Isotopes of rhodium

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Isotopes of rhodium  (45Rh)
Main isotopes [1] Decay
Isotope abun­dance half-life (t1/2) mode pro­duct
99Rh synth 16.1 d β+ 99Ru
100Rhsynth20.8 hβ+ 100Ru
101Rhsynth4.07 y ε 101Ru
101mRhsynth4.343 dε 101Ru
IT 101Rh
102Rhsynth207 dβ+ 102Ru
β 102Pd
102mRhsynth3.742 yβ+102Ru
IT102Rh
103Rh100% stable
105Rhsynth35.34 hβ 105Pd
Standard atomic weight Ar°(Rh)

Naturally occurring rhodium (45Rh) is composed of only one stable isotope, 103Rh. [4] The most stable radioisotopes are 101Rh with a half-life of 4.07 years, 102Rh with a half-life of 207 days, and 99Rh with a half-life of 16.1 days. Thirty other radioisotopes have been characterized ranging from 89Rh to 122Rh - these have half-lives that are less than an hour except 100Rh (20.8 hours) and 105Rh (35.34 hours). There are also numerous meta states with the most stable being 102mRh with a half-life of 3.74 years and 101mRh with a half-life of 4.34 days.

Contents

The primary decay mode before the only stable isotope, 103Rh, is electron capture to ruthenium isotopes, and the primary mode after is beta emission to palladium isotopes. Mass numbers 102 and 104 are capable of decay in either sense.

List of isotopes

Nuclide
[n 1]
Z N Isotopic mass (Da) [5]
[n 2] [n 3]
Discovery
year [6] [7]
Half-life [1]
[n 4]
Decay
mode
[1]
[n 5]
Daughter
isotope

[n 6]
Spin and
parity [1]
[n 7] [n 4]
Isotopic
abundance
Excitation energy [n 4]
89Rh454488.95099(39)# (1995) <120 ns β+?89Ru9/2+#
p?88Ru
β+, p?88Tc
90Rh454589.94457(22)# 1994 29(3) ms β+ 90Ru(0+)
β+, p? (<0.7%)89Tc
90mRh [n 8] 0(500)# keV 2001 0.56(2) sβ+ (90.4%)90Ru(7+)
β+, p (9.6%)89Tc
91Rh454690.93712(32)# 1994 1.47(22) sβ+ (98.7%)91Ru(9/2+)
β+, p (1.3%)90Tc
91mRh172.9(4) keV 2005 1.8# sβ+?91Ru1/2−#
β+, p?90Tc
IT?91Rh
92Rh454791.9323677(47) 1994 5.61(8) sβ+ (97.95%)92Ru(6+)
β+, p (2.05%)91Tc
92m1Rh50(100)# keV 2004 3.18(22) sβ+ (98.3%)92Ru(2+)
β+, p (1.7%)91Tc
92m2Rh105(100)# keV 2017 232(15) nsIT92Rh(4+)
93Rh454892.9259128(28) 1994 13.9(16) sβ+93Ru9/2+#
93mRh [8] 267(48) keV(2023) [n 9] (1/2−)
94Rh454993.9217305(36) 1979 70.6(6) sβ+ (98.2%)94Ru(4+)
β+, p (1.8%)93Tc
94m1Rh54.60(20)# keV 2006 480(30) nsIT94Rh(2+)
94m2Rh [n 8] 300(200)# keV 1980 25.8(2) sβ+94Ru(8+)
95Rh455094.9158979(42) 1967 5.02(10) minβ+95Ru(9/2)+
95mRh543.3(3) keV 1975 1.96(4) minIT (88%)95Rh(1/2)−
β+ (12%)95Ru
96Rh455195.914452(11) 1967 9.90(10) minβ+96Ru6+
96mRh51.98(9) keV 1967 1.51(2) minIT (60%)96Rh3+
β+ (40%)96Ru
97Rh455296.911328(38) 1955 30.7(6) minβ+97Ru9/2+
97mRh258.76(18) keV 1971 46.2(16) minβ+ (94.4%)97Ru1/2−
IT (5.6%)97Rh
98Rh455397.910708(13) 1955 8.72(12) minβ+98Ru(2)+
98mRh [n 8] 56.3(10) keV 1966 3.6(2) minIT (89%)98Rh(5+)
β+ (11%)98Ru
99Rh455498.908121(21) 1952 16.1(2) dβ+99Ru1/2−
99mRh64.4(5) keV 1965 4.7(1) hβ+99Ru9/2+
IT?99Rh
100Rh455599.908114(19) 1948 20.8(1) h EC (95.1%)100Ru1−
β+ (4.9%)100Ru
100m1Rh74.782(14) keV 1965 214.0(20) nsIT100Rh(2)+
100m2Rh107.6(2) keV 1974 4.6(2) minIT (98.3%)100Rh(5+)
β+ (1.7%)100Ru
100m3Rh219.61(22) keV 1984 130(10) nsIT100Rh(7+)
101Rh4556100.9061589(63) 1948 4.07(5) yEC101Ru1/2−
101mRh157.32(3) keV 1965 4.343(10) dEC (92.80%)101Ru9/2+
IT (7.20%)101Rh
102Rh4557101.9068343(69) 1941 207.0(15) dβ+ (78%)102Ru2−
β (22%)102Pd
102mRh140.73(9) keV 1963 3.742(10) yβ+ (99.77%)102Ru6+
IT (0.233%)102Rh
103Rh [n 10] 4558102.9054941(25) 1934 Stable1/2−1.0000
103mRh [n 10] 39.753(6) keV 1944 56.114(9) minIT103Rh7/2+
104Rh4559103.9066453(25) 1939 42.3(4) sβ (99.55%)104Pd1+
β+ (0.45%)104Ru
104mRh128.9679(5) keV 1939 4.34(3) minIT (99.87%)104Rh5+
β (0.13%)104Pd
105Rh [n 10] 4560104.9056878(27) 1946 35.341(19) hβ105Pd7/2+
105mRh [n 10] 129.742(4) keV 1951 42.8(3) sIT105Rh1/2−
106Rh [n 10] 4561105.9072859(58) 1946 30.07(35) sβ106Pd1+
106mRh132(11) keV 1955 131(2) minβ106Pd(6)+
107Rh4562106.906748(13) 1951 21.7(4) minβ107Pd7/2+
107mRh268.36(4) keV 1986 >10 μsIT107Rh1/2−
108Rh4563107.908715(15) 1955 16.8(5) sβ108Pd1+
108mRh115(18) keV 1969 6.0(3) minβ108Pd(5+)
109Rh4564108.9087496(43) 1972 80.8(7) sβ109Pd7/2+
109mRh225.873(19) keV 1987 1.66(4) μsIT109Rh3/2+
110Rh4565109.911080(19) 1963 3.35(12) sβ110Pd(1+)
110mRh [n 8] 220(150)# keV 1970 28.5(13) sβ110Pd(6+)
111Rh4566110.9116432(74) 1975 11(1) sβ111Pd(7/2+)
112Rh4567111.914405(47) 1971 3.4(4) sβ112Pd(1+)
112mRh340(70) keV 1988 6.73(15) sβ112Pd(6+)
113Rh4568112.9154402(77) 1971 2.80(12) sβ113Pd(7/2+)
114Rh4569113.918722(77) 1988 1.85(5) sβ114Pd1+
114mRh [n 8] 200(150)# keV 1988 1.85(5) sβ114Pd(7−)
115Rh4570114.9203116(79) 1988 1.03(3) sβ115Pd(7/2+)
β, n?114Pd
116Rh4571115.924062(79) 1970 685(39) msβ (>97.9%)116Pd1+
β, n? (<2.1%)115Pd
116mRh [n 8] 200(150)# keV 1988 570(50) msβ (>97.9%)116Pd(6−)
β, n? (<2.1%)115Pd
117Rh4572116.9260363(95) 1991 421(30) msβ117Pd7/2+#
β, n? (<7.6%)116Pd
117mRh321.2(10) keV 2013 138(17) nsIT117Rh3/2+#
118Rh4573117.930341(26) 1994 282(9) msβ (96.9%)118Pd1+#
β, n (3.1%)117Pd
118mRh [n 8] 200(150)# keV 2000 310(30) msβ (96.9%)118Pd6−#
β, n (3.1%)117Pd
IT?118Rh
119Rh4574118.932557(10) 1994 190(6) msβ (93.6%)119Pd7/2+#
β, n (6.4%)118Pd
120Rh4575119.93707(22)# 1994 129.6(42) msβ120Pd8−#
β, n (<9.3%)119Pd
β, 2n?118Pd
120mRh157.2(7) keV 2012 295(16) nsIT120Rh6#
121Rh4576120.93961(67) 1994 74(4) msβ121Pd7/2+#
β, n (>11%)120Pd
122Rh4577121.94431(32)# 1997 51(6) msβ122Pd7−#
β, n (<3.9%)121Pd
β, 2n?120Pd
122mRh271.0(7) keV 2012 830(120) nsIT122Rh4+#
123Rh4578122.94719(43)# 2010 42(4) msβ123Pd7/2+#
β, n (>24%)122Pd
β, 2n?121Pd
124Rh4579123.95200(43)# 2010 30(2) msβ124Pd2+#
β, n (<31%)123Pd
β, 2n?122Pd
125Rh4580124.95509(54)# 2010 26.5(20) msβ125Pd7/2+#
β, n?124Pd
β, 2n?123Pd
126Rh4581125.96006(54)# 2010 19(3) msβ126Pd1−#
β, n?125Pd
β, 2n?124Pd
127Rh4582126.96379(64)# 2015 28(14) msβ127Pd7/2+#
β, n?126Pd
β, 2n?125Pd
128Rh4583127.97065(32)# 2018 8# ms
[> 550 ns]
β?128Pd
β, n?127Pd
β, 2n?126Pd
This table header & footer:
  1. mRh  Excited nuclear isomer.
  2. ()  Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
  3. #  Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
  4. 1 2 3 #  Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  5. Modes of decay:
    EC: Electron capture
    IT: Isomeric transition
    n: Neutron emission
    p: Proton emission
  6. Bold symbol as daughter  Daughter product is stable.
  7. () spin value  Indicates spin with weak assignment arguments.
  8. 1 2 3 4 5 6 7 Order of ground state and isomer is uncertain.
  9. Not included in the discovery database yet.
  10. 1 2 3 4 5 Fission product

See also

Daughter products other than rhodium

References

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  2. "Standard Atomic Weights: Rhodium". CIAAW. 2017.
  3. Prohaska, Thomas; Irrgeher, Johanna; Benefield, Jacqueline; Böhlke, John K.; Chesson, Lesley A.; Coplen, Tyler B.; Ding, Tiping; Dunn, Philip J. H.; Gröning, Manfred; Holden, Norman E.; Meijer, Harro A. J. (2022-05-04). "Standard atomic weights of the elements 2021 (IUPAC Technical Report)". Pure and Applied Chemistry. doi:10.1515/pac-2019-0603. ISSN   1365-3075.
  4. John W. Arblaster (April 2011). "The Discoverers of the Rhodium Isotopes. The thirty-eight known rhodium isotopes found between 1934 and 2010". Platinum Metals Review. 55 (2): 124–134. doi: 10.1595/147106711X555656 .
  5. Wang, Meng; Huang, W.J.; Kondev, F.G.; Audi, G.; Naimi, S. (2021). "The AME 2020 atomic mass evaluation (II). Tables, graphs and references*". Chinese Physics C. 45 (3) 030003. doi:10.1088/1674-1137/abddaf.
  6. FRIB Nuclear Data Group. "Discovery of Nuclides Project, Isotope Database". doi:10.11578/frib/2279152.
  7. FRIB Nuclear Data Group. "Discovery of Nuclides Project, Isomer Database". doi:10.11578/frib/2572219.
  8. Xing, Y. M.; Yuan, C. X.; Wang, M.; Zhang, Y. H.; Zhou, X. H.; Litvinov, Yu. A.; Blaum, K.; Xu, H. S.; Bao, T.; Chen, R. J.; Fu, C. Y.; Gao, B. S.; Ge, W. W.; He, J. J.; Huang, W. J.; Liao, T.; Li, J. G.; Li, H. F.; Litvinov, S.; Naimi, S.; Shuai, P.; Sun, M. Z.; Wang, Q.; Xu, X.; Xu, F. R.; Yamaguchi, T.; Yan, X. L.; Yang, J. C.; Yuan, Y. J.; Zeng, Q.; Zhang, M.; Zhou, X. (11 January 2023). "Isochronous mass measurements of neutron-deficient nuclei from Sn 112 projectile fragmentation". Physical Review C. 107 (1) 014304. doi:10.1103/PhysRevC.107.014304.