Isotopes of ruthenium
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Naturally occurring
radioisotopes, the most stable are 106Ru, with a half-life
of 373.59 days; 103Ru, with a half-life of 39.26 days and 97Ru, with a half-life of 2.9 days.
Twenty-four other radioisotopes have been characterized with
u
(87Ru) to 119.95 u (120Ru). Most of these have half-lives that are less than five minutes, except 94Ru (half-life: 51.8 minutes), 95Ru (half-life: 1.643 hours), and 105Ru (half-life: 4.44 hours).
The primary
beta emission. The primary decay product before 102Ru is technetium and the primary product after is rhodium
.
Because of the very high volatility of ruthenium tetroxide (RuO
4) ruthenium radioactive isotopes with their relative short half-life are considered as the second most hazardous gaseous isotopes after iodine-131 in case of release by a nuclear accident.[4][5][6] The two most important isotopes of ruthenium in case of nuclear accident are these with the longest half-life: 103Ru (39.26 days) and 106Ru (373.59 days).[5]
List of isotopes
Nuclide [n 1] |
Z | N | Isotopic mass (Da) [n 2][n 3] |
Half-life [n 4] |
Daughter isotope [n 6] |
Natural abundance (mole fraction) | |||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Excitation energy[n 4] | Normal proportion | Range of variation | |||||||||||||||||
87Ru | 44 | 43 | 86.94918(64)# | 50# ms [>1.5 µs] | β+ | 87Tc | 1/2−# | ||||||||||||
88Ru | 44 | 44 | 87.94026(43)# | 1.3(3) s [1.2(+3−2) s] | β+ | 88Tc | 0+ | ||||||||||||
89Ru | 44 | 45 | 88.93611(54)# | 1.38(11) s | β+ | 89Tc | (7/2)(+#) | ||||||||||||
90Ru | 44 | 46 | 89.92989(32)# | 11.7(9) s | β+ | 90Tc | 0+ | ||||||||||||
91Ru | 44 | 47 | 90.92629(63)# | 7.9(4) s | β+ | 91Tc | (9/2+) | ||||||||||||
91mRu | 80(300)# keV | 7.6(8) s | β+ (>99.9%) | 91Tc | (1/2−) | ||||||||||||||
IT (<.1%)
|
91Ru | ||||||||||||||||||
β+, p (<.1%) | 90Mo | ||||||||||||||||||
92Ru | 44 | 48 | 91.92012(32)# | 3.65(5) min | β+ | 92Tc | 0+ | ||||||||||||
93Ru | 44 | 49 | 92.91705(9) | 59.7(6) s | β+ | 93Tc | (9/2)+ | ||||||||||||
93m1Ru | 734.40(10) keV | 10.8(3) s | β+ (78%) | 93Tc | (1/2)− | ||||||||||||||
IT (22%) | 93Ru | ||||||||||||||||||
β+, p (.027%) | 92Mo | ||||||||||||||||||
93m2Ru | 2082.6(9) keV | 2.20(17) µs | (21/2)+ | ||||||||||||||||
94Ru | 44 | 50 | 93.911360(14) | 51.8(6) min | β+ | 94Tc | 0+ | ||||||||||||
94mRu | 2644.55(25) keV | 71(4) µs | (8+) | ||||||||||||||||
95Ru | 44 | 51 | 94.910413(13) | 1.643(14) h | β+ | 95Tc | 5/2+ | ||||||||||||
96Ru | 44 | 52 | 95.907598(8) | Observationally Stable[n 8]
|
0+ | 0.0554(14) | |||||||||||||
97Ru | 44 | 53 | 96.907555(9) | 2.791(4) d | β+ | 97mTc | 5/2+ | ||||||||||||
98Ru | 44 | 54 | 97.905287(7) | Stable | 0+ | 0.0187(3) | |||||||||||||
99Ru | 44 | 55 | 98.9059393(22) | Stable | 5/2+ | 0.1276(14) | |||||||||||||
100Ru | 44 | 56 | 99.9042195(22) | Stable | 0+ | 0.1260(7) | |||||||||||||
101Ru[n 9] | 44 | 57 | 100.9055821(22) | Stable | 5/2+ | 0.1706(2) | |||||||||||||
101mRu | 527.56(10) keV | 17.5(4) µs | 11/2− | ||||||||||||||||
102Ru[n 9] | 44 | 58 | 101.9043493(22) | Stable | 0+ | 0.3155(14) | |||||||||||||
103Ru[n 9] | 44 | 59 | 102.9063238(22) | 39.26(2) d | β− | 103Rh | 3/2+ | ||||||||||||
103mRu | 238.2(7) keV | 1.69(7) ms | IT | 103Ru | 11/2− | ||||||||||||||
104Ru[n 9] | 44 | 60 | 103.905433(3) | Observationally Stable[n 10] | 0+ | 0.1862(27) | |||||||||||||
105Ru[n 9] | 44 | 61 | 104.907753(3) | 4.44(2) h | β− | 105Rh | 3/2+ | ||||||||||||
106Ru[n 9] | 44 | 62 | 105.907329(8) | 373.59(15) d | β− | 106Rh | 0+ | ||||||||||||
107Ru | 44 | 63 | 106.90991(13) | 3.75(5) min | β− | 107Rh | (5/2)+ | ||||||||||||
108Ru | 44 | 64 | 107.91017(12) | 4.55(5) min | β− | 108Rh | 0+ | ||||||||||||
109Ru | 44 | 65 | 108.91320(7) | 34.5(10) s | β− | 109Rh | (5/2+)# | ||||||||||||
110Ru | 44 | 66 | 109.91414(6) | 11.6(6) s | β− | 110Rh | 0+ | ||||||||||||
111Ru | 44 | 67 | 110.91770(8) | 2.12(7) s | β− | 111Rh | (5/2+) | ||||||||||||
112Ru | 44 | 68 | 111.91897(8) | 1.75(7) s | β− | 112Rh | 0+ | ||||||||||||
113Ru | 44 | 69 | 112.92249(8) | 0.80(5) s | β− | 113Rh | (5/2+) | ||||||||||||
113mRu | 130(18) keV | 510(30) ms | (11/2−) | ||||||||||||||||
114Ru | 44 | 70 | 113.92428(25)# | 0.53(6) s | β− (>99.9%) | 114Rh | 0+ | ||||||||||||
β−, n (<.1%) | 113Rh | ||||||||||||||||||
115Ru | 44 | 71 | 114.92869(14) | 740(80) ms | β− (>99.9%) | 115Rh | |||||||||||||
β−, n (<.1%) | 114Rh | ||||||||||||||||||
116Ru | 44 | 72 | 115.93081(75)# | 400# ms [>300 ns] | β− | 116Rh | 0+ | ||||||||||||
117Ru | 44 | 73 | 116.93558(75)# | 300# ms [>300 ns] | β− | 117Rh | |||||||||||||
118Ru | 44 | 74 | 117.93782(86)# | 200# ms [>300 ns] | β− | 118Rh | 0+ | ||||||||||||
119Ru | 44 | 75 | 118.94284(75)# | 170# ms [>300 ns] | |||||||||||||||
120Ru | 44 | 76 | 119.94531(86)# | 80# ms [>300 ns] | 0+ | ||||||||||||||
This table header & footer: |
- ^ mRu – 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:
IT: Isomeric transitionn: Neutron emission p: Proton emission - ^ Bold symbol as daughter – Daughter product is stable.
- ^ ( ) spin value – Indicates spin with weak assignment arguments.
- ^ Believed to undergo β+β+ decay to 96Mo with a half-life over 6.7×1016 years
- ^ Fission product
- ^ Believed to undergo β−β− decay to 104Pd
- 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.[citation needed]
- In September 2017 an estimated amount of 100 to 300 TBq (0.3 to 1 g) of 106Ru was released in Russia, probably in the Ural region. It was, after ruling out release from a reentering satellite, concluded that the source is to be found either in nuclear fuel cycle facilities or radioactive source production. In France levels up to 0.036mBq/m3 of air were measured. It is estimated that over distances of the order of a few tens of kilometres around the location of the release levels may exceed the limits for non-dairy foodstuffs.[7]
References
- .
- ^ "Standard Atomic Weights: Ruthenium". CIAAW. 1983.
- ISSN 1365-3075.
- ^ Ronneau, C., Cara, J., & Rimski-Korsakov, A. (1995). Oxidation-enhanced emission of ruthenium from nuclear fuel. Journal of Environmental Radioactivity, 26(1), 63-70.
- ^ a b Backman, U., Lipponen, M., Auvinen, A., Jokiniemi, J., & Zilliacus, R. (2004). Ruthenium behaviour in severe nuclear accident conditions. Final report (No. NKS–100). Nordisk Kernesikkerhedsforskning.
- ^ Beuzet, E., Lamy, J. S., Perron, H., Simoni, E., & Ducros, G. (2012). Ruthenium release modelling in air and steam atmospheres under severe accident conditions using the MAAP4 code[dead link]. Nuclear Engineering and Design, 246, 157-162.
- ^ [1] Detection of ruthenium 106 in France and in Europe, IRSN France (9 Nov 2017)
- Isotope masses from:
- Audi, Georges; Bersillon, Olivier; Blachot, Jean;
- Isotopic compositions and standard atomic masses from:
- .
- Wieser, Michael E. (2006). "Atomic weights of the elements 2005 (IUPAC Technical Report)". .
- "News & Notices: Standard Atomic Weights Revised". International Union of Pure and Applied Chemistry. 19 October 2005.
- Half-life, spin, and isomer data selected from the following sources.
- Audi, Georges; Bersillon, Olivier; Blachot, Jean;
- National Nuclear Data Center. "NuDat 2.x database". Brookhaven National Laboratory.
- Holden, Norman E. (2004). "11. Table of the Isotopes". In Lide, David R. (ed.). ISBN 978-0-8493-0485-9.