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(Reference retrieved automatically from Web of Science through information on FAPESP grant and its corresponding number as mentioned in the publication by the authors.)

Hydrodynamics of two-dimensional compressible fluid with broken parity: Variational principle and free surface dynamics in the absence of dissipation

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Author(s):
Abanov, Alexander G. [1, 2] ; Can, Tankut [3] ; Ganeshan, Sriram [4] ; Monteiro, Gustavo M. [5, 6]
Total Authors: 4
Affiliation:
[1] SUNY Stony Brook, Dept Phys & Astron, Stony Brook, NY 11794 - USA
[2] Simons Ctr Geometry & Phys, Stony Brook, NY 11794 - USA
[3] CUNY, Grad Ctr, Initiat Theoret Sci, New York, NY 10012 - USA
[4] CUNY City Coll, Dept Phys, New York, NY 10031 - USA
[5] Univ Estadual Campinas, Inst Fis Gleb Wataghin, UNICAMP, BR-13083859 Campinas, SP - Brazil
[6] Int Inst Phys, Campus Univ Lagoa Nova, BR-59078970 Natal, RN - Brazil
Total Affiliations: 6
Document type: Journal article
Source: PHYSICAL REVIEW FLUIDS; v. 5, n. 10 OCT 21 2020.
Web of Science Citations: 0
Abstract

We consider an isotropic compressible nondissipative fluid with broken parity subject to free surface boundary conditions in two spatial dimensions. The hydrodynamic equations describing the bulk dynamics of the fluid and the free surface boundary conditions depend explicitly on the parity-breaking nondissipative odd viscosity term. We construct an effective action which gives both bulk hydrodynamic equations and free surface boundary conditions. The free surface boundary conditions require an additional boundary term in the action which resembles a 1 + 1D chiral boson field coupled to the background geometry. We solve the linearized hydrodynamic equations for the deep water case and derive the dispersion of chiral surface waves. We show that in the long-wavelength limit the flow profile exhibits an oscillating vortical boundary layer near the free surface. The layer thickness is controlled by the ratio between the odd viscosity (nu(o)) and the sound velocity (c(s)), delta similar to nu(o)/c(s). In the incompressible limit, c(s) -> infinity, the vortical boundary layer becomes singular with the vorticity within the layer diverging as omega similar to c(s). The boundary layer is formed by odd viscosity coupling the divergence of velocity del center dot nu to vorticity del x nu. It results in nontrivial chiral free surface dynamics even in the absence of external forces. The structure of the odd-viscosity-induced boundary layer is very different from the conventional free surface boundary layer associated with dissipative shear viscosity. (AU)

FAPESP's process: 16/13517-0 - Topological and transport properties of chiral materials
Grantee:Gustavo Machado Monteiro
Support Opportunities: Scholarships in Brazil - Post-Doctoral