This is an old revision of this page, as edited by Achim1999 (talk | contribs) at 16:49, 19 June 2009 (←Created page with '= Nuclides sorted by Half-Life = In reality so called Stable nuclides may are instable due to very long half-lifes and thus a [[radioactive ...'). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.
Revision as of 16:49, 19 June 2009 by Achim1999 (talk | contribs) (←Created page with '= Nuclides sorted by Half-Life = In reality so called Stable nuclides may are instable due to very long half-lifes and thus a [[radioactive ...')(diff) ← Previous revision | Latest revision (diff) | Newer revision → (diff)Nuclides sorted by Half-Life
In reality so called Stable nuclides may are instable due to very long half-lifes and thus a radioactive decay was not experimentally observed until today. Therefore for those nuclides where no half-life is known, these are sorted by theoretically expected decay-mode and then by relative mass excess (column energy in the following list).
hint: 3.15576/cdot 10 sec = 1 year
decay mode legend
@ | alpha-decay |
- | beta- decay |
K | electron capture |
+ | beta+ decay |
F | spontaneous fission |
2 | double beta- decay |
Z | double beta+ decay |
I | isomeric transition |
list of nuclides
The colum labled "energy" denotes the mass of a nuclide for each nucleon in MeV relative to the mass of a neutron (so all nuclides gets a positive value)
no | nuclide | energy | half-life (sec) | decay mode | decay energy (MeV) |
---|---|---|---|---|---|
1 | Fe | 9.153567 | |||
2 | Ni | 9.147877 | |||
3 | Ni | 9.145862 | |||
4 | Fe | 9.142938 | |||
5 | Cr | 9.137037 | |||
6 | Fe | 9.127119 | |||
7 | Co | 9.126046 | |||
8 | Cr | 9.125633 | |||
9 | Ni | 9.124129 | |||
91 | Mo | 9.011856 | (F) | < 4.485 | |
92 | Nb | 9.009051 | (F) | < 0.943 | |
93 | Mo | 8.996229 | (F) | < 5.771 | |
94 | Mo | 8.994564 | (F) | < 4.531 | |
95 | Mo | 8.973806 | (F) | < 6.226 | |
96 | Ru | 8.971572 | (F) | < 11.690 | |
97 | Ru | 8.963517 | (F) | < 13.634 | |
98 | Ru | 8.956348 | (F) | < 12.368 | |
99 | Ru | 8.944837 | (F) | < 12.049 | |
220 | Hg | 8.208956 | (@) | 0.3341 | |
221 | Hg | 8.206703 | (@) | 0.1363 | |
222 | Tl | 8.198230 | (@) | 0.9108 | |
223 | Hg | 8.192358 | (2) | 0.4163 | |
224 | Tl | 8.187526 | (@) | 0.1567 | |
225 | Pb | 8.186791 | (@) | 1.1366 | |
226 | Pb | 8.179791 | (@) | 0.3915 | |
227 | Pb | 8.175888 | (@) | 0.5188 | |
228 | Ge | 9.034656 | 3.787*10 | 2 | 2.039 |
229 | Te | 8.743261 | > 1.578*10 | 2 | 2.530 |
230 | Xe | 8.728973 | > 1.830*10 | 2 | 0.825 |
231 | Ca | 8.942485 | > 9.467*10 | Z | 0.194 |
232 | Ba | 8.741288 | > 9.467*10 | Z | 0.846 |
233 | Xe | 8.706805 | > 7.574*10 | 2 | 2.462 |
234 | Zr | 8.961359 | > 1.231*10 | 2 | 3.348 |
235 | Kr | 9.022349 | > 7.258*10 | Z | 2.846 |
284 | U | 7.872551 | 1.410*10 | @ F | 4.270 |
285 | K | 8.909707 | 3.938*10 | – K + | 1.311 , 1.505 , 1.505 |
286 | U | 7.897198 | 2.222*10 | @ F | 4.679 |
287 | Sm | 8.626136 | 3.250*10 | @ | 2.529 |
288 | Pu | 7.826221 | 2.525*10 | @ F | 4.666 |