Non-local transport and the Hall viscosity of 2D hydrodynamic electron liquids
arXiv:1706.08363 · doi:10.1103/PhysRevB.96.195401
Abstract
In a fluid subject to a magnetic field the viscous stress tensor has a dissipationless antisymmetric component controlled by the so-called Hall viscosity. We here propose an all-electrical scheme that allows a determination of the Hall viscosity of a two-dimensional electron liquid in a solid-state device.
12 pages, 4 figures
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