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physics.atom-ph2026

Parity non-conservation in isotope chain of tin

V. A. Dzuba, V. V. Flambaum, D. DeMille +2

We calculate parity non-conservation (PNC) amplitudes for all magnetic-dipole (M1) transitions within the ground configuration of Sn, including the standard model interactio…

physics.atom-ph2026

Shielded inner-shell transitions in atomic samarium for tests of fundamental physics

R. Aramyan, D. Budker, V. A. Dzuba +5

Forbidden atomic transitions provide some of the most stringent low-energy tests of physics beyond the Standard Model, with sensitivity set by the interplay between the sought-for…

physics.atom-ph2026

Parity Nonconservation in Rb and Sr due to Low-Mass Vector Boson

V. A. Dzuba, V. V. Flambaum, G. K. Vong

We calculate the parity non-conserving (PNC) electric-dipole () transition amplitudes for the and transitions in Rb and Sr. Our results include bo…

physics.atom-ph2025

Hf ion: Highly Charged Ion for Next-Generation Atomic Clocks and Tests of Fundamental Physics

Saleh O. Allehabi, V. A. Dzuba, V. V. Flambaum

We use advanced computational techniques to study the electronic structure of the Hf ion, with the goal of assessing its potential for use in highly accurate atomic optical…

physics.atom-ph2025

Isotope shift for total electron binding energy of atoms

V. A. Dzuba, V. V. Flambaum

We compute the isotope shifts of the \emph{total} electron binding energy of neutral atoms and singly charged ions up to element , using relativistic Hartree-Fock method inc…

physics.atom-ph2025

Electronic structure calculation for superheavy elements Livermorium (Lv, Z=116) and Tennessine (Ts, Z=117) and their lighter analogs Te, I, Po, and At

V. A. Dzuba, V. V. Flambaum, G. K. Vong

Advanced theoretical techniques that combine the linearized coupled-cluster method, configuration interaction method, and perturbation theory are used to calculate energy levels, i…