ENTRY M0922 20240508 M132M0922 0 1 SUBENT M0922001 20240508 M132M0922 1 1 BIB 9 34 M0922 1 2 TITLE Data on photoneutron reactions from various M0922 1 3 experiments for 133Cs, 138Ba and 209Bi nuclei. M0922 1 4 AUTHOR (V.V.Varlamov,B.S.Ishkhanov,V.N.Orlin, N.N.Peskov) M0922 1 5 REFERENCE (J,PAN,79,501,2016) M0922 1 6 #doi:10.1134/S1063778816040219 M0922 1 7 English translation of YF,79,(4),315,2016. M0922 1 8 (J,YF,79,315,2016) M0922 1 9 #doi:10.7868/S004400271604022X M0922 1 10 INSTITUTE (4RUSMOS) M0922 1 11 INC-SOURCE (QMPH,ARAD) M0922 1 12 ANALYSIS The joint analysis of data for total (g,xn) and M0922 1 13 partial (g,n), (g,2n) and (g,3n) reactions obtained M0922 1 14 in various experiments was carried out. The new M0922 1 15 approach to analysis of systematic disagreements M0922 1 16 between data was proposed on the base of new M0922 1 17 criteria of systematic uncertainties presence - M0922 1 18 specially proposed transitional multiplicity M0922 1 19 functions M0922 1 20 Fi-theor = SIG(g,in)/SIG(g,xn). M0922 1 21 Using these functions calculated in the frame of M0922 1 22 combined photonuclear reaction model new reliable M0922 1 23 and free from problems of neutron multiplicity M0922 1 24 sorting data for photoneutron partial reactions M0922 1 25 cross sections M0922 1 26 SIG-eval(g,in) = Fi-theor x SIG-exp(g,xn) M0922 1 27 were evaluated using experimental neutron yield M0922 1 28 reaction cross sections SIG-exp(g,xn). M0922 1 29 ERR-ANALYS (DATA-ERR) Mean-root-squared errors. M0922 1 30 STATUS (APRVD) Approved by V.Varlamov. M0922 1 31 HISTORY (20160808C) Data were compiled at the Russia MSU SINP M0922 1 32 CDFE by V.Varlamov. M0922 1 33 (20190110A) Corrected by V.Varlamov: STATUS. M0922 1 34 (20240508A) Corrected by V. Varlamov: REFERENCE, M0922 1 35 STATUS, REACTION (free text) in SUBENT 006. M0922 1 36 ENDBIB 34 0 M0922 1 37 NOCOMMON 0 0 M0922 1 38 ENDSUBENT 37 0 M0922 199999 SUBENT M0922002 20240508 M132M0922 2 1 BIB 4 12 M0922 2 2 REACTION (55-CS-133(G,X)0-NN-1,UNW,SIG,,,EVAL) M0922 2 3 ANALYSIS The total neutron reaction cross section obtained as M0922 2 4 sum: SIG(g,sn) = SIG(g,n) + SIG(g,2n) + SIG(g,3n). M0922 2 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 2 6 Data plotted in Fig. 3. M0922 2 7 (DEP,M0922003) M0922 2 8 Evaluated (g,n) reaction cross section. M0922 2 9 (DEP,M0922004) M0922 2 10 Evaluated (g,2n) reaction cross section. M0922 2 11 (DEP,M0922005) M0922 2 12 Evaluated (g,3n) reaction cross section. M0922 2 13 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 2 14 ENDBIB 12 0 M0922 2 15 NOCOMMON 0 0 M0922 2 16 DATA 3 66 M0922 2 17 EN DATA DATA-ERR M0922 2 18 MEV MB MB M0922 2 19 9.05 4.25 3.11 M0922 2 20 9.36 22.37 7.88 M0922 2 21 9.67 32.69 8.95 M0922 2 22 9.98 39.14 10.34 M0922 2 23 10.31 61.99 14.33 M0922 2 24 10.60 54.16 13.01 M0922 2 25 10.90 54.67 11.79 M0922 2 26 11.22 69.87 15.97 M0922 2 27 11.52 76.37 17.32 M0922 2 28 11.83 85.16 18.96 M0922 2 29 12.14 102.70 22.25 M0922 2 30 12.45 119.60 25.51 M0922 2 31 12.76 144.80 30.29 M0922 2 32 13.07 165.40 34.22 M0922 2 33 13.38 192.90 39.44 M0922 2 34 13.69 251.20 50.29 M0922 2 35 14.00 258.00 51.03 M0922 2 36 14.31 278.80 54.42 M0922 2 37 14.62 309.20 59.57 M0922 2 38 14.93 322.90 61.77 M0922 2 39 15.24 326.80 62.28 M0922 2 40 15.55 300.60 57.80 M0922 2 41 15.86 288.60 53.59 M0922 2 42 16.17 266.80 52.22 M0922 2 43 16.48 242.10 48.44 M0922 2 44 16.79 214.20 44.96 M0922 2 45 17.10 206.40 44.50 M0922 2 46 17.41 187.30 42.10 M0922 2 47 17.72 162.20 38.08 M0922 2 48 18.03 146.00 35.46 M0922 2 49 18.34 129.70 32.35 M0922 2 50 18.65 126.20 31.64 M0922 2 51 18.96 122.70 31.37 M0922 2 52 19.27 106.20 27.77 M0922 2 53 19.58 95.50 25.45 M0922 2 54 19.89 91.45 24.80 M0922 2 55 20.20 95.57 25.80 M0922 2 56 20.51 82.28 22.71 M0922 2 57 20.82 75.35 21.18 M0922 2 58 21.13 71.20 20.15 M0922 2 59 21.43 69.17 19.73 M0922 2 60 21.75 68.15 19.49 M0922 2 61 22.06 73.72 20.74 M0922 2 62 22.36 69.97 20.12 M0922 2 63 22.67 64.42 17.37 M0922 2 64 22.98 61.62 18.22 M0922 2 65 23.29 57.77 17.69 M0922 2 66 23.60 55.22 17.04 M0922 2 67 23.91 43.78 14.77 M0922 2 68 24.22 47.54 15.68 M0922 2 69 24.53 43.08 14.85 M0922 2 70 24.84 42.56 14.83 M0922 2 71 25.15 35.42 13.76 M0922 2 72 25.46 34.43 14.16 M0922 2 73 25.77 35.08 15.04 M0922 2 74 26.08 29.44 15.29 M0922 2 75 26.39 44.05 19.07 M0922 2 76 27.01 29.44 17.55 M0922 2 77 27.32 36.82 19.03 M0922 2 78 27.63 29.82 17.05 M0922 2 79 27.94 26.04 16.05 M0922 2 80 28.25 17.58 13.42 M0922 2 81 28.56 27.00 16.55 M0922 2 82 28.87 20.55 14.76 M0922 2 83 29.18 20.86 16.89 M0922 2 84 29.49 20.62 19.57 M0922 2 85 ENDDATA 68 0 M0922 2 86 ENDSUBENT 85 0 M0922 299999 SUBENT M0922003 20240508 M132M0922 3 1 BIB 5 25 M0922 3 2 REACTION ((55-CS-133(G,N)55-CS-132,,SIG,,,EVAL)+ M0922 3 3 (55-CS-133(G,N+P)54-XE-131,,SIG,,,EVAL)) M0922 3 4 ANALYSIS The contribution of partial reaction (g,n) cross M0922 3 5 section into the experimental total neutron yield M0922 3 6 reaction (g,xn) cross section obtained using M0922 3 7 quasimonoenergetic annihilation photons at Livermore M0922 3 8 (USA) was evaluated using specially theoretically M0922 3 9 calculated transitional multiplicity function - M0922 3 10 ratio M0922 3 11 F1-theor = SIG-theor(g,n)/SIG-theor(g,xn) M0922 3 12 by the way M0922 3 13 SIG-eval(g,n) = (F1-theor)x(SIG-exp(g,xn)). M0922 3 14 REL-REF (R,L0014008,B.L.Berman+,J,PR,177,1745,1969) M0922 3 15 Experimental data for the total neutron yield M0922 3 16 reaction (g,xn)= (g,n) + 2(g,2n) + 3(g,3n) cross M0922 3 17 section. M0922 3 18 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M0922 3 19 Theoretical preequilibrium model of photonuclear M0922 3 20 reactions based on the Fermi gas densities. M0922 3 21 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 3 22 Data plotted in Fig. 3. M0922 3 23 (DEP,L0014008) M0922 3 24 The neutron yield reaction (g,xn) = (g,n) + 2(g,2n) M0922 3 25 + 3(g,3n) cross section. M0922 3 26 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 3 27 ENDBIB 25 0 M0922 3 28 NOCOMMON 0 0 M0922 3 29 DATA 3 66 M0922 3 30 EN DATA DATA-ERR M0922 3 31 MEV MB MB M0922 3 32 9.05 4.25 3.04 M0922 3 33 9.36 22.37 7.63 M0922 3 34 9.67 32.69 8.60 M0922 3 35 9.98 39.14 9.92 M0922 3 36 10.31 61.99 13.66 M0922 3 37 10.60 54.16 12.42 M0922 3 38 10.90 54.67 11.19 M0922 3 39 11.22 69.87 15.20 M0922 3 40 11.52 76.37 16.48 M0922 3 41 11.83 85.16 18.03 M0922 3 42 12.14 102.70 21.13 M0922 3 43 12.45 119.60 24.20 M0922 3 44 12.76 144.80 28.71 M0922 3 45 13.07 165.40 32.41 M0922 3 46 13.38 192.90 37.33 M0922 3 47 13.69 251.20 47.54 M0922 3 48 14.00 258.00 48.21 M0922 3 49 14.31 278.80 51.37 M0922 3 50 14.62 309.20 56.18 M0922 3 51 14.93 322.90 58.23 M0922 3 52 15.24 326.80 58.70 M0922 3 53 15.55 300.60 54.51 M0922 3 54 15.86 288.40 50.41 M0922 3 55 16.17 263.30 48.96 M0922 3 56 16.48 226.70 43.84 M0922 3 57 16.79 181.30 38.28 M0922 3 58 17.10 152.60 35.35 M0922 3 59 17.41 118.90 31.24 M0922 3 60 17.72 88.06 26.57 M0922 3 61 18.03 68.43 23.52 M0922 3 62 18.34 53.41 20.61 M0922 3 63 18.65 46.50 19.65 M0922 3 64 18.96 41.26 19.00 M0922 3 65 19.27 33.21 16.44 M0922 3 66 19.58 28.30 14.79 M0922 3 67 19.89 26.20 14.21 M0922 3 68 20.20 27.05 14.79 M0922 3 69 20.51 23.55 12.89 M0922 3 70 20.82 22.27 11.99 M0922 3 71 21.13 22.09 11.48 M0922 3 72 21.43 22.64 11.33 M0922 3 73 21.75 23.49 11.32 M0922 3 74 22.06 26.34 12.24 M0922 3 75 22.36 25.44 11.82 M0922 3 76 22.67 23.45 10.46 M0922 3 77 22.98 22.14 10.55 M0922 3 78 23.29 20.32 10.05 M0922 3 79 23.60 18.94 9.59 M0922 3 80 23.91 14.60 7.97 M0922 3 81 24.22 15.43 8.46 M0922 3 82 24.53 13.63 7.82 M0922 3 83 24.84 13.15 7.73 M0922 3 84 25.15 10.72 6.99 M0922 3 85 25.46 10.21 7.18 M0922 3 86 25.77 10.19 7.66 M0922 3 87 26.08 8.40 7.18 M0922 3 88 26.39 12.36 9.64 M0922 3 89 27.01 8.01 7.79 M0922 3 90 27.32 9.88 8.98 M0922 3 91 27.63 7.88 7.75 M0922 3 92 27.94 6.79 7.11 M0922 3 93 28.25 4.52 5.49 M0922 3 94 28.56 6.85 7.42 M0922 3 95 28.87 5.14 6.22 M0922 3 96 29.18 5.15 6.80 M0922 3 97 29.49 5.03 7.44 M0922 3 98 ENDDATA 68 0 M0922 3 99 ENDSUBENT 98 0 M0922 399999 SUBENT M0922004 20240508 M132M0922 4 1 BIB 5 24 M0922 4 2 REACTION ((55-CS-133(G,2N)55-CS-131,,SIG,,,EVAL)+ M0922 4 3 (55-CS-133(G,2N+P)54-XE-130,,SIG,,,EVAL)) M0922 4 4 ANALYSIS The contribution of partial reaction (g,n) cross M0922 4 5 section into the experimental total neutron yield M0922 4 6 reaction (g,xn) = (g,n) + 2(g,2n) cross section M0922 4 7 obtained using quasimonoenergetic annihilation M0922 4 8 photons at Livermore (USA) was evaluated using M0922 4 9 specially theoretically calculated transitional M0922 4 10 multiplicity function - ratio M0922 4 11 F2-theor = SIG-theor(g,n)/SIG-theor(g,xn) M0922 4 12 by the way M0922 4 13 SIG-eval(g,n) = (F2-theor)x(SIG-exp(g,xn)). M0922 4 14 REL-REF (R,L0014008,B.L.Berman+,J,PR,177,1745,1969) M0922 4 15 Experimental data for the total neutron yield M0922 4 16 reaction (g,xn) cross section. M0922 4 17 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M0922 4 18 Theoretical preequilibrium model of photonuclear M0922 4 19 reactions based on the Fermi gas densities. M0922 4 20 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 4 21 Data plotted in Fig. 3. M0922 4 22 (DEP,L0014008) M0922 4 23 The neutron yield reaction (g,xn) = (g,n) + 2(g,2n) + M0922 4 24 3(g,3n) cross section. M0922 4 25 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 4 26 ENDBIB 24 0 M0922 4 27 NOCOMMON 0 0 M0922 4 28 DATA 3 44 M0922 4 29 EN DATA DATA-ERR M0922 4 30 MEV MB MB M0922 4 31 15.86 0.26 3.07 M0922 4 32 16.17 3.52 3.17 M0922 4 33 16.48 15.38 4.50 M0922 4 34 16.79 32.93 6.59 M0922 4 35 17.10 53.73 9.06 M0922 4 36 17.41 68.41 10.77 M0922 4 37 17.72 74.17 11.43 M0922 4 38 18.03 77.53 11.87 M0922 4 39 18.34 76.29 11.67 M0922 4 40 18.65 79.65 11.91 M0922 4 41 18.96 81.41 12.30 M0922 4 42 19.27 72.98 11.27 M0922 4 43 19.58 67.19 10.60 M0922 4 44 19.89 65.25 10.53 M0922 4 45 20.20 68.52 10.95 M0922 4 46 20.51 58.73 9.76 M0922 4 47 20.82 53.08 9.14 M0922 4 48 21.13 49.11 8.63 M0922 4 49 21.43 46.53 8.35 M0922 4 50 21.75 44.66 8.13 M0922 4 51 22.06 47.38 8.46 M0922 4 52 22.36 44.53 8.26 M0922 4 53 22.67 40.98 6.87 M0922 4 54 22.98 39.47 7.63 M0922 4 55 23.29 37.44 7.60 M0922 4 56 23.60 36.29 7.42 M0922 4 57 23.91 29.18 6.78 M0922 4 58 24.22 32.11 7.19 M0922 4 59 24.53 29.45 7.01 M0922 4 60 24.84 29.41 7.08 M0922 4 61 25.15 24.70 6.75 M0922 4 62 25.46 24.21 6.95 M0922 4 63 25.77 24.82 7.34 M0922 4 64 26.08 20.81 8.01 M0922 4 65 26.39 30.82 9.16 M0922 4 66 27.01 19.44 8.89 M0922 4 67 27.32 23.18 8.73 M0922 4 68 27.63 17.70 7.62 M0922 4 69 27.94 14.42 6.84 M0922 4 70 28.25 12.74 5.60 M0922 4 71 28.56 9.01 6.02 M0922 4 72 28.87 8.90 5.16 M0922 4 73 29.18 8.26 5.57 M0922 4 74 29.49 7.44 6.08 M0922 4 75 ENDDATA 46 0 M0922 4 76 ENDSUBENT 75 0 M0922 499999 SUBENT M0922005 20240508 M132M0922 5 1 BIB 5 24 M0922 5 2 REACTION ((55-CS-133(G,3N)55-CS-130,,SIG,,,EVAL)+ M0922 5 3 (55-CS-133(G,3N+P)54-XE-129,,SIG,,,EVAL)) M0922 5 4 ANALYSIS The contribution of partial reaction (g,n) cross M0922 5 5 section into the experimental total neutron yield M0922 5 6 reaction (g,xn) = (g,n) + 2(g,2n) cross section M0922 5 7 obtained using quasimonoenergetic annihilation M0922 5 8 photons at Livermore (USA) was evaluated using M0922 5 9 specially theoretically calculated transitional M0922 5 10 multiplicity function - ratio M0922 5 11 F2-theor = SIG-theor(g,n)/SIG-theor(g,xn) M0922 5 12 by the way M0922 5 13 SIG-eval(g,n) = (F2-theor)x(SIG-exp(g,xn)). M0922 5 14 REL-REF (R,L0014008,B.L.Berman+,J,PR,177,1745,1969) M0922 5 15 Experimental data for the total neutron yield M0922 5 16 reaction (g,xn) cross section. M0922 5 17 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M0922 5 18 Theoretical preequilibrium model of photonuclear M0922 5 19 reactions based on the Fermi gas densities. M0922 5 20 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 5 21 Data plotted in Fig. 3. M0922 5 22 (DEP,L0014008) M0922 5 23 The neutron yield reaction (g,xn) = (g,n) + 2(g,2n) + M0922 5 24 3(g,3n) cross section. M0922 5 25 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 5 26 ENDBIB 24 0 M0922 5 27 NOCOMMON 0 0 M0922 5 28 DATA 3 13 M0922 5 29 EN DATA DATA-ERR M0922 5 30 MEV MB MB M0922 5 31 25.46 0.01 0.03 M0922 5 32 25.77 0.07 0.04 M0922 5 33 26.08 0.23 0.10 M0922 5 34 26.39 0.87 0.27 M0922 5 35 27.01 1.98 0.86 M0922 5 36 27.32 3.77 1.31 M0922 5 37 27.63 4.24 1.68 M0922 5 38 27.94 4.05 2.10 M0922 5 39 28.25 4.83 2.33 M0922 5 40 28.56 6.51 3.11 M0922 5 41 28.87 7.41 3.39 M0922 5 42 29.18 7.45 4.52 M0922 5 43 29.49 8.15 6.05 M0922 5 44 ENDDATA 15 0 M0922 5 45 ENDSUBENT 44 0 M0922 599999 SUBENT M0922006 20240508 M132M0922 6 1 BIB 4 13 M0922 6 2 REACTION (56-BA-138(G,X)0-NN-1,UNW,SIG,,,EVAL) M0922 6 3 ANALYSIS The total neutron reaction cross section obtained as M0922 6 4 sum: SIG(g,sn) = SIG(g,n) + SIG(g,2n) + SIG(g,3n). M0922 6 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 6 6 Data plotted in Fig. 5. M0922 6 7 (DEP,M0922007) M0922 6 8 Evaluated (g,n) reaction cross section. M0922 6 9 (DEP,M0922008) M0922 6 10 Evaluated (g,2n) reaction cross section. M0922 6 11 (DEP,M0922009) M0922 6 12 Evaluated (g,3n) reaction cross section. M0922 6 13 HISTORY (20240508U) Corrected by V.Varlamov: REACTION, M0922 6 14 (free text), STATUS. M0922 6 15 ENDBIB 13 0 M0922 6 16 NOCOMMON 0 0 M0922 6 17 DATA 3 61 M0922 6 18 EN DATA DATA-ERR M0922 6 19 MEV MB MB M0922 6 20 8.48 1.50 1.03 M0922 6 21 8.79 14.27 3.94 M0922 6 22 9.10 21.48 4.59 M0922 6 23 9.41 35.57 7.37 M0922 6 24 9.72 30.58 5.86 M0922 6 25 10.03 37.12 6.73 M0922 6 26 10.34 41.58 7.38 M0922 6 27 10.65 52.84 8.96 M0922 6 28 10.96 54.26 7.94 M0922 6 29 11.27 63.67 10.45 M0922 6 30 11.57 78.22 12.83 M0922 6 31 11.89 83.91 12.80 M0922 6 32 12.19 101.20 14.73 M0922 6 33 12.50 122.10 17.42 M0922 6 34 12.81 147.80 20.81 M0922 6 35 13.12 170.60 23.65 M0922 6 36 13.43 194.10 26.80 M0922 6 37 13.74 214.10 29.34 M0922 6 38 14.05 245.70 32.33 M0922 6 39 14.36 267.80 34.97 M0922 6 40 14.67 307.00 40.00 M0922 6 41 14.98 319.20 41.56 M0922 6 42 15.29 335.80 43.83 M0922 6 43 15.60 314.50 41.42 M0922 6 44 15.91 302.00 39.90 M0922 6 45 16.22 260.70 37.07 M0922 6 46 16.53 235.40 34.56 M0922 6 47 16.84 207.20 31.48 M0922 6 48 17.15 176.00 27.81 M0922 6 49 17.46 161.30 26.88 M0922 6 50 17.77 141.10 23.64 M0922 6 51 18.08 135.20 23.10 M0922 6 52 18.39 122.40 21.17 M0922 6 53 18.70 112.40 19.82 M0922 6 54 19.01 96.60 17.56 M0922 6 55 19.32 91.64 17.53 M0922 6 56 19.63 81.62 16.10 M0922 6 57 19.94 76.22 15.32 M0922 6 58 20.25 74.98 15.02 M0922 6 59 20.56 79.58 16.11 M0922 6 60 20.87 63.18 13.64 M0922 6 61 21.18 67.42 14.44 M0922 6 62 21.48 74.04 15.63 M0922 6 63 21.80 68.52 14.83 M0922 6 64 22.11 45.51 11.33 M0922 6 65 22.41 46.95 10.18 M0922 6 66 22.72 45.47 11.01 M0922 6 67 23.03 49.91 11.81 M0922 6 68 23.34 49.25 11.80 M0922 6 69 23.65 38.99 10.15 M0922 6 70 23.96 33.88 9.48 M0922 6 71 24.27 29.88 9.20 M0922 6 72 24.58 22.46 7.78 M0922 6 73 24.89 24.93 9.03 M0922 6 74 25.20 33.42 10.50 M0922 6 75 25.51 26.17 10.25 M0922 6 76 25.82 17.41 8.54 M0922 6 77 26.13 20.44 9.36 M0922 6 78 26.44 26.09 10.99 M0922 6 79 26.75 20.93 9.85 M0922 6 80 27.06 16.53 9.05 M0922 6 81 ENDDATA 63 0 M0922 6 82 ENDSUBENT 81 0 M0922 699999 SUBENT M0922007 20240508 M132M0922 7 1 BIB 5 24 M0922 7 2 REACTION ((56-BA-138(G,N)56-BA-137,,SIG,,,EVAL)+ M0922 7 3 (56-BA-138(G,N+P)55-CS-136,,SIG,,,EVAL)) M0922 7 4 ANALYSIS The contribution of partial reaction (g,n) cross M0922 7 5 section into the experimental total neutron yield M0922 7 6 reaction (g,xn) cross section obtained using M0922 7 7 quasimonoenergetic annihilation photons at Livermore M0922 7 8 (USA) was evaluated using specially theoretically M0922 7 9 calculated transitional multiplicity function - M0922 7 10 ratio M0922 7 11 F1-theor = SIG-theor(g,n)/SIG-theor(g,xn) M0922 7 12 by the way M0922 7 13 SIG-eval(g,n) = (F1-theor)x(SIG-exp(g,xn)). M0922 7 14 REL-REF (R,L0019004,B.L.Berman+,J,PR/C,2,2318,1970) M0922 7 15 Experimental data for the total neutron yield M0922 7 16 reaction (g,xn)= (g,n) + 2(g,2n) cross section. M0922 7 17 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M0922 7 18 Theoretical preequilibrium model of photonuclear M0922 7 19 reactions based on the Fermi gas densities. M0922 7 20 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 7 21 Data plotted in Fig. 5. M0922 7 22 (DEP,L0019004) M0922 7 23 The neutron yield reaction (g,xn) = (g,n) + 2(g,2n) M0922 7 24 + 3(g,3n) cross section19 M0922 7 25 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 7 26 ENDBIB 24 0 M0922 7 27 NOCOMMON 0 0 M0922 7 28 DATA 3 61 M0922 7 29 EN DATA DATA-ERR M0922 7 30 MEV MB MB M0922 7 31 8.48 1.50 0.95 M0922 7 32 8.79 14.27 3.73 M0922 7 33 9.10 21.48 4.35 M0922 7 34 9.41 35.57 6.97 M0922 7 35 9.72 30.58 5.52 M0922 7 36 10.03 37.12 6.32 M0922 7 37 10.34 41.58 6.91 M0922 7 38 10.65 52.84 8.37 M0922 7 39 10.96 54.26 7.34 M0922 7 40 11.27 63.67 9.74 M0922 7 41 11.57 78.22 11.96 M0922 7 42 11.89 83.91 11.86 M0922 7 43 12.19 101.20 13.61 M0922 7 44 12.50 122.10 16.06 M0922 7 45 12.81 147.80 19.16 M0922 7 46 13.12 170.60 21.75 M0922 7 47 13.43 194.10 24.63 M0922 7 48 13.74 214.10 26.95 M0922 7 49 14.05 245.70 29.60 M0922 7 50 14.36 267.80 31.99 M0922 7 51 14.67 307.00 36.58 M0922 7 52 14.98 319.10 38.00 M0922 7 53 15.29 333.90 39.97 M0922 7 54 15.60 304.30 37.04 M0922 7 55 15.91 275.00 34.17 M0922 7 56 16.22 216.00 29.96 M0922 7 57 16.53 171.90 25.97 M0922 7 58 16.84 130.10 21.93 M0922 7 59 17.15 94.19 18.07 M0922 7 60 17.46 73.83 16.36 M0922 7 61 17.77 56.17 13.79 M0922 7 62 18.08 47.66 12.98 M0922 7 63 18.39 38.71 11.55 M0922 7 64 18.70 32.42 10.52 M0922 7 65 19.01 25.83 9.06 M0922 7 66 19.32 22.89 8.70 M0922 7 67 19.63 19.11 7.77 M0922 7 68 19.94 16.89 7.24 M0922 7 69 20.25 15.93 7.06 M0922 7 70 20.56 16.34 7.48 M0922 7 71 20.87 12.61 6.08 M0922 7 72 21.18 13.15 6.44 M0922 7 73 21.48 14.24 7.00 M0922 7 74 21.80 13.27 6.56 M0922 7 75 22.11 9.01 4.67 M0922 7 76 22.41 9.55 4.54 M0922 7 77 22.72 9.46 4.66 M0922 7 78 23.03 10.53 5.08 M0922 7 79 23.34 10.48 5.05 M0922 7 80 23.65 8.33 4.18 M0922 7 81 23.96 7.25 3.77 M0922 7 82 24.27 6.42 3.51 M0922 7 83 24.58 4.85 2.83 M0922 7 84 24.89 5.39 3.23 M0922 7 85 25.20 7.21 4.09 M0922 7 86 25.51 5.61 3.73 M0922 7 87 25.82 3.68 2.92 M0922 7 88 26.13 4.25 3.28 M0922 7 89 26.44 5.33 3.99 M0922 7 90 26.75 4.18 3.41 M0922 7 91 27.06 3.22 2.94 M0922 7 92 ENDDATA 63 0 M0922 7 93 ENDSUBENT 92 0 M0922 799999 SUBENT M0922008 20240508 M132M0922 8 1 BIB 5 24 M0922 8 2 REACTION ((56-BA-138(G,2N)56-BA-136,,SIG,,,EVAL)+ M0922 8 3 (56-BA-138(G,2N+P)55-CS-135,,SIG,,,EVAL)) M0922 8 4 ANALYSIS The contribution of partial reaction (g,n) cross M0922 8 5 section into the experimental total neutron yield M0922 8 6 reaction (g,xn) = (g,n) + 2(g,2n) cross section M0922 8 7 obtained using quasimonoenergetic annihilation M0922 8 8 photons at Livermore (USA) was evaluated using M0922 8 9 specially theoretically calculated transitional M0922 8 10 multiplicity function - ratio M0922 8 11 F2-theor = SIG-theor(g,n)/SIG-theor(g,xn) M0922 8 12 by the way M0922 8 13 SIG-eval(g,n) = (F2-theor)x(SIG-exp(g,xn)). M0922 8 14 REL-REF (R,L0019004,B.L.Berman+,J,PR/C,2,2318,1970) M0922 8 15 Experimental data for the total neutron yield M0922 8 16 reaction (g,xn)= (g,n) + 2(g,2n)cross section. M0922 8 17 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M0922 8 18 Theoretical preequilibrium model of photonuclear M0922 8 19 reactions based on the Fermi gas densities. M0922 8 20 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 8 21 Data plotted in Fig. 5. M0922 8 22 (DEP,L0019004) M0922 8 23 The neutron yield reaction (g,xn) = (g,n) + 2(g,2n) M0922 8 24 + 3(g,3n) cross section. M0922 8 25 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 8 26 ENDBIB 24 0 M0922 8 27 NOCOMMON 0 0 M0922 8 28 DATA 3 40 M0922 8 29 EN DATA DATA-ERR M0922 8 30 MEV MB MB M0922 8 31 14.98 0.08 3.41 M0922 8 32 15.29 1.88 3.70 M0922 8 33 15.60 10.24 4.23 M0922 8 34 15.91 26.99 5.58 M0922 8 35 16.22 44.65 6.97 M0922 8 36 16.53 63.49 8.45 M0922 8 37 16.84 77.13 9.42 M0922 8 38 17.15 81.78 9.62 M0922 8 39 17.46 87.51 10.41 M0922 8 40 17.77 84.97 9.74 M0922 8 41 18.08 87.56 10.01 M0922 8 42 18.39 83.66 9.52 M0922 8 43 18.70 79.94 9.21 M0922 8 44 19.01 70.77 8.43 M0922 8 45 19.32 68.74 8.75 M0922 8 46 19.63 62.51 8.26 M0922 8 47 19.94 59.33 8.02 M0922 8 48 20.25 59.05 7.90 M0922 8 49 20.56 63.24 8.56 M0922 8 50 20.87 50.58 7.51 M0922 8 51 21.18 54.28 7.95 M0922 8 52 21.48 59.80 8.56 M0922 8 53 21.80 55.25 8.21 M0922 8 54 22.11 36.50 6.62 M0922 8 55 22.41 37.40 5.59 M0922 8 56 22.72 36.02 6.31 M0922 8 57 23.03 39.38 6.69 M0922 8 58 23.34 38.77 6.71 M0922 8 59 23.65 30.66 5.95 M0922 8 60 23.96 26.63 5.68 M0922 8 61 24.27 23.46 5.66 M0922 8 62 24.58 17.61 4.93 M0922 8 63 24.89 19.53 5.78 M0922 8 64 25.20 26.14 6.37 M0922 8 65 25.51 20.30 6.42 M0922 8 66 25.82 13.26 5.43 M0922 8 67 26.13 15.17 5.71 M0922 8 68 26.44 18.70 6.34 M0922 8 69 26.75 14.36 5.57 M0922 8 70 27.06 10.75 5.00 M0922 8 71 ENDDATA 42 0 M0922 8 72 ENDSUBENT 71 0 M0922 899999 SUBENT M0922009 20240508 M132M0922 9 1 BIB 5 24 M0922 9 2 REACTION ((56-BA-138(G,3N)56-BA-135,,SIG,,,EVAL)+ M0922 9 3 (56-BA-138(G,3N+P)55-CS-134,,SIG,,,EVAL)) M0922 9 4 ANALYSIS The contribution of partial reaction (g,n) cross M0922 9 5 section into the experimental total neutron yield M0922 9 6 reaction (g,xn) = (g,n) + 2(g,2n) cross section M0922 9 7 obtained using quasimonoenergetic annihilation M0922 9 8 photons at Livermore (USA) was evaluated using M0922 9 9 specially theoretically calculated transitional M0922 9 10 multiplicity function - ratio M0922 9 11 F2-theor = SIG-theor(g,n)/SIG-theor(g,xn) M0922 9 12 by the way M0922 9 13 SIG-eval(g,n) = (F2-theor)x(SIG-exp(g,xn)). M0922 9 14 REL-REF (R,L0019004,B.L.Berman+,J,PR/C,2,2318,1970) M0922 9 15 Experimental data for the total neutron yield M0922 9 16 reaction (g,xn)= (g,n) + 2(g,2n)cross section. M0922 9 17 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M0922 9 18 Theoretical preequilibrium model of photonuclear M0922 9 19 reactions based on the Fermi gas densities. M0922 9 20 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 9 21 Data plotted in Fig. 5. M0922 9 22 (DEP,L0019004) M0922 9 23 The neutron yield reaction (g,xn) = (g,n) + 2(g,2n) M0922 9 24 + 3(g,3n) cross section. M0922 9 25 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 9 26 ENDBIB 24 0 M0922 9 27 NOCOMMON 0 0 M0922 9 28 DATA 3 7 M0922 9 29 EN DATA DATA-ERR M0922 9 30 MEV MB MB M0922 9 31 25.20 0.07 0.04 M0922 9 32 25.51 0.27 0.10 M0922 9 33 25.82 0.47 0.20 M0922 9 34 26.13 1.01 0.37 M0922 9 35 26.44 2.06 0.66 M0922 9 36 26.75 2.40 0.87 M0922 9 37 27.06 2.56 1.11 M0922 9 38 ENDDATA 9 0 M0922 9 39 ENDSUBENT 38 0 M0922 999999 SUBENT M0922010 20240508 M132M0922 10 1 BIB 4 12 M0922 10 2 REACTION (83-BI-209(G,X)0-NN-1,UNW,SIG,,,EVAL) M0922 10 3 ANALYSIS The total neutron reaction cross section obtained as M0922 10 4 sum: SIG(g,sn) = SIG(g,n) + SIG(g,2n) + SIG(g,3n). M0922 10 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 10 6 Data plotted in Fig. 7. M0922 10 7 (DEP,M0922011) M0922 10 8 Evaluated (g,n) reaction cross section. M0922 10 9 (DEP,M0922012) M0922 10 10 Evaluated (g,2n) reaction cross section. M0922 10 11 (DEP,M0922013) M0922 10 12 Evaluated (g,3n) reaction cross section. M0922 10 13 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 10 14 ENDBIB 12 0 M0922 10 15 NOCOMMON 0 0 M0922 10 16 DATA 3 109 M0922 10 17 EN DATA DATA-ERR M0922 10 18 MEV MB MB M0922 10 19 8.01 37.96 7.16 M0922 10 20 8.17 36.71 6.98 M0922 10 21 8.32 42.47 7.60 M0922 10 22 8.48 47.50 8.27 M0922 10 23 8.63 70.00 13.42 M0922 10 24 8.79 47.50 8.27 M0922 10 25 8.94 70.00 13.43 M0922 10 26 9.10 73.50 13.91 M0922 10 27 9.25 59.50 12.17 M0922 10 28 9.41 80.00 14.69 M0922 10 29 9.56 74.50 14.49 M0922 10 30 9.72 92.50 17.20 M0922 10 31 9.87 92.00 17.15 M0922 10 32 10.03 112.50 18.62 M0922 10 33 10.18 112.00 19.59 M0922 10 34 10.34 112.00 18.56 M0922 10 35 10.49 135.00 21.37 M0922 10 36 10.65 145.00 22.48 M0922 10 37 10.80 162.50 24.71 M0922 10 38 10.96 181.00 26.78 M0922 10 39 11.11 199.50 29.22 M0922 10 40 11.27 226.00 31.17 M0922 10 41 11.42 237.00 33.81 M0922 10 42 11.57 274.00 37.91 M0922 10 43 11.73 275.50 38.51 M0922 10 44 11.89 302.00 47.26 M0922 10 45 12.04 324.00 50.43 M0922 10 46 12.19 332.50 49.91 M0922 10 47 12.35 358.00 53.57 M0922 10 48 12.50 384.00 57.28 M0922 10 49 12.66 426.00 67.64 M0922 10 50 12.81 425.50 66.88 M0922 10 51 12.97 530.00 80.27 M0922 10 52 13.12 478.00 73.21 M0922 10 53 13.28 510.00 77.80 M0922 10 54 13.43 511.50 77.29 M0922 10 55 13.59 544.00 82.67 M0922 10 56 13.74 501.00 77.29 M0922 10 57 13.90 515.00 79.98 M0922 10 58 14.05 515.00 78.25 M0922 10 59 14.21 454.00 66.72 M0922 10 60 14.36 477.70 68.09 M0922 10 61 14.52 444.20 66.91 M0922 10 62 14.67 407.10 64.50 M0922 10 63 14.83 371.30 60.15 M0922 10 64 14.98 368.30 56.64 M0922 10 65 15.14 324.30 53.47 M0922 10 66 15.29 338.20 54.83 M0922 10 67 15.45 293.70 46.31 M0922 10 68 15.60 277.80 46.77 M0922 10 69 15.76 264.50 47.19 M0922 10 70 15.91 242.40 44.27 M0922 10 71 16.07 228.80 40.63 M0922 10 72 16.22 206.90 40.81 M0922 10 73 16.38 205.60 39.75 M0922 10 74 16.53 206.60 43.30 M0922 10 75 16.68 186.50 40.62 M0922 10 76 16.84 162.20 36.94 M0922 10 77 17.00 167.30 37.80 M0922 10 78 17.15 149.50 34.62 M0922 10 79 17.30 147.20 34.33 M0922 10 80 17.46 174.70 39.16 M0922 10 81 17.61 149.80 35.12 M0922 10 82 17.77 135.50 32.43 M0922 10 83 17.92 118.30 29.93 M0922 10 84 18.08 120.10 30.40 M0922 10 85 18.23 108.80 28.09 M0922 10 86 18.39 105.90 28.15 M0922 10 87 18.54 109.80 28.22 M0922 10 88 18.70 99.75 26.43 M0922 10 89 18.85 93.66 25.71 M0922 10 90 19.01 117.00 30.59 M0922 10 91 19.32 84.70 23.99 M0922 10 92 19.47 96.80 26.54 M0922 10 93 19.63 83.67 25.68 M0922 10 94 19.78 83.49 25.25 M0922 10 95 19.94 75.92 22.88 M0922 10 96 20.09 81.80 25.39 M0922 10 97 20.25 102.50 32.60 M0922 10 98 20.40 91.02 30.49 M0922 10 99 20.56 89.28 24.59 M0922 10 100 20.71 78.19 23.30 M0922 10 101 20.87 83.04 23.94 M0922 10 102 21.02 67.43 20.93 M0922 10 103 21.18 72.88 22.34 M0922 10 104 21.33 81.50 24.99 M0922 10 105 21.48 83.30 24.31 M0922 10 106 21.64 89.11 25.42 M0922 10 107 21.80 73.21 22.40 M0922 10 108 21.95 88.49 29.80 M0922 10 109 22.11 72.25 21.92 M0922 10 110 22.26 68.32 22.15 M0922 10 111 22.41 74.43 24.17 M0922 10 112 22.57 65.58 25.81 M0922 10 113 22.72 54.69 20.31 M0922 10 114 22.88 76.89 24.72 M0922 10 115 23.03 69.70 22.72 M0922 10 116 23.19 40.90 18.24 M0922 10 117 23.34 54.72 27.08 M0922 10 118 23.65 74.19 27.87 M0922 10 119 23.96 36.37 21.11 M0922 10 120 24.27 50.04 24.01 M0922 10 121 24.58 57.51 26.04 M0922 10 122 24.89 49.48 24.99 M0922 10 123 25.20 45.96 22.67 M0922 10 124 25.51 34.54 21.80 M0922 10 125 25.82 51.43 27.57 M0922 10 126 26.13 46.46 29.77 M0922 10 127 26.44 65.55 32.64 M0922 10 128 ENDDATA 111 0 M0922 10 129 ENDSUBENT 128 0 M0922 1099999 SUBENT M0922011 20240508 M132M0922 11 1 BIB 5 27 M0922 11 2 REACTION ((83-BI-209(G,N)83-BI-208,,SIG,,,EVAL)+ M0922 11 3 (83-BI-209(G,N+P)82-PB-207,,SIG,,,EVAL)) M0922 11 4 ANALYSIS The contribution of partial reaction (g,n) cross M0922 11 5 section into the experimental total neutron yield M0922 11 6 reaction (g,xn) = (g,n) + 2(g,2n) + 2(g,2n) cross M0922 11 7 section obtained using quasimonoenergetic M0922 11 8 annihilation photons at Livermore (USA) was evaluated M0922 11 9 using specially theoretically calculated transitional M0922 11 10 multiplicity function ratio M0922 11 11 F1-theor = SIG-theor(g,n)/SIG-theor(g,xn) M0922 11 12 by the way M0922 11 13 SIG-eval(g,n) = (F1-theor)x(SIG-exp(g,xn)). M0922 11 14 REL-REF (R,L0007011,R.R.Harvey+,J,PR,136,B126,1964) M0922 11 15 Experimental data for the total neutron yield M0922 11 16 reaction (g,xn) = (g,n) + 2(g,2n) + 3(g,3n) M0922 11 17 cross section. M0922 11 18 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M0922 11 19 Theoretical preequilibrium model of photonuclear M0922 11 20 reactions based on the Fermi gas densities. M0922 11 21 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 11 22 Data plotted in Fig. 7. M0922 11 23 (DEP,L0007011) M0922 11 24 The neutron yield reaction (g,xn) = (g,n) + 2(g,2n) M0922 11 25 + 2(g,2n) cross section. M0922 11 26 (SPSDD,M0912008) M0922 11 27 HISTORY (20190110A) Corrected by V.Varlamov: STATUS. M0922 11 28 (20240508U) Corrected by V.Varlamov: STATUS. M0922 11 29 ENDBIB 27 0 M0922 11 30 NOCOMMON 0 0 M0922 11 31 DATA 3 109 M0922 11 32 EN DATA DATA-ERR M0922 11 33 MEV MB MB M0922 11 34 8.01 37.96 7.09 M0922 11 35 8.17 36.71 6.91 M0922 11 36 8.32 42.47 7.53 M0922 11 37 8.48 47.50 8.18 M0922 11 38 8.63 70.00 13.29 M0922 11 39 8.79 47.50 8.18 M0922 11 40 8.94 70.00 13.30 M0922 11 41 9.10 73.50 13.78 M0922 11 42 9.25 59.50 12.06 M0922 11 43 9.41 80.00 14.54 M0922 11 44 9.56 74.50 14.36 M0922 11 45 9.72 92.50 17.03 M0922 11 46 9.87 92.00 16.98 M0922 11 47 10.03 112.50 18.41 M0922 11 48 10.18 112.00 19.38 M0922 11 49 10.34 112.00 18.35 M0922 11 50 10.49 135.00 21.12 M0922 11 51 10.65 145.00 22.21 M0922 11 52 10.80 162.50 24.41 M0922 11 53 10.96 181.00 26.45 M0922 11 54 11.11 199.50 28.85 M0922 11 55 11.27 226.00 30.75 M0922 11 56 11.42 237.00 33.36 M0922 11 57 11.57 274.00 37.41 M0922 11 58 11.73 275.50 38.00 M0922 11 59 11.89 302.00 46.70 M0922 11 60 12.04 324.00 49.82 M0922 11 61 12.19 332.50 49.29 M0922 11 62 12.35 358.00 52.90 M0922 11 63 12.50 384.00 56.58 M0922 11 64 12.66 426.00 66.84 M0922 11 65 12.81 425.50 66.09 M0922 11 66 12.97 530.00 79.28 M0922 11 67 13.12 478.00 72.33 M0922 11 68 13.28 510.00 76.85 M0922 11 69 13.43 511.50 76.34 M0922 11 70 13.59 544.00 81.66 M0922 11 71 13.74 501.00 76.36 M0922 11 72 13.90 515.00 79.02 M0922 11 73 14.05 515.00 77.30 M0922 11 74 14.21 453.90 65.87 M0922 11 75 14.36 477.50 67.19 M0922 11 76 14.52 443.30 66.01 M0922 11 77 14.67 404.80 63.50 M0922 11 78 14.83 364.60 58.80 M0922 11 79 14.98 352.00 54.14 M0922 11 80 15.14 301.60 50.23 M0922 11 81 15.29 307.30 50.81 M0922 11 82 15.45 258.90 41.98 M0922 11 83 15.60 234.70 41.14 M0922 11 84 15.76 212.90 40.33 M0922 11 85 15.91 185.80 36.72 M0922 11 86 16.07 166.70 32.85 M0922 11 87 16.22 142.90 31.72 M0922 11 88 16.38 134.20 30.05 M0922 11 89 16.53 127.10 31.44 M0922 11 90 16.68 108.00 28.39 M0922 11 91 16.84 88.29 24.89 M0922 11 92 17.00 85.68 24.72 M0922 11 93 17.15 72.03 21.98 M0922 11 94 17.30 66.80 21.13 M0922 11 95 17.46 74.79 23.89 M0922 11 96 17.61 60.64 20.61 M0922 11 97 17.77 51.96 18.60 M0922 11 98 17.92 43.12 16.46 M0922 11 99 18.08 41.73 16.50 M0922 11 100 18.23 36.16 14.83 M0922 11 101 18.39 33.74 14.54 M0922 11 102 18.54 33.66 14.52 M0922 11 103 18.70 29.50 13.32 M0922 11 104 18.85 26.82 12.59 M0922 11 105 19.01 32.53 15.19 M0922 11 106 19.32 22.40 11.31 M0922 11 107 19.47 25.11 12.61 M0922 11 108 19.63 21.34 11.54 M0922 11 109 19.78 20.98 11.37 M0922 11 110 19.94 18.84 10.26 M0922 11 111 20.09 20.09 11.22 M0922 11 112 20.25 24.97 14.18 M0922 11 113 20.40 22.05 12.98 M0922 11 114 20.56 21.56 11.39 M0922 11 115 20.71 18.88 10.44 M0922 11 116 20.87 20.08 10.85 M0922 11 117 21.02 16.36 9.23 M0922 11 118 21.18 17.77 9.87 M0922 11 119 21.33 19.99 11.12 M0922 11 120 21.48 20.59 11.03 M0922 11 121 21.64 22.22 11.75 M0922 11 122 21.80 18.43 10.01 M0922 11 123 21.95 22.48 12.90 M0922 11 124 22.11 18.51 9.89 M0922 11 125 22.26 17.64 9.80 M0922 11 126 22.41 19.35 10.66 M0922 11 127 22.57 17.16 10.65 M0922 11 128 22.72 14.38 8.54 M0922 11 129 22.88 20.29 11.06 M0922 11 130 23.03 18.43 10.07 M0922 11 131 23.19 10.83 7.24 M0922 11 132 23.34 14.51 10.37 M0922 11 133 23.65 19.66 11.72 M0922 11 134 23.96 9.56 7.70 M0922 11 135 24.27 12.94 9.21 M0922 11 136 24.58 14.58 10.47 M0922 11 137 24.89 12.23 9.48 M0922 11 138 25.20 11.07 9.15 M0922 11 139 25.51 8.15 8.07 M0922 11 140 25.82 11.93 10.27 M0922 11 141 26.13 10.58 11.63 M0922 11 142 26.44 14.76 12.49 M0922 11 143 ENDDATA 111 0 M0922 11 144 ENDSUBENT 143 0 M0922 1199999 SUBENT M0922012 20240508 M132M0922 12 1 BIB 5 27 M0922 12 2 REACTION ((83-BI-209(G,2N)83-BI-207,,SIG,,,EVAL)+ M0922 12 3 (83-BI-209(G,2N+P)82-PB-206,,SIG,,,EVAL)) M0922 12 4 ANALYSIS The contribution of partial reaction (g,n) cross M0922 12 5 section into the experimental total neutron yield M0922 12 6 reaction (g,xn) = (g,n) + 2(g,2n) + 3(g,3n) M0922 12 7 cross section obtained using M0922 12 8 quasimonoenergetic annihilation photons at Livermore M0922 12 9 (USA)was evaluated using specially theoretically M0922 12 10 calculated transitional multiplicity function - M0922 12 11 ratio M0922 12 12 F2-theor = SIG-theor(g,n)/SIG-theor(g,xn) M0922 12 13 by the way M0922 12 14 SIG-eval(g,n) = (F2-theor)x(SIG-exp(g,xn)). M0922 12 15 REL-REF (R,L0007011,R.R.Harvey+,J,PR,136,B126,1964) M0922 12 16 Experimental data for the total neutron yield M0922 12 17 reaction (g,xn) cross section. M0922 12 18 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M0922 12 19 Theoretical preequilibrium model of photonuclear M0922 12 20 reactions based on the Fermi gas densities. M0922 12 21 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 12 22 Data plotted in Fig. 7. M0922 12 23 (DEP,L0007011) M0922 12 24 The neutron yield reaction (g,xn) = (g,n) + 2(g,2n) M0922 12 25 cross section. M0922 12 26 (SPSDD,M0912009) M0922 12 27 HISTORY (20190110A) Corrected by V.Varlamov: STATUS. M0922 12 28 (20240508U) Corrected by V.Varlamov: STATUS. M0922 12 29 ENDBIB 27 0 M0922 12 30 NOCOMMON 0 0 M0922 12 31 DATA 3 71 M0922 12 32 EN DATA DATA-ERR M0922 12 33 MEV MB MB M0922 12 34 14.05 0.01 0.94 M0922 12 35 14.21 0.05 0.84 M0922 12 36 14.36 0.26 0.89 M0922 12 37 14.52 0.84 0.90 M0922 12 38 14.67 2.36 0.99 M0922 12 39 14.83 6.70 1.33 M0922 12 40 14.98 16.24 2.49 M0922 12 41 15.14 22.71 3.23 M0922 12 42 15.29 30.84 4.01 M0922 12 43 15.45 34.80 4.32 M0922 12 44 15.60 43.17 5.63 M0922 12 45 15.76 51.54 6.86 M0922 12 46 15.91 56.61 7.55 M0922 12 47 16.07 62.17 7.77 M0922 12 48 16.22 64.06 9.09 M0922 12 49 16.38 71.42 9.69 M0922 12 50 16.53 79.45 11.86 M0922 12 51 16.68 78.49 12.22 M0922 12 52 16.84 73.86 12.04 M0922 12 53 17.00 81.66 13.07 M0922 12 54 17.15 77.49 12.64 M0922 12 55 17.30 80.36 13.20 M0922 12 56 17.46 99.86 15.26 M0922 12 57 17.61 89.18 14.51 M0922 12 58 17.77 83.52 13.82 M0922 12 59 17.92 75.19 13.47 M0922 12 60 18.08 78.39 13.90 M0922 12 61 18.23 72.67 13.26 M0922 12 62 18.39 72.14 13.61 M0922 12 63 18.54 76.17 13.70 M0922 12 64 18.70 70.25 13.11 M0922 12 65 18.85 66.84 13.12 M0922 12 66 19.01 84.49 15.40 M0922 12 67 19.32 62.30 12.67 M0922 12 68 19.47 71.70 13.93 M0922 12 69 19.63 62.33 14.13 M0922 12 70 19.78 62.52 13.88 M0922 12 71 19.94 57.08 12.61 M0922 12 72 20.09 61.71 14.16 M0922 12 73 20.25 77.51 18.42 M0922 12 74 20.40 68.97 17.51 M0922 12 75 20.56 67.72 13.20 M0922 12 76 20.71 59.31 12.85 M0922 12 77 20.87 62.96 13.08 M0922 12 78 21.02 51.07 11.70 M0922 12 79 21.18 55.11 12.47 M0922 12 80 21.33 61.50 13.87 M0922 12 81 21.48 62.71 13.28 M0922 12 82 21.64 66.90 13.66 M0922 12 83 21.80 54.79 12.39 M0922 12 84 21.95 66.01 16.89 M0922 12 85 22.11 53.74 12.03 M0922 12 86 22.26 50.68 12.35 M0922 12 87 22.41 55.07 13.51 M0922 12 88 22.57 48.42 15.17 M0922 12 89 22.72 40.31 11.77 M0922 12 90 22.88 56.60 13.65 M0922 12 91 23.03 51.26 12.64 M0922 12 92 23.19 30.05 11.00 M0922 12 93 23.34 40.15 16.68 M0922 12 94 23.65 54.26 16.06 M0922 12 95 23.96 26.49 13.25 M0922 12 96 24.27 36.24 14.45 M0922 12 97 24.58 41.36 14.99 M0922 12 98 24.89 34.99 14.57 M0922 12 99 25.20 31.76 12.33 M0922 12 100 25.51 23.30 12.13 M0922 12 101 25.82 33.42 14.68 M0922 12 102 26.13 28.72 14.56 M0922 12 103 26.44 38.64 15.39 M0922 12 104 28.08 18.01 6.00 M0922 12 105 ENDDATA 73 0 M0922 12 106 ENDSUBENT 105 0 M0922 1299999 SUBENT M0922013 20240508 M132M0922 13 1 BIB 5 25 M0922 13 2 REACTION ((83-BI-209(G,3N)83-BI-206,,SIG,,,EVAL)+ M0922 13 3 (83-BI-209(G,3N+P)82-PB-205,,SIG,,,EVAL)) M0922 13 4 ANALYSIS The contribution of partial reaction (g,n) cross M0922 13 5 section into the experimental total neutron yield M0922 13 6 reaction (g,xn) = (g,n) + 2(g,2n) + 3(g,3n) M0922 13 7 cross section obtained using M0922 13 8 quasimonoenergetic annihilation photons at Livermore M0922 13 9 (USA)was evaluated using specially theoretically M0922 13 10 calculated transitional multiplicity function - M0922 13 11 ratio M0922 13 12 F2-theor = SIG-theor(g,n)/SIG-theor(g,xn) M0922 13 13 by the way M0922 13 14 SIG-eval(g,n) = (F2-theor)x(SIG-exp(g,xn)). M0922 13 15 REL-REF (R,L0007011,R.R.Harvey+,J,PR,136,B126,1964) M0922 13 16 Experimental data for the total neutron yield M0922 13 17 reaction (g,xn) cross section. M0922 13 18 (E,,B.S.Ishkhanov+,J,YF,71,517,2008) M0922 13 19 Theoretical preequilibrium model of photonuclear M0922 13 20 reactions based on the Fermi gas densities. M0922 13 21 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 13 22 Data plotted in Fig. 7. M0922 13 23 (DEP,L0007011) M0922 13 24 The neutron yield reaction (g,xn) = (g,n) + 2(g,2n) M0922 13 25 cross section. M0922 13 26 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 13 27 ENDBIB 25 0 M0922 13 28 NOCOMMON 0 0 M0922 13 29 DATA 3 13 M0922 13 30 EN DATA DATA-ERR M0922 13 31 MEV MB MB M0922 13 32 23.03 0.01 0.01 M0922 13 33 23.19 0.02 0.01 M0922 13 34 23.34 0.06 0.03 M0922 13 35 23.65 0.27 0.08 M0922 13 36 23.96 0.32 0.16 M0922 13 37 24.27 0.86 0.34 M0922 13 38 24.58 1.57 0.57 M0922 13 39 24.89 2.26 0.94 M0922 13 40 25.20 3.14 1.19 M0922 13 41 25.51 3.08 1.60 M0922 13 42 25.82 6.08 2.62 M0922 13 43 26.13 7.16 3.57 M0922 13 44 26.44 12.16 4.76 M0922 13 45 ENDDATA 15 0 M0922 13 46 ENDSUBENT 45 0 M0922 1399999 SUBENT M0922014 20240508 M132M0922 14 1 BIB 4 6 M0922 14 2 REACTION (55-CS-133(G,X)0-NN-1,UNW,INT,,,EVAL) M0922 14 3 ANALYSIS Integration of evaluated cross section. M0922 14 4 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,(4),501,2016) M0922 14 5 Data from the Table 1. M0922 14 6 (DEP,M0922002) Evaluated cross section. M0922 14 7 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 14 8 ENDBIB 6 0 M0922 14 9 NOCOMMON 0 0 M0922 14 10 DATA 3 3 M0922 14 11 EN-MAX DATA DATA-ERR M0922 14 12 MEV MB*MEV MB*MEV M0922 14 13 16.2 1107.8 36.2 M0922 14 14 25.4 1919.0 42.8 M0922 14 15 29.5 2009.5 43.0 M0922 14 16 ENDDATA 5 0 M0922 14 17 ENDSUBENT 16 0 M0922 1499999 SUBENT M0922015 20240508 M132M0922 15 1 BIB 4 7 M0922 15 2 REACTION ((55-CS-133(G,N)55-CS-132,,INT,,,EVAL)+ M0922 15 3 (55-CS-133(G,N+P)54-XE-131,,INT,,,EVAL)) M0922 15 4 ANALYSIS Integration of evaluated cross section. M0922 15 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 15 6 Data from the Table 1. M0922 15 7 (DEP,M0922003) Evaluated cross section. M0922 15 8 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 15 9 ENDBIB 7 0 M0922 15 10 NOCOMMON 0 0 M0922 15 11 DATA 3 3 M0922 15 12 EN-MAX DATA DATA-ERR M0922 15 13 MEV MB*MEV MB*MEV M0922 15 14 16.2 1110.1 36.3 M0922 15 15 25.4 1543.9 39.8 M0922 15 16 29.5 1568.2 39.8 M0922 15 17 ENDDATA 5 0 M0922 15 18 ENDSUBENT 17 0 M0922 1599999 SUBENT M0922016 20240508 M132M0922 16 1 BIB 4 7 M0922 16 2 REACTION ((55-CS-133(G,2N)55-CS-131,,INT,,,EVAL)+ M0922 16 3 (55-CS-133(G,2N+P)54-XE-130,,INT,,,EVAL)) M0922 16 4 ANALYSIS Integration of evaluated cross section. M0922 16 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 16 6 Data from the Table 1. M0922 16 7 (DEP,M0922004) Evaluated cross section. M0922 16 8 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 16 9 ENDBIB 7 0 M0922 16 10 NOCOMMON 0 0 M0922 16 11 DATA 3 2 M0922 16 12 EN-MAX DATA DATA-ERR M0922 16 13 MEV MB*MEV MB*MEV M0922 16 14 25.4 375.1 9.5 M0922 16 15 29.5 429.2 9.8 M0922 16 16 ENDDATA 4 0 M0922 16 17 ENDSUBENT 16 0 M0922 1699999 SUBENT M0922017 20240508 M132M0922 17 1 BIB 4 7 M0922 17 2 REACTION ((55-CS-133(G,3N)55-CS-130,,INT,,,EVAL)+ M0922 17 3 (55-CS-133(G,3N+P)54-XE-129,,INT,,,EVAL)) M0922 17 4 ANALYSIS Integration of evaluated cross section. M0922 17 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 17 6 Data from the Table 1. M0922 17 7 (DEP,M0922004) Evaluated cross section. M0922 17 8 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 17 9 ENDBIB 7 0 M0922 17 10 NOCOMMON 0 0 M0922 17 11 DATA 3 1 M0922 17 12 EN-MAX DATA DATA-ERR M0922 17 13 MEV MB*MEV MB*MEV M0922 17 14 29.5 11.9 0.7 M0922 17 15 ENDDATA 3 0 M0922 17 16 ENDSUBENT 15 0 M0922 1799999 SUBENT M0922018 20240508 M132M0922 18 1 BIB 4 6 M0922 18 2 REACTION (56-BA-138(G,X)0-NN-1,UNW,INT,,,EVAL) M0922 18 3 ANALYSIS Integration of evaluated cross section. M0922 18 4 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 18 5 Data from the Table 2. M0922 18 6 (DEP,M0922006) Evaluated cross section. M0922 18 7 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 18 8 ENDBIB 6 0 M0922 18 9 NOCOMMON 0 0 M0922 18 10 DATA 3 3 M0922 18 11 EN-MAX DATA DATA-ERR M0922 18 12 MEV MB*MEV MB*MEV M0922 18 13 15.5 957.4 28.9 M0922 18 14 24.6 1940.1 43.5 M0922 18 15 27.1 2036.1 44.1 M0922 18 16 ENDDATA 5 0 M0922 18 17 ENDSUBENT 16 0 M0922 1899999 SUBENT M0922019 20240508 M132M0922 19 1 BIB 4 7 M0922 19 2 REACTION ((56-BA-138(G,N)56-BA-137,,INT,,,EVAL)+ M0922 19 3 (56-BA-138(G,N+P)55-CS-136,,INT,,,EVAL)) M0922 19 4 ANALYSIS Integration of evaluated cross section. M0922 19 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 19 6 Data from the Table 2. M0922 19 7 (DEP,M0922007) Evaluated cross section. M0922 19 8 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 19 9 ENDBIB 7 0 M0922 19 10 NOCOMMON 0 0 M0922 19 11 DATA 3 3 M0922 19 12 EN-MAX DATA DATA-ERR M0922 19 13 MEV MB*MEV MB*MEV M0922 19 14 15.5 956.3 28.9 M0922 19 15 24.6 1442.7 33.7 M0922 19 16 27.1 1459.8 33.7 M0922 19 17 ENDDATA 5 0 M0922 19 18 ENDSUBENT 17 0 M0922 1999999 SUBENT M0922020 20240508 M132M0922 20 1 BIB 4 7 M0922 20 2 REACTION ((56-BA-138(G,2N)56-BA-136,,INT,,,EVAL)+ M0922 20 3 (56-BA-138(G,2N+P)55-CS-135,,INT,,,EVAL)) M0922 20 4 ANALYSIS Integration of evaluated cross section. M0922 20 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 20 6 Data from the Table 2. M0922 20 7 (DEP,M0922008) Evaluated cross section. M0922 20 8 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 20 9 ENDBIB 7 0 M0922 20 10 NOCOMMON 0 0 M0922 20 11 DATA 3 2 M0922 20 12 EN-MAX DATA DATA-ERR M0922 20 13 MEV MB*MEV MB*MEV M0922 20 14 24.6 492.1 10.9 M0922 20 15 27.1 564.0 11.4 M0922 20 16 ENDDATA 4 0 M0922 20 17 ENDSUBENT 16 0 M0922 2099999 SUBENT M0922021 20240508 M132M0922 21 1 BIB 4 7 M0922 21 2 REACTION ((56-BA-138(G,3N)56-BA-135,,INT,,,EVAL)+ M0922 21 3 (56-BA-138(G,3N+P)55-CS-134,,INT,,,EVAL)) M0922 21 4 ANALYSIS Integration of evaluated cross section. M0922 21 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 21 6 Data from the Table 2. M0922 21 7 (DEP,M0922009) Evaluated cross section. M0922 21 8 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 21 9 ENDBIB 7 0 M0922 21 10 NOCOMMON 0 0 M0922 21 11 DATA 3 1 M0922 21 12 EN-MAX DATA DATA-ERR M0922 21 13 MEV MB*MEV MB*MEV M0922 21 14 27.1 4.0 0.3 M0922 21 15 ENDDATA 3 0 M0922 21 16 ENDSUBENT 15 0 M0922 2199999 SUBENT M0922022 20240508 M132M0922 22 1 BIB 5 9 M0922 22 2 CRITIQUE Integrated cross section calculated up to EN-MAX = M0922 22 3 14.4 MeV is 2816.4 mb*MeV, not 1816.4 mb*MeV as in M0922 22 4 article. M0922 22 5 REACTION (83-BI-209(G,X)0-NN-1,UNW,INT,,,EVAL) M0922 22 6 ANALYSIS Integration of evaluated cross section. M0922 22 7 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 22 8 Data from the Table 3. M0922 22 9 (DEP,M0922010) Evaluated cross section. M0922 22 10 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 22 11 ENDBIB 9 0 M0922 22 12 NOCOMMON 0 0 M0922 22 13 DATA 3 3 M0922 22 14 EN-MAX DATA DATA-ERR M0922 22 15 MEV MB*MEV MB*MEV M0922 22 16 14.4 2816.4 53.9 M0922 22 17 22.4 2841.7 58.2 M0922 22 18 26.4 3110.0 58.2 M0922 22 19 ENDDATA 5 0 M0922 22 20 ENDSUBENT 19 0 M0922 2299999 SUBENT M0922023 20240508 M132M0922 23 1 BIB 4 7 M0922 23 2 REACTION ((83-BI-209(G,N)83-BI-208,,INT,,,EVAL)+ M0922 23 3 (83-BI-209(G,N+P)82-PB-207,,INT,,,EVAL)) M0922 23 4 ANALYSIS Integration of evaluated cross section. M0922 23 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 23 6 Data from the Table 3. M0922 23 7 (DEP,M0922011) Evaluated cross section. M0922 23 8 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 23 9 ENDBIB 7 0 M0922 23 10 NOCOMMON 0 0 M0922 23 11 DATA 3 3 M0922 23 12 EN-MAX DATA DATA-ERR M0922 23 13 MEV MB*MEV MB*MEV M0922 23 14 14.4 1815.5 61.9 M0922 23 15 22.4 2421.6 33.7 M0922 23 16 26.4 2482.9 66.8 M0922 23 17 ENDDATA 5 0 M0922 23 18 ENDSUBENT 17 0 M0922 2399999 SUBENT M0922024 20240508 M132M0922 24 1 BIB 4 7 M0922 24 2 REACTION ((83-BI-209(G,2N)83-BI-207,,INT,,,EVAL)+ M0922 24 3 (83-BI-209(G,2N+P)82-PB-206,,INT,,,EVAL)) M0922 24 4 ANALYSIS Integration of evaluated cross section. M0922 24 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 24 6 Data from the Table 3. M0922 24 7 (DEP,M0922012) Evaluated cross section. M0922 24 8 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 24 9 ENDBIB 7 0 M0922 24 10 NOCOMMON 0 0 M0922 24 11 DATA 3 2 M0922 24 12 EN-MAX DATA DATA-ERR M0922 24 13 MEV MB*MEV MB*MEV M0922 24 14 22.4 418.8 12.1 M0922 24 15 26.4 611.0 13.9 M0922 24 16 ENDDATA 4 0 M0922 24 17 ENDSUBENT 16 0 M0922 2499999 SUBENT M0922025 20240508 M132M0922 25 1 BIB 4 75 M0922 25 2 REACTION ((83-BI-209(G,3N)83-BI-206,,INT,,,EVAL)+ M0922 25 3 (83-BI-209(G,3N+P)82-PB-205,,INT,,,EVAL)) M0922 25 4 ANALYSIS Integration of evaluated cross section. M0922 25 5 STATUS (TABLE,,V.V.Varlamov+,J,PAN,79,501,2016) M0922 25 6 Data from the Table 3. M0922 25 7 (DEP,M0922013) Evaluated cross section. M0922 25 8 HISTORY (20240508U) Corrected by V.Varlamov: STATUS. M0922 25 9 ENDBIB 7 0 M0922 25 10 NOCOMMON 0 0 M0922 25 11 DATA 3 1 M0922 25 12 EN-MAX DATA DATA-ERR M0922 25 13 MEV MB*MEV MB*MEV M0922 25 14 26.4 8.2 0.6 M0922 25 15 ENDDATA 3 0 M0922 25 16 ENDSUBENT 15 0 M0922 2599999 ENDENTRY 25 0 M092299999999