Electron Hydrodynamics: Viscosity Tensor and effects of a Magnetic field

Anubhav Srivastava, Subroto Mukerjee

TL;DR

Addresses how Berry curvature $oldsymbol{ ext{Ω}}_{oldsymbol{k}}$ and magnetic field $oldsymbol{B}$ modify hydrodynamic electron transport in ultra-clean 2D systems by deriving the full viscosity tensor, including odd components $L^9$, and the vortical transport coefficients. The authors show that Berry curvature induces dissipationless odd viscosity via the intrinsic angular momentum of Bloch wavepackets and provide explicit results for a tilted Dirac cone model with Berry curvature $ ext{Ω}_{s eq 0}(oldsymbol{k})$. They formulate the non-equilibrium distribution $g$ using a semiclassical Boltzmann equation, obtaining $g_1$ and $g_2$ up to second order in $ au_{ee}$ and demonstrate Onsager reciprocity relations under transformations $oldsymbol{B} o -oldsymbol{B}$ and $oldsymbol{Ω}_{oldsymbol{k}} o -oldsymbol{Ω}_{-oldsymbol{k}}$. The work shows that magnetic-field–induced vortical currents stem from the out-of-equilibrium sector and remains consistent with Curie symmetry in centrosymmetric limits. Overall, it provides a comprehensive framework linking Berry-geometry, magnetotransport, and hydrodynamic viscosity in 2D electron fluids.

Abstract

Transport due to electrons in ultra-clean two dimensional systems can be hydrodynamic in nature with the momentum of the electrons being conserved in the bulk. This hydrodynamic behavior coupled with effects of Berry curvature arising from band structure can give rise to novel vortical transport coefficients relating the stress tensor to gradients in the electrostatic potential and temperature. These coefficients have been calculated in the absence of a magnetic field and have been shown to depend only on the equilibrium distribution function~\cite{Chadha_Mukerjee2024}. In this paper, we first obtain an expression for the viscosity tensor and show that the Berry curvature generates odd components of the viscosity tensor arising from the intrinsic angular momentum of the Bloch wavepackets. We calculate the viscosity tensor for a two-dimensional microscopic model of tilted Dirac cones. We next obtain the vortical coefficients and the viscosity tensor in the presence of a magnetic field and extend the Onsager relations for them to include both the magnetic field and the Berry curvature. We show that the field dependence of the coefficients manifests itself in the non-equilibrium part of the distribution function and calculate them to second order in the electron-electron scattering time. We explicitly show that the expressions we obtain are consistent with the Onsager relations.

Electron Hydrodynamics: Viscosity Tensor and effects of a Magnetic field

TL;DR

Addresses how Berry curvature

and magnetic field

modify hydrodynamic electron transport in ultra-clean 2D systems by deriving the full viscosity tensor, including odd components

, and the vortical transport coefficients. The authors show that Berry curvature induces dissipationless odd viscosity via the intrinsic angular momentum of Bloch wavepackets and provide explicit results for a tilted Dirac cone model with Berry curvature

. They formulate the non-equilibrium distribution

using a semiclassical Boltzmann equation, obtaining

and

up to second order in

and demonstrate Onsager reciprocity relations under transformations

and

. The work shows that magnetic-field–induced vortical currents stem from the out-of-equilibrium sector and remains consistent with Curie symmetry in centrosymmetric limits. Overall, it provides a comprehensive framework linking Berry-geometry, magnetotransport, and hydrodynamic viscosity in 2D electron fluids.

Abstract

Transport due to electrons in ultra-clean two dimensional systems can be hydrodynamic in nature with the momentum of the electrons being conserved in the bulk. This hydrodynamic behavior coupled with effects of Berry curvature arising from band structure can give rise to novel vortical transport coefficients relating the stress tensor to gradients in the electrostatic potential and temperature. These coefficients have been calculated in the absence of a magnetic field and have been shown to depend only on the equilibrium distribution function~\cite{Chadha_Mukerjee2024}. In this paper, we first obtain an expression for the viscosity tensor and show that the Berry curvature generates odd components of the viscosity tensor arising from the intrinsic angular momentum of the Bloch wavepackets. We calculate the viscosity tensor for a two-dimensional microscopic model of tilted Dirac cones. We next obtain the vortical coefficients and the viscosity tensor in the presence of a magnetic field and extend the Onsager relations for them to include both the magnetic field and the Berry curvature. We show that the field dependence of the coefficients manifests itself in the non-equilibrium part of the distribution function and calculate them to second order in the electron-electron scattering time. We explicitly show that the expressions we obtain are consistent with the Onsager relations.