2018
DOI: 10.1103/physrevlett.121.230801
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Quantum-Limited Loss Sensing: Multiparameter Estimation and Bures Distance between Loss Channels

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Cited by 59 publications
(70 citation statements)
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“…The attention has been triggered because the key mechanism leading to quantum enhancement can often be understood as the non-classicality of the probe state [1,5,6]. For example, in single-mode loss parameter estimation, the photon number state having no uncertainty in the intensity is known to be the optimal state, providing the maximal quantum enhancement [7,8]. In phase parameter estimation, it is known that the squeezed vacuum state reaches the QFI scaled with N 2 [9], leading to a Heisenberg scaling of -N 1 in precision, where N is the average photon number of the probe state.…”
Section: Introductionmentioning
confidence: 99%
“…The attention has been triggered because the key mechanism leading to quantum enhancement can often be understood as the non-classicality of the probe state [1,5,6]. For example, in single-mode loss parameter estimation, the photon number state having no uncertainty in the intensity is known to be the optimal state, providing the maximal quantum enhancement [7,8]. In phase parameter estimation, it is known that the squeezed vacuum state reaches the QFI scaled with N 2 [9], leading to a Heisenberg scaling of -N 1 in precision, where N is the average photon number of the probe state.…”
Section: Introductionmentioning
confidence: 99%
“…The last assertion of Theorem 1 implies the following 12 Since the operator V satisfies condition (18), the r.h.s. of (30) tends to zero as n → +∞.…”
Section: The Main Resultsmentioning
confidence: 68%
“…emphasise that this operator is defined by formula (21) not assuming existence of densely defined adjoint operator V * Φ . 14 Estimations of this distance for real quantum channels can be found in [12]. Lemma 5.…”
Section: The Main Resultsmentioning
confidence: 99%
“…We first show that the fidelity between the ideal displacement and its experimental approximation when acting on a fixed input state is equal to the fidelity between a pure-loss channel and an ideal channel when acting on the same input state. We then provide an analytical expression to upper bound the Shirokov-Winter energy-constrained diamond distance between an ideal displacement and its experimental approximations, by using the recent result of [Nai18]. Furthermore, we study different performance metrics to analyze how well an experimental approximation simulates a tensor product of different displacement operators.…”
Section: Introductionmentioning
confidence: 99%