2018
DOI: 10.1364/oe.26.016292
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Maximal quantum Fisher information for phase estimation without initial parity

Abstract: Mach-Zehnder interferometer is a common device in quantum phase estimation and the photon losses in it are an important issue for achieving a high phase accuracy. Here we thoroughly discuss the precision limit of the phase in the Mach-Zehnder interferometer with a coherent state and a superposition of coherent states as input states. By providing a general analytical expression of quantum Fisher information, the phase-matching condition and optimal initial parity are given. Especially, in the photon loss scena… Show more

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Cited by 31 publications
(14 citation statements)
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“…the QFI for arbitrary Fock states into a single MZI, which matches known results from similar scenarios [28,29]. Note that the QFI for all multimode interferometers we consider are summarised in Table I.…”
Section: The Separable Interferometer a General Fisher Informationsupporting
confidence: 77%
“…the QFI for arbitrary Fock states into a single MZI, which matches known results from similar scenarios [28,29]. Note that the QFI for all multimode interferometers we consider are summarised in Table I.…”
Section: The Separable Interferometer a General Fisher Informationsupporting
confidence: 77%
“…|ψ in . This is especially advantageous in the balanced case (ϑ = ϑ ′ = π/2) because the output state can be simply written as [27,38,39]…”
Section: The Quantum Optical Description Of An Unbalanced Mzimentioning
confidence: 99%
“…Other authors, though, consider the full interferometer (see Fig. 1), some in the case of the classical Fisher information [12] (see also the supplementary material of [10]), but mostly in the case of QFI [27,38,39]. Indeed, in the balanced case, starting from equation (8) and due to the exponential form of the generator (i. e. Ûϕ = e iϕ Ĝ, see reference [18]) the QFI is simply [27,38,39,50,52]…”
Section: Appendix B: Shorthand Notationsmentioning
confidence: 99%
“…This space can be further reduced when additional restrictions are invoked. For example, if the probe state in one import is restricted to be an odd or even state, then the maximal QFI can be achieved when the states of the two modes satisfy the phase-matching condition [89], which forms a basis for the state optimization in the MZI [89][90][91]. In practice, the phase of the input states require extra resources to identify, such as an external phase reference.…”
Section: A Analytical Optimizationmentioning
confidence: 99%