ISOTOPES OF ERBIUM
Naturally occurring 'Erbium' ('Er') is composed of 6 stable isotopes, Er-162, Er-164, Er-166, Er-167, Er-168, and Er-170 with Er-166 being the most abundant (33.503% natural abundance). 29 radioisotopes have been characterized, with the most stable being Er-169 with a half life of 9.4 days, Er-172 with a half-life of 49.3 hours, Er-160 with a half-life of 28.58 hours, Er-165 with a half-life of 10.36 hours, and Er-171 with a half life of 7.516 hours. All of the remaining radioactive isotopes have half-lifes that are less than 3.5 hours, and the majority of these have half lifes that are less than 4 minutes. This element also has 13 meta states, with the most stable being Er-167m (t½ 2.269 seconds).
The isotopes of erbium range in atomic weight from 142.9663 u (Er-143) to 176.9541 u (Er-177). The primary decay mode before the most abundant stable isotope, Er-166, is electron capture, and the primary mode after is beta decay. The primary decay products before Er-166 are element 67 (holmium) isotopes, and the primary products after are element 69 (thulium) isotopes.
Standard atomic mass: 167.259(3) u
★ Geologically exceptional samples are known in which the isotopic composition lies outside the reported range. The uncertainty in the atomic mass may exceed the stated value for such specimens.
★ 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.
★ 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.
The isotopes of erbium range in atomic weight from 142.9663 u (Er-143) to 176.9541 u (Er-177). The primary decay mode before the most abundant stable isotope, Er-166, is electron capture, and the primary mode after is beta decay. The primary decay products before Er-166 are element 67 (holmium) isotopes, and the primary products after are element 69 (thulium) isotopes.
Standard atomic mass: 167.259(3) u
| Contents |
| Table |
| Notes |
| References |
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 | |||||||
| 143Er | 68 | 75 | 142.96634(64)# | 200# ms | 9/2-# | ||
| 144Er | 68 | 76 | 143.96038(43)# | 400# ms [>200 ns] | 0+ | ||
| 145Er | 68 | 77 | 144.95739(43)# | 900(300) ms | 1/2+# | ||
| 146Er | 68 | 78 | 145.95200(32)# | 1.7(6) s | 0+ | ||
| 147Er | 68 | 79 | 146.94949(32)# | ~2.5 s | (1/2+) | ||
| 147mEr | 100(50)# keV | 2.5(2) s | (11/2-) | ||||
| 148Er | 68 | 80 | 147.94455(21)# | 4.6(2) s | 0+ | ||
| 149Er | 68 | 81 | 148.94231(3) | 4(2) s | (1/2+) | ||
| 149m1Er | 741.8(2) keV | 8.9(2) s | (11/2-) | ||||
| 149m2Er | 2611.1(3) keV | 0.61(8) µs | (19/2+) | ||||
| 149m3Er | 3242.7+X keV | 4.8(1) µs | (27/2-) | ||||
| 150Er | 68 | 82 | 149.937914(18) | 18.5(7) s | 0+ | ||
| 151Er | 68 | 83 | 150.937449(18) | 23.5(13) s | (7/2-) | ||
| 151m1Er | 2585.5(6) keV | 580(20) ms | (27/2-) | ||||
| 151m2Er | 10286+X keV | 0.42(5) µs | (67/2,69/2,71/2) | ||||
| 152Er | 68 | 84 | 151.935050(11) | 10.3(1) s | 0+ | ||
| 153Er | 68 | 85 | 152.935063(9) | 37.1(2) s | 7/2(-) | ||
| 154Er | 68 | 86 | 153.932783(6) | 3.73(9) min | 0+ | ||
| 155Er | 68 | 87 | 154.933209(7) | 5.3(3) min | 7/2- | ||
| 156Er | 68 | 88 | 155.931065(26) | 19.5(10) min | 0+ | ||
| 157Er | 68 | 89 | 156.93192(3) | 18.65(10) min | 3/2- | ||
| 157mEr | 155.4(3) keV | 76(6) ms | (9/2+) | ||||
| 158Er | 68 | 90 | 157.929893(27) | 2.29(6) h | 0+ | ||
| 159Er | 68 | 91 | 158.930684(5) | 36(1) min | 3/2- | ||
| 159m1Er | 182.602(24) keV | 337(14) ns | 9/2+ | ||||
| 159m2Er | 429.05(3) keV | 590(60) ns | 11/2- | ||||
| 160Er | 68 | 92 | 159.929083(26) | 28.58(9) h | 0+ | ||
| 161Er | 68 | 93 | 160.929995(10) | 3.21(3) h | 3/2- | ||
| 161mEr | 396.44(4) keV | 7.5(7) µs | 11/2- | ||||
| 162Er | 68 | 94 | 161.928778(4) | STABLE [>140E+12 a] | 0+ | 0.00139(5) | |
| 163Er | 68 | 95 | 162.930033(6) | 75.0(4) min | 5/2- | ||
| 163mEr | 445.5(6) keV | 580(100) ns | (11/2-) | ||||
| 164Er | 68 | 96 | 163.929200(3) | STABLE | 0+ | 0.01601(3) | |
| 165Er | 68 | 97 | 164.930726(3) | 10.36(4) h | 5/2- | ||
| 166Er | 68 | 98 | 165.9302931(27) | STABLE | 0+ | 0.33503(36) | |
| 167Er | 68 | 99 | 166.9320482(27) | STABLE | 7/2+ | 0.22869(9) | |
| 167mEr | 207.801(5) keV | 2.269(6) s | 1/2- | ||||
| 168Er | 68 | 100 | 167.9323702(27) | STABLE | 0+ | 0.26978(18) | |
| 169Er | 68 | 101 | 168.9345904(27) | 9.392(18) d | 1/2- | ||
| 170Er | 68 | 102 | 169.9354643(30) | STABLE [>320E+15 a] | 0+ | 0.14910(36) | |
| 171Er | 68 | 103 | 170.9380298(30) | 7.516(2) h | 5/2- | ||
| 171mEr | 198.6(1) keV | 210(10) ns | 1/2- | ||||
| 172Er | 68 | 104 | 171.939356(5) | 49.3(3) h | 0+ | ||
| 173Er | 68 | 105 | 172.94240(21)# | 1.434(17) min | (7/2-) | ||
| 174Er | 68 | 106 | 173.94423(32)# | 3.2(2) min | 0+ | ||
| 175Er | 68 | 107 | 174.94777(43)# | 1.2(3) min | (9/2+) | ||
| 176Er | 68 | 108 | 175.95008(43)# | 20# s | 0+ | ||
| 177Er | 68 | 109 | 176.95405(54)# | 3# s | 1/2-# | ||
Notes
★ Geologically exceptional samples are known in which the isotopic composition lies outside the reported range. The uncertainty in the atomic mass may exceed the stated value for such specimens.
★ 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.
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.
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