Physics:Isotopes of cadmium
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| Standard atomic weight Ar, standard(Cd) |
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Naturally occurring cadmium (
48Cd) is composed of 8 isotopes. For two of them, natural radioactivity has been observed, and three others are predicted to possibly decay though this has not been observed; it may be presumed the half-lives are extremely long. The two natural radioactive isotopes are 113
Cd (beta decay, half-life 8.04×1015 years) and 116
Cd (double beta decay, half-life 2.69×1019 years). The other three are 106
Cd, 108
Cd (double electron capture), and 114
Cd (double beta decay); only lower limits on their decays have been set. Only three isotopes—110
Cd, 111
Cd, and 112
Cd—are theoretically stable. Among the isotopes absent in natural cadmium, the most long-lived are 109
Cd with a half-life of 461.3 days, and 115
Cd with a half-life of 53.46 hours. All of the remaining radioactive isotopes have half-lives that are less than 7 hours and the majority of these are less than 5 minutes. This element also has 12 known meta states, with the most stable being 113m
Cd (Template:T-half 13.9 years), 115m
Cd (Template:T-half 44.6 days) and 117m
Cd (Template:T-half 3.44 hours).
The known isotopes of cadmium range from 95
Cd to 132
Cd. The primary decay mode before the stable isotope 112
Cd is electron capture to isotopes of silver, and after, beta emission to isotopes of indium.
A 2021 study has shown at high ionic strengths, cadmium isotope fractionation mainly depends on its complexation with carboxylic sites. At low ionic strengths, nonspecific cadmium binding induced by electrostatic attractions plays a dominant role and promotes cadmium isotope fractionation during complexation.[2]
List of isotopes
| Nuclide [n 1] |
Z | N | Isotopic mass (u) [n 2][n 3] |
Half-life [n 4] |
Decay mode [n 5] |
Daughter isotope [n 6][n 7] |
Spin and parity [n 8][n 9] |
Physics:Natural abundance (mole fraction) | |
|---|---|---|---|---|---|---|---|---|---|
| Excitation energy[n 9] | Normal proportion | Range of variation | |||||||
| 94 Cd |
48 | 46 | 93.95659(54)# | 80# ms [> 760 ns] |
0+ | ||||
| 95 Cd |
48 | 47 | 94.94948(61)# | 32(3) ms | β+ (95.4%) | 95 Ag |
9/2+# | ||
| β+, p (4.6%) | 94 Pd | ||||||||
| 96 Cd |
48 | 48 | 95.94034(44)# | 1.003(47) s | β+ (98.4%) | 96 Ag |
0+ | ||
| β+, p (1.6%) | 95 Pd | ||||||||
| 96m1 Cd |
6000(1400) keV | 511(26) ms | β+ (84.6%) | 96 Ag |
16+ | ||||
| β+, p (15.4%) | 95 Pd | ||||||||
| 96m2 Cd |
5605(5) keV | 198(18) ns | IT | 96 Cd |
(12−,13−) | ||||
| 97 Cd |
48 | 49 | 96.93480(45) | 1.16(5) s | β+ (92.6%) | 97 Ag |
(9/2+) | ||
| β+, p (7.4%) | 96 Pd | ||||||||
| 97m1 Cd |
1245.1(2) keV | 730(70) μs | IT | 97 Cd |
(1/2−) | ||||
| 97m2 Cd |
2620(580) keV | 3.86(6) s | β+ (74.9%) | 97 Ag |
(25/2+) | ||||
| β+, p (25.1%) | 96 Pd | ||||||||
| 98 Cd |
48 | 50 | 97.927389(56) | 9.29(10) s | β+ (>99.97%) | 98 Ag |
0+ | ||
| β+, p (<0.029%) | 97 Pd | ||||||||
| 98m1 Cd |
2428.3(4) keV | 154(16) ns | IT | 98 Cd |
(8+) | ||||
| 98m2 Cd |
6635(2) keV | 224(5) ns | IT | 98 Cd |
(12+) | ||||
| 99 Cd |
48 | 51 | 98.9249258(17) | 17(1) s | β+ (99.79%) | 99 Ag |
5/2+# | ||
| β+, p (0.21%) | 98 Pd | ||||||||
| β+, α (<10−4%) | 95 Rh | ||||||||
| 100 Cd |
48 | 52 | 99.9203488(18) | 49.1(5) s | β+ | 100 Ag |
0+ | ||
| 101 Cd |
48 | 53 | 100.9185862(16) | 1.36(5) min | β+ | 101 Ag |
5/2+ | ||
| 102 Cd |
48 | 54 | 101.9144818(18) | 5.5(5) min | β+ | 102 Ag |
0+ | ||
| 103 Cd |
48 | 55 | 102.9134169(19) | 7.3(1) min | β+ | 103 Ag |
5/2+ | ||
| 104 Cd |
48 | 56 | 103.9098562(18) | 57.7(10) min | β+ | 104 Ag |
0+ | ||
| 105 Cd |
48 | 57 | 104.9094639(15) | 55.5(4) min | β+ | 105 Ag |
5/2+ | ||
| 105m Cd |
2517.6(5) keV | 4.5(5) μs | IT | 105 Cd |
(21/2+) | ||||
| 106 Cd |
48 | 58 | 105.9064598(12) | Observationally stable[n 10] | 0+ | 0.01245(22) | |||
| 107 Cd |
48 | 59 | 106.9066120(18) | 6.50(2) h | β+ | 107 Ag |
5/2+ | ||
| 108 Cd |
48 | 60 | 107.9041836(12) | Observationally stable[n 11] | 0+ | 0.00888(11) | |||
| 109 Cd |
48 | 61 | 108.9049867(16) | 461.3(5) d | EC | 109 Ag |
5/2+ | ||
| 109m1 Cd |
59.60(7) keV | 11.8(16) μs | IT | 109 Cd |
1/2+ | ||||
| 109m2 Cd |
463.10(11) keV | 10.6(4) μs | IT | 109 Cd |
11/2− | ||||
| 110 Cd |
48 | 62 | 109.90300747(41) | Stable | 0+ | 0.12470(61) | |||
| 111 Cd[n 12] |
48 | 63 | 110.90418378(38) | Stable | 1/2+ | 0.12795(12) | |||
| 111m Cd |
396.214(21) keV | 48.50(9) min | IT | 111 Cd |
11/2− | ||||
| 112 Cd[n 12] |
48 | 64 | 111.90276390(27) | Stable | 0+ | 0.24109(7) | |||
| 113 Cd[n 12][n 13] |
48 | 65 | 112.90440811(26) | 8.04(5)×1015 y | β− | 113 In |
1/2+ | 0.12227(7) | |
| 113m Cd[n 12] |
263.54(3) keV | 13.89(11) y | β− (99.90%) | 113 In |
11/2− | ||||
| IT (0.0964%) | 113 Cd | ||||||||
| 114 Cd[n 12] |
48 | 66 | 113.90336500(30) | Observationally stable[n 14] | 0+ | 0.28754(81) | |||
| 115 Cd[n 12] |
48 | 67 | 114.90543743(70) | 53.46(5) h | β− | 115m In |
1/2+ | ||
| 115m Cd[n 12] |
181.0(5) keV | 44.56(24) d | β− | 115 In |
11/2− | ||||
| 116 Cd[n 12][n 13] |
48 | 68 | 115.90476323(17) | 2.69(9)×1019 y | β−β− | 116 Sn |
0+ | 0.07512(54) | |
| 117 Cd |
48 | 69 | 116.9072260(11) | 2.503(5) h | β− | 117 In |
1/2+ | ||
| 117m Cd |
136.4(2) keV | 3.441(9) h | β− | 117 In |
11/2− | ||||
| 118 Cd |
48 | 70 | 117.906922(21) | 50.3(2) min | β− | 118 In |
0+ | ||
| 119 Cd |
48 | 71 | 118.909847(40) | 2.69(2) min | β− | 119 In |
1/2+ | ||
| 119m Cd |
146.54(11) keV | 2.20(2) min | β− | 119 In |
11/2− | ||||
| 120 Cd |
48 | 72 | 119.9098681(40) | 50.80(21) s | β− | 120 In |
0+ | ||
| 121 Cd |
48 | 73 | 120.9129637(21) | 13.5(3) s | β− | 121 In |
3/2+ | ||
| 121m Cd |
214.86(15) keV | 8.3(8) s | β− | 121 In |
11/2− | ||||
| 122 Cd |
48 | 74 | 121.9134591(25) | 5.98(10) s[3] | β− | 122 In |
0+ | ||
| 123 Cd |
48 | 75 | 122.9168925(29) | 2.10(2) s | β− | 123 In |
3/2+ | ||
| 123m Cd |
143(4) keV | 1.82(3) s | β− (?%) | 123 In |
11/2− | ||||
| IT (?%) | 123 Cd | ||||||||
| 124 Cd |
48 | 76 | 123.9176598(28) | 1.25(2) s | β− | 124 In |
0+ | ||
| 125 Cd |
48 | 77 | 124.9212576(31) | 680(40) ms | β− | 125 In |
3/2+ | ||
| 125m1 Cd |
186(4) keV | 480(30) ms | β− | 125 In |
11/2− | ||||
| 125m2 Cd |
1648(4) keV | 19(3) μs | IT | 125 Cd |
(19/2+) | ||||
| 126 Cd |
48 | 78 | 125.9224303(25) | 512(5) ms | β− | 126 In |
0+ | ||
| 127 Cd |
48 | 79 | 126.9262033(67) | 480(100) ms | β− | 127 In |
3/2+ | ||
| 127m1 Cd |
285(8) keV | 360(40) ms | β− | 127 In |
11/2− | ||||
| 127m2 Cd |
1845(8) keV | 17.5(3) μs | IT | 127 Cd |
(19/2+) | ||||
| 128 Cd |
48 | 80 | 127.9278168(69) | 246(2) ms | β− | 128 In |
0+ | ||
| 128m1 Cd |
1870.5(3) keV | 270(7) ns | IT | 128 Cd |
(5−) | ||||
| 128m2 Cd |
2714.6(4) keV | 3.56(6) μs | IT | 128 Cd |
(10+) | ||||
| 128m3 Cd |
4286.6(15) keV | 6.3(8) ms | IT | 128 Cd |
(15−) | ||||
| 129 Cd |
48 | 81 | 128.9322356(57) | 147(3) ms | β− (?%) | 129 In |
11/2− | ||
| β−, n (?%) | 128 In | ||||||||
| 129m1 Cd |
343(8) keV | 157(8) ms | β− (?%) | 129 In |
3/2+ | ||||
| β−, n (?%) | 128 In | ||||||||
| 129m2 Cd |
2283(8) keV | 3.6(2) ms | IT | 129 Cd |
(21/2+) | ||||
| 130 Cd |
48 | 82 | 129.934388(24) | 126.8(18) ms | β− (96.5%) | 130 In |
0+ | ||
| β−, n (3.5%) | 129 In | ||||||||
| 130m Cd |
2129.6(10) keV | 240(16) ns | IT | 130 Cd |
(8+) | ||||
| 131 Cd |
48 | 83 | 130.940728(21) | 98(2) ms | β− (96.5%) | 131 In |
7/2−# | ||
| β−, n (3.5%) | 130 In | ||||||||
| 132 Cd |
48 | 84 | 131.945823(64) | 84(5) ms | β−, n (60%) | 131 In |
0+ | ||
| β− (40%) | 132 In | ||||||||
| 133 Cd |
48 | 85 | 132.95261(22)# | 61(6) ms | β− (?%) | 133 In |
7/2−# | ||
| β−, n (?%) | 132 In | ||||||||
| 134 Cd |
48 | 86 | 133.95764(32)# | 65(15) ms | β− | 134 In |
0+ | ||
- ↑ mCd – Excited nuclear isomer.
- ↑ ( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
- ↑ # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
- ↑ Bold half-life – nearly stable, half-life longer than age of universe.
- ↑
Modes of decay:
EC: Electron capture IT: Isomeric transition n: Neutron emission p: Proton emission - ↑ Bold italics symbol as daughter – Daughter product is nearly stable.
- ↑ Bold symbol as daughter – Daughter product is stable.
- ↑ ( ) spin value – Indicates spin with weak assignment arguments.
- ↑ 9.0 9.1 # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
- ↑ Believed to decay by β+β+ to 106
Pd with a half-life over 1.1×1021 years - ↑ Believed to decay by β+β+ to 108
Pd with a half-life over 4.1×1017 years - ↑ 12.0 12.1 12.2 12.3 12.4 12.5 12.6 12.7 Fission product
- ↑ 13.0 13.1 Primordial radionuclide
- ↑ Believed to undergo β−β− decay to 114
Sn with a half-life over 9.2×1016 years
Cadmium-113m
| Prop: Unit: |
t½ (a) |
Yield (%) |
Q * (keV) |
βγ * |
|---|---|---|---|---|
| 155Eu | 4.76 | 0.0803 | 252 | βγ |
| 85Kr | 10.76 | 0.2180 | 687 | βγ |
| 113mCd | 14.1 | 0.0008 | 316 | β |
| 90Sr | 28.9 | 4.505 | 2826 | β |
| 137Cs | 30.23 | 6.337 | 1176 | βγ |
| 121mSn | 43.9 | 0.00005 | 390 | βγ |
| 151Sm | 88.8 | 0.5314 | 77 | β |
Cadmium-113m is a cadmium radioisotope and nuclear isomer with a half-life of 13.9 years. In a normal thermal reactor, it has a very low fission product yield, plus its large neutron capture cross section means that most of even the small amount produced is destroyed in the course of the nuclear fuel's burnup; thus, this isotope is not a significant contributor to nuclear waste.
Fast fission or fission of some heavier actinides[which?] will produce 113m
Cd at higher yields.
See also
Daughter products other than cadmium
References
- ↑ Meija, Juris; Coplen, Tyler B.; Berglund, Michael; Brand, Willi A.; De Bièvre, Paul; Gröning, Manfred; Holden, Norman E.; Irrgeher, Johanna et al. (2016). "Atomic weights of the elements 2013 (IUPAC Technical Report)". Pure and Applied Chemistry 88 (3): 265–91. doi:10.1515/pac-2015-0305.
- ↑ Ratié, Gildas; Chrastný, Vladislav; Guinoiseau, Damien; Marsac, Rémi; Vaňková, Zuzana; Komárek, Michael (2021-06-01). "Cadmium Isotope Fractionation during Complexation with Humic Acid". Environmental Science & Technology 55 (11): 7430–7444. doi:10.1021/acs.est.1c00646. ISSN 0013-936X. PMID 33970606. Bibcode: 2021EnST...55.7430R. https://doi.org/10.1021/acs.est.1c00646.
- ↑ Nesterenko, D. A.; Ruotsalainen, J.; Stryjczyk, M.; Kankainen, A.; Al Ayoubi, L.; Beliuskina, O.; Delahaye, P.; Eronen, T. et al. (1 November 2023). "High-precision measurements of low-lying isomeric states in In 120 – 124 with the JYFLTRAP double Penning trap". Physical Review C 108 (5). doi:10.1103/PhysRevC.108.054301.
- Isotope masses from:
- Audi, Georges; Bersillon, Olivier; Blachot, Jean; Wapstra, Aaldert Hendrik (2003), "The NUBASE evaluation of nuclear and decay properties", Nuclear Physics A 729: 3–128, doi:10.1016/j.nuclphysa.2003.11.001, Bibcode: 2003NuPhA.729....3A, https://hal.archives-ouvertes.fr/in2p3-00020241/document
- Isotopic compositions and standard atomic masses from:
- Template:CIAAW2003
- Wieser, Michael E. (2006). "Atomic weights of the elements 2005 (IUPAC Technical Report)". Pure and Applied Chemistry 78 (11): 2051–2066. doi:10.1351/pac200678112051.
- Half-life, spin, and isomer data selected from the following sources.
- Audi, Georges; Bersillon, Olivier; Blachot, Jean; Wapstra, Aaldert Hendrik (2003), "The NUBASE evaluation of nuclear and decay properties", Nuclear Physics A 729: 3–128, doi:10.1016/j.nuclphysa.2003.11.001, Bibcode: 2003NuPhA.729....3A, https://hal.archives-ouvertes.fr/in2p3-00020241/document
- National Nuclear Data Center. "NuDat 2.x database". Brookhaven National Laboratory. http://www.nndc.bnl.gov/nudat2/.
- Lide, David R., ed (2004). "11. Table of the Isotopes". CRC Handbook of Chemistry and Physics (85th ed.). Boca Raton, Florida: CRC Press. ISBN 978-0-8493-0485-9.
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