On the probabilistic description of a multipartite correlation scenario with arbitrary numbers of settings and outcomes per site
arXiv:0804.2398 · doi:10.1088/1751-8113/41/44/445303
Abstract
We consistently formalize the probabilistic description of multipartite joint measurements performed on systems of any nature. This allows us: (1) to specify in probabilistic terms the difference between nonsignaling, the Einstein- Podolsky-Rosen (EPR) locality and Bell's locality; (2) to introduce the notion of an LHV model for an S_{1}x...xS_{N}-setting N-partite correlation experiment, with outcomes of any spectral type, discrete or continuous, and to prove both general and specific "quantum" statements on an LHV simulation in an arbitrary multipartite case; (3) to classify LHV models for a multipartite quantum state, in particular, to show that any N-partite quantum state, pure or mixed, admits an Sx1x...x1 -setting LHV description; (4) to evaluate a threshold visibility for a noisy bipartite quantum state to admit an S_{1}xS_ {2}-setting LHV description under any generalized quantum measurements of two parties. In a sequel to this paper, we shall introduce a single general representation incorporating in a unique manner all Bell-type inequalities for either joint probabilities or correlation functions that have been introduced or will be introduced in the literature.
26 pages; added section Conclusions and some references for section 3
References in corpus (5)
- Hidden Variables and the Two Theorems of John Bell
- Multipartite Bell-type inequalities for arbitrary numbers of settings and outcomes per site
- "Local Realism", Bell's Theorem and Quantum "Locally Realistic" Inequalities
- Class of bipartite quantum states satisfying the original Bell inequality
- Threshold bounds for noisy bipartite states
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- Positive phase space transformation incompatible with classical physics
- Context-invariant quasi hidden variable (qHV) modelling of all joint von Neumann measurements for an arbitrary Hilbert space
- On the existence of a local quasi hidden variable (LqHV) model for each N-qudit state and the maximal quantum violation of Bell inequalities
- New concise upper bounds on quantum violation of general multipartite Bell inequalities
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- Local hidden variable modelling, classicality, quantum separability, and the original Bell inequality
- Specifying nonlocality of a pure bipartite state and analytical relations between measures for bipartite nonlocality and entanglement
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