Proton transport from the antimatter factory of CERN
- 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. A. Devlin
- Y. Matsuda
- C. Ospelkaus
- W. Quint
- A. Soter
- J. Walz
- Y. Yamazaki
- S. Ulmer
- C. Smorra
2025-05-14
Precision measurements using low-energy antiprotons, exclusively available at the antimatter factory (AMF) of CERN 1 , offer stringent tests of charge–parity–time (CPT) invariance, which is a fundamental symmetry in the Standard Model of particle physics 2 . These tests have been realized, for example, in antiprotonic helium 3 and antihydrogen 4 . In our cryogenic Penning-trap experiments 5 , we measure the magnetic moments 6,7 and charge-to-mass ratios of protons and antiprotons and now provide the most precise test of CPT invariance in the baryon sector 8 . 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-STEP 9 —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 truck 10 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 ions 13,14 .