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Lecture notes in physics

The Emergence of Classical Physics

Τ. Padmanabhan

Published Jan 1, 2015• 0 citations
Publisher
DOI
10.1007/978-3-319-13443-7_2

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The problem of emergence in physical theories makes necessary to build a general theory of the relationships between the observed system and the observing system. It can be shown that there exists a correspondence between classical systems and computational dynamics according to the Shannon-Turing model. A classical system is an informational closed system with respect to the observer; this characterizes the emergent processes in classical physics as phenomenological emergence. In quantum systems, the analysis based on the computation theory fails. It is here shown that a quantum system is an informational open system with respect to the observer and able to exhibit processes of observational, radical emergence. Finally, we take into consideration the role of computation in describing the physical world.
The problem of emergence in physical theories makes necessary to build a general theory of the relationships between the observed system and the observing system. It can be shown that there exists a correspondence between classical systems and computational dynamics according to the Shannon-Turing model. A classical system is an informational closed system with respect to the observer; this characterizes the emergent processes in classical physics as phenomenological emergence. In quantum systems, the analysis based on the computation theory fails. It is here shown that a quantum system is an informational open system with respect to the observer and able to exhibit processes of observational, radical emergence. Finally, we take into consideration the role of computation in describing the physical world.
The problem of emergence of classicality from quantum mechanics has been addressed over time through numerous frameworks, from Bohr's correspondence principle to quantum Darwinism. Traditional approaches associate the emergence of classicality with the decoherence process induced by large reservoirs on the system's state. In this work, we present an effective mechanism by which classicality emerges through the establishment of elements of reality. This involves the process of successive monitoring of noncommuting observables. To assess physical reality, we employ the realism criterion introduced by Bilobran and Angelo [EPL, 112 (2015) 40005], as well as their quantifier for the violations of this criterion. With these tools, we formally demonstrate, for generic systems, that a quasi-classical regime can always be reached with a sufficiently large number of incompatible measurements. Thus, instead of diagnosing the emergence of the classical regime in terms of the resulting algebraic characteristics for the density operator under the action of large reservoirs, our results reveal that classicality can emerge, at the level of physical elements of reality, from the coupling of the system with environments of a few degrees of freedom.