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! &nbsp;<br />isotopic mass (u)<br />&nbsp;
! &nbsp;<br />isotopic mass (u)<br />&nbsp;
! rowspan="2" | half-life
! rowspan="2" | half-life
! rowspan="2" | decay<br>mode(s)<ref>http://www.nucleonica.net/unc.aspx</ref><ref group="n">Abbreviations:<br>EC: [[Electron capture]]<br>IT: [[Isomeric transition]]<br>SF: [[Spontaneous fission]]</ref>
! rowspan="2" | daughter<br>isotope(s)
! rowspan="2" | nuclear<br />spin
! rowspan="2" | nuclear<br />spin
|-
|-
! colspan="3" | excitation energy
! colspan="3" | excitation energy
|-
|-
| <sup>245</sup>Md
| rowspan=2|<sup>245</sup>Md
| style="text-align:right" | 101
| rowspan=2 style="text-align:right" | 101
| style="text-align:right" | 144
| rowspan=2 style="text-align:right" | 144
| 245.08083(35)#
| rowspan=2|245.08083(35)#
| 0.90(25) ms
| rowspan=2|0.90(25) ms
| [[Spontaneous fission|SF]]
| (1/2-)#
| (various)
| rowspan=2|(1/2-)#
|-
|-
| [[alpha decay|α]] (rare)
| style="text-indent:1em" | <sup>245m</sup>Md
| <sup>241</sup>Es
| colspan="3" style="text-indent:2em" | 200(100)# keV
| 400(200) ms<br>[0.35(+23-16) s]
| (7/2+)
|-
|-
| <sup>246</sup>Md
| rowspan=2 style="text-indent:1em" | <sup>245m</sup>Md
| style="text-align:right" | 101
| rowspan=2 colspan="3" style="text-indent:2em" | 200(100)# keV
| rowspan=2|400(200) ms<br>[0.35(+23-16) s]
| style="text-align:right" | 145
| α
| 246.08189(35)#
| <sup>241</sup>Es
| 1.0(4) s
| rowspan=2|(7/2+)
|
|-
|-
| <sup>247</sup>Md
| [[beta decay|β<sup>+</sup>]] (rare)
| <sup>245</sup>Fm
| style="text-align:right" | 101
| style="text-align:right" | 146
| 247.08164(35)#
| 1.12(22) s
| 1/2-#
|-
|-
| style="text-indent:1em" | <sup>247m</sup>Md
| rowspan=2|<sup>246</sup>Md
| colspan="3" style="text-indent:2em" |
| rowspan=2 style="text-align:right" | 101
| rowspan=2 style="text-align:right" | 145
| ~0.2 s
| rowspan=2|246.08189(35)#
|
| rowspan=2|1.0(4) s
| α
| <sup>242</sup>Es
| rowspan=2|
|-
|-
| <sup>248</sup>Md
| β<sup>+</sup> (rare)
| <sup>246</sup>Fm
| style="text-align:right" | 101
| style="text-align:right" | 147
| 248.08282(26)#
| 7(3) s
|
|-
|-
| <sup>249</sup>Md
| rowspan=2|<sup>247</sup>Md
| style="text-align:right" | 101
| rowspan=2 style="text-align:right" | 101
| style="text-align:right" | 148
| rowspan=2 style="text-align:right" | 146
| 249.08301(24)#
| rowspan=2|247.08164(35)#
| 24(4) s
| rowspan=2|1.12(22) s
| (7/2-)
| SF
| (various)
| rowspan=2|1/2-#
|-
| α (rare)
| <sup>243</sup>Es
|-
| rowspan=2 style="text-indent:1em" | <sup>247m</sup>Md
| rowspan=2 colspan="3" style="text-indent:2em" |
| rowspan=2|~0.2 s
| α (99.99%)
| <sup>243</sup>Es
| rowspan=2|
|-
| SF (1E-4%)
| (various)
|-
| rowspan=3|<sup>248</sup>Md
| rowspan=3 style="text-align:right" | 101
| rowspan=3 style="text-align:right" | 147
| rowspan=3|248.08282(26)#
| rowspan=3|7(3) s
| β<sup>+</sup> (80%)
| <sup>248</sup>Fm
| rowspan=3|
|-
| α (20%)
| <sup>244</sup>Es
|-
| β<sup>+</sup>, SF (.05%)
| (various)
|-
| rowspan=2|<sup>249</sup>Md
| rowspan=2 style="text-align:right" | 101
| rowspan=2 style="text-align:right" | 148
| rowspan=2|249.08301(24)#
| rowspan=2|24(4) s
| α (60%)
| <sup>245</sup>Es
| rowspan=2|(7/2-)
|-
| β<sup>+</sup> (40%)
| <sup>249</sup>Fm
|-
|-
| style="text-indent:1em" | <sup>249m</sup>Md
| style="text-indent:1em" | <sup>249m</sup>Md
| colspan="3" style="text-indent:2em" | 100(100)# keV
| colspan="3" style="text-indent:2em" | 100(100)# keV
| 1.9(9) s
| 1.9(9) s
|
|
| (1/2-)
| (1/2-)
|-
|-
| <sup>250</sup>Md
| rowspan=3|<sup>250</sup>Md
| style="text-align:right" | 101
| rowspan=3 style="text-align:right" | 101
| style="text-align:right" | 149
| rowspan=3 style="text-align:right" | 149
| 250.08442(32)#
| rowspan=3|250.08442(32)#
| 52(6) s
| rowspan=3|52(6) s
| β<sup>+</sup> (93%)
|
| <sup>250</sup>Fm
| rowspan=3|
|-
|-
| α (7%)
| <sup>251</sup>Md
| <sup>246</sup>Es
| style="text-align:right" | 101
| style="text-align:right" | 150
| 251.08484(22)#
| 4.0(5) min
| 7/2-#
|-
|-
| <sup>252</sup>Md
| β<sup>+</sup>, SF (.02%)
| (various)
| style="text-align:right" | 101
| style="text-align:right" | 151
| 252.08656(21)#
| 2.3(8) min
|
|-
|-
| <sup>253</sup>Md
| rowspan=2|<sup>251</sup>Md
| style="text-align:right" | 101
| rowspan=2 style="text-align:right" | 101
| style="text-align:right" | 152
| rowspan=2 style="text-align:right" | 150
| 253.08728(22)#
| rowspan=2|251.08484(22)#
| rowspan=2|4.0(5) min
| 12(8) min<br>[6(+12-3) min]
| β<sup>+</sup> (90%)
| 7/2-#
| <sup>251</sup>Fm
| rowspan=2|7/2-#
|-
|-
| α (10%)
| <sup>254</sup>Md
| <sup>247</sup>Es
| style="text-align:right" | 101
| style="text-align:right" | 153
| 254.08966(11)#
| 10(3) min
| (0-)
|-
|-
| style="text-indent:1em" | <sup>254m</sup>Md
| rowspan=2|<sup>252</sup>Md
| colspan="3" style="text-indent:2em" | 50(100)# keV
| rowspan=2 style="text-align:right" | 101
| rowspan=2 style="text-align:right" | 151
| 28(8) min
| rowspan=2|252.08656(21)#
| (3-)
| rowspan=2|2.3(8) min
| β<sup>+</sup> (50%)
| <sup>252</sup>Fm
| rowspan=2|
|-
|-
| α (50%)
| <sup>255</sup>Md
| <sup>248</sup>Es
| style="text-align:right" | 101
| style="text-align:right" | 154
| 255.091083(7)
| 27(2) min
| (7/2-)
|-
|-
| <sup>256</sup>Md
| rowspan=2|<sup>253</sup>Md
| style="text-align:right" | 101
| rowspan=2 style="text-align:right" | 101
| style="text-align:right" | 155
| rowspan=2 style="text-align:right" | 152
| rowspan=2|253.08728(22)#
| 256.09406(6)
| 77(2) min
| rowspan=2|12(8) min<br>[6(+12-3) min]
| β<sup>+</sup>
| (1-)
| <sup>249</sup>Fm
| rowspan=2|7/2-#
|-
|-
| α
| <sup>257</sup>Md
| <sup>249</sup>Es
| style="text-align:right" | 101
| style="text-align:right" | 156
| 257.095541(3)
| 5.52(5) h
| (7/2-)
|-
|-
| <sup>258</sup>Md
| rowspan=2|<sup>254</sup>Md
| style="text-align:right" | 101
| rowspan=2 style="text-align:right" | 101
| style="text-align:right" | 157
| rowspan=2 style="text-align:right" | 153
| rowspan=2|254.08966(11)#
| 258.098431(5)
| 51.5(3) d
| rowspan=2|10(3) min
| β<sup>+</sup>
| (8-)#
| <sup>254</sup>Fm
| rowspan=2|(0-)
|-
|-
| α (rare)
| style="text-indent:1em" | <sup>258m</sup>Md
| <sup>250</sup>Es
| colspan="3" style="text-indent:2em" | 0(200)# keV
| 57.0(9) min
| 1-#
|-
|-
| <sup>259</sup>Md
| rowspan=2 style="text-indent:1em" | <sup>254m</sup>Md
| style="text-align:right" | 101
| rowspan=2 colspan="3" style="text-indent:2em" | 50(100)# keV
| rowspan=2|28(8) min
| style="text-align:right" | 158
| β<sup>+</sup>
| 259.10051(22)#
| <sup>254</sup>Fm
| 1.60(6) h
| 7/2-#
| rowspan=2|(3-)
|-
|-
| α (rare)
| <sup>260</sup>Md<ref group="n">First isotope synthesized, also first isotope of any element to be produced one atom at a time</ref>
| <sup>250</sup>Es
| style="text-align:right" | 101
|-
| style="text-align:right" | 159
| rowspan=3|<sup>255</sup>Md
| 260.10365(34)#
| rowspan=3 style="text-align:right" | 101
| 27.8(8) d
| rowspan=3 style="text-align:right" | 154
|
| rowspan=3|255.091083(7)
| rowspan=3|27(2) min
| β<sup>+</sup> (92%)
| <sup>255</sup>Fm
| rowspan=3|(7/2-)
|-
| α (8%)
| <sup>251</sup>Es
|-
| SF (.15%)
| (various)
|-
| rowspan=2|<sup>256</sup>Md
| rowspan=2 style="text-align:right" | 101
| rowspan=2 style="text-align:right" | 155
| rowspan=2|256.09406(6)
| rowspan=2|77(2) min
| β<sup>+</sup> (89%)
| <sup>256</sup>Fm
| rowspan=2|(1-)
|-
| α (11%)
| <sup>252</sup>Es
|-
| rowspan=3|<sup>257</sup>Md
| rowspan=3 style="text-align:right" | 101
| rowspan=3 style="text-align:right" | 156
| rowspan=3|257.095541(3)
| rowspan=3|5.52(5) h
| [[Electron capture|EC]] (84.8%)
| <sup>257</sup>Fm
| rowspan=3|(7/2-)
|-
| α (15.2%)
| <sup>253</sup>Es
|-
| SF (1%)
| (various)
|-
| rowspan=3|<sup>258</sup>Md
| rowspan=3 style="text-align:right" | 101
| rowspan=3 style="text-align:right" | 157
| rowspan=3|258.098431(5)
| rowspan=3|51.5(3) d
| α (99.99%)
| <sup>254</sup>Es
| rowspan=3|(8-)#
|-
| β<sup>-</sup> (.0015%)
| <sup>258</sup>No
|-
| β<sup>+</sup> (.0015%)
| <sup>258</sup>Fm
|-
| rowspan=4 style="text-indent:1em" | <sup>258m</sup>Md
| rowspan=4 colspan="3" style="text-indent:2em" | 0(200)# keV
| rowspan=4|57.0(9) min
| EC (70%)
| <sup>258</sup>Fm
| rowspan=4|1-#
|-
| SF (20%)
| (various)
|-
| β<sup>-</sup> (10%)
| <sup>258</sup>No
|-
| α (1.2%)
| <sup>254</sup>Es
|-
| rowspan=2|<sup>259</sup>Md
| rowspan=2 style="text-align:right" | 101
| rowspan=2 style="text-align:right" | 158
| rowspan=2|259.10051(22)#
| rowspan=2|1.60(6) h
| SF (98.7%)
| (various)
| rowspan=2|7/2-#
|-
| α (1.3%)
| <sup>255</sup>Es
|-
| rowspan=4|<sup>260</sup>Md<ref group="n">First isotope synthesized, also first isotope of any element to be produced one atom at a time</ref>
| rowspan=4 style="text-align:right" | 101
| rowspan=4 style="text-align:right" | 159
| rowspan=4|260.10365(34)#
| rowspan=4|27.8(8) d
| SF (85%)
| (various)
| rowspan=4|
|-
| α (5%)
| <sup>256</sup>Es
|-
| EC (5%)
| <sup>260</sup>Fm
|-
| β<sup>-</sup> (3.5%)
| <sup>260</sup>No
|-
|-
| <sup>261</sup>Md
| <sup>261</sup>Md
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| 261.10572(70)#
| 261.10572(70)#
| 40# min
| 40# min
|
|
| 7/2-#
| 7/2-#
|-
|-
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| 262.10887(63)#
| 262.10887(63)#
| 3# min
| 3# min
|
|
|
|
|}
|}

Revision as of 14:35, 22 May 2011

Mendelevium (Md) has no stable isotopes. There are 18 known radioisotopes, ranging in atomic mass from 245Md to 262Md, and 5 isomers. The isotope with the longest half-life is 258Md with a half-life of 51.3 days, and the longest-lived isomer is 258mMd with a half-life of 58.0 minutes. A standard atomic mass cannot be given due to mendelevium being artificial.

Table

nuclide
symbol
Z(p) N(n)  
isotopic mass (u)
 
half-life decay
mode(s)[1][n 1]
daughter
isotope(s)
nuclear
spin
excitation energy
245Md 101 144 245.08083(35)# 0.90(25) ms SF (various) (1/2-)#
α (rare) 241Es
245mMd 200(100)# keV 400(200) ms
[0.35(+23-16) s]
α 241Es (7/2+)
β+ (rare) 245Fm
246Md 101 145 246.08189(35)# 1.0(4) s α 242Es
β+ (rare) 246Fm
247Md 101 146 247.08164(35)# 1.12(22) s SF (various) 1/2-#
α (rare) 243Es
247mMd ~0.2 s α (99.99%) 243Es
SF (1E-4%) (various)
248Md 101 147 248.08282(26)# 7(3) s β+ (80%) 248Fm
α (20%) 244Es
β+, SF (.05%) (various)
249Md 101 148 249.08301(24)# 24(4) s α (60%) 245Es (7/2-)
β+ (40%) 249Fm
249mMd 100(100)# keV 1.9(9) s (1/2-)
250Md 101 149 250.08442(32)# 52(6) s β+ (93%) 250Fm
α (7%) 246Es
β+, SF (.02%) (various)
251Md 101 150 251.08484(22)# 4.0(5) min β+ (90%) 251Fm 7/2-#
α (10%) 247Es
252Md 101 151 252.08656(21)# 2.3(8) min β+ (50%) 252Fm
α (50%) 248Es
253Md 101 152 253.08728(22)# 12(8) min
[6(+12-3) min]
β+ 249Fm 7/2-#
α 249Es
254Md 101 153 254.08966(11)# 10(3) min β+ 254Fm (0-)
α (rare) 250Es
254mMd 50(100)# keV 28(8) min β+ 254Fm (3-)
α (rare) 250Es
255Md 101 154 255.091083(7) 27(2) min β+ (92%) 255Fm (7/2-)
α (8%) 251Es
SF (.15%) (various)
256Md 101 155 256.09406(6) 77(2) min β+ (89%) 256Fm (1-)
α (11%) 252Es
257Md 101 156 257.095541(3) 5.52(5) h EC (84.8%) 257Fm (7/2-)
α (15.2%) 253Es
SF (1%) (various)
258Md 101 157 258.098431(5) 51.5(3) d α (99.99%) 254Es (8-)#
β- (.0015%) 258No
β+ (.0015%) 258Fm
258mMd 0(200)# keV 57.0(9) min EC (70%) 258Fm 1-#
SF (20%) (various)
β- (10%) 258No
α (1.2%) 254Es
259Md 101 158 259.10051(22)# 1.60(6) h SF (98.7%) (various) 7/2-#
α (1.3%) 255Es
260Md[n 2] 101 159 260.10365(34)# 27.8(8) d SF (85%) (various)
α (5%) 256Es
EC (5%) 260Fm
β- (3.5%) 260No
261Md 101 160 261.10572(70)# 40# min 7/2-#
262Md 101 161 262.10887(63)# 3# min
  1. ^ Abbreviations:
    EC: Electron capture
    IT: Isomeric transition
    SF: Spontaneous fission
  2. ^ First isotope synthesized, also first isotope of any element to be produced one atom at a time

Notes

  • Values marked # are not purely derived from experimental data, but at least partly from systematic trends. Spins with weak assignment arguments are enclosed in parentheses.
  • Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values denote one standard deviation, except isotopic composition and standard atomic mass from IUPAC which use expanded uncertainties.

References

  • Isotope masses from:
    • G. Audi, A. H. Wapstra, C. Thibault, J. Blachot and O. Bersillon (2003). "The NUBASE evaluation of nuclear and decay properties" (PDF). Nuclear Physics A. 729: 3–128. doi:10.1016/j.nuclphysa.2003.11.001.{{cite journal}}: CS1 maint: multiple names: authors list (link)
  • Isotopic compositions and standard atomic masses from:
  • Half-life, spin, and isomer data selected from the following sources. See editing notes on this article's talk page.