22.–23. Jan. 2026
GSI
Europe/Berlin Zeitzone

Towards Testing Three-Loop QED and Nuclear Deformation Effects in Heliumlike Uranium

22.01.2026, 18:00
1 h 30m
Canteen Side Room (GSI)

Canteen Side Room

GSI

Sprecher

Martino Trassinelli (Insitut des NanoSciences de Paris)

Beschreibung

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. By accurately measuring the relative energies between $2p_{3/2} \to 2s_{1/2}$ transitions (of an energy of about 4.5 keV) 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. Such a precise measurement has been obtained by implementing a novel multi-reference method based on Doppler-tuned x-ray emission from fast ions stored in the ESR ring of the GSI/FAIR facility and using a pair of crystal diffractometers.
Experimental outlooks will also be presented, in which a new calibration scheme using a light reference ion and the implementation of a new time- and position-sensitive detector will be used. Together, these improvements are expected to reduce uncertainties to about 9 meV—ten times lower than current theoretical predictions and nuclear deformation effects. This approach opens a new pathway for probing the nuclear properties of heavy nuclei.

Autoren

Martino Trassinelli (Insitut des NanoSciences de Paris) R. Loetzsch (Helmholtz-Institut Jena, Jena, Germany) H.F. Beyer (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) L. Duval (Laboratoire Kastler Brossel, Sorbonne Université, ENS-PSL, Collège de France, CNRS, Paris, France) U. Spillmann (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) D. Banas (Institute of Physics, Jan Kochanowski University, Kielce, Poland) P. Dergham (Institut des NanoSciences de Paris, CNRS, Sorbonne Université, Paris, France) F.M. Kröger (Helmholtz-Institut Jena, Jena, Germany) J. Glorius (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) R.E. Grisenti (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) M. Guerra (Laboratory of Instrumentation, Biomedical Engineering and Radiation Physics, NOVA University Lisbon, Caparica, Portugal) A. Gumberidze (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) R. Heiss (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) P.-M. Hillenbrand (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) P. Indelicato (Laboratoire Kastler Brossel, Sorbonne Université, ENS-PSL, Collège de France, CNRS, Paris, France) P. Jagodzinski (4Institute of Physics, Jan Kochanowski University, Kielce, Poland) E. Lamour (Institut des NanoSciences de Paris, CNRS, Sorbonne Université, Paris, France) B. Lorentz (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) S. Litvinov (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) Yu.A. Litvinov (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) J. Machado (Laboratory of Instrumentation, Biomedical Engineering and Radiation Physics, NOVA University Lisbon, Caparica, Portugal) S. Mekhloufi (Institut des NanoSciences de Paris, CNRS, Sorbonne Université, Paris, France) G.G. Paulus (Helmholtz-Institut Jena, Jena, Germany) N. Paul (Laboratoire Kastler Brossel, Sorbonne Université, ENS-PSL, Collège de France, CNRS, Paris, France) G.G. Paulus (Helmholtz-Institut Jena, Jena, Germany) N. Petridis (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) M. Steck (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany) S. Steydli (Institut des NanoSciences de Paris, CNRS, Sorbonne Université, Paris, France) K. Szary (Institute of Physics, Jan Kochanowski University, Kielce, Poland) S. Trotsenko (Helmholtz-Institut Jena, Jena, Germany) I. Uschmann (Helmholtz-Institut Jena, Jena, Germany) G. Weber (Helmholtz-Institut Jena, Jena, Germany) Th. Stöhlker (GSI Helmholtzzentrum für Schwerionenforschung, Darmstadt, Germany)

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