Persistence of nonlocality for bipartite quantum spin systems
arXiv:0903.3020 · doi:10.1088/1751-8113/44/31/315305
Abstract
Generic forms of the entangled states of two spin-1 (and spin-3/2) particles, along with the set of appropriate spin observables that together exhibit maximum nonlocality under the Hardy's nonlocality test are given; the maximum nonlocality is shown to be 0.09017. It is conjectured that this result holds good for a system of two spin- particles for all values of . It is also shown that no maximally entangled state of two spin- particles responds to the Hardy's nonlocality test.
Revised version in Revtex format, 20 pages, single column; few small corrections made, two small subsections added, two .eps figures added
References in corpus (4)
- Bell's theorem with and without inequalities for the three-qubit Greenberger-Horne-Zeilinger and W states
- Nonlocality without inequality for almost all two-qubit entangled state based on Cabello's nonlocality argument
- Nonlocality without inequality for spin-s system
- Hardy's Test versus the CHSH Test of Quantum Non-Locality: Fundamental and Practical Aspects
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