ENTRY M0693 20191017 M103M069300000001 SUBENT M0693001 20191017 M103M069300100001 BIB 8 21 M069300100002 TITLE Evaluation of 127I photoneutron reaction cross M069300100003 sections. M069300100004 AUTHOR (V.V.Varlamov,B.S.Ishkhanov,I.V.Makarenko,V.N.Orlin, M069300100005 N.N.Peskov) M069300100006 REFERENCE (R,MSU-INP-2006-9/808,2006) M069300100007 INSTITUTE (4RUSMOS) M069300100008 INC-SOURCE (BRST) M069300100009 (QMPH,ARAD) M069300100010 COMMENT Joint combined evaluation of total (g,xn) and (g,sn) M069300100011 and partial (g,n), (g,2n) and (g,3n) photoneutron M069300100012 reactions cross sections for 127I was carried out M069300100013 based on the results of investigation of those in M069300100014 experiments used the bremsstrahlung and M069300100015 quasimonoenergetic annihilation photon beams. The M069300100016 reasons of data disagreements were analyzed, the M069300100017 values of normalization factors for putting all data M069300100018 in consistency to each other were obtained. M069300100019 STATUS (TABLE,APRVD) By V.V.Varlamov. M069300100020 HISTORY (20060712C) Data were compiled at Russia MSU SINP M069300100021 CDFE by V.Varlamov. M069300100022 (20191017C) Corrected by V.Varlamov: STATUS. M069300100023 ENDBIB 21 0 M069300100024 NOCOMMON 0 0 M069300100025 ENDSUBENT 24 0 M069300199999 SUBENT M0693002 20191017 M103M069300200001 BIB 6 35 M069300200002 REACTION (53-I-127(G,X)0-NN-1,,SIG,,,EVAL) M069300200003 ANALYSIS The method analogue to that used for combined M069300200004 analysis of photoneutron reaction cross sections M069300200005 obtained using beams of quasimonoenergerical photons M069300200006 at Saclay (France) and Livermore (USA) was used. M069300200007 Normalization coefficient were obtained 1.2 for M069300200008 Livermore data and 0.9 for Saclay data. M069300200009 REL-REF (E,M0635001,V.V.Varlamov,J,YK,1-2,48,2003). The M069300200010 method of data analysis. M069300200011 (E,M0511002,R.P.Rassool+,J,PR/C,39,1631,1989). M069300200012 Photoneutron reaction (g,sn) cross section obtained M069300200013 using bremsstrahlung. M069300200014 (E,M0511003,R.P.Rassool+,J,PR/C,39,1631,1989). M069300200015 Photoneutron reaction (g,2n) cross section obtained M069300200016 using bremsstrahlung. M069300200017 (E,L0009002,R.L.Bramblett+,J,PR,148,1198,1966). Total M069300200018 photoneutron reaction (g,xn) cross section obtained M069300200019 using quasimonoenergetic annihilation photons at M069300200020 Livermore. M069300200021 (E,L0015027,R.Bergere+,J,NP/A,133,417,1969). Total M069300200022 photoneutron reaction (g,xn) cross section obtained M069300200023 using quasimonoenergetic annihilation photons at M069300200024 Saclay. M069300200025 ERR-ANALYS (DATA-ERR) Root-mean-square errors. M069300200026 STATUS (DEP,L0009002) Livermore data multiplied by 1.2. M069300200027 (SPSDD,M0984002) M069300200028 The neutron yield reaction cross section obtained as M069300200029 sum: SIG(g,xn) = SIG(g,1n)+2SIG(g,2n))+3SIG(g,3n). M069300200030 Because experimental data for the total neutron yield M069300200031 reaction (g,xn) cross section for 127I were obtained M069300200032 only up to energy 24.89 MeV in evaluation procedure M069300200033 the sum (g,1n)+2(g,2n)+3(g,3n) of experimental cross M069300200034 sections was obtained up to energy 31.2 MeV. M069300200035 HISTORY (20191017C) Corrected by V.Varlamov: STATUS, M069300200036 REACTION in SUBENT 004. M069300200037 ENDBIB 35 0 M069300200038 NOCOMMON 0 0 M069300200039 DATA 3 86 M069300200040 EN DATA DATA-ERR M069300200041 MEV MB MB M069300200042 8.78 -0.07 0.33 M069300200043 9.09 1.36 0.39 M069300200044 9.17 7.06 2.13 M069300200045 9.25 9.12 0.88 M069300200046 9.33 8.13 4.51 M069300200047 9.40 17.69 1.22 M069300200048 9.48 20.56 1.61 M069300200049 9.56 22.36 1.86 M069300200050 9.63 25.67 1.89 M069300200051 9.71 26.88 3.09 M069300200052 9.79 25.46 1.54 M069300200053 9.87 28.56 2.08 M069300200054 9.94 30.22 2.17 M069300200055 10.03 28.03 2.04 M069300200056 10.1 29.00 2.15 M069300200057 10.18 32.11 2.30 M069300200058 10.34 33.13 2.42 M069300200059 10.65 43.52 3.00 M069300200060 10.96 48.22 3.28 M069300200061 11.27 57.37 3.73 M069300200062 11.57 67.69 3.72 M069300200063 11.89 79.27 4.23 M069300200064 12.19 87.44 4.61 M069300200065 12.5 111.10 5.63 M069300200066 12.81 137.60 6.69 M069300200067 13.12 157.30 7.53 M069300200068 13.43 182.10 8.48 M069300200069 13.74 218.10 9.94 M069300200070 14.05 239.20 11.08 M069300200071 14.36 258.10 12.62 M069300200072 14.67 254.70 12.73 M069300200073 14.98 267.10 13.11 M069300200074 15.29 256.00 13.59 M069300200075 15.6 258.20 13.87 M069300200076 15.91 247.60 14.01 M069300200077 16.22 232.50 10.72 M069300200078 16.38 231.2 13.4 M069300200079 16.53 244.30 14.06 M069300200080 16.61 235.90 13.95 M069300200081 16.68 234.60 11.61 M069300200082 16.76 225.30 13.83 M069300200083 16.84 245.30 14.65 M069300200084 16.92 243.40 14.79 M069300200085 17. 237.20 14.58 M069300200086 17.07 236.70 14.72 M069300200087 17.15 243.60 12.55 M069300200088 17.46 240.70 15.57 M069300200089 17.77 224.90 15.49 M069300200090 18.08 239.90 16.41 M069300200091 18.39 214.10 16.12 M069300200092 18.7 203.90 15.89 M069300200093 19.01 183.30 12.38 M069300200094 19.32 177.60 15.18 M069300200095 19.63 172.90 16.14 M069300200096 19.94 159.60 16.04 M069300200097 20.25 146.60 15.86 M069300200098 20.56 131.50 11.26 M069300200099 20.87 131.50 14.34 M069300200100 21.18 114.80 14.02 M069300200101 21.48 124.20 14.72 M069300200102 21.8 111.10 14.55 M069300200103 22.11 144.60 16.06 M069300200104 22.41 115.20 15.44 M069300200105 22.72 115.60 15.47 M069300200106 23.03 92.39 15.04 M069300200107 23.34 93.48 15.31 M069300200108 23.65 106.00 16.18 M069300200109 23.96 104.60 16.27 M069300200110 24.27 70.57 18.65 M069300200111 24.58 60.20 18.45 M069300200112 24.89 79.28 18.87 M069300200113 25.2 66.82 20.49 M069300200114 25.51 66.4 19.26 M069300200115 25.82 60.47 19.57 M069300200116 26.13 61.69 17.11 M069300200117 26.44 53.52 22.47 M069300200118 26.75 58.37 22.48 M069300200119 27.06 73.82 22.94 M069300200120 27.37 63.58 18.11 M069300200121 27.68 72.24 22.79 M069300200122 27.99 43.6 18.05 M069300200123 28.3 76.96 25.40 M069300200124 28.61 35.32 21.21 M069300200125 28.92 54.56 28.68 M069300200126 29.23 29.90 29.18 M069300200127 29.54 20.96 26.16 M069300200128 ENDDATA 88 0 M069300200129 ENDSUBENT 128 0 M069300299999 SUBENT M0693003 20191017 M103M069300300001 BIB 6 18 M069300300002 REACTION (53-I-127(G,X)0-NN-1,UNW,SIG,,,EVAL) M069300300003 ANALYSIS The procedure analogue to that used for combined M069300300004 analysis of photoneutron reaction cross sections M069300300005 obtained using beams of quasimonoenergerical photons M069300300006 at Saclay (France) and Livermore (USA) was used. M069300300007 REL-REF (E,M0635001,V.V.Varlamov,J,YK,1-2,48,2003). The M069300300008 method of data analysis. M069300300009 (E,L0009009,R.L.Bramblett+,J,PR,148,1198,1966). Total M069300300010 photoneutron reaction (g,sn) cross section obtained M069300300011 using quasimonoenergetic annihilation photons at M069300300012 Livermore. M069300300013 ERR-ANALYS (DATA-ERR) Root-mean-square errors. M069300300014 STATUS (DEP,L0009009) Livermore data multiplied by 1.2. M069300300015 (SPSDD,M0984003) M069300300016 Data obtained using the new method of evaluation M069300300017 basing on the objective physical criteria of data M069300300018 reliability. M069300300019 HISTORY (20191017C) Corrected by V.Varlamov: STATUS. M069300300020 ENDBIB 18 0 M069300300021 NOCOMMON 0 0 M069300300022 DATA 3 86 M069300300023 EN DATA DATA-ERR M069300300024 MEV MB MB M069300300025 8.78 -0.07 0.33 M069300300026 9.09 1.36 0.39 M069300300027 9.17 7.06 2.13 M069300300028 9.25 9.12 0.88 M069300300029 9.33 8.13 4.51 M069300300030 9.40 17.69 1.22 M069300300031 9.48 20.56 1.61 M069300300032 9.56 22.36 1.86 M069300300033 9.63 25.67 1.89 M069300300034 9.71 26.88 3.09 M069300300035 9.79 25.46 1.54 M069300300036 9.87 28.56 2.08 M069300300037 9.94 30.22 2.17 M069300300038 10.03 28.03 2.04 M069300300039 10.1 29.00 2.15 M069300300040 10.18 32.11 2.30 M069300300041 10.34 33.13 2.42 M069300300042 10.65 43.52 3.00 M069300300043 10.96 48.22 3.28 M069300300044 11.27 57.37 3.73 M069300300045 11.57 67.69 3.72 M069300300046 11.89 79.27 4.23 M069300300047 12.19 87.44 4.61 M069300300048 12.5 111.10 5.63 M069300300049 12.81 137.60 6.69 M069300300050 13.12 157.30 7.53 M069300300051 13.43 182.10 8.48 M069300300052 13.74 218.10 9.94 M069300300053 14.05 235.9 10.5 M069300300054 14.36 258.4 12.0 M069300300055 14.67 249.20 11.86 M069300300056 14.98 265.80 12.27 M069300300057 15.29 255.00 12.64 M069300300058 15.6 264.10 13.15 M069300300059 15.91 254.30 13.17 M069300300060 16.22 231.80 10.22 M069300300061 16.38 229.60 13.12 M069300300062 16.53 241.60 13.71 M069300300063 16.61 227.50 13.31 M069300300064 16.68 222.90 10.97 M069300300065 16.76 207.40 12.74 M069300300066 16.84 222.80 13.36 M069300300067 16.92 215.00 13.19 M069300300068 17. 210.20 13.07 M069300300069 17.07 205.60 13.01 M069300300070 17.15 200.90 10.63 M069300300071 17.46 185.1 12.7 M069300300072 17.77 157.30 12.06 M069300300073 18.08 168.2 12.8 M069300300074 18.39 133.8 12.0 M069300300075 18.7 126.60 11.96 M069300300076 19.01 104.80 8.93 M069300300077 19.32 97.14 11.13 M069300300078 19.63 102.60 12.26 M069300300079 19.94 86.35 11.97 M069300300080 20.25 80.56 11.99 M069300300081 20.56 68.39 8.43 M069300300082 20.87 56.40 10.33 M069300300083 21.18 52.52 10.48 M069300300084 21.48 65.78 11.23 M069300300085 21.8 59.83 11.30 M069300300086 22.11 98.11 12.86 M069300300087 22.41 66.05 12.07 M069300300088 22.72 71.86 12.28 M069300300089 23.03 52.19 11.95 M069300300090 23.34 45.31 11.90 M069300300091 23.65 71.44 13.11 M069300300092 23.96 69.00 13.15 M069300300093 24.27 42.34 12.83 M069300300094 24.58 42.44 12.93 M069300300095 24.89 45.32 13.27 M069300300096 25.2 54.55 14.00 M069300300097 25.51 45.17 13.56 M069300300098 25.82 36.52 13.70 M069300300099 26.13 18.08 12.68 M069300300100 26.44 32.81 16.68 M069300300101 26.75 55.39 17.88 M069300300102 27.06 55.33 18.18 M069300300103 27.37 31.76 14.34 M069300300104 27.68 46.88 17.89 M069300300105 27.99 27.77 14.61 M069300300106 28.3 59.35 20.18 M069300300107 28.61 30.40 17.94 M069300300108 28.92 35.90 23.36 M069300300109 29.23 41.99 22.64 M069300300110 29.54 29.18 21.53 M069300300111 ENDDATA 88 0 M069300300112 ENDSUBENT 111 0 M069300399999 SUBENT M0693004 20191017 M103M069300400001 BIB 6 19 M069300400002 REACTION ((53-I-127(G,N)53-I-126,,SIG,,,EVAL)+ M069300400003 (53-I-127(G,N+P)52-TE-125,,SIG,,,EVAL)) M069300400004 ANALYSIS The procedure analogue to that used for combined M069300400005 analysis of photoneutron reaction cross sections M069300400006 obtained using beams of quasimonoenergerical photons M069300400007 at Saclay (France) and Livermore (USA) was used. M069300400008 REL-REF (E,M0635001,V.V.Varlamov,J,YK,1-2,48,2003). The M069300400009 method of data analysis. M069300400010 (E,L0009003,R.L.Bramblett+,J,PR,148,1198,1966). M069300400011 Partial photoneutron reaction (g,n) cross section M069300400012 obtained using quasimonoenergetic annihilation M069300400013 photons at Livermore. M069300400014 ERR-ANALYS (DATA-ERR) Root-mean-square errors. M069300400015 STATUS (DEP,L0009003) Livermore data multiplied by 1.2. M069300400016 (SPSDD,M0984004) M069300400017 Data obtained using the new method of evaluation M069300400018 basing on the objective physical criteria of data M069300400019 reliability. M069300400020 HISTORY (20191017C) Corrected by V.Varlamov: REACTION, STATUS. M069300400021 ENDBIB 19 0 M069300400022 NOCOMMON 0 0 M069300400023 DATA 3 83 M069300400024 EN DATA DATA-ERR M069300400025 MEV MB MB M069300400026 8.78 -0.07 0.33 M069300400027 9.09 1.36 0.39 M069300400028 9.17 7.06 2.22 M069300400029 9.25 9.12 0.88 M069300400030 9.33 8.13 4.34 M069300400031 9.40 17.69 1.23 M069300400032 9.48 20.56 1.61 M069300400033 9.56 22.36 1.86 M069300400034 9.63 25.67 1.89 M069300400035 9.71 26.88 3.00 M069300400036 9.79 25.46 1.54 M069300400037 9.87 28.60 2.08 M069300400038 9.94 30.25 2.17 M069300400039 10.03 28.06 2.04 M069300400040 10.1 29.00 2.15 M069300400041 10.18 32.09 2.30 M069300400042 10.34 33.06 2.42 M069300400043 10.65 43.45 3.00 M069300400044 10.96 48.29 3.28 M069300400045 11.27 57.62 3.74 M069300400046 11.57 68.02 3.72 M069300400047 11.89 79.49 4.24 M069300400048 12.19 87.38 4.60 M069300400049 12.5 110.70 5.62 M069300400050 12.81 136.90 6.67 M069300400051 13.12 156.60 7.52 M069300400052 13.43 181.50 8.48 M069300400053 13.74 218.00 9.93 M069300400054 14.05 233.10 11.59 M069300400055 14.36 259.90 13.65 M069300400056 14.67 245.30 13.48 M069300400057 14.98 266.10 14.24 M069300400058 15.29 255.40 14.89 M069300400059 15.6 270.7 15.6 M069300400060 15.91 260.80 15.94 M069300400061 16.22 229.60 11.38 M069300400062 16.38 225.90 13.65 M069300400063 16.53 236.30 14.31 M069300400064 16.61 216.30 13.95 M069300400065 16.68 208.1 11.3 M069300400066 16.76 186.20 13.35 M069300400067 16.84 196.90 13.96 M069300400068 16.92 182.90 13.84 M069300400069 17. 179.50 13.65 M069300400070 17.07 170.80 13.63 M069300400071 17.15 154.40 10.72 M069300400072 17.46 126.00 13.28 M069300400073 17.77 86.45 12.58 M069300400074 18.08 94.33 13.45 M069300400075 18.39 52.85 12.73 M069300400076 18.7 50.68 12.71 M069300400077 19.01 29.81 9.01 M069300400078 19.32 22.16 11.99 M069300400079 19.63 39.55 13.80 M069300400080 19.94 21.52 13.57 M069300400081 20.25 23.45 13.98 M069300400082 20.56 13.97 9.30 M069300400083 20.87 -10.99 12.06 M069300400084 21.18 -3.63 12.33 M069300400085 21.48 11.35 13.18 M069300400086 21.8 10.26 13.30 M069300400087 22.11 50.90 15.16 M069300400088 22.41 14.10 14.44 M069300400089 22.72 23.54 14.81 M069300400090 23.03 6.25 14.59 M069300400091 23.34 -9.10 14.44 M069300400092 23.65 30.85 16.16 M069300400093 23.96 28.22 16.07 M069300400094 24.27 7.29 17.17 M069300400095 24.58 16.27 17.40 M069300400096 24.89 15.11 17.75 M069300400097 25.2 39.48 19.72 M069300400098 25.51 25.88 18.46 M069300400099 25.82 19.52 18.98 M069300400100 26.13 -16.01 16.40 M069300400101 26.44 13.39 22.23 M069300400102 26.75 51.38 23.22 M069300400103 27.06 32.96 22.74 M069300400104 27.37 -7.35 17.78 M069300400105 27.68 12.00 23.96 M069300400106 27.99 1.75 21.31 M069300400107 28.3 41.78 26.63 M069300400108 28.61 43.84 23.93 M069300400109 ENDDATA 85 0 M069300400110 ENDSUBENT 109 0 M069300499999 SUBENT M0693005 20191017 M103M069300500001 BIB 6 18 M069300500002 REACTION (53-I-127(G,2N)53-I-125,,SIG,,,EVAL) M069300500003 ANALYSIS The procedure analogue to that used for combined M069300500004 analysis of photoneutron reaction cross sections M069300500005 obtained using beams of quasimonoenergerical photons M069300500006 at Saclay (France) and Livermore (USA) was used. M069300500007 REL-REF (E,M0635001,V.V.Varlamov,J,YK,1-2,48,2003). The M069300500008 method of data analysis. M069300500009 (E,L0009004,R.L.Bramblett+,J,PR,148,1198,1966). M069300500010 Partial photoneutron reaction (g,2n) cross section M069300500011 obtained using quasimonoenergetic annihilation M069300500012 photons at Livermore. M069300500013 ERR-ANALYS (DATA-ERR) Root-mean-square errors. M069300500014 STATUS (DEP,L0009004) Livermore data multiplied by 1.2. M069300500015 (SPSDD,M0984005) M069300500016 Data obtained using the new method of evaluation M069300500017 basing on the objective physical criteria of data M069300500018 reliability. M069300500019 HISTORY (20191017C) Corrected by V.Varlamov: STATUS. M069300500020 ENDBIB 18 0 M069300500021 NOCOMMON 0 0 M069300500022 DATA 3 56 M069300500023 EN DATA DATA-ERR M069300500024 MEV MB MB M069300500025 14.05 3.31 2.25 M069300500026 14.36 -0.37 2.69 M069300500027 14.67 5.47 3.10 M069300500028 14.98 1.35 3.15 M069300500029 15.29 1.03 3.55 M069300500030 15.60 -5.83 3.33 M069300500031 15.91 -6.72 3.68 M069300500032 16.22 0.72 2.14 M069300500033 16.38 1.59 1.91 M069300500034 16.53 2.66 2.16 M069300500035 16.61 8.41 2.80 M069300500036 16.68 11.68 2.27 M069300500037 16.76 17.90 3.61 M069300500038 16.84 22.48 4.01 M069300500039 16.92 28.44 4.52 M069300500040 17.00 27.01 4.38 M069300500041 17.07 31.01 4.72 M069300500042 17.15 42.71 4.27 M069300500043 17.46 55.54 6.48 M069300500044 17.77 67.66 7.28 M069300500045 18.08 71.74 7.68 M069300500046 18.39 80.34 8.40 M069300500047 18.70 77.30 8.17 M069300500048 19.01 78.47 6.53 M069300500049 19.32 80.50 8.31 M069300500050 19.63 70.27 8.52 M069300500051 19.94 73.25 8.81 M069300500052 20.25 66.04 8.65 M069300500053 20.56 63.10 5.84 M069300500054 20.87 75.08 8.40 M069300500055 21.18 62.23 7.90 M069300500056 21.48 58.44 8.01 M069300500057 21.80 51.24 7.79 M069300500058 22.11 46.52 7.97 M069300500059 22.41 49.13 8.26 M069300500060 22.72 43.75 8.03 M069300500061 23.03 40.20 8.00 M069300500062 23.34 48.17 8.44 M069300500063 23.65 34.52 8.27 M069300500064 23.96 35.62 8.37 M069300500065 24.27 28.24 12.81 M069300500066 24.58 17.76 12.54 M069300500067 24.89 33.96 12.60 M069300500068 25.20 12.26 14.25 M069300500069 25.51 21.23 13.00 M069300500070 25.82 23.95 13.35 M069300500071 26.13 43.61 10.73 M069300500072 26.44 20.71 14.47 M069300500073 26.75 2.97 13.09 M069300500074 27.06 18.49 13.22 M069300500075 27.37 31.81 10.25 M069300500076 27.68 25.36 13.32 M069300500077 27.99 15.83 10.07 M069300500078 28.30 17.60 14.64 M069300500079 28.61 4.92 10.97 M069300500080 28.92 18.66 16.01 M069300500081 ENDDATA 58 0 M069300500082 ENDSUBENT 81 0 M069300599999 SUBENT M0693006 20191017 M103M069300600001 BIB 6 18 M069300600002 REACTION (53-I-127(G,3N)53-I-124,,SIG,,,EVAL) M069300600003 ANALYSIS The procedure analogue to that used for combined M069300600004 analysis of photoneutron reaction cross sections M069300600005 obtained using beams of quasimonoenergerical photons M069300600006 at Saclay (France) and Livermore (USA) was used. M069300600007 REL-REF (E,M0635001,V.V.Varlamov,J,YK,1-2,48,2003). The M069300600008 method of data analysis. M069300600009 (E,L0015005,R.Bergere+,J,NP/A,133,417,1969). M069300600010 Partial photoneutron reaction (g,3n) cross section M069300600011 obtained using quasimonoenergetic annihilation M069300600012 photons at Saclay. M069300600013 ERR-ANALYS (DATA-ERR) Root-mean-square errors. M069300600014 STATUS (DEP,L0015005) Saclay data multiplied by 0.9. M069300600015 (SPSDD,M0984006) M069300600016 Data obtained using the new method of evaluation M069300600017 basing on the objective physical criteria of data M069300600018 reliability. M069300600019 HISTORY (20191017C) Corrected by V.Varlamov: STATUS. M069300600020 ENDBIB 18 0 M069300600021 NOCOMMON 0 0 M069300600022 DATA 3 14 M069300600023 EN DATA DATA-ERR M069300600024 MEV MB MB M069300600025 25.76 0.27 4.50 M069300600026 26.03 3.15 4.57 M069300600027 26.3 -1.62 4.46 M069300600028 26.57 -1.17 4.47 M069300600029 26.84 -0.09 4.49 M069300600030 27.12 2.07 4.54 M069300600031 27.66 1.71 4.53 M069300600032 28.2 2.25 4.55 M069300600033 28.48 5.67 4.62 M069300600034 29.02 6.75 4.65 M069300600035 29.56 9.45 4.71 M069300600036 30.11 8.91 4.69 M069300600037 30.65 10.98 4.74 M069300600038 31.2 10.89 4.74 M069300600039 ENDDATA 16 0 M069300600040 ENDSUBENT 39 0 M069300699999 SUBENT M0693007 20061114 M041M069300700001 BIB 5 25 M069300700002 REACTION (53-I-127(G,X)0-NN-1,,INT,,,EVAL) M069300700003 ANALYSIS The procedure analogue to that used for combined M069300700004 analysis of photoneutron reaction cross sections M069300700005 obtained using beams of quasimonoenergerical photons M069300700006 at Saclay (France) and Livermore (USA) was used. M069300700007 Normalization coefficient were obtained 1.2 for M069300700008 Livermore data and 0.9 for Saclay data. M069300700009 REL-REF (E,M0635001,V.V.VARLAMOV,J,YK,1-2,48,2003). The M069300700010 method of data analysis. M069300700011 (E,M0511002,R.P.RASSOOL+,J,PR/C,39,1631,1989). M069300700012 Photoneutron reaction (g,sn) cross section obtained M069300700013 using bremsstrahlung. M069300700014 (E,M0511003,R.P.RASSOOL+,J,PR/C,39,1631,1989). M069300700015 Photoneutron reaction (g,2n) cross section obtained M069300700016 using bremsstrahlung. M069300700017 (E,L0009002,R.L.BRAMBLETT+,J,PR,148,1198,1966). Total M069300700018 photoneutron reaction (g,xn) cross section obtained M069300700019 using quasimonoenergetical annihilation photons at M069300700020 Livermore. M069300700021 (E,L0015027,R.BERGERE+,J,NP/A,133,417,1969). Total M069300700022 photoneutron reaction (g,xn) cross section obtained M069300700023 using quasimonoenergetical annihilation photons at M069300700024 Saclay. M069300700025 ERR-ANALYS No data. M069300700026 STATUS (DEP,L0009002) Livermore data multiplied by 1.2. M069300700027 ENDBIB 25 0 M069300700028 NOCOMMON 0 0 M069300700029 DATA 2 1 M069300700030 EN-MAX DATA M069300700031 MEV MB*MEV M069300700032 29.5 2605.8 M069300700033 ENDDATA 3 0 M069300700034 ENDSUBENT 33 0 M069300799999 SUBENT M0693008 20061114 M041M069300800001 BIB 5 13 M069300800002 REACTION (53-I-127(G,X)0-NN-1,UNW,INT,,,EVAL) M069300800003 ANALYSIS The procedure analogue to that used for combined M069300800004 analysis of photoneutron reaction cross sections M069300800005 obtained using beams of quasimonoenergerical photons M069300800006 at Saclay (France) and Livermore (USA) was used. M069300800007 REL-REF (E,M0635001,V.V.VARLAMOV,J,YK,1-2,48,2003). The M069300800008 method of data analysis. M069300800009 (E,L0009009,R.L.BRAMBLETT+,J,PR,148,1198,1966). Total M069300800010 photoneutron reaction (g,sn) cross section obtained M069300800011 using quasimonoenergetical annihilation photons at M069300800012 Livermore. M069300800013 ERR-ANALYS No data. M069300800014 STATUS (DEP,L0009009) Livermore data multiplied by 1.2. M069300800015 ENDBIB 13 0 M069300800016 NOCOMMON 0 0 M069300800017 DATA 2 1 M069300800018 EN-MAX DATA M069300800019 MEV MB*MEV M069300800020 29.5 2075.7 M069300800021 ENDDATA 3 0 M069300800022 ENDSUBENT 21 0 M069300899999 SUBENT M0693009 20061114 M041M069300900001 BIB 5 13 M069300900002 REACTION (53-I-127(G,N)53-I-126,,INT,,,EVAL) M069300900003 ANALYSIS The procedure analogue to that used for combined M069300900004 analysis of photoneutron reaction cross sections M069300900005 obtained using beams of quasimonoenergerical photons M069300900006 at Saclay (France) and Livermore (USA) was used. M069300900007 REL-REF (E,M0635001,V.V.VARLAMOV,J,YK,1-2,48,2003). The M069300900008 method of data analysis. M069300900009 (E,L0009003,R.L.BRAMBLETT+,J,PR,148,1198,1966). M069300900010 Partial photoneutron reaction (g,n) cross section M069300900011 obtained using quasimonoenergetical annihilation M069300900012 photons at Livermore. M069300900013 ERR-ANALYS No data. M069300900014 STATUS (DEP,L0009003) Livermore data multiplied by 1.2. M069300900015 ENDBIB 13 0 M069300900016 NOCOMMON 0 0 M069300900017 DATA 2 1 M069300900018 EN-MAX DATA M069300900019 MEV MB*MEV M069300900020 28.5 1508.4 M069300900021 ENDDATA 3 0 M069300900022 ENDSUBENT 21 0 M069300999999 SUBENT M0693010 20061114 M041M069301000001 BIB 5 13 M069301000002 REACTION (53-I-127(G,2N)53-I-125,,INT,,,EVAL) M069301000003 ANALYSIS The procedure analogue to that used for combined M069301000004 analysis of photoneutron reaction cross sections M069301000005 obtained using beams of quasimonoenergerical photons M069301000006 at Saclay (France) and Livermore (USA) was used. M069301000007 REL-REF (E,M0635001,V.V.VARLAMOV,J,YK,1-2,48,2003). The M069301000008 method of data analysis. M069301000009 (E,L0009004,R.L.BRAMBLETT+,J,PR,148,1198,1966). M069301000010 Partial photoneutron reaction (g,2n) cross section M069301000011 obtained using quasimonoenergetical annihilation M069301000012 photons at Livermore. M069301000013 ERR-ANALYS No data. M069301000014 STATUS (DEP,L0009004) Livermore data multiplied by 1.2. M069301000015 ENDBIB 13 0 M069301000016 NOCOMMON 0 0 M069301000017 DATA 2 1 M069301000018 EN-MAX DATA M069301000019 MEV MB*MEV M069301000020 28.5 527.3 M069301000021 ENDDATA 3 0 M069301000022 ENDSUBENT 21 0 M069301099999 SUBENT M0693011 20061114 M041M069301100001 BIB 5 13 M069301100002 REACTION (53-I-127(G,3N)53-I-124,,INT,,,EVAL) M069301100003 ANALYSIS The procedure analogue to that used for combined M069301100004 analysis of photoneutron reaction cross sections M069301100005 obtained using beams of quasimonoenergerical photons M069301100006 at Saclay (France) and Livermore (USA) was used. M069301100007 REL-REF (E,M0635001,V.V.VARLAMOV,J,YK,1-2,48,2003). The M069301100008 method of data analysis. M069301100009 (E,L0015005,R.BERGERE+,J,NP/A,133,417,1969). M069301100010 Partial photoneutron reaction (g,3n) cross section M069301100011 obtained using quasimonoenergetical annihilation M069301100012 photons at Saclay. M069301100013 ERR-ANALYS No data. M069301100014 STATUS (DEP,L0015005) Saclay data multiplied by 0.9. M069301100015 ENDBIB 13 0 M069301100016 NOCOMMON 0 0 M069301100017 DATA 2 1 M069301100018 EN-MAX DATA M069301100019 MEV MB*MEV M069301100020 31.2 27.7 M069301100021 ENDDATA 3 0 M069301100022 ENDSUBENT 21 0 M069301199999 ENDENTRY 11 0 M069399999999