June 30, 2025 to July 4, 2025
Europe/Vienna timezone

Testing quantum electrodynamics in extreme fields using helium-like uranium

Jul 4, 2025, 11:30 AM
30m
Invited Speaker Fundamental physics, precision measurements, atom interferometry and atomic clocks Fundamental 2

Speaker

Martino Trassinelli (CNRS, Institut des NanoSciences)

Description

Transition energy measurements in heavy, few-electron ions are unique tools to test bound-state quantum electrodynamics (QED) in extremely high Coulomb fields, where perturbative methods cannot be implemented. In such fields, the effects of the quantum vacuum fluctuations on the atomic energies are enhanced by several orders of magnitude with respect to light atoms. However, up to now, experiments have been unable to achieve sensitivity to higher-order (two-loop) QED effects in this strong regime. Here we present a novel multi-reference method based on Doppler-tuned x-ray emission from fast uranium ions stored in the ESR ring of the GSI/FAIR facility. By accurately measuring the relative energies between $2p_{3/2} \to 2s_{1/2}$ transitions in two-, three-, and four-electron uranium ions, we were able, for the first time in this regime, to disentangle and test separately high-order (two-loop) one-electron and two-electron QED effects, and set a new important benchmark for this theory in the strong field domain [1]. The achieved accuracy of 37 parts per million allows us to discriminate between different theoretical approaches developed throughout the last decades for describing He-like systems. Experimental outlooks will be presented, as new calibration schemes and the implementation of a new time- and position-sensitive detector, based on Timepix3 technology. These considered improvements will allow for a reduction of the uncertainties by another order of magnitude, lower than the present theoretical prediction uncertainties and nuclear deformation effects.

[1] R. Loetzsch et al., Nature 625, 673-678 (2024).

Authors

R. Loetzsch (Helmholtz-Institut Jena) H. F. Beyer (GSI Helmholtzzentrum für Schwerionenforschung) Louis Duval (Institut des NanoSciences de Paris, CNRS and Sorbonne University and Laboratoire Kastler Brossel, CNRS, ENS-PSL, Collège de France, Sorbonne Université) U. Spilmann (GSI Helmholtzzentrum für Schwerionenforschung) D. Banas (Institute of Physics, Jan Kochanowski University) Perla Dergham (Institut des NanoSciences de Paris, CNRS and Sorbonne University) F. M. Kröger (Helmholtz-Institut Jena, Jena, Germany) Jan Glorius (GSI Helmholtzzentrum für Schwerionenforschung) R. Grisenti (GSI Helmholtzzentrum für Schwerionenforschung) M. Guerra (Laboratory of Instrumentation, Biomedical Engineering and Radiation Physics, NOVA University) A. Gumberidze (GSI Helmholtzzentrum für Schwerionenforschung) R. Hess (GSI Helmholtzzentrum für Schwerionenforschung) Pierre-Michele Hillenbrand (Justus-Liebig-Universität Gießen) P. Indelicato (Laboratoire Kastler Brossel, Sorbonne Université, ENS-PSL, Collège de France, CNRS) P. Jagodzinsk (Institute of Physics, Jan Kochanowski University) Emily Lamour (Institut des NanoSciences de Paris, CNRS and Sorbonne University) B. Lorentz (GSI Helmholtzzentrum für Schwerionenforschung) S. Litvinov (GSI Helmholtzzentrum für Schwerionenforschung) Y. A. Litvinov (GSI Helmholtzzentrum für Schwerionenforschung) J. Machado (Laboratory of Instrumentation, Biomedical Engineering and Radiation Physics, NOVA University) N. Paul (3Laboratoire Kastler Brossel, Sorbonne Université, ENS-PSL, Collège de France, CNRS) G. G. Paulus (Helmholtz-Institut Jena, Jena, Germany) N. Petridis (GSI Helmholtzzentrum für Schwerionenforschung) J. P. Santos (Laboratory of Instrumentation, Biomedical Engineering and Radiation Physics, NOVA University) M. Scheidel (GSI Helmholtzzentrum für Schwerionenforschung) R.S. Sidhu (GSI Helmholtzzentrum für Schwerionenforschung) M. Steck (GSI Helmholtzzentrum für Schwerionenforschung) Sébastien Steydli (Institut des NanoSciences de Paris, CNRS and Sorbonne University) K. Szary (Institute of Physics, Jan Kochanowski University) S. Trotsenko (GSI Helmholtzzentrum für Schwerionenforschung) I. Uschmann (Institut für Optik und Quantenelektronik, Friedrich-Schiller-Universität) G. Weber (GSI Helmholtzzentrum für Schwerionenforschung) T. Stöhlker (GSI Helmholtzzentrum für Schwerionenforschung) Martino Trassinelli (CNRS, Institut des NanoSciences)

Presentation materials

There are no materials yet.