +-2.03E-05 5.241 5.852 1.16E-03 +-1.67E-05 5.852 6.536 9.19E-04 +-1.34E-05 6.536 7.299 8.31E-04 +-1.19E-05 7.299 8.151 5.60E-04 +-9.45E-06 8.151 9.103 5.04E-04 +-8.53E-06 9.103 10.17 3.92E-04 +-7.14E-06 10.17 11.35 3.16E-04 +-6.13E-06 11.35 12.68 2.58E-04 +-5.36E-06 12.68 14.16 2.13E-04 +-4.76E-06 14.16 15.81 2.13E-04 +-4.57E-06 15.81 17.66 1.47E-04 +-3.67E-06 17.66 19.72 1.26E-04 +-3.23E-06 19.72 22.02 1.08E-04 +-2.80E-06 22.02 24.59 9.43E-05 +-2.42E-06 24.59 27.46 7.74E-05 +-2.06E-06 27.46 30.67 6.10E-05 +-1.74E-06 30.67 34.25 5.03E-05 +-1.50E-06 34.25 38.25 4.08E-05 +-1.30E-06 38.25 42.72 2.86E-05 +-4.43E-07 42.72 47.7 2.17E-05 +-3.55E-07 47.7 53.27 1.45E-05 +-2.63E-07 53.27 59.49 1.09E-05 +-2.13E-07 59.49 66.44 7.04E-06 +-1.61E-07 66.44 74.2 4.38E-06 +-1.22E-07 74.2 82.86 2.71E-06 +-9.52E-08 82.86 92.54 1.42E-06 +-7.07E-08 92.54 103.3 8.22E-07 +-5.61E-08 103.3 115.4 2.70E-07 +-3.96E-08 115.4 128.9 1.10E-07 +-3.33E-08 128.9 143.9 7.10E-08 +-2.93E-08 143.9 160.7 3.94E-08 +-2.64E-08 \END; /* Data (Fig. 10, p741 in reference) received by e-mail from S.Yonai (2003.12.8) */ /* '59' Statistical error */ \\EXP,8; RCT=FE(P,N)X; PHQ=ANGL-DSTRN; ANL=INCASC'60'; /* '60' MCNPX [L.S.Waters(Ed.) MCNPX User's Manual Version 2.4.0, LA-CP-02-408, LANL, 2002] and NMTC/JAM [K.Niita et al., Nucl. Instr. Meth. B184(2001)406]. */ /* Analysis: - Integration of energy distribution (Integration for energy range above 5 MeV) */ \\DATA,8; INC-ENGY-LAB=210MEV; SYS-ERR=(<5%'61',<2%'62',<5%'63',<18%'64',X%'65'); /* '61' Maximum normalization uncertainty in the beam current measured with a current integrator */ /* '62' Maximum uncertainty in the solid angle dominated by the uncertainty in the flight path length of neutron */ /* '63' Maximum uncertainty in neutron energy correction factor in terms of absorption and scattering between target and detector */ /* '64' Maximum uncertainty in total normalization */ /* '65' Uncertainty in the calculated detection efficiency is from 4% to 6% in the energy region below 38.3 MeV, and within 10% in the energy region above 38.3 MeV. */ EMT=N; ENGY-EMT-LAB-MIN=5.0MEV'66'; /* '66' Lower limit energy to obtain double differential multiplicity integrated over neutron energy */ \DATA; THTL DN/DOMEGA DELTA-DN/DOMEGA'67' (DEG) (1/SR/PARTCL) (1/SR/PARTCL) 0 7.64E-02 +-8.34E-05 7.5 6.12E-02 +-6.69E-05 15 5.23E-02 +-6.21E-05 30 4.53E-02 +-7.96E-05 60 1.88E-02 +-3.09E-05 90 1.00E-02 +-3.56E-05 110 7.34E-03 +-3.16E-05 \END; /* Data (Fig. 11, p742 in reference) received by e-mail from S.Yonai (2003.12.8) */ /* '67' Statistical error */ \\EXP,9; RCT=FE(P,N)X; PHQ=N-MLT; /* Analysis: - Integration of energy distribution (Integrated over energy range above 5 MeV) - Integration of angular distribution (Integrated over whole angular range) */ \\DATA,9; INC-ENGY-LAB=210MEV; SYS-ERR=(<5%'68',<2%'69',<5%'70',<18%'71',X%'72'); /* '68' Maximum normalization uncertainty in the beam current measured with a current integrator */ /* '69' Maximum uncertainty in the solid angle dominated by the uncertainty in the flight path length of neutron */ /* '70' Maximum uncertainty in neutron energy correction factor in terms of absorption and scattering between target and detector */ /* '71' Maximum uncertainty in total normalization */ /* '72' Uncertainty in the calculated detection efficiency is from 4% to 6% in the energy region below 38.3 MeV, and within 10% in the energy region above 38.3 MeV. */ EMT=N; ENGY-EMT-LAB-MIN=5.0MEV'73'; /* '73' Lower limit energy to obtain double differential multiplicity integrated over neutron energy */ \DATA; MLT DELTA-MLT'74' (NODIM) (NODIM) 2.06E-01 +-1.64E-04 \END; /* Data (Fig. 13, p743 in reference) received by e-mail from S.Yonai (2003.12.8) */ /* '74' Statistical error */ \\END;