Abstract

In a recent work, it was shown by one of us (EGC) that Bell-Kochen-Specker inequality violations in phenomena satisfying the no-disturbance condition (a generalisation of the no-signalling condition) cannot in general be explained with a faithful classical causal model---that is, a classical causal model that satisfies the assumption of no fine-tuning. The proof of that claim however was restricted to Bell scenarios involving 2 parties or Kochen-Specker-contextuality scenarios involving 2 measurements per context. Here we show that the result holds in the general case of arbitrary numbers of parties or measurements per context; it is not an artefact of the simplest scenarios. This result unifies, in full generality, Bell nonlocality and Kochen-Specker contextuality as violations of a fundamental principle of classical causality. We identify, however, an implicit assumption in the former proof, making it explicit here: that certain operational symmetries of the phenomenon are reflected in the model, rather than requiring fine-tuned choices of model parameters. This clarifies a subtle but important distinction between Bell nonlocality and Kochen-Specker contextuality.

Highlights

  • Bell nonlocality [1] and Kochen-Specker (KS) contextuality [2] are classically forbidden correlations characteristic of quantum phenomena

  • Bell nonlocality is a key resource for quantum communication, with applications such as reducing communication complexity [5] and secure communication [6]

  • Since classical simulation of Bell correlations is possible via the addition of communication channels between the parties in the Bell test [7, 8], quantum over classical advantages provided by Bell nonlocality can be understood as quantum protocols having access to correlations that can only be simulated classically with the aid of extra resources

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Summary

Introduction

Bell nonlocality [1] and Kochen-Specker (KS) contextuality [2] are classically forbidden correlations characteristic of quantum phenomena. Considering a classical causal model to be (essentially) a classical simulation of a quantum phenomenon, this provides a novel approach to understanding the quantum over classical advantage provided by Bell-KS correlations: fine-tuning can be considered an unavoidable resource waste in any classical simulation, relative to the quantum realisation of the same correlations. We generalise the framework of [15] to arbitrary numbers of parties or measurements per context, demonstrating in full generality the need for fine-tuning in classical causal models for Bell-KS inequality violations. That definition did not account for the possibility that the same measurement could have different statistics depending on which random variable in a causal model it is associated with, which would represent a form of contextuality not ruled out by the notion of no fine-tuning used in that work.

Causal models
Main result
Example scenario based on the Peres-Mermin square
Proof of Theorem 1
Findings
Conclusion
Full Text
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