More Chemistry
All atomic nuclei of the chemical element ruthenium are summarized under ruthenium isotopes; these all consist of an atomic nucleus with 44 protons and, in the uncharged state, 44 electrons. The difference between each ruthenium isotope is based on the number of neutrons in the nucleus.
Natural ruthenium deposits consist of a mixture of seven different stable isotopes:
Atomic Mass ma | Quantity | Half-life | Spin | |
Ruthenium Isotopic mixture | 101,07 u | 100 % | ||
Isotope 96Ru | 95,907590(3) u | 5,54(14) % | stable | 0+ |
Isotope 98Ru | 97,90529(5) u | 1,87(3) % | stable | 0+ |
Isotope 99Ru | 98,905934(7) u | 12,76(14) % | stable | 5/2+ |
Isotope 100Ru | 99,904214(7) u | 12,60(7) % | stable | 0+ |
Isotope 101Ru | 100,905577(8) u | 17,06(2) % | stable | 5/2+ |
Isotope 102Ru | 101,904344(8) u | 31,55(14) % | stable | 0+ |
Isotope 104Ru | 103,90543(2) u | 18,62(27) % | stable | 0+ |
All other ruthenium nuclides known and characterized to date are unstable and have no significance for technical applications.
Isotope Nuclide | E | N | Atomic Mass [Nuclear Mass] {Mass Excess} | Spin I (h/2π) | Parent |
---|---|---|---|---|---|
1 | 2 | 3 | 4 | 5 | 6 |
Ruthenium-85 | 8544Ru | 41 | 84.96677(54) u [84.9426337 u] {-30.95355 MeV} | ||
Ruthenium-86 | 8644Ru | 42 | 85.95730(43) u [85.9331637 u] {-39.77479 MeV} | 0+ | |
Ruthenium-87 | 8744Ru | 43 | 86.94918(64) u [86.9250437 u] {-47.33853 MeV} | ||
Ruthenium-88 | 8844Ru | 44 | 87.94166(32) u [87.9175237 u] {-54.34336 MeV} | 0+ | |
Ruthenium-89 | 8944Ru | 45 | 88.93745(32) u [88.9133137 u] {-58.26495 MeV} | (9/2+) | |
Ruthenium-90 | 9044Ru | 46 | 89.930344(4) u [89.9062077 u] {-64.88415 MeV} | 0+ | |
Ruthenium-91 | 9144Ru | 47 | 90.9267415(24) u [90.9026052 u] {-68.23985 MeV} | (9/2+) | |
Ruthenium-91m | 91m44Ru | 47 | 90.9267415(24) u [90.9026052 u] {-68.23985 MeV} | (1/2-) | |
Ruthenium-92 | 9244Ru | 48 | 91.9202344(24) u [91.8960981 u] {-74.30118 MeV} | 0+ | 92Rh 93Pd |
Ruthenium-93 | 9344Ru | 49 | 92.9171044(22) u [92.8929681 u] {-77.21675 MeV} | (9/2)+ | |
Ruthenium-93m1 | 93m144Ru | 49 | 92.9171044(22) u [92.8929681 u] {-77.21675 MeV} | (1/2)- | |
Ruthenium-93m2 | 93m244Ru | 49 | 92.9171044(22) u [92.8929681 u] {-77.21675 MeV} | (21/2)+ | |
Ruthenium-94 | 9444Ru | 50 | 93.911343(3) u [93.8872067 u] {-82.58346 MeV} | 0+ | 94Rh 95Pd |
Ruthenium-94m | 94m44Ru | 50 | 93.911343(3) u [93.8872067 u] {-82.58346 MeV} | 8+ | |
Ruthenium-95 | 9544Ru | 51 | 94.910404(10) u [94.8862677 u] {-83.45814 MeV} | 5/2+ | 95Rh |
Ruthenium-96 | 9644Ru | 52 | 95.907590(3) u [95.8834537 u] {-86.07936 MeV} | 0+ | 96Rh |
Ruthenium-97 | 9744Ru | 53 | 96.907546(3) u [96.8834097 u] {-86.12035 MeV} | 5/2+ | 97Rh |
Ruthenium-98 | 9844Ru | 54 | 97.90529(5) u [97.8811537 u] {-88.2218 MeV} | 0+ | 98Rh 98Tc |
Ruthenium-99 | 9944Ru | 55 | 98.905934(7) u [98.8817977 u] {-87.62191 MeV} | 5/2+ | 99Rh 99Tc |
Ruthenium-100 | 10044Ru | 56 | 99.904214(7) u [99.8800777 u] {-89.22408 MeV} | 0+ | 100Rh 100Tc 100Mo |
Ruthenium-101 | 10144Ru | 57 | 100.905577(8) u [100.8814407 u] {-87.95446 MeV} | 5/2+ | 101Rh 101Tc |
Ruthenium-101m | 101m44Ru | 57 | 100.905577(8) u [100.8814407 u] {-87.95446 MeV} | 11/2- | |
Ruthenium-102 | 10244Ru | 58 | 101.904344(8) u [101.8802077 u] {-89.10299 MeV} | 0+ | 102Rh 102Tc |
Ruthenium-103 | 10344Ru | 59 | 102.9063148(5) u [102.8821785 u] {-87.2672 MeV} | 3/2+ | 103Tc |
Ruthenium-103m | 103m44Ru | 59 | 102.9063148(5) u [102.8821785 u] {-87.2672 MeV} | 11/2- | |
Ruthenium-104 | 10444Ru | 60 | 103.90543(2) u [103.8812937 u] {-88.09139 MeV} | 0+ | 104Rh 104Tc |
Ruthenium-105 | 10544Ru | 61 | 104.9077455(27) u [104.8836092 u] {-85.93451 MeV} | 3/2+ | 105Tc |
Ruthenium-105m | 105m44Ru | 61 | 104.9077455(27) u [104.8836092 u] {-85.93451 MeV} | (5/2)+ | |
Ruthenium-106 | 10644Ru | 62 | 105.907328(6) u [105.8831917 u] {-86.32341 MeV} | 0+ | 106Tc |
Ruthenium-107 | 10744Ru | 63 | 106.909970(9) u [106.8858337 u] {-83.8624 MeV} | (5/2)+ | 107Tc |
Ruthenium-108 | 10844Ru | 64 | 107.910186(9) u [107.8860497 u] {-83.6612 MeV} | 0+ | 108Tc 252Cf |
Ruthenium-109 | 10944Ru | 65 | 108.913324(10) u [108.8891877 u] {-80.73817 MeV} | (5/2+) | 109Tc 252Cf |
Ruthenium-109m | 109m44Ru | 65 | 108.913324(10) u [108.8891877 u] {-80.73817 MeV} | (1/2+) | |
Ruthenium-110 | 11044Ru | 66 | 109.914039(10) u [109.8899027 u] {-80.07216 MeV} | 0+ | 110Tc |
Ruthenium-111 | 11144Ru | 67 | 110.917568(10) u [110.8934317 u] {-76.78491 MeV} | 5/2+ | 111Tc 252Cf 248Cm |
Ruthenium-112 | 11244Ru | 68 | 111.918807(10) u [111.8946707 u] {-75.63079 MeV} | 0+ | 112Tc |
Ruthenium-113 | 11344Ru | 69 | 112.92285(4) u [112.8987137 u] {-71.86476 MeV} | (1/2+) | 252Cf |
Ruthenium-113m | 113m44Ru | 69 | 112.92285(4) u [112.8987137 u] {-71.86476 MeV} | (7/2-) | |
Ruthenium-114 | 11444Ru | 70 | 113.924614(4) u [113.9004777 u] {-70.22161 MeV} | 0+ | 248Cm |
Ruthenium-115 | 11544Ru | 71 | 114.92894(10) u [114.9048037 u] {-66.19196 MeV} | (3/2+) | |
Ruthenium-116 | 11644Ru | 72 | 115.931219(4) u [115.9070827 u] {-64.06909 MeV} | 0+ | |
Ruthenium-117 | 11744Ru | 73 | 116.93613(46) u [116.9119937 u] {-59.49452 MeV} | ||
Ruthenium-118 | 11844Ru | 74 | 117.93853(21) u [117.9143937 u] {-57.25894 MeV} | 0+ | |
Ruthenium-119 | 11944Ru | 75 | 118.94357(32) u [118.9194337 u] {-52.56421 MeV} | ||
Ruthenium-120 | 12044Ru | 76 | 119.94631(43) u [119.9221737 u] {-50.01191 MeV} | 0+ | |
Ruthenium-121 | 12144Ru | 77 | 120.95164(43) u [120.9275037 u] {-45.04705 MeV} | ||
Ruthenium-122 | 12244Ru | 78 | 121.95475(54) u [121.9306137 u] {-42.1501 MeV} | 0+ | |
Ruthenium-123 | 12344Ru | 79 | 122.96019(54) u [122.9360537 u] {-37.08278 MeV} | ||
Ruthenium-124 | 12444Ru | 80 | 123.96354(64) u [123.9394037 u] {-33.96227 MeV} | 0+ |
Isotope | Radioactive Decay | Extern | |||
---|---|---|---|---|---|
Half-life | Decay Mode | Probability | Energy | ||
7 | 8 | 9 | 10 | 11 | 12 |
Ru-85 | 450 ns | EC/β+ → 85Tc EC, p → 84Mo p → 84Tc | ? ? ? | 14.9 MeV | |
Ru-86 | 438 ns | EC/β+ → 86Tc EC, p → 85Mo | ? ? | 11.8 MeV | |
Ru-87 | > 1.5 μs | EC/β+ → 87Tc | AL | ||
Ru-88 | 1.2 s | EC/β+ → 88Tc EC, p → 87Mo | 100 % ? | 7.34(33) MeV | AL |
Ru-89 | 1.5(2) s | EC/β+ → 89Tc ε, p → 88Mo | ca. 97 % ca. 3 % | 9.13(30) MeV | AL |
Ru-90 | 11(3) s | EC/β+ → 90Tc | 100 % | 5.841(4) MeV | AL |
Ru-91 | 8.0(4) s | EC/β+ → 91Tc | 100 % | 7.747(3) MeV | AL |
Ru-91m | 7.6(8) s | EC/β+ → 91Tc EC, p → 90Mo Iso → 91Ru | > 0 % > 0 % ? | ||
Ru-92 | 3.65(5) min | EC/β+ → 92Tc | 100 % | 4.624(4) MeV | AL |
Ru-93 | 59.7(6) s | EC/β+ → 93Tc | 100 % | 6.3894(23) MeV | AL |
Ru-93m1 | 10.8(3) s | EC/β+ → 93Tc ε, p → 92Mo Iso → 93Ru | 78.0(23) % 0.027(5) % 22.0(23) % | ||
Ru-93m2 | 2.49(15) μs | ||||
Ru-94 | 51.8(6) min | EC → 94Tc | 100 % | 1.575(5) MeV | AL |
Ru-94m | 71(4) μ s | Iso → 94Ru | 100 % | ||
Ru-95 | 1.643(13) h | EC/β+ → 95Tc | 100 % | 2.564(11) MeV | AL |
Ru-96 | stable | AL | |||
Ru-97 | 2.83(23) d | EC/β+ → 97Tc | 100 % | 1.104(5) MeV | AL |
Ru-98 | stable | AL | |||
Ru-99 | stable | AL | |||
Ru-100 | stable | AL | |||
Ru-101 | stable | AL | |||
Ru-101m | 17.5(4) μs | Iso → 101Ru | 100 % | ||
Ru-102 | stable | AL | |||
Ru-103 | 39.247(13) d | β- → 103Rh | 100 % | 0.7645(23) MeV | AL |
Ru-103m | 1.69(7) ms | Iso → 103Ru | 100 % | ||
Ru-104 | stable | AL | |||
Ru-105 | 4.44(2) h | β- → 105Rh | 100 % | 1.916(8) MeV | AL |
Ru-105 | 340(15) ns | ||||
Ru-106 | 371.8(18) d | β- → 106Rh | 100 % | 0.03940(21) MeV | AL |
Ru-107 | 3.75(5) min | β- → 107Rh | 100 % | 3.001(15) MeV | AL |
Ru-108 | 4.55(5) min | β- → 108Rh | 100 % | 1.370(16) MeV | AL |
Ru-109 | 34.4(2) s | β- → 109Rh | 100 % | 4.261(10) MeV | AL |
Ru-109m | 0.50(12) μs | ||||
Ru-110 | 12.04(17) s | β- → 110Rh | 100 % | 2.756(19) MeV | AL |
Ru-111 | 2.12(7) s | β- → 111Rh | 100 % | 5.519(12) MeV | AL |
Ru-112 | 1.75(7) s | β- → 112Rh | 100 % | 4.10(5) MeV | AL |
Ru-113 | 0.80(5) s | β- → 113Rh | 100 % | 6.90(4) MeV | AL |
Ru-113m | 510(30) ms | β- → 113Rh | ca. 100 % | ||
Ru-114 | 0.54(3) s | β- → 114Rh | 100 % | 5.49(7) MeV | AL |
Ru-115 | 318(19) ms | β- → 115Rh β-, n → 114Rh | 100 % ? | 8.04(9) MeV 1.45(11) MeV | AL |
Ru-116 | 204(6) ms | β- → 116Rh β-, n → 115Rh | ? | 6.67(7) MeV 2.09(8) MeV | AL |
Ru-117 | 151(3) ms | β- → 117Rh β-, n → 116Rh | 100 % ? | 9.41(43) MeV 3.17(44) MeV | AL |
Ru-118 | 99(3) ms | β- → 118Rh β-, n → 117Rh | ? | 7.63(20) MeV 3.57(20) MeV | AL |
Ru-119 | 69.5(20) ms | β- → 119Rh β-, n → β-, 2n → | ? ? | 10.26(30) MeV 4.25(30) MeV | AL |
Ru-120 | 42(2) ms | β- → 120Rh β-, n → 119Rh | 8.80(45) MeV 4.74(40) MeV | AL | |
Ru-121 | 29(2) ms | β- → 121Rh β-, n → 120Rh β-, 2n → 119Rh | ? ? | 11.20(74) MeV 5.70(45) MeV | AL |
Ru-122 | 25(1) ms | β- → 122Rh β-, n → 121Rh β-, 2n → | ? ? | 9.93(58) MeV 6.03(80) MeV | AL |
Ru-123 | 19(2) ms | β- → 123Rh β-, n → 122Rh β-, 2n → 121Rh | ? ? | 12.28(64) MeV 6.93(58) MeV | AL |
Ru-124 | 15(3) ms | β- → 124Rh β-, n → 123Rh β-, 2n → 122Rh | ? ? | 10.93(72) MeV 7.33(72) MeV | AL |
Notes (related to the columns):
1 - name of the nuclide, isotope.
2 - E: isotope symbol with mass number (superscript; number of nucleons) and atomic number (subscript; number of protons).
3 - N: number of neutrons.
4 - relative atomic mass of the Ruthenium isotope (isotopic mass including electrons) and the mass of the atomic nucleus in square brackets (nuclear mass, nuclide mass without electrons), each related to 12C = 12.00000 [2]. In addition, the mass excess is given in MeV.
5 - nuclear spin I, unit: h/2π.
6 - source nuclides: Possible, assumed or actual source nuclides (mother nuclides, parent nuclides). If applicable, the corresponding decay modes can be found in the data for the respective starting nuclide.
7 - isotope notation in short form.
8 - decay: half-live of the Ruthenium isotope (a = years; ; d = days; h = hours; min = minutes; s = seconds).
9 - decay mode: type of decay into the respective daughter nuclides with n = neutron emission; p = proton emission; α = alpha decay; β- = beta minus decay with electron emission; EC = electron capture; β+ = positron emission; ε = β+ and/or EC; Iso = isomeric transition; CD = cluster decay; SF = spontaneous decay.
10 - decay probability in percent (%).
11 - decay energy; Particle energy related to decay type.
12 - other information and notes: AL = Adopted Levels (link to external data [1]).
Miscellaneous:
()- Numbers in brackets: uncertainty to represent the spread of the reported value.
~ - Theoretical values or systematic trends.
- unlisted-: Nuclides that have already been mentioned in the literature but for some reason can no longer be found in the current nuclide tables because their discovery e.g. has not confirmed.
Nuclide quantity 1) spin | Nuclear magnetic moment μ/μN | Gyromagnetic ratio {Quadrupole moment} | Resonant frequency v0 bei 1 T | Relative sensitivity H0 = const. v0 = const. 3) |
---|---|---|---|---|
99Ru 12,76(14) % 5/2+ | - 0,641(5) | - 1,2286 {+ 7,9(4)} | 1,9553 | 0,00113 0,5358 |
101Ru 17,06(2) % 5/2+ | - 0.718(6) | - 1,3773 {+ 45,7(23)} | 2,1916 | 0,00159 0,6005 |
1) Quantity Percentage of natural occurrence.
2) Gyromagnetic ratio: 107 rad T-1 s-1
Quadrupole moment: Q fm-2
3) Related to 1H = 1,000.
According to the Radiation Protection Ordinance (StrlSchV 2018, Germany), the following values (columns 1 to 7) apply to the handling of Ruthenium radionuclides:
Nuclide | Limit Value | HASS limit | SC | Daughter Nuclides | Half-life | |
---|---|---|---|---|---|---|
Ru-94 | 106 Bq | 100 Bq/g | 51.8 min | |||
Ru-97 | 107 Bq | 10 Bq/g | 0,3 TBq | 10 Bq cm-2 | 2.9 d | |
Ru-103+ | 106 Bq | 1 Bq/g | 0,1 TBq | 10 Bq cm-2 | Rh-102m | 39.3 d |
Ru-105+ | 106 Bq | 10 Bq/g | 0,08 TBq | 1 Bq cm-2 | 4.4 h | |
Ru-106+ | 105 Bq | 0,1 Bq/g | 0,3 TBq | 10 Bq cm-2 | Rh-106 | 372.6 d |
(HASS = High-Activity Sealed Radioactive Sources; SC = surface contamination)
Properties of the Ruthenium nucleides
[1] - NuDat: National Nuclear Data Center, Brookhaven National Laboratory, based on ENSDF and the Nuclear Wallet Cards.
[2] - G. Audi et. al.: The NUBASE evaluation of nuclear and decay properties. Nuclear Physics, (2003), DOI 10.1016/j.nuclphysa.2003.11.001.
[3] - Live Chart of Nuclides. Nuclear structure and decay data.
Ruthenium: NMR properties - 99Ru-NMR, 101Ru-NMR
[4] - N. J. Stone: Table of nuclear magnetic dipole and electric quadrupole moments. Atomic Data and Nuclear Data Tables, (2005), DOI 10.1016/j.adt.2005.04.001.
[5] - Pekka Pyykkö: Year-2008 nuclear quadrupole moments. Molecular Physics, (2008), DOI 10.1080/00268970802018367.
[6] - Pekka Pyykkö: Year-2017 nuclear quadrupole moments. Molecular Physics, (2018), DOI 10.1080/00268976.2018.1426131.
[7] - N. J. Stone: Table of recommended nuclear magnetic dipole moments. IAEA, (2019).
More sources:
[8] - Isotopic abundances, atomic weights and isotopic masses: see respective keyword.
[9] - John W. Arblaster:
The Discoverers of the Ruthenium Isotopes.
In: Platinum Metals Review, (2011), DOI 10.1595/147106711x592448.
[10] - A. Nystrom, M. Thoennessen:
Discovery of Yttrium, Zirconium, Niobium, Technetium, and Ruthenium Isotopes.
In: Atomic Data and Nuclear Data Tables, (2012), DOI 10.1016/j.adt.2011.12.002.
Last update: 2022-12-12
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