There are two natural isotopes of iridium (77Ir), and 37 radioisotopes, the most stable radioisotope being 192Ir with a half-life of 73.82 days, and many nuclear isomers, the most stable of which is 192m2Ir with a half-life of 241 years. All other isomers have half-lives under two weeks, most under a day. All isotopes of iridium are either radioactive or observationally stable, meaning that they are predicted to be radioactive but no actual decay has been observed.[4]
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Standard atomic weight Ar°(Ir) | |||||||||||||||||||||||||||||||||||||||||||
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The isotope 191Ir was the first one of any element to be shown to present a Mössbauer effect. This renders it useful for Mössbauer spectroscopy for research in physics, chemistry, biochemistry, metallurgy, and mineralogy.[5]
List of isotopes
edit
Nuclide [n 1] |
Z | N | Isotopic mass (Da)[6] [n 2][n 3] |
Half-life[1] [n 4] |
Decay mode[1] [n 5] |
Daughter isotope [n 6][n 7] |
Spin and parity[1] [n 8][n 4] |
Natural abundance (mole fraction) | |||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Excitation energy[n 4] | Normal proportion[1] | Range of variation | |||||||||||||||||
164Ir[n 9][7] | 77 | 87 | 163.99197(34)# | <0.5 μs | p? | 163Os | 2−# | ||||||||||||
164mIr | 260(100)# keV | 70(10) μs | p (96%) | 163Os | (9+) | ||||||||||||||
α (4%) | 160mRe | ||||||||||||||||||
165Ir | 77 | 88 | 165.98572(22)# | 1.20+0.82 −0.74 μs[8] |
p | 164Os | (1/2+) | ||||||||||||
165mIr[7] | ~255 keV | 340(40) μs | p (88%) | 164Os | (11/2−) | ||||||||||||||
α (12%) | 161mRe | ||||||||||||||||||
166Ir | 77 | 89 | 165.98582(22)# | 10.5(22) ms | α (93%) | 162Re | (2)− | ||||||||||||
p (7%) | 165Os | ||||||||||||||||||
166mIr | 171(6) keV | 15.1(9) ms | α (98.2%) | 162Re | (9)+ | ||||||||||||||
p (1.8%) | 165Os | ||||||||||||||||||
167Ir | 77 | 90 | 166.981672(20) | 29.3(6) ms | α (43.5%) | 163Re | 1/2+ | ||||||||||||
p (38.6%) | 166Os | ||||||||||||||||||
β+ (17.9%) | 167Os | ||||||||||||||||||
167mIr | 175.5(21) keV | 28.5(5) ms | α (89%) | 163Re | 11/2− | ||||||||||||||
β+ (11%) | 167Os | ||||||||||||||||||
p (0.41%) | 166Os | ||||||||||||||||||
168Ir | 77 | 91 | 167.979961(59) | 230(50) ms | α | 164Re | (2)- | ||||||||||||
168mIr[n 10] | 40(250) keV | 163(16) ms | α (77%) | 164Re | (9,10)+ | ||||||||||||||
β+? | 168Os | ||||||||||||||||||
β+, p? | 167Re | ||||||||||||||||||
169Ir | 77 | 92 | 168.976282(25) | 353(4) ms | α (53%) | 165Re | (1/2+) | ||||||||||||
β+ (47%) | 169Os | ||||||||||||||||||
169mIr | 153(22) keV | 280(1) ms | α (79%) | 165Re | (11/2−) | ||||||||||||||
β+? | 169Os | ||||||||||||||||||
p? | 168Os | ||||||||||||||||||
170Ir | 77 | 93 | 169.97511(11)# | 910(150) ms | β+ (94.8%) | 170Os | (3−) | ||||||||||||
α (5.2%) | 166Re | ||||||||||||||||||
170mIr[n 10] | 40(50)# keV | 811(18) ms | α (38%) | 166Re | (8+) | ||||||||||||||
β+? | 170Os | ||||||||||||||||||
IT? | 170Ir | ||||||||||||||||||
171Ir | 77 | 94 | 170.971646(41) | 3.1(3) s | β+ (85%) | 171Os | 1/2+ | ||||||||||||
α (15%) | 167Re | ||||||||||||||||||
171mIr | 164(11)# keV | 1.47(6) s | α (54%) | 167Re | (11/2−) | ||||||||||||||
β+? | 171Os | ||||||||||||||||||
p? | 170Os | ||||||||||||||||||
172Ir | 77 | 95 | 171.970607(35) | 4.4(3) s | β+ (~98%) | 172Os | (3−,4−) | ||||||||||||
α (~2%) | 168Re | ||||||||||||||||||
172mIr | 139(10) keV | 2.19(7) s | β+ (90.5%) | 172Os | (7+) | ||||||||||||||
α (9.5%) | 168Re | ||||||||||||||||||
173Ir | 77 | 96 | 172.967505(11) | 9.0(8) s | β+ (96.5%) | 173Os | (1/2+,3/2+) | ||||||||||||
α (3.5%) | 169Re | ||||||||||||||||||
173mIr | 226(9) keV | 2.20(5) s | β+ (88%) | 173Os | 11/2− | ||||||||||||||
α (12%) | 169Re | ||||||||||||||||||
174Ir | 77 | 97 | 173.966950(12) | 7.9(6) s | β+ (99.5%) | 174Os | (2+,3−) | ||||||||||||
α (0.5%) | 170Re | ||||||||||||||||||
174mIr | 124(16) keV | 4.9(3) s | β+ (97.5%) | 174Os | (6,7,8,9) | ||||||||||||||
α (2.5%) | 170Re | ||||||||||||||||||
175Ir | 77 | 98 | 174.964150(13) | 9(2) s | β+ (99.15%) | 175Os | (1/2+) | ||||||||||||
α (0.85%) | 171Re | ||||||||||||||||||
175m1Ir | 50(40)# keV | 33(4) s | β+ | 175Os | 9/2−# | ||||||||||||||
175m2Ir | 97.4(7) keV | 6.58(15) μs | IT | 175Ir | (5/2−) | ||||||||||||||
176Ir | 77 | 99 | 175.9636263(87) | 8.7(5) s | β+ (96.9%) | 176Os | (3+) | ||||||||||||
α (3.1%) | 172Re | ||||||||||||||||||
177Ir | 77 | 100 | 176.961302(21) | 29.8(17) s | β+ (99.94%) | 177Os | 5/2− | ||||||||||||
α (0.06%) | 173Re | ||||||||||||||||||
177mIr | 180.9(4) keV | >100 ns | IT | 177Ir | (5/2+) | ||||||||||||||
178Ir | 77 | 101 | 177.961079(20) | 12(2) s | β+ | 178Os | 3+# | ||||||||||||
179Ir | 77 | 102 | 178.959118(10) | 79(1) s | β+ | 179Os | (5/2)− | ||||||||||||
180Ir | 77 | 103 | 179.959229(23) | 1.5(1) min | β+ | 180Os | (5+) | ||||||||||||
181Ir | 77 | 104 | 180.9576347(56) | 4.90(15) min | β+ | 181Os | 5/2− | ||||||||||||
181m1Ir | 289.33(13) keV | 298 ns | IT | 181Ir | 5/2+ | ||||||||||||||
181m2Ir | 366.30(22) keV | 126(6) ns | IT | 181Ir | 9/2− | ||||||||||||||
182Ir | 77 | 105 | 181.958076(23) | 15.0(10) min | β+ | 182Os | 3+ | ||||||||||||
182m1Ir | 71.02(17) keV | 170(40) ns | IT | 182Ir | (5)+ | ||||||||||||||
182m2Ir | 176.4(3) keV | 130(50) ns | IT | 182Ir | (6−) | ||||||||||||||
183Ir | 77 | 106 | 182.956841(26) | 58(5) min | β+ | 183Os | 5/2− | ||||||||||||
184Ir | 77 | 107 | 183.957476(30) | 3.09(3) h | β+ | 184Os | 5− | ||||||||||||
184m1Ir | 225.65(11) keV | 470(30) μs | IT | 184Ir | 3+ | ||||||||||||||
184m2Ir | 328.40(24) keV | 350(90) ns | IT | 184Ir | 7+ | ||||||||||||||
185Ir | 77 | 108 | 184.956698(30) | 14.4(1) h | β+ | 185Os | 5/2− | ||||||||||||
185mIr | 2197(23) keV | 120(20) ns | IT | 185Ir | (23/2,25/2)# | ||||||||||||||
186Ir | 77 | 109 | 185.957947(18) | 16.64(3) h | β+ | 186Os | 5+ | ||||||||||||
186mIr | 0.8(4) keV | 1.92(5) h | β+ (~75%) | 186Os | 2− | ||||||||||||||
IT (~25%) | 186Ir | ||||||||||||||||||
187Ir | 77 | 110 | 186.957542(30) | 10.5(3) h | β+ | 187Os | 3/2+ | ||||||||||||
187m1Ir | 186.16(4) keV | 30.3(6) ms | IT | 187Ir | 9/2− | ||||||||||||||
187m2Ir | 433.75(6) keV | 152(12) ns | IT | 187Ir | 11/2− | ||||||||||||||
187m3Ir | 2487.7(4) keV | 1.8(5) μs | IT | 187Ir | 29/2− | ||||||||||||||
188Ir | 77 | 111 | 187.958835(10) | 41.5(5) h | β+ | 188Os | 1− | ||||||||||||
188mIr | 964(23) keV | 4.15(15) ms | IT | 188Ir | 11−# | ||||||||||||||
189Ir | 77 | 112 | 188.958723(14) | 13.2(1) d | EC | 189Os | 3/2+ | ||||||||||||
189m1Ir | 372.17(4) keV | 13.3(3) ms | IT | 189Ir | 11/2− | ||||||||||||||
189m2Ir | 2332.8(3) keV | 3.7(2) ms | IT | 189Ir | 25/2+ | ||||||||||||||
190Ir | 77 | 113 | 189.9605434(15) | 11.7511(20) d[9] | EC | 190Os | 4− | ||||||||||||
β+ (<0.002%)[9] | |||||||||||||||||||
190m1Ir | 26.1(1) keV | 1.120(3) h | IT | 190Ir | 1− | ||||||||||||||
190m2Ir | 36.154(25) keV | >2 μs | IT | 190Ir | 4+ | ||||||||||||||
190m3Ir | 376.4(1) keV | 3.087(12) h | EC (91.4%) | 190Os | 11− | ||||||||||||||
IT (8.6%) | 190Ir | ||||||||||||||||||
191Ir | 77 | 114 | 190.9605915(14) | Observationally Stable[n 11] | 3/2+ | 0.373(2) | |||||||||||||
191m1Ir | 171.29(4) keV | 4.899(23) s | IT | 191Ir | 11/2− | ||||||||||||||
191m2Ir | 2101.0(9) keV | 5.7(4) s | IT | 191Ir | 31/2(+) | ||||||||||||||
192Ir | 77 | 115 | 191.9626024(14) | 73.820(14) d | β− (95.24%) | 192Pt | 4+ | ||||||||||||
EC (4.76%) | 192Os | ||||||||||||||||||
192m1Ir | 56.720(5) keV | 1.45(5) min | IT (99.98%) | 192Ir | 1− | ||||||||||||||
β− (0.0175%) | 192Pt | ||||||||||||||||||
192m2Ir | 168.14(12) keV | 241(9) y | IT | 192Ir | (11−) | ||||||||||||||
193Ir | 77 | 116 | 192.9629238(14) | Observationally Stable[n 12] | 3/2+ | 0.627(2) | |||||||||||||
193m1Ir | 80.238(6) keV | 10.53(4) d | IT | 193Ir | 11/2− | ||||||||||||||
193m2Ir | 2278.9(5) keV | 124.8(21) μs | IT | 193Ir | 31/2+ | ||||||||||||||
194Ir | 77 | 117 | 193.9650757(14) | 19.35(7) h | β− | 194Pt | 1− | ||||||||||||
194m1Ir | 147.072(2) keV | 31.85(24) ms | IT | 194Ir | 4+ | ||||||||||||||
194m2Ir | 370(70) keV | 171(11) d | β− | 194Pt | (11−) | ||||||||||||||
195Ir | 77 | 118 | 194.9659769(14) | 2.29(17) h | β− | 195Pt | 3/2+ | ||||||||||||
195m1Ir | 100(5) keV | 3.74(7) h | β− | 195Pt | 11/2− | ||||||||||||||
195m2Ir | 2354(6) keV | 4.4(6) μs | IT | 195Ir | (27/2+) | ||||||||||||||
196Ir | 77 | 119 | 195.968400(41) | 52.0(11) s | β− | 196Pt | (1,2−) | ||||||||||||
196mIr | 210(40) keV | 1.40(2) h | β− | 196Pt | 11−# | ||||||||||||||
197Ir | 77 | 120 | 196.969657(22) | 5.8(5) min | β− | 197Pt | 3/2+ | ||||||||||||
197m1Ir | 115(5) keV | 8.9(3) min | β− | 197Pt | 11/2− | ||||||||||||||
197m2Ir | 1700(500)# keV | 30(8) μs | IT | 197Ir | |||||||||||||||
197m3Ir | 2800(500)# keV | 15(9) μs | IT | 197Ir | |||||||||||||||
198Ir | 77 | 121 | 197.97240(22)# | 8.7(4) s | β− | 198Pt | 1− | ||||||||||||
199Ir | 77 | 122 | 198.973807(44) | 7(5) s | β− | 199Pt | 3/2+# | ||||||||||||
200Ir | 77 | 123 | 199.97684(21)# | 43(6) s | β− | 200Pt | (2−, 3−) | ||||||||||||
201Ir | 77 | 124 | 200.97870(22)# | 21(5) s | β− | 201Pt | (3/2+) | ||||||||||||
202Ir | 77 | 125 | 201.98214(32)# | 11(3) s | β− | 202Pt | (2−) | ||||||||||||
202mIr | 2600(300)# keV | 3.4(6) μs | IT | 202Ir | |||||||||||||||
203Ir | 77 | 126 | 202.98457(43)# | 7# s [>300 ns] |
3/2+# | ||||||||||||||
203mIr | 2140(50)# keV | 798(350) ns | IT | 203Ir | |||||||||||||||
204Ir | 77 | 127 | 203.98973(43)# | 2# s [>300 ns] |
3/2+# | ||||||||||||||
205Ir | 77 | 128 | 204.99399(54)# | 1# s [>300 ns] |
3/2+# | ||||||||||||||
This table header & footer: |
- ^ mIr – 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).
- ^ a b c # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
- ^
Modes of decay:
α: Alpha decay β+: Positron emission EC: Electron capture β−: Beta decay IT: Isomeric transition
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.
- ^ Discovery of this isotope is unconfirmed
- ^ a b Order of ground state and isomer is uncertain.
- ^ Believed to undergo α decay to 187Re[10][11]
- ^ Believed to undergo α decay to 189Re[10]
Iridium-192
editIridium-192 (symbol 192Ir) is a radioactive isotope of iridium, with a half-life of 73.82 days.[12] It decays by emitting beta (β) particles and gamma (γ) radiation. 95.24% of 192Ir decays occur via β- emission, leading to 192Pt; the remaining 4.76% occur via electron capture to 192Os; both modes involve gamma emission. Iridium-192 is normally produced by neutron activation of natural-abundance iridium metal.[13]
Iridium-192 is used in brachytherapy and in industrial radiography, particularly for nondestructive testing of welds in steel in the oil and gas industries.
See also
editDaughter products other than iridium
References
edit- ^ a b c d e Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3): 030001. doi:10.1088/1674-1137/abddae.
- ^ "Standard Atomic Weights: Iridium". CIAAW. 2017.
- ^ Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (2022-05-04). "Standard atomic weights of the elements 2021 (IUPAC Technical Report)". Pure and Applied Chemistry. doi:10.1515/pac-2019-0603. ISSN 1365-3075.
- ^ Belli, P.; Bernabei, R.; Danevich, F. A.; et al. (2019). "Experimental searches for rare alpha and beta decays". European Physical Journal A. 55 (8): 140–1–140–7. arXiv:1908.11458. Bibcode:2019EPJA...55..140B. doi:10.1140/epja/i2019-12823-2. ISSN 1434-601X. S2CID 201664098.
- ^ Chereminisoff, N. P. (1990). Handbook of Ceramics and Composites. CRC Press. p. 424. ISBN 978-0-8247-8006-7.
- ^ Wang, Meng; Huang, W.J.; Kondev, F.G.; Audi, G.; Naimi, S. (2021). "The AME 2020 atomic mass evaluation (II). Tables, graphs and references*". Chinese Physics C. 45 (3): 030003. doi:10.1088/1674-1137/abddaf.
- ^ a b Drummond, M. C.; O'Donnell, D.; Page, R. D.; Joss, D. T.; Capponi, L.; Cox, D. M.; Darby, I. G.; Donosa, L.; Filmer, F.; Grahn, T.; Greenlees, P. T.; Hauschild, K.; Herzan, A.; Jakobsson, U.; Jones, P. M.; Julin, R.; Juutinen, S.; Ketelhut, S.; Leino, M.; Lopez-Martens, A.; Mistry, A. K.; Nieminen, P.; Peura, P.; Rahkila, P.; Rinta-Antila, S.; Ruotsalainen, P.; Sandzelius, M.; Sarén, J.; Sayğı, B.; Scholey, C.; Simpson, J.; Sorri, J.; Thornthwaite, A.; Uusitalo, J. (16 June 2014). "α decay of the π h 11 / 2 isomer in Ir 164". Physical Review C. 89 (6): 064309. Bibcode:2014PhRvC..89f4309D. doi:10.1103/PhysRevC.89.064309. ISSN 0556-2813. Retrieved 21 June 2023.
- ^ Hilton, Joshua Ben. "Decays of new nuclides 169Au, 170Hg, 165Pt and the ground state of 165Ir discovered using MARA". University of Liverpool. ProQuest 2448649087. Retrieved 21 June 2023.
- ^ a b Janiak, Ł.; Gierlik, M.; Kosinski, T.; Matusiak, M.; Madejowski, G.; Wronka, S.; Rzadkiewicz, J. (2024). "Half-life of 190Ir". Physical Review C. 110 (014306). doi:10.1103/PhysRevC.110.014306.
- ^ a b Danevich, F. A.; Andreotti, E.; Hult, M.; Marissens, G.; Tretyak, V. I.; Yuksel, A. (2012). "Search for α decay of 151Eu to the first excited level of 147Pm using underground γ-ray spectrometry". European Physical Journal A. 48 (157): 157. arXiv:1301.3465. Bibcode:2012EPJA...48..157D. doi:10.1140/epja/i2012-12157-7. S2CID 118657922.
- ^ Belli, P.; Bernabei, R.; Danevich, F. A.; et al. (2019). "Experimental searches for rare alpha and beta decays". European Physical Journal A. 55 (8): 140–1–140–7. arXiv:1908.11458. Bibcode:2019EPJA...55..140B. doi:10.1140/epja/i2019-12823-2. ISSN 1434-601X. S2CID 201664098.
- ^ "Radioisotope Brief: Iridium-192 (Ir-192)". Retrieved 20 March 2012.
- ^ "Isotope Supplier: Stable Isotopes and Radioisotopes from ISOFLEX - Iridium-192". www.isoflex.com. Retrieved 2017-10-11.
External links
edit- NLM Hazardous Substances Databank – Iridium, Radioactive (referring to iridium-192)