Whenever a quantum environment emerges as a classical system, it behaves like a measuring apparatus

We study the dynamics of a quantum system $\Gamma$ with an environment $\Xi$ made of $N$ elementary quantum components. We aim at answering the following questions: can the evolution of $\Gamma$ be characterized by some general features when $N$ becomes very large, regardless of the specific form of...

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Main Authors: Caterina Foti, Teiko Heinosaari, Sabrina Maniscalco, Paola Verrucchi
Format: Article
Language:English
Published: Verein zur Förderung des Open Access Publizierens in den Quantenwissenschaften 2019-08-01
Series:Quantum
Online Access:https://quantum-journal.org/papers/q-2019-08-26-179/pdf/
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spelling doaj-de11823e88c34158831ed317b85e3a302020-11-25T01:30:38ZengVerein zur Förderung des Open Access Publizierens in den QuantenwissenschaftenQuantum2521-327X2019-08-01317910.22331/q-2019-08-26-17910.22331/q-2019-08-26-179Whenever a quantum environment emerges as a classical system, it behaves like a measuring apparatusCaterina FotiTeiko HeinosaariSabrina ManiscalcoPaola VerrucchiWe study the dynamics of a quantum system $\Gamma$ with an environment $\Xi$ made of $N$ elementary quantum components. We aim at answering the following questions: can the evolution of $\Gamma$ be characterized by some general features when $N$ becomes very large, regardless of the specific form of its interaction with each and every component of $\Xi$? In other terms: should we expect all quantum systems with a macroscopic environment to undergo a somehow similar evolution? And if yes, of what type? In order to answer these questions we use well established results from large-$N$ quantum field theories, particularly referring to the conditions ensuring a large-$N$ quantum model to be effectively described by a classical theory. We demonstrate that the fulfillment of these conditions, when properly imported into the framework of the open quantum systems dynamics, guarantees that the evolution of $\Gamma$ is always of the same type of that expected if $\Xi$ were a measuring apparatus, no matter the details of the actual interaction. On the other hand, such details are found to determine the specific basis w.r.t. which $\Gamma$ undergoes the decoherence dictated by the dynamical description of the quantum measurement process. This result wears two hats: on the one hand it clarifies the physical origin of the formal statement that, under certain conditions, any channel from $\rho_\Gamma$ to $\rho_\Xi$ takes the form of a measure-and-prepare map, as recently shown in Ref. \cite{BrandaoPH15}; on the other hand, it formalizes the qualitative argument that the reason why we do not observe state superpositions is the continual measurement performed by the environment.https://quantum-journal.org/papers/q-2019-08-26-179/pdf/
collection DOAJ
language English
format Article
sources DOAJ
author Caterina Foti
Teiko Heinosaari
Sabrina Maniscalco
Paola Verrucchi
spellingShingle Caterina Foti
Teiko Heinosaari
Sabrina Maniscalco
Paola Verrucchi
Whenever a quantum environment emerges as a classical system, it behaves like a measuring apparatus
Quantum
author_facet Caterina Foti
Teiko Heinosaari
Sabrina Maniscalco
Paola Verrucchi
author_sort Caterina Foti
title Whenever a quantum environment emerges as a classical system, it behaves like a measuring apparatus
title_short Whenever a quantum environment emerges as a classical system, it behaves like a measuring apparatus
title_full Whenever a quantum environment emerges as a classical system, it behaves like a measuring apparatus
title_fullStr Whenever a quantum environment emerges as a classical system, it behaves like a measuring apparatus
title_full_unstemmed Whenever a quantum environment emerges as a classical system, it behaves like a measuring apparatus
title_sort whenever a quantum environment emerges as a classical system, it behaves like a measuring apparatus
publisher Verein zur Förderung des Open Access Publizierens in den Quantenwissenschaften
series Quantum
issn 2521-327X
publishDate 2019-08-01
description We study the dynamics of a quantum system $\Gamma$ with an environment $\Xi$ made of $N$ elementary quantum components. We aim at answering the following questions: can the evolution of $\Gamma$ be characterized by some general features when $N$ becomes very large, regardless of the specific form of its interaction with each and every component of $\Xi$? In other terms: should we expect all quantum systems with a macroscopic environment to undergo a somehow similar evolution? And if yes, of what type? In order to answer these questions we use well established results from large-$N$ quantum field theories, particularly referring to the conditions ensuring a large-$N$ quantum model to be effectively described by a classical theory. We demonstrate that the fulfillment of these conditions, when properly imported into the framework of the open quantum systems dynamics, guarantees that the evolution of $\Gamma$ is always of the same type of that expected if $\Xi$ were a measuring apparatus, no matter the details of the actual interaction. On the other hand, such details are found to determine the specific basis w.r.t. which $\Gamma$ undergoes the decoherence dictated by the dynamical description of the quantum measurement process. This result wears two hats: on the one hand it clarifies the physical origin of the formal statement that, under certain conditions, any channel from $\rho_\Gamma$ to $\rho_\Xi$ takes the form of a measure-and-prepare map, as recently shown in Ref. \cite{BrandaoPH15}; on the other hand, it formalizes the qualitative argument that the reason why we do not observe state superpositions is the continual measurement performed by the environment.
url https://quantum-journal.org/papers/q-2019-08-26-179/pdf/
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