ENTRY 22882 20131117 22382288200000001 SUBENT 22882001 20131117 22382288200100001 BIB 14 92 2288200100002 TITLE Measurement of neutron-induced fission cross section 2288200100003 for Bi-209, Pb-nat, Pb-208, Au-197, W-nat and Ta-181 2288200100004 in the intermediate energy region 2288200100005 AUTHOR (A.N.Smirnov,V.P.Eismont,N.P.Filatov,J.Blomgren, 2288200100006 H.Conde,A.V.Prokofiev,P.-U.Renberg,N.Olsson) 2288200100007 INSTITUTE (4RUSRI) Smirnov,Eismont,Filatov,Prokofiev 2288200100008 (2SWDUPP) Blomgren,Conde,Prokofiev,Renberg,Olsson 2288200100009 (2SWDFOI) Olsson 2288200100010 REFERENCE (J,PR/C,70,054603,2004) Main reference, data are given 2288200100011 (C,2004SANTA,,637,200405) Graphs are given 2288200100012 (J,NSTS,2,238,2002) 2288200100013 Proc.Intern.Conf.Nuclear Data for Science and 2288200100014 Technology (ND2001), Tsukuba, Japan, 7-12 October, 2288200100015 2001, Vol.1, p.238 (2002). 2288200100016 Pb isotopes, Bi, Tl relative prelim. c-s . 2288200100017 (R,ISTC-540-97,199910) For data of Hg. Also 2288200100018 nat-Pb/209-Bi,208-Pb/209-Bi,nat-Hg/209-Bi, 2288200100019 197-Au/209-Bi,nat-W/209-Bi,181-Ta/209-Bi and 2288200100020 (n,f) cross-sections. Project manager V.Eismont. 2288200100021 (R,ISTC-1309-99,200211) Project manager V.Eismont. 2288200100022 Preliminary results also in : 2288200100023 V.P.Eismont, A.V.Prokofiev, A.N.Smirnov, H.Conde, 2288200100024 K.Elmgren, N.Olsson, P.-U.Renberg. Neutron-induced 2288200100025 fission cross sections of 181-Ta, nat-W, 197-Au, 2288200100026 nat-Hg, 197-Au, 208-Pb, nat-Pb, and 209-Bi nuclei in 2288200100027 the energy range 35-175 MeV. TSL Progress Report 2288200100028 1998-1999, Ed. A.Ingemarsson, Uppsala University 2288200100029 (2000), p. 38. 2288200100030 FACILITY (CYCLO,2SWDUPP) TSL neutron beam facility, using 2288200100031 Gustaf Werner cyclotron. 2288200100032 METHOD (TOF) To determine the fraction of peak fission events,2288200100033 supplemented by model calculation (for U-238). 2288200100034 Flight path 10 m at 0 deg. 2288200100035 INC-SOURCE (P-LI7) Lithium target of enrichment 99.98% in Li-7. 2288200100036 INC-SPECT High-energy peak and low-energy tail. 2288200100037 Primary Li-7 target Proton Neutron 2288200100038 proton thickness energy energy 2288200100039 energy average average 2288200100040 in target at peak 2288200100041 (MeV) (mm) (MeV) (MeV) 2288200100042 37.96+-0.07 4 36.4 34.5 2288200100043 49.2+-0.1 4 48.2 46.3 2288200100044 69.1+-0.2 4 68.4 66.6 2288200100045 76.4+-0.2 4 75.8 73.9 2288200100046 92.1+-0.3 4 91.4 89.6 2288200100047 96.8 4 96.3 94.5 2288200100048 8 95.6 93.8 2288200100049 114.2+-2.0 8 113.1 111.3 2288200100050 136.7+-1.0 15 134.7 132.9 2288200100051 148.4+-0.6 15 146.4 144.6 2288200100052 177.3+-1.0 15 175.2 173.3 2288200100053 The peak neutron energy averaged over two production 2288200100054 modes is 94.1 MeV for primary proton energy 96.8 MeV. 2288200100055 .EN - Neutron energy at peak of counts number. 2288200100056 PART-DET (FF) 2288200100057 DETECTOR (TFBC) TFBC-based chambers with samples for count-rate 2288200100058 determination. Mosaic arrangements of 6 TFBCs of 1cm 2288200100059 diameter,placed symmetrically, perpendicular to 2288200100060 neutron beam direction. 2288200100061 6 samples of same studied nuclides or monitor were 2288200100062 placed face-to-face to detectors at distance 0.5 mm. 2288200100063 Silicon dioxide layer of 0.3mm thickness. 2288200100064 0.2-mm-thick aluminum foils as entrance and exit 2288200100065 windows . 2288200100066 Experimental setup consisted of 6 to 9 chambers 2288200100067 stacked along neutron beam direction. 2288200100068 Threshold Behavior: insensitivity to light charged 2288200100069 particles,neutrons and g-radiation, 2288200100070 real-time operation and good timing properties, 2288200100071 easy operation(no high voltage,no gases,large output 2288200100072 signals), compact design, long-term stability under 2288200100073 heavy radiation conditions. 2288200100074 .Arrangement provides output pulse height 1-2 V, 2288200100075 time resolution 2 ns (full width at half maximum). 2288200100076 (THRES) Semiconductor detectors for direct 2288200100077 alpha-spectroscopy measurements of actinide 2288200100078 contamination of samples. 2288200100079 (TRD) Low-background track detectors for alpha-activity2288200100080 measurements of actinide contamination of samples. 2288200100081 SAMPLE 1 cm**2 area containing Cf-252 as calibration sample. 2288200100082 Other samples area is 1 cm**2. 2288200100083 ADD-RES (THEO) Parameters for (n,f) cross-section calculation 2288200100084 STATUS (COREL,O1837001) Data for proton-induced reaction of 2288200100085 2004SANTA are in Entry O1837 . 2288200100086 HISTORY (20051129C) MM/SM 2288200100087 (20080512U) Reference added - SM 2288200100088 (20100112A) MM. Page of 2004SANTA corrected into 637. 2288200100089 Error of neutron energy added in Subents 002-013 from 2288200100090 tables received from author A.Smirnov 31.12.2009. 2288200100091 Subents 014-023 were added. 2288200100092 (20131117U) SD: Ref. 2001TSUKUB deleted according to 2288200100093 MEMO CP-D/791. 2288200100094 ENDBIB 92 0 2288200100095 NOCOMMON 0 0 2288200100096 ENDSUBENT 95 0 2288200199999 SUBENT 22882002 20100112 22212288200200001 BIB 7 42 2288200200002 REACTION ((83-BI-209(N,F),,SIG)/(92-U-238(N,F),,SIG)) 2288200200003 SAMPLE U-238: U3-O8 oxide, chemical composition; 2288200200004 multiple smearing deposition technique; 2288200200005 0.1-1.1 mg/cm2 sample thickness,averaged over 2288200200006 corresponding mosaic arrangement; 2288200200007 U-238 isotopic purity - 99.999%. 2288200200008 Bi-209: monoisotopic element; 2288200200009 vacuum evaporation deposition technique; 2288200200010 1.1 - 3.1 mg/cm2 sample thickness, averaged 2288200200011 over corresponding mosaic arrangement; 2288200200012 METHOD (RELFY) Fission cross-section ratio was measured with 2288200200013 pair of sandwich arrangements, stacked one after2288200200014 other in neutron beam. 2288200200015 MISC-COL (MISC1) Fraction of detected fissions at the peak 2288200200016 for U-238. 2288200200017 (MISC2) Fraction of fissions due at the peak for Bi-2092288200200018 ,obtained by employment of iterative unfolding 2288200200019 procedure. 2288200200020 COMMENT Of author A.Smirnov.The data at 160.0 MeV was published2288200200021 in J,PR/C,53,2911,1996. It's revised in this work. 2288200200022 STATUS (TABLE) From Tables III, IV of J,PR/C,70,054603,2004 . 2288200200023 Previously published data in Table 3-2 of 2288200200024 R,ISTC-1309-99,2002. 2288200200025 ERR-ANALYS Considered uncertainties: 2288200200026 (ERR-T) Total uncertainty (10-15%) 2288200200027 (ERR-1,2.,7.) Uncertainty of sample thickness 2288200200028 determination (2-7%) 2288200200029 (ERR-2,1.,2.) Uncertainty of counting statistics in 2288200200030 Cf-252 calibration(1-2%) 2288200200031 (ERR-3) Uncertainty of calculation of relative 2288200200032 detection efficiency 2288200200033 (ERR-4,,0.3) Maximal uncertainty of variation of 2288200200034 neutron beam intensity, sample thickness . 2288200200035 (ERR-5) Uncertainty of detection efficiency from 2288200200036 one sandwich to another in mosaic arrangement 2288200200037 (ERR-6,0.5,50.) Uncertainty of in-beam counting 2288200200038 statistics and subtraction of background 2288200200039 (0.5-50%) 2288200200040 (ERR-7,,4.) Maximal uncertainty of determination of 2288200200041 fraction of peak fission events 2288200200042 (ERR-8,,0.1) Maximal uncertainty of direct measurement 2288200200043 of irradiation geometry 2288200200044 ENDBIB 42 0 2288200200045 COMMON 2 3 2288200200046 ERR-3 ERR-5 2288200200047 PER-CENT PER-CENT 2288200200048 5. 0.6 2288200200049 ENDCOMMON 3 0 2288200200050 DATA 8 11 2288200200051 EN EN-ERR DATA ERR-T MISC1 MISC1-ERR 2288200200052 MISC2 MISC2-ERR 2288200200053 MEV MEV NO-DIM NO-DIM NO-DIM NO-DIM 2288200200054 NO-DIM NO-DIM 2288200200055 34.5 1.4 1.90E-4 0.20E-4 0.55 0.02 2288200200056 0.98 0.02 2288200200057 46.3 1.2 1.05E-3 0.10E-3 0.44 0.01 2288200200058 0.95 0.03 2288200200059 66.6 0.9 0.0054 0.0005 0.37 0.01 2288200200060 0.82 0.01 2288200200061 73.9 1.0 0.0082 0.0007 0.36 0.01 2288200200062 0.81 0.01 2288200200063 89.6 0.8 0.0133 0.0012 0.37 0.01 2288200200064 0.73 0.02 2288200200065 94.1 1.4 0.0157 0.0014 0.37 0.01 2288200200066 0.71 0.02 2288200200067 111.3 1.1 0.0247 0.0027 0.37 0.01 2288200200068 0.67 0.02 2288200200069 132.9 1.9 0.0307 0.0027 0.39 0.01 2288200200070 0.64 0.01 2288200200071 144.6 1.8 0.0335 0.0031 0.35 0.01 2288200200072 0.61 0.01 2288200200073 160.0 1.8 0.0415 0.0038 2288200200074 2288200200075 173.3 1.9 0.0417 0.0040 0.42 0.01 2288200200076 0.63 0.01 2288200200077 ENDDATA 26 0 2288200200078 ENDSUBENT 77 0 2288200299999 SUBENT 22882003 20100112 22212288200300001 BIB 9 24 2288200300002 REACTION (83-BI-209(N,F),,SIG) 2288200300003 SAMPLE U-238: U3-O8 chemical composition; 2288200300004 multiple smearing deposition technique; 2288200300005 0.1-1.1 mg/cm2 sample thickness,averaged over 2288200300006 corresponding mosaic arrangement; 2288200300007 U-238 isotopic purity - 99.999%. 2288200300008 Bi-209: monoisotopic element; 2288200300009 vacuum evaporation deposition technique; 2288200300010 1.1 - 3.1 mg/cm2 sample thickness, averaged 2288200300011 over corresponding mosaic arrangement; 2288200300012 METHOD (RELFY) Fission cross-section ratio was measured with 2288200300013 pair of sandwich arrangements, stacked one after2288200300014 other in neutron beam. 2288200300015 MONITOR (92-U-238(N,F),,SIG) 2288200300016 MONIT-REF (,A.D.Carlson+,R,INDC(NDS)-368,199705) 2288200300017 INC-SPECT .EN - Neutron energy at peak of counts number. 2288200300018 COMMENT Of author A.Smirnov.The data at 160.0 MeV was published2288200300019 in J,PR/C,53,2911,1996. It's revised in this work. 2288200300020 STATUS (DEP,22882002) 2288200300021 (TABLE) From Table IV of J,PR/C,70,054603,2004 . 2288200300022 ERR-ANALYS Considered uncertainties: 2288200300023 (ERR-T) Total uncertainty (10-15%) 2288200300024 (MONIT-ERR,2.,5.) Uncertainty in standard U-238(n,f) 2288200300025 cross section (2-5%) 2288200300026 ENDBIB 24 0 2288200300027 NOCOMMON 0 0 2288200300028 DATA 4 11 2288200300029 EN EN-ERR DATA ERR-T 2288200300030 MEV MEV MB MB 2288200300031 34.5 1.4 0.311 0.034 2288200300032 46.3 1.2 1.71 0.17 2288200300033 66.6 0.9 8.42 0.81 2288200300034 73.9 1.0 12.6 1.2 2288200300035 89.6 0.8 19.2 1.9 2288200300036 94.1 1.4 22.4 2.2 2288200300037 111.3 1.1 33.5 3.9 2288200300038 132.9 1.9 40.5 4.1 2288200300039 144.6 1.8 44.2 4.7 2288200300040 160.0 1.8 54.6 5.7 2288200300041 173.3 1.9 54.9 5.9 2288200300042 ENDDATA 13 0 2288200300043 ENDSUBENT 42 0 2288200399999 SUBENT 22882004 20100112 22212288200400001 BIB 6 35 2288200400002 REACTION ((82-PB-0(N,F),,SIG)/(83-BI-209(N,F),,SIG)) 2288200400003 SAMPLE Bi-209: monoisotopic element; 2288200400004 vacuum evaporation deposition technique; 2288200400005 1.1 - 3.1 mg/cm2 sample thickness, averaged 2288200400006 over corresponding mosaic arrangement. 2288200400007 Pb-nat: natural lead; 2288200400008 vacuum evaporation deposition technique; 2288200400009 1.1-2.4 mg/cm2 sample thickness, averaged 2288200400010 over corresponding mosaic arrangement. 2288200400011 METHOD (RELFY) Fission cross-section ratio was measured with2288200400012 pair of sandwich arrangements, stacked one after2288200400013 other in neutron beam. 2288200400014 INC-SPECT .EN - Neutron energy at the peak of counts number. 2288200400015 STATUS (TABLE) From Table V of J,PR/C,70,054603,2004 . 2288200400016 Previously published data in Table 3-2 of 2288200400017 R,ISTC-1309-99,2002. 2288200400018 ERR-ANALYS Considered uncertainties: 2288200400019 (ERR-T) Total uncertainty (10-15%) 2288200400020 (ERR-1,2.,7.) Uncertainty of sample thickness 2288200400021 determination (2-7%) 2288200400022 (ERR-2,1.,2.) Uncertainty of counting statistics in 2288200400023 Cf-252 calibration(1-2%) 2288200400024 (ERR-3) Uncertainty of calculation of relative 2288200400025 detection efficiency 2288200400026 (ERR-4,,0.3) Maximal uncertainty of variation of 2288200400027 neutron beam intensity, sample thickness . 2288200400028 (ERR-5) Uncertainty of detection efficiency from 2288200400029 one sandwich to another in mosaic arrangement 2288200400030 (ERR-6,0.5,50.) Uncertainty of in-beam counting 2288200400031 statistics and subtraction of background 2288200400032 (0.5-50%) 2288200400033 (ERR-7,,1.) Maximal uncertainty of determination of 2288200400034 fraction of peak fission events 2288200400035 (ERR-8,,0.1) Maximal uncertainty of direct measurement 2288200400036 of irradiation geometry 2288200400037 ENDBIB 35 0 2288200400038 COMMON 2 3 2288200400039 ERR-3 ERR-5 2288200400040 PER-CENT PER-CENT 2288200400041 5. 0.6 2288200400042 ENDCOMMON 3 0 2288200400043 DATA 4 8 2288200400044 EN EN-ERR DATA ERR-T 2288200400045 MEV MEV NO-DIM NO-DIM 2288200400046 34.5 1.4 0.15 0.07 2288200400047 46.3 1.2 0.197 0.019 2288200400048 66.6 0.9 0.306 0.023 2288200400049 73.9 1.0 0.336 0.026 2288200400050 94.1 1.4 0.383 0.028 2288200400051 132.9 1.9 0.414 0.031 2288200400052 144.6 1.8 0.452 0.034 2288200400053 173.3 1.9 0.50 0.04 2288200400054 ENDDATA 10 0 2288200400055 ENDSUBENT 54 0 2288200499999 SUBENT 22882005 20100112 22212288200500001 BIB 5 34 2288200500002 REACTION ((82-PB-208(N,F),,SIG)/(83-BI-209(N,F),,SIG)) 2288200500003 SAMPLE Bi-209: monoisotopic element; 2288200500004 vacuum evaporation deposition technique; 2288200500005 1.1 - 3.1 mg/cm2 sample thickness, averaged 2288200500006 over corresponding mosaic arrangement. 2288200500007 Pb-208: Pb-208 of 98.7% purity, 2288200500008 vacuum evaporation deposition technique; 2288200500009 1.3-2.4 mg/cm2 sample thickness, averaged 2288200500010 over corresponding mosaic arrangement. 2288200500011 METHOD (RELFY) Fission cross-section ratio was measured with 2288200500012 pair of sandwich arrangements, stacked one after2288200500013 other in neutron beam. 2288200500014 STATUS (TABLE) From Table V of J,PR/C,70,054603,2004 . 2288200500015 Previously published data in Table 3-2 of 2288200500016 R,ISTC-1309-99,2002. 2288200500017 ERR-ANALYS Considered uncertainties: 2288200500018 (ERR-T) Total uncertainty (10-15%) 2288200500019 (ERR-1,2.,7.) Uncertainty of sample thickness 2288200500020 determination (2-7%) 2288200500021 (ERR-2,1.,2.) Uncertainty of counting statistics in 2288200500022 Cf-252 calibration(1-2%) 2288200500023 (ERR-3) Uncertainty of calculation of relative 2288200500024 detection efficiency 2288200500025 (ERR-4,,0.3) Maximal uncertainty of variation of 2288200500026 neutron beam intensity, sample thickness . 2288200500027 (ERR-5) Uncertainty of detection efficiency from 2288200500028 one sandwich to another in mosaic arrangement 2288200500029 (ERR-6,0.5,50.) Uncertainty of in-beam counting 2288200500030 statistics and subtraction of background 2288200500031 (0.5-50%) 2288200500032 (ERR-7,,1.) Maximal uncertainty of determination of 2288200500033 fraction of peak fission events 2288200500034 (ERR-8,,0.1) Maximal uncertainty of direct measurement 2288200500035 of irradiation geometry 2288200500036 ENDBIB 34 0 2288200500037 COMMON 2 3 2288200500038 ERR-3 ERR-5 2288200500039 PER-CENT PER-CENT 2288200500040 5. 0.6 2288200500041 ENDCOMMON 3 0 2288200500042 DATA 4 10 2288200500043 EN EN-ERR DATA ERR-T 2288200500044 MEV MEV NO-DIM NO-DIM 2288200500045 34.5 1.4 0.028 0.006 2288200500046 46.3 1.2 0.084 0.007 2288200500047 66.6 0.9 0.208 0.016 2288200500048 73.9 1.0 0.230 0.018 2288200500049 89.6 0.8 0.252 0.020 2288200500050 94.1 1.4 0.297 0.023 2288200500051 111.3 1.1 0.301 0.026 2288200500052 132.9 1.9 0.310 0.024 2288200500053 144.6 1.8 0.39 0.03 2288200500054 173.3 1.9 0.36 0.03 2288200500055 ENDDATA 12 0 2288200500056 ENDSUBENT 55 0 2288200599999 SUBENT 22882006 20100112 22212288200600001 BIB 5 32 2288200600002 REACTION ((79-AU-197(N,F),,SIG)/(83-BI-209(N,F),,SIG)) 2288200600003 SAMPLE Bi-209: monoisotopic element; 2288200600004 vacuum evaporation deposition technique; 2288200600005 1.1 - 3.1 mg/cm2 sample thickness, averaged 2288200600006 over corresponding mosaic arrangement. 2288200600007 Au-197: monoisotopic element, 2288200600008 vacuum evaporation deposition technique; 2288200600009 2.8 mg/cm2 sample thickness, averaged over 2288200600010 corresponding mosaic arrangement. 2288200600011 METHOD (RELFY) Fission cross-section ratio was measured with 2288200600012 pair of sandwich arrangements, stacked one after2288200600013 other in neutron beam. 2288200600014 STATUS (TABLE) From Table V of J,PR/C,70,054603,2004 . 2288200600015 ERR-ANALYS Considered uncertainties: 2288200600016 (ERR-T) Total uncertainty (10-15%) 2288200600017 (ERR-1,2.,7.) Uncertainty of sample thickness 2288200600018 determination (2-7%) 2288200600019 (ERR-2,1.,2.) Uncertainty of counting statistics in 2288200600020 Cf-252 calibration(1-2%) 2288200600021 (ERR-3) Uncertainty of calculation of relative 2288200600022 detection efficiency 2288200600023 (ERR-4,,0.3) Maximal uncertainty of variation of 2288200600024 neutron beam intensity, sample thickness . 2288200600025 (ERR-5) Uncertainty of detection efficiency from 2288200600026 one sandwich to another in mosaic arrangement 2288200600027 (ERR-6,0.5,50.) Uncertainty of in-beam counting 2288200600028 statistics and subtraction of background 2288200600029 (0.5-50%) 2288200600030 (ERR-7,,1.) Maximal uncertainty of determination of 2288200600031 fraction of peak fission events 2288200600032 (ERR-8,,0.1) Maximal uncertainty of direct measurement 2288200600033 of irradiation geometry 2288200600034 ENDBIB 32 0 2288200600035 COMMON 2 3 2288200600036 ERR-3 ERR-5 2288200600037 PER-CENT PER-CENT 2288200600038 5. 0.6 2288200600039 ENDCOMMON 3 0 2288200600040 DATA 5 8 2288200600041 EN EN-ERR DATA ERR-T DATA-MAX 2288200600042 MEV MEV NO-DIM NO-DIM NO-DIM 2288200600043 34.5 1.4 0.012 2288200600044 46.3 1.2 0.060 0.011 2288200600045 66.6 0.9 0.096 0.011 2288200600046 73.9 1.0 0.096 0.010 2288200600047 94.1 1.4 0.126 0.013 2288200600048 132.9 1.9 0.151 0.017 2288200600049 144.6 1.8 0.184 0.021 2288200600050 173.3 1.9 0.187 0.023 2288200600051 ENDDATA 10 0 2288200600052 ENDSUBENT 51 0 2288200699999 SUBENT 22882007 20100112 22212288200700001 BIB 5 32 2288200700002 REACTION ((74-W-0(N,F),,SIG)/(83-BI-209(N,F),,SIG)) 2288200700003 SAMPLE Bi-209: monoisotopic element; 2288200700004 vacuum evaporation deposition technique; 2288200700005 1.1 - 3.1 mg/cm2 sample thickness, averaged 2288200700006 over corresponding mosaic arrangement. 2288200700007 W-nat : thrioxide of natural uranium, 2288200700008 vacuum evaporation deposition technique; 2288200700009 2. mg/cm2 sample thickness, averaged over 2288200700010 corresponding mosaic arrangement. 2288200700011 METHOD (RELFY) Fission cross-section ratio was measured with 2288200700012 pair of sandwich arrangements, stacked one after2288200700013 other in neutron beam. 2288200700014 STATUS (TABLE) From Table V of J,PR/C,70,054603,2004 . 2288200700015 ERR-ANALYS Considered uncertainties: 2288200700016 (ERR-T) Total uncertainty (10-15%) 2288200700017 (ERR-1,2.,7.) Uncertainty of sample thickness 2288200700018 determination (2-7%) 2288200700019 (ERR-2,1.,2.) Uncertainty of counting statistics in 2288200700020 Cf-252 calibration(1-2%) 2288200700021 (ERR-3) Uncertainty of calculation of relative 2288200700022 detection efficiency 2288200700023 (ERR-4,,0.3) Maximal uncertainty of variation of 2288200700024 neutron beam intensity, sample thickness . 2288200700025 (ERR-5) Uncertainty of detection efficiency from 2288200700026 one sandwich to another in mosaic arrangement 2288200700027 (ERR-6,0.5,50.) Uncertainty of in-beam counting 2288200700028 statistics and subtraction of background 2288200700029 (0.5-50%) 2288200700030 (ERR-7,,1.) Maximal uncertainty of determination of 2288200700031 fraction of peak fission events 2288200700032 (ERR-8,,0.1) Maximal uncertainty of direct measurement 2288200700033 of irradiation geometry 2288200700034 ENDBIB 32 0 2288200700035 COMMON 2 3 2288200700036 ERR-3 ERR-5 2288200700037 PER-CENT PER-CENT 2288200700038 5. 0.6 2288200700039 ENDCOMMON 3 0 2288200700040 DATA 5 7 2288200700041 EN EN-ERR DATA ERR-T DATA-MAX 2288200700042 MEV MEV NO-DIM NO-DIM NO-DIM 2288200700043 46.3 1.2 0.0023 2288200700044 66.6 0.9 0.0023 0.0011 2288200700045 73.9 1.0 0.0033 0.0006 2288200700046 94.1 1.4 0.0063 0.0007 2288200700047 132.9 1.9 0.0132 0.0015 2288200700048 144.6 1.8 0.0127 0.0014 2288200700049 173.3 1.9 0.019 0.002 2288200700050 ENDDATA 9 0 2288200700051 ENDSUBENT 50 0 2288200799999 SUBENT 22882008 20100112 22212288200800001 BIB 5 32 2288200800002 REACTION ((73-TA-181(N,F),,SIG)/(83-BI-209(N,F),,SIG)) 2288200800003 SAMPLE Bi-209: monoisotopic element; 2288200800004 vacuum evaporation deposition technique; 2288200800005 1.1 - 3.1 mg/cm2 sample thickness, averaged 2288200800006 over corresponding mosaic arrangement. 2288200800007 Ta-181: monoisotopic element, 2288200800008 magnetron evaporation deposition technique; 2288200800009 0.5-1.2 mg/cm2 sample thickness, averaged over2288200800010 corresponding mosaic arrangement. 2288200800011 METHOD (RELFY) Fission cross-section ratio was measured with 2288200800012 pair of sandwich arrangements, stacked one after2288200800013 other in neutron beam. 2288200800014 STATUS (TABLE) From Table V of J,PR/C,70,054603,2004 . 2288200800015 ERR-ANALYS Considered uncertainties: 2288200800016 (ERR-T) Total uncertainty (10-15%) 2288200800017 (ERR-1,2.,7.) Uncertainty of sample thickness 2288200800018 determination (2-7%) 2288200800019 (ERR-2,1.,2.) Uncertainty of counting statistics in 2288200800020 Cf-252 calibration(1-2%) 2288200800021 (ERR-3) Uncertainty of calculation of relative 2288200800022 detection efficiency 2288200800023 (ERR-4,,0.3) Maximal uncertainty of variation of 2288200800024 neutron beam intensity, sample thickness . 2288200800025 (ERR-5) Uncertainty of detection efficiency from 2288200800026 one sandwich to another in mosaic arrangement 2288200800027 (ERR-6,0.5,50.) Uncertainty of in-beam counting 2288200800028 statistics and subtraction of background 2288200800029 (0.5-50%) 2288200800030 (ERR-7,,1.) Maximal uncertainty of determination of 2288200800031 fraction of peak fission events 2288200800032 (ERR-8,,0.1) Maximal uncertainty of direct measurement 2288200800033 of irradiation geometry 2288200800034 ENDBIB 32 0 2288200800035 COMMON 2 3 2288200800036 ERR-3 ERR-5 2288200800037 PER-CENT PER-CENT 2288200800038 5. 0.6 2288200800039 ENDCOMMON 3 0 2288200800040 DATA 4 6 2288200800041 EN EN-ERR DATA ERR-T 2288200800042 MEV MEV NO-DIM NO-DIM 2288200800043 66.6 0.9 7.2E-04 2.8E-04 2288200800044 73.9 1.0 0.0016 0.0004 2288200800045 94.1 1.4 0.0028 0.0003 2288200800046 132.9 1.9 0.0059 0.0007 2288200800047 144.6 1.8 0.0066 0.0008 2288200800048 173.3 1.9 0.0076 0.0009 2288200800049 ENDDATA 8 0 2288200800050 ENDSUBENT 49 0 2288200899999 SUBENT 22882009 20100112 22212288200900001 BIB 5 7 2288200900002 REACTION (82-PB-0(N,F),,SIG) 2288200900003 MONITOR (83-BI-209(N,F),,SIG) 2288200900004 MONIT-REF (22882003,A.N.Smirnov+,J,PR/C,70,054603,2004) 2288200900005 STATUS (DEP,22882004) 2288200900006 (TABLE) From Table VI of J,PR/C,70,054603,2004 . 2288200900007 ERR-ANALYS (ERR-T) Total uncertainty includes uncertainty of 2288200900008 209-Bi(n,f) cross-section data. 2288200900009 ENDBIB 7 0 2288200900010 NOCOMMON 0 0 2288200900011 DATA 4 8 2288200900012 EN EN-ERR DATA ERR-T 2288200900013 MEV MEV MB MB 2288200900014 34.5 1.4 0.047 0.021 2288200900015 46.3 1.2 0.336 0.044 2288200900016 66.6 0.9 2.58 0.03 2288200900017 73.9 1.0 4.24 0.47 2288200900018 94.1 1.4 8.6 1.0 2288200900019 132.9 1.9 16.8 1.7 2288200900020 144.6 1.8 20.0 2.3 2288200900021 173.3 1.9 27.5 3.7 2288200900022 ENDDATA 10 0 2288200900023 ENDSUBENT 22 0 2288200999999 SUBENT 22882010 20100112 22212288201000001 BIB 6 12 2288201000002 REACTION (82-PB-208(N,F),,SIG) 2288201000003 MONITOR (83-BI-209(N,F),,SIG) 2288201000004 MONIT-REF (22882003,A.N.Smirnov+,J,PR/C,70,054603,2004) 2288201000005 COMMENT Of compiler.In the table received from author A.Smirnov2288201000006 (31.12.2009) 3 data points are little different: 2288201000007 34.5 MeV - 0.009 +- 0.006 mb, 2288201000008 89.6 MeV - 4.84 +- 0.53 mb, 2288201000009 94.1 MeV - 6.64 +- 0.76 mb. 2288201000010 STATUS (DEP,22882005) 2288201000011 (TABLE) From Table VI of J,PR/C,70,054603,2004 . 2288201000012 ERR-ANALYS (ERR-T) Total uncertainty includes uncertainty of 2288201000013 209-Bi(n,f) cross-section data. 2288201000014 ENDBIB 12 0 2288201000015 NOCOMMON 0 0 2288201000016 DATA 4 10 2288201000017 EN EN-ERR DATA ERR-T 2288201000018 MEV MEV MB MB 2288201000019 34.5 1.4 0.0087 0.0021 2288201000020 46.3 1.2 0.143 0.018 2288201000021 66.6 0.9 1.75 0.21 2288201000022 73.9 1.0 2.90 0.33 2288201000023 89.6 0.8 4.8 0.5 2288201000024 94.1 1.4 6.6 0.8 2288201000025 111.3 1.1 10.1 1.3 2288201000026 132.9 1.9 12.6 1.3 2288201000027 144.6 1.8 17.3 2.0 2288201000028 173.3 1.9 19.9 2.7 2288201000029 ENDDATA 12 0 2288201000030 ENDSUBENT 29 0 2288201099999 SUBENT 22882011 20100112 22212288201100001 BIB 5 7 2288201100002 REACTION (79-AU-197(N,F),,SIG) 2288201100003 MONITOR (83-BI-209(N,F),,SIG) 2288201100004 MONIT-REF (22882003,A.N.Smirnov+,J,PR/C,70,054603,2004) 2288201100005 STATUS (DEP,22882006) 2288201100006 (TABLE) From Table VI of J,PR/C,70,054603,2004 . 2288201100007 ERR-ANALYS (ERR-T) Total uncertainty includes uncertainty of 2288201100008 209-Bi(n,f) cross-section data. 2288201100009 ENDBIB 7 0 2288201100010 NOCOMMON 0 0 2288201100011 DATA 5 8 2288201100012 EN EN-ERR DATA ERR-T DATA-MAX 2288201100013 MEV MEV MB MB MB 2288201100014 34.5 1.4 0.0038 2288201100015 46.3 1.2 0.103 0.019 2288201100016 66.6 0.9 0.81 0.12 2288201100017 73.9 1.0 1.20 0.17 2288201100018 94.1 1.4 2.81 0.39 2288201100019 132.9 1.9 6.1 0.9 2288201100020 144.6 1.8 8.1 1.2 2288201100021 173.3 1.9 10.3 1.6 2288201100022 ENDDATA 10 0 2288201100023 ENDSUBENT 22 0 2288201199999 SUBENT 22882012 20100112 22212288201200001 BIB 5 7 2288201200002 REACTION (74-W-0(N,F),,SIG) 2288201200003 MONITOR (83-BI-209(N,F),,SIG) 2288201200004 MONIT-REF (22882003,A.N.Smirnov+,J,PR/C,70,054603,2004) 2288201200005 STATUS (DEP,22882007) 2288201200006 (TABLE) From Table VI of J,PR/C,70,054603,2004 . 2288201200007 ERR-ANALYS (ERR-T) Total uncertainty includes uncertainty of 2288201200008 209-Bi(n,f) cross-section data. 2288201200009 ENDBIB 7 0 2288201200010 NOCOMMON 0 0 2288201200011 DATA 5 7 2288201200012 EN EN-ERR DATA ERR-T DATA-MAX 2288201200013 MEV MEV MB MB MB 2288201200014 46.3 1.2 0.004 2288201200015 66.6 0.9 0.020 0.010 2288201200016 73.9 1.0 0.041 0.008 2288201200017 94.1 1.4 0.141 0.020 2288201200018 132.9 1.9 0.53 0.08 2288201200019 144.6 1.8 0.56 0.08 2288201200020 173.3 1.9 1.04 0.42 2288201200021 ENDDATA 9 0 2288201200022 ENDSUBENT 21 0 2288201299999 SUBENT 22882013 20100112 22212288201300001 BIB 5 7 2288201300002 REACTION (73-TA-181(N,F),,SIG) 2288201300003 MONITOR (83-BI-209(N,F),,SIG) 2288201300004 MONIT-REF (22882003,A.N.Smirnov+,J,PR/C,70,054603,2004) 2288201300005 STATUS (DEP,22882008) 2288201300006 (TABLE) From Table VI of J,PR/C,70,054603,2004 . 2288201300007 ERR-ANALYS (ERR-T) Total uncertainty includes uncertainty of 2288201300008 209-Bi(n,f) cross-section data. 2288201300009 ENDBIB 7 0 2288201300010 NOCOMMON 0 0 2288201300011 DATA 4 6 2288201300012 EN EN-ERR DATA ERR-T 2288201300013 MEV MEV MB MB 2288201300014 66.6 0.9 0.0061 0.0024 2288201300015 73.9 1.0 0.020 0.005 2288201300016 94.1 1.4 0.063 0.009 2288201300017 132.9 1.9 0.24 0.04 2288201300018 144.6 1.8 0.29 0.05 2288201300019 173.3 1.9 0.42 0.07 2288201300020 ENDDATA 8 0 2288201300021 ENDSUBENT 20 0 2288201399999 SUBENT 22882014 20100112 22212288201400001 BIB 5 30 2288201400002 REACTION ((82-PB-204(N,F),,SIG)/(83-BI-209(N,F),,SIG)) 2288201400003 SAMPLE Bi-209 - metallic. 2288201400004 Pb-204 sample isotopic composition: 2288201400005 Pb-208 < 0.01%, Pb-207 < 0.01%, 2288201400006 Pb-204 - (66.5+-0.6) % . 2288201400007 Deposited on the round aluminum foil backings of 2288201400008 0.1 mm thick and of 1 cm**2 area; made by vacuum 2288201400009 evaporation technique with the use of special design 2288201400010 allowing a manufacturing up to 26 targets 2288201400011 simultaneously with homogeneity not worse than 20% 2288201400012 (for different targets). 2288201400013 METHOD (RELFY) Fission cross-section ratio was measured with 2288201400014 pair of sandwich arrangements, stacked one after2288201400015 other in neutron beam. 2288201400016 STATUS (TABLE) From Table 3-2 of R,ISTC-1309-99,2002. 2288201400017 Data were received from author A.Smirnov 31.12.2009. 2288201400018 ERR-ANALYS (ERR-T) Total uncertainty . 2288201400019 (ERR-S,1.,3.) Statistical uncertainty. 2288201400020 (ERR-1) Uncertainty of chambers mosaic arrangement 2288201400021 registration efficiency. 2288201400022 (ERR-2,,1.) Maximal uncertainty of correction 2288201400023 coefficients ratio at peak. 2288201400024 (ERR-3,,1.) Maximal uncertainty of ratio of 2288201400025 registration efficiencies. 2288201400026 (ERR-4,,3.) Targets were weighted with the accuracy not2288201400027 worse than 3% with the use of precise analytical 2288201400028 balance. 2288201400029 (ERR-5,,0.0001) Upper limit of admixture of actinides 2288201400030 for lead isotopes determined by means of analysis of 2288201400031 results of measurement at 35 MeV neutrons 2288201400032 ENDBIB 30 0 2288201400033 COMMON 1 3 2288201400034 ERR-1 2288201400035 PER-CENT 2288201400036 3. 2288201400037 ENDCOMMON 3 0 2288201400038 DATA 4 9 2288201400039 EN EN-ERR DATA ERR-T 2288201400040 MEV MEV NO-DIM NO-DIM 2288201400041 34.5 1.4 1.04 0.09 2288201400042 46.3 1.2 1.06 0.05 2288201400043 66.6 0.9 1.02 0.05 2288201400044 89.6 0.8 1.06 0.08 2288201400045 94.1 1.4 0.98 0.05 2288201400046 111.3 1.1 1.06 0.09 2288201400047 132.9 1.9 1.00 0.06 2288201400048 144.6 1.8 1.02 0.07 2288201400049 173.3 1.9 1.00 0.04 2288201400050 ENDDATA 11 0 2288201400051 ENDSUBENT 50 0 2288201499999 SUBENT 22882015 20100112 22212288201500001 BIB 5 30 2288201500002 REACTION ((82-PB-206(N,F),,SIG)/(83-BI-209(N,F),,SIG)) 2288201500003 SAMPLE Bi-209 - metallic. 2288201500004 Pb-206 sample isotopic composition: 2288201500005 Pb-208 - 0.4 %, Pb-207 - 1.4 %, 2288201500006 Pb-206 - (90.4 +- 0.3) %, Pb-204 - 16.1 % . 2288201500007 Deposited on the round aluminum foil backings of 2288201500008 0.1 mm thick and of 1 cm**2 area; made by vacuum 2288201500009 evaporation technique with the use of special design 2288201500010 allowing a manufacturing up to 26 targets 2288201500011 simultaneously with homogeneity not worse than 20% 2288201500012 (for different targets). 2288201500013 METHOD (RELFY) Fission cross-section ratio was measured with 2288201500014 pair of sandwich arrangements, stacked one after2288201500015 other in neutron beam. 2288201500016 STATUS (TABLE) From Table 3-2 of R,ISTC-1309-99,2002. 2288201500017 Data were received from author A.Smirnov 31.12.2009. 2288201500018 ERR-ANALYS (ERR-T) Total uncertainty . 2288201500019 (ERR-S,1.,3.) Statistical uncertainty. 2288201500020 (ERR-1) Uncertainty of chambers mosaic arrangement 2288201500021 registration efficiency. 2288201500022 (ERR-2,,1.) Maximal uncertainty of correction 2288201500023 coefficients ratio at peak. 2288201500024 (ERR-3,,1.) Maximal uncertainty of ratio of 2288201500025 registration efficiencies. 2288201500026 (ERR-4,,3.) Targets were weighted with the accuracy not2288201500027 worse than 3% with the use of precise analytical 2288201500028 balance. 2288201500029 (ERR-5,,0.0001) Upper limit of admixture of actinides 2288201500030 for lead isotopes determined by means of analysis of 2288201500031 results of measurement at 35 MeV neutrons 2288201500032 ENDBIB 30 0 2288201500033 COMMON 1 3 2288201500034 ERR-1 2288201500035 PER-CENT 2288201500036 3. 2288201500037 ENDCOMMON 3 0 2288201500038 DATA 4 9 2288201500039 EN EN-ERR DATA ERR-T 2288201500040 MEV MEV NO-DIM NO-DIM 2288201500041 34.5 1.4 0.17 0.02 2288201500042 46.3 1.2 0.32 0.02 2288201500043 66.6 0.9 0.45 0.02 2288201500044 89.6 0.8 0.49 0.03 2288201500045 94.1 1.4 0.49 0.02 2288201500046 111.3 1.1 0.55 0.04 2288201500047 132.9 1.9 0.59 0.03 2288201500048 144.6 1.8 0.65 0.04 2288201500049 173.3 1.9 0.61 0.02 2288201500050 ENDDATA 11 0 2288201500051 ENDSUBENT 50 0 2288201599999 SUBENT 22882016 20100112 22212288201600001 BIB 5 30 2288201600002 REACTION ((82-PB-207(N,F),,SIG)/(83-BI-209(N,F),,SIG)) 2288201600003 SAMPLE Bi-209 - metallic. 2288201600004 Pb-207 sample isotopic composition: 2288201600005 Pb-208 - 0.6 %, Pb-207 - (93.2 +- 0.2) %, 2288201600006 Pb-206 - 6.7 %, Pb-204 - 7.5 % . 2288201600007 Deposited on the round aluminum foil backings of 2288201600008 0.1 mm thick and of 1 cm**2 area; made by vacuum 2288201600009 evaporation technique with the use of special design 2288201600010 allowing a manufacturing up to 26 targets 2288201600011 simultaneously with homogeneity not worse than 20% 2288201600012 (for different targets). 2288201600013 METHOD (RELFY) Fission cross-section ratio was measured with 2288201600014 pair of sandwich arrangements, stacked one after2288201600015 other in neutron beam. 2288201600016 STATUS (TABLE) From Table 3-2 of R,ISTC-1309-99,2002. 2288201600017 Data were received from author A.Smirnov 31.12.2009. 2288201600018 ERR-ANALYS (ERR-T) Total uncertainty . 2288201600019 (ERR-S,1.,3.) Statistical uncertainty. 2288201600020 (ERR-1) Uncertainty of chambers mosaic arrangement 2288201600021 registration efficiency. 2288201600022 (ERR-2,,1.) Maximal uncertainty of correction 2288201600023 coefficients ratio at peak. 2288201600024 (ERR-3,,1.) Maximal uncertainty of ratio of 2288201600025 registration efficiencies. 2288201600026 (ERR-4,,3.) Targets were weighted with the accuracy not2288201600027 worse than 3% with the use of precise analytical 2288201600028 balance. 2288201600029 (ERR-5,,0.0001) Upper limit of admixture of actinides 2288201600030 for lead isotopes determined by means of analysis of 2288201600031 results of measurement at 35 MeV neutrons 2288201600032 ENDBIB 30 0 2288201600033 COMMON 1 3 2288201600034 ERR-1 2288201600035 PER-CENT 2288201600036 3. 2288201600037 ENDCOMMON 3 0 2288201600038 DATA 4 9 2288201600039 EN EN-ERR DATA ERR-T 2288201600040 MEV MEV NO-DIM NO-DIM 2288201600041 34.5 1.4 0.13 0.02 2288201600042 46.3 1.2 0.19 0.01 2288201600043 66.6 0.9 0.29 0.01 2288201600044 89.6 0.8 0.37 0.03 2288201600045 94.1 1.4 0.36 0.02 2288201600046 111.3 1.1 0.46 0.03 2288201600047 132.9 1.9 0.44 0.02 2288201600048 144.6 1.8 0.50 0.03 2288201600049 173.3 1.9 0.47 0.02 2288201600050 ENDDATA 11 0 2288201600051 ENDSUBENT 50 0 2288201699999 SUBENT 22882017 20100112 22212288201700001 BIB 5 23 2288201700002 REACTION ((81-TL-205(N,F),,SIG)/(83-BI-209(N,F),,SIG)) 2288201700003 SAMPLE Bi-209 0 metallic. 2288201700004 Tl-205 enriched sample isotopic composition: 2288201700005 99.8% of 205-Tl, 0.02% of 203-Tl. 2288201700006 METHOD (RELFY) Fission cross-section ratio was measured with 2288201700007 pair of sandwich arrangements, stacked one after2288201700008 other in neutron beam. 2288201700009 STATUS (TABLE) From Table 3-2 of R,ISTC-1309-99,2002. 2288201700010 Data were received from author A.Smirnov 31.12.2009. 2288201700011 ERR-ANALYS (ERR-T) Total uncertainty . 2288201700012 (ERR-S,1.,3.) Statistical uncertainty. 2288201700013 (ERR-1) Uncertainty of chambers mosaic arrangement 2288201700014 registration efficiency. 2288201700015 (ERR-2,,1.) Maximal uncertainty of correction 2288201700016 coefficients ratio at peak. 2288201700017 (ERR-3,,1.) Maximal uncertainty of ratio of 2288201700018 registration efficiencies. 2288201700019 (ERR-4,,3.) Targets were weighted with the accuracy not2288201700020 worse than 3% with the use of precise analytical 2288201700021 balance. 2288201700022 (ERR-5,,0.0001) Upper limit of admixture of actinides 2288201700023 determined by means of analysis of results of 2288201700024 measurement at 35 MeV neutrons. 2288201700025 ENDBIB 23 0 2288201700026 COMMON 1 3 2288201700027 ERR-1 2288201700028 PER-CENT 2288201700029 3. 2288201700030 ENDCOMMON 3 0 2288201700031 DATA 4 9 2288201700032 EN EN-ERR DATA ERR-T 2288201700033 MEV MEV NO-DIM NO-DIM 2288201700034 34.5 1.4 0.020 0.007 2288201700035 46.3 1.2 0.067 0.004 2288201700036 66.6 0.9 0.105 0.005 2288201700037 89.6 0.8 0.16 0.01 2288201700038 94.1 1.4 0.164 0.006 2288201700039 111.3 1.1 0.204 0.016 2288201700040 132.9 1.9 0.23 0.01 2288201700041 144.6 1.8 0.25 0.01 2288201700042 173.3 1.9 0.25 0.01 2288201700043 ENDDATA 11 0 2288201700044 ENDSUBENT 43 0 2288201799999 SUBENT 22882018 20100112 22212288201800001 BIB 5 20 2288201800002 REACTION (82-PB-204(N,F),,SIG) 2288201800003 MONITOR (83-BI-209(N,F),,SIG) 2288201800004 MONIT-REF (22882003,A.N.Smirnov+,J,PR/C,70,054603,2004) 2288201800005 STATUS (TABLE) From Table of R,ISTC-1309-99,2002. 2288201800006 (DEP,22882014) 2288201800007 (DEP,22882003) 2288201800008 Data were received from author A.Smirnov 31.12.2009. 2288201800009 Data are presented on Fig.1,right, of C,2004SANTA . 2288201800010 ERR-ANALYS (ERR-T) Total uncertainty . 2288201800011 (ERR-S,1.,3.) Statistical uncertainty of counting by 2288201800012 each of 12 chambers. 2288201800013 (ERR-1) Uncertainty of sample average thickness. 2288201800014 (ERR-2) Uncertainty of solid angle. 2288201800015 (ERR-3,,3.) Maximal uncertainty of correction 2288201800016 coefficient. 2288201800017 (ERR-4,,3.) Maximal statistical uncertainty due to 2288201800018 gamma-spectrum measurement and analysis. 2288201800019 (ERR-5,,1.) Maximal uncertainty due to proton beam 2288201800020 fluctuations. 2288201800021 Monitor cross sections uncertainty. 2288201800022 ENDBIB 20 0 2288201800023 COMMON 2 3 2288201800024 ERR-1 ERR-2 2288201800025 PER-CENT PER-CENT 2288201800026 3. 3. 2288201800027 ENDCOMMON 3 0 2288201800028 DATA 4 9 2288201800029 EN EN-ERR DATA ERR-T 2288201800030 MEV MEV MB MB 2288201800031 34.5 1.4 0.32 0.04 2288201800032 46.3 1.2 1.81 0.22 2288201800033 66.6 0.9 8.6 1.1 2288201800034 89.6 0.8 20.4 2.2 2288201800035 94.1 1.4 22.0 2.5 2288201800036 111.3 1.1 35.5 4.4 2288201800037 132.9 1.9 40.5 4.1 2288201800038 144.6 1.8 45.1 5.1 2288201800039 173.3 1.9 54.9 7.3 2288201800040 ENDDATA 11 0 2288201800041 ENDSUBENT 40 0 2288201899999 SUBENT 22882019 20100112 22212288201900001 BIB 5 21 2288201900002 REACTION (82-PB-206(N,F),,SIG) 2288201900003 MONITOR (83-BI-209(N,F),,SIG) 2288201900004 MONIT-REF (22882003,A.N.Smirnov+,J,PR/C,70,054603,2004) 2288201900005 STATUS (TABLE) Data were received from author A.Smirnov 2288201900006 31.12.2009. 2288201900007 (DEP,22882015) 2288201900008 (DEP,22882003) 2288201900009 Data were received from author A.Smirnov 31.12.2009. 2288201900010 Data are presented on Fig.1,right, of C,2004SANTA . 2288201900011 ERR-ANALYS (ERR-T) Total uncertainty . 2288201900012 (ERR-S,1.,3.) Statistical uncertainty of counting by 2288201900013 each of 12 chambers. 2288201900014 (ERR-1) Uncertainty of sample average thickness. 2288201900015 (ERR-2) Uncertainty of solid angle. 2288201900016 (ERR-3,,3.) Maximal uncertainty of correction 2288201900017 coefficient. 2288201900018 (ERR-4,,3.) Maximal statistical uncertainty due to 2288201900019 gamma-spectrum measurement and analysis. 2288201900020 (ERR-5,,1.) Maximal uncertainty due to proton beam 2288201900021 fluctuations. 2288201900022 Monitor cross sections uncertainty. 2288201900023 ENDBIB 21 0 2288201900024 COMMON 2 3 2288201900025 ERR-1 ERR-2 2288201900026 PER-CENT PER-CENT 2288201900027 3. 3. 2288201900028 ENDCOMMON 3 0 2288201900029 DATA 4 9 2288201900030 EN EN-ERR DATA ERR-T 2288201900031 MEV MEV MB MB 2288201900032 34.5 1.4 0.053 0.009 2288201900033 46.3 1.2 0.55 0.07 2288201900034 66.6 0.9 3.79 0.47 2288201900035 89.6 0.8 9.4 1.0 2288201900036 94.1 1.4 11.0 1.3 2288201900037 111.3 1.1 18.4 2.3 2288201900038 132.9 1.9 23.9 2.4 2288201900039 144.6 1.8 28.7 3.2 2288201900040 173.3 1.9 33.5 4.3 2288201900041 ENDDATA 11 0 2288201900042 ENDSUBENT 41 0 2288201999999 SUBENT 22882020 20100112 22212288202000001 BIB 5 21 2288202000002 REACTION (82-PB-207(N,F),,SIG) 2288202000003 MONITOR (83-BI-209(N,F),,SIG) 2288202000004 MONIT-REF (22882003,A.N.Smirnov+,J,PR/C,70,054603,2004) 2288202000005 STATUS (TABLE) Data were received from author A.Smirnov 2288202000006 31.12.2009. 2288202000007 (DEP,22882016) 2288202000008 (DEP,22882003) 2288202000009 Data were received from author A.Smirnov 31.12.2009. 2288202000010 Data are presented on Fig.1,right, of C,2004SANTA . 2288202000011 ERR-ANALYS (ERR-T) Total uncertainty . 2288202000012 (ERR-S,1.,3.) Statistical uncertainty of counting by 2288202000013 each of 12 chambers. 2288202000014 (ERR-1) Uncertainty of sample average thickness. 2288202000015 (ERR-2) Uncertainty of solid angle. 2288202000016 (ERR-3,,3.) Maximal uncertainty of correction 2288202000017 coefficient. 2288202000018 (ERR-4,,3.) Maximal statistical uncertainty due to 2288202000019 gamma-spectrum measurement and analysis. 2288202000020 (ERR-5,,1.) Maximal uncertainty due to proton beam 2288202000021 fluctuations. 2288202000022 Monitor cross sections uncertainty. 2288202000023 ENDBIB 21 0 2288202000024 COMMON 2 3 2288202000025 ERR-1 ERR-2 2288202000026 PER-CENT PER-CENT 2288202000027 3. 3. 2288202000028 ENDCOMMON 3 0 2288202000029 DATA 4 9 2288202000030 EN EN-ERR DATA ERR-T 2288202000031 MEV MEV MB MB 2288202000032 34.5 1.4 0.040 0.006 2288202000033 46.3 1.2 0.325 0.040 2288202000034 66.6 0.9 2.44 0.30 2288202000035 89.6 0.8 7.1 0.8 2288202000036 94.1 1.4 8.1 0.9 2288202000037 111.3 1.1 15.4 1.9 2288202000038 132.9 1.9 17.8 1.8 2288202000039 144.6 1.8 22.1 2.4 2288202000040 173.3 1.9 25.8 3.3 2288202000041 ENDDATA 11 0 2288202000042 ENDSUBENT 41 0 2288202099999 SUBENT 22882021 20100112 22212288202100001 BIB 5 21 2288202100002 REACTION (81-TL-205(N,F),,SIG) 2288202100003 MONITOR (83-BI-209(N,F),,SIG) 2288202100004 MONIT-REF (22882003,A.N.Smirnov+,J,PR/C,70,054603,2004) 2288202100005 STATUS (TABLE) Data were received from author A.Smirnov 2288202100006 31.12.2009. 2288202100007 (DEP,22882016) 2288202100008 (DEP,22882003) 2288202100009 Data were received from author A.Smirnov 31.12.2009. 2288202100010 Data are presented on Fig.1,right, of C,2004SANTA . 2288202100011 ERR-ANALYS (ERR-T) Total uncertainty . 2288202100012 (ERR-S,1.,3.) Statistical uncertainty of counting by 2288202100013 each of 12 chambers. 2288202100014 (ERR-1) Uncertainty of sample average thickness. 2288202100015 (ERR-2) Uncertainty of solid angle. 2288202100016 (ERR-3,,3.) Maximal uncertainty of correction 2288202100017 coefficient. 2288202100018 (ERR-4,,3.) Maximal statistical uncertainty due to 2288202100019 gamma-spectrum measurement and analysis. 2288202100020 (ERR-5,,1.) Maximal uncertainty due to proton beam 2288202100021 fluctuations. 2288202100022 Monitor cross sections uncertainty. 2288202100023 ENDBIB 21 0 2288202100024 COMMON 2 3 2288202100025 ERR-1 ERR-2 2288202100026 PER-CENT PER-CENT 2288202100027 3. 3. 2288202100028 ENDCOMMON 3 0 2288202100029 DATA 4 9 2288202100030 EN EN-ERR DATA ERR-T 2288202100031 MEV MEV MB MB 2288202100032 34.5 1.4 0.006 0.002 2288202100033 46.3 1.2 0.115 0.014 2288202100034 66.6 0.9 0.88 0.11 2288202100035 89.6 0.8 3.07 0.33 2288202100036 94.1 1.4 3.67 0.41 2288202100037 111.3 1.1 6.83 0.83 2288202100038 132.9 1.9 9.31 0.92 2288202100039 144.6 1.8 11.1 1.3 2288202100040 173.3 1.9 13.7 1.7 2288202100041 ENDDATA 11 0 2288202100042 ENDSUBENT 41 0 2288202199999 SUBENT 22882022 20100112 22212288202200001 BIB 6 21 2288202200002 REACTION ((80-HG-0(N,F),,SIG)/(83-BI-209(N,F),,SIG)) 2288202200003 SAMPLE Hg-nat, chemical composition Hg(2)-Cl(2), 2288202200004 chemical enrichment 99.6%, produced by vacuum 2288202200005 evaporation, number of targets - 12, average layer 2288202200006 thickness 0.3 or 0.8 mg/cm**2. 2288202200007 METHOD (RELFY) Fission cross-section ratio was measured with 2288202200008 pair of sandwich arrangements, stacked one after2288202200009 other in neutron beam. 2288202200010 FLAG (1.) Data point was not used for absolute cross-section2288202200011 due to it's probable defect ( author's comment). 2288202200012 STATUS (TABLE) Data received from author A.Smirnov 31.12.2009.2288202200013 Published in: V.P.Eismont,I.V.Ryzhov,A.N.Smirnov et al.2288202200014 "Intermediate energy neutron-induced fission cross 2288202200015 sections for prospective neutron production target 2288202200016 in ADS." Proc. of 6th OECD/NEA Information Exchange 2288202200017 Meeting on Partitioning and Transmutation of Actinides2288202200018 and Fission Products . Madrid, Spain December 11-13, 2288202200019 2000 (CD ROM publication, paper P-36). 2288202200020 Also Table 3.1 of R,ISTC-540-97,1999 - prelim.data. 2288202200021 ERR-ANALYS (ERR-T) Total uncertainty . 2288202200022 (ERR-1,6.,14.) Uncertainty in layer thickness 6-14 % . 2288202200023 ENDBIB 21 0 2288202200024 NOCOMMON 0 0 2288202200025 DATA 6 7 2288202200026 EN EN-ERR DATA ERR-T DATA-MAX FLAG 2288202200027 MEV MEV NO-DIM NO-DIM NO-DIM NO-DIM 2288202200028 46.3 1.2 0.036 2288202200029 66.6 0.9 0.127 0.026 2288202200030 73.9 1.0 0.099 0.021 1. 2288202200031 94.1 1.4 0.158 0.017 2288202200032 132.9 1.9 0.199 0.019 2288202200033 144.6 1.8 0.158 0.019 1. 2288202200034 173.3 1.9 0.215 0.040 2288202200035 ENDDATA 9 0 2288202200036 ENDSUBENT 35 0 2288202299999 SUBENT 22882023 20100112 22212288202300001 BIB 5 16 2288202300002 REACTION (80-HG-0(N,F),,SIG) 2288202300003 MONITOR (83-BI-209(N,F),,SIG) 2288202300004 MONIT-REF (22882003,A.N.Smirnov+,J,PR/C,70,054603,2004) 2288202300005 STATUS (TABLE) Data received from author A.Smirnov 31.12.2009.2288202300006 Table 3.4 of R,ISTC-504-97,199910 - prelim.data. 2288202300007 Published in: V.P.Eismont,I.V.Ryzhov,A.N.Smirnov et al.2288202300008 "Intermediate energy neutron-induced fission cross 2288202300009 sections for prospective neutron production target 2288202300010 in ADS." Proc. of 6th OECD/NEA Information Exchange 2288202300011 Meeting on Partitioning and Transmutation of Actinides2288202300012 and Fission Products . Madrid, Spain December 11-13, 2288202300013 2000 (CD ROM publication, paper P-36). 2288202300014 (DEP,22882022) 2288202300015 (DEP,22882003) 2288202300016 ERR-ANALYS (ERR-T) Total uncertainty. 2288202300017 (ERR-1,6.,14.) Uncertainty in layer thickness 6-14 % . 2288202300018 ENDBIB 16 0 2288202300019 NOCOMMON 0 0 2288202300020 DATA 5 5 2288202300021 EN EN-ERR DATA ERR-T DATA-MAX 2288202300022 MEV MEV MB MB MB 2288202300023 46.3 1.2 0.06 2288202300024 66.6 0.9 1.07 0.28 2288202300025 94.1 1.4 3.57 0.52 2288202300026 132.9 1.9 8.1 1.0 2288202300027 173.3 1.9 11.8 2.1 2288202300028 ENDDATA 7 0 2288202300029 ENDSUBENT 28 0 2288202399999 ENDENTRY 23 0 2288299999999