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Gravitational Aharonov-Bohm Effect as a Generalization of the Gravitational Redshift

ORAL

Abstract

The Aharonov-Bohm effect is a quantum mechanical phenomenon that demonstrates how potentials can have observable effects even when the classical fields associated with those potentials are absent. Initially proposed for electromagnetic interactions, this effect has been experimentally confirmed and extensively studied over the years. More recently, the effect has been observed in the context of gravitational interactions using atom interferometry1. Additionally, recent predictions suggest that temporal variations in the phase of an electron wave function will induce modulation sidebands in the energy levels of an atomic clock, solely driven by a time-varying scalar gravitational potential2. In this study, we consider the atomic clock as a two-level system undergoing continuous Rabi oscillations between the electron's ground and excited state3. We assume the photons driving the transition are precisely frequency-stabilized to match the transition, enabling accurate clock comparisons. Our analysis takes into account, that when an atom transitions from its ground state to an excited state, it absorbs energy, increasing its mass according to the mass-energy equivalence principle. Due to the mass difference between the two energy levels, we predict that an atomic clock in an eccentric orbit will exhibit a constant frequency shift relative to a ground clock corresponding to the orbit's average gravitational redshift, with additional modulation sidebands due to the time-varying gravitational potential.

1. C Overstreet, P Asenbaum, J Curti, M Kim, MA Kasevich, Science 375, 226 (2022).

2. RY Chiao, NA Inan, M Scheibner, J Sharping, DA Singleton, ME Tobar, Phys. Rev. D 109, 064073 (2024).

3. ME Tobar, MT Hatzon, GR Flower, M Goryachev, Appl. Phys. Lett. 26, 125 (9): 094002 (2024).

Publication: Michael E. Tobar, Michael T. Hatzon, Graeme R. Flower, Maxim Goryachev; Scalar gravitational Aharonov–Bohm effect: Generalization of the gravitational redshift. Appl. Phys. Lett. 26 August 2024; 125 (9): 094002. https://doi.org/10.1063/5.0226310

Presenters

  • Michael E Tobar

    Quantum Technologies and Dark Matter Labs, Department of Physics, University of Western Australia, Quantum Technologies and Dark Matter Labs, Department of Physics, the University of Western Australia

Authors

  • Michael E Tobar

    Quantum Technologies and Dark Matter Labs, Department of Physics, University of Western Australia, Quantum Technologies and Dark Matter Labs, Department of Physics, the University of Western Australia

  • Michael T Hatzon

    Quantum Technologies and Dark Matter Labs, Department of Physics, University of Western Australia, Quantum Technologies and Dark Matter Labs, Department of Physics, the University of Western Australia

  • Graeme R Flower

    Quantum Technologies and Dark Matter Labs, Department of Physics, University of Western Australia, Quantum Technologies and Dark Matter Labs, Department of Physics, the University of Western Australia

  • Maxim Goryachev

    Quantum Technologies and Dark Matter Labs, Department of Physics, University of Western Australia, Quantum Technologies and Dark Matter Labs, Department of Physics, the University of Western Australia