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arXiv:0712.2307 · Physical Review A

Local and nonlocal content of bipartite qubit and qutrit correlations

Valerio Scarani

Published Apr 17, 2008• 42 citations
arXivHTMLPDF

Abstract

The local and nonlocal contents of nonlocal probability distributions are studied using the approach of Elitzur, Popescu, and Rohrlich [A. Elitzur, S. Popescu, and D. Rohrlich, Phys. Lett. A 162, 25 (1992)]. This work focuses on distributions that can be obtained by single-copy von Neumann measurements on bipartite quantum systems. For pure two-qubit states $|\ensuremath{\Psi}(\ensuremath{\theta})⟩=\text{cos}\text{ }\ensuremath{\theta}|00⟩+\text{sin}\text{ }\ensuremath{\theta}|11⟩$ (with $\text{cos}\text{ }\ensuremath{\theta}\ensuremath{\ge}\text{sin}\text{ }\ensuremath{\theta}$), the local content of the corresponding probability distribution is found to lie between $1\ensuremath{-}\text{sin}\text{ }2\ensuremath{\theta}$ and $\text{cos}\text{ }2\ensuremath{\theta}$. For the family $|\ensuremath{\Psi}(\ensuremath{\gamma})⟩=(|00⟩+|11⟩+\ensuremath{\gamma}|22⟩)/\sqrt{2+{\ensuremath{\gamma}}^{2}}$ of two-qutrit states, nonzero local content is found for $\ensuremath{\gamma}>2$.

DOI
10.1103/physreva.77.042112

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The local and nonlocal contents of nonlocal probability distributions are studied using the approach of Elitzur, Popescu, and Rohrlich [A. Elitzur, S. Popescu, and D. Rohrlich, Phys. Lett. A 162, 25 (1992)]. This work focuses on distributions that can be obtained by single-copy von Neumann measurements on bipartite quantum systems. For pure two-qubit states ∣\ensuremathΨ(\ensuremathθ)⟩=cos \ensuremathθ∣00⟩+sin \ensuremathθ∣11⟩|\ensuremath{\Psi}(\ensuremath{\theta})⟩=\text{cos}\text{ }\ensuremath{\theta}|00⟩+\text{sin}\text{ }\ensuremath{\theta}|11⟩∣\ensuremathΨ(\ensuremathθ)⟩=cos \ensuremathθ∣00⟩+sin \ensuremathθ∣11⟩ (with cos \ensuremathθ\ensuremath≥sin \ensuremathθ\text{cos}\text{ }\ensuremath{\theta}\ensuremath{\ge}\text{sin}\text{ }\ensuremath{\theta}cos \ensuremathθ\ensuremath≥sin \ensuremathθ), the local content of the corresponding probability distribution is found to lie between 1\ensuremath−sin 2\ensuremathθ1\ensuremath{-}\text{sin}\text{ }2\ensuremath{\theta}1\ensuremath−sin 2\ensuremathθ and cos 2\ensuremathθ\text{cos}\text{ }2\ensuremath{\theta}cos 2\ensuremathθ. For the family ∣\ensuremathΨ(\ensuremathγ)⟩=(∣00⟩+∣11⟩+\ensuremathγ∣22⟩)/2+\ensuremathγ2|\ensuremath{\Psi}(\ensuremath{\gamma})⟩=(|00⟩+|11⟩+\ensuremath{\gamma}|22⟩)/\sqrt{2+{\ensuremath{\gamma}}^{2}}∣\ensuremathΨ(\ensuremathγ)⟩=(∣00⟩+∣11⟩+\ensuremathγ∣22⟩)/2+\ensuremathγ2​ of two-qutrit states, nonzero local content is found for \ensuremathγ>2\ensuremath{\gamma}>2\ensuremathγ>2.
One of the last open problems concerning two qubits in a pure state is to find the exact local content of their correlation, in the sense of Elitzur, Popescu, and Rohrlich (EPR2) [A. C. Elitzur, S. Popescu, and D. Rohrlich, Phys. Lett. A162, 25 (1992)]. We propose an EPR2 decomposition that allows us to prove, for a wide range of states $|\ensuremath{\psi}(\ensuremath{\theta})\ensuremath{\rangle}=\mathrm{cos}\ensuremath{\theta}|00\ensuremath{\rangle}+\mathrm{sin}\ensuremath{\theta}|11\ensuremath{\rangle}$, that their local content is $\overline{{p}_{L}}(\ensuremath{\theta})=\mathrm{cos}2\ensuremath{\theta}$. We also share reflections on how to possibly extend this result to all two-qubit pure states.
The machinery of qubit-portraits of qudit states, recently presented, is consider here in more details in order to characterize the presence of quantum correlations in bipartite qudit states. In the tomographic representation of quantum mechanics, Bell-like inequalities are interpreted as peculiar properties of a family of classical joint probability distributions which describe the quantum state of two qudits. By means of the qubit-portraits machinery a semigroup of stochastic matrices can be associated to a given quantum state. The violation of the CHSH inequalities is discussed in this framework with some examples, we found that quantum correlations in qutrit isotropic states can be detected by the suggested method while it cannot in the case of qutrit Werner states.
The machinery of qubit-portraits of qudit states, recently presented, is consider here in more details in order to characterize the presence of quantum correlations in bipartite qudit states. In the tomographic representation of quantum mechanics, Bell-like inequalities are interpreted as peculiar properties of a family of classical joint probability distributions which describe the quantum state of two qudits. By means of the qubit-portraits machinery a semigroup of stochastic matrices can be associated to a given quantum state. The violation of the CHSH inequalities is discussed in this framework with some examples, we found that quantum correlations in qutrit isotropic states can be detected by the suggested method while it cannot in the case of qutrit Werner states.
In Phys. Lett. A 166, 293 (1992), Popescu and Rohrlich characterized nonlocality of pure nnn-partite entangled systems by studying bipartite violation of local realism when $n\ensuremath{-}2$ number of parties perform projective measurements on their particles. A pertinent question in this scenario is whether similar characterization is possible for nnn-partite mixed entangled states also. In the present work we have followed an analogous approach so as to explore whether given a tripartite mixed entangled state the conditional bipartite states obtained by performing projective measurement on the third party demonstrate a weaker form of nonlocality, quantum steering. We also compare this phenomenon of conditional steering with existing notions of tripartite correlations.
Abstract The observables of a bipartite quantum system are represented by the set of all self adjoint operators on the tensor product of two Hilbert spaces H1 ® ‘H2, whose dimensions we shall denote by d1 and d2, taking d1 :S: d2 without loss of generality. It is well known that when d1 2: 2 the states of the system can be nonseparable, and it is this possibility that much of the new technology associated with quantum information and computation theory relies upon. Prompted by concerns about whether the very noisy mixed states exploited by certain models of NMR quantum computing are truly nonseparable (Braunstein et al. 1999, Linden & Popescu 2001), de­ tailed investigations have shown that, whenever d2 < oo, there is always an open neighborhood of separable states surrounding the maximally mixed state (d1d2)­1 I® I (Zyczkowski et al. 1998, Caves