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Naturally occurring cerium (58Ce) is composed of 4 stable isotopes: 136Ce, 138Ce, 140Ce, and 142Ce, with 140Ce being the most abundant (88.48% natural abundance) and the only one theoretically stable; 136Ce, 138Ce, and 142Ce are predicted to undergo double beta decay but this process has never been observed. There are 35 radioisotopes that have been characterized, with the most stable being 144Ce, with a half-life of 284.893 days; 139Ce, with a half-life of 137.640 days and 141Ce, with a half-life of 32.501 days. All of the remaining radioactive isotopes have half-lives that are less than 4 days and the majority of these have half-lives that are less than 10 minutes. This element also has 10 meta states. The isotopes of cerium range in atomic weight from 119 u (119Ce) to 157 u (157Ce).


List of isotopes

, - , 119Ce , style="text-align:right" , 58 , style="text-align:right" , 61 , 118.95276(64)# , 200# ms , β+ , 119La , 5/2+# , , , - , 120Ce , style="text-align:right" , 58 , style="text-align:right" , 62 , 119.94664(75)# , 250# ms , β+ , 120La , 0+ , , , - , 121Ce , style="text-align:right" , 58 , style="text-align:right" , 63 , 120.94342(54)# , 1.1(1) s , β+ , 121La , (5/2)(+#) , , , - , rowspan=2, 122Ce , rowspan=2 style="text-align:right" , 58 , rowspan=2 style="text-align:right" , 64 , rowspan=2, 121.93791(43)# , rowspan=2, 2# s , β+ , 122La , rowspan=2, 0+ , rowspan=2, , rowspan=2, , - , β+, p , 121Ba , - , rowspan=2, 123Ce , rowspan=2 style="text-align:right" , 58 , rowspan=2 style="text-align:right" , 65 , rowspan=2, 122.93540(32)# , rowspan=2, 3.8(2) s , β+ , 123La , rowspan=2, (5/2)(+#) , rowspan=2, , rowspan=2, , - , β+, p , 122Ba , - , 124Ce , style="text-align:right" , 58 , style="text-align:right" , 66 , 123.93041(32)# , 9.1(12) s , β+ , 124La , 0+ , , , - , rowspan=2, 125Ce , rowspan=2 style="text-align:right" , 58 , rowspan=2 style="text-align:right" , 67 , rowspan=2, 124.92844(21)# , rowspan=2, 9.3(3) s , β+ , 125La , rowspan=2, (7/2−) , rowspan=2, , rowspan=2, , - , β+, p , 124Ba , - , 126Ce , style="text-align:right" , 58 , style="text-align:right" , 68 , 125.92397(3) , 51.0(3) s , β+ , 126La , 0+ , , , - , 127Ce , style="text-align:right" , 58 , style="text-align:right" , 69 , 126.92273(6) , 29(2) s , β+ , 127La , 5/2+# , , , - , 128Ce , style="text-align:right" , 58 , style="text-align:right" , 70 , 127.91891(3) , 3.93(2) min , β+ , 128La , 0+ , , , - , 129Ce , style="text-align:right" , 58 , style="text-align:right" , 71 , 128.91810(3) , 3.5(3) min , β+ , 129La , (5/2+) , , , - , 130Ce , style="text-align:right" , 58 , style="text-align:right" , 72 , 129.91474(3) , 22.9(5) min , β+ , 130La , 0+ , , , - , style="text-indent:1em" , 130mCe , colspan="3" style="text-indent:2em" , 2453.6(3) keV , 100(8) ns , , , (7−) , , , - , 131Ce , style="text-align:right" , 58 , style="text-align:right" , 73 , 130.91442(4) , 10.2(3) min , β+ , 131La , (7/2+) , , , - , style="text-indent:1em" , 131mCe , colspan="3" style="text-indent:2em" , 61.8(1) keV , 5.0(10) min , β+ , 131La , (1/2+) , , , - , 132Ce , style="text-align:right" , 58 , style="text-align:right" , 74 , 131.911460(22) , 3.51(11) h , β+ , 132La , 0+ , , , - , style="text-indent:1em" , 132mCe , colspan="3" style="text-indent:2em" , 2340.8(5) keV , 9.4(3) ms , IT , 132Ce , (8−) , , , - , 133Ce , style="text-align:right" , 58 , style="text-align:right" , 75 , 132.911515(18) , 97(4) min , β+ , 133La , 1/2+ , , , - , style="text-indent:1em" , 133mCe , colspan="3" style="text-indent:2em" , 37.1(8) keV , 4.9(4) d , β+ , 133La , 9/2− , , , - , 134Ce , style="text-align:right" , 58 , style="text-align:right" , 76 , 133.908925(22) , 3.16(4) d , EC , 134La , 0+ , , , - , 135Ce , style="text-align:right" , 58 , style="text-align:right" , 77 , 134.909151(12) , 17.7(3) h , β+ , 135La , 1/2(+) , , , - , style="text-indent:1em" , 135mCe , colspan="3" style="text-indent:2em" , 445.8(2) keV , 20(1) s , IT , 135Ce , (11/2−) , , , - , 136Ce , style="text-align:right" , 58 , style="text-align:right" , 78 , 135.907172(14) , colspan=3 align=center, Observationally StableTheorized to undergo β+β+ decay to 136Ba with a half-life over 38×1015 years , 0+ , 0.00185(2) , 0.00185–0.00186 , - , style="text-indent:1em" , 136mCe , colspan="3" style="text-indent:2em" , 3095.5(4) keV , 2.2(2) µs , , , 10+ , , , - , 137Ce , style="text-align:right" , 58 , style="text-align:right" , 79 , 136.907806(14) , 9.0(3) h , β+ , 137La , 3/2+ , , , - , rowspan=2 style="text-indent:1em" , 137mCe , rowspan=2 colspan="3" style="text-indent:2em" , 254.29(5) keV , rowspan=2, 34.4(3) h , IT (99.22%) , 137Ce , rowspan=2, 11/2− , rowspan=2, , rowspan=2, , - , β+ (.779%) , 137La , - , 138Ce , style="text-align:right" , 58 , style="text-align:right" , 80 , 137.905991(11) , colspan=3 align=center, Observationally StableTheorized to undergo β+β+ decay to 138Ba with a half-life over 150×1012 years , 0+ , 0.00251(2) , 0.00251–0.00254 , - , style="text-indent:1em" , 138mCe , colspan="3" style="text-indent:2em" , 2129.17(12) keV , 8.65(20) ms , IT , 138Ce , 7- , , , - , 139Ce , style="text-align:right" , 58 , style="text-align:right" , 81 , 138.906653(8) , 137.641(20) d , EC , 139La , 3/2+ , , , - , style="text-indent:1em" , 139mCe , colspan="3" style="text-indent:2em" , 754.24(8) keV , 56.54(13) s , IT , 139Ce , 11/2− , , , - , 140Ce
Fission product Nuclear fission products are the atomic fragments left after a large atomic nucleus undergoes nuclear fission. Typically, a large nucleus like that of uranium fissions by splitting into two smaller nuclei, along with a few neutrons, the release ...
, style="text-align:right" , 58 , style="text-align:right" , 82 , 139.9054387(26) , colspan=3 align=center, StableTheoretically capable of
spontaneous fission Spontaneous fission (SF) is a form of radioactive decay that is found only in very heavy chemical elements. The nuclear binding energy of the elements reaches its maximum at an atomic mass number of about 56 (e.g., iron-56); spontaneous breakdo ...
, 0+ , 0.88450(51) , 0.88446–0.88449 , - , style="text-indent:1em" , 140mCe , colspan="3" style="text-indent:2em" , 2107.85(3) keV , 7.3(15) µs , , , 6+ , , , - , 141Ce , style="text-align:right" , 58 , style="text-align:right" , 83 , 140.9082763(26) , 32.508(13) d , β , 141Pr , 7/2− , , , - , 142Ce , style="text-align:right" , 58 , style="text-align:right" , 84 , 141.909244(3) , colspan=3 align=center, Observationally Stable , 0+ , 0.11114(51) , 0.11114–0.11114 , - , 143Ce , style="text-align:right" , 58 , style="text-align:right" , 85 , 142.912386(3) , 33.039(6) h , β , 143Pr , 3/2− , , , - , 144Ce , style="text-align:right" , 58 , style="text-align:right" , 86 , 143.913647(4) , 284.91(5) d , β , 144mPr , 0+ , , , - , 145Ce , style="text-align:right" , 58 , style="text-align:right" , 87 , 144.91723(4) , 3.01(6) min , β , 145Pr , (3/2−) , , , - , 146Ce , style="text-align:right" , 58 , style="text-align:right" , 88 , 145.91876(7) , 13.52(13) min , β , 146Pr , 0+ , , , - , 147Ce , style="text-align:right" , 58 , style="text-align:right" , 89 , 146.92267(3) , 56.4(10) s , β , 147Pr , (5/2−) , , , - , 148Ce , style="text-align:right" , 58 , style="text-align:right" , 90 , 147.92443(3) , 56(1) s , β , 148Pr , 0+ , , , - , 149Ce , style="text-align:right" , 58 , style="text-align:right" , 91 , 148.9284(1) , 5.3(2) s , β , 149Pr , (3/2−)# , , , - , 150Ce , style="text-align:right" , 58 , style="text-align:right" , 92 , 149.93041(5) , 4.0(6) s , β , 150Pr , 0+ , , , - , 151Ce , style="text-align:right" , 58 , style="text-align:right" , 93 , 150.93398(11) , 1.02(6) s , β , 151Pr , 3/2−# , , , - , 152Ce , style="text-align:right" , 58 , style="text-align:right" , 94 , 151.93654(21)# , 1.4(2) s , β , 152Pr , 0+ , , , - , 153Ce , style="text-align:right" , 58 , style="text-align:right" , 95 , 152.94058(43)# , 500# ms 300 ns, β , 153Pr , 3/2−# , , , - , 154Ce , style="text-align:right" , 58 , style="text-align:right" , 96 , 153.94342(54)# , 300# ms 300 ns, β , 154Pr , 0+ , , , - , 155Ce , style="text-align:right" , 58 , style="text-align:right" , 97 , 154.94804(64)# , 200# ms 300 ns, β , 155Pr , 5/2−# , , , - , 156Ce , style="text-align:right" , 58 , style="text-align:right" , 98 , 155.95126(64)# , 150# ms , β , 156Pr , 0+ , , , - , 157Ce , style="text-align:right" , 58 , style="text-align:right" , 99 , 156.95634(75)# , 50# ms , β , 157Pr , 7/2+# , ,


References

* Isotope masses from: ** * Isotopic compositions and standard atomic masses from: ** ** * Half-life, spin, and isomer data selected from the following sources. ** ** ** {{Authority control Cerium Cerium