2005
DOI: 10.1016/j.physleta.2005.08.003
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Optimal measurements in quantum mechanics

Abstract: Four common optimality criteria for measurements are formulated using relations in the set of observables, and their connections are clarified. As case studies, 1-0 observables, localization observables, and photon counting observables are considered.Comment: minor correction

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Cited by 29 publications
(43 citation statements)
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“…The specifical form of an effect in quantum mechanics is as follows. A generalized observable or positive operator valued measure (POVM) [23][24][25] will be represented by a mapping E : B(R) → B(H) such that…”
Section: A Effectsmentioning
confidence: 99%
“…The specifical form of an effect in quantum mechanics is as follows. A generalized observable or positive operator valued measure (POVM) [23][24][25] will be represented by a mapping E : B(R) → B(H) such that…”
Section: A Effectsmentioning
confidence: 99%
“…Let us first recall, following [2] Definition States ρ and ϕ are distinguished by semispectral measure e if…”
Section: State Distinction and State Determinationmentioning
confidence: 99%
“…Proof On account of [1,2] for spectral measure E, set D E consists only of vector states ϕ such that their density matrices are one-dimensional projections from the range of E. So…”
Section: Theorem 2 If E Is a Spectral Measure With Values In P(h) Anmentioning
confidence: 99%
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