Isotopes of rubidium
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Standard atomic weight (Ar) |
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Rubidium (37Rb) has 32 isotopes, with naturally occurring rubidium being composed of just two isotopes; 85Rb (72.2%) and the radioactive 87Rb (27.8%). Normal mixes of rubidium are radioactive enough to fog photographic film in approximately 30 to 60 days.
87Rb has a half-life of 4.92×1010 years. It readily substitutes for potassium in minerals, and is therefore fairly widespread. 87Rb has been used extensively in dating rocks; 87Rb decays to stable strontium-87 by emission of a negative beta particle, i.e. an electron ejected from the nucleus. During fractional crystallization, Sr tends to become concentrated in plagioclase, leaving Rb in the liquid phase. Hence, the Rb/Sr ratio in residual magma may increase over time, resulting in rocks with increasing Rb/Sr ratios with increasing differentiation. Highest ratios (10 or higher) occur in pegmatites. If the initial amount of Sr is known or can be extrapolated, the age can be determined by measurement of the Rb and Sr concentrations and the 87Sr/86Sr ratio. The dates indicate the true age of the minerals only if the rocks have not been subsequently altered. See rubidium-strontium dating for a more detailed discussion.
Other than 87Rb, the longest-lived radioisotopes are 83Rb with a half-life of 86.2 days, 84Rb with a half-life of 33.1 days and 86Rb with a half-life of 18.642 days. All other radioisotopes have half-lives less than a day.
82Rb is used in some cardiac PET scans to assess myocardial perfusion. It has a half-life of 1.273 minutes. It does not exist naturally, but can be made from the decay of 82Sr.
Rubidium-87
Rubidium-87 is an isotope of rubidium. Rubidium-87 was the first and the most popular atom for making Bose–Einstein condensates in dilute atomic gases. Even though rubidium-85 is more abundant, rubidium-87 has a positive scattering length, which means it is mutually repulsive, at low temperatures. This prevents a collapse of all but the smallest condensates. It is also easy to evaporatively cool, with a consistent strong mutual scattering. There is also a strong supply of cheap uncoated diode lasers typically used in CD writers, which can operate at the correct wavelength.
Rubidium-87 has an atomic mass of 86.9091835 u, and a binding energy of 757,853 keV. Its atomic percent abundance is 27.835%, and has a half-life of ×1010 years. 4.92
List of isotopes
nuclide symbol |
Z(p) | N(n) | isotopic mass (u) |
half-life[n 1] | decay mode(s)[2][n 2] |
daughter isotope(s)[n 3] |
nuclear spin |
representative isotopic composition (mole fraction) |
range of natural variation (mole fraction) |
---|---|---|---|---|---|---|---|---|---|
excitation energy | |||||||||
71Rb | 37 | 34 | 70.96532(54)# | p | 70Kr | 5/2−# | |||
72Rb | 37 | 35 | 71.95908(54)# | <1.5 µs | p | 71Kr | 3+# | ||
72mRb | 100(100)# keV | 1# µs | p | 71Kr | 1−# | ||||
73Rb | 37 | 36 | 72.95056(16)# | <30 ns | p | 72Kr | 3/2−# | ||
74Rb | 37 | 37 | 73.944265(4) | 64.76(3) ms | β+ | 74Kr | (0+) | ||
75Rb | 37 | 38 | 74.938570(8) | 19.0(12) s | β+ | 75Kr | (3/2−) | ||
76Rb | 37 | 39 | 75.9350722(20) | 36.5(6) s | β+ | 76Kr | 1(−) | ||
β+, α (3.8×10−7%) | 72Se | ||||||||
76mRb | 316.93(8) keV | 3.050(7) µs | (4+) | ||||||
77Rb | 37 | 40 | 76.930408(8) | 3.77(4) min | β+ | 77Kr | 3/2− | ||
78Rb | 37 | 41 | 77.928141(8) | 17.66(8) min | β+ | 78Kr | 0(+) | ||
78mRb | 111.20(10) keV | 5.74(5) min | β+ (90%) | 78Kr | 4(−) | ||||
IT (10%) | 78Rb | ||||||||
79Rb | 37 | 42 | 78.923989(6) | 22.9(5) min | β+ | 79Kr | 5/2+ | ||
80Rb | 37 | 43 | 79.922519(7) | 33.4(7) s | β+ | 80Kr | 1+ | ||
80mRb | 494.4(5) keV | 1.6(2) µs | 6+ | ||||||
81Rb | 37 | 44 | 80.918996(6) | 4.570(4) h | β+ | 81Kr | 3/2− | ||
81mRb | 86.31(7) keV | 30.5(3) min | IT (97.6%) | 81Rb | 9/2+ | ||||
β+ (2.4%) | 81Kr | ||||||||
82Rb | 37 | 45 | 81.9182086(30) | 1.273(2) min | β+ | 82Kr | 1+ | ||
82mRb | 69.0(15) keV | 6.472(5) h | β+ (99.67%) | 82Kr | 5− | ||||
IT (.33%) | 82Rb | ||||||||
83Rb | 37 | 46 | 82.915110(6) | 86.2(1) d | EC | 83Kr | 5/2− | ||
83mRb | 42.11(4) keV | 7.8(7) ms | IT | 83Rb | 9/2+ | ||||
84Rb | 37 | 47 | 83.914385(3) | 33.1(1) d | β+ (96.2%) | 84Kr | 2− | ||
β− (3.8%) | 84Sr | ||||||||
84mRb | 463.62(9) keV | 20.26(4) min | IT (>99.9%) | 84Rb | 6− | ||||
β+ (<.1%) | 84Kr | ||||||||
85Rb[n 4] | 37 | 48 | 84.911789738(12) | Stable | 5/2− | 0.7217(2) | |||
86Rb | 37 | 49 | 85.91116742(21) | 18.642(18) d | β− (99.9948%) | 86Sr | 2− | ||
EC (.0052%) | 86Kr | ||||||||
86mRb | 556.05(18) keV | 1.017(3) min | IT | 86Rb | 6− | ||||
87Rb[n 5][n 6][n 4] | 37 | 50 | 86.909180527(13) | 4.923(22)×1010 y | β− | 87Sr | 3/2− | 0.2783(2) | |
88Rb | 37 | 51 | 87.91131559(17) | 17.773(11) min | β− | 88Sr | 2− | ||
89Rb | 37 | 52 | 88.912278(6) | 15.15(12) min | β− | 89Sr | 3/2− | ||
90Rb | 37 | 53 | 89.914802(7) | 158(5) s | β− | 90Sr | 0− | ||
90mRb | 106.90(3) keV | 258(4) s | β− (97.4%) | 90Sr | 3− | ||||
IT (2.6%) | 90 Rb | ||||||||
91Rb | 37 | 54 | 90.916537(9) | 58.4(4) s | β− | 91Sr | 3/2(−) | ||
92Rb | 37 | 55 | 91.919729(7) | 4.492(20) s | β− (99.98%) | 92Sr | 0− | ||
β−, n (.0107%) | 91Sr | ||||||||
93Rb | 37 | 56 | 92.922042(8) | 5.84(2) s | β− (98.65%) | 93Sr | 5/2− | ||
β−, n (1.35%) | 92Sr | ||||||||
93mRb | 253.38(3) keV | 57(15) µs | (3/2−,5/2−) | ||||||
94Rb | 37 | 57 | 93.926405(9) | 2.702(5) s | β− (89.99%) | 94Sr | 3(−) | ||
β−, n (10.01%) | 93Sr | ||||||||
95Rb | 37 | 58 | 94.929303(23) | 377.5(8) ms | β− (91.27%) | 95Sr | 5/2− | ||
β−, n (8.73%) | 94Sr | ||||||||
96Rb | 37 | 59 | 95.93427(3) | 202.8(33) ms | β− (86.6%) | 96Sr | 2+ | ||
β−, n (13.4%) | 95Sr | ||||||||
96mRb | 0(200)# keV | 200# ms [>1 ms] | β− | 96Sr | 1(−#) | ||||
IT | 96Rb | ||||||||
β−, n | 95Sr | ||||||||
97Rb | 37 | 60 | 96.93735(3) | 169.9(7) ms | β− (74.3%) | 97Sr | 3/2+ | ||
β−, n (25.7%) | 96Sr | ||||||||
98Rb | 37 | 61 | 97.94179(5) | 114(5) ms | β−(86.14%) | 98Sr | (0,1)(−#) | ||
β−, n (13.8%) | 97Sr | ||||||||
β−, 2n (.051%) | 96Sr | ||||||||
98mRb | 290(130) keV | 96(3) ms | β− | 97Sr | (3,4)(+#) | ||||
99Rb | 37 | 62 | 98.94538(13) | 50.3(7) ms | β− (84.1%) | 99Sr | (5/2+) | ||
β−, n (15.9%) | 98Sr | ||||||||
100Rb | 37 | 63 | 99.94987(32)# | 51(8) ms | β− (94.25%) | 100Sr | (3+) | ||
β−, n (5.6%) | 99Sr | ||||||||
β−, 2n (.15%) | 98Sr | ||||||||
101Rb | 37 | 64 | 100.95320(18) | 32(5) ms | β− (69%) | 101Sr | (3/2+)# | ||
β−, n (31%) | 100Sr | ||||||||
102Rb | 37 | 65 | 101.95887(54)# | 37(5) ms | β− (82%) | 102Sr | |||
β−, n (18%) | 101Sr |
- ↑ Bold for isotopes with half-lives longer than the age of the universe (nearly stable)
- ↑ Abbreviations:
EC: Electron capture
IT: Isomeric transition - ↑ Bold for stable isotopes
- 1 2 Fission product
- ↑ Primordial radionuclide
- ↑ Used in rubidium-strontium dating
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
- ↑ Meija, J.; et al. (2016). "Atomic weights of the elements 2013 (IUPAC Technical Report)". Pure Appl. Chem. 88 (3): 265–91. doi:10.1515/pac-2015-0305.
- ↑ "Universal Nuclide Chart". nucleonica. (Registration required (help)).
- Isotope masses from:
- 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.
- Isotopic compositions and standard atomic masses from:
- 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.
- 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.
- Half-life, spin, and isomer data selected from the following sources. See editing notes on this article's talk page.
- 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.
- National Nuclear Data Center. "NuDat 2.1 database". Brookhaven National Laboratory. Retrieved September 2005. Check date values in:
|access-date=
(help) - N. E. Holden (2004). "Table of the Isotopes". In D. R. Lide. CRC Handbook of Chemistry and Physics (85th ed.). CRC Press. Section 11. ISBN 978-0-8493-0485-9.
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