Sympathetic cooling of a trapped proton mediated by an LC circuit

• DOI: 10.1038/s41586-021-03784-w
• Publication Date: 2021-08-25T16:03:37Z
• Authors: M. Bohman; V. Grunhofer; C. Smorra; M. Wiesinger; C. Will; M. J. Borchert; J. A. Devlin; S. Erlewein; M. Fleck; S. Gavranovic; J. Harrington; B. Latacz; A. Mooser; D. Popper; E. Wursten; K. Blaum; Y. Matsuda; C. Ospelkaus; W. Quint; J. Walz; S. Ulmer
• Keywords: Quantum Physics; cooling; Atomic Physics (physics.atom-ph); 500; FOS: Physical sciences; 7. Clean energy; Article; experimental study; Physics - Atomic Physics; unclassified drug; trapped proton; Präzisionsexperimente - Abteilung Blaum; Quantum Physics (quant-ph); Dewey Decimal Classification::500 | Naturwissenschaften; info:eu-repo/classification/ddc/500; proton

AbstractEfficient cooling of trapped charged particles is essential to many fundamental physics experiments1,2, to high-precision metrology3,4 and to quantum technology5,6. Until now, sympathetic cooling has required close-range Coulomb interactions7,8, but there has been a sustained desire to bring laser-cooling techniques to particles in macroscopically separated traps5,9,10, extending quantum control techniques to previously inaccessible particles such as highly charged ions, molecular ions and antimatter. Here we demonstrate sympathetic cooling of a single proton using laser-cooled Be+ ions in spatially separated Penning traps. The traps are connected by a superconducting LC circuit that enables energy exchange over a distance of 9 cm. We also demonstrate the cooling of a resonant mode of a macroscopic LC circuit with laser-cooled ions and sympathetic cooling of an individually trapped proton, reaching temperatures far below the environmental temperature. Notably, as this technique uses only image–current interactions, it can be easily applied to an experiment with antiprotons1, facilitating improved precision in matter–antimatter comparisons11 and dark matter searches12,13.