Isotopes of tellurium
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There are 39 known isotopes and 17 nuclear isomers of tellurium (52Te), with atomic masses that range from 104 to 142. These are listed in the table below.
Naturally-occurring tellurium on Earth consists of eight isotopes. Two of these have been found to be
The very-long-lived radioisotopes 128Te and 130Te are the two most common isotopes of tellurium. Of elements with at least one stable isotope, only indium and rhenium likewise have a radioisotope in greater abundance than a stable one.
It has been claimed that electron capture of 123Te was observed, but more recent measurements of the same team have disproved this.[6] The half-life of 123Te is longer than 9.2 × 1016 years, and probably much longer.[6]
124Te can be used as a starting material in the production of
The short-lived isotope 135Te (half-life 19 seconds) is produced as a
With the exception of
List of isotopes
Nuclide [n 1] |
Z | N | Isotopic mass (Da) [n 2][n 3] |
Half-life [n 4][n 5] |
Daughter isotope [n 7] |
Natural abundance (mole fraction) | |||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Excitation energy | Normal proportion | Range of variation | |||||||||||||||||
104Te[7] | 52 | 52 | <18 ns | α | 100Sn | 0+ | |||||||||||||
105Te | 52 | 53 | 104.94364(54)# | 620(70) ns | α | 101Sn | 5/2+# | ||||||||||||
106Te | 52 | 54 | 105.93750(14) | 70(20) µs [70(+20−10) µs] |
α | 102Sn | 0+ | ||||||||||||
107Te | 52 | 55 | 106.93501(32)# | 3.1(1) ms | α (70%) | 103Sn | 5/2+# | ||||||||||||
β+ (30%) | 107Sb | ||||||||||||||||||
108Te | 52 | 56 | 107.92944(11) | 2.1(1) s | α (49%) | 104Sn | 0+ | ||||||||||||
β+ (48.5%) | 108Sb | ||||||||||||||||||
β+, p (2.4%) | 107Sn | ||||||||||||||||||
β+, α (.065%) | 104In | ||||||||||||||||||
109Te | 52 | 57 | 108.92742(7) | 4.6(3) s | β+ (86.99%) | 109Sb | (5/2+) | ||||||||||||
β+, p (9.4%) | 108Sn | ||||||||||||||||||
α (7.9%) | 105Sn | ||||||||||||||||||
β+, α (.005%) | 105In | ||||||||||||||||||
110Te | 52 | 58 | 109.92241(6) | 18.6(8) s | β+ (99.99%) | 110Sb | 0+ | ||||||||||||
β+, p (.003%) | 109Sn | ||||||||||||||||||
111Te | 52 | 59 | 110.92111(8) | 19.3(4) s | β+ | 111Sb | (5/2)+# | ||||||||||||
β+, p (rare) | 110Sn | ||||||||||||||||||
112Te | 52 | 60 | 111.91701(18) | 2.0(2) min | β+ | 112Sb | 0+ | ||||||||||||
113Te | 52 | 61 | 112.91589(3) | 1.7(2) min | β+ | 113Sb | (7/2+) | ||||||||||||
114Te | 52 | 62 | 113.91209(3) | 15.2(7) min | β+ | 114Sb | 0+ | ||||||||||||
115Te | 52 | 63 | 114.91190(3) | 5.8(2) min | β+ | 115Sb | 7/2+ | ||||||||||||
115m1Te | 10(7) keV | 6.7(4) min | β+ | 115Sb | (1/2)+ | ||||||||||||||
IT
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115Te | ||||||||||||||||||
115m2Te | 280.05(20) keV | 7.5(2) µs | 11/2− | ||||||||||||||||
116Te | 52 | 64 | 115.90846(3) | 2.49(4) h | β+ | 116Sb | 0+ | ||||||||||||
117Te | 52 | 65 | 116.908645(14) | 62(2) min | β+ | 117Sb | 1/2+ | ||||||||||||
117mTe | 296.1(5) keV | 103(3) ms | IT | 117Te | (11/2−) | ||||||||||||||
118Te | 52 | 66 | 117.905828(16) | 6.00(2) d | EC | 118Sb | 0+ | ||||||||||||
119Te | 52 | 67 | 118.906404(9) | 16.05(5) h | β+ | 119Sb | 1/2+ | ||||||||||||
119mTe | 260.96(5) keV | 4.70(4) d | β+ (99.99%) | 119Sb | 11/2− | ||||||||||||||
IT (.008%) | 119Te | ||||||||||||||||||
120Te | 52 | 68 | 119.90402(1) | Observationally Stable[n 9]
|
0+ | 9(1)×10−4 | |||||||||||||
121Te | 52 | 69 | 120.904936(28) | 19.16(5) d | β+ | 121Sb | 1/2+ | ||||||||||||
121mTe | 293.991(22) keV | 154(7) d | IT (88.6%) | 121Te | 11/2− | ||||||||||||||
β+ (11.4%) | 121Sb | ||||||||||||||||||
122Te | 52 | 70 | 121.9030439(16) | Stable | 0+ | 0.0255(12) | |||||||||||||
123Te | 52 | 71 | 122.9042700(16) | Observationally Stable[n 10] | 1/2+ | 0.0089(3) | |||||||||||||
123mTe | 247.47(4) keV | 119.2(1) d | IT | 123Te | 11/2− | ||||||||||||||
124Te | 52 | 72 | 123.9028179(16) | Stable | 0+ | 0.0474(14) | |||||||||||||
125Te[n 11] | 52 | 73 | 124.9044307(16) | Stable | 1/2+ | 0.0707(15) | |||||||||||||
125mTe | 144.772(9) keV | 57.40(15) d | IT | 125Te | 11/2− | ||||||||||||||
126Te | 52 | 74 | 125.9033117(16) | Stable | 0+ | 0.1884(25) | |||||||||||||
127Te[n 11] | 52 | 75 | 126.9052263(16) | 9.35(7) h | β− | 127I | 3/2+ | ||||||||||||
127mTe | 88.26(8) keV | 109(2) d | IT (97.6%) | 127Te | 11/2− | ||||||||||||||
β− (2.4%) | 127I | ||||||||||||||||||
128Te[n 11][n 12] | 52 | 76 | 127.9044631(19) | 2.2(3)×1024 y[n 13] | β−β− | 128Xe | 0+ | 0.3174(8) | |||||||||||
128mTe | 2790.7(4) keV | 370(30) ns | 10+ | ||||||||||||||||
129Te[n 11] | 52 | 77 | 128.9065982(19) | 69.6(3) min | β− | 129I | 3/2+ | ||||||||||||
129mTe | 105.50(5) keV | 33.6(1) d | β− (36%) | 129I | 11/2− | ||||||||||||||
IT (64%) | 129Te | ||||||||||||||||||
130Te[n 11][n 12] | 52 | 78 | 129.9062244(21) | 8.2(0.2 (stat.), 0.6 (syst.))×1020 y | β−β− | 130Xe | 0+ | 0.3408(62) | |||||||||||
130m1Te | 2146.41(4) keV | 115(8) ns | (7)− | ||||||||||||||||
130m2Te | 2661(7) keV | 1.90(8) µs | (10+) | ||||||||||||||||
130m3Te | 4375.4(18) keV | 261(33) ns | |||||||||||||||||
131Te[n 11] | 52 | 79 | 130.9085239(21) | 25.0(1) min | β− | 131I | 3/2+ | ||||||||||||
131mTe | 182.250(20) keV | 30(2) h | β− (77.8%) | 131I | 11/2− | ||||||||||||||
IT (22.2%) | 131Te | ||||||||||||||||||
132Te[n 11] | 52 | 80 | 131.908553(7) | 3.204(13) d | β− | 132I | 0+ | ||||||||||||
133Te | 52 | 81 | 132.910955(26) | 12.5(3) min | β− | 133I | (3/2+) | ||||||||||||
133mTe | 334.26(4) keV | 55.4(4) min | β− (82.5%) | 133I | (11/2−) | ||||||||||||||
IT (17.5%) | 133Te | ||||||||||||||||||
134Te | 52 | 82 | 133.911369(11) | 41.8(8) min | β− | 134I | 0+ | ||||||||||||
134mTe | 1691.34(16) keV | 164.1(9) ns | 6+ | ||||||||||||||||
135Te[n 14] | 52 | 83 | 134.91645(10) | 19.0(2) s | β− | 135I | (7/2−) | ||||||||||||
135mTe | 1554.88(17) keV | 510(20) ns | (19/2−) | ||||||||||||||||
136Te | 52 | 84 | 135.92010(5) | 17.63(8) s | β− (98.7%) | 136I | 0+ | ||||||||||||
β−, n (1.3%) | 135I | ||||||||||||||||||
137Te | 52 | 85 | 136.92532(13) | 2.49(5) s | β− (97.01%) | 137I | 3/2−# | ||||||||||||
β−, n (2.99%) | 136I | ||||||||||||||||||
138Te | 52 | 86 | 137.92922(22)# | 1.4(4) s | β− (93.7%) | 138I | 0+ | ||||||||||||
β−, n (6.3%) | 137I | ||||||||||||||||||
139Te | 52 | 87 | 138.93473(43)# | 500 ms [>300 ns]# |
β− | 139I | 5/2−# | ||||||||||||
β−, n | 138I | ||||||||||||||||||
140Te | 52 | 88 | 139.93885(32)# | 300 ms [>300 ns]# |
β− | 140I | 0+ | ||||||||||||
β−, n | 139I | ||||||||||||||||||
141Te | 52 | 89 | 140.94465(43)# | 100 ms [>300 ns]# |
β− | 141I | 5/2−# | ||||||||||||
β−, n | 140I | ||||||||||||||||||
142Te | 52 | 90 | 141.94908(64)# | 50 ms [>300 ns]# |
β− | 142I | 0+ | ||||||||||||
This table header & footer: |
- ^ mTe – 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).
- age of universe.
- ^ a b # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
- ^
Modes of decay:
EC: Electron capture 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 120Sn with a half-life over 2.2×1016 years
- ^ Believed to undergo β+ decay to 123Sb with a half-life over 9.2×1016 years
- ^ Fission product
- ^ a b Primordial radionuclide
- ^ Longest measured half-life of any nuclide
- fission product, responsible for the iodine pit as precursor of 135Xevia 135I
References
- 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.
- Alduino, C.; Alfonso, K.; Artusa, D. R.; Avignone, F. T.; Azzolini, O.; Banks, T. I.; Bari, G.; Beeman, J. W.; Bellini, F. (2017-01-01). "Measurement of the two-neutrino double-beta decay half-life of 130Te with the CUORE-0 experiment". The European Physical Journal C. 77 (1): 13. S2CID 254105128.