Difference between revisions of "ENDF file definitions and supplied nuclear data"
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Revision as of 11:28, 8 September 2016
FISPACT-II employs the standard ENDF reaction MTs to identify incident particle reactions, residual nuclide production, dpa and kerma, depending on the library used and the completeness of the data. Below are descriptive lists of ENDF reaction MTs. For more information on the MT numbers, see the ENDF Format Manual.
Projectile | Products | MT | dZ | dZ | NSEC | Secondaries |
---|---|---|---|---|---|---|
n | total | 1 | 0 | 0 | 0 | |
n | E | 2 | 0 | 0 | 0 | |
n | nonel | 3 | 0 | 0 | 0 | |
n | n | 4 | 0 | 0 | 0 | |
n | O | 5 | 0 | |||
n | 2nd | 11 | -1 | -3 | 1 | $^2$H |
n | 2n | 16 | 0 | -1 | 0 | |
n | 3n | 17 | 0 | -2 | 0 | |
n | F | 18 | 0 | |||
n | nα | 22 | -2 | -4 | 1 | $^4$He |
n | n3α | 23 | -6 | -12 | 3 | $^4$He $^4$He $^4$He |
n | 2nα | 24 | -2 | -5 | 1 | $^4$He |
n | 3nα | 25 | -2 | -6 | 1 | $^4$He |
n | np | 28 | -1 | -1 | 1 | $^1$H |
n | n2α | 29 | -4 | -8 | 2 | $^4$He $^4$He |
n | 2n2α | 30 | -4 | -9 | 2 | $^4$He $^4$He |
n | nd | 32 | -1 | -2 | 1 | $^2$H |
n | nt | 33 | -1 | -3 | 1 | $^3$H |
n | nh | 34 | -2 | -3 | 1 | $^3$He |
n | nd2α | 35 | -5 | -10 | 3 | $^2$H $^4$He $^4$He |
n | nt2α | 36 | -5 | -11 | 3 | $^3$H $^4$He $^4$He |
n | 4n | 37 | 0 | -3 | 0 | |
n | 2np | 41 | -1 | -2 | 1 | $^1$H |
n | 3np | 42 | -1 | -3 | 1 | $^1$H |
n | n2p | 44 | -2 | -2 | 2 | $^1$H $^1$H |
n | npα | 45 | -3 | -5 | 2 | $^1$H $^4$He |
n | γ | 102 | 0 | 1 | 0 | |
n | p | 103 | -1 | 0 | 1 | $^1$H |
n | d | 104 | -1 | -1 | 1 | $^2$H |
n | t | 105 | -1 | -2 | 1 | $^3$H |
n | h | 106 | -2 | -2 | 1 | $^3$He |
n | α | 107 | -2 | -3 | 1 | $^4$He |
n | 2α | 108 | -4 | -7 | 2 | $^4$He $^4$He |
n | 3α | 109 | -6 | -11 | 3 | $^4$He $^4$He $^4$He |
n | 2p | 111 | -2 | -1 | 2 | $^1$H $^1$H |
n | pα | 112 | -3 | -4 | 2 | $^1$H $^4$He |
n | t2α | 113 | -5 | -10 | 3 | $^3$H $^4$He $^4$He |
n | d2α | 114 | -5 | -9 | 3 | $^2$H $^4$He $^4$He |
n | pd | 115 | -2 | -2 | 2 | $^1$H $^2$H |
n | pt | 116 | -2 | -3 | 2 | $^1$H $^3$H |
n | dα | 117 | -3 | -5 | 2 | $^2$H $^4$He |
n | 5n | 152 | 0 | -4 | 0 | |
n | 6n | 153 | 0 | -5 | 0 | |
n | 2nt | 154 | -1 | -4 | 1 | $^3$H |
n | tα | 155 | -3 | -6 | 2 | $^3$H $^4$He |
n | 4np | 156 | -1 | -4 | 1 | $^1$H |
n | 3nd | 157 | -1 | -4 | 1 | $^2$H |
n | ndα | 158 | -3 | -6 | 2 | $^2$H $^4$He |
n | 2npα | 159 | -3 | -6 | 2 | $^1$H $^4$He |
n | 7n | 160 | 0 | -6 | 0 | |
n | 8n | 161 | 0 | -7 | 0 | |
n | 5np | 162 | -1 | -5 | 1 | $^1$H |
n | 6np | 163 | -1 | -6 | 1 | $^1$H |
n | 7np | 164 | -1 | -7 | 1 | $^1$H |
n | 4nα | 165 | -2 | -7 | 1 | $^4$He |
n | 5nα | 166 | -2 | -8 | 1 | $^4$He |
n | 6nα | 167 | -2 | -9 | 1 | $^4$He |
n | 7nα | 168 | -2 | -10 | 1 | $^4$He |
n | 4nd | 169 | -1 | -5 | 1 | $^2$H |
n | 5nd | 170 | -1 | -6 | 1 | $^2$H |
n | 6nd | 171 | -1 | -7 | 1 | $^2$H |
n | 3nt | 172 | -1 | -5 | 1 | $^3$H |
n | 4nt | 173 | -1 | -6 | 1 | $^3$H |
n | 5nt | 174 | -1 | -7 | 1 | $^3$H |
n | 6nt | 175 | -1 | -8 | 1 | $^3$H |
n | 2nh | 176 | -2 | -4 | 1 | $^3$He |
n | 3nh | 177 | -2 | -5 | 1 | $^3$He |
n | 4nh | 178 | -2 | -6 | 1 | $^3$He |
n | 3n2p | 179 | -2 | -4 | 2 | $^1$H $^1$H |
n | 3n2α | 180 | -4 | -10 | 2 | $^4$He $^4$He |
n | 3npα | 181 | -3 | -7 | 2 | $^1$H $^4$He |
n | dt | 182 | -2 | -4 | 2 | $^2$H $^3$H |
n | npd | 183 | -2 | -3 | 2 | $^1$H $^2$H |
n | npt | 184 | -2 | -4 | 2 | $^1$H $^3$H |
n | ndt | 185 | -2 | -5 | 2 | $^2$H $^3$H |
n | nph | 186 | -3 | -4 | 2 | $^1$H $^3$He |
n | ndh | 187 | -3 | -5 | 2 | $^2$H $^3$He |
n | nth | 188 | -3 | -6 | 2 | $^3$H $^3$He |
n | ntα | 189 | -3 | -7 | 2 | $^3$H $^4$He |
n | 2n2p | 190 | -2 | -3 | 2 | $^1$H $^1$H |
n | ph | 191 | -3 | -3 | 2 | $^1$H $^3$He |
n | dh | 192 | -3 | -4 | 2 | $^2$H $^3$He |
n | hα | 193 | -4 | -6 | 2 | $^3$He $^4$He |
n | 4n2p | 194 | -2 | -5 | 2 | $^1$H $^1$H |
n | 4n2α | 195 | -4 | -11 | 2 | $^4$He $^4$He |
n | 4npα | 196 | -3 | -8 | 2 | $^1$H $^4$He |
n | 3p | 197 | -3 | -2 | 3 | $^1$H $^1$H $^1$H |
n | n3p | 198 | -3 | -3 | 3 | $^1$H $^1$H $^1$H |
n | 3n2pα | 199 | -4 | -8 | 3 | $^1$H $^1$H $^4$He |
n | 5n2p | 200 | -2 | -6 | 2 | $^1$H $^1$H |
MT | Description |
---|---|
201 | (z,Xn) Total neutron production |
202 | (z,X$gamma$) Total gamma production |
203 | (z,Xp) Total proton production |
204 | (z,Xd) Total deuteron production |
205 | (z,Xt) Total triton production |
206 | (z,Xh) Total helion (3He) production |
207 | (z,Xα) Total alpha particle production |
301 | Kerma total (eV-barns) |
302 | Kerma elastic |
303 | Kerma non-elastic (all but mt=2) |
304 | Kerma inelastic (mt={51-91}) |
318 | Kerma fission (mt=18 or mt= {19, 20, 21, 38}) |
401 | Kerma disappearance (mt={102-120}) |
402 | Kerma radiative capture (mt=102) |
403 | Kerma proton production (mt=103) |
407 | Kerma α production (mt=107) |
442 | Total photon (eV-barns) |
443 | Total kinematic kerma (high limit) |
444 | Dpa total (eV-barns) |
445 | Dpa elastic (mt=2) |
446 | Dpa inelastic (mt={51-91}) |
447 | Dpa disappearance (mt={102-120}) |