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Main Authors: Fünfhaus, Axel, García-Díez, Mikel, Vergniory, M. G., Kopp, Thilo, Winter, Stephen M., Valentí, Roser
Format: Preprint
Published: 2025
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Online Access:https://arxiv.org/abs/2501.11396
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author Fünfhaus, Axel
García-Díez, Mikel
Vergniory, M. G.
Kopp, Thilo
Winter, Stephen M.
Valentí, Roser
author_facet Fünfhaus, Axel
García-Díez, Mikel
Vergniory, M. G.
Kopp, Thilo
Winter, Stephen M.
Valentí, Roser
contents In the study of quantum spin liquids, the Kitaev model plays a pivotal role due to the fact that its ground state is exactly known as well as the fact that it may be realized in strongly frustrated materials such as $α$-RuCl${}_3$. While topological insulators and superconductors can be investigated by means of topological band theory -- in particular the topological quantum chemistry (TQC) formalism -- the Kitaev model evades such a treatment, as it is not possible to set up a proper single-particle Green's function for it. We instead associate spin operators with ``orbitals'' that give rise to a band structure. It is thereby possible to analyze the corresponding excitation spectrum engendered by these localized excitations by means of TQC. Special attention is given to the low-energy topological edge mode spectrum. Our work sheds light on the question how the TQC formalism may be generalized to strongly correlated and topologically ordered systems like the Kitaev model.
format Preprint
id arxiv_https___arxiv_org_abs_2501_11396
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Band representations in Strongly Correlated Settings: The Kitaev Honeycomb Model
Fünfhaus, Axel
García-Díez, Mikel
Vergniory, M. G.
Kopp, Thilo
Winter, Stephen M.
Valentí, Roser
Strongly Correlated Electrons
In the study of quantum spin liquids, the Kitaev model plays a pivotal role due to the fact that its ground state is exactly known as well as the fact that it may be realized in strongly frustrated materials such as $α$-RuCl${}_3$. While topological insulators and superconductors can be investigated by means of topological band theory -- in particular the topological quantum chemistry (TQC) formalism -- the Kitaev model evades such a treatment, as it is not possible to set up a proper single-particle Green's function for it. We instead associate spin operators with ``orbitals'' that give rise to a band structure. It is thereby possible to analyze the corresponding excitation spectrum engendered by these localized excitations by means of TQC. Special attention is given to the low-energy topological edge mode spectrum. Our work sheds light on the question how the TQC formalism may be generalized to strongly correlated and topologically ordered systems like the Kitaev model.
title Band representations in Strongly Correlated Settings: The Kitaev Honeycomb Model
topic Strongly Correlated Electrons
url https://arxiv.org/abs/2501.11396