Optimal Gaussian squeezed states for atom-interferometry in the presence of phase diffusion
arXiv:1008.4114 · doi:10.1103/PhysRevA.82.043624
Abstract
We optimize the signal-to-noise ratio of a Mach-Zehnder atom interferometer with Gaussian squeezed input states, in the presence interactions. For weak interactions, our results coincide with Phys. Rev. Lett. {\bf 100}, 250406 (2008), with optimal initial number-variance and optimal signal-to-noise ratio for total atom number . As the interaction strength increases past unity, phase-diffusion becomes dominant, leading to a transition in the optimal squeezing from initial number-squeezing to initial {\it phase}-squeezing with and shot-noise scaling. The initial phase-squeezing translates into hold-time number-squeezing, which is less sensitive to interactions than coherent states and improves by a factor of .
8 pages, 6 figures
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- Effect of one-, two-, and three-body atom loss processes on superpositions of phase states in Bose-Josephson junctions
- Information and backaction due to phase contrast imaging measurements of cold atomic gases: beyond Gaussian states
- Squeezing as a resource to counteract phase diffusion in optical phase estimation
- Quantum-limited measurement of magnetic-field gradient with entangled atoms
- Phase noise mitigation by a realistic optical parametric oscillator
- Simple atom interferometer in a double-well potential
- Many-body quantum metrology with scalar bosons in a single potential well
- Robust sub-shot-noise measurement via Rabi-Josephson oscillations in bimodal Bose-Einstein condensates