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Akbar Fahmi

Publications and source records attributed to Akbar Fahmi.

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Space Isotropy and Homogeneity Principles Determine the Maximum Nonlocality of Nature

One of the fundamental questions in physics concerns the relation between spacetime and quantum entanglement. The spacetime is usually considered as a fixed background physical space, and the quantum entanglement is usually manifested as a ``spooky action at a distance" or the existence of ``nonlocality" in nature. Here, we propose the flat-space isotropy and homogeneity principles as the fundamental criteria for determining the maximum degree of nonlocality of nature. More specifically, we consider abstract and deterministic nonlocal-box models which have stronger correlations than in quantum mechanics, whereas therein instantaneous communication remains impossible. We impose space-symmetry group structures on these models and derive a measure for the degree of space symmetries. Surprisingly, there is a tradeoff or inconsistency between the degree of space symmetries and the degree of nonlocality, where this inconsistency is exactly lifted at the Tsirelson bound, as predicted by quantum physics and also predicted in the experiments. Moreover, we prove this result in the general framework of deterministic nonlocal models and conclude that the probabilistic interpretation of the nonlocal box models is an emergent property of the flat-space symmetries.

quant-ph

Almost-quantum correlations violate the isotropy and homogeneity principles in flat space

One of fascinating phenomena of nature is quantum nonlocality, which is observed upon measurements on spacelike entangled systems. However, there are sets of post-quantum models which have stronger correlations than quantum mechanics, wherein instantaneous communication remains impossible. The set of almost quantum correlations is one of post-quantum models which satisfies all kinematic axioms of standard quantum correlations except one, meanwhile they contain correlations slightly stronger than quantum correlations. There arises the natural question whether there is some fundamental principle of nature which can genuinely characterizes quantum correlations. Here, we provide an answer and close this gap by invoking the isotropy and homogeneity principles of the flat space as a conclusive and distinguishing criterion to rule out the almost-quantum correlations model. In particular, to characterize quantum correlations we impose the isotropy and homogeneity symmetry group structure on the almost quantum correlations model and request that the joint probability distributions corresponding to the Born rule remain invariant. We prove that this condition is sufficient (and necessary) to reduce the almost quantum correlations model to quantum mechanics in both bipartite and multipartite systems.

quant-ph

Simulation of Quantum Correlation Functions is not Sufficient Resource to Describe Quantum Entanglement

The Bell theorem expresses that quantum mechanics is not a local-realistic theory, which is often interpreted as nonlocality of the nature. This result has led to this belief that nonlocality and entanglement are the same resources. However, this belief has been critically challenged in the literature. Here, we reexamine the relation between nonlocality and entanglement in light of the Brassard-Cleve-Tapp (BCT) model, which was originally proposed for simulating quantum correlation of Bell's states by using shared random variables augmented by classical communications. We derive a new criterion for distinguishing quantum mechanics from the BCT model through suggesting an observable event based on the perfect correlations (anti-correlations) relation. In particular, we show that in the BCT model one can obtain equal outputs for two opposite input settings with the nonzero probability 0.284. Hence, in this sense we argue that the BCT model can give rise to an unphysical result. We also show the same problem with a nonlocal version of the BCT model.

quant-ph