6,240 research outputs found

    Proposal for revealing quantum nonlocality via local contextuality

    Full text link
    Two distant systems can exhibit quantum nonlocality even though the correlations between them admit a local model. This nonlocality can be revealed by testing extra correlations between successive measurements on one of the systems which do not admit a noncontextual model whatever the reduced state of this system is. This shows that quantum contextuality plays a fundamental role in quantum nonlocality, and allows an experimental test of the Kochen-Specker with locality theorem.Comment: REVTeX4-1, 4 pages, 1 figur

    Quantum correlations are not contained in the initial state

    Get PDF
    Two proofs are presented which show that quantum mechanics is incompatible with the following assumption: all possible correlations between subsystems of an individual isolated composite quantum system are contained in the initial quantum state of the whole system, although just a subset of them is revealed by the actual experiment.Comment: REVTeX, 4 pages, 1 figur

    Bosonic bunching does not reveal stronger quantum contextuality

    Full text link
    In a recent paper, Kurzynski et al. present a gedanken experiment that, they claim, violates the Klyachko-Can-Binicioglu-Shumovsky (KCBS) noncontextuality (NC) inequality beyond its maximum quantum value, and a similar experiment that, they claim, violates Specker's NC inequality, which is not violated by quantum mechanics. We argue that these claims are baseless, since these experiments do not satisfy the conditions required for any observation of contextuality through the experimental violation of a NC inequality. Moreover, the physical events in the experiments of Kurzynski et al. do not have the relationships of exclusivity which the authors assume they have.Comment: REVTeX4, 3 page

    Minimal proofs of state-independent contextuality

    Full text link
    It has been recently shown that state-independent contextuality (SIC) is a fundamental resource linked with a type of nonlocality which cannot be improved by nonsignaling resources. Therefore, it is of fundamental importance to identify the simplest sets of quantum observables needed to prove SIC. We show that d+10 rank-1 projectors are sufficient to prove SIC for any physical system in dimension d>2. This result outperforms both the best Kochen-Specker proofs and the results presented by Yu and Oh in arXiv:1112.5513v1.Comment: REVTeX4, 2 page

    Quantum key distribution in the Holevo limit

    Get PDF
    A theorem by Shannon and the Holevo theorem impose that the efficiency of any protocol for quantum key distribution, E\cal E, defined as the number of secret (i.e., allowing eavesdropping detection) bits per transmitted bit plus qubit, is E≤1{\cal E} \le 1. The problem addressed here is whether the limit E=1{\cal E} =1 can be achieved. It is showed that it can be done by splitting the secret bits between several qubits and forcing Eve to have only a sequential access to the qubits, as proposed by Goldenberg and Vaidman. A protocol with E=1{\cal E} =1 based on polarized photons and in which Bob's state discrimination can be implemented with linear optical elements is presented.Comment: REVTeX, 4 pages, 2 figure

    Comment on "Non-contextual hidden variables and physical measurements"

    Get PDF
    Kent's conclusion that ``non-contextual hidden variable theories cannot be excluded by theoretical arguments of the Kochen-Specker type once the imprecision in real world experiments is taken into account'' [Phys. Rev. Lett. 83, 3755 (1999)], is criticized. The Kochen-Specker theorem just points out that it is impossible even conceive a hidden variable model in which the outcomes of all measurements are pre-determined; it does not matter if these measurements are performed or not, or even if these measurements can be achieved only with finite precision.Comment: 2 page

    Exclusivity principle and the quantum bound of the Bell inequality

    Full text link
    We show that, for general probabilistic theories admitting sharp measurements, the exclusivity principle together with two assumptions exactly singles out the Tsirelson bound of the Clauser-Horne-Shimony-Holt Bell inequality.Comment: REVTeX4, 4 pages, 1 figur

    Specker's fundamental principle of quantum mechanics

    Full text link
    I draw attention to the fact that three recently proposed physical principles, namely "local orthogonality", "global exclusive disjunction", and "compatible orthogonality" are not new principles, but different versions of a principle that Ernst Specker noticed long ago. I include a video of Specker stating this principle in 2009 in the following terms: "Do you know what, according to me, is the fundamental theorem of quantum mechanics? (...) That is, if you have several questions and you can answer any two of them, then you can also answer all of them". I overview some results that suggest that Specker's principle may be of fundamental importance for explaining quantum contextuality. Specker passed away in December 10, 2011, at the age of 91.Comment: REVTeX4, 4 pages, 1 figure, 1 vide

    Proposed experiment to exclude higher-than-quantum violations of the Bell inequality

    Full text link
    We show that a recent observation by Yan leads to a method to experimentally test whether a higher-than-quantum violation of the Clauser-Horne-Shimony-Holt Bell inequality is possible (assuming that the sum of probabilities of pairwise exclusive propositions cannot exceed 1). The test requires reaching the maximum quantum violation of a noncontextuality inequality involving sequences of three compatible measurements on a five-dimensional quantum system.Comment: REVTeX4, 4 pages, 1 figur

    Simple explanation of the quantum violation of a fundamental inequality

    Full text link
    We show that the maximum quantum violation of the Klyachko-Can-Binicioglu-Shumovsky (KCBS) inequality is exactly the maximum value satisfying the following principle: The sum of probabilities of pairwise exclusive events cannot exceed 1. We call this principle "global exclusivity," since its power shows up when it is applied to global events resulting from enlarged scenarios in which the events in the inequality are considered jointly with other events. We identify scenarios in which this principle singles out quantum contextuality, and show that a recent proof excluding nonlocal boxes follows from the maximum violation imposed by this principle to the KCBS inequality.Comment: REVTeX4, 6 pages, 3 figure
    • …
    corecore