Gauge theory for topological waves in continuum fluids with odd viscosity

Fuente: arXiv
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Main Authors: Fujii, Keisuke, Ashida, Yuto
Format: Preprint
Published: 2024
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_version_ 1866908506257358848
author Fujii, Keisuke
Ashida, Yuto
author_facet Fujii, Keisuke
Ashida, Yuto
contents We consider two-dimensional continuum fluids with odd viscosity under a chiral body force. The chiral body force makes the low-energy excitation spectrum of the fluids gapped, and the odd viscosity allows us to introduce the first Chern number of each energy band in the fluids. Employing a mapping between hydrodynamic variables and U(1) gauge-field strengths, we derive a U(1) gauge theory for topologically nontrivial waves. The resulting U(1) gauge theory is given by the Maxwell-Chern-Simons theory with an additional term associated with odd viscosity. We then solve the equations of motion for the gauge fields concretely in the presence of the boundary and find edge-mode solutions. We finally discuss the fate of bulk-boundary correspondence (BBC) in the context of continuum systems.
format Preprint
id arxiv_https___arxiv_org_abs_2411_02958
institution arXiv
publishDate 2024
record_format arxiv
spellingShingle Gauge theory for topological waves in continuum fluids with odd viscosity
Fujii, Keisuke
Ashida, Yuto
Soft Condensed Matter
Strongly Correlated Electrons
High Energy Physics - Phenomenology
High Energy Physics - Theory
Atmospheric and Oceanic Physics
We consider two-dimensional continuum fluids with odd viscosity under a chiral body force. The chiral body force makes the low-energy excitation spectrum of the fluids gapped, and the odd viscosity allows us to introduce the first Chern number of each energy band in the fluids. Employing a mapping between hydrodynamic variables and U(1) gauge-field strengths, we derive a U(1) gauge theory for topologically nontrivial waves. The resulting U(1) gauge theory is given by the Maxwell-Chern-Simons theory with an additional term associated with odd viscosity. We then solve the equations of motion for the gauge fields concretely in the presence of the boundary and find edge-mode solutions. We finally discuss the fate of bulk-boundary correspondence (BBC) in the context of continuum systems.
title Gauge theory for topological waves in continuum fluids with odd viscosity
topic Soft Condensed Matter
Strongly Correlated Electrons
High Energy Physics - Phenomenology
High Energy Physics - Theory
Atmospheric and Oceanic Physics
url https://arxiv.org/abs/2411.02958