Hf$^{12+}$ ion: Highly Charged Ion for Next-Generation Atomic Clocks and Tests of Fundamental Physics
Saleh O. Allehabi, V. A. Dzuba, V. V. Flambaum
TL;DR
This paper evaluates Hf$^{12+}$ as a candidate for next-generation optical clocks and sensitive tests of fundamental physics. Using the CIPT method to handle its open $4f$ shell, the authors compute energies, lifetimes, and transition properties for two clock transitions: a strongly $p$–$f$-type transition with high $\alpha$-sensitivity and an anchor E2 transition within the ground-state configuration. They demonstrate exceptionally small polarizabilities and Blackbody Radiation shifts, along with reduced quadrupole shifts, and propose sympathetic cooling with Be$^+$ to enable practical implementation. The study shows that Hf$^{12+}$ combines high precision timekeeping with powerful sensitivity to potential variations in the fine-structure constant, offering a viable route for precision metrology and tests of new physics.
Abstract
We use advanced computational techniques to study the electronic structure of the Hf$^{12+}$ ion, with the goal of assessing its potential for use in highly accurate atomic optical clocks and search for new physics. Such clocks should combine low sensitivity to external perturbations with high sensitivity to a possible time variation of the fine-structure constant $α$. The system features two clock transitions. One is an $f-p$ transition in terms of single-electron states, which exhibits strong sensitivity to variations in $α$. The other is an electric-quadrupole (E2) transition between states of the ground-state configuration, which can serve as an anchor transition for measuring one frequency against the other. All three relevant states possess very small and nearly equal static dipole polarizabilities, resulting in an extremely small blackbody-radiation shift. The quadrupole shift is also small and can be further suppressed. Altogether, Hf$^{12+}$ appears to be a highly promising candidate for both precision timekeeping and searches for new physics.
