Conformal QED in two-dimensional topological insulators
Abstract It has been shown that local four-fermion interactions on the edges of two-dimensional time-reversal-invariant topological insulators give rise to a new non-Fermi-liquid phase, called helical Luttinger liquid (HLL). Here, we provide a first-principle derivation of this HLL based on the gaug...
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2017
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oai:doaj.org-article:33986a7ddb584d39891938ad7c43b75c2021-12-02T11:53:07ZConformal QED in two-dimensional topological insulators10.1038/s41598-017-14635-y2045-2322https://doaj.org/article/33986a7ddb584d39891938ad7c43b75c2017-10-01T00:00:00Zhttps://doi.org/10.1038/s41598-017-14635-yhttps://doaj.org/toc/2045-2322Abstract It has been shown that local four-fermion interactions on the edges of two-dimensional time-reversal-invariant topological insulators give rise to a new non-Fermi-liquid phase, called helical Luttinger liquid (HLL). Here, we provide a first-principle derivation of this HLL based on the gauge-theory approach. We start by considering massless Dirac fermions confined on the one-dimensional boundary of the topological insulator and interacting through a three-dimensional quantum dynamical electromagnetic field. Within these assumptions, through a dimensional-reduction procedure, we derive the effective 1 + 1-dimensional interacting fermionic theory and reveal its underlying gauge theory. In the low-energy regime, the gauge theory that describes the edge states is given by a conformal quantum electrodynamics (CQED), which can be mapped exactly into a HLL with a Luttinger parameter and a renormalized Fermi velocity that depend on the value of the fine-structure constant α.Natália MenezesGiandomenico PalumboCristiane Morais SmithNature PortfolioarticleMedicineRScienceQENScientific Reports, Vol 7, Iss 1, Pp 1-6 (2017) |
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Medicine R Science Q Natália Menezes Giandomenico Palumbo Cristiane Morais Smith Conformal QED in two-dimensional topological insulators |
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Abstract It has been shown that local four-fermion interactions on the edges of two-dimensional time-reversal-invariant topological insulators give rise to a new non-Fermi-liquid phase, called helical Luttinger liquid (HLL). Here, we provide a first-principle derivation of this HLL based on the gauge-theory approach. We start by considering massless Dirac fermions confined on the one-dimensional boundary of the topological insulator and interacting through a three-dimensional quantum dynamical electromagnetic field. Within these assumptions, through a dimensional-reduction procedure, we derive the effective 1 + 1-dimensional interacting fermionic theory and reveal its underlying gauge theory. In the low-energy regime, the gauge theory that describes the edge states is given by a conformal quantum electrodynamics (CQED), which can be mapped exactly into a HLL with a Luttinger parameter and a renormalized Fermi velocity that depend on the value of the fine-structure constant α. |
format |
article |
author |
Natália Menezes Giandomenico Palumbo Cristiane Morais Smith |
author_facet |
Natália Menezes Giandomenico Palumbo Cristiane Morais Smith |
author_sort |
Natália Menezes |
title |
Conformal QED in two-dimensional topological insulators |
title_short |
Conformal QED in two-dimensional topological insulators |
title_full |
Conformal QED in two-dimensional topological insulators |
title_fullStr |
Conformal QED in two-dimensional topological insulators |
title_full_unstemmed |
Conformal QED in two-dimensional topological insulators |
title_sort |
conformal qed in two-dimensional topological insulators |
publisher |
Nature Portfolio |
publishDate |
2017 |
url |
https://doaj.org/article/33986a7ddb584d39891938ad7c43b75c |
work_keys_str_mv |
AT nataliamenezes conformalqedintwodimensionaltopologicalinsulators AT giandomenicopalumbo conformalqedintwodimensionaltopologicalinsulators AT cristianemoraissmith conformalqedintwodimensionaltopologicalinsulators |
_version_ |
1718394858457006080 |