# Isotopes of technetium

Technetium ($_{43}$Tc) is one of the two elements with Z < 83 that have no stable isotopes; the other such element is promethium. It is primarily artificial, with only trace quantities existing in nature produced by spontaneous fission (there are an estimated 2.5×10$^{−13}$ grams of $^{99}$Tc per gram of pitchblende) or neutron capture by molybdenum. The first isotopes to be synthesized were $^{97}$Tc and $^{99}$Tc in 1936, the first artificial element to be produced. The most stable radioisotopes are $^{97}$Tc (half-life of 4.21 million years), $^{98}$Tc (half-life: 4.2 million years), and $^{99}$Tc (half-life: 211,100 years).
Thirty-three other radioisotopes have been characterized with atomic masses ranging from $^{85}$Tc to $^{120}$Tc. Most of these have half-lives that are less than an hour; the exceptions are $^{93}$Tc (half-life: 2.75 hours), $^{94}$Tc (half-life: 4.883 hours), $^{95}$Tc (half-life: 20 hours), and $^{96}$Tc (half-life: 4.28 days).
Technetium also has numerous meta states. $^{97m}$Tc is the most stable, with a half-life of 91.0 days (0.097 MeV). This is followed by $^{95m}$Tc (half-life: 61 days, 0.038 MeV) and $^{99m}$Tc (half-life: 6.04 hours, 0.143 MeV). $^{99m}$Tc only emits gamma rays, subsequently decaying to $^{99}$Tc.
For isotopes lighter than $^{98}$Tc, the primary decay mode is electron capture to isotopes of molybdenum. For the heavier isotopes, the primary mode is beta emission to isotopes of ruthenium, with the exception that $^{100}$Tc can decay both by beta emission and electron capture.
Technetium-99m is the hallmark technetium isotope employed in the nuclear medicine industry. Its low-energy isomeric transition, which yields a gamma-ray at ~140.5 keV, is ideal for imaging using Single Photon Emission Computed Tomography (SPECT). Several technetium isotopes, such as $^{94m}$Tc, $^{95}$Tc, and $^{96}$Tc, which are produced via (p,n) reactions using a cyclotron on molybdenum targets, have also been identified as potential Positron Emission Tomography (PET) or gamma-emitting agents for medical imaging. Technetium-101 has been produced using a D-D fusion-based neutron generator from the $^{100}$Mo(n,γ)$^{101}$Mo reaction on natural molybdenum and subsequent beta-minus decay of $^{101}$Mo to $^{101}$Tc. Despite its shorter half-life (i.e., 14.22 min), $^{101}$Tc exhibits unique decay characteristics suitable for radioisotope diagnostic or therapeutic procedures, where it has been proposed that its implementation, as a supplement for dual-isotopic imaging or replacement for $^{99m}$Tc, could be performed by on-site production and dispensing at the point of patient care.
Technetium-99 is the most common and most readily available isotope, as it is a major fission product from fission of actinides like uranium and plutonium with a fission product yield of 6% or more, and in fact the most significant long-lived fission product. Lighter isotopes of technetium are almost never produced in fission because the initial fission products normally have a higher neutron/proton ratio than is stable for their mass range, and therefore undergo beta decay until reaching the ultimate product. Beta decay of fission products of mass 95–98 stops at the stable isotopes of molybdenum of those masses and does not reach technetium. For mass 100 and greater, the technetium isotopes of those masses are very short-lived and quickly beta decay to isotopes of ruthenium. Therefore, the technetium in spent nuclear fuel is practically all $^{99}$Tc. In the presence of fast neutrons a small amount of $^{98}$ Tc will be produced by (n,2n) "knockout" reactions. If nuclear transmutation of fission-derived Technetium or Technetium waste from medical applications is desired, fast neutrons are therefore not desirable as the long lived $^{98}$ Tc increases rather than reducing the longevity of the radioactivity in the material.
One gram of $^{99}$Tc produces 6.2×10$^8$ disintegrations a second (that is, 0.62 GBq/g).
Technetium has no primordial isotopes and does not occur in nature in significant quantities, and thus a standard atomic weight cannot be given.

## List of isotopes

| Nuclide | Z | N | Isotopic mass (Da) | Half-life | Decay mode | Daughter isotope | Spin and parity | Isotopic abundance |
| Isotopic abundance |||
| $^{86}$Tc | 43 | 43 | 85.94464(32)# | 55(7) ms | β$^+$ | $^{86}$Mo | (0+) | |
| $^{86m}$Tc | 1524(10) keV | 1524(10) keV | 1524(10) keV | 1.10(12) μs | IT | $^{86}$Tc | (6+) | |
| $^{87}$Tc | 43 | 44 | 86.9380672(45) | 2.14(17) s | β$^+$ | $^{87}$Mo | 9/2+# | |
| $^{87}$Tc | 43 | 44 | 86.9380672(45) | 2.14(17) s | β$^+$, p (<0.7%) | $^{86}$Nb | 9/2+# | |
| $^{87m}$Tc | 71(1) keV | 71(1) keV | 71(1) keV | 647(24) ns | IT | $^{87}$Tc | 7/2+# | |
| $^{88}$Tc | 43 | 45 | 87.9337942(44) | 6.4(8) s | β$^+$ | $^{88}$Mo | (2+) | |
| $^{88m1}$Tc | 70(3) keV | 70(3) keV | 70(3) keV | 5.8(2) s | β$^+$ | $^{88}$Mo | (6+) | |
| $^{88m2}$Tc | 95(1) keV | 95(1) keV | 95(1) keV | 146(12) ns | IT | $^{88}$Tc | (4+) | |
| $^{89}$Tc | 43 | 46 | 88.9276486(41) | 12.8(9) s | β$^+$ | $^{89}$Mo | (9/2+) | |
| $^{89m}$Tc | 62.6(5) keV | 62.6(5) keV | 62.6(5) keV | 12.9(8) s | β$^+$ | $^{89}$Mo | (1/2−) | |
| $^{90}$Tc | 43 | 47 | 89.9240739(11) | 49.2(4) s | β$^+$ | $^{90}$Mo | (8+) | |
| $^{90m}$Tc | 144.0(17) keV | 144.0(17) keV | 144.0(17) keV | 8.7(2) s | β$^+$ | $^{90}$Mo | 1+ | |
| $^{91}$Tc | 43 | 48 | 90.9184250(25) | 3.14(2) min | β$^+$ | $^{91}$Mo | (9/2)+ | |
| $^{91m}$Tc | 139.3(3) keV | 139.3(3) keV | 139.3(3) keV | 3.3(1) min | β$^+$ (99%) | $^{91}$Mo | (1/2)− | |
| $^{92}$Tc | 43 | 49 | 91.9152698(33) | 4.25(15) min | β$^+$ | $^{92}$Mo | (8)+ | |
| $^{92m1}$Tc | 270.09(8) keV | 270.09(8) keV | 270.09(8) keV | 1.03(6) μs | IT | $^{92}$Tc | (4+) | |
| $^{92m2}$Tc | 529.42(13) keV | 529.42(13) keV | 529.42(13) keV | <0.1 μs | IT | $^{92}$Tc | (3+) | |
| $^{92m3}$Tc | 711.33(15) keV | 711.33(15) keV | 711.33(15) keV | <0.1 μs | IT | $^{92}$Tc | 1+ | |
| $^{93}$Tc | 43 | 50 | 92.9102451(11) | 2.75(5) h | β$^+$ | $^{93}$Mo | 9/2+ | |
| $^{93m1}$Tc | 391.84(8) keV | 391.84(8) keV | 391.84(8) keV | 43.5(10) min | IT (77.4%) | $^{93}$Tc | 1/2− | |
| $^{93m1}$Tc | 391.84(8) keV | 391.84(8) keV | 391.84(8) keV | 43.5(10) min | β$^+$ (22.6%) | $^{93}$Mo | 1/2− | |
| $^{93m2}$Tc | 2185.16(15) keV | 2185.16(15) keV | 2185.16(15) keV | 10.2(3) μs | IT | $^{93}$Tc | (17/2)− | |
| $^{94}$Tc | 43 | 51 | 93.9096523(44) | 293(1) min | β$^+$ | $^{94}$Mo | 7+ | |
| $^{94m}$Tc | 76(3) keV | 76(3) keV | 76(3) keV | 52(1) min | β$^+$ (>99.82%) | $^{94}$Mo | (2)+ | |
| $^{94m}$Tc | 76(3) keV | 76(3) keV | 76(3) keV | 52(1) min | IT (<0.18%) | $^{94}$Tc | (2)+ | |
| $^{95}$Tc | 43 | 52 | 94.9076523(55) | 19.258(26) h | β$^+$ | $^{95}$Mo | 9/2+ | |
| $^{95m}$Tc | 38.91(4) keV | 38.91(4) keV | 38.91(4) keV | 61.96(24) d | β$^+$ (96.1%) | $^{95}$Mo | 1/2− | |
| $^{95m}$Tc | 38.91(4) keV | 38.91(4) keV | 38.91(4) keV | 61.96(24) d | IT (3.9%) | $^{95}$Tc | 1/2− | |
| $^{96}$Tc | 43 | 53 | 95.9078667(55) | 4.28(7) d | β$^+$ | $^{96}$Mo | 7+ | |
| $^{96m}$Tc | 34.23(4) keV | 34.23(4) keV | 34.23(4) keV | 51.5(10) min | IT (98.0%) | $^{96}$Tc | 4+ | |
| $^{96m}$Tc | 34.23(4) keV | 34.23(4) keV | 34.23(4) keV | 51.5(10) min | β$^+$ (2.0%) | $^{96}$Mo | 4+ | |
| $^{97}$Tc | 43 | 54 | 96.9063607(44) | 4.21(16)×10$^6$ y | EC | $^{97}$Mo | 9/2+ | |
| $^{97m}$Tc | 96.57(6) keV | 96.57(6) keV | 96.57(6) keV | 91.1(6) d | IT (96.06%) | $^{97}$Tc | 1/2− | |
| $^{97m}$Tc | 96.57(6) keV | 96.57(6) keV | 96.57(6) keV | 91.1(6) d | EC (3.94%) | $^{97}$Mo | 1/2− | |
| $^{98}$Tc | 43 | 55 | 97.9072112(36) | 4.2(3)×10$^6$ y | β$^−$ | $^{98}$Ru | 6+ | |
| $^{98m}$Tc | 90.77(16) keV | 90.77(16) keV | 90.77(16) keV | 14.7(5) μs | IT | $^{98}$Tc | (2,3)− | |
| $^{99}$Tc | 43 | 56 | 98.90624968(97) | 2.111(12)×10$^5$ y | β$^−$ | $^{99}$Ru | 9/2+ | trace |
| $^{99m}$Tc | 142.6836(11) keV | 142.6836(11) keV | 142.6836(11) keV | 6.0066(2) h | IT | $^{99}$Tc | 1/2− | |
| $^{99m}$Tc | 142.6836(11) keV | 142.6836(11) keV | 142.6836(11) keV | 6.0066(2) h | β$^−$ (0.0037%) | $^{99}$Ru | 1/2− | |
| $^{100}$Tc | 43 | 57 | 99.9076527(15) | 15.46(19) s | β$^−$ | $^{100}$Ru | 1+ | |
| $^{100}$Tc | 43 | 57 | 99.9076527(15) | 15.46(19) s | EC (0.0018%) | $^{100}$Mo | 1+ | |
| $^{100m1}$Tc | 200.67(4) keV | 200.67(4) keV | 200.67(4) keV | 8.32(14) μs | IT | $^{100}$Tc | (4)+ | |
| $^{100m2}$Tc | 243.95(4) keV | 243.95(4) keV | 243.95(4) keV | 3.2(2) μs | IT | $^{100}$Tc | (6)+ | |
| $^{101}$Tc | 43 | 58 | 100.907305(26) | 14.22(1) min | β$^−$ | $^{101}$Ru | 9/2+ | |
| $^{101m}$Tc | 207.526(20) keV | 207.526(20) keV | 207.526(20) keV | 636(8) μs | IT | $^{101}$Tc | 1/2− | |
| $^{102}$Tc | 43 | 59 | 101.9092072(98) | 5.28(15) s | β$^−$ | $^{102}$Ru | 1+ | |
| $^{102m}$Tc | 50(50)# keV | 50(50)# keV | 50(50)# keV | 4.35(7) min | β$^−$ | $^{102}$Ru | (4+) | |
| $^{103}$Tc | 43 | 60 | 102.909174(11) | 54.2(8) s | β$^−$ | $^{103}$Ru | 5/2+ | |
| $^{104}$Tc | 43 | 61 | 103.911434(27) | 18.3(3) min | β$^−$ | $^{104}$Ru | (3−) | |
| $^{104m1}$Tc | 69.7(2) keV | 69.7(2) keV | 69.7(2) keV | 3.5(3) μs | IT | $^{104}$Tc | (5−) | |
| $^{104m2}$Tc | 106.1(3) keV | 106.1(3) keV | 106.1(3) keV | 400(20) ns | IT | $^{104}$Tc | 4# | |
| $^{105}$Tc | 43 | 62 | 104.911662(38) | 7.64(6) min | β$^−$ | $^{105}$Ru | (3/2−) | |
| $^{106}$Tc | 43 | 63 | 105.914357(13) | 35.6(6) s | β$^−$ | $^{106}$Ru | (1,2)(+#) | |
| $^{107}$Tc | 43 | 64 | 106.9154584(93) | 21.2(2) s | β$^−$ | $^{107}$Ru | (3/2−) | |
| $^{107m1}$Tc | 30.1(1) keV | 30.1(1) keV | 30.1(1) keV | 3.85(5) μs | IT | $^{107}$Tc | (1/2+) | |
| $^{107m2}$Tc | 65.72(14) keV | 65.72(14) keV | 65.72(14) keV | 184(3) ns | IT | $^{107}$Tc | (5/2+) | |
| $^{108}$Tc | 43 | 65 | 107.9184935(94) | 5.17(7) s | β$^−$ | $^{108}$Ru | (2)+ | |
| $^{109}$Tc | 43 | 66 | 108.920254(10) | 905(21) ms | β$^−$ (99.92%) | $^{109}$Ru | (5/2+) | |
| $^{109}$Tc | 43 | 66 | 108.920254(10) | 905(21) ms | β$^−$, n (0.08%) | $^{108}$Ru | (5/2+) | |
| $^{110}$Tc | 43 | 67 | 109.923741(10) | 900(13) ms | β$^−$ (99.96%) | $^{110}$Ru | (2+,3+) | |
| $^{110}$Tc | 43 | 67 | 109.923741(10) | 900(13) ms | β$^−$, n (0.04%) | $^{109}$Ru | (2+,3+) | |
| $^{111}$Tc | 43 | 68 | 110.925899(11) | 350(11) ms | β$^−$ (99.15%) | $^{111}$Ru | 5/2+# | |
| $^{111}$Tc | 43 | 68 | 110.925899(11) | 350(11) ms | β$^−$, n (0.85%) | $^{110}$Ru | 5/2+# | |
| $^{112}$Tc | 43 | 69 | 111.9299417(59) | 323(6) ms | β$^−$ (98.5%) | $^{112}$Ru | (2+) | |
| $^{112}$Tc | 43 | 69 | 111.9299417(59) | 323(6) ms | β$^−$, n (1.5%) | $^{111}$Ru | (2+) | |
| $^{112m}$Tc | 352.3(7) keV | 352.3(7) keV | 352.3(7) keV | 150(17) ns | IT | $^{112}$Tc | | |
| $^{113}$Tc | 43 | 70 | 112.9325690(36) | 152(8) ms | β$^−$ (97.9%) | $^{113}$Ru | 5/2+# | |
| $^{113}$Tc | 43 | 70 | 112.9325690(36) | 152(8) ms | β$^−$, n (2.1%) | $^{112}$Ru | 5/2+# | |
| $^{113m}$Tc | 114.4(5) keV | 114.4(5) keV | 114.4(5) keV | 527(16) ns | IT | $^{113}$Tc | 5/2−# | |
| $^{114}$Tc | 43 | 71 | 113.93709(47) | 121(9) ms | β$^−$ (98.7%) | $^{114}$Ru | 5+# | |
| $^{114}$Tc | 43 | 71 | 113.93709(47) | 121(9) ms | β$^−$, n (1.3%) | $^{113}$Ru | 5+# | |
| $^{114m}$Tc | 160(430) keV | 160(430) keV | 160(430) keV | 90(20) ms | β$^−$ (98.7%) | $^{114}$Ru | 1+# | |
| $^{114m}$Tc | 160(430) keV | 160(430) keV | 160(430) keV | 90(20) ms | β$^−$, n (1.3%) | $^{113}$Ru | 1+# | |
| $^{115}$Tc | 43 | 72 | 114.94010(21)# | 78(2) ms | β$^−$ | $^{115}$Ru | 5/2+# | |
| $^{116}$Tc | 43 | 73 | 115.94502(32)# | 57(3) ms | β$^−$ | $^{116}$Ru | 2+# | |
| $^{117}$Tc | 43 | 74 | 116.94832(43)# | 44.5(30) ms | β$^−$ | $^{117}$Ru | 5/2+# | |
| $^{118}$Tc | 43 | 75 | 117.95353(43)# | 30(4) ms | β$^−$ | $^{118}$Ru | 2+# | |
| $^{119}$Tc | 43 | 76 | 118.95688(54)# | 22(3) ms | β$^−$ | $^{119}$Ru | 5/2+# | |
| $^{120}$Tc | 43 | 77 | 119.96243(54)# | 21(5) ms | β$^−$ | $^{120}$Ru | 3+# | |
| $^{121}$Tc | 43 | 78 | 120.96614(54)# | 22(6) ms | β$^−$ | $^{121}$Ru | 5/2+# | |
| $^{122}$Tc | 43 | 79 | 121.97176(32)# | 13# ms [>550 ns] | | | 1+# | |
| This table header & footer: view |||||||||
* ↑ $^m$Tc – 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).
* ↑ Modes of decay: EC:Electron capture IT:Isomeric transition n:Neutron emission p:Proton emission
* ↑ Bold italics symbol as daughter – Daughter product is nearly stable.
* ↑ Bold symbol as daughter – Daughter product is stable.
* ↑ ( ) spin value – Indicates spin with weak assignment arguments.
* 1 2 # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
* ↑ Long-lived fission product
* ↑ Used in medicine
* 1 2 Order of ground state and isomer is uncertain.

## Stability of technetium isotopes

Technetium and promethium are unusual light elements in that they have no stable isotopes. Using the liquid drop model for atomic nuclei, one can derive a semiempirical formula for the binding energy of a nucleus. This formula predicts a "valley of beta stability" along which nuclides do not undergo beta decay. Nuclides that lie "up the walls" of the valley tend to decay by beta decay towards the center (by emitting an electron, emitting a positron, or capturing an electron). For a fixed number of nucleons A, the binding energies lie on one or more parabolas, with the most stable nuclide at the bottom. One can have more than one parabola because isotopes with an even number of protons and an even number of neutrons are more stable than isotopes with an odd number of neutrons and an odd number of protons. A single beta decay then transforms one into the other. When there is only one parabola, there can be only one stable isotope lying on that parabola. When there are two parabolas, that is, when the number of nucleons is even, it can happen (rarely) that there is a stable nucleus with an odd number of neutrons and an odd number of protons (although this happens only in five instances: $^2$H, $^6$Li, $^{10}$B, $^{14}$N and $^{180m}$Ta). However, if this happens, there can be no stable isotope with an even number of neutrons and an even number of protons.
For technetium (Z = 43), the valley of beta stability is centered at around 98 nucleons. However, for every number of nucleons from 94 to 102, there is already at least one stable nuclide of either molybdenum (Z = 42) or ruthenium (Z = 44), and the Mattauch isobar rule states that two adjacent isobars cannot both be stable. For the isotopes with odd numbers of nucleons, this immediately rules out a stable isotope of technetium, since there can be only one stable nuclide with a fixed odd number of nucleons. For the isotopes with an even number of nucleons, since technetium has an odd number of protons, any isotope must also have an odd number of neutrons. In such a case, the presence of a stable nuclide having the same number of nucleons and an even number of protons rules out the possibility of a stable nucleus.