Abstract
Relativistic causality forbids superluminal signaling between distant observers. By exploiting the non-signaling principle, we derive the exact relationship between the chained Clauser–Horne–Shimony–Holt sum of correlations \(\text {CHSH}_K\) and the success probability \(P_K\) associated with Hardy’s ladder test of nonlocality for two qubits and \(K+1\) observables per qubit. Then, by invoking the Tsirelson bound for \(\text {CHSH}_K\), the derived relationship allows us to establish an upper limit on \(P_K\). In addition, we draw the connection between \(\text {CHSH}_K\) and the chained version of the Clauser–Horne (CH) inequality.
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Notes
A few technical lemmas concerning a version of the \(\text {CHSH}_K\) expression (7) have been derived in a series of papers by Colbeck and Renner (see, for instance, Refs. [12–14]). Interestingly, as shown by these authors, the use of a chained Bell inequality allows one to construct a program to rule out a broad class of hidden variable theories.
Incidentally, it is worth pointing out that, in this limit, a direct (“all or nothing”) contradiction between quantum mechanics and local realism emerges in Hardy’s ladder scenario [23].
Note that, from relation (8), the limit \(P_K = 0.5\) can never be surpassed since this would entail that \(\text {CHSH}_K > 2K +2\), which is impossible by the very definition of \(\text {CHSH}_K\).
The IC principle states that communication of m classical bits causes information gain of at most m bits. The NS principle is just IC for \(m=0\).
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The author would like to thank the Associate Editor Michael Frey and two anonymous referees for their comments and suggestions regarding an earlier version of this paper.
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Cereceda, J.L. Chained Clauser–Horne–Shimony–Holt inequality for Hardy’s ladder test of nonlocality. Quantum Inf Process 15, 1779–1792 (2016). https://doi.org/10.1007/s11128-015-1217-4
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DOI: https://doi.org/10.1007/s11128-015-1217-4