Isotopes of californium: Difference between revisions
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Semi-stub with masses and abundances, part of Wikipedia:WikiProject Isotopes |
Table expanded with half-lives, spins, isomers |
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== Table == |
== Table == |
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{| class="wikitable" style="font-size:95%; white-space:nowrap" |
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{| border="1" cellspacing="0" cellpadding="2" |
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! rowspan="2" | nuclide<br />symbol |
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! style="width:8%" | Z([[proton|p]]) |
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! |
! Z([[proton|p]]) |
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! N([[neutron|n]]) |
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! style="width:25%" | isotopic mass (u) |
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! |
! <br />isotopic mass (u)<br /> |
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! rowspan="2" | half-life |
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! style="width:22%" | representative<br />isotopic<br />composition<br />(mole fraction) |
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! rowspan="2" | nuclear<br />spin |
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! style="width:25%" | range of natural<br />variation<br />(mole fraction) |
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! rowspan="2" | representative<br />isotopic<br />composition<br />(mole fraction) |
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! rowspan="2" | range of natural<br />variation<br />(mole fraction) |
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|- |
|- |
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! colspan="3" | excitation energy |
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| style="text-align:right" | 98 || style="text-align:right" | 139 || 237.06207(54)# |
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| style="text-align:center" | Cf-237 || || |
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|- |
|- |
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| Cf-237 |
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| style="text-align:right" | 98 || style="text-align:right" | 140 || 238.06141(43)# |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 139 |
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| 237.06207(54)# |
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| 2.1(3) s |
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| 5/2+# |
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| |
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| |
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|- |
|- |
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| Cf-238 |
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| style="text-align:right" | 98 || style="text-align:right" | 141 || 239.06242(23)# |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 140 |
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| 238.06141(43)# |
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| 21.1(13) ms |
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| 0+ |
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| |
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| |
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|- |
|- |
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| Cf-239 |
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| style="text-align:right" | 98 || style="text-align:right" | 142 || 240.06230(22)# |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 141 |
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| 239.06242(23)# |
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| 60(30) s [39(+37-12) s] |
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| 5/2+# |
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| |
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| |
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|- |
|- |
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| Cf-240 |
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| style="text-align:right" | 98 || style="text-align:right" | 143 || 241.06373(27)# |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 142 |
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| 240.06230(22)# |
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| 1.06(15) min |
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| 0+ |
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|- |
|- |
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| Cf-241 |
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| style="text-align:right" | 98 || style="text-align:right" | 144 || 242.06370(4) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 143 |
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| 241.06373(27)# |
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| 3.78(70) min |
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| 7/2-# |
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| |
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| |
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|- |
|- |
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| Cf-242 |
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| style="text-align:right" | 98 || style="text-align:right" | 145 || 243.06543(15)# |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 144 |
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| 242.06370(4) |
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| 3.49(15) min |
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| 0+ |
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| |
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| |
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|- |
|- |
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| Cf-243 |
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| style="text-align:right" | 98 || style="text-align:right" | 146 || 244.066001(3) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 145 |
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| 243.06543(15)# |
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| 10.7(5) min |
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| (1/2+) |
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| |
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| |
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|- |
|- |
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| Cf-244 |
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| style="text-align:right" | 98 || style="text-align:right" | 147 || 245.068049(3) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 146 |
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| 244.066001(3) |
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| 19.4(6) min |
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| 0+ |
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|- |
|- |
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| Cf-245 |
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| style="text-align:right" | 98 || style="text-align:right" | 148 || 246.0688053(22) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 147 |
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| 245.068049(3) |
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| 45.0(15) min |
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| (5/2+) |
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|- |
|- |
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| Cf-246 |
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| style="text-align:right" | 98 || style="text-align:right" | 149 || 247.071001(9) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 148 |
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| 246.0688053(22) |
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| 35.7(5) h |
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| 0+ |
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|- |
|- |
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| Cf-247 |
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| style="text-align:right" | 98 || style="text-align:right" | 150 || 248.072185(6) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 149 |
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| 247.071001(9) |
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| 3.11(3) h |
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| (7/2+)# |
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|- |
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| Cf-248 |
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| style="text-align:right" | 98 || style="text-align:right" | 151 || 249.0748535(24) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 150 |
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| 248.072185(6) |
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| 333.5(28) d |
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| 0+ |
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|- |
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| Cf-249 |
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| style="text-align:right" | 98 || style="text-align:right" | 152 || 250.0764061(22) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 151 |
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| 249.0748535(24) |
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| 351(2) a |
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| 9/2- |
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|- |
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| style="text- |
| style="text-indent:1em" | Cf-249m |
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| style="text- |
| colspan="3" style="text-indent:2em" | 144.98(5) keV |
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| 45(5) µs |
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| 5/2+ |
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|- |
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| Cf-250 |
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| style="text-align:right" | 98 || style="text-align:right" | 154 || 252.081626(5) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 152 |
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| 250.0764061(22) |
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| 13.08(9) a |
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| 0+ |
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|- |
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| Cf-251 |
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| style="text-align:right" | 98 || style="text-align:right" | 155 || 253.085133(7) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 153 |
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| 251.079587(5) |
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| 900(40) a |
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| 1/2+ |
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|- |
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| Cf-252 |
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| style="text-align:right" | 98 || style="text-align:right" | 156 || 254.087323(13) |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 154 |
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| 252.081626(5) |
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| 2.645(8) a |
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| 0+ |
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|- |
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| Cf-253 |
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| style="text-align:right" | 98 || style="text-align:right" | 157 || 255.09105(22)# |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 155 |
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| 253.085133(7) |
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| 17.81(8) d |
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| (7/2+) |
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|- |
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| Cf-254 |
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| style="text-align:right" | 98 || style="text-align:right" | 158 || 256.09344(32)# |
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| style="text-align: |
| style="text-align:right" | 98 |
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| style="text-align:right" | 156 |
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| 254.087323(13) |
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| 60.5(2) d |
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| 0+ |
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|- |
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| Cf-255 |
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| style="text-align:right" | 98 |
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| style="text-align:right" | 157 |
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| 255.09105(22)# |
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| 85(18) min |
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| (7/2+) |
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|- |
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| Cf-256 |
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| style="text-align:right" | 98 |
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| style="text-align:right" | 158 |
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| 256.09344(32)# |
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| 12.3(12) min |
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| 0+ |
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=== Notes === |
=== Notes === |
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* Values marked # are not purely derived from experimental data, but at least partly from systematic trends. |
* 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. |
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* Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values |
* 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. |
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== References == |
== References == |
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* Isotope masses from [http://www.nndc.bnl.gov/amdc/index.html Ame2003 Atomic Mass Evaluation] by G. Audi, A.H. Wapstra, C. Thibault, J. Blachot and O. Bersillon in ''Nuclear Physics'' A729 (2003). |
* Isotope masses from [http://www.nndc.bnl.gov/amdc/index.html Ame2003 Atomic Mass Evaluation] by G. Audi, A.H. Wapstra, C. Thibault, J. Blachot and O. Bersillon in ''Nuclear Physics'' A729 (2003). |
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* Isotopic compositions and standard atomic masses from [http://www.iupac.org/publications/pac/2003/ |
* Isotopic compositions and standard atomic masses from [http://www.iupac.org/publications/pac/2003/7506/7506x0683.html Atomic weights of the elements. Review 2000 (IUPAC Technical Report)]. ''Pure Appl. Chem.'' Vol. 75, No. 6, pp. 683-800, (2003) and [http://www.iupac.org/news/archives/2005/atomic-weights_revised05.html Atomic Weights Revised (2005)]. |
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* Half-life, spin, and isomer data selected from these sources. Editing notes on this article's talk page. |
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** Audi, Bersillon, Blachot, Wapstra. [http://amdc.in2p3.fr/web/nubase_en.html The Nubase2003 evaluation of nuclear and decay properties], Nuc. Phys. A 729, pp. 3-128 (2003). |
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** National Nuclear Data Center, Brookhaven National Laboratory. Information extracted from the [http://www.nndc.bnl.gov/nudat2/ NuDat 2.1 database] (retrieved Sept. 2005). |
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** David R. Lide (ed.), Norman E. Holden in ''CRC Handbook of Chemistry and Physics, 85th Edition'', online version. CRC Press. Boca Raton, Florida (2005). Section 11, Table of the Isotopes. |
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{{Isotope nav | element=californium | lighter=Isotopes of berkelium | heavier=Isotopes of einsteinium }} |
{{Isotope nav | element=californium | lighter=Isotopes of berkelium | heavier=Isotopes of einsteinium }} |
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---- |
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<div class="boilerplate" id="stub">''This article is a [[Wikipedia:Stub|stub]] with no decay data yet. You can help define a format at [[Wikipedia:WikiProject Isotopes]].''</div> |
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[[Category:Isotopes]] |
[[Category:Isotopes]] |
Revision as of 11:31, 17 November 2005
Californium (Cf)
Has no stable isotopes. A standard atomic mass cannot be given.
Table
nuclide symbol |
Z(p) | N(n) | isotopic mass (u) |
half-life | nuclear spin |
representative isotopic composition (mole fraction) |
range of natural variation (mole fraction) |
---|---|---|---|---|---|---|---|
excitation energy | |||||||
Cf-237 | 98 | 139 | 237.06207(54)# | 2.1(3) s | 5/2+# | ||
Cf-238 | 98 | 140 | 238.06141(43)# | 21.1(13) ms | 0+ | ||
Cf-239 | 98 | 141 | 239.06242(23)# | 60(30) s [39(+37-12) s] | 5/2+# | ||
Cf-240 | 98 | 142 | 240.06230(22)# | 1.06(15) min | 0+ | ||
Cf-241 | 98 | 143 | 241.06373(27)# | 3.78(70) min | 7/2-# | ||
Cf-242 | 98 | 144 | 242.06370(4) | 3.49(15) min | 0+ | ||
Cf-243 | 98 | 145 | 243.06543(15)# | 10.7(5) min | (1/2+) | ||
Cf-244 | 98 | 146 | 244.066001(3) | 19.4(6) min | 0+ | ||
Cf-245 | 98 | 147 | 245.068049(3) | 45.0(15) min | (5/2+) | ||
Cf-246 | 98 | 148 | 246.0688053(22) | 35.7(5) h | 0+ | ||
Cf-247 | 98 | 149 | 247.071001(9) | 3.11(3) h | (7/2+)# | ||
Cf-248 | 98 | 150 | 248.072185(6) | 333.5(28) d | 0+ | ||
Cf-249 | 98 | 151 | 249.0748535(24) | 351(2) a | 9/2- | ||
Cf-249m | 144.98(5) keV | 45(5) µs | 5/2+ | ||||
Cf-250 | 98 | 152 | 250.0764061(22) | 13.08(9) a | 0+ | ||
Cf-251 | 98 | 153 | 251.079587(5) | 900(40) a | 1/2+ | ||
Cf-252 | 98 | 154 | 252.081626(5) | 2.645(8) a | 0+ | ||
Cf-253 | 98 | 155 | 253.085133(7) | 17.81(8) d | (7/2+) | ||
Cf-254 | 98 | 156 | 254.087323(13) | 60.5(2) d | 0+ | ||
Cf-255 | 98 | 157 | 255.09105(22)# | 85(18) min | (7/2+) | ||
Cf-256 | 98 | 158 | 256.09344(32)# | 12.3(12) min | 0+ |
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 Ame2003 Atomic Mass Evaluation by G. Audi, A.H. Wapstra, C. Thibault, J. Blachot and O. Bersillon in Nuclear Physics A729 (2003).
- Isotopic compositions and standard atomic masses from Atomic weights of the elements. Review 2000 (IUPAC Technical Report). Pure Appl. Chem. Vol. 75, No. 6, pp. 683-800, (2003) and Atomic Weights Revised (2005).
- Half-life, spin, and isomer data selected from these sources. Editing notes on this article's talk page.
- Audi, Bersillon, Blachot, Wapstra. The Nubase2003 evaluation of nuclear and decay properties, Nuc. Phys. A 729, pp. 3-128 (2003).
- National Nuclear Data Center, Brookhaven National Laboratory. Information extracted from the NuDat 2.1 database (retrieved Sept. 2005).
- David R. Lide (ed.), Norman E. Holden in CRC Handbook of Chemistry and Physics, 85th Edition, online version. CRC Press. Boca Raton, Florida (2005). Section 11, Table of the Isotopes.