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Isotopes of lawrencium: Difference between revisions

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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>SF: [[Spontaneous fission]]</ref>
! rowspan="2" | daughter<br>isotope(s)
! rowspan="2" | nuclear<br />spin
! rowspan="2" | nuclear<br />spin
|-
|-
Line 19: Line 21:
| -->
| -->
|-
|-
| <sup>252</sup>Lr
| rowspan=3|<sup>252</sup>Lr
| style="text-align:right" | 103
| rowspan=3 style="text-align:right" | 103
| style="text-align:right" | 149
| rowspan=3 style="text-align:right" | 149
| 252.09537(27)#
| rowspan=3|252.09537(27)#
| 390(90) ms<br>[0.36(+11-7) s]
| rowspan=3|390(90) ms<br>[0.36(+11-7) s]
| [[alpha decay|α]] (90%)
|
| <sup>248</sup>Md
| rowspan=3|
|-
|-
| <sup>253</sup>Lr
| [[beta decay|β<sup>+</sup>]] (10%)
| <sup>252</sup>No
| style="text-align:right" | 103
|-
| style="text-align:right" | 150
| [[Spontaneous fission|SF]] (1%)
| 253.09521(24)#
| (various)
| 580(70) ms<br>[0.57(+7-6) s]
| (7/2-)
|-
| rowspan=3|<sup>253</sup>Lr
| rowspan=3 style="text-align:right" | 103
| rowspan=3 style="text-align:right" | 150
| rowspan=3|253.09521(24)#
| rowspan=3|580(70) ms<br>[0.57(+7-6) s]
| α (90%)
| <sup>249</sup>Md
| rowspan=3|(7/2-)
|-
| SF (9%)
| (various)
|-
| β<sup>+</sup> (1%)
| <sup>253</sup>No
|-
|-
| style="text-indent:1em" | <sup>253m</sup>Lr
| style="text-indent:1em" | <sup>253m</sup>Lr
| colspan="3" style="text-indent:2em" | 30(100)# keV
| colspan="3" style="text-indent:2em" | 30(100)# keV
| 1.5(3) s<br>[1.5(+3-2) s]
| 1.5(3) s<br>[1.5(+3-2) s]
|
|
| (1/2-)
| (1/2-)
|-
|-
| <sup>254</sup>Lr
| rowspan=3|<sup>254</sup>Lr
| style="text-align:right" | 103
| rowspan=3 style="text-align:right" | 103
| style="text-align:right" | 151
| rowspan=3 style="text-align:right" | 151
| 254.09645(36)#
| rowspan=3|254.09645(36)#
| 13(3) s
| rowspan=3|13(3) s
| α (78%)
|
| <sup>250</sup>Md
| rowspan=3|
|-
|-
| <sup>255</sup>Lr
| β<sup>+</sup> (22%)
| <sup>254</sup>No
| style="text-align:right" | 103
| style="text-align:right" | 152
| 255.09668(22)#
| 22(4) s
| 7/2-#
|-
|-
| SF (.1%)
| <sup>256</sup>Lr
| (various)
| style="text-align:right" | 103
| style="text-align:right" | 153
| 256.09863(24)#
| 27(3) s
|
|-
|-
| <sup>257</sup>Lr
| rowspan=3|<sup>255</sup>Lr
| style="text-align:right" | 103
| rowspan=3 style="text-align:right" | 103
| style="text-align:right" | 154
| rowspan=3 style="text-align:right" | 152
| 257.09956(22)#
| rowspan=3|255.09668(22)#
| 646(25) ms
| rowspan=3|22(4) s
| α (69%)
| 9/2+#
| <sup>251</sup>Md
| rowspan=3|7/2-#
|-
|-
| <sup>258</sup>Lr<ref group="n">First isotope synthesized</ref>
| β<sup>+</sup> (30%)
| <sup>255</sup>No
| style="text-align:right" | 103
| style="text-align:right" | 155
| 258.10181(11)#
| 4.1(3) s
|
|-
|-
| SF (1%)
| <sup>259</sup>Lr
| (various)
| style="text-align:right" | 103
| style="text-align:right" | 156
| 259.10290(8)#
| 6.2(3) s
| 9/2+#
|-
|-
| <sup>260</sup>Lr
| rowspan=3|<sup>256</sup>Lr
| style="text-align:right" | 103
| rowspan=3 style="text-align:right" | 103
| style="text-align:right" | 157
| rowspan=3 style="text-align:right" | 153
| 260.10550(12)#
| rowspan=3|256.09863(24)#
| rowspan=3|27(3) s
| 2.7 min
| α (80%)
|
| <sup>252</sup>Md
| rowspan=3|
|-
|-
| <sup>261</sup>Lr
| β<sup>+</sup> (20%)
| <sup>256</sup>No
| style="text-align:right" | 103
| style="text-align:right" | 158
| 261.10688(22)#
| 44 min
|
|-
|-
| SF (.01%)
| <sup>262</sup>Lr
| (various)
| style="text-align:right" | 103
|-
| style="text-align:right" | 159
| rowspan=3|<sup>257</sup>Lr
| 262.10963(22)#
| rowspan=3 style="text-align:right" | 103
| 216 min
| rowspan=3 style="text-align:right" | 154
|
| rowspan=3|257.09956(22)#
| rowspan=3|646(25) ms
| α (99.99%)
| <sup>253</sup>Md
| rowspan=3|9/2+#
|-
| β<sup>+</sup> (.01%)
| <sup>257</sup>No
|-
| SF (.001%)
| (various)
|-
| rowspan=2|<sup>258</sup>Lr<ref group="n">First isotope synthesized</ref>
| rowspan=2 style="text-align:right" | 103
| rowspan=2 style="text-align:right" | 155
| rowspan=2|258.10181(11)#
| rowspan=2|4.1(3) s
| α (95%)
| <sup>254</sup>Md
| rowspan=2|
|-
| β<sup>+</sup> (5%)
| <sup>258</sup>No
|-
| rowspan=3|<sup>259</sup>Lr
| rowspan=3 style="text-align:right" | 103
| rowspan=3 style="text-align:right" | 156
| rowspan=3|259.10290(8)#
| rowspan=3|6.2(3) s
| α (77%)
| <sup>255</sup>Md
| rowspan=3|9/2+#
|-
| SF (23%)
| (various)
|-
| β<sup>+</sup> (.5%)
| <sup>259</sup>No
|-
| rowspan=3|<sup>260</sup>Lr
| rowspan=3 style="text-align:right" | 103
| rowspan=3 style="text-align:right" | 157
| rowspan=3|260.10550(12)#
| rowspan=3|2.7 min
| α (75%)
| <sup>256</sup>Md
| rowspan=3|
|-
| β<sup>+</sup> (15%)
| <sup>260</sup>No
|-
| SF (10%)
| (various)
|-
| rowspan=2|<sup>261</sup>Lr
| rowspan=2 style="text-align:right" | 103
| rowspan=2 style="text-align:right" | 158
| rowspan=2|261.10688(22)#
| rowspan=2|44 min
| SF
| (various)
| rowspan=2|
|-
| α (rare)
| <sup>257</sup>Md
|-
| rowspan=2|<sup>262</sup>Lr
| rowspan=2 style="text-align:right" | 103
| rowspan=2 style="text-align:right" | 159
| rowspan=2|262.10963(22)#
| rowspan=2|216 min
| β<sup>+</sup>
| <sup>262</sup>No
| rowspan=2|
|-
| α (rare)
| <sup>258</sup>Md
<!-- |-
<!-- |-
| <sup>263</sup>Lr
| <sup>263</sup>Lr

Revision as of 14:59, 22 May 2011

Lawrencium (Lr) has no stable isotopes. There are eleven known radioisotopes from 252Lr to 262Lr, and 1 isomer (253mLr). The isotope with the longest half-life is 262Lr with a half-life of 216 minutes. Heavier isotopes are expected to have longer half-lives. A standard atomic mass cannot be given as lawrencium is 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
252Lr 103 149 252.09537(27)# 390(90) ms
[0.36(+11-7) s]
α (90%) 248Md
β+ (10%) 252No
SF (1%) (various)
253Lr 103 150 253.09521(24)# 580(70) ms
[0.57(+7-6) s]
α (90%) 249Md (7/2-)
SF (9%) (various)
β+ (1%) 253No
253mLr 30(100)# keV 1.5(3) s
[1.5(+3-2) s]
(1/2-)
254Lr 103 151 254.09645(36)# 13(3) s α (78%) 250Md
β+ (22%) 254No
SF (.1%) (various)
255Lr 103 152 255.09668(22)# 22(4) s α (69%) 251Md 7/2-#
β+ (30%) 255No
SF (1%) (various)
256Lr 103 153 256.09863(24)# 27(3) s α (80%) 252Md
β+ (20%) 256No
SF (.01%) (various)
257Lr 103 154 257.09956(22)# 646(25) ms α (99.99%) 253Md 9/2+#
β+ (.01%) 257No
SF (.001%) (various)
258Lr[n 2] 103 155 258.10181(11)# 4.1(3) s α (95%) 254Md
β+ (5%) 258No
259Lr 103 156 259.10290(8)# 6.2(3) s α (77%) 255Md 9/2+#
SF (23%) (various)
β+ (.5%) 259No
260Lr 103 157 260.10550(12)# 2.7 min α (75%) 256Md
β+ (15%) 260No
SF (10%) (various)
261Lr 103 158 261.10688(22)# 44 min SF (various)
α (rare) 257Md
262Lr 103 159 262.10963(22)# 216 min β+ 262No
α (rare) 258Md
  1. ^ Abbreviations:
    SF: Spontaneous fission
  2. ^ First isotope synthesized

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.