In resonant-mode atom-interferometer gravitational wave detectors, the optimal number of pulses is set mainly by per-pulse atom loss, and current large-pulse-number proposals demand fidelities roughly two orders of magnitude beyond the state of the art.
Finite-Speed-of-Light Effects in Atom Interferometry: Diffraction Mechanisms and Resonance Conditions
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abstract
Light-pulse atom interferometers serve as tools for high-precision metrology and are targeting measurements of relativistic effects. This development is facilitated by extended interrogation times and large-momentum-transfer techniques generating quantum superpositions of both interferometer arms on large distances. Due to the finite speed of light, diffracting light pulses cannot interact simultaneously with both arms, inducing phase perturbations that compromise the accuracy of the sensor -- an effect that becomes progressively important as spatial separations increase. For a consistent framework, we develop a theory for finite-speed-of-light effects in atom interferometers alongside with other relativistic effects such as the mass defect. Our analysis shows that their magnitude depends crucially on the diffraction mechanism and the specific interferometer geometry. We demonstrate that the velocity of the atomic cloud at the mirror pulse of a Mach-Zehnder interferometer is less critical than the precise tuning of the lasers for resonant diffraction. Finally, we propose an experiment to test our predictions based on recoilless transitions and discuss mitigation strategies to reduce the bias in gravimetric applications.
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Spatial and Pulse Efficiency Constraints in Atom Interferometric Gravitational Wave Detectors
In resonant-mode atom-interferometer gravitational wave detectors, the optimal number of pulses is set mainly by per-pulse atom loss, and current large-pulse-number proposals demand fidelities roughly two orders of magnitude beyond the state of the art.