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Squeezing of nonlinear spin observables by one axis twisting in the presence of decoherence: An analytical study
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In an ensemble of two-level atoms that can be described in terms of a collective spin, entangled states can be used to enhance the sensitivity of interferometric precision measurements. While non-Gaussian spin states can produce larger quantum enhancements than spin-squeezed Gaussian states, their use requires the measurement of observables that are nonlinear functions of the three components of the collective spin. In this paper we develop strategies that achieve the optimal quantum enhancements using non-Gaussian states produced by a nonlinear one-axis-twisting Hamiltonian, and show that measurement-after-interaction techniques, known to amplify the output signals in quantum parameter estimation protocols, are effective in measuring nonlinear spin observables. Including the presence of the relevant decoherence processes from atomic experiments, we determine analytically the quantum enhancement of non-Gaussian over-squeezed states as a function of the noise parameters for arbitrary atom numbers.
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Cited by 1 Pith paper
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From dynamical to steady-state many-body metrology: Precision limits and their attainability with two-body interactions
Many-body interactions drive a product-state spin probe to Heisenberg-limited sensitivity, and explicit two-body Hamiltonians can saturate the corresponding steady-state bounds.
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