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Hydrodynamic Electron Flow and Hall Viscosity

MPG-Autoren
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Nandi,  Nabhanila
Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

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Schmidt,  Burkhard
Burkhard Schmidt, Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

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Mackenzie,  Andrew P.
Andrew Mackenzie, Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society;

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Zitation

Scaffidi, T., Nandi, N., Schmidt, B., Mackenzie, A. P., & Moore, J. E. (2017). Hydrodynamic Electron Flow and Hall Viscosity. Physical Review Letters, 118(22): 226601, pp. 1-5. doi:10.1103/PhysRevLett.118.226601.


Zitierlink: https://hdl.handle.net/11858/00-001M-0000-002D-7927-8
Zusammenfassung
In metallic samples of small enough size and sufficiently strong momentum-conserving scattering, the viscosity of the electron gas can become the dominant process governing transport. In this regime, momentum is a long-lived quantity whose evolution is described by an emergent hydrodynamical theory. Furthermore, breaking time-reversal symmetry leads to the appearance of an odd component to the viscosity called the Hall viscosity, which has attracted considerable attention recently due to its quantized nature in gapped systems but still eludes experimental confirmation. Based on microscopic calculations, we discuss how to measure the effects of both the even and odd components of the viscosity using hydrodynamic electronic transport in mesoscopic samples under applied magnetic fields.