ENTRY M0831 20141113 M075M083100000001 SUBENT M0831001 20141113 M075M083100100001 BIB 8 39 M083100100002 TITLE Analysis of reliability of experimental data on total M083100100003 and partial photoneutron reaction cross sections. M083100100004 New evaluated data for 159Tb. M083100100005 AUTHOR (V.V.Varlamov,B.S.Ishkhanov,V.N.Orlin,T.S.Polevich, M083100100006 M.E.Stepanov) M083100100007 REFERENCE (R,MSU-INP-2011-5/869,2011) In Russian. M083100100008 (J,YF,75,(11),1414,2012) M083100100009 V.V.Varlamov,B.S.Ishkhanov,V.N.Orlin. New approach M083100100010 to analyzing and evaluating cross sections for M083100100011 partial photoneutron reactions. M083100100012 (J,PAN,75,(11),1339,2012) English translation of M083100100013 YF,75,(11),1414,2012 M083100100014 #doi:10.1134/S1063778812110191 M083100100015 (J,EPJ/A,50,114,2014) M083100100016 #doi:10.1140/epja/i2014-14114-x M083100100017 INSTITUTE (4RUSMOS) M083100100018 INC-SOURCE (QMPH,ARAD) M083100100019 STATUS (TABLE,APRVD) Approved by V.Varlamov. M083100100020 COMMENT For 159Tb the combined analysis was carried out for M083100100021 experimental data for cross sections of total M083100100022 (g,xn) and partial photoneutron reactions obtained M083100100023 using bremsstrahlung and quasimonoenergetic M083100100024 annihilation photons. The analysis of concrete M083100100025 experiment data reliability was carried out using M083100100026 the special transitional multiplicity function F2 = M083100100027 SIG(g,2n)/SIG(g,xn). In the frame of the new M083100100028 experimental-theoretical treatment for evaluation M083100100029 of partial reaction cross sections the evaluated M083100100030 data for SIG(g,n), SIG(g,2n), SIG(g,3n) and M083100100031 SIG(g,sn) = SIG(g,n) + SIG(g,2n) + SI(g,3n) reaction M083100100032 cross sections for 158Tb free from the shortcomings M083100100033 of experimental neutron multiplicity sorting methods M083100100034 were obtained using as initial the experimental data M083100100035 on total photoneutron yield reaction (g,xn) cross M083100100036 section obtained at Saclay (France). M083100100037 HISTORY (20111024C) Data were compiled at the Russia MSU SINP M083100100038 CDFE by V.Varlamov. M083100100039 (20130123A) Corrected by V.Varlamov: REFERENCE, doi. M083100100040 (20141113A) Corrected by V.Varlamov: REFERENCE, doi. M083100100041 ENDBIB 39 0 M083100100042 NOCOMMON 0 0 M083100100043 ENDSUBENT 42 0 M083100199999 SUBENT M0831002 20111024 M060M083100200001 BIB 5 22 M083100200002 REACTION ((65-TB-159(G,N)65-TB-158,,SIG,,,EVAL)+ M083100200003 (65-TB-159(G,N+P)64-GD-157,,SIG,,,EVAL)) M083100200004 ANALYSIS The contribution of partial reaction (g,n) cross M083100200005 section into the experimental total neutron yield M083100200006 reaction (g,xn) cross section obtained using M083100200007 quasimonoenergetic annihilation photons at Saclay M083100200008 (France) was evaluated using specially theoretically M083100200009 calculated transitional multiplicity function - M083100200010 ratio M083100200011 F1-theor = SIG-theor(g,n)/SIG-theor(g,xn) M083100200012 by the way M083100200013 SIG-eval(g,n) = (F1-theor)x(SIG-exp(g,xn)). M083100200014 ERR-ANALYS (DATA-ERR) Root-mean-square errors. M083100200015 REL-REF (R,L0012006,R.Bergere+,J,NP/A,121,463,1968) M083100200016 Experimental data for the total neutron yield M083100200017 reaction (g,xn) cross section. M083100200018 (E,,B.S.ISHKHANOV+,J,YF,71,517,2008) M083100200019 Theoretical preequilibrium model of photonuclear M083100200020 reactions based on the Fermi gas densities. M083100200021 STATUS (DEP,L0012006) M083100200022 The total neutron yield reaction (g,xn) cross M083100200023 section. M083100200024 ENDBIB 22 0 M083100200025 NOCOMMON 0 0 M083100200026 DATA 3 198 M083100200027 EN DATA DATA-ERR M083100200028 MEV MB MB M083100200029 7.7 9.9 1.8 M083100200030 7.8 11.3 1.8 M083100200031 7.9 12.8 1.8 M083100200032 8. 14.5 3.7 M083100200033 8.1 16.4 5.2 M083100200034 8.2 18.5 5.2 M083100200035 8.3 20.8 5.3 M083100200036 8.4 23.1 5.3 M083100200037 8.5 25.7 5.4 M083100200038 8.6 28.3 5.5 M083100200039 8.7 31.1 5.5 M083100200040 8.8 34. 5.6 M083100200041 8.9 37.1 5.6 M083100200042 9. 40.4 5.7 M083100200043 9.1 43.9 5.8 M083100200044 9.2 47.8 5.8 M083100200045 9.3 51.9 5.9 M083100200046 9.4 56.3 5.9 M083100200047 9.5 61. 6. M083100200048 9.6 66. 6. M083100200049 9.7 71.2 6.1 M083100200050 9.8 76.7 6.2 M083100200051 9.9 82.4 6.2 M083100200052 10. 88.5 6.3 M083100200053 10.1 94.8 6.3 M083100200054 10.2 101.5 6.4 M083100200055 10.3 108.5 6.4 M083100200056 10.4 115.8 6.5 M083100200057 10.5 123.4 6.5 M083100200058 10.6 131.4 6.6 M083100200059 10.7 139.7 6.7 M083100200060 10.8 148.2 6.7 M083100200061 10.9 156.9 6.8 M083100200062 11. 165.9 6.8 M083100200063 11.1 174.9 6.9 M083100200064 11.2 183.9 7. M083100200065 11.3 192.9 7. M083100200066 11.4 201.7 7.1 M083100200067 11.5 210.1 7.1 M083100200068 11.6 218.1 7.2 M083100200069 11.7 225.4 7.2 M083100200070 11.8 232. 7.3 M083100200071 11.9 237.6 7.3 M083100200072 12. 242.2 7.4 M083100200073 12.1 245.8 7.5 M083100200074 12.2 248.2 7.5 M083100200075 12.3 249.5 7.6 M083100200076 12.4 249.9 7.6 M083100200077 12.5 249.5 7.7 M083100200078 12.6 248.4 7.8 M083100200079 12.7 246.7 7.8 M083100200080 12.8 244.8 7.9 M083100200081 12.9 242.8 7.9 M083100200082 13. 240.7 8.1 M083100200083 13.1 238.9 8.7 M083100200084 13.2 237.4 9.3 M083100200085 13.3 236.2 9.6 M083100200086 13.4 235.4 9.6 M083100200087 13.5 235. 9.7 M083100200088 13.6 234.9 9.7 M083100200089 13.7 235.2 9.8 M083100200090 13.8 235.7 9.8 M083100200091 13.9 236.5 9.9 M083100200092 14. 237.5 9.9 M083100200093 14.1 238.9 10. M083100200094 14.2 240.8 10. M083100200095 14.3 243.1 10.1 M083100200096 14.4 246. 10.1 M083100200097 14.5 249.5 10.2 M083100200098 14.6 253.7 10.2 M083100200099 14.7 258.6 10.3 M083100200100 14.8 264. 10.3 M083100200101 14.9 262.3 10.4 M083100200102 15. 258.1 10.4 M083100200103 15.1 250. 10.5 M083100200104 15.2 238.9 10.6 M083100200105 15.3 225.7 10.7 M083100200106 15.4 210.8 10.9 M083100200107 15.5 195.2 11. M083100200108 15.6 179.7 11.2 M083100200109 15.7 164.9 11.4 M083100200110 15.8 151.5 11.6 M083100200111 15.9 139.5 11.7 M083100200112 16. 129.2 11.9 M083100200113 16.1 120.1 12. M083100200114 16.2 112.4 12.2 M083100200115 16.3 105.5 12.3 M083100200116 16.4 99.5 12.4 M083100200117 16.5 94. 12.5 M083100200118 16.6 89. 12.6 M083100200119 16.7 84.5 12.7 M083100200120 16.8 80.3 12.7 M083100200121 16.9 76.4 12.8 M083100200122 17. 72.7 12.8 M083100200123 17.1 69.3 12.9 M083100200124 17.2 66.3 12.9 M083100200125 17.3 63.4 13. M083100200126 17.4 60.5 13. M083100200127 17.5 57.8 13. M083100200128 17.6 55.3 13. M083100200129 17.7 52.8 13.1 M083100200130 17.8 50.5 13.1 M083100200131 17.9 48.3 13.2 M083100200132 18. 46.2 13.2 M083100200133 18.1 44.1 13.3 M083100200134 18.2 42.2 13.3 M083100200135 18.3 40.3 13.3 M083100200136 18.4 38.6 13.3 M083100200137 18.5 37.0 13.4 M083100200138 18.6 35.5 13.4 M083100200139 18.7 34. 13.4 M083100200140 18.8 32.7 13.4 M083100200141 18.9 31.5 13.5 M083100200142 19. 30.4 13.5 M083100200143 19.1 29.3 13.5 M083100200144 19.2 28.4 13.5 M083100200145 19.3 27.4 13.5 M083100200146 19.4 26.6 13.5 M083100200147 19.5 25.8 13.5 M083100200148 19.6 25.1 13.6 M083100200149 19.7 24.4 13.6 M083100200150 19.8 23.7 13.7 M083100200151 19.9 23.1 13.7 M083100200152 20. 22.5 13.7 M083100200153 20.1 22. 13.7 M083100200154 20.2 21.5 13.8 M083100200155 20.3 21.1 13.8 M083100200156 20.4 20.7 13.8 M083100200157 20.5 20.4 13.8 M083100200158 20.6 20.1 13.8 M083100200159 20.7 19.9 13.8 M083100200160 20.8 19.7 13.9 M083100200161 20.9 19.5 13.9 M083100200162 21. 19.3 13.9 M083100200163 21.1 19. 13.9 M083100200164 21.2 18.8 13.9 M083100200165 21.3 18.6 13.9 M083100200166 21.4 18.3 13.8 M083100200167 21.5 18. 13.9 M083100200168 21.6 17.8 13.9 M083100200169 21.7 17.5 14. M083100200170 21.8 17.3 14. M083100200171 21.9 17.1 14. M083100200172 22. 16.9 14. M083100200173 22.1 16.8 14. M083100200174 22.2 16.7 14.1 M083100200175 22.3 16.7 14.1 M083100200176 22.4 16.6 14.1 M083100200177 22.5 16.6 14.1 M083100200178 22.6 16.6 14.1 M083100200179 22.7 16.5 14.1 M083100200180 22.8 16.5 14.5 M083100200181 22.9 16.5 15.5 M083100200182 23. 16.5 16.5 M083100200183 23.1 16.6 16.9 M083100200184 23.2 16.7 16.9 M083100200185 23.3 16.8 16.9 M083100200186 23.4 17. 17. M083100200187 23.5 17.3 17. M083100200188 23.6 16.9 17. M083100200189 23.7 17. 17. M083100200190 23.8 17.1 17. M083100200191 23.9 17.1 17. M083100200192 24. 17. 17. M083100200193 24.1 16.9 17. M083100200194 24.2 16.7 17. M083100200195 24.3 16.4 17. M083100200196 24.4 16.1 16.9 M083100200197 24.5 15.7 16.9 M083100200198 24.6 15.3 16.9 M083100200199 24.7 14.9 16.8 M083100200200 24.8 14.5 16.8 M083100200201 24.9 14.1 16.7 M083100200202 25. 13.7 16.6 M083100200203 25.1 13.4 16.6 M083100200204 25.2 12.9 16.5 M083100200205 25.3 12.2 16.5 M083100200206 25.4 11.9 16.5 M083100200207 25.5 12.5 16.4 M083100200208 25.6 11.9 16.4 M083100200209 25.7 11.2 16.4 M083100200210 25.8 11.5 16.4 M083100200211 25.9 10.9 16.4 M083100200212 26. 10.2 16.4 M083100200213 26.1 10.5 16.5 M083100200214 26.2 10. 16.5 M083100200215 26.3 9.4 16.6 M083100200216 26.4 9.7 16.6 M083100200217 26.5 9.3 16.6 M083100200218 26.6 8.8 16.7 M083100200219 26.7 9. 16.7 M083100200220 26.8 8.7 16.8 M083100200221 26.9 8.3 16.8 M083100200222 27. 8.5 16.9 M083100200223 27.1 8.2 16.9 M083100200224 27.2 7.9 17. M083100200225 27.3 8. 17. M083100200226 27.4 7.8 17.1 M083100200227 ENDDATA 200 0 M083100200228 ENDSUBENT 227 0 M083100299999 SUBENT M0831003 20111024 M060M083100300001 BIB 5 23 M083100300002 REACTION ((65-TB-159(G,2N)65-TB-157,,SIG,,,EVAL)+ M083100300003 (65-TB-159(G,2N+P)64-GD-156,,SIG,,,EVAL)) M083100300004 The threshold of (g,np) reaction is 14 MeV. M083100300005 ANALYSIS The contribution of partial reaction (g,2n) cross M083100300006 section into the experimental total neutron yield M083100300007 reaction (g,xn) cross section obtained using M083100300008 quasimonoenergetic annihilation photons at Saclay M083100300009 (France) was evaluated using specially theoretically M083100300010 calculated transitional multiplicity function - M083100300011 ratio M083100300012 F2-theor = SIG-theor(g,2n)/SIG-theor(g,xn) M083100300013 by the way M083100300014 SIG-eval(g,2n) = (F2-theor)x(SIG-exp(g,xn)). M083100300015 ERR-ANALYS (DATA-ERR) Root-mean-square errors. M083100300016 REL-REF (R,L0012006,R.Bergere+,J,NP/A,121,463,1968) M083100300017 Experimental data for the total neutron yield M083100300018 reaction (g,xn) cross section. M083100300019 (E,,B.S.ISHKHANOV+,J,YF,71,517,2008) M083100300020 Theoretical preequilibrium model of photonuclear M083100300021 reactions based on the Fermi gas densities. M083100300022 STATUS (DEP,L0012006) M083100300023 The total neutron yield reaction (g,xn) cross M083100300024 section. M083100300025 ENDBIB 23 0 M083100300026 NOCOMMON 0 0 M083100300027 DATA 3 127 M083100300028 EN DATA DATA-ERR M083100300029 MEV MB MB M083100300030 14.8 0.0 0.1 M083100300031 14.9 3.8 0.1 M083100300032 15. 9. 0.3 M083100300033 15.1 16.4 0.6 M083100300034 15.2 25.2 0.9 M083100300035 15.3 35.1 1.3 M083100300036 15.4 45.7 1.6 M083100300037 15.5 56.5 2. M083100300038 15.6 67. 2.3 M083100300039 15.7 76.9 2.6 M083100300040 15.8 85.8 2.9 M083100300041 15.9 93.8 3.1 M083100300042 16. 100.5 3.3 M083100300043 16.1 106.3 3.5 M083100300044 16.2 111.1 3.7 M083100300045 16.3 115.1 3.8 M083100300046 16.4 118.4 3.9 M083100300047 16.5 121. 4. M083100300048 16.6 122.9 4.1 M083100300049 16.7 124.2 4.2 M083100300050 16.8 125. 4.3 M083100300051 16.9 125.4 4.3 M083100300052 17. 125.3 4.4 M083100300053 17.1 124.9 4.4 M083100300054 17.2 124.1 4.5 M083100300055 17.3 122.9 4.5 M083100300056 17.4 121.6 4.5 M083100300057 17.5 120. 4.6 M083100300058 17.6 118.1 4.6 M083100300059 17.7 116.1 4.6 M083100300060 17.8 113.8 4.7 M083100300061 17.9 111.3 4.7 M083100300062 18. 108.7 4.7 M083100300063 18.1 105.9 4.7 M083100300064 18.2 103.1 4.8 M083100300065 18.3 100.3 4.8 M083100300066 18.4 97.4 4.8 M083100300067 18.5 94.6 4.8 M083100300068 18.6 91.9 4.8 M083100300069 18.7 89.3 4.8 M083100300070 18.8 86.8 4.9 M083100300071 18.9 84.3 4.9 M083100300072 19. 82. 4.9 M083100300073 19.1 79.8 4.9 M083100300074 19.2 77.7 4.9 M083100300075 19.3 75.7 4.9 M083100300076 19.4 73.7 4.9 M083100300077 19.5 71.9 4.9 M083100300078 19.6 70.1 4.9 M083100300079 19.7 68.4 5. M083100300080 19.8 66.7 5. M083100300081 19.9 65. 5. M083100300082 20. 63.4 5. M083100300083 20.1 61.8 5. M083100300084 20.2 60.3 5. M083100300085 20.3 58.9 5. M083100300086 20.4 57.7 5. M083100300087 20.5 56.5 5. M083100300088 20.6 55.5 5. M083100300089 20.7 54.5 5. M083100300090 20.8 53.6 5. M083100300091 20.9 52.7 5. M083100300092 21. 51.7 5. M083100300093 21.1 50.7 5. M083100300094 21.2 49.7 5. M083100300095 21.3 48.6 5. M083100300096 21.4 47.5 5. M083100300097 21.5 46.4 5. M083100300098 21.6 45.3 5. M083100300099 21.7 44.2 5. M083100300100 21.8 43.2 5. M083100300101 21.9 42.3 5. M083100300102 22. 41.5 5. M083100300103 22.1 40.8 5. M083100300104 22.2 40.1 5. M083100300105 22.3 39.6 5. M083100300106 22.4 39.2 5. M083100300107 22.5 38.8 5. M083100300108 22.6 38.4 5. M083100300109 22.7 38. 5. M083100300110 22.8 37.7 5.2 M083100300111 22.9 37.5 5.5 M083100300112 23. 37.3 5.9 M083100300113 23.1 37.2 6. M083100300114 23.2 37.3 6. M083100300115 23.3 37.5 6. M083100300116 23.4 37.8 6. M083100300117 23.5 38.2 6. M083100300118 23.6 38.8 6. M083100300119 23.7 39.3 6. M083100300120 23.8 39.8 6. M083100300121 23.9 40.2 6. M083100300122 24. 40.5 6. M083100300123 24.1 40.5 6. M083100300124 24.2 40.2 5.9 M083100300125 24.3 39.5 5.9 M083100300126 24.4 38.5 5.8 M083100300127 24.5 37.1 5.7 M083100300128 24.6 35.4 5.6 M083100300129 24.7 33.5 5.5 M083100300130 24.8 31.5 5.4 M083100300131 24.9 29.5 5.2 M083100300132 25. 27.5 5.1 M083100300133 25.1 25.6 4.9 M083100300134 25.2 24. 4.8 M083100300135 25.3 22.7 4.6 M083100300136 25.4 21.5 4.5 M083100300137 25.5 19.9 4.2 M083100300138 25.6 19.1 4.1 M083100300139 25.7 18.4 3.9 M083100300140 25.8 17.3 3.7 M083100300141 25.9 16.7 3.6 M083100300142 26. 16.1 3.4 M083100300143 26.1 15.1 3.2 M083100300144 26.2 14.4 3.1 M083100300145 26.3 13.9 3. M083100300146 26.4 13. 2.8 M083100300147 26.5 12.4 2.7 M083100300148 26.6 12. 2.7 M083100300149 26.7 11.2 2.5 M083100300150 26.8 10.8 2.4 M083100300151 26.9 10.4 2.3 M083100300152 27. 9.8 2.2 M083100300153 27.1 9.4 2.1 M083100300154 27.2 9.1 2.1 M083100300155 27.3 8.6 2. M083100300156 27.4 8.3 1.9 M083100300157 ENDDATA 129 0 M083100300158 ENDSUBENT 157 0 M083100399999 SUBENT M0831004 20111024 M060M083100400001 BIB 5 22 M083100400002 REACTION ((65-TB-159(G,3N)65-TB-156,,SIG,,,EVAL)+ M083100400003 (65-TB-159(G,3N+P)64-GD-155,,SIG,,,EVAL)) M083100400004 ANALYSIS The contribution of partial reaction (g,3n) cross M083100400005 section into the experimental total neutron yield M083100400006 reaction (g,xn) cross section obtained using M083100400007 quasimonoenergetic annihilation photons at Saclay M083100400008 (France) was evaluated using specially theoretically M083100400009 calculated transitional multiplicity function - M083100400010 ratio M083100400011 F3-theor = SIG-theor(g,3n)/SIG-theor(g,xn) M083100400012 by the way M083100400013 SIG-eval(g,3n) = (F3-theor)x(SIG-exp(g,xn)). M083100400014 ERR-ANALYS (DATA-ERR) Root-mean-square errors. M083100400015 REL-REF (R,L0012006,R.Bergere+,J,NP/A,121,463,1968) M083100400016 Experimental data for the total neutron yield M083100400017 reaction (g,xn) cross section. M083100400018 (E,,B.S.ISHKHANOV+,J,YF,71,517,2008) M083100400019 Theoretical preequilibrium model of photonuclear M083100400020 reactions based on the Fermi gas densities. M083100400021 STATUS (DEP,L0012006) M083100400022 The total neutron yield reaction (g,xn) cross M083100400023 section. M083100400024 ENDBIB 22 0 M083100400025 NOCOMMON 0 0 M083100400026 DATA 3 39 M083100400027 EN DATA DATA-ERR M083100400028 MEV MB MB M083100400029 23.6 0.2 0.1 M083100400030 23.7 0.3 0.1 M083100400031 23.8 0.4 0.1 M083100400032 23.9 0.5 0.1 M083100400033 24. 0.6 0.1 M083100400034 24.1 0.8 0.1 M083100400035 24.2 1.1 0.2 M083100400036 24.3 1.4 0.2 M083100400037 24.4 1.7 0.3 M083100400038 24.5 2. 0.3 M083100400039 24.6 2.4 0.4 M083100400040 24.7 2.8 0.5 M083100400041 24.8 3.2 0.5 M083100400042 24.9 3.6 0.6 M083100400043 25. 3.9 0.7 M083100400044 25.1 4.3 0.8 M083100400045 25.2 4.8 0.9 M083100400046 25.3 5.2 1.1 M083100400047 25.4 5.7 1.2 M083100400048 25.5 6.3 1.3 M083100400049 25.6 6.9 1.5 M083100400050 25.7 7.5 1.6 M083100400051 25.8 8.1 1.7 M083100400052 25.9 8.7 1.9 M083100400053 26. 9.3 2. M083100400054 26.1 9.8 2.1 M083100400055 26.2 10.3 2.2 M083100400056 26.3 10.7 2.3 M083100400057 26.4 11.1 2.4 M083100400058 26.5 11.5 2.5 M083100400059 26.6 11.8 2.6 M083100400060 26.7 12.1 2.7 M083100400061 26.8 12.4 2.8 M083100400062 26.9 12.7 2.9 M083100400063 27. 13. 2.9 M083100400064 27.1 13.2 3. M083100400065 27.2 13.5 3.1 M083100400066 27.3 13.7 3.1 M083100400067 27.4 13.9 3.2 M083100400068 ENDDATA 41 0 M083100400069 ENDSUBENT 68 0 M083100499999 SUBENT M0831005 20111024 M060M083100500001 BIB 4 15 M083100500002 REACTION (65-TB-159(G,X)0-NN-1,UNW,SIG,,,EVAL) M083100500003 ANALYSIS The contribution of total reaction (g,sn) cross M083100500004 sections into the experimental total neutron yield M083100500005 reaction (g,xn) cross section obtained using M083100500006 quasimonoenergetic annihilation photons at Saclay M083100500007 (France) was evaluated using M083100500008 SIG-eval(g,2n) = (F2-theor)x(SIG-exp(g,xn)) M083100500009 by the way M083100500010 SIG-eval(g,sn) = SIG-exp(g,xn) - SIG-eval(g,2n). M083100500011 ERR-ANALYS (DATA-ERR) Root-mean-square errors. M083100500012 STATUS (DEP,L0012006) M083100500013 The total neutron yield reaction (g,xn) cross M083100500014 section. M083100500015 (DEP,M0831002) M083100500016 Evaluated (g,2n) reaction cross section. M083100500017 ENDBIB 15 0 M083100500018 NOCOMMON 0 0 M083100500019 DATA 3 198 M083100500020 EN DATA DATA-ERR M083100500021 MEV MB MB M083100500022 7.7 9.9 1.8 M083100500023 7.8 11.3 1.8 M083100500024 7.9 12.8 1.8 M083100500025 8.0 14.5 3.7 M083100500026 8.1 16.4 5.2 M083100500027 8.2 18.5 5.2 M083100500028 8.3 20.8 5.3 M083100500029 8.4 23.1 5.3 M083100500030 8.5 25.7 5.4 M083100500031 8.6 28.3 5.5 M083100500032 8.7 31.1 5.5 M083100500033 8.8 34. 5.6 M083100500034 8.9 37.1 5.6 M083100500035 9. 40.4 5.7 M083100500036 9.1 43.9 5.8 M083100500037 9.2 47.8 5.8 M083100500038 9.3 51.9 5.9 M083100500039 9.4 56.3 5.9 M083100500040 9.5 61. 6. M083100500041 9.6 66. 6. M083100500042 9.7 71.2 6.1 M083100500043 9.8 76.7 6.2 M083100500044 9.9 82.4 6.2 M083100500045 10. 88.5 6.3 M083100500046 10.1 94.8 6.3 M083100500047 10.2 101.5 6.4 M083100500048 10.3 108.5 6.4 M083100500049 10.4 115.8 6.5 M083100500050 10.5 123.4 6.5 M083100500051 10.6 131.4 6.6 M083100500052 10.7 139.7 6.7 M083100500053 10.8 148.2 6.7 M083100500054 10.9 156.9 6.8 M083100500055 11. 165.9 6.8 M083100500056 11.1 174.9 6.9 M083100500057 11.2 183.9 7. M083100500058 11.3 192.9 7. M083100500059 11.4 201.7 7.1 M083100500060 11.5 210.1 7.1 M083100500061 11.6 218.1 7.2 M083100500062 11.7 225.4 7.2 M083100500063 11.8 232. 7.3 M083100500064 11.9 237.6 7.3 M083100500065 12. 242.2 7.4 M083100500066 12.1 245.8 7.5 M083100500067 12.2 248.2 7.5 M083100500068 12.3 249.5 7.6 M083100500069 12.4 249.9 7.6 M083100500070 12.5 249.5 7.7 M083100500071 12.6 248.4 7.8 M083100500072 12.7 246.7 7.8 M083100500073 12.8 244.8 7.9 M083100500074 12.9 242.8 7.9 M083100500075 13. 240.7 8.1 M083100500076 13.1 238.9 8.7 M083100500077 13.2 237.4 9.3 M083100500078 13.3 236.2 9.6 M083100500079 13.4 235.4 9.6 M083100500080 13.5 235. 9.7 M083100500081 13.6 234.9 9.7 M083100500082 13.7 235.2 9.8 M083100500083 13.8 235.7 9.8 M083100500084 13.9 236.5 9.9 M083100500085 14. 237.5 9.9 M083100500086 14.1 238.9 10. M083100500087 14.2 240.8 10. M083100500088 14.3 243.1 10.1 M083100500089 14.4 246. 10.1 M083100500090 14.5 249.5 10.2 M083100500091 14.6 253.7 10.2 M083100500092 14.7 258.6 10.3 M083100500093 14.8 264. 10.3 M083100500094 14.9 266.1 10.4 M083100500095 15. 267.1 10.4 M083100500096 15.1 266.4 10.5 M083100500097 15.2 264.1 10.6 M083100500098 15.3 260.8 10.6 M083100500099 15.4 256.5 10.7 M083100500100 15.5 251.7 10.8 M083100500101 15.6 246.7 10.9 M083100500102 15.7 241.8 11.1 M083100500103 15.8 237.3 11.2 M083100500104 15.9 233.3 11.3 M083100500105 16. 229.7 11.4 M083100500106 16.1 226.4 11.5 M083100500107 16.2 223.5 11.6 M083100500108 16.3 220.7 11.7 M083100500109 16.4 217.8 11.8 M083100500110 16.5 214.9 11.9 M083100500111 16.6 211.9 11.9 M083100500112 16.7 208.7 12. M083100500113 16.8 205.3 12. M083100500114 16.9 201.8 12.1 M083100500115 17. 198.1 12.1 M083100500116 17.1 194.2 12.1 M083100500117 17.2 190.3 12.2 M083100500118 17.3 186.3 12.2 M083100500119 17.4 182.1 12.2 M083100500120 17.5 177.8 12.2 M083100500121 17.6 173.4 12.2 M083100500122 17.7 168.9 12.2 M083100500123 17.8 164.3 12.3 M083100500124 17.9 159.6 12.3 M083100500125 18. 154.8 12.4 M083100500126 18.1 150. 12.4 M083100500127 18.2 145.3 12.4 M083100500128 18.3 140.6 12.4 M083100500129 18.4 136. 12.4 M083100500130 18.5 131.6 12.5 M083100500131 18.6 127.4 12.5 M083100500132 18.7 123.3 12.5 M083100500133 18.8 119.5 12.5 M083100500134 18.9 115.8 12.6 M083100500135 19. 112.4 12.6 M083100500136 19.1 109.1 12.6 M083100500137 19.2 106. 12.6 M083100500138 19.3 103.1 12.6 M083100500139 19.4 100.3 12.6 M083100500140 19.5 97.7 12.6 M083100500141 19.6 95.2 12.7 M083100500142 19.7 92.8 12.7 M083100500143 19.8 90.5 12.7 M083100500144 19.9 88.2 12.8 M083100500145 20. 85.9 12.8 M083100500146 20.1 83.8 12.8 M083100500147 20.2 81.8 12.8 M083100500148 20.3 80. 12.8 M083100500149 20.4 78.4 12.8 M083100500150 20.5 77. 12.9 M083100500151 20.6 75.6 12.9 M083100500152 20.7 74.4 12.9 M083100500153 20.8 73.3 12.9 M083100500154 20.9 72.2 12.9 M083100500155 21. 71. 12.9 M083100500156 21.1 69.8 13. M083100500157 21.2 68.5 12.9 M083100500158 21.3 67.1 12.9 M083100500159 21.4 65.8 12.9 M083100500160 21.5 64.4 12.9 M083100500161 21.6 63. 13. M083100500162 21.7 61.7 13.1 M083100500163 21.8 60.5 13.1 M083100500164 21.9 59.4 13.1 M083100500165 22. 58.4 13.1 M083100500166 22.1 57.6 13.1 M083100500167 22.2 56.9 13.1 M083100500168 22.3 56.3 13.1 M083100500169 22.4 55.8 13.2 M083100500170 22.5 55.4 13.2 M083100500171 22.6 54.9 13.2 M083100500172 22.7 54.6 13.2 M083100500173 22.8 54.2 13.6 M083100500174 22.9 54. 14.5 M083100500175 23. 53.8 15.4 M083100500176 23.1 53.8 15.8 M083100500177 23.2 54. 15.8 M083100500178 23.3 54.3 15.9 M083100500179 23.4 54.8 15.9 M083100500180 23.5 55.5 15.9 M083100500181 23.6 55.9 15.9 M083100500182 23.7 56.6 15.9 M083100500183 23.8 57.3 15.9 M083100500184 23.9 57.8 15.9 M083100500185 24. 58.1 15.9 M083100500186 24.1 58.2 16. M083100500187 24.2 57.9 15.9 M083100500188 24.3 57.3 15.9 M083100500189 24.4 56.2 15.9 M083100500190 24.5 54.8 15.9 M083100500191 24.6 53.1 15.9 M083100500192 24.7 51.2 15.9 M083100500193 24.8 49.2 15.9 M083100500194 24.9 47.1 15.9 M083100500195 25. 45.1 15.8 M083100500196 25.1 43.3 15.8 M083100500197 25.2 41.6 15.8 M083100500198 25.3 40.1 15.8 M083100500199 25.4 39.1 15.8 M083100500200 25.5 38.7 15.8 M083100500201 25.6 37.9 15.8 M083100500202 25.7 37.1 15.9 M083100500203 25.8 36.9 15.9 M083100500204 25.9 36.3 15.9 M083100500205 26. 35.6 16. M083100500206 26.1 35.4 16. M083100500207 26.2 34.7 16.1 M083100500208 26.3 34. 16.1 M083100500209 26.4 33.8 16.1 M083100500210 26.5 33.2 16.2 M083100500211 26.6 32.6 16.3 M083100500212 26.7 32.4 16.3 M083100500213 26.8 31.9 16.4 M083100500214 26.9 31.5 16.4 M083100500215 27. 31.3 16.5 M083100500216 27.1 30.9 16.5 M083100500217 27.2 30.5 16.6 M083100500218 27.3 30.3 16.6 M083100500219 27.4 30. 16.7 M083100500220 ENDDATA 200 0 M083100500221 ENDSUBENT 220 0 M083100599999 ENDENTRY 5 0 M083199999999