Physics:Isotopes of yttrium
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| Standard atomic weight Ar, standard(Y) |
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Natural yttrium (39Y) is composed of the single stable isotope, 89Y. The most stable radioisotopes are 88Y, which has a half-life of 106.63 days, and 91Y, with a half-life of 58.51 days. All the other isotopes and isomers have half-lives of less than 15 hours, except 87Y with 79.8 hours and 90Y with 64.05 hours. The dominant decay mode below the stable 89Y is electron capture to isotopes of strontium and the dominant mode after it is beta emission to isotopes of zirconium.
In total, the isotopes characterized range from 76Y to 109Y.
In products of nuclear fission, 90Y exists in equilibrium with its parent isotope strontium-90. This isotope alone is also used in medicine; see yttrium-90.
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 4] |
Physics:Natural abundance (mole fraction) | |
|---|---|---|---|---|---|---|---|---|---|
| Excitation energy[n 4] | Normal proportion | Range of variation | |||||||
| 76Y | 39 | 37 | 75.95894(32)# | 28(9) ms | β+? | 76Sr | 1−# | ||
| p? | 75Sr | ||||||||
| β+, p? | 75Rb | ||||||||
| 77Y | 39 | 38 | 76.95015(22)# | 63(17) ms | β+ | 77Sr | 5/2+# | ||
| p? | 76Sr | ||||||||
| β+, p? | 76Rb | ||||||||
| 78Y | 39 | 39 | 77.94399(32)# | 54(5) ms | β+ | 78Sr | (0+) | ||
| β+, p? | 77Rb | ||||||||
| 78mY[n 9] | ~300 keV[n 10] | 5.8(6) s | β+ | 78Sr | (5+) | ||||
| β+, p? | 77Rb | ||||||||
| 79Y | 39 | 40 | 78.937752(14)[2] | 14.8(6) s | β+ | 79Sr | 5/2+# | ||
| 80Y | 39 | 41 | 79.9343548(67) | 30.1(5) s | β+ | 80Sr | 4− | ||
| 80m1Y | 228.5(1) keV | 4.8(3) s | IT (81%) | 80Y | 1− | ||||
| β+ (19%) | 80Sr | ||||||||
| 80m2Y | 312.6(9) keV | 4.7(3) μs | IT | 80Y | (2+) | ||||
| 81Y | 39 | 42 | 80.9294459(30)[3] | 70.4(10) s | β+ | 81Sr | (5/2+) | ||
| 82Y | 39 | 43 | 81.9269302(59) | 8.30(20) s | β+ | 82Sr | 1+ | ||
| 82m1Y | 402.63(14) keV | 258(22) ns | IT | 82Y | 4− | ||||
| 82m2Y | 507.50(13) keV | 148(6) ns | IT | 82Y | 6+ | ||||
| 83Y | 39 | 44 | 82.922484(20) | 7.08(8) min | β+ | 83Sr | (9/2+) | ||
| 83mY | 62.04(10) keV | 2.85(2) min | β+ (60%) | 83Sr | (3/2−) | ||||
| IT (40%) | 83Y | ||||||||
| 84Y | 39 | 45 | 83.9206711(46) | 39.5(8) min | β+ | 84Sr | (6+) | ||
| 84m1Y | 67.0(2) keV | 4.6(2) s | β+ | 84Sr | 1+ | ||||
| 84m2Y | 210.42(16) keV | 292(10) ns | IT | 84Y | 4− | ||||
| 85Y | 39 | 46 | 84.916433(20) | 2.68(5) h | β+ | 85Sr | (1/2)− | ||
| 85m1Y | 19.68(17) keV | 4.86(20) h | β+ | 85Sr | (9/2)+ | ||||
| IT? | 85Y | ||||||||
| 85m2Y | 266.18(10) keV | 178(7) ns | IT | 85Y | (5/2)− | ||||
| 86Y | 39 | 47 | 85.914886(15) | 14.74(2) h | β+ | 86Sr | 4− | ||
| 86m1Y | 218.21(9) keV | 47.4(4) min | IT (99.31%) | 86Y | (8+) | ||||
| β+ (0.69%) | 86Sr | ||||||||
| 86m2Y | 302.18(9) keV | 125.3(55) ns | IT | 86Y | 6+ | ||||
| 87Y | 39 | 48 | 86.9108761(12) | 79.8(3) h | β+ | 87Sr | 1/2− | ||
| 87mY | 380.82(7) keV | 13.37(3) h | IT (98.43%) | 87Y | 9/2+ | ||||
| β+ (1.57%) | 87Sr | ||||||||
| 88Y | 39 | 49 | 87.9095013(16) | 106.629(24) d | β+ | 88Sr | 4− | ||
| 88m1Y | 392.86(9) keV | 301(3) μs | IT | 88Y | 1+ | ||||
| 88m2Y | 674.55(4) keV | 13.98(17) ms | IT | 88Y | 8+ | ||||
| 89Y[n 11] | 39 | 50 | 88.90583816(36) | Stable | 1/2− | 1.0000 | |||
| 89mY | 908.97(3) keV | 15.663(5) s | IT | 89Y | 9/2+ | ||||
| 90Y[n 11] | 39 | 51 | 89.90714175(38) | 64.05(5) h | β− | 90Zr | 2− | ||
| 90mY | 682.01(5) keV | 3.226(11) h | IT | 90Y | 7+ | ||||
| β− (0.0018%) | 90Zr | ||||||||
| 91Y[n 11] | 39 | 52 | 90.9072980(20) | 58.51(6) d | β− | 91Zr | 1/2− | ||
| 91mY | 555.58(5) keV | 49.71(4) min | IT | 91Y | 9/2+ | ||||
| β−? | 91Zr | ||||||||
| 92Y | 39 | 53 | 91.9089458(98) | 3.54(1) h | β− | 92Zr | 2− | ||
| 92mY | 807(50)# keV | 3.7(5) μs | IT | 92Y | 7+# | ||||
| 93Y | 39 | 54 | 92.909578(11) | 10.18(8) h | β− | 93Zr | 1/2− | ||
| 93mY | 758.719(21) keV | 820(40) ms | IT | 93Y | 9/2+ | ||||
| 94Y | 39 | 55 | 93.9115921(68) | 18.7(1) min | β− | 94Zr | 2− | ||
| 94mY | 1202.3(10) keV | 1.304(12) μs | IT | 94Y | (5+) | ||||
| 95Y | 39 | 56 | 94.9128197(73) | 10.3(1) min | β− | 95Zr | 1/2− | ||
| 95mY | 1087.6(6) keV | 48.6(5) μs | IT | 95Y | 9/2+ | ||||
| 96Y | 39 | 57 | 95.9159093(65) | 5.34(5) s | β− | 96Zr | 0− | ||
| 96m1Y | 1540(9) keV | 9.6(2) s | β− | 96Zr | 8+ | ||||
| 96m2Y | 1655.0(11) keV | 181(9) ns | IT | 96Y | (6+) | ||||
| 97Y | 39 | 58 | 96.9182867(72) | 3.75(3) s | β− (99.945%) | 97Zr | 1/2− | ||
| β−, n (0.055%) | 96Zr | ||||||||
| 97m1Y | 667.52(23) keV | 1.17(3) s | β− (>99.2%) | 97Zr | 9/2+ | ||||
| IT (<0.7%) | 97Y | ||||||||
| β−, n (0.11%) | 96Zr | ||||||||
| 97m2Y | 3522.6(4) keV | 142(8) ms | IT (94.8%) | 97Y | (27/2−) | ||||
| β− (5.2%) | 97Zr | ||||||||
| 98Y | 39 | 59 | 97.9223948(85) | 548(2) ms | β− (99.67%) | 98Zr | 0− | ||
| β−, n (0.33%) | 97Zr | ||||||||
| 98m1Y | 170.78(5) keV | 615(8) ns | IT | 98Y | 2− | ||||
| 98m2Y | 465.7(7) keV | 2.32(8) s | β− (96.56%) | 98Zr | (6,7)+ | ||||
| β−, n (3.44%) | 97Zr | ||||||||
| IT? | 98Y | ||||||||
| 98m3Y | 496.10(11) keV | 6.90(54) μs | IT | 98Y | (4)− | ||||
| 98m4Y | 594(10) keV | 180(7) ns | IT | 98Y | (3−,4−) | ||||
| 98m5Y | 972.17(20) keV | 450(150) ns | IT | 98Y | (8+) | ||||
| 98m6Y | 1181.50(18) keV | 762(14) ns | IT | 98Y | (10−) | ||||
| 99Y | 39 | 60 | 98.9241608(71) | 1.484(7) s | β− (98.23%) | 99Zr | 5/2+ | ||
| β−, n (1.77%) | 98Zr | ||||||||
| 99mY | 2141.65(19) keV | 8.2(4) μs | IT | 99Y | (17/2+) | ||||
| 100Y | 39 | 61 | 99.927728(12) | 940(30) ms | β− | 100Zr | 4+ | ||
| β−, n? | 99Zr | ||||||||
| 100mY | 144(16) keV | 727(6) ms | β− (98.92%) | 100Zr | 1+# | ||||
| β−, n (1.08%) | 99Zr | ||||||||
| 101Y | 39 | 62 | 100.9301608(76) | 426(20) ms | β− (97.7%) | 101Zr | 5/2+ | ||
| β−, n (2.3%) | 100Zr | ||||||||
| 101mY | 1205.0(10) keV | 870(90) ns | IT | 101Y | 13/2−# | ||||
| 102Y | 39 | 63 | 101.9343285(44) | 360(40) ms | β− (>97.4%) | 102Zr | (5−) | ||
| β−, n (<2.6%) | 101Zr | ||||||||
| 102mY[n 9] | 100(100)# keV | 300(100) ms | β− (>97.4%) | 102Zr | (0−,1−) | ||||
| β−, n (<2.6%) | 101Zr | ||||||||
| IT? | 102Y | ||||||||
| 103Y | 39 | 64 | 102.937244(12) | 239(12) ms | β− (92.0%) | 103Zr | 5/2+# | ||
| β−, n (8.0%) | 102Zr | ||||||||
| 104Y | 39 | 65 | 103.94194(22)# | 197(4) ms | β− (66%) | 104Zr | (0+,1+)# | ||
| β−, n (34%) | 103Zr | ||||||||
| β−, 2n? | 102Zr | ||||||||
| 105Y | 39 | 66 | 104.94571(43)# | 95(9) ms | β− | 105Zr | 5/2+# | ||
| β−, n (<82%) | 104Zr | ||||||||
| β−, 2n? | 103Zr | ||||||||
| 106Y | 39 | 67 | 105.95084(54)# | 75(6) ms | β− | 106Zr | 2+# | ||
| β−, n? | 105Zr | ||||||||
| β−, 2n? | 104Zr | ||||||||
| 107Y | 39 | 68 | 106.95494(54)# | 33.5(3) ms | β− | 107Zr | 5/2+# | ||
| β−, n? | 106Zr | ||||||||
| β−, 2n? | 105Zr | ||||||||
| 108Y | 39 | 69 | 107.96052(64)# | 30(5) ms | β− | 108Zr | 6−# | ||
| β−, n? | 107Zr | ||||||||
| β−, 2n? | 106Zr | ||||||||
| 109Y | 39 | 70 | 108.96513(75)# | 25(5) ms | β− | 109Zr | 5/2+# | ||
| β−, n? | 108Zr | ||||||||
| β−, 2n? | 107Zr | ||||||||
| 110Y[4] | 39 | 71 | |||||||
| 111Y[4] | 39 | 72 | |||||||
- ↑ mY – 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).
- ↑ 4.0 4.1 4.2 # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
- ↑
Modes of decay:
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 Order of ground state and isomer is uncertain.
- ↑ Measured mass is 77.944220(16) Da.[2]
- ↑ 11.0 11.1 11.2 Fission product
See also
Daughter products other than yttrium
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.
- ↑ 2.0 2.1 Kimura, S.; Wada, M.; Fu, C. Y.; Fukuda, N.; Hirayama, Y.; Hou, D. S.; Iimura, S.; Ishiyama, H. et al. (8 October 2025). "Precision Mass Measurements around Mo 84 Rule Out ZrNb Cycle Formation in the Rapid Proton-Capture Process at Type I X-Ray Bursts". Physical Review Letters 135 (15). doi:10.1103/2dyn-q7wp. PMID 41138077.
- ↑ Xing, Y. M.; Yuan, C. X.; Wang, M.; Zhang, Y. H.; Zhou, X. H.; Litvinov, Yu. A.; Blaum, K.; Xu, H. S. et al. (11 January 2023). "Isochronous mass measurements of neutron-deficient nuclei from Sn 112 projectile fragmentation". Physical Review C 107 (1). doi:10.1103/PhysRevC.107.014304.
- ↑ 4.0 4.1 Sumikama, T. (2021). "Observation of new neutron-rich isotopes in the vicinity of 110Zr". Physical Review C 103 (1). doi:10.1103/PhysRevC.103.014614. Bibcode: 2021PhRvC.103a4614S. https://journals.aps.org/prc/abstract/10.1103/PhysRevC.103.014614.
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