Abstract
When Th nuclei are doped in CaF_{2} crystals, a set of electronic defect states appear in the crystal band gap which would otherwise provide complete transparency to vacuum-ultraviolet radiation. The coupling of these defect states to the 8eV ^{229m}Th nuclear isomer in the CaF_{2} crystal is investigated theoretically. We show that although previously viewed as a nuisance, the defect states provide a starting point for nuclear excitation via electronic bridge mechanisms involving stimulated emission or absorption using an optical laser. The rates of these processes are at least 2 orders of magnitude larger than direct photoexcitation of the isomeric state using available light sources. The nuclear isomer population can also undergo quenching when triggered by the reverse mechanism, leading to a fast and controlled decay via the electronic shell. These findings are relevant for a possible solid-state nuclear clock based on the ^{229m}Th isomeric transition.
Highlights
Recent years have witnessed the increased interest for a “nuclear anomaly” in the actinide region: the first excited state of the 229Th isotope lies only 8 eV above the ground state [1,2,3]
When Th nuclei are doped in CaF2 crystals, a set of electronic defect states appear in the crystal band gap which would otherwise provide complete transparency to vacuum-ultraviolet radiation
Theoretical density functional theory (DFT) predictions confirm the presence of defect states caused by Th doping within the crystal band gap for CaF2 in the vicinity of the nuclear transition energy [30]
Summary
Recent years have witnessed the increased interest for a “nuclear anomaly” in the actinide region: the first excited state of the 229Th isotope lies only 8 eV above the ground state [1,2,3]. Nuclear Excitation of the 229Th Isomer via Defect States in Doped Crystals
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