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