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Actinium (89Ac) has no stable isotopes and no characteristic terrestrial isotopic composition, thus a standard atomic weight cannot be given. There are 34 known isotopes, from Ac to Ac, and 7 isomers. Three isotopes are found in nature, Ac, Ac and Ac, as intermediate decay products of, respectively, Np, U, and Th. Ac and Ac are extremely rare, so almost all natural actinium is Ac.
The most stable isotopes are Ac with a half-life of 21.772 years, Ac with a half-life of 10.0 days, and Ac with a half-life of 29.37 hours. All other isotopes have half-lives under 10 hours, and most under a minute. The shortest-lived known isotope is Ac with a half-life of 69 ns.
Purified Ac comes into equilibrium with its decay products (Th and Fr) after 185 days.
List of isotopes
Nuclide |
Historic name |
Z | N | Isotopic mass (Da) |
Half-life |
Decay mode |
Daughter isotope |
Spin and parity |
Isotopic abundance | ||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Excitation energy | |||||||||||||||||||
Ac | 89 | 114 | 56+269 −26 μs |
α | Fr | (1/2+) | |||||||||||||
Ac | 89 | 115 | 7.4+2.2 −1.4 ms |
α | Fr | ||||||||||||||
Ac | 89 | 116 | 7.7+2.7 −1.6 ms |
α | Fr | 9/2−? | |||||||||||||
Ac | 89 | 117 | 206.01450(8) | 25(7) ms | α | Fr | (3+) | ||||||||||||
Ac | 80(50) keV | 15(6) ms | α | Fr | |||||||||||||||
Ac | 290(110)# keV | 41(16) ms | α | Fr | (10−) | ||||||||||||||
Ac | 89 | 118 | 207.01195(6) | 31(8) ms |
α | Fr | 9/2−# | ||||||||||||
Ac | 89 | 119 | 208.01155(6) | 97(16) ms |
α (99%) | Fr | (3+) | ||||||||||||
β (1%) | Ra | ||||||||||||||||||
Ac | 506(26) keV | 28(7) ms |
α (89%) | Fr | (10−) | ||||||||||||||
IT (10%) | Ac | ||||||||||||||||||
β (1%) | Ra | ||||||||||||||||||
Ac | 89 | 120 | 209.00949(5) | 92(11) ms | α (99%) | Fr | (9/2−) | ||||||||||||
β (1%) | Ra | ||||||||||||||||||
Ac | 89 | 121 | 210.00944(6) | 350(40) ms | α (96%) | Fr | 7+# | ||||||||||||
β (4%) | Ra | ||||||||||||||||||
Ac | 89 | 122 | 211.00773(8) | 213(25) ms | α (99.8%) | Fr | 9/2−# | ||||||||||||
β (.2%) | Ra | ||||||||||||||||||
Ac | 89 | 123 | 212.00781(7) | 920(50) ms | α (97%) | Fr | 6+# | ||||||||||||
β (3%) | Ra | ||||||||||||||||||
Ac | 89 | 124 | 213.00661(6) | 731(17) ms | α | Fr | (9/2−)# | ||||||||||||
β (rare) | Ra | ||||||||||||||||||
Ac | 89 | 125 | 214.006902(24) | 8.2(2) s | α (89%) | Fr | (5+)# | ||||||||||||
β (11%) | Ra | ||||||||||||||||||
Ac | 89 | 126 | 215.006454(23) | 0.17(1) s | α (99.91%) | Fr | 9/2− | ||||||||||||
β (.09%) | Ra | ||||||||||||||||||
Ac | 89 | 127 | 216.008720(29) | 440(16) μs | α | Fr | (1−) | ||||||||||||
Ac | 38(5) keV | 441(7) μs | α | Fr | (9−) | ||||||||||||||
Ac | 422#(100#) keV | ~300 ns | IT | Ac | |||||||||||||||
Ac | 89 | 128 | 217.009347(14) | 69(4) ns | α | Fr | 9/2− | ||||||||||||
Ac | 2012(20) keV | 740(40) ns | (29/2)+ | ||||||||||||||||
Ac | 89 | 129 | 218.01164(5) | 1.08(9) μs | α | Fr | (1−)# | ||||||||||||
Ac | 607(86)# keV | 103(11) ns | IT | Ac | (11+) | ||||||||||||||
Ac | 89 | 130 | 219.01242(5) | 11.8(15) μs | α | Fr | 9/2− | ||||||||||||
β (10%) | Ra | ||||||||||||||||||
Ac | 89 | 131 | 220.014763(16) | 26.36(19) ms | α | Fr | (3−) | ||||||||||||
β (5×10%) | Ra | ||||||||||||||||||
Ac | 89 | 132 | 221.01559(5) | 52(2) ms | α | Fr | 9/2−# | ||||||||||||
Ac | 89 | 133 | 222.017844(6) | 5.0(5) s | α (99%) | Fr | 1− | ||||||||||||
β (1%) | Ra | ||||||||||||||||||
Ac | 200(150)# keV | 1.05(7) min | α (88.6%) | Fr | high | ||||||||||||||
IT (10%) | Ac | ||||||||||||||||||
β (1.4%) | Ra | ||||||||||||||||||
Ac | 89 | 134 | 223.019137(8) | 2.10(5) min | α (99%) | Fr | (5/2−) | ||||||||||||
EC (1%) | Ra | ||||||||||||||||||
CD (3.2×10%) | Bi C | ||||||||||||||||||
Ac | 89 | 135 | 224.021723(4) | 2.78(17) h | β (90.9%) | Ra | 0− | ||||||||||||
α (9.1%) | Fr | ||||||||||||||||||
β (1.6%) | Th | ||||||||||||||||||
Ac | 89 | 136 | 225.023230(5) | 10.0(1) d | α | Fr | (3/2−) | Trace | |||||||||||
CD (6×10%) | Bi C | ||||||||||||||||||
Ac | 89 | 137 | 226.026098(4) | 29.37(12) h | β (83%) | Th | (1)(−#) | ||||||||||||
EC (17%) | Ra | ||||||||||||||||||
α (.006%) | Fr | ||||||||||||||||||
Ac | Actinium | 89 | 138 | 227.0277521(26) | 21.772(3) y | β (98.62%) | Th | 3/2− | Trace | ||||||||||
α (1.38%) | Fr | ||||||||||||||||||
Ac | Mesothorium 2 | 89 | 139 | 228.0310211(27) | 6.13(2) h | β | Th | 3+ | Trace | ||||||||||
Ac | 89 | 140 | 229.03302(4) | 62.7(5) min | β | Th | (3/2+) | ||||||||||||
Ac | 89 | 141 | 230.03629(32) | 122(3) s | β | Th | (1+) | ||||||||||||
Ac | 89 | 142 | 231.03856(11) | 7.5(1) min | β | Th | (1/2+) | ||||||||||||
Ac | 89 | 143 | 232.04203(11) | 119(5) s | β | Th | (1+) | ||||||||||||
Ac | 89 | 144 | 233.04455(32)# | 145(10) s | β | Th | (1/2+) | ||||||||||||
Ac | 89 | 145 | 234.04842(43)# | 44(7) s | β | Th | |||||||||||||
Ac | 89 | 146 | 235.05123(38)# | 60(4) s | β | Th | 1/2+# | ||||||||||||
Ac | 89 | 147 | 236.05530(54)# | 72+345 −33 s |
β | Th | |||||||||||||
This table header & footer: |
- Ac – 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).
-
Modes of decay:
CD: Cluster decay EC: Electron capture IT: Isomeric transition - Bold italics symbol as daughter – Daughter product is nearly stable.
- ( ) spin value – Indicates spin with weak assignment arguments.
- ^ # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
- Has medical uses
- Intermediate decay product of Np
- Source of element's name
- Intermediate decay product of U
- Intermediate decay product of Th
Actinides vs fission products
Actinides and fission products by half-life | ||||||||
---|---|---|---|---|---|---|---|---|
Actinides by decay chain | Half-life range (a) |
Fission products of U by yield | ||||||
4n | 4n + 1 | 4n + 2 | 4n + 3 | 4.5–7% | 0.04–1.25% | <0.001% | ||
Ra | 4–6 a | Eu | ||||||
Bk | > 9 a | |||||||
Cm | Pu | Cf | Ac | 10–29 a | Sr | Kr | Cd | |
U | Pu | Cm | 29–97 a | Cs | Sm | Sn | ||
Cf | Am | 141–351 a |
No fission products have a half-life | |||||
Am | Cf | 430–900 a | ||||||
Ra | Bk | 1.3–1.6 ka | ||||||
Pu | Th | Cm | Am | 4.7–7.4 ka | ||||
Cm | Cm | 8.3–8.5 ka | ||||||
Pu | 24.1 ka | |||||||
Th | Pa | 32–76 ka | ||||||
Np | U | U | 150–250 ka | Tc | Sn | |||
Cm | Pu | 327–375 ka | Se | |||||
1.33 Ma | Cs | |||||||
Np | 1.61–6.5 Ma | Zr | Pd | |||||
U | Cm | 15–24 Ma | I | |||||
Pu | 80 Ma |
... nor beyond 15.7 Ma | ||||||
Th | U | U | 0.7–14.1 Ga | |||||
|
Notable isotopes
Actinium-225
Main article: Actinium-225Actinium-225 is a highly radioactive isotope with 136 neutrons. It is an alpha emitter and has a half-life of 9.919 days. As of 2024, it is being researched as a possible alpha source in targeted alpha therapy. Actinium-225 undergoes a series of three alpha decays – via the short-lived francium-221 and astatine-217 – to Bi, which itself is used as an alpha source. Another benefit is that the decay chain of Ac ends in the nuclide Bi, which has a considerably shorter biological half-life than lead. However, a major factor limiting its usage is the difficulty in producing the short-lived isotope, as it is most commonly isolated from aging parent nuclides (such as U); it may also be produced in cyclotrons, linear accelerators, or fast breeder reactors.
Actinium-226
Actinium-226 is an isotope of actinium with a half-life of 29.37 hours. It mainly (83%) undergos beta decay, sometimes (17%) undergo electron capture, and rarely (0.006%) undergo alpha decay. There are researches on Ac to use it in SPECT.
Actinium-227
Actinium-227 is the most stable isotope of actinium, with a half-life of 21.772 years. It mainly (98.62%) undergos beta decay, but sometimes (1.38%) it will undergo alpha decay instead. Ac is a member of the actinium series. It is found only in traces in uranium ores – one tonne of uranium in ore contains about 0.2 milligrams of Ac. Ac is prepared, in milligram amounts, by the neutron irradiation of Ra in a nuclear reactor.
Ac is highly radioactive and was therefore studied for use as an active element of radioisotope thermoelectric generators, for example in spacecraft. The oxide of Ac pressed with beryllium is also an efficient neutron source with the activity exceeding that of the standard americium-beryllium and radium-beryllium pairs. In all those applications, Ac (a beta source) is merely a progenitor which generates alpha-emitting isotopes upon its decay. Beryllium captures alpha particles and emits neutrons owing to its large cross-section for the (α,n) nuclear reaction:
The AcBe neutron sources can be applied in a neutron probe – a standard device for measuring the quantity of water present in soil, as well as moisture/density for quality control in highway construction. Such probes are also used in well logging applications, in neutron radiography, tomography and other radiochemical investigations.
The medium half-life of Ac makes it a very convenient radioactive isotope in modeling the slow vertical mixing of oceanic waters. The associated processes cannot be studied with the required accuracy by direct measurements of current velocities (of the order 50 meters per year). However, evaluation of the concentration depth-profiles for different isotopes allows estimating the mixing rates. The physics behind this method is as follows: oceanic waters contain homogeneously dispersed U. Its decay product, Pa, gradually precipitates to the bottom, so that its concentration first increases with depth and then stays nearly constant. Pa decays to Ac; however, the concentration of the latter isotope does not follow the Pa depth profile, but instead increases toward the sea bottom. This occurs because of the mixing processes which raise some additional Ac from the sea bottom. Thus analysis of both Pa and Ac depth profiles allows researchers to model the mixing behavior.
See also
Notes
- Bismuth-209 decays into thallium-205 with a half-life exceeding 10 years, but this half-life is so long that for practical purposes bismuth-209 can be considered stable.
References
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"The isotopic analyses disclosed a species of mass 248 in constant abundance in three samples analysed over a period of about 10 months. This was ascribed to an isomer of Bk with a half-life greater than 9 . No growth of Cf was detected, and a lower limit for the β half-life can be set at about 10 . No alpha activity attributable to the new isomer has been detected; the alpha half-life is probably greater than 300 ." - This is the heaviest nuclide with a half-life of at least four years before the "sea of instability".
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- Isotope masses from:
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