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Nuclear clock based on the Th V ion

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arxiv 2503.04081 v2 pith:AA3FBJEH submitted 2025-03-06 physics.atom-ph

classification physics.atom-ph
keywords nuclearclockfrequencyomegablack-bodyelectronsenergyions
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

We propose that a nuclear clock based on the Th V ion can surpass the accuracy of clocks built with other thorium ions. The Th$^{4+}$ ion has a rigid closed-shell core with zero total electron angular momentum, suppressing frequency shifts from black-body radiation and stray external fields that act mainly on electrons. We calculate the energy shift of the nuclear clock transition frequency in $^{229}$Th due to the Coulomb field of atomic electrons and find a relative frequency difference of $2.8 \times 10^{-7}$ between Th IV and Th V - twelve orders of magnitude larger than the projected $10^{-19}$ fractional uncertainty of a nuclear clock. We also perform calculations for Th V energy levels, ionization potential, static polarizability, and the black-body radiation shift of the nuclear line. Additionally, we determine the nuclear transition frequencies in two thorium ions and neutral atom: $\omega_N=2,020,406.964(70)$ GHz in Th III, $\omega_N=2,020,408.264(100)$ GHz in Th II, and $\omega_N=2,020,408.364(100)$ GHz in Th I.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Using the Th III Ion for a Nuclear Clock and Searches for New Physics

    physics.atom-ph 2024-12 conditional novelty 6.0 of 10

    Predicted 10,000-fold electronic-bridge enhancement for exciting the 229Th nuclear clock transition in Th III, plus a 1.7-times lifetime reduction and strong new-physics sensitivity factors.

  2. Electronic Bridge processes in $^{229}$Th-doped LiCAF and LiSAF

    physics.atom-ph 2025-07 conditional novelty 5.0 of 10

    In thorium-doped LiCAF and LiSAF crystals, laser-assisted electronic bridge processes can excite and quench the 229Th nuclear clock transition far faster than direct laser excitation or radiative decay.

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