Detection-resolution limits of large-momentum-transfer atom gravimetry
- URL: http://arxiv.org/abs/2607.28749v1
- Date: Thu, 30 Jul 2026 18:16:06 GMT
- Title: Detection-resolution limits of large-momentum-transfer atom gravimetry
- Abstract summary: Large momentum transfer (LMT) enhances the gravitational phase of a light-pulse atom interferometer by a factor $n$.<n> mirrorless operation with momentum-resolved detection can quadruple the phase-carrying quantum Fisher information.<n>We analyze this trade-off in a solvable model with instantaneous sensitivity $n$-photon pulses, a Gaussian source, and Gaussian detection blur.
- Score: 1.2633386045916446
- License: http://creativecommons.org/licenses/by/4.0/
- Abstract: Large momentum transfer (LMT) enhances the gravitational phase of a light-pulse atom interferometer by a factor $n$, while mirrorless operation with momentum-resolved detection can quadruple the phase-carrying quantum Fisher information. These gains compete in practice because the momentum-space fringe period scales as $1/n$, making the fringe signal increasingly vulnerable to finite detector resolution. We analyze this trade-off in a solvable model with instantaneous lossless $n$-photon pulses, a Gaussian source, and Gaussian detection blur, allowing continuous interpolation between Kasevich--Chu and mirrorless geometries. Closed-form expressions for the blurred output distributions and classical Fisher information are obtained, with a fringe-phase averaging approximation whose error is exponentially suppressed and agrees with numerical simulations at the $10^{-8}$ level. We find that mirrorless operation surpasses a conventional interferometer with the same momentum transfer only when $σ_p < 0.91\,m/(n k_0 T)$. Fringe-based readout exhibits an optimal momentum transfer $n^* \simeq 0.93\,m/(σ_p k_0 T)$ and a resolution-limited sensitivity floor $Δg \simeq 4.4\,σ_p/(mT\sqrt{N})$, independent of photon momentum. When this criterion is not satisfied, partial mirror asymmetry can recover part of the enhancement, whereas population-based readout remains insensitive to detector blur and ultimately favors the conventional sequence at sufficiently large $n$. Estimates for $^{87}$Rb sensors show that the mirrorless advantage is primarily restricted to short-baseline instruments.
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