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Testing Strong-Field QED to Second Order in the Highly Correlated Atomic System Berylliumlike Pb78+ by Electron-Ion Collision Spectroscopy

S. Schippers1,2, C. Brandau1,3, S. Fuchs1,2, M. Lestinsky3, S. X. Wang1,2, C. Y. Zhang4, N. R. Badnell4, A. Borovik, Jr.1,5, M. Fogle6 et al.

V. Hannen7, Z. Harman8, P.-M. Hillenbrand1,3, E. B. Menz3,5, Y. Zhang8,9, Z. Andelkovic3, F. Herfurth3, R. Heß3, A. Kalinin3, C. Kozhuharov3, C. Krantz3, S. Litvinov3, B. Lorentz3, U. Spillmann3, M. Steck3, G. Vorobyev3, D. Banaś10, S. Fritzsche3,5,11, E. Lindroth12, X. Ma13, A. Müller1, R. Schuch12, A. Surzhykov14,15, M. Trassinelli16, K. Ueberholz7, C. Weinheimer7, and Th. Stöhlker3,5,17

Phys. Rev. Lett. 135, 113001 – Published 10 September, 2025

DOI: https://doi.org/10.1103/6j3v-lwxj

Abstract

A low-energy storage ring with an ultracold electron cooler has been coupled with a heavy-ion accelerator facilitating high-resolution electron-ion collision spectroscopy of the heaviest few-electron ions. In the present Letter resonant electron-ion recombination of berylliumlike Pb78+ ions was measured in the collision-energy range 9.3–16.5 eV and a value of 244.937(30) eV is derived for the Pb78+(2s2 S10−2s2p P31) excitation energy. This result agrees with the most recent (less accurate) theoretical value of 244.942(52) eV [Malyshev et al., Phys. Rev. A 110, 062824 (2024)], which has been calculated by applying strong-field QED rigorously up to the second order. The present investigation suggests that further technical improvements can potentially increase the experimental accuracy by an order of magnitude.

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