CPT tests with the antihydrogen molecular ion
arXiv:1802.01514 · doi:10.1103/PhysRevA.98.010101
Abstract
High precision radio-frequency, microwave and infrared spectroscopic measurements of the antihydrogen molecular ion () compared with its normal matter counterpart provide direct tests of the CPT theorem. The sensitivity to a difference between the positron/antiproton and electron/proton mass ratios, and to a difference between the positron-antiproton and electron-proton hyperfine interactions, can exceed that obtained by comparing antihydrogen with hydrogen by several orders of magnitude. Practical schemes are outlined for measurements on a single ion in a cryogenic Penning trap, that use non-destructive state identification by measuring the cyclotron frequency and bound-positron spin-flip frequency; and also for creating an ion and initializing its quantum state.
Revised version for Phys Rev A(RC), with figure
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Cited by in corpus (10)
- Sympathetic cooling of a trapped proton mediated by an LC circuit
- Perspectives on testing fundamental physics with highly charged ions in Penning traps
- Higher-order corrections to spin-orbit and spin-spin tensor interactions in hydrogen molecular ions: theory and application to H
- Precision measurements of the fundamental properties of the proton and antiproton
- Stark quenching of rovibrational states of H2+ due to motion in a magnetic field
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- Quantum control of a single molecular ion
- Penning-trap eigenfrequency measurements with optical radiofrequency detectors
- Production and study of antideuterium with the GBAR beamline
- Bounds on Lorentz and CPT violation from the - transition in antihydrogen