Isotopes of yttrium
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Natural yttrium (Y) is composed of only one isotope (Y-89). The most stable radioisotopes are Y-88 which has a half life of 106.65 days and Y-91 with a half life of 58.51 days. All the other isotopes have half lives of less than a day except Y-87 which has a half life of 79.8 hours. The dominant decay mode below the stable Y-89 is electron capture and the dominant mode after it is beta emission. Twenty six unstable isotopes have been characterized.
Y-90 exists in equilibrium with its parent isotope strontium-90, which is a product of nuclear explosions.
Standard atomic mass: 88.90585(2) u
[edit] Table
nuclide symbol |
Z(p) | N(n) | isotopic mass (u) |
half-life | nuclear spin |
representative isotopic composition (mole fraction) |
range of natural variation (mole fraction) |
---|---|---|---|---|---|---|---|
excitation energy | |||||||
76Y | 39 | 37 | 75.95845(54)# | 500# ns [>170 ns] | |||
77Y | 39 | 38 | 76.94965(7)# | 63(17) ms | 5/2+# | ||
78Y | 39 | 39 | 77.94361(43)# | 54(5) ms | (0+) | ||
78mY | 0(500)# keV | 5.8(5) s | 5+# | ||||
79Y | 39 | 40 | 78.93735(48) | 14.8(6) s | (5/2+)# | ||
80Y | 39 | 41 | 79.93428(19) | 30.1(5) s | 4- | ||
80m1Y | 228.5(1) keV | 4.8(3) s | (1-) | ||||
80m2Y | 312.6(9) keV | 4.7(3) µs | (2+) | ||||
81Y | 39 | 42 | 80.92913(7) | 70.4(10) s | (5/2+) | ||
82Y | 39 | 43 | 81.92679(11) | 8.30(20) s | 1+ | ||
82m1Y | 402.63(14) keV | 268(25) ns | 4- | ||||
82m2Y | 507.50(13) keV | 147(7) ns | 6+ | ||||
83Y | 39 | 44 | 82.92235(5) | 7.08(6) min | 9/2+ | ||
83mY | 61.98(11) keV | 2.85(2) min | (3/2-) | ||||
84Y | 39 | 45 | 83.92039(10) | 4.6(2) s | 1+ | ||
84mY | -80(190) keV | 39.5(8) min | (5-) | ||||
85Y | 39 | 46 | 84.916433(20) | 2.68(5) h | (1/2)- | ||
85m1Y | 19.8(5) keV | 4.86(13) h | 9/2+ | ||||
85m2Y | 266.30(20) keV | 178(6) ns | 5/2- | ||||
86Y | 39 | 47 | 85.914886(15) | 14.74(2) h | 4- | ||
86m1Y | 218.30(20) keV | 48(1) min | (8+) | ||||
86m2Y | 302.2(5) keV | 125(6) ns | (7-) | ||||
87Y | 39 | 48 | 86.9108757(17) | 79.8(3) h | 1/2- | ||
87mY | 380.82(7) keV | 13.37(3) h | 9/2+ | ||||
88Y | 39 | 49 | 87.9095011(20) | 106.616(13) d | 4- | ||
88m1Y | 674.55(4) keV | 13.9(2) ms | (8)+ | ||||
88m2Y | 392.86(9) keV | 300(3) µs | 1+ | ||||
89Y | 39 | 50 | 88.9058483(27) | STABLE | 1/2- | 1.0000 | |
89mY | 908.97(3) keV | 15.663(5) s | 9/2+ | ||||
90Y | 39 | 51 | 89.9071519(27) | 64.053(20) h | 2- | ||
90mY | 681.67(10) keV | 3.19(6) h | 7+ | ||||
91Y | 39 | 52 | 90.907305(3) | 58.51(6) d | 1/2- | ||
91mY | 555.58(5) keV | 49.71(4) min | 9/2+ | ||||
92Y | 39 | 53 | 91.908949(10) | 3.54(1) h | 2- | ||
93Y | 39 | 54 | 92.909583(11) | 10.18(8) h | 1/2- | ||
93mY | 758.719(21) keV | 820(40) ms | 7/2+ | ||||
94Y | 39 | 55 | 93.911595(8) | 18.7(1) min | 2- | ||
95Y | 39 | 56 | 94.912821(8) | 10.3(1) min | 1/2- | ||
96Y | 39 | 57 | 95.915891(25) | 5.34(5) s | 0- | ||
96mY | 1140(30) keV | 9.6(2) s | (8)+ | ||||
97Y | 39 | 58 | 96.918134(13) | 3.75(3) s | (1/2-) | ||
97m1Y | 667.51(23) keV | 1.17(3) s | (9/2)+ | ||||
97m2Y | 3523.3(4) keV | 142(8) ms | (27/2-) | ||||
98Y | 39 | 59 | 97.922203(26) | 0.548(2) s | (0)- | ||
98m1Y | 170.74(6) keV | 620(80) ns | (2)- | ||||
98m2Y | 410(30) keV | 2.0(2) s | (5+,4-) | ||||
98m3Y | 496.19(15) keV | 7.6(4) µs | (2-) | ||||
98m4Y | 1181.1(4) keV | 0.83(10) µs | (8-) | ||||
99Y | 39 | 60 | 98.924636(26) | 1.470(7) s | (5/2+) | ||
99mY | 2141.65(19) keV | 8.6(8) µs | (17/2+) | ||||
100Y | 39 | 61 | 99.92776(8) | 735(7) ms | 1-,2- | ||
100mY | 200(200)# keV | 940(30) ms | (3,4,5)(+#) | ||||
101Y | 39 | 62 | 100.93031(10) | 426(20) ms | (5/2+) | ||
102Y | 39 | 63 | 101.93356(9) | 0.30(1) s | |||
102mY | 200(200)# keV | 360(40) ms | high | ||||
103Y | 39 | 64 | 102.93673(32)# | 224(19) ms | 5/2+# | ||
104Y | 39 | 65 | 103.94105(43)# | 180(60) ms | |||
105Y | 39 | 66 | 104.94487(54)# | 60# ms [>300 ns] | 5/2+# | ||
106Y | 39 | 67 | 105.94979(75)# | 50# ms [>300 ns] | |||
107Y | 39 | 68 | 106.95414(54)# | 30# ms [>300 ns] | 5/2+# | ||
108Y | 39 | 69 | 107.95948(86)# | 20# [>300 ns] |
[edit] 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.
[edit] References
- Isotope masses from Ame2003 Atomic Mass Evaluation by G. Audi, A.H. Wapstra, C. Thibault, J. Blachot and O. Bersillon in Nuclear Physics A729 (2003).
- Isotopic compositions and standard atomic masses from Atomic weights of the elements. Review 2000 (IUPAC Technical Report). Pure Appl. Chem. Vol. 75, No. 6, pp. 683-800, (2003) and Atomic Weights Revised (2005).
- Half-life, spin, and isomer data selected from these sources. Editing notes on this article's talk page.
- Audi, Bersillon, Blachot, Wapstra. The Nubase2003 evaluation of nuclear and decay properties, Nuc. Phys. A 729, pp. 3-128 (2003).
- National Nuclear Data Center, Brookhaven National Laboratory. Information extracted from the NuDat 2.1 database (retrieved Sept. 2005).
- David R. Lide (ed.), Norman E. Holden in CRC Handbook of Chemistry and Physics, 85th Edition, online version. CRC Press. Boca Raton, Florida (2005). Section 11, Table of the Isotopes.
Isotopes of strontium | Isotopes of yttrium | Isotopes of zirconium |
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