Abstract
The nucleus has a long-lived isomeric state at 8.338(24) eV [Kraemer et al., Nature (London) 617, 706 (2023)]. This state is connected to the ground state by an M1 transition. For a hydrogen-like Th ion in the state the hyperfine structure splitting is about 0.7 eV. This means that the hyperfine interaction can mix the nuclear ground state with the isomeric state with a mixing coefficient of about 0.03. If the electron is suddenly removed from this system, the nucleus will be left in the mixed state. The probability to find the nucleus in the isomeric state is equal to . For the state the effect is roughly 2 orders of magnitude smaller. An atom with a hole in the or shell is similar to the hydrogen-like atom, only the hole has a short lifetime . After the hole is filled, there is a nonzero probability to find the nucleus in the state. Estimates of this probability are presented along with a discussion of possible experiments on Th-doped xenotime-type orthophosphate crystals and other broad band-gap materials.
- Received 15 August 2023
- Revised 25 February 2024
- Accepted 18 March 2024
DOI:https://doi.org/10.1103/PhysRevA.109.042806
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