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Characterization of the nonclassical relation between measurement outcomes represented by nonorthogonal quantum states

Ming Ji and Holger F. Hofmann
Phys. Rev. A 107, 022208 – Published 9 February 2023

Abstract

Quantum mechanics describes seemingly paradoxical relations between the outcomes of measurements that cannot be performed jointly. In Hilbert space, the outcomes of such incompatible measurements are represented by nonorthogonal states. In this paper we investigate how the relation between outcomes represented by nonorthogonal quantum states differs from the relations suggested by a joint assignment of measurement outcomes that do not depend on the actual measurement context. The analysis is based on a well-known scenario where three statements about the impossibilities of certain outcomes would seem to make a specific fourth outcome impossible as well, yet quantum theory allows the observation of that outcome with a nonvanishing probability. We show that the Hilbert space formalism modifies the relation between the four measurement outcomes by defining a lower bound of the fourth probability that increases as the total probability of the first three outcomes drops to zero. Quantum theory thus not only makes the violation of noncontextual consistency between the measurement outcomes possible, but actually requires it as a necessary consequence of the Hilbert space inner products that describe the contextual relation between the outcomes of different measurements.

  • Figure
  • Received 3 November 2022
  • Accepted 31 January 2023

DOI:https://doi.org/10.1103/PhysRevA.107.022208

©2023 American Physical Society

Physics Subject Headings (PhySH)

General PhysicsQuantum Information, Science & TechnologyAtomic, Molecular & Optical

Authors & Affiliations

Ming Ji and Holger F. Hofmann*

  • Graduate School of Advanced Science and Engineering, Hiroshima University, Kagamiyama 1-3-1, Higashi Hiroshima 739-8530, Japan

  • *hofmann@hiroshima-u.ac.jp

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Issue

Vol. 107, Iss. 2 — February 2023

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Images

  • Figure 1
    Figure 1

    Illustration of the lower bound of PWW(a,a) given by Eq. (24). Quantum mechanics defines a forbidden region around the noncontextual expectation that PS=0 requires PWW(a,a)=0. The dashed line shows the value of the critical probability sum Pcr=0.0243 below which quantum mechanics requires a violation of the inequality given in Eq. (1).

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