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arxiv: 1609.06114 · v4 · pith:5Q343I33new · submitted 2016-09-20 · 🪐 quant-ph · math-ph· math.FA· math.MP

Better local hidden variable models for two-qubit Werner states and an upper bound on the Grothendieck constant K_G(3)

classification 🪐 quant-ph math-phmath.FAmath.MP
keywords grothendiecklocalsimeqstatewernerarbitraryboundconstant
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We consider the problem of reproducing the correlations obtained by arbitrary local projective measurements on the two-qubit Werner state $\rho = v |\psi_- > <\psi_- | + (1- v ) \frac{1}{4}$ via a local hidden variable (LHV) model, where $|\psi_- >$ denotes the singlet state. We show analytically that these correlations are local for $ v = 999\times689\times{10^{-6}}$ $\cos^4(\pi/50) \simeq 0.6829$. In turn, as this problem is closely related to a purely mathematical one formulated by Grothendieck, our result implies a new bound on the Grothendieck constant $K_G(3) \leq 1/v \simeq 1.4644$. We also present a LHV model for reproducing the statistics of arbitrary POVMs on the Werner state for $v \simeq 0.4553$. The techniques we develop can be adapted to construct LHV models for other entangled states, as well as bounding other Grothendieck constants.

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  1. Can outcome communication explain Bell nonlocality?

    quant-ph 2025-10 unverdicted novelty 7.0

    For any qubit-qudit state under all projective measurements, an LHV model with outcome communication exists if and only if a standard LHV model without communication exists.