Device-independent bounds from Cabello's nonlocality argument
arXiv:2103.09919 · doi:10.1103/PhysRevA.103.062219
Abstract
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.
arXiv comment8 pages, 1 figure, title slightly modified, close to published version
References in corpus (26)
- Bell nonlocality
- A convergent hierarchy of semidefinite programs characterizing the set of quantum correlations
- Non-local correlations as an information theoretic resource
- Bounding the set of quantum correlations
- Self-testing of quantum systems: a review
- Bell's theorem with and without inequalities for the three-qubit Greenberger-Horne-Zeilinger and W states
- All Pure Bipartite Entangled States can be Self-Tested
- Classical randomness in quantum measurements
- Geometry of the set of quantum correlations
- Asymptotic violation of Bell inequalities and distillability
- Device-independent bounds for Hardy's experiment
- Degree of Complementarity Determines the Nonlocality in Quantum Mechanics
- Concentration phenomena in the geometry of Bell correlations
- Hardy's nonlocality argument as witness for post-quantum correlation
- Geometry of quantum correlations
- Bound on Hardy's non-locality from the principle of Information Causality
- Geometry of the quantum set on no-signaling faces
- Nonlocality without inequality for almost all two-qubit entangled state based on Cabello's nonlocality argument
- Persistence of nonlocality for bipartite quantum spin systems
- Device and semi-device independent random numbers based on non-inequality paradox
- A unified view on Hardy's paradox and the CHSH inequality
- Necessary and sufficient criterion for extremal quantum correlations in the simplest Bell scenario
- Local randomness in Hardy's correlations: Implications from information causality principle
- Local Orthogonality provides better upper bound for Hardy's nonlocality
- All tight correlation Bell inequalities have quantum violations
- Several foundational and information theoretic implications of Bell's theorem
Cited by in corpus (6)
- Self-testing quantum states via nonmaximal violation in Hardy's test of nonlocality
- Quantum correlations on the no-signaling boundary: self-testing and more
- Self-testing of multiple unsharpness parameters through sequential violations of non-contextual inequality
- Hardy-type paradoxes for an arbitrary symmetric bipartite Bell scenario
- Robust self-testing and certified randomness based on chained Bell inequality
- Bipartite polygon models: entanglement classes and their nonlocal behaviour