TL;DR
This paper explores the structure of non-signaling theories, especially the two non-signaling boxes model, comparing it with quantum and classical theories, and investigates its implications for quantum logic and information theory.
Contribution
It reconstructs the probability theory for non-signaling boxes and analyzes their differences from quantum and classical probabilities, highlighting unique features and limitations.
Findings
Non-signaling boxes violate quantum bounds like CHSH but respect relativistic causality.
Measurements in non-signaling theories are necessarily destructive.
The subset of classically correlated states does not reproduce classical physics.
Abstract
We analyze the structure of the so called non-signaling theories respecting relativistic causality but allowing correlations violating bounds imposed by quantum mechanics such as CHSH inequality. We discuss relations among such theories, quantum mechanics, and classical physics. In particular we reconstruct the probability theory adequate for the simplest instance of a non-signaling theory, the two non-signaling boxes world, and exhibit its differences in comparison with classical and quantum probabilities. We show that the question whether such a theory can be treated as a kind of "generalization" of the quantum theory of the two-qubit system cannot be answered positively. Some of its features put it closer to the quantum world, for example measurements must be destructive, on the other hand the Heisenberg uncertainty relations are not satisfied. Another interesting property…
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