Isotopes of californium#Californium-256
{{Short description|none}}
{{Infobox californium isotopes}}
Californium ({{sub|98}}Cf) is an artificial element, and thus a standard atomic weight cannot be given. Like all artificial elements, it has no stable isotopes. The first isotope to be synthesized was {{sup|245}}Cf in 1950. There are 20 known radioisotopes ranging from {{sup|237}}Cf to {{sup|256}}Cf and one nuclear isomer, {{sup|249m}}Cf. The longest-lived isotope is {{sup|251}}Cf with a half-life of 898 years.
List of isotopes
{{Isotopes table
|symbol=Cf
|refs=NUBASE2020, AME2020 II
|notes=m, unc(), mass#, spin(), spin#, SF, EC
}}
|-id=Californium-237
| rowspan=3|{{sup|237}}Cf
| rowspan=3 style="text-align:right" | 98
| rowspan=3 style="text-align:right" | 139
| rowspan=3|237.06220(10)
| rowspan=3|0.8(2) s
| α (70%)
| {{sup|233}}Cm
| rowspan=3|5/2+#
|-
| SF (30%)
| (various)
|-
| beta decay (rare)
| {{sup|237}}Bk
|-id=Californium-238
| rowspan=2|{{sup|238}}Cf
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 140
| rowspan=2|238.06149(32)#
| rowspan=2|21.1(13) ms
| SFLightest nuclide known to undergo spontaneous fission as its main decay mode
| (various)
| rowspan=2|0+
|-
| α (<5%)
| {{sup|234}}Cm
|-id=Californium-239
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 141
| rowspan=2|239.06248(13)#
| rowspan=2|28(2) s
| α (65%)
| {{sup|235}}Cm
| rowspan=2|(5/2+)
|-
| Beta decay (35%)
| {{sup|239}}Bk
|-id=Californium-240
| rowspan=3|{{sup|240}}Cf
| rowspan=3 style="text-align:right" | 98
| rowspan=3 style="text-align:right" | 142
| rowspan=3|240.062253(19)
| rowspan=3|40.3(9) s
| α (98.5%)
| {{sup|236}}Cm
| rowspan=3|0+
|-
| SF (1.5%)
| (various)
|-
| β{{sup|+}}?
| {{sup|240}}Bk
|-id=Californium-241
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 143
| rowspan=2|241.06369(18)#
| rowspan=2|2.35(18) min
| β{{sup|+}} (85%)
| {{sup|241}}Bk
| rowspan=2|(7/2−)
|-
| α (15%)
| {{sup|237}}Cm
|-id=Californium-242
| rowspan=3|{{sup|242}}Cf
| rowspan=3 style="text-align:right" | 98
| rowspan=3 style="text-align:right" | 144
| rowspan=3|242.063755(14)
| rowspan=3|3.49(15) min
| α (61%)
| {{sup|238}}Cm
| rowspan=3|0+
|-
| β{{sup|+}} (39%)
| {{sup|242}}Bk
|-
| SF (<0.014%)
| (various)
|-id=Californium-243
| rowspan=2|{{sup|243}}Cf
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 145
| rowspan=2|243.06548(19)#
| rowspan=2|10.8(3) min
| β{{sup|+}} (86%)
| {{sup|243}}Bk
| rowspan=2|(1/2+)
|-
| α (14%)
| {{sup|239}}Cm
|-id=Californium-244
| rowspan=2|{{sup|244}}Cf
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 146
| rowspan=2|244.0659994(28)
| rowspan=2|19.5(5) min
| α (75%)
| {{sup|240}}Cm
| rowspan=2|0+
|-
| EC (25%)
| {{sup|244}}Bk
|-id=Californium-245
| rowspan=2|{{sup|245}}Cf
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 147
| rowspan=2|245.0680468(26)
| rowspan=2|45.0(15) min
| β{{sup|+}} (64.7%)
| {{sup|245}}Bk
| rowspan=2|1/2+
|-
| α (35.3%)
| {{sup|241}}Cm
|-id=Californium-245m
| style="text-indent:1em" | {{sup|245m}}Cf
| colspan="3" style="text-indent:2em" | 57(4) keV
| >100# ns
| IT
| {{sup|245}}Cf
| (7/2+)
|-id=Californium-246
| rowspan=3|{{sup|246}}Cf
| rowspan=3 style="text-align:right" | 98
| rowspan=3 style="text-align:right" | 148
| rowspan=3|246.0688037(16)
| rowspan=3|35.7(5) h
| α
| {{sup|242}}Cm
| rowspan=3|0+
|-
| SF (2.4×10{{sup|−4}}%)
| (various)
|-
| EC?
| {{sup|246}}Bk
|-id=Californium-247
| rowspan=2|{{sup|247}}Cf
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 149
| rowspan=2|247.070971(15)
| rowspan=2|3.11(3) h
| EC (99.965%)
| {{sup|247}}Bk
| rowspan=2|(7/2+)
|-
| α (.035%)
| {{sup|243}}Cm
|-id=Californium-248
| rowspan=2|{{sup|248}}Cf
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 150
| rowspan=2|248.0721829(55)
| rowspan=2|333.5(28) d
| α (99.997%)
| {{sup|244}}Cm
| rowspan=2|0+
|-
| SF (.0029%)
| (various)
|-id=Californium-249
| rowspan=2|{{sup|249}}Cf
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 151
| rowspan=2|249.0748504(13)
| rowspan=2|351(2) y
| α
| {{sup|245}}Cm
| rowspan=2|9/2−
|-
| SF (5×10{{sup|−7}}%)
| (various)
|-id=Californium-249m
| style="text-indent:1em" | {{sup|249m}}Cf
| colspan="3" style="text-indent:2em" | 144.98(5) keV
| 45(5) μs
| IT
| {{sup|249}}Cf
| 5/2+
|-id=Californium-250
| rowspan=2|{{sup|250}}Cf
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 152
| rowspan=2|250.0764045(17)
| rowspan=2|13.08(9) y
| α (99.923%)
| {{sup|246}}Cm
| rowspan=2|0+
|-
| SF (.077%)
| (various)
|-id=Californium-251
| {{sup|251}}CfHigh neutron cross-section, tends to absorb neutrons
| style="text-align:right" | 98
| style="text-align:right" | 153
| 251.0795872(42)
| 898(44) y
| α
| {{sup|247}}Cm
| 1/2+
|-id=Californium-251m
| style="text-indent:1em" | {{sup|251m}}Cf
| colspan="3" style="text-indent:2em" | 370.47(3) keV
| 1.3(1) μs
| IT
| {{sup|251}}Cf
| 11/2−
|-
| rowspan=2|{{sup|252}}CfMost common isotope
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 154
| rowspan=2|252.0816265(25)
| rowspan=2|2.645(8) y
| α (96.8972%)
| {{sup|248}}Cm
| rowspan=2|0+
|-
| SF (3.1028%)High neutron emitter, average 3.7 neutrons per fission
| (various)
|-id=Californium-253
| rowspan=2|{{sup|253}}Cf
| rowspan=2 style="text-align:right" | 98
| rowspan=2 style="text-align:right" | 155
| rowspan=2|253.0851337(46)
| rowspan=2|17.81(8) d
| β{{sup|−}} (99.69%)
| {{sup|253}}Es
| rowspan=2|(7/2+)
|-
| α (.31%)
| {{sup|249}}Cm
|-id=Californium-254
| rowspan=3|{{sup|254}}Cf
| rowspan=3 style="text-align:right" | 98
| rowspan=3 style="text-align:right" | 156
| rowspan=3|254.087324(12)
| rowspan=3|60.5(2) d
| SF (99.69%)
| (various)
| rowspan=3|0+
|-
| α (.31%)
| {{sup|250}}Cm
|-
| {{sup|254}}Fm
|-id=Californium-255
| rowspan=3|{{sup|255}}Cf
| rowspan=3 style="text-align:right" | 98
| rowspan=3 style="text-align:right" | 157
| rowspan=3|255.09105(22)#
| rowspan=3|85(18) min
| β{{sup|−}}
| {{sup|255}}Es
| rowspan=3|(7/2+)
|-
| SF?
| (various)
|-
| α?
| {{sup|251}}Cm
|-id=Californium-256
| rowspan=3|{{sup|256}}Cf
| rowspan=3 style="text-align:right" | 98
| rowspan=3 style="text-align:right" | 158
| rowspan=3|256.09344(34)#
| rowspan=3|12.3(12) min
| SF
| (various)
| rowspan=3|0+
|-
| α?
| {{sup|252}}Cm
|-
| β{{sup|−}}β{{sup|−}}?
| {{sup|256}}Fm
|-
{{Isotopes table/footer}}
Actinides vs fission products
{{Actinidesvsfissionproducts}}
{{clear}}
Californium-252
Californium-252 (Cf-252, {{sup|252}}Cf) undergoes spontaneous fission with a branching ratio of 3.09% and is used in small neutron sources. Fission neutrons have an energy range of 0 to 13 MeV with a mean value of 2.3 MeV and a most probable value of 1 MeV.{{cite journal|title = Radiation Quality of Californium-252|journal = Physics in Medicine and Biology|first1 = J. F.|last1 = Dicello |last2=Gross |first2=W. |last3=Kraljevic |first3=U. |year = 1972 |doi= 10.1088/0031-9155/17/3/301 |volume=17 |issue= 3 |pages = 345–355|pmid = 5070445|bibcode = 1972PMB....17..345D | s2cid=250786668 }}
This isotope produces high neutron emissions and has a number of uses in industries such as nuclear energy, medicine, and petrochemical exploration.
= Nuclear reactors =
Californium-252 neutron sources are most notably used in the start-up of nuclear reactors. Once a reactor is filled with nuclear fuel, the stable neutron emission from said source starts the chain reaction.
= Military and defense =
The portable isotopic neutron spectroscopy (PINS) used by United States Armed Forces, the National Guard, Homeland Security, and Customs and Border Protection, uses {{sup|252}}Cf sources to detect hazardous contents inside artillery projectiles, mortar projectiles, rockets, bombs, land mines, and improvised explosive devices (IED).{{Cite web|title = Portable Isotopic Neutron Spectroscopy (PINS) for the Military|url = http://www.frontier-cf252.com/portable-isotopic-neutron-spectroscopy-military.html|website = Frontier Technology Corp.|access-date = 2016-02-24|archive-date = 2018-06-16|archive-url = https://web.archive.org/web/20180616132135/http://www.frontier-cf252.com/portable-isotopic-neutron-spectroscopy-military.html|url-status = dead}}{{Cite journal|title = Production, distribution and applications of californium-252 neutron sources|journal = Applied Radiation and Isotopes|date = 2000-11-01|issn = 0969-8043|pmid = 11003521|pages = 785–792|volume = 53|issue = 4–5|first1 = R. C.|last1 = Martin|first2 = J. B.|last2 = Knauer|first3 = P. A.|last3 = Balo|doi=10.1016/s0969-8043(00)00214-1|url = https://digital.library.unt.edu/ark:/67531/metadc623566/}}
= Oil and petroleum =
In the oil industry, {{sup|252}}Cf is used to find layers of petroleum and water in a well. Instrumentation is lowered into the well, which bombards the formation with high energy neutrons to determine porosity, permeability, and hydrocarbon presence along the length of the borehole.{{Cite web|title = Californium-252 & Antimony-Beryllium Sources|url = http://www.frontier-cf252.com|website = Frontier Technology Corp.|access-date = 2016-02-24}}
= Medicine =
Californium-252 has also been used in the treatment of serious forms of cancer. For certain types of brain and cervical cancer, {{sup|252}}Cf can be used as a more cost-effective substitute for radium.{{Cite journal|title = Five-year cure of cervical cancer treated using californium-252 neutron brachytherapy|journal = American Journal of Clinical Oncology|date = 1984-10-01|issn = 0277-3732|pmid = 6391143|pages = 487–493|volume = 7|issue = 5|first1 = Y.|last1 = Maruyama|first2 = J. R.|last2 = van Nagell|first3 = J.|last3 = Yoneda|first4 = E.|last4 = Donaldson|first5 = M.|last5 = Hanson|first6 = A.|last6 = Martin|first7 = L. C.|last7 = Wilson|first8 = C. W.|last8 = Coffey|first9 = J.|last9 = Feola|doi=10.1097/00000421-198410000-00018|s2cid = 12553815}}
References
{{Reflist}}
Sources
- {{cite book
| title = Handbook of Chemistry and Physics
| editor-first = David R.|editor-last = Lide
| edition = 87th
| date = 2006
| publisher = CRC Press, Taylor & Francis Group
| isbn = 978-0-8493-0487-3
| ref = {{sfnRef|CRC|2006}}
}}
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