Characterization of informational completeness for covariant phase space observables

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OriginalspracheEnglisch
Seiten (von - bis)102103
Seitenumfang1
FachzeitschriftJ. Math. Phys.
Jahrgang53
PublikationsstatusVeröffentlicht - 2012

Abstract

A covariant phase space observable is uniquely characterized by a positive operator of trace one and, in turn, by the Fourier-Weyl transform of this operator. We study three properties of such observables, and characterize them in terms of the zero set of this transform. The first is informational completeness, for which it is necessary and sufficient that the zero set has dense complement. The second is a version of informational completeness for the Hilbert-Schmidt class, equivalent to the zero set being of measure zero, and the third, known as regularity, is equivalent to the zero set being empty. We give examples demonstrating that all three conditions are distinct. The three conditions are the special cases for $p=1,2, of a more general notion of $p$-regularity defined as the norm density of the span of translates of the operator in the Schatten-$p$ class. We show that the relation between zero sets and $p$-regularity can be mapped completely to the corresponding relation for functions in classical harmonic analysis.

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Characterization of informational completeness for covariant phase space observables. / Kiukas, Jukka; Lahti, Pekka; Schultz, Jussi et al.
in: J. Math. Phys., Jahrgang 53, 2012, S. 102103.

Publikation: Beitrag in FachzeitschriftArtikelForschungPeer-Review

Kiukas, Jukka ; Lahti, Pekka ; Schultz, Jussi et al. / Characterization of informational completeness for covariant phase space observables. in: J. Math. Phys. 2012 ; Jahrgang 53. S. 102103.
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T1 - Characterization of informational completeness for covariant phase space observables

AU - Kiukas, Jukka

AU - Lahti, Pekka

AU - Schultz, Jussi

AU - Werner, Reinhard F.

N1 - Funding information: This work was partially supported by the Academy of Finland Grant No. 138135. J.S. was supported by the Finnish Cultural Foundation. J.K. was supported by Emil Aaltonen Foundation.

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N2 - A covariant phase space observable is uniquely characterized by a positive operator of trace one and, in turn, by the Fourier-Weyl transform of this operator. We study three properties of such observables, and characterize them in terms of the zero set of this transform. The first is informational completeness, for which it is necessary and sufficient that the zero set has dense complement. The second is a version of informational completeness for the Hilbert-Schmidt class, equivalent to the zero set being of measure zero, and the third, known as regularity, is equivalent to the zero set being empty. We give examples demonstrating that all three conditions are distinct. The three conditions are the special cases for $p=1,2, of a more general notion of $p$-regularity defined as the norm density of the span of translates of the operator in the Schatten-$p$ class. We show that the relation between zero sets and $p$-regularity can be mapped completely to the corresponding relation for functions in classical harmonic analysis.

AB - A covariant phase space observable is uniquely characterized by a positive operator of trace one and, in turn, by the Fourier-Weyl transform of this operator. We study three properties of such observables, and characterize them in terms of the zero set of this transform. The first is informational completeness, for which it is necessary and sufficient that the zero set has dense complement. The second is a version of informational completeness for the Hilbert-Schmidt class, equivalent to the zero set being of measure zero, and the third, known as regularity, is equivalent to the zero set being empty. We give examples demonstrating that all three conditions are distinct. The three conditions are the special cases for $p=1,2, of a more general notion of $p$-regularity defined as the norm density of the span of translates of the operator in the Schatten-$p$ class. We show that the relation between zero sets and $p$-regularity can be mapped completely to the corresponding relation for functions in classical harmonic analysis.

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