A Shortcut from Categorical Quantum Theory to Convex Operational Theories

This paper charts a very direct path between the categorical approach to quantum mechanics, due to Abramsky and Coecke, and the older convex-operational approach based on ordered vector spaces (recently reincarnated as "generalized probabilistic theories"). In the former, the objects of a...

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Main Author: Alexander Wilce
Format: Article
Language:English
Published: Open Publishing Association 2018-02-01
Series:Electronic Proceedings in Theoretical Computer Science
Online Access:http://arxiv.org/pdf/1803.00707v1
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spelling doaj-044842c53d8a4f5683245ada122e0d3d2020-11-24T21:43:51ZengOpen Publishing AssociationElectronic Proceedings in Theoretical Computer Science2075-21802018-02-01266Proc. QPL 201722223610.4204/EPTCS.266.15:52A Shortcut from Categorical Quantum Theory to Convex Operational TheoriesAlexander Wilce0 Susquehanna University This paper charts a very direct path between the categorical approach to quantum mechanics, due to Abramsky and Coecke, and the older convex-operational approach based on ordered vector spaces (recently reincarnated as "generalized probabilistic theories"). In the former, the objects of a symmetric monoidal category C are understood to represent physical systems and morphisms, physical processes. Elements of the monoid C(I,I) are interpreted somewhat metaphorically as probabilities. Any monoid homomorphism from the scalars of a symmetric monoidal category C gives rise to a covariant functor V_o from C to a category of dual-pairs of ordered vector spaces. Specifying a natural transformation u from V_o to 1 (where 1 is the trivial such functor) allows us to identify normalized states, and, thus, to regard the image category V_o(C) as consisting of concrete operational models. In this case, if A and B are objects in C, then V_o(A x B) defines a non-signaling composite of V_o(A) and V_o(B). Provided either that C satisfies a "local tomography" condition, or that C is compact closed, this defines a symmetric monoidal structure on the image category, and makes V_o a (strict) monoidal functor.http://arxiv.org/pdf/1803.00707v1
collection DOAJ
language English
format Article
sources DOAJ
author Alexander Wilce
spellingShingle Alexander Wilce
A Shortcut from Categorical Quantum Theory to Convex Operational Theories
Electronic Proceedings in Theoretical Computer Science
author_facet Alexander Wilce
author_sort Alexander Wilce
title A Shortcut from Categorical Quantum Theory to Convex Operational Theories
title_short A Shortcut from Categorical Quantum Theory to Convex Operational Theories
title_full A Shortcut from Categorical Quantum Theory to Convex Operational Theories
title_fullStr A Shortcut from Categorical Quantum Theory to Convex Operational Theories
title_full_unstemmed A Shortcut from Categorical Quantum Theory to Convex Operational Theories
title_sort shortcut from categorical quantum theory to convex operational theories
publisher Open Publishing Association
series Electronic Proceedings in Theoretical Computer Science
issn 2075-2180
publishDate 2018-02-01
description This paper charts a very direct path between the categorical approach to quantum mechanics, due to Abramsky and Coecke, and the older convex-operational approach based on ordered vector spaces (recently reincarnated as "generalized probabilistic theories"). In the former, the objects of a symmetric monoidal category C are understood to represent physical systems and morphisms, physical processes. Elements of the monoid C(I,I) are interpreted somewhat metaphorically as probabilities. Any monoid homomorphism from the scalars of a symmetric monoidal category C gives rise to a covariant functor V_o from C to a category of dual-pairs of ordered vector spaces. Specifying a natural transformation u from V_o to 1 (where 1 is the trivial such functor) allows us to identify normalized states, and, thus, to regard the image category V_o(C) as consisting of concrete operational models. In this case, if A and B are objects in C, then V_o(A x B) defines a non-signaling composite of V_o(A) and V_o(B). Provided either that C satisfies a "local tomography" condition, or that C is compact closed, this defines a symmetric monoidal structure on the image category, and makes V_o a (strict) monoidal functor.
url http://arxiv.org/pdf/1803.00707v1
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