Difference between revisions of "Isotopes of fermium"
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| — | | — | ||
| align=center | 0 | | align=center | 0 | ||
| − | | | + | | 0.8(2) ms |
| SF (? %); α (? %) | | SF (? %); α (? %) | ||
| + | |- | ||
| + | | <sup>243</sup>Fm | ||
| + | | 100 | ||
| + | | 143 | ||
| + | | | ||
| + | | 69260(220)# | ||
| + | | | ||
| + | | align=center | −{{frac|7|2}}# | ||
| + | | 210(60) ms | ||
| + | | α;<ref group="Note">The α ranching ratio depends on the uncertain branching ratio of the daughter <sup>239</sup>Cf.</ref> β<sup>+</sup> (? %); SF (59%#) | ||
| + | |- | ||
| + | | <sup>244</sup>Fm | ||
| + | | 100 | ||
| + | | 144 | ||
| + | | | ||
| + | | 69010(280) | ||
| + | | | ||
| + | | align=center | 0 | ||
| + | | 3.3(0.5) ms | ||
| + | | SF (≈100%); α (0.4%#) | ||
| + | |- | ||
| + | | <sup>245</sup>Fm | ||
| + | | 100 | ||
| + | | 145 | ||
| + | | | ||
| + | | 70220(280)# | ||
| + | | | ||
| + | | align=center | +½# | ||
| + | | 4.2(13) s | ||
| + | | α (? %); β<sup>+</sup> (4.2%#); SF (0.13%#) | ||
|- | |- | ||
| colspan=10 | Values marked # are estimated from systematic trends rather than experimentally measured.<br/>Spins quoted in parentheses are uncertain in value and/or parity.<br/>''Sources'': Except as otherwise noted, | | colspan=10 | Values marked # are estimated from systematic trends rather than experimentally measured.<br/>Spins quoted in parentheses are uncertain in value and/or parity.<br/>''Sources'': Except as otherwise noted, | ||
Revision as of 15:19, 24 September 2010
Fermium is an artificial element, and has no stable or naturally occuring isotopes. The first isotope to be discovered was 255100Fm, in fallout from the first test of a hydrogen bomb, codenamed 'Ivy Mike', in 1952. 250100Fm was discovered independently in 1954.
| Symbol | Z(p) | N(n) | Mass/u | Excess energy MeV |
Binding energy/A MeV |
β−-decay energy MeV |
Spin | Half life | Decay mode, proportion |
|---|---|---|---|---|---|---|---|---|---|
| Excitation energy/MeV | |||||||||
| 242Fm | 100 | 142 | 242.073 43(43)# | 68 400(401)# | 7465(2)# | — | 0 | 0.8(2) ms | SF (? %); α (? %) |
| 243Fm | 100 | 143 | 69260(220)# | −7⁄2# | 210(60) ms | α;[Note 1] β+ (? %); SF (59%#) | |||
| 244Fm | 100 | 144 | 69010(280) | 0 | 3.3(0.5) ms | SF (≈100%); α (0.4%#) | |||
| 245Fm | 100 | 145 | 70220(280)# | +½# | 4.2(13) s | α (? %); β+ (4.2%#); SF (0.13%#) | |||
| Values marked # are estimated from systematic trends rather than experimentally measured. Spins quoted in parentheses are uncertain in value and/or parity. Sources: Except as otherwise noted, | |||||||||
Notes and references
Notes
- ↑ The α ranching ratio depends on the uncertain branching ratio of the daughter 239Cf.
References
- ↑ Wapstra, A. H.; Audi, G.; Thibault, C. The AME2003 atomic mass evaluation (I). Evaluation of input data, adjustment procedures. Nucl. Phys. A 2003, 729, 129–336. DOI: 10.1016/j.nuclphysa.2003.11.002. Wapstra, A. H.; Audi, G.; Thibault, C. The AME2003 atomic mass evaluation (II). Tables, graphs, and references. Nucl. Phys. A 2003, 729, 337–676. DOI: 10.1016/j.nuclphysa.2003.11.003. Data tables.
- ↑ Audi, G.; Bersillon, O.; Blachot, J.; Wapstra, A. H. The NUBASE evaluation of nuclear and decay properties. Nucl. Phys. A 2003, 729, 3–128. doi:10.1016/j.nuclphysa.2003.11.001, <http://amdc.in2p3.fr/nubase/Nubase2003.pdf>.
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