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Proton transport from the antimatter factory of CERN

Author

Listed:
  • M. Leonhardt

    (Heinrich Heine Universität Düsseldorf
    RIKEN)

  • D. Schweitzer

    (Heinrich Heine Universität Düsseldorf
    Johannes Gutenberg-Universität)

  • F. Abbass

    (Heinrich Heine Universität Düsseldorf
    Johannes Gutenberg-Universität)

  • K. K. Anjum

    (GSI-Helmholtzzentrum für Schwerionenforschung)

  • B. Arndt

    (GSI-Helmholtzzentrum für Schwerionenforschung
    Max-Planck-Institut für Kernphysik)

  • S. Erlewein

    (Heinrich Heine Universität Düsseldorf
    CERN)

  • S. Endoh

    (RIKEN
    University of Tokyo)

  • P. Geissler

    (RIKEN)

  • T. Imamura

    (Leibniz Universität
    Physikalisch-Technische Bundesanstalt)

  • J. I. Jäger

    (Max-Planck-Institut für Kernphysik
    CERN)

  • B. M. Latacz

    (CERN)

  • P. Micke

    (Max-Planck-Institut für Kernphysik
    CERN
    Friedrich-Schiller-Universität Jena)

  • F. Voelksen

    (Heinrich Heine Universität Düsseldorf)

  • H. Yildiz

    (Johannes Gutenberg-Universität)

  • K. Blaum

    (Max-Planck-Institut für Kernphysik)

  • J. A. Devlin

    (Imperial College London)

  • Y. Matsuda

    (University of Tokyo)

  • C. Ospelkaus

    (Leibniz Universität
    Physikalisch-Technische Bundesanstalt)

  • W. Quint

    (GSI-Helmholtzzentrum für Schwerionenforschung)

  • A. Soter

    (ETH Zürich)

  • J. Walz

    (Johannes Gutenberg-Universität
    Helmholtz-Institut Mainz)

  • Y. Yamazaki

    (RIKEN)

  • S. Ulmer

    (Heinrich Heine Universität Düsseldorf
    RIKEN)

  • C. Smorra

    (Heinrich Heine Universität Düsseldorf)

Abstract

Precision measurements using low-energy antiprotons, exclusively available at the antimatter factory (AMF) of CERN1, offer stringent tests of charge–parity–time (CPT) invariance, which is a fundamental symmetry in the Standard Model of particle physics2. These tests have been realized, for example, in antiprotonic helium3 and antihydrogen4. In our cryogenic Penning-trap experiments5, we measure the magnetic moments6,7 and charge-to-mass ratios of protons and antiprotons and now provide the most precise test of CPT invariance in the baryon sector8. Our experiments are limited by magnetic field fluctuations imposed by the decelerators in the AMF; therefore, we are advancing the relocation of antiprotons to dedicated precision laboratories. Here we present the successful transport of a trapped proton cloud from the AMF using BASE-STEP9—a transportable, superconducting, autonomous and open Penning-trap system that can distribute antiprotons into other experiments. We transferred the trapped protons from our experimental area at the AMF onto a truck and transported them across the Meyrin site of CERN, demonstrating autonomous operation without external power for 4 h and loss-free proton relocation. We thereby confirm the feasibility of transferring particles into low-noise laboratories in the vicinity of the AMF and of using a power generator on the truck10 to reach laboratories throughout Europe. This marks the potential start of a new era in precision antimatter research, enabling low-noise measurements of antiprotons, the charged antimatter ions $${\bar{{\rm{H}}}}^{+}$$ H ¯ + 11 and $${\bar{{\rm{H}}}}_{2}^{-}$$ H ¯ 2 − (ref. 12), and other accelerator-produced ions, such as hydrogen-like lead or uranium ions13,14.

Suggested Citation

  • M. Leonhardt & D. Schweitzer & F. Abbass & K. K. Anjum & B. Arndt & S. Erlewein & S. Endoh & P. Geissler & T. Imamura & J. I. Jäger & B. M. Latacz & P. Micke & F. Voelksen & H. Yildiz & K. Blaum & J. , 2025. "Proton transport from the antimatter factory of CERN," Nature, Nature, vol. 641(8064), pages 871-875, May.
  • Handle: RePEc:nat:nature:v:641:y:2025:i:8064:d:10.1038_s41586-025-08926-y
    DOI: 10.1038/s41586-025-08926-y
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