2004
DOI: 10.1214/009053604000000436
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Maximum Fisher information in mixed state quantum systems

Abstract: We deal with the maximization of classical Fisher information in a quantum system depending on an unknown parameter. This problem has been raised by physicists, who defined [Helstrom (1967) Phys. Lett. A 25 101-102] a quantum counterpart of classical Fisher information, which has been found to constitute an upper bound for classical information itself [Braunstein and Caves (1994) Phys. Rev. Lett. 72 3439-3443]. It has then become of relevant interest among statisticians, who investigated the relations between … Show more

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Cited by 31 publications
(30 citation statements)
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References 7 publications
(16 reference statements)
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“…(16) are usually expressed in terms of the eigen decomposition of L ξ . A complete POVM {M x ,x ∈ X } with general significance known [4,5,10] to satisfy Eq. (16) is the von Neumann measurement made by the rank-one projectors on the eigenstates of L ξ .…”
Section: A Optimal Performance In Estimationmentioning
confidence: 99%
“…(16) are usually expressed in terms of the eigen decomposition of L ξ . A complete POVM {M x ,x ∈ X } with general significance known [4,5,10] to satisfy Eq. (16) is the von Neumann measurement made by the rank-one projectors on the eigenstates of L ξ .…”
Section: A Optimal Performance In Estimationmentioning
confidence: 99%
“…Recall, that for a single parameter the bound by the classical Fisher information matrix could be saturated by an appropriately chosen POVM, (54). This is no longer the case for the the estimation of multiple parameters [14,15]. That is, the final lower bound in (57) can not be obtained.…”
Section: The χ 2 -Test and Its Connection To Quantum Parameter Esmentioning
confidence: 97%
“…For quantum systems with a bidimensional Hilbert space, as those we are investigating in this paper, the optimal measurement is a projective one [49,50]. Besides, using Eqs.…”
Section: The Physical Modelmentioning
confidence: 99%