Fundamental Limitations of Cavity-assisted Atom Interferometry
arXiv:1710.02448 · doi:10.1103/PhysRevA.96.053820
Abstract
Atom interferometers employing optical cavities to enhance the beam splitter pulses promise significant advances in science and technology, notably for future gravitational wave detectors. Long cavities, on the scale of hundreds of meters, have been proposed in experiments aiming to observe gravitational waves with frequencies below 1 Hz, where laser interferometers, such as LIGO, have poor sensitivity. Alternatively, short cavities have also been proposed for enhancing the sensitivity of more portable atom interferometers. We explore the fundamental limitations of two-mirror cavities for atomic beam splitting, and establish upper bounds on the temperature of the atomic ensemble as a function of cavity length and three design parameters: the cavity g-factor, the bandwidth, and the optical suppression factor of the first and second order spatial modes. A lower bound to the cavity bandwidth is found which avoids elongation of the interaction time and maximizes power enhancement. An upper limit to cavity length is found for symmetric two-mirror cavities, restricting the practicality of long baseline detectors. For shorter cavities, an upper limit on the beam size was derived from the geometrical stability of the cavity. These findings aim to aid the design of current and future cavity-assisted atom interferometers.
arXiv comment11 pages, 12 figures
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- Fast control of atom-light interaction in a narrow linewidth cavity
- Degenerate optical resonator for the enhancement of large laser beams
- Doppler Compensated Cavity For Atom Interferometry
- Circulating pulse cavity enhancement as a method for extreme momentum transfer atom interferometry