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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Verein zur Förderung des Open Access Publizierens in den Quantenwissenschaften
2019-08-01
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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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