Isotope: Technetium-122
General data
| Element name | Technetium |
|---|---|
| Chemical symbol | Tc |
| Atomic number Z | 43 |
| Isotope name (symbol) | Technetium-122 (Tc-122) |
| Neutron number N | 79 |
| Mass number A=Z+N | 122 |
Ground state
| Half-life | unknown |
|---|---|
| Mass excess | -26300 ± 300 keV (S) |
Decay branches
β⁻ 100% β⁻n β⁻2nIsomers
no isomers in the NNDC data
No half-life data - simulation unavailable.
Produced by decay of
NNDC data contain no decay that leads to this isotope.
Many isotopes are also produced, often mainly, in nuclear reactions (e.g. Co-60 from Co-59 by neutron capture, C-14 from nitrogen-14 in the atmosphere) and in fission (e.g. Cs-137, I-131) - those routes are not listed here.
Radioactive decay series
- Technetium-122 unknown
- Ruthenium-122 25 ms
- Rhodium-122 52.3 ms
- Palladium-122 195 ms · 88.7%
- Silver-122 0.55 s · 86.7%
- Cadmium-122 5.24 s · 86.6%
- Indium-122 1.5 s · 86.6%
- Tin-122 stable · 86.6%
- Palladium-121 290 ms · 11.3%
- Silver-121 0.781 s · 13.2%
- Cadmium-121 13.5 s · 13.3%
- Indium-121 23.1 s · 13.3%
- Tin-121 27.05 h · 13.3%
- Antimony-121 stable · 13.3%
- Silver-120 1.52 s · 0.09%
- Cadmium-120 50.80 s · 0.1%
- Indium-120 3.08 s · 0.1%
- Tin-120 stable · 0.1%
Rare branches (below 0.01%)
Rare branches are transformations that occur in fewer than 0.01% of decays, e.g. double beta decay or cluster emission. The nuclides they produce are practically absent from a sample, so they are hidden by default to keep the main path clear. In this series: branches - 1, nuclides - 3.
- Cadmium-119 2.69 min · 2.7×10⁻⁶%
- Indium-119 2.4 min · 2.7×10⁻⁶%
- Tin-119 stable · 2.7×10⁻⁶%
Decay notation
| Notation | Name | On the chart | Description |
|---|---|---|---|
| α | alpha decay | Alpha decay is the emission of a helium nucleus (2 protons + 2 neutrons): Z−2, A−4. | |
| β⁻, 2β⁻ | beta-minus decay | In beta-minus decay a neutron turns into a proton and the nucleus emits an electron: Z+1, A unchanged. 2β⁻ is double beta decay. | |
| EC, EC/β⁺ | electron capture / beta-plus decay | A proton turns into a neutron: the nucleus captures a shell electron (EC) or emits a positron (β⁺): Z−1, A unchanged. | |
| p, 2p, 3p | proton emission | Proton emission is the ejection of a proton from the nucleus: Z−1, A−1. 2p, 3p - two, three protons. | |
| n, 2n…4n | neutron emission | Neutron emission is the ejection of a neutron from the nucleus: A−1, Z unchanged. 2n…4n - several neutrons. | |
| ¹⁴C, ²⁴Ne… | cluster emission | Cluster emission is the ejection of a light nucleus, e.g. ¹⁴C, ²⁰O, ²⁴Ne, ²⁸Mg, ³⁴Si. It is a very rare transformation. | |
| IT | isomeric transition | An isomeric transition takes a nucleus from an excited state (an isomer, e.g. Pa-234m) to the ground state, usually emitting a γ photon: Z and A unchanged. | |
| β⁻n, ECp, ECα… | delayed emission | Delayed emission is the emission of a particle (n, p or α) right after β⁻ decay or electron capture. The arrow has the colour of the emitted particle and its label shows the transformation, e.g. “β⁻n 63%”. | |
| SF | spontaneous fission | no arrow | Spontaneous fission is the splitting of a nucleus into two fragments of random masses. There is no single daughter, so the chart shows no arrow - it is listed in the decay branches and in the tile tooltip. |
Data sources
- NNDC Wallet Cards 2023 - Data as of 15 October 2024 - licence: Public domain