Isotopes of polonium
| |||||||||||||||||||||||||||||||
Polonium (84Po) has 33 isotopes, all of which are radioactive, with between 186 and 227 nucleons. 210Po with a half-life of 138.376 days has the longest half-life of naturally occurring polonium. 209Po with a half-life of 125 years has the longest half-life of all isotopes of polonium. 209Po and 208Po (half-life 2.9 years) can be made through the alpha, proton, or deuteron bombardment of lead or bismuth in a cyclotron.
Polonium-210
210Po is an alpha emitter that has a half-life of 138.376 days; it decays directly to stable 206Pb. A milligram of 210Po emits as many alpha particles per second as 5 grams of 226Ra.[2] A few curies (1 curie equals 37 gigabecquerels) of 210Po emit a blue glow caused by excitation of surrounding air. A single gram of 210Po generates 140 watts of power.[3] Because it emits many alpha particles, which are stopped within a very short distance in dense media and release their energy, 210Po has been used as a lightweight heat source to power thermoelectric cells in artificial satellites; for instance, a 210Po heat source was also in each of the Lunokhod rovers deployed on the surface of the Moon, to keep their internal components warm during the lunar nights.[4] Some anti-static brushes, used for neutralizing static electricity on materials like photographic film, contain a few microcuries of 210Po as a source of charged particles.[5] 210Po is also used in initiators for atomic bombs through the (α,n) reaction with beryllium.
The majority of the time 210Po decays by emission of an alpha particle only, not by emission of an alpha particle and a gamma ray. About one in 100,000 decays results in the emission of a gamma ray.[6] This low gamma ray production rate makes it more difficult to find and identify this isotope. Rather than gamma ray spectroscopy, alpha spectroscopy is the best method of measuring this isotope.
210Po occurs in minute amounts in nature, where it is an intermediate isotope in the uranium series decay chain. It is generated via beta decay from 210Bi.
210Po is extremely toxic, with one microgram being enough to kill the average adult (250,000 times more toxic than hydrogen cyanide by weight).[7] 210Po was used to kill Russian dissident and ex-FSB officer Alexander V. Litvinenko in 2006,[8] and was suspected as a possible cause of Yasser Arafat's death, following exhumation and analysis of his corpse in 2012–2013.[9]
List of isotopes
nuclide symbol |
historic name |
Z(p) [10][11] |
N(n) [10][11] |
isotopic mass (u) [12] |
half-life [12][13][14] |
decay mode(s) [15][n 1] |
daughter isotope(s) [n 2] |
nuclear spin [12][13][14] |
representative isotopic composition (mole fraction) |
range of natural variation (mole fraction) |
---|---|---|---|---|---|---|---|---|---|---|
excitation energy | ||||||||||
188Po | 84 | 104 | 187.999422(21) | 430(180) µs [0.40(+20−15) ms] |
0+ | |||||
189Po | 84 | 105 | 188.998481(24) | 5(1) ms | 3/2−# | |||||
190Po | 84 | 106 | 189.995101(14) | 2.46(5) ms | α (99.9%) | 186Pb | 0+ | |||
β+ (.1%) | 190Bi | |||||||||
191Po | 84 | 107 | 190.994574(12) | 22(1) ms | α | 187Pb | 3/2−# | |||
β+ (rare) | 191Bi | |||||||||
191mPo | 130(21) keV | 93(3) ms | (13/2+) | |||||||
192Po | 84 | 108 | 191.991335(13) | 32.2(3) ms | α (99%) | 188Pb | 0+ | |||
β+ (1%) | 192Bi | |||||||||
192mPo | 2600(500)# keV | ~1 µs | 12+# | |||||||
193Po | 84 | 109 | 192.99103(4) | 420(40) ms [370(+46−40) ms] |
α | 189Pb | 3/2−# | |||
β+ (rare) | 193Bi | |||||||||
193mPo | 100(30)# keV | 240(10) ms [243(+11−10) ms] |
α | 189Pb | (13/2+) | |||||
β+ (rare) | 193Bi | |||||||||
194Po | 84 | 110 | 193.988186(13) | 0.392(4) s | α | 190Pb | 0+ | |||
β+ (rare) | 194Bi | |||||||||
194mPo | 2525(2) keV | 15(2) µs | (11−) | |||||||
195Po | 84 | 111 | 194.98811(4) | 4.64(9) s | α (75%) | 191Pb | 3/2−# | |||
β+ (25%) | 195Bi | |||||||||
195mPo | 110(50) keV | 1.92(2) s | α (90%) | 191Pb | 13/2+# | |||||
β+ (10%) | 195Bi | |||||||||
IT (.01%) | 195Po | |||||||||
196Po | 84 | 112 | 195.985535(14) | 5.56(12) s | α (94%) | 192Pb | 0+ | |||
β+ (6%) | 196Bi | |||||||||
196mPo | 2490.5(17) keV | 850(90) ns | (11−) | |||||||
197Po | 84 | 113 | 196.98566(5) | 53.6(10) s | β+ (54%) | 197Bi | (3/2−) | |||
α (44%) | 193Pb | |||||||||
197mPo | 230(80)# keV | 25.8(1) s | α (84%) | 193Pb | (13/2+) | |||||
β+ (16%) | 197Bi | |||||||||
IT (.01%) | 197Po | |||||||||
198Po | 84 | 114 | 197.983389(19) | 1.77(3) min | α (57%) | 194Pb | 0+ | |||
β+ (43%) | 198Bi | |||||||||
198m1Po | 2565.92(20) keV | 200(20) ns | 11− | |||||||
198m2Po | 2691.86(20) keV | 750(50) ns | 12+ | |||||||
199Po | 84 | 115 | 198.983666(25) | 5.48(16) min | β+ (92.5%) | 199Bi | (3/2−) | |||
α (7.5%) | 195Pb | |||||||||
199mPo | 312.0(28) keV | 4.17(4) min | β+ (73.5%) | 199Bi | 13/2+ | |||||
α (24%) | 195Pb | |||||||||
IT (2.5%) | 199Po | |||||||||
200Po | 84 | 116 | 199.981799(15) | 11.5(1) min | β+ (88.8%) | 200Bi | 0+ | |||
α (11.1%) | 196Pb | |||||||||
201Po | 84 | 117 | 200.982260(6) | 15.3(2) min | β+ (98.4%) | 201Bi | 3/2− | |||
α (1.6%) | 197Pb | |||||||||
201mPo | 424.1(24) keV | 8.9(2) min | IT (56%) | 201Po | 13/2+ | |||||
EC (41%) | 201Bi | |||||||||
α (2.9%) | 197Pb | |||||||||
202Po | 84 | 118 | 201.980758(16) | 44.7(5) min | β+ (98%) | 202Bi | 0+ | |||
α (2%) | 198Pb | |||||||||
202mPo | 2626.7(7) keV | >200 ns | 11− | |||||||
203Po | 84 | 119 | 202.981420(28) | 36.7(5) min | β+ (99.89%) | 203Bi | 5/2− | |||
α (.11%) | 199Pb | |||||||||
203m1Po | 641.49(17) keV | 45(2) s | IT (99.96%) | 203Po | 13/2+ | |||||
α (.04%) | 199Pb | |||||||||
203m2Po | 2158.5(6) keV | >200 ns | ||||||||
204Po | 84 | 120 | 203.980318(12) | 3.53(2) h | β+ (99.33%) | 204Bi | 0+ | |||
α (.66%) | 200Pb | |||||||||
205Po | 84 | 121 | 204.981203(21) | 1.66(2) h | β+ (99.96%) | 205Bi | 5/2− | |||
α (.04%) | 201Pb | |||||||||
205m1Po | 143.166(17) keV | 310(60) ns | 1/2− | |||||||
205m2Po | 880.30(4) keV | 645 µs | 13/2+ | |||||||
205m3Po | 1461.21(21) keV | 57.4(9) ms | IT | 205Po | 19/2− | |||||
205m4Po | 3087.2(4) keV | 115(10) ns | 29/2− | |||||||
206Po | 84 | 122 | 205.980481(9) | 8.8(1) d | β+ (94.55%) | 206Bi | 0+ | |||
α (5.45%) | 202Pb | |||||||||
206m1Po | 1585.85(11) keV | 222(10) ns | (8+)# | |||||||
206m2Po | 2262.22(14) keV | 1.05(6) µs | (9−)# | |||||||
207Po | 84 | 123 | 206.981593(7) | 5.80(2) h | β+ (99.97%) | 207Bi | 5/2− | |||
α (.021%) | 203Pb | |||||||||
207m1Po | 68.573(14) keV | 205(10) ns | 1/2− | |||||||
207m2Po | 1115.073(16) keV | 49(4) µs | 13/2+ | |||||||
207m3Po | 1383.15(6) keV | 2.79(8) s | IT | 207Po | 19/2− | |||||
208Po | 84 | 124 | 207.9812457(19) | 2.898(2) y | α (99.99%) | 204Pb | 0+ | |||
β+ (.00277%) | 208Bi | |||||||||
209Po | 84 | 125 | 208.9824304(20) | 125.2(3.3) y[16] | α (99.52%) | 205Pb | 1/2− | |||
β+ (.48%) | 209Bi | |||||||||
210Po | Radium F | 84 | 126 | 209.9828737(13) | 138.376(2) d | α | 206Pb | 0+ | Trace[n 3] | |
210mPo | 5057.61(4) keV | 263(5) ns | 16+ | |||||||
211Po | Actinium C' | 84 | 127 | 210.9866532(14) | 0.516(3) s | α | 207Pb | 9/2+ | Trace[n 4] | |
211m1Po | 1462(5) keV | 25.2(6) s | α (99.98%) | 207Pb | (25/2+) | |||||
IT (.016%) | 211Po | |||||||||
211m2Po | 2135.7(9) keV | 243(21) ns | (31/2−) | |||||||
211m3Po | 4873.3(17) keV | 2.8(7) µs | (43/2+) | |||||||
212Po | Thorium C' | 84 | 128 | 211.9888680(13) | 299(2) ns | α | 208Pb | 0+ | Trace[n 5] | |
212mPo | 2911(12) keV | 45.1(6) s | α (99.93%) | 208Pb | (18+) | |||||
IT (.07%) | 212Po | |||||||||
213Po | 84 | 129 | 212.992857(3) | 3.65(4) µs | α | 209Pb | 9/2+ | |||
214Po | Radium C' | 84 | 130 | 213.9952014(16) | 164.3(20) µs | α | 210Pb | 0+ | Trace[n 3] | |
215Po | Actinium A | 84 | 131 | 214.9994200(27) | 1.781(4) ms | α (99.99%) | 211Pb | 9/2+ | Trace[n 4] | |
β− (2.3×10−4%) | 215At | |||||||||
216Po | Thorium A | 84 | 132 | 216.0019150(24) | 0.145(2) s | α | 212Pb | 0+ | Trace[n 5] | |
β−β− (rare) | 216Rn | |||||||||
217Po | 84 | 133 | 217.006335(7) | 1.47(5) s | α (95%) | 213Pb | 5/2+# | |||
β− (5%) | 217At | |||||||||
218Po | Radium A | 84 | 134 | 218.0089730(26) | 3.10(1) min | α (99.98%) | 214Pb | 0+ | Trace[n 3] | |
β− (.02%) | 218At | |||||||||
219Po | 84 | 135 | 219.01374(39)# | 2# min [>300 ns] |
7/2+# | |||||
220Po | 84 | 136 | 220.01660(39)# | 40# s [>300 ns] |
0+ |
- ↑ Abbreviations:
EC: Electron capture
IT: Isomeric transition - ↑ Bold for stable isotopes, bold italics for nearly stable isotopes (half-life longer than the age of the universe)
- 1 2 3 Intermediate decay product of Uranium-238
- 1 2 Intermediate decay product of Uranium-235
- 1 2 Intermediate decay product of Thorium-232
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.
- Half-life abbreviations are y=year, d=day, min=minute, s=second, ms=millisecond, µs=microsecond, ns=nanosecond.
- A superscripted m (or m2, etc.) refers to an isomer of that particular isotope.
References
- ↑ Boutin, Chad. "Polonium's Most Stable Isotope Gets Revised Half-Life Measurement". nist.gov. NIST Tech Beat. Retrieved 9 September 2014.
- ↑ C. R. Hammond. "The Elements" (PDF). Fermi National Accelerator Laboratory. p. 4-22.
- ↑ "Polonium" (PDF). Argonne National Laboratory. Archived from the original (PDF) on 2012-03-10.
- ↑ Andrew Wilson, Solar System Log, (London: Jane's Publishing Company Ltd, 1987), p. 64.
- ↑ "Staticmaster Alpha Ionizing Brush". Company 7.
- ↑ 210PO A DECAY Archived February 24, 2015, at the Wayback Machine.
- ↑ Sublette, Carey. "Polonium Poisoning".
- ↑ Cowell, Alan (November 24, 2006). "Radiation Poisoning Killed Ex-Russian Spy". The New York Times.
- ↑ "Arafat's death: what is Polonium-210?". Al Jazeera. July 10, 2012.
- 1 2 J. R. de Laeter; J. K. Böhlke; P. De Bièvre; H. Hidaka; H. S. Peiser; K. J. R. Rosman; P. D. P. Taylor (2003). "Atomic weights of the elements. Review 2000 (IUPAC Technical Report)". Pure and Applied Chemistry. 75 (6): 683–800. doi:10.1351/pac200375060683.
- 1 2 M. E. Wieser (2006). "Atomic weights of the elements 2005 (IUPAC Technical Report)". Pure and Applied Chemistry. 78 (11): 2051–2066. doi:10.1351/pac200678112051. Lay summary.
- 1 2 3 G. Audi; A. H. Wapstra; C. Thibault; J. Blachot; O. Bersillon (2003). "The NUBASE evaluation of nuclear and decay properties" (PDF). Nuclear Physics A. 729: 3–128. Bibcode:2003NuPhA.729....3A. doi:10.1016/j.nuclphysa.2003.11.001. Archived from the original (PDF) on 2008-09-23.
- 1 2 National Nuclear Data Center. "NuDat 2.1 database". Brookhaven National Laboratory. Retrieved September 2005. Check date values in:
|access-date=
(help) - 1 2 N. E. Holden (2004). "Table of the Isotopes". In D. R. Lide. CRC Handbook of Chemistry and Physics (85th ed.). CRC Press. p. 11-50. ISBN 978-0-8493-0485-9.
- ↑ "Universal Nuclide Chart". nucleonica. (Registration required (help)).
- ↑ Boutin, Chad. "Polonium's Most Stable Isotope Gets Revised Half-Life Measurement". nist.gov. NIST Tech Beat. Retrieved 9 September 2014.
Isotopes of bismuth | Isotopes of polonium | Isotopes of astatine |
Table of nuclides |