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Isotopes of antimony

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Isotopes of antimony (51Sb)
Main isotopes[1] Decay
abun­dance half-life (t1/2) mode pro­duct
121Sb 57.2% stable
123Sb 42.8% stable
125Sb synth 2.7576 y β 125Te
Standard atomic weight Ar°(Sb)

Antimony (51Sb) occurs in two stable isotopes, 121Sb and 123Sb. There are 37 artificial radioactive isotopes, the longest-lived of which are 125Sb, with a half-life of 2.75856 years; 124Sb, with half-life 60.2 days; and 126Sb, with half-life 12.35 days. All other isotopes have half-lives less than 4 days, most less than an hour. There are also many isomers, the longest-lived of which is 120m1Sb with half-life 5.76 days.

Except for beryllium, antimony is the lightest element observed to have isotopes capable of alpha decay; 104Sb is seen to undergo this mode of decay. Some light elements, namely those near 8Be, have isotopes with delayed alpha emission (following proton or beta emission) as a rare branch.

List of isotopes

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

[n 5][n 6]
Spin and
parity[1]
[n 7][n 8]
Natural abundance (mole fraction)
Excitation energy[n 8] Normal proportion[1] Range of variation
104Sb 51 53 103.93634(11)# 470(130) ms β ? 104Sn
p (<7%) 103Sn
β , p (<7%) 103In
α? 100In
105Sb 51 54 104.931277(23) 1.12(16) s β (>99.9%) 105Sn (5/2 )
p (<0.1%) 104Sn
β , p? 104In
106Sb 51 55 105.9286380(80) 0.6(2) s β 106Sn (2 )
106mSb 103.5(3) keV 226(14) ns IT 106Sb (4 )
107Sb 51 56 106.9241506(45) 4.0(2) s β 107Sn 5/2 #
108Sb 51 57 107.9222267(59) 7.4(3) s β 108Sn (4 )
109Sb 51 58 108.9181412(57) 17.2(5) s β 109Sn 5/2 #
110Sb 51 59 109.9168543(64) 23.6(3) s β 110Sn (3 )
111Sb 51 60 110.9132182(95) 75(1) s β 111Sn (5/2 )
112Sb 51 61 111.912400(19) 53.5(6) s β 112Sn (3 )
112mSb 825.9(4) keV 536(22) ns IT 112Sb (8−)
113Sb 51 62 112.909375(18) 6.67(7) min β 113Sn 5/2
114Sb 51 63 113.909289(21) 3.49(3) min β 114Sn 3
114mSb 495.5(7) keV 219(12) μs IT 114Sb (8−)
115Sb 51 64 114.906598(17) 32.1(3) min β 115Sn 5/2
115mSb 2796.26(9) keV 159(3) ns IT 115Sb (19/2)−
116Sb 51 65 115.9067927(55) 15.8(8) min β 116Sn 3
116m1Sb 93.99(5) keV 194(4) ns IT 116Sb 1
116m2Sb 390(40) keV 60.3(6) min β 116Sn 8−
117Sb 51 66 116.9048415(91) 2.97(2) h β 117Sn 5/2
117m1Sb 3130.76(19) keV 355(17) μs IT 117Sb (25/2)
117m2Sb 3230.7(2) keV 290(5) ns IT 117Sb (23/2−)
118Sb 51 67 117.9055322(32) 3.6(1) min β 118Sn 1
118m1Sb 50.814(21) keV 20.6(6) μs IT 118Sb 3
118m2Sb 250(6) keV 5.01(3) h β 118Sn 8−
119Sb 51 68 118.9039441(75) 38.19(22) h EC 119Sn 5/2
119m1Sb 2553.6(3) keV 130(3) ns IT 119Sb 19/2−
119m2Sb 2841.7(4) keV 835(81) ms IT 119Sb 25/2
120Sb 51 69 119.9050803(77) 15.89(4) min β 120Sn 1
120m1Sb[n 9] 0(100)# keV 5.76(2) d β 120Sn 8−
120m2Sb 78.16(5) keV 246(2) ns IT 120Sb (3 )
120m3Sb 2328(100)# keV 400(8) ns IT 120Sb 13
121Sb[n 10] 51 70 120.9038114(27) Stable 5/2 0.5721(5)
121mSb 2751(17) keV 179(6) μs IT 121Sb (25/2 )
122Sb 51 71 121.9051693(27) 2.7238(2) d β (97.59%) 122Te 2−
β (2.41%) 122Sn
122m1Sb 61.4131(5) keV 1.86(8) μs IT 122Sb 3
122m2Sb 137.4726(8) keV 0.53(3) ms IT 122Sb 5
122m3Sb 163.5591(17) keV 4.191(3) min IT 122Sb 8−
123Sb[n 10] 51 72 122.9042153(15) Stable 7/2 0.4279(5)
123m1Sb 2237.8(3) keV 214(3) ns IT 123Sb 19/2−
123m2Sb 2613.4(4) keV 65(1) μs IT 123Sb 23/2
124Sb 51 73 123.9059371(15) 60.20(3) d β 124Te 3−
124m1Sb 10.8627(8) keV 93(5) s IT (75%) 124Sb 5
β (25%) 124Te
124m2Sb 36.8440(14) keV 20.2(2) min IT 124m1Sb (8)−
124m3Sb 40.8038(7) keV 3.2(3) μs IT 124Sb (3 )
125Sb 51 74 124.9052543(27) 2.7576(11) y β 125Te 7/2
125m1Sb 1971.25(20) keV 4.1(2) μs IT 125Sb 15/2−
125m2Sb 2112.1(3) keV 28.5(5) μs IT 125Sb 19/2−
125m3Sb 2471.0(4) keV 277.0(64) ns IT 125Sb (23/2)
126Sb 51 75 125.907253(34) 12.35(6) d β 126Te 8−
126m1Sb 17.7(3) keV 19.15(8) min β (86%) 126Te 5
IT (14%) 126Sb
126m2Sb 40.4(3) keV ~11 s IT 126m1Sb 3−
126m3Sb 104.6(3) keV 553(5) ns IT 126Sb 3
126m4Sb 1810.7(17) keV 90(16) ns IT 126Sb (13 )
127Sb 51 76 126.9069256(55) 3.85(5) d β 127Te 7/2
127m1Sb 1920.19(21) keV 11.7(1) μs IT 127Sb 15/2−
127m2Sb 2324.7(4) keV 269(5) ns IT 127Sb 23/2
128Sb 51 77 127.909146(20) 9.05(4) h β 128Te 8−
128m1Sb[n 9] 10(6) keV 10.41(18) min β (96.4%) 128Te 5
IT (3.6%) 128Sb
128m2Sb 1617.3(7) keV 500(20) ns IT 128Sb (11 )
128m3Sb 1769.9(12) keV 217(7) ns IT 128Sb (13 )
129Sb 51 78 128.909147(23) 4.366(26) h β 129Te 7/2
129m1Sb 1851.31(6) keV 17.7(1) min β (85%) 129Te 19/2−
IT (15%) 129Sb
129m2Sb 1861.06(5) keV 2.23(17) μs IT 129Sb 15/2−
129m3Sb 2139.4(3) keV 0.89(3) μs IT 129Sb 23/2
130Sb 51 79 129.911663(15) 39.5(8) min β 130Te 8−
130m1Sb 4.80(20) keV 6.3(2) min β 130Te 4
130m2Sb 84.67(4) keV 800(100) ns IT 130Sb 6−
130m3Sb 1508(1) keV 600(15) ns IT 130Sb (11 )
130m4Sb 1544.7(5) keV 1.25(1) μs IT 130Sb (13 )
131Sb 51 80 130.9119893(22) 23.03(4) min β 131Te 7/2
131m1Sb 1676.06(6) keV 64.2(26) μs IT 131Sb 15/2−
131m2Sb 1687.2(9) keV 4.3(8) μs IT 131Sb 19/2−
131m3Sb 2165.6(15) keV 0.97(3) μs IT 131Sb 23/2
132Sb 51 81 131.9145141(29)[5] 2.79(7) min β 132Te (4)
132m1Sb 139.3(20) keV[5] 4.10(5) min β 132Te (8−)
132m2Sb 254.5(3) keV 102(4) ns IT 132Sb (6−)
133Sb 51 82 132.9152721(34) 2.34(5) min β 133Te (7/2 )
133mSb 4541(9) keV 16.54(19) μs IT 133Sb (21/2 )
134Sb 51 83 133.9205373(33) 674(4) ms β 134Te (0-)
β, n? 133Te
134mSb 279(1) keV 10.01(4) s β (99.91%) 134Te (7−)
β, n (0.088%) 133Te
135Sb 51 84 134.9251844(28) 1.668(9) s β (80.9%) 135Te (7/2 )
β, n (19.1%) 134Te
136Sb 51 85 135.9307490(63) 0.923(14) s β (75.2%) 136Te (1−)
β, n (24.7%) 135Te
β, 2n (0.14%) 134Te
136mSb 269.3(5) keV 570(5) ns IT 136Sb (6−)
137Sb 51 86 136.935523(56) 497(21) ms β (51%) 137Te 7/2 #
β, n (49%) 136Te
β, 2n? 135Te
138Sb 51 87 137.94133(32)# 333(7) ms β, n (72%) 137Te (3−)
β (28%) 138Te
β, 2n? 136Te
139Sb 51 88 138.94627(43)# 182(9) ms β, n (90%) 138Te 7/2 #
β (10%) 139Te
β, 2n? 137Te
140Sb 51 89 139.95235(64)# 170(6) ms β (69%) 140Te (3−)
β, n (23%) 139Te
β, 2n (7.6%) 138Te
140mSb 330(30)# keV 41(8) μs IT 140Sb (6−,7−)
141Sb 51 90 140.95755(54)# 103(29) ms β 141Te 7/2 #
β, n? 140Te
β, 2n? 139Te
142Sb 51 91 141.96392(32)# 80(50) ms β 142Te
β, n? 141Te
β, 2n? 130Te
This table header & footer:
  1. ^ mSb – 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. ^ Modes of decay:
    EC: Electron capture
    IT: Isomeric transition
    n: Neutron emission
    p: Proton emission
  5. ^ Bold italics symbol as daughter – Daughter product is nearly stable.
  6. ^ Bold symbol as daughter – Daughter product is stable.
  7. ^ ( ) spin value – Indicates spin with weak assignment arguments.
  8. ^ a b # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
  9. ^ a b Order of ground state and isomer is uncertain.
  10. ^ a b Fission product

References

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  1. ^ a b c d e Kondev, F. G.; Wang, M.; Huang, W. J.; Naimi, S.; Audi, G. (2021). "The NUBASE2020 evaluation of nuclear properties" (PDF). Chinese Physics C. 45 (3): 030001. doi:10.1088/1674-1137/abddae.
  2. ^ "Standard Atomic Weights: Antimony". CIAAW. 1993.
  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. ^ 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.
  5. ^ a b Jaries, A.; Stryjczyk, M.; Kankainen, A.; Ayoubi, L. Al; Beliuskina, O.; Canete, L.; de Groote, R. P.; Delafosse, C.; Delahaye, P.; Eronen, T.; Flayol, M.; Ge, Z.; Geldhof, S.; Gins, W.; Hukkanen, M.; Imgram, P.; Kahl, D.; Kostensalo, J.; Kujanpää, S.; Kumar, D.; Moore, I. D.; Mougeot, M.; Nesterenko, D. A.; Nikas, S.; Patel, D.; Penttilä, H.; Pitman-Weymouth, D.; Pohjalainen, I.; Raggio, A.; Ramalho, M.; Reponen, M.; Rinta-Antila, S.; de Roubin, A.; Ruotsalainen, J.; Srivastava, P. C.; Suhonen, J.; Vilen, M.; Virtanen, V.; Zadvornaya, A. "Physical Review C - Accepted Paper: Isomeric states of fission fragments explored via Penning trap mass spectrometry at IGISOL". journals.aps.org. arXiv:2403.04710.