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Isotopes of californium: Difference between revisions

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Table expanded with half-lives, spins, isomers
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== Table ==
== Table ==
{| class="wikitable" style="font-size:95%; white-space:nowrap"
{| border="1" cellspacing="0" cellpadding="2"
! rowspan="2" | nuclide<br />symbol
! style="width:8%" | Z([[proton|p]])
! style="width:8%" | N([[neutron|n]])
! Z([[proton|p]])
! N([[neutron|n]])
! style="width:25%" | isotopic mass (u)
! style="width:12%" | nuclide<br />symbol
! &nbsp;<br />isotopic mass (u)<br />&nbsp;
! rowspan="2" | half-life
! style="width:22%" | representative<br />isotopic<br />composition<br />(mole fraction)
! rowspan="2" | nuclear<br />spin
! style="width:25%" | range of natural<br />variation<br />(mole fraction)
! rowspan="2" | representative<br />isotopic<br />composition<br />(mole fraction)
! rowspan="2" | range of natural<br />variation<br />(mole fraction)
|-
|-
! colspan="3" | excitation energy
| style="text-align:right" | 98 || style="text-align:right" | 139 || 237.06207(54)#
| style="text-align:center" | Cf-237 || ||
|-
|-
| Cf-237
| style="text-align:right" | 98 || style="text-align:right" | 140 || 238.06141(43)#
| style="text-align:center" | Cf-238 || ||
| style="text-align:right" | 98
| style="text-align:right" | 139
| 237.06207(54)#
| 2.1(3) s
| 5/2+#
|
|
|-
|-
| Cf-238
| style="text-align:right" | 98 || style="text-align:right" | 141 || 239.06242(23)#
| style="text-align:center" | Cf-239 || ||
| style="text-align:right" | 98
| style="text-align:right" | 140
| 238.06141(43)#
| 21.1(13) ms
| 0+
|
|
|-
|-
| Cf-239
| style="text-align:right" | 98 || style="text-align:right" | 142 || 240.06230(22)#
| style="text-align:center" | Cf-240 || ||
| style="text-align:right" | 98
| style="text-align:right" | 141
| 239.06242(23)#
| 60(30) s [39(+37-12) s]
| 5/2+#
|
|
|-
|-
| Cf-240
| style="text-align:right" | 98 || style="text-align:right" | 143 || 241.06373(27)#
| style="text-align:center" | Cf-241 || ||
| style="text-align:right" | 98
| style="text-align:right" | 142
| 240.06230(22)#
| 1.06(15) min
| 0+
|
|
|-
|-
| Cf-241
| style="text-align:right" | 98 || style="text-align:right" | 144 || 242.06370(4)
| style="text-align:center" | Cf-242 || ||
| style="text-align:right" | 98
| style="text-align:right" | 143
| 241.06373(27)#
| 3.78(70) min
| 7/2-#
|
|
|-
|-
| Cf-242
| style="text-align:right" | 98 || style="text-align:right" | 145 || 243.06543(15)#
| style="text-align:center" | Cf-243 || ||
| style="text-align:right" | 98
| style="text-align:right" | 144
| 242.06370(4)
| 3.49(15) min
| 0+
|
|
|-
|-
| Cf-243
| style="text-align:right" | 98 || style="text-align:right" | 146 || 244.066001(3)
| style="text-align:center" | Cf-244 || ||
| style="text-align:right" | 98
| style="text-align:right" | 145
| 243.06543(15)#
| 10.7(5) min
| (1/2+)
|
|
|-
|-
| Cf-244
| style="text-align:right" | 98 || style="text-align:right" | 147 || 245.068049(3)
| style="text-align:center" | Cf-245 || ||
| style="text-align:right" | 98
| style="text-align:right" | 146
| 244.066001(3)
| 19.4(6) min
| 0+
|
|
|-
|-
| Cf-245
| style="text-align:right" | 98 || style="text-align:right" | 148 || 246.0688053(22)
| style="text-align:center" | Cf-246 || ||
| style="text-align:right" | 98
| style="text-align:right" | 147
| 245.068049(3)
| 45.0(15) min
| (5/2+)
|
|
|-
|-
| Cf-246
| style="text-align:right" | 98 || style="text-align:right" | 149 || 247.071001(9)
| style="text-align:center" | Cf-247 || ||
| style="text-align:right" | 98
| style="text-align:right" | 148
| 246.0688053(22)
| 35.7(5) h
| 0+
|
|
|-
|-
| Cf-247
| style="text-align:right" | 98 || style="text-align:right" | 150 || 248.072185(6)
| style="text-align:center" | Cf-248 || ||
| style="text-align:right" | 98
| style="text-align:right" | 149
| 247.071001(9)
| 3.11(3) h
| (7/2+)#
|
|
|-
|-
| Cf-248
| style="text-align:right" | 98 || style="text-align:right" | 151 || 249.0748535(24)
| style="text-align:center" | Cf-249 || ||
| style="text-align:right" | 98
| style="text-align:right" | 150
| 248.072185(6)
| 333.5(28) d
| 0+
|
|
|-
|-
| Cf-249
| style="text-align:right" | 98 || style="text-align:right" | 152 || 250.0764061(22)
| style="text-align:center" | Cf-250 || ||
| style="text-align:right" | 98
| style="text-align:right" | 151
| 249.0748535(24)
| 351(2) a
| 9/2-
|
|
|-
|-
| style="text-align:right" | 98 || style="text-align:right" | 153 || 251.079587(5)
| style="text-indent:1em" | Cf-249m
| style="text-align:center" | Cf-251 || ||
| colspan="3" style="text-indent:2em" | 144.98(5) keV
| 45(5) µs
| 5/2+
|
|
|-
|-
| Cf-250
| style="text-align:right" | 98 || style="text-align:right" | 154 || 252.081626(5)
| style="text-align:center" | Cf-252 || ||
| style="text-align:right" | 98
| style="text-align:right" | 152
| 250.0764061(22)
| 13.08(9) a
| 0+
|
|
|-
|-
| Cf-251
| style="text-align:right" | 98 || style="text-align:right" | 155 || 253.085133(7)
| style="text-align:center" | Cf-253 || ||
| style="text-align:right" | 98
| style="text-align:right" | 153
| 251.079587(5)
| 900(40) a
| 1/2+
|
|
|-
|-
| Cf-252
| style="text-align:right" | 98 || style="text-align:right" | 156 || 254.087323(13)
| style="text-align:center" | Cf-254 || ||
| style="text-align:right" | 98
| style="text-align:right" | 154
| 252.081626(5)
| 2.645(8) a
| 0+
|
|
|-
|-
| Cf-253
| style="text-align:right" | 98 || style="text-align:right" | 157 || 255.09105(22)#
| style="text-align:center" | Cf-255 || ||
| style="text-align:right" | 98
| style="text-align:right" | 155
| 253.085133(7)
| 17.81(8) d
| (7/2+)
|
|
|-
|-
| Cf-254
| style="text-align:right" | 98 || style="text-align:right" | 158 || 256.09344(32)#
| style="text-align:center" | Cf-256 || ||
| style="text-align:right" | 98
| style="text-align:right" | 156
| 254.087323(13)
| 60.5(2) d
| 0+
|
|
|-
| Cf-255
| style="text-align:right" | 98
| style="text-align:right" | 157
| 255.09105(22)#
| 85(18) min
| (7/2+)
|
|
|-
| Cf-256
| style="text-align:right" | 98
| style="text-align:right" | 158
| 256.09344(32)#
| 12.3(12) min
| 0+
|
|
|}
|}


=== Notes ===
=== Notes ===
* 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.
* Uncertainties are given in concise form in parentheses after the corresponding last digits. Uncertainty values from Ame2003 denote one standard deviation. Values from IUPAC are expanded uncertainties.
* 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 ==
== References ==
* 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).
* Isotopic compositions and standard atomic masses from [http://www.iupac.org/publications/pac/2003/pdf/7506x0683.pdf Atomic Weights of the Elements: Review 2000 (IUPAC Technical Report)]. ''Pure Appl. Chem.'', Vol. 75, No. 6, pp. 683-800, (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)].
* Half-life, spin, and isomer data selected from these sources. Editing notes on this article's talk page.
** 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).
** National Nuclear Data Center, Brookhaven National Laboratory. Information extracted from the [http://www.nndc.bnl.gov/nudat2/ 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.


{{Isotope nav | element=californium | lighter=Isotopes of berkelium | heavier=Isotopes of einsteinium }}
{{Isotope nav | element=californium | lighter=Isotopes of berkelium | heavier=Isotopes of einsteinium }}

----
<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>


[[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