Testing quantum electrodynamics in extreme fields using helium-like uranium

R. Loetzsch, H. F. Beyer, L. Duval, U. Spillmann, D. Banaś, P. Dergham, F. M. Kröger, J. Glorius, R. E. Grisenti, M. Guerra, A. Gumberidze, R. Heß,P.-M. Hillenbrand, P. Indelicato, P. Jagodzinski, E. Lamour,B. Lorentz, S. Litvinov,Yu. A. Litvinov, J. Machado,N. Paul, G. G. Paulus,N. Petridis,J. P. Santos, M. Scheidel, R. S. Sidhu, M. Steck, S. Steydli, K. Szary, S. Trotsenko, I. Uschmann, G. Weber,Th. Stöhlker,M. Trassinelli

Nature(2024)

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摘要
Quantum electrodynamics (QED), the quantum field theory that describes the interaction between light and matter, is commonly regarded as the best-tested quantum theory in modern physics. However, this claim is mostly based on extremely precise studies performed in the domain of relatively low field strengths and light atoms and ions 1 – 6 . In the realm of very strong electromagnetic fields such as in the heaviest highly charged ions (with nuclear charge Z ≫ 1), QED calculations enter a qualitatively different, non-perturbative regime. Yet, the corresponding experimental studies are very challenging, and theoretical predictions are only partially tested. Here we present an experiment sensitive to higher-order QED effects and electron–electron interactions in the high- Z regime. This is achieved by using a multi-reference method based on Doppler-tuned X-ray emission from stored relativistic uranium ions with different charge states. The energy of the 1 s 1/2 2 p 3/2 J = 2 → 1 s 1/2 2 s 1/2 J = 1 intrashell transition in the heaviest two-electron ion (U 90+ ) is obtained with an accuracy of 37 ppm. Furthermore, a comparison of uranium ions with different numbers of bound electrons enables us to disentangle and to test separately the one-electron higher-order QED effects and the bound electron–electron interaction terms without the uncertainty related to the nuclear radius. Moreover, our experimental result can discriminate between several state-of-the-art theoretical approaches and provides an important benchmark for calculations in the strong-field domain.
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