Abstract

The effect of gravity and proper acceleration on the frequency spectrum of an optical resonator—both rigid or deformable—is considered in the framework of general relativity. The optical resonator is modeled either as a rod of matter connecting two mirrors or as a dielectric rod whose ends function as mirrors. Explicit expressions for the frequency spectrum are derived for the case that it is only perturbed slightly and variations are slow enough to avoid any elastic resonances of the rod. For a deformable resonator, the perturbation of the frequency spectrum depends on the speed of sound in the rod supporting the mirrors. A connection is found to a relativistic concept of rigidity when the speed of sound approaches the speed of light. In contrast, the corresponding result for the assumption of Born rigidity is recovered when the speed of sound becomes infinite. The results presented in this article can be used as the basis for the description of optical and opto-mechanical systems in a curved spacetime. We apply our results to the examples of a uniformly accelerating resonator and an optical resonator in the gravitational field of a small moving sphere. To exemplify the applicability of our approach beyond the framework of linearized gravity, we consider the fictitious situation of an optical resonator falling into a black hole.

Highlights

  • In general relativity (GR), as coordinates have no physical meaning, there is no unique concept for the length of a matter system

  • The results presented in this article can be used as the basis for the description of optical and opto-mechanical systems in a curved spacetime

  • 0, which means that the phase a l is constant along the light rays. We will use these properties of the eikonal function and its gradient to derive the frequency spectrum of the optical resonator in the following

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Summary

18 May 2018

Dennis Rätzel , Fabienne Schneiter, Daniel Braun , Tupac Bravo, Richard Howl, Maximilian P E Lock and Ivette Fuentes. Any further distribution of rigid or deformable—is considered in the framework of general relativity. Perturbed slightly and variations are slow enough to avoid any elastic resonances of the rod. The perturbation of the frequency spectrum depends on the speed of sound in the rod supporting the mirrors. A connection is found to a relativistic concept of rigidity when the speed of sound approaches the speed of light. The corresponding result for the assumption of Born rigidity is recovered when the speed of sound becomes infinite. To exemplify the applicability of our approach beyond the framework of linearized gravity, we consider the fictitious situation of an optical resonator falling into a black hole

Introduction
A rigid one-dimensional resonator in a curved spacetime
Resonance frequencies
Born rigid optical resonators
Deformable optical resonators
Deformable dielectric optical resonators
Example: uniform acceleration
Example: plunge into a black hole
Example: an oscillating mass
10. Conclusions and outlook
Full Text
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