2013
DOI: 10.48550/arxiv.1306.5211
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Contradictory entropic joint uncertainty relations for complementary observables in two-level systems

Abstract: We show that different entropic measures of fluctuations lead to contradictory uncertainty relations for two complementary observables. We apply Tsallis and Rényi entropies to the joint distribution emerging from a noisy simultaneous measurement of both observables as well as to the product of their individual statistics, either intrinsic or of operational origin.

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Cited by 3 publications
(3 citation statements)
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“…Entropic bounds in terms of generalized entropies entropic bounds were utilized in studying many topics such as the case of conjugate observables [48,49], quantifying number-phase uncertainties [50,51], incompatibilities of anti-commuting observables [52] and reformulations in quasi-Hermitian models [53]. In the context of simultaneous measurements of complementary observables, uncertainty relations in terms of both the Tsallis and Rényi entropies are examined in [54]. The method of Maassen and Uffink uses the Riesz theorem.…”
Section: Uncertainty Relations Of the Maassen-uffink Typementioning
confidence: 99%
“…Entropic bounds in terms of generalized entropies entropic bounds were utilized in studying many topics such as the case of conjugate observables [48,49], quantifying number-phase uncertainties [50,51], incompatibilities of anti-commuting observables [52] and reformulations in quasi-Hermitian models [53]. In the context of simultaneous measurements of complementary observables, uncertainty relations in terms of both the Tsallis and Rényi entropies are examined in [54]. The method of Maassen and Uffink uses the Riesz theorem.…”
Section: Uncertainty Relations Of the Maassen-uffink Typementioning
confidence: 99%
“…The added noise is minimum in the sense that the Euclidean distance between p Z and the marginal probability pZ (defined in Eq. ( 7) below) is minimum [26]. It is worth noting that there is a deep connection of this measurement with the problem of state discrimination between two nonorthogonal states, such as |a ± (see e.g.…”
Section: Statistics and Simultaneous Measurementsmentioning
confidence: 96%
“…As shown in appendix A of Ref. [43], the optimum choice holds for 2ϑ − θ = π/2. To gain insight, and without loss of generality, we can consider such a case.…”
Section: Joint Observation and Inversionmentioning
confidence: 99%