Abstract

We study the total quantum dimension in the thermodynamic limit of topologically ordered systems. In particular, using the anyons (or superselection sectors) of such models, we define a secret sharing scheme, storing information invisible to a malicious party, and argue that the total quantum dimension quantifies how well we can perform this task. We then argue that this can be made mathematically rigorous using the index theory of subfactors, originally due to Jones and later extended by Kosaki and Longo. This theory provides us with a ‘relative entropy’ of two von Neumann algebras and a quantum channel, and we argue how these can be used to quantify how much classical information two parties can hide form an adversary. We also review the total quantum dimension in finite systems, in particular how it relates to topological entanglement entropy. It is known that the latter also has an interpretation in terms of secret sharing schemes, although this is shown by completely different methods from ours. Our work provides a different and independent take on this, which at the same time is completely mathematically rigorous. This complementary point of view might be beneficial, for example, when studying the stability of the total quantum dimension when the system is perturbed.

Highlights

  • Quantum phases can be understood as equivalence classes of ground states of quantum many body systems [1]

  • We review the total quantum dimension in finite systems, in particular how it relates to topological entanglement entropy

  • In the thermodynamic limit of topologically ordered systems the total quantum dimension can be related to the Jones–Kosaki–Longo (JKL) index of certain inclusions of algebras of observables localised in cones [11]

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Summary

20 February 2017

This theory provides us with a ‘relative entropy’ of two von Neumann algebras and a quantum channel, and we argue how these can be used to quantify how much classical information two parties can hide form an adversary. It is known that the latter has an interpretation in terms of secret sharing schemes, this is shown by completely different methods from ours. Our work provides a different and independent take on this, which at the same time is completely mathematically rigorous. This complementary point of view might be beneficial, for example, when studying the stability of the total quantum dimension when the system is perturbed

Introduction
Finite dimensions
Thermodynamic limit
JKL index
Superselection sectors
Secret sharing
Channels and entropy
Relative entropies and classical information
Total quantum dimension
Private quantum subsystems
Stability under perturbations
Summary and discussion
Full Text
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