ENTRY M0916 20150901 M081M091600000001 SUBENT M0916001 20150901 M081M091600100001 BIB 9 32 M091600100002 TITLE Reliable cross sections of partial photoneutron M091600100003 reactions on 188,189Os isotopes free of neutron M091600100004 multiplicity sorting problems. M091600100005 AUTHOR (V.V.Varlamov,M.A.Makarov,N.N.Peskov,M.E.Stepanov) M091600100006 REFERENCE (J,IZV,78,(5),599,2014) M091600100007 #doi:10.7868/S0367676514050263 M091600100008 (J,BAS,78,(5),412,2014) M091600100009 #doi:10.3103/S1062873814050207 M091600100010 English translation of IZV,78,(5),599,2014. M091600100011 (R,MSU-INP-2013-1/884,2013) In Russian. M091600100012 INSTITUTE (4RUSMOS) M091600100013 INC-SOURCE (QMPH,ARAD) M091600100014 ANALYSIS The joint analysis of data for total (g,xn) and M091600100015 partial (g,n), (g,2n) and (g,3n) reactions obtained M091600100016 in various experiments was carried out. The new M091600100017 approach to analysis of systematic disagreements M091600100018 between data was proposed on the base of new criteria M091600100019 of systematic uncertainties presence - specially M091600100020 proposed transitional multiplicity functions M091600100021 Fi-theor = SIG(g,in)/SIG(g,xn). M091600100022 Using these functions calculated in the frame of M091600100023 combined photonuclear reaction model new reliable M091600100024 and free from problems of neutron multiplicity M091600100025 sorting data for photoneutron partial reactions M091600100026 cross sections M091600100027 SIG-eval(g,in) = Fi-theor x SIG-exp(g,xn) M091600100028 were evaluated using experimental neutron yield M091600100029 reaction cross sections SIG-exp(g,xn). M091600100030 ERR-ANALYS (DATA-ERR) Root-mean-square errors. M091600100031 STATUS (TABLE,APRVD) Approved by V.Varlamov. M091600100032 HISTORY (20150901C) Data were compiled at the Russia MSU SINP M091600100033 CDFE by V.Varlamov. M091600100034 ENDBIB 32 0 M091600100035 NOCOMMON 0 0 M091600100036 ENDSUBENT 35 0 M091600199999 SUBENT M0916002 20150901 M081M091600200001 BIB 4 22 M091600200002 REACTION ((76-OS-188(G,N)76-OS-187,,SIG,,,EVAL)+ M091600200003 (76-OS-188(G,N+P)75-RE-186,,SIG,,,EVAL)) M091600200004 ANALYSIS The contribution of partial reaction (g,n) cross M091600200005 section into the experimental total neutron yield M091600200006 reaction (g,xn) cross section obtained using M091600200007 quasimonoenergetic annihilation photons at Livermore M091600200008 (USA) was evaluated using specially theoretically M091600200009 calculated transitional multiplicity function - M091600200010 ratio M091600200011 F1-theor = SIG-theor(g,n)/SIG-theor(g,xn) M091600200012 by the way M091600200013 SIG-eval(g,n) = (F1-theor)x(SIG-exp(g,xn)). M091600200014 REL-REF (R,L0046008,B.L.Berman+,J,PR/C,19,1205,1979) M091600200015 Experimental data for the total neutron yield M091600200016 reaction (g,xn) cross section. M091600200017 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M091600200018 Theoretical preequilibrium model of photonuclear M091600200019 reactions based on the Fermi gas densities. M091600200020 STATUS Data plotted in Fig. 3. M091600200021 (DEP,L0011008) M091600200022 The total neutron yield reaction (g,xn) cross M091600200023 section. M091600200024 ENDBIB 22 0 M091600200025 NOCOMMON 0 0 M091600200026 DATA 3 84 M091600200027 EN DATA DATA-ERR M091600200028 MEV MB MB M091600200029 7.44 5.76 1.73 M091600200030 7.93 9.39 2.03 M091600200031 8.42 38.28 5.78 M091600200032 8.91 50.30 7.45 M091600200033 9.40 58.18 8.51 M091600200034 9.89 76.22 10.98 M091600200035 10.13 90.27 13.00 M091600200036 10.38 110.89 15.90 M091600200037 10.62 126.32 18.11 M091600200038 10.87 139.06 19.90 M091600200039 11.11 165.94 23.68 M091600200040 11.35 193.93 27.63 M091600200041 11.60 236.27 33.64 M091600200042 11.84 277.08 39.41 M091600200043 12.09 327.41 46.55 M091600200044 12.33 371.62 52.89 M091600200045 12.58 411.16 58.42 M091600200046 12.82 446.78 63.37 M091600200047 13.06 446.90 63.52 M091600200048 13.31 469.30 66.54 M091600200049 13.55 478.12 67.81 M091600200050 13.80 486.91 69.05 M091600200051 14.04 488.87 69.33 M091600200052 14.29 478.20 67.84 M091600200053 14.53 489.18 69.39 M091600200054 14.78 468.12 66.33 M091600200055 15.02 425.13 60.28 M091600200056 15.26 365.09 52.02 M091600200057 15.51 307.75 43.89 M091600200058 15.75 243.37 34.76 M091600200059 16.00 186.81 26.73 M091600200060 16.12 167.03 23.90 M091600200061 16.24 142.88 20.50 M091600200062 16.36 124.67 17.86 M091600200063 16.49 105.08 15.13 M091600200064 16.61 93.27 13.44 M091600200065 16.73 80.20 11.62 M091600200066 16.85 75.12 10.88 M091600200067 16.98 65.57 9.57 M091600200068 17.10 63.48 9.27 M091600200069 17.22 51.31 7.57 M091600200070 17.34 51.10 7.56 M091600200071 17.46 40.09 6.05 M091600200072 17.71 35.75 5.41 M091600200073 17.95 31.70 4.79 M091600200074 18.20 28.74 4.30 M091600200075 18.44 23.82 3.60 M091600200076 18.69 22.36 3.38 M091600200077 18.93 18.97 2.96 M091600200078 19.17 18.46 2.91 M091600200079 19.42 16.47 2.68 M091600200080 19.66 16.14 2.65 M091600200081 19.91 14.86 2.47 M091600200082 20.15 13.68 2.15 M091600200083 20.40 13.21 2.32 M091600200084 20.64 13.33 2.38 M091600200085 20.89 13.96 2.44 M091600200086 21.13 13.99 2.50 M091600200087 21.37 12.84 2.40 M091600200088 21.62 15.46 2.71 M091600200089 21.86 18.64 3.08 M091600200090 22.11 20.12 3.30 M091600200091 22.35 22.10 3.64 M091600200092 22.60 17.19 2.88 M091600200093 22.84 23.32 4.03 M091600200094 23.09 21.50 3.98 M091600200095 23.33 20.59 3.90 M091600200096 23.57 18.99 3.72 M091600200097 23.82 17.21 2.92 M091600200098 24.06 15.82 2.74 M091600200099 24.31 15.16 3.19 M091600200100 24.55 11.85 2.82 M091600200101 25.04 11.86 2.63 M091600200102 25.53 10.44 2.38 M091600200103 26.02 6.73 2.05 M091600200104 26.51 3.06 1.85 M091600200105 27. 4.61 1.79 M091600200106 27.48 4.46 1.78 M091600200107 27.97 4.63 1.71 M091600200108 28.46 3.22 1.59 M091600200109 28.95 1.77 1.48 M091600200110 29.44 2.66 1.98 M091600200111 29.93 1.40 2.01 M091600200112 30.42 3.19 2.20 M091600200113 ENDDATA 86 0 M091600200114 ENDSUBENT 113 0 M091600299999 SUBENT M0916003 20150901 M081M091600300001 BIB 4 22 M091600300002 REACTION ((76-OS-188(G,2N)76-OS-186,,SIG,,,EVAL)+ M091600300003 (76-OS-188(G,2N+P)75-RE-185,,SIG,,,EVAL)) M091600300004 ANALYSIS The contribution of partial reaction (g,n) cross M091600300005 section into the experimental total neutron yield M091600300006 reaction (g,xn) cross section obtained using M091600300007 quasimonoenergetic annihilation photons at Livermore M091600300008 (USA) was evaluated using specially theoretically M091600300009 calculated transitional multiplicity function - M091600300010 ratio M091600300011 F2-theor = SIG-theor(g,2n)/SIG-theor(g,xn) M091600300012 by the way M091600300013 SIG-eval(g,n) = (F2-theor)x(SIG-exp(g,xn)). M091600300014 REL-REF (R,L0046008,B.L.Berman+,J,PR/C,19,1205,1979) M091600300015 Experimental data for the total neutron yield M091600300016 reaction (g,xn) cross section. M091600300017 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M091600300018 Theoretical preequilibrium model of photonuclear M091600300019 reactions based on the Fermi gas densities. M091600300020 STATUS Data plotted in Fig. 3. M091600300021 (DEP,L0011008) M091600300022 The total neutron yield reaction (g,xn) cross M091600300023 section. M091600300024 ENDBIB 22 0 M091600300025 NOCOMMON 0 0 M091600300026 DATA 3 60 M091600300027 EN DATA DATA-ERR M091600300028 MEV MB MB M091600300029 14.53 7.25 8.55 M091600300030 14.78 26.44 16.60 M091600300031 15.02 55.72 24.46 M091600300032 15.26 90.68 31.52 M091600300033 15.51 126.62 37.76 M091600300034 15.75 153.39 41.19 M091600300035 16.00 171.09 42.71 M091600300036 16.12 179.66 43.67 M091600300037 16.24 180.74 42.92 M091600300038 16.36 184.35 42.86 M091600300039 16.49 177.33 40.67 M091600300040 16.61 179.15 40.53 M091600300041 16.73 170.58 38.30 M091600300042 16.85 176.42 39.25 M091600300043 16.98 168.96 37.42 M091600300044 17.10 176.75 38.93 M091600300045 17.22 154.01 33.91 M091600300046 17.34 161.78 35.53 M091600300047 17.46 133.37 29.46 M091600300048 17.71 129.29 28.47 M091600300049 17.95 122.66 26.87 M091600300050 18.20 118.61 25.80 M091600300051 18.44 103.68 22.59 M091600300052 18.69 101.85 22.16 M091600300053 18.93 89.87 19.81 M091600300054 19.17 89.82 19.88 M091600300055 19.42 81.93 18.42 M091600300056 19.66 81.75 18.47 M091600300057 19.91 77.04 17.51 M091600300058 20.15 72.18 15.91 M091600300059 20.40 70.23 16.45 M091600300060 20.64 70.84 16.74 M091600300061 20.89 73.79 17.28 M091600300062 21.13 72.33 17.22 M091600300063 21.37 63.39 15.60 M091600300064 21.62 71.39 17.12 M091600300065 21.86 80.01 18.78 M091600300066 22.11 79.86 18.84 M091600300067 22.35 81.40 19.37 M091600300068 22.60 59.32 14.33 M091600300069 22.84 76.65 18.84 M091600300070 23.09 68.99 17.65 M091600300071 23.33 65.43 17.08 M091600300072 23.57 59.93 16.17 M091600300073 23.82 53.36 13.77 M091600300074 24.06 47.60 12.83 M091600300075 24.31 43.70 13.36 M091600300076 24.55 32.48 10.95 M091600300077 25.04 28.89 10.25 M091600300078 25.53 22.46 8.80 M091600300079 26.02 13.02 6.12 M091600300080 26.51 5.40 3.90 M091600300081 27. 7.41 4.33 M091600300082 27.48 6.57 4.05 M091600300083 27.97 6.35 3.94 M091600300084 28.46 4.18 3.00 M091600300085 28.95 2.18 2.17 M091600300086 29.44 3.12 2.91 M091600300087 29.93 1.58 2.45 M091600300088 30.42 3.51 3.18 M091600300089 ENDDATA 62 0 M091600300090 ENDSUBENT 89 0 M091600399999 SUBENT M0916004 20150901 M081M091600400001 BIB 4 22 M091600400002 REACTION ((76-OS-188(G,3N)76-OS-185,,SIG,,,EVAL)+ M091600400003 (76-OS-188(G,3N+P)75-RE-184,,SIG,,,EVAL)) M091600400004 ANALYSIS The contribution of partial reaction (g,n) cross M091600400005 section into the experimental total neutron yield M091600400006 reaction (g,xn) cross section obtained using M091600400007 quasimonoenergetic annihilation photons at Livermore M091600400008 (USA) was evaluated using specially theoretically M091600400009 calculated transitional multiplicity function - M091600400010 ratio M091600400011 F3-theor = SIG-theor(g,3n)/SIG-theor(g,xn) M091600400012 by the way M091600400013 SIG-eval(g,n) = (F3-theor)x(SIG-exp(g,xn)). M091600400014 REL-REF (R,L0046008,B.L.Berman+,J,PR/C,19,1205,1979) M091600400015 Experimental data for the total neutron yield M091600400016 reaction (g,xn) cross section. M091600400017 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M091600400018 Theoretical preequilibrium model of photonuclear M091600400019 reactions based on the Fermi gas densities. M091600400020 STATUS Data plotted in Fig. 3. M091600400021 (DEP,L0011008) M091600400022 The total neutron yield reaction (g,xn) cross M091600400023 section. M091600400024 ENDBIB 22 0 M091600400025 NOCOMMON 0 0 M091600400026 DATA 3 19 M091600400027 EN DATA DATA-ERR M091600400028 MEV MB MB M091600400029 23.09 0.34 1.04 M091600400030 23.33 1.63 2.27 M091600400031 23.57 3.71 3.38 M091600400032 23.82 6.36 4.32 M091600400033 24.06 9.49 5.27 M091600400034 24.31 13.36 6.56 M091600400035 24.55 14.08 6.44 M091600400036 25.04 21.72 8.59 M091600400037 25.53 25.86 9.60 M091600400038 26.02 20.70 8.46 M091600400039 26.51 11.15 7.33 M091600400040 27. 19.02 8.82 M091600400041 27.48 20.22 9.49 M091600400042 27.97 22.42 9.89 M091600400043 28.46 16.32 8.96 M091600400044 28.95 9.34 8.08 M091600400045 29.44 14.39 11.26 M091600400046 29.93 7.76 11.28 M091600400047 30.42 17.73 12.92 M091600400048 ENDDATA 21 0 M091600400049 ENDSUBENT 48 0 M091600499999 SUBENT M0916005 20150901 M081M091600500001 BIB 3 10 M091600500002 REACTION (76-OS-188(G,X)0-NN-1,UNW,SIG,,,EVAL) M091600500003 ANALYSIS The total neutron reaction cross section obtained as M091600500004 sum: SIG(g,sn) = SIG(g,n) + SIG(g,2n) + SIG(g,3n). M091600500005 STATUS Data plotted in Fig. 13. M091600500006 (DEP,M0916002) M091600500007 Evaluated (g,n) reaction cross section. M091600500008 (DEP,M0916003) M091600500009 Evaluated (g,2n) reaction cross section. M091600500010 (DEP,M0916004) M091600500011 Evaluated (g,3n) reaction cross section. M091600500012 ENDBIB 10 0 M091600500013 NOCOMMON 0 0 M091600500014 DATA 3 84 M091600500015 EN DATA DATA-ERR M091600500016 MEV MB MB M091600500017 7.44 5.76 1.73 M091600500018 7.93 9.39 2.03 M091600500019 8.42 38.28 5.78 M091600500020 8.91 50.3 7.45 M091600500021 9.40 58.18 8.51 M091600500022 9.89 76.22 10.98 M091600500023 10.13 90.27 13.00 M091600500024 10.38 110.89 15.90 M091600500025 10.62 126.32 18.11 M091600500026 10.87 139.06 19.90 M091600500027 11.11 165.94 23.68 M091600500028 11.35 193.93 27.63 M091600500029 11.60 236.27 33.64 M091600500030 11.84 277.08 39.41 M091600500031 12.09 327.41 46.55 M091600500032 12.33 371.62 52.89 M091600500033 12.58 411.16 58.42 M091600500034 12.82 446.78 63.37 M091600500035 13.06 446.9 63.52 M091600500036 13.31 469.3 66.54 M091600500037 13.55 478.12 67.81 M091600500038 13.80 486.91 69.05 M091600500039 14.04 488.87 69.33 M091600500040 14.29 478.2 67.84 M091600500041 14.53 496.44 69.91 M091600500042 14.78 494.55 68.37 M091600500043 15.02 480.84 65.06 M091600500044 15.26 455.78 60.83 M091600500045 15.51 434.37 57.90 M091600500046 15.75 396.77 53.90 M091600500047 16.00 357.91 50.39 M091600500048 16.12 346.69 49.78 M091600500049 16.24 323.62 47.57 M091600500050 16.36 309.02 46.43 M091600500051 16.49 282.42 43.39 M091600500052 16.61 272.43 42.70 M091600500053 16.73 250.79 40.03 M091600500054 16.85 251.54 40.74 M091600500055 16.98 234.53 38.62 M091600500056 17.10 240.24 40.01 M091600500057 17.22 205.32 34.74 M091600500058 17.34 212.89 36.33 M091600500059 17.46 173.46 30.08 M091600500060 17.71 165.05 28.98 M091600500061 17.95 154.36 27.29 M091600500062 18.20 147.35 26.15 M091600500063 18.44 127.51 22.88 M091600500064 18.69 124.22 22.42 M091600500065 18.93 108.85 20.03 M091600500066 19.17 108.28 20.10 M091600500067 19.42 98.40 18.61 M091600500068 19.66 97.89 18.66 M091600500069 19.91 91.91 17.68 M091600500070 20.15 85.86 16.06 M091600500071 20.40 83.44 16.61 M091600500072 20.64 84.18 16.91 M091600500073 20.89 87.76 17.45 M091600500074 21.13 86.32 17.41 M091600500075 21.37 76.24 15.79 M091600500076 21.62 86.86 17.34 M091600500077 21.86 98.66 19.03 M091600500078 22.11 99.99 19.13 M091600500079 22.35 103.50 19.70 M091600500080 22.60 76.52 14.61 M091600500081 22.84 99.97 19.26 M091600500082 23.09 90.83 18.12 M091600500083 23.33 87.67 17.67 M091600500084 23.57 82.65 16.94 M091600500085 23.82 76.94 14.73 M091600500086 24.06 72.92 14.14 M091600500087 24.31 72.23 15.23 M091600500088 24.55 58.41 13.02 M091600500089 25.04 62.47 13.63 M091600500090 25.53 58.77 13.24 M091600500091 26.02 40.46 10.65 M091600500092 26.51 19.62 8.50 M091600500093 27. 31.06 9.99 M091600500094 27.48 31.26 10.47 M091600500095 27.97 33.41 10.78 M091600500096 28.46 23.73 9.59 M091600500097 28.95 13.31 8.50 M091600500098 29.44 20.18 11.80 M091600500099 29.93 10.75 11.72 M091600500100 30.42 24.44 13.49 M091600500101 ENDDATA 86 0 M091600500102 ENDSUBENT 101 0 M091600599999 SUBENT M0916006 20150901 M081M091600600001 BIB 4 22 M091600600002 REACTION ((76-OS-189(G,N)76-OS-188,,SIG,,,EVAL)+ M091600600003 (76-OS-189(G,N+P)75-RE-187,,SIG,,,EVAL)) M091600600004 ANALYSIS The contribution of partial reaction (g,n) cross M091600600005 section into the experimental total neutron yield M091600600006 reaction (g,xn) cross section obtained using M091600600007 quasimonoenergetic annihilation photons at Livermore M091600600008 (USA) was evaluated using specially theoretically M091600600009 calculated transitional multiplicity function - M091600600010 ratio M091600600011 F1-theor = SIG-theor(g,n)/SIG-theor(g,xn) M091600600012 by the way M091600600013 SIG-eval(g,n) = (F1-theor)x(SIG-exp(g,xn)). M091600600014 REL-REF (R,L0046012,B.L.Berman+,J,PR/C,19,1205,1979) M091600600015 Experimental data for the total neutron yield M091600600016 reaction (g,xn) cross section. M091600600017 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M091600600018 Theoretical preequilibrium model of photonuclear M091600600019 reactions based on the Fermi gas densities. M091600600020 STATUS Data plotted in Fig. 8. M091600600021 (DEP,L0011008) M091600600022 The total neutron yield reaction (g,xn) cross M091600600023 section. M091600600024 ENDBIB 22 0 M091600600025 NOCOMMON 0 0 M091600600026 DATA 3 77 M091600600027 EN DATA DATA-ERR M091600600028 MEV MB MB M091600600029 7.44 24.27 3.27 M091600600030 7.93 29.56 3.59 M091600600031 8.42 37.29 4.31 M091600600032 8.91 46.01 5.14 M091600600033 9.40 59.37 6.38 M091600600034 9.89 83.86 8.69 M091600600035 10.13 87.33 9.09 M091600600036 10.38 103.28 10.69 M091600600037 10.62 126.21 12.94 M091600600038 10.87 146.86 15.03 M091600600039 11.11 170.51 17.35 M091600600040 11.35 198.77 20.20 M091600600041 11.60 239.55 24.31 M091600600042 11.84 287.01 29.04 M091600600043 12.09 337.15 34.08 M091600600044 12.33 390.95 39.48 M091600600045 12.58 419.21 42.32 M091600600046 12.82 440.69 44.49 M091600600047 13.06 451.41 45.55 M091600600048 13.31 466.08 46.99 M091600600049 13.55 469.54 47.39 M091600600050 13.80 467.05 47.12 M091600600051 14.04 446.77 45.07 M091600600052 14.29 400.16 40.41 M091600600053 14.53 353.25 35.61 M091600600054 14.78 292.30 29.41 M091600600055 15.02 238.97 24.10 M091600600056 15.26 193.58 19.80 M091600600057 15.51 153.58 15.78 M091600600058 15.75 128.98 13.29 M091600600059 16.00 109.97 11.40 M091600600060 16.24 89.94 9.40 M091600600061 16.49 76.40 8.05 M091600600062 16.73 65.07 6.93 M091600600063 16.98 59.51 6.37 M091600600064 17.22 50.91 5.49 M091600600065 17.46 44.31 4.84 M091600600066 17.71 37.76 4.21 M091600600067 17.95 32.30 3.72 M091600600068 18.20 29.72 3.48 M091600600069 18.44 26.07 3.11 M091600600070 18.69 25.99 3.11 M091600600071 18.93 22.09 2.84 M091600600072 19.17 18.34 2.66 M091600600073 19.42 18.62 2.68 M091600600074 19.66 19.41 2.76 M091600600075 19.91 16.74 2.47 M091600600076 20.15 16.88 2.40 M091600600077 20.40 16.50 2.61 M091600600078 20.64 16.49 2.50 M091600600079 20.89 14.47 2.30 M091600600080 21.13 16.81 2.78 M091600600081 21.37 16.00 2.84 M091600600082 21.62 18.32 2.97 M091600600083 21.86 16.46 2.88 M091600600084 22.11 21.16 3.19 M091600600085 22.35 16.64 3.04 M091600600086 22.60 15.03 3.13 M091600600087 22.84 17.40 3.28 M091600600088 23.09 17.60 3.33 M091600600089 23.33 18.82 3.44 M091600600090 23.57 17.75 3.18 M091600600091 23.82 17.51 2.57 M091600600092 24.06 16.41 2.46 M091600600093 24.31 14.22 2.85 M091600600094 24.55 14.43 2.71 M091600600095 25.04 13.81 2.68 M091600600096 25.53 10.47 2.20 M091600600097 26.02 6.78 2.10 M091600600098 26.51 6.65 2.10 M091600600099 27. 7.24 1.96 M091600600100 27.48 5.26 1.90 M091600600101 27.97 4.75 1.80 M091600600102 28.46 3.17 1.65 M091600600103 28.95 2.11 1.57 M091600600104 29.44 3.27 1.66 M091600600105 29.93 1.49 1.66 M091600600106 ENDDATA 79 0 M091600600107 ENDSUBENT 106 0 M091600699999 SUBENT M0916007 20150901 M081M091600700001 BIB 4 22 M091600700002 REACTION ((76-OS-189(G,2N)76-OS-187,,SIG,,,EVAL)+ M091600700003 (76-OS-189(G,2N+P)75-RE-186,,SIG,,,EVAL)) M091600700004 ANALYSIS The contribution of partial reaction (g,n) cross M091600700005 section into the experimental total neutron yield M091600700006 reaction (g,xn) cross section obtained using M091600700007 quasimonoenergetic annihilation photons at Livermore M091600700008 (USA) was evaluated using specially theoretically M091600700009 calculated transitional multiplicity function - M091600700010 ratio M091600700011 F2-theor = SIG-theor(g,2n)/SIG-theor(g,xn) M091600700012 by the way M091600700013 SIG-eval(g,n) = (F2-theor)x(SIG-exp(g,xn)). M091600700014 REL-REF (R,L0046012,B.L.Berman+,J,PR/C,19,1205,1979) M091600700015 Experimental data for the total neutron yield M091600700016 reaction (g,xn) cross section. M091600700017 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M091600700018 Theoretical preequilibrium model of photonuclear M091600700019 reactions based on the Fermi gas densities. M091600700020 STATUS Data plotted in Fig. 8. M091600700021 (DEP,L0011008) M091600700022 The total neutron yield reaction (g,xn) cross M091600700023 section. M091600700024 ENDBIB 22 0 M091600700025 NOCOMMON 0 0 M091600700026 DATA 3 56 M091600700027 EN DATA DATA-ERR M091600700028 MEV MB MB M091600700029 13.80 6.27 0.63 M091600700030 14.04 26.79 2.70 M091600700031 14.29 59.23 5.98 M091600700032 14.53 101.33 10.21 M091600700033 14.78 142.09 14.29 M091600700034 15.02 179.35 18.08 M091600700035 15.26 211.04 21.59 M091600700036 15.51 219.10 22.52 M091600700037 15.75 224.73 23.16 M091600700038 16.00 223.67 23.20 M091600700039 16.24 206.88 21.62 M091600700040 16.49 189.24 19.94 M091600700041 16.73 168.81 17.99 M091600700042 16.98 160.66 17.19 M091600700043 17.22 143.41 15.46 M091600700044 17.46 131.81 14.41 M091600700045 17.71 117.98 13.18 M091600700046 17.95 105.93 12.21 M091600700047 18.20 100.88 11.81 M091600700048 18.44 91.32 10.92 M091600700049 18.69 93.17 11.15 M091600700050 18.93 81.44 10.49 M091600700051 19.17 69.24 10.06 M091600700052 19.42 71.80 10.33 M091600700053 19.66 76.16 10.83 M091600700054 19.91 67.23 9.94 M091600700055 20.15 68.83 9.80 M091600700056 20.40 67.89 10.75 M091600700057 20.64 67.76 10.27 M091600700058 20.89 58.88 9.36 M091600700059 21.13 66.14 10.95 M091600700060 21.37 59.97 10.65 M091600700061 21.62 64.39 10.44 M091600700062 21.86 53.14 9.32 M091600700063 22.11 61.58 9.30 M091600700064 22.35 43.34 7.92 M091600700065 22.60 34.76 7.24 M091600700066 22.84 35.53 6.70 M091600700067 23.09 32.13 6.07 M091600700068 23.33 31.12 5.69 M091600700069 23.57 26.99 4.84 M091600700070 23.82 24.86 3.65 M091600700071 24.06 22.20 3.33 M091600700072 24.31 18.53 3.72 M091600700073 24.55 18.05 3.39 M091600700074 25.04 16.23 3.15 M091600700075 25.53 11.62 2.44 M091600700076 26.02 7.21 2.23 M091600700077 26.51 6.80 2.15 M091600700078 27. 7.11 1.93 M091600700079 27.48 4.99 1.80 M091600700080 27.97 4.36 1.66 M091600700081 28.46 2.83 1.47 M091600700082 28.95 1.84 1.37 M091600700083 29.44 2.78 1.41 M091600700084 29.93 1.24 1.38 M091600700085 ENDDATA 58 0 M091600700086 ENDSUBENT 85 0 M091600799999 SUBENT M0916008 20150901 M081M091600800001 BIB 4 22 M091600800002 REACTION ((76-OS-189(G,3N)76-OS-186,,SIG,,,EVAL)+ M091600800003 (76-OS-189(G,3N+P)75-RE-185,,SIG,,,EVAL)) M091600800004 ANALYSIS The contribution of partial reaction (g,n) cross M091600800005 section into the experimental total neutron yield M091600800006 reaction (g,xn) cross section obtained using M091600800007 quasimonoenergetic annihilation photons at Livermore M091600800008 (USA) was evaluated using specially theoretically M091600800009 calculated transitional multiplicity function - M091600800010 ratio M091600800011 F3-theor = SIG-theor(g,3n)/SIG-theor(g,xn) M091600800012 by the way M091600800013 SIG-eval(g,n) = (F3-theor)x(SIG-exp(g,xn)). M091600800014 REL-REF (R,L0046012,B.L.Berman+,J,PR/C,19,1205,1979) M091600800015 Experimental data for the total neutron yield M091600800016 reaction (g,xn) cross section. M091600800017 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M091600800018 Theoretical preequilibrium model of photonuclear M091600800019 reactions based on the Fermi gas densities. M091600800020 STATUS Data plotted in Fig. 8. M091600800021 (DEP,L0011008) M091600800022 The total neutron yield reaction (g,xn) cross M091600800023 section. M091600800024 ENDBIB 22 0 M091600800025 NOCOMMON 0 0 M091600800026 DATA 3 27 M091600800027 EN DATA DATA-ERR M091600800028 MEV MB MB M091600800029 20.89 0.04 0.01 M091600800030 21.13 0.80 0.13 M091600800031 21.37 1.95 0.34 M091600800032 21.62 4.14 0.67 M091600800033 21.86 5.84 1.02 M091600800034 22.11 10.59 1.59 M091600800035 22.35 10.80 1.97 M091600800036 22.60 11.91 2.48 M091600800037 22.84 16.09 3.03 M091600800038 23.09 18.55 3.51 M091600800039 23.33 22.36 4.08 M091600800040 23.57 23.53 4.22 M091600800041 23.82 25.78 3.78 M091600800042 24.06 26.76 4.02 M091600800043 24.31 25.59 5.14 M091600800044 24.55 28.45 5.35 M091600800045 25.04 32.11 6.24 M091600800046 25.53 28.13 5.92 M091600800047 26.02 20.57 6.37 M091600800048 26.51 22.38 7.08 M091600800049 27. 26.40 7.15 M091600800050 27.48 20.54 7.43 M091600800051 27.97 19.55 7.42 M091600800052 28.46 13.61 7.09 M091600800053 28.95 9.37 6.99 M091600800054 29.44 14.76 7.49 M091600800055 29.93 6.75 7.51 M091600800056 ENDDATA 29 0 M091600800057 ENDSUBENT 56 0 M091600899999 SUBENT M0916009 20150901 M081M091600900001 BIB 3 10 M091600900002 REACTION (76-OS-189(G,X)0-NN-1,UNW,SIG,,,EVAL) M091600900003 ANALYSIS The total neutron reaction cross section obtained M091600900004 as sum: SIG(g,sn) = SIG(g,n) + SIG(g,2n) + SIG(g,3n). M091600900005 STATUS Data plotted in Fig. 8. M091600900006 (DEP,M0916006) M091600900007 Evaluated (g,n) reaction cross section. M091600900008 (DEP,M0916007) M091600900009 Evaluated (g,2n) reaction cross section. M091600900010 (DEP,M0916008) M091600900011 Evaluated (g,3n) reaction cross section. M091600900012 ENDBIB 10 0 M091600900013 NOCOMMON 0 0 M091600900014 DATA 3 77 M091600900015 EN DATA DATA-ERR M091600900016 MEV MB MB M091600900017 7.44 24.27 3.27 M091600900018 7.93 29.56 3.59 M091600900019 8.42 37.29 4.31 M091600900020 8.91 46.01 5.14 M091600900021 9.40 59.37 6.38 M091600900022 9.89 83.86 8.69 M091600900023 10.13 87.33 9.09 M091600900024 10.38 103.28 10.69 M091600900025 10.62 126.21 12.94 M091600900026 10.87 146.86 15.03 M091600900027 11.11 170.51 17.35 M091600900028 11.35 198.77 20.20 M091600900029 11.60 239.55 24.31 M091600900030 11.84 287.01 29.04 M091600900031 12.09 337.15 34.08 M091600900032 12.33 390.95 39.48 M091600900033 12.58 419.21 42.32 M091600900034 12.82 440.69 44.49 M091600900035 13.06 451.41 45.55 M091600900036 13.31 466.08 46.99 M091600900037 13.55 469.54 47.39 M091600900038 13.80 473.32 47.13 M091600900039 14.04 473.56 45.15 M091600900040 14.29 459.39 40.85 M091600900041 14.53 454.59 37.05 M091600900042 14.78 434.40 32.70 M091600900043 15.02 418.32 30.13 M091600900044 15.26 404.63 29.29 M091600900045 15.51 372.69 27.50 M091600900046 15.75 353.72 26.70 M091600900047 16.00 333.64 25.85 M091600900048 16.24 296.82 23.58 M091600900049 16.49 265.64 21.51 M091600900050 16.73 233.89 19.28 M091600900051 16.98 220.17 18.34 M091600900052 17.22 194.33 16.40 M091600900053 17.46 176.12 15.20 M091600900054 17.71 155.75 13.84 M091600900055 17.95 138.24 12.77 M091600900056 18.20 130.61 12.31 M091600900057 18.44 117.40 11.36 M091600900058 18.69 119.17 11.58 M091600900059 18.93 103.54 10.87 M091600900060 19.17 87.58 10.41 M091600900061 19.42 90.42 10.67 M091600900062 19.66 95.58 11.18 M091600900063 19.91 83.97 10.24 M091600900064 20.15 85.71 10.09 M091600900065 20.40 84.39 11.06 M091600900066 20.64 84.26 10.57 M091600900067 20.89 73.41 9.64 M091600900068 21.13 83.76 11.29 M091600900069 21.37 77.94 11.03 M091600900070 21.62 86.86 10.88 M091600900071 21.86 75.44 9.82 M091600900072 22.11 93.34 9.96 M091600900073 22.35 70.80 8.71 M091600900074 22.60 61.72 8.27 M091600900075 22.84 69.03 8.05 M091600900076 23.09 68.28 7.77 M091600900077 23.33 72.31 7.80 M091600900078 23.57 68.27 7.17 M091600900079 23.82 68.16 5.85 M091600900080 24.06 65.38 5.78 M091600900081 24.31 58.35 6.96 M091600900082 24.55 60.95 6.90 M091600900083 25.04 62.15 7.49 M091600900084 25.53 50.23 6.77 M091600900085 26.02 34.57 7.07 M091600900086 26.51 35.84 7.70 M091600900087 27. 40.76 7.67 M091600900088 27.48 30.80 7.88 M091600900089 27.97 28.67 7.82 M091600900090 28.46 19.61 7.43 M091600900091 28.95 13.32 7.29 M091600900092 29.44 20.82 7.80 M091600900093 29.93 9.49 7.82 M091600900094 ENDDATA 79 0 M091600900095 ENDSUBENT 94 0 M091600999999 ENDENTRY 9 0 M091699999999