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Physical Review A

Phase estimation in an atom interferometer with finite-resolution single-atom position measurements

Katarzyna Kowalczyk-Murynka

Published Aug 27, 2015• 0 citations
Publisher

Abstract

We conduct a detailed analysis of a phase estimation experiment with a Bose-Einstein condensate in a double potential well. Our goal is to confront the theoretical considerations with the conditions of a real experiment. We present a typical experimental procedure and the theoretical model. We simulate the estimation of phase between two modes in two cases: based on the full correlation function measurement for two atoms and on the center of mass position measurement for 20 atoms. We show that a lossless atom detection lets us exceed the shot noise (that is purely classical) limit of phase estimation precision with the currently available spatial resolution, while a few times higher resolution will make it possible to approach the highest precision allowed by quantum physics.

DOI
10.1103/physreva.92.023639

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We conduct a detailed analysis of a phase estimation experiment with a Bose-Einstein condensate in a double potential well. Our goal is to confront the theoretical considerations with the conditions of a real experiment. We present a typical experimental procedure and the theoretical model. We simulate the estimation of phase between two modes in two cases: based on the full correlation function measurement for two atoms and on the center of mass position measurement for 20 atoms. We show that a lossless atom detection lets us exceed the shot noise (that is purely classical) limit of phase estimation precision with the currently available spatial resolution, while a few times higher resolution will make it possible to approach the highest precision allowed by quantum physics.
We study the measurement of the positions of atoms as a means of estimating the relative phase between two Bose–Einstein condensates. We consider N bosonic atoms released from a double-well trap, which form an interference pattern; we show that the measurement of the position of N atoms has a sensitivity that saturates the bound set by the quantum Fisher information, and allows for estimation at the Heisenberg limit of precision. Phase estimation through the measurement of the center of mass of the interference pattern can also provide sub-shot-noise sensitivity. Finally, we study the effect of an overlap of the two clouds on the estimation precision when Mach–Zehnder interferometry is performed in a double well. We find that a nonzero overlap of the clouds strongly reduces the phase sensitivity.
We investigate how to estimate from atom-position measurements the relative phase of two Bose-Einstein condensates released from a double-well potential. We demonstrate that the phase-estimation sensitivity via the fit of the average density to the interference pattern is fundamentally bounded by shot noise. The shot noise can be overcome by estimating the phase from the measurement of order N\sqrt{N}N​ (or higher) correlation functions. The optimal estimation strategy, saturating the quantum Fisher information, requires the measurement of the NNNth-order correlation function. We demonstrate that a different estimation method---based on the detection of the center of mass of the interference pattern---also provides sub-shot-noise sensitivity. The implementation of both protocols, however, might be experimentally challenging.
We study the measurement of the positions of atoms as a means of estimating the relative phase between two Bose–Einstein condensates. We consider N bosonic atoms released from a double-well trap, which form an interference pattern; we show that the measurement of the position of N atoms has a sensitivity that saturates the bound set by the quantum Fisher information, and allows for estimation at the Heisenberg limit of precision. Phase estimation through the measurement of the center of mass of the interference pattern can also provide sub-shot-noise sensitivity. Finally, we study the effect of an overlap of the two clouds on the estimation precision when Mach–Zehnder interferometry is performed in a double well. We find that a nonzero overlap of the clouds strongly reduces the phase sensitivity.
We derive the asymptotic maximum-likelihood phase estimation uncertainty for any interferometric protocol where the positions of the probe particles are measured to infer the phase, but where correlations between the particles are not accessible. First, we apply our formula to the estimation of the phase acquired in the Mach–Zehnder interferometer and recover the well-known momentum formula for the phase sensitivity. Then, we apply our results to interferometers with two spatially separated modes, which could be implemented with a Bose–Einstein condensate trapped in a double-well potential. We show that in a simple protocol which estimates the phase from an interference pattern, a sub-shot-noise phase uncertainty of up to Δ θ ∝ N −2/3 can be achieved. One important property of this estimation protocol is that its sensitivity does not depend on the value of the phase θ , contrary to the sensitivity given by the momentum formula for the Mach–Zehnder transformation. Finally, we study the experimental implementation of the above protocol in detail, by numerically simulating the full statistics as well as by considering the main sources of detection noise, and argue that the shot-noise limit could be surpassed with current technology.
Whenever the value of an unknown parameter $\ensuremath{\theta}$ is extracted from a series of experiments, the result is inevitably burdened by the uncertainty $\ensuremath{\Delta}\ensuremath{\theta}$. If the system that is the subject of measurement consists of unentangled particles, this uncertainty is bounded by the shot-noise limit. To overcome this limitation, it is necessary to use a properly entangled state, which is usually prepared in a dedicated procedure. We show that quantum correlations arising from the indistinguishability of bosons are a sufficient resource for the sub-shot-noise interferometry. To this end, we consider an interferometer, which operates on two independently prepared Bose-Einstein condensates with fluctuating numbers of particles. We calculate the sensitivity obtained from the measurement of the number of atoms and compare it with the ultimate achievable bound. Our main conclusion is that even in the presence of major atom number fluctuations, an interferometer operating on two independently prepared condensates can give very high precision. These observations indicate a new possibility for an interferometer operating below the shot-noise limit.
We discuss practical schemes for using entangled Bose-Einstein condensates to detect phase shifts with a resolution better than the shot-noise limit. We begin by outlining a procedure for demonstrating how squeezed matter waves can be used to make measurements by simply lowering and raising a potential barrier between two condensates. The phase shift is read out by a scheme which involves releasing the condensates and studying the collapses and revivals of the visibility of the observed interference fringes. Finally we show how this scheme could be extended to measurements of other quantities such as gravity. All the steps of this process are attainable with current technology and so may provide a practical route for achieving enhanced resolution measurements with matter waves.