Detailed Information on Publication Record
2021
Device-independent bounds from Cabello's nonlocality argument
RAI, A., Matej PIVOLUSKA, Martin PLESCH, S. SASMAL, M. BANIK et. al.Basic information
Original name
Device-independent bounds from Cabello's nonlocality argument
Authors
RAI, A., Matej PIVOLUSKA (703 Slovakia, belonging to the institution), Martin PLESCH (703 Slovakia, belonging to the institution), S. SASMAL, M. BANIK and S. GHOSH
Edition
Physical review A, New York, The American Physical Society, 2021, 2469-9926
Other information
Language
English
Type of outcome
Článek v odborném periodiku
Field of Study
10201 Computer sciences, information science, bioinformatics
Country of publisher
United States of America
Confidentiality degree
není předmětem státního či obchodního tajemství
References:
Impact factor
Impact factor: 2.971
RIV identification code
RIV/00216224:14610/21:00121949
Organization unit
Institute of Computer Science
UT WoS
000665117900001
Keywords (in Czech)
non-locality; entanglement
Keywords in English
non-locality; entanglement
Tags
International impact, Reviewed
Změněno: 6/5/2022 11:51, RNDr. Matej Pivoluska, Ph.D.
Abstract
V originále
Hardy-type arguments manifest Bell nonlocality in one of the simplest possible ways. Except for demonstrating nonclassical signature of entangled states in question, they can also serve for device-independent self-testing of states, as shown, e.g., in Phys. Rev. Lett. 109, 180401 (2012). Here we develop and broaden these results to an extended version of Hardy's argument, often referred to as Cabello's nonlocality argument. We show that, as in the simpler case of Hardy's nonlocality argument, the maximum quantum value for Cabello's nonlocality is achieved by a pure two-qubit state and projective measurements that are unique up to local isometries. We also examine the properties of a more realistic case when small errors in the ideal constraints are accepted within the probabilities obtained and prove that also in this case the two-qubit state and measurements are sufficient for obtaining the maximum quantum violation of the classical bound.
Links
MUNI/G/1596/2019, interní kód MU |
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