2004
DOI: 10.1088/1464-4266/6/6/005
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Informationally complete measurements and group representation

Abstract: Abstract. Informationally complete measurements on a quantum system allow to estimate the expectation value of any arbitrary operator by just averaging functions of the experimental outcomes. We show that such kind of measurements can be achieved through positive-operator valued measures (POVM's) related to unitary irreducible representations of a group on the Hilbert space of the system. With the help of frame theory we provide a constructive way to evaluate the data-processing function for arbitrary operator… Show more

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Cited by 106 publications
(110 citation statements)
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“…(6)(7)(8) and (13) that, if |ψ = d−1 r=0 ψ r |e r is a GP fiducial vector, then so is the vector |ψ * = d−1 r=0 ψ * r |e r obtained by complex conjugation. So to make the analysis complete we need to consider automorphisms of GP(d) which are generated by anti-unitary operators.…”
Section: The Extended Clifford Groupmentioning
confidence: 99%
See 1 more Smart Citation
“…(6)(7)(8) and (13) that, if |ψ = d−1 r=0 ψ r |e r is a GP fiducial vector, then so is the vector |ψ * = d−1 r=0 ψ * r |e r obtained by complex conjugation. So to make the analysis complete we need to consider automorphisms of GP(d) which are generated by anti-unitary operators.…”
Section: The Extended Clifford Groupmentioning
confidence: 99%
“…The concept of informational completeness is originally due to Prugovečki [5] (also see Busch [6], Busch et al [2], d'Ariano et al [7], Flammia et al [8], Finkelstein [9], and references cited therein). It has an obvious relevance to the problem of quantum state determination.…”
Section: Introductionmentioning
confidence: 99%
“…(17) in this case can be detected by measuring d 2 − 1 observables via a local setting and classical processing of the measurement outcomes. Actually, a set of generalised Bell projectors can be written as follows [11] …”
mentioning
confidence: 99%
“…We exploit the existence, proved in Ref. [28] for every dimension of the Hilbert space, of (rank-one) informationally complete measurements, that are POVMs whose elements form a basis for the operator space. In other words, there always exists a POVM {P i } i such that Tr[XP i ] = 0 for all i if and only if X = 0.…”
Section: Entanglement Of Formation and Approximate Channel Correctionmentioning
confidence: 99%