Turbulent hydrodynamics in strongly correlated Kagome metals
arXiv:1911.06810 · doi:10.1038/s41467-020-17663-x
Abstract
A current challenge in condensed matter physics is the realization of strongly correlated, viscous electron fluids. These fluids are not amenable to the perturbative methods of Fermi liquid theory, but can be described by holography, that is, by mapping them onto a weakly curved gravitational theory via gauge/gravity duality. The canonical system considered for realizations has been graphene, which possesses Dirac dispersions at low energies as well as significant Coulomb interactions between the electrons. In this work, we show that Kagome systems with electron fillings adjusted to the Dirac nodes of their band structure provide a much more compelling platform for realizations of viscous electron fluids, including non-linear effects such as turbulence. In particular, we find that in stoichiometric Scandium (Sc) Herbertsmithite, the fine-structure constant, which measures the effective Coulomb interaction and hence reflects the strength of the correlations, is enhanced by a factor of about 3.2 as compared to graphene, due to orbital hybridization. We employ holography to estimate the ratio of the shear viscosity over the entropy density in Sc-Herbertsmithite, and find it about three times smaller than in graphene. These findings put, for the first time, the turbulent flow regime described by holography within the reach of experiments.
4 pages plus supplement, 2 figures, 1 table
References in corpus (35)
- Quantum ESPRESSO: a modular and open-source software project for quantum simulations of materials
- Two-Dimensional Gas of Massless Dirac Fermions in Graphene
- Phonons and related properties of extended systems from density-functional perturbation theory
- Viscosity in Strongly Interacting Quantum Field Theories from Black Hole Physics
- Shear viscosity of strongly coupled N=4 supersymmetric Yang-Mills plasma
- EPW: Electron-phonon coupling, transport and superconducting properties using maximally localized Wannier functions
- Frequency-dependent local interactions and low-energy effective models from electronic structure calculations
- Negative local resistance caused by viscous electron backflow in graphene
- Universality of the shear viscosity in supergravity
- Strength of effective Coulomb interactions in graphene and graphite
- Unconventional Fermi surface instabilities in the Kagome Hubbard Model
- Evidence for hydrodynamic electron flow in PdCoO
- Superballistic flow of viscous electron fluid through graphene constrictions
- Coupling Constant Dependence in the Thermodynamics of N=4 Supersymmetric Yang-Mills Theory
- Electron Viscosity, Current Vortices and Negative Nonlocal Resistance in Graphene
- Quantum critical transport in clean graphene
- Coupling constant dependence of the shear viscosity in N=4 supersymmetric Yang-Mills theory
- Sublattice Interference in the Kagome Hubbard Model
- Electrical and Thermal Transport at the Planckian Bound of Dissipation in the Hydrodynamic Electron Fluid of WP2
- Non-local transport and the hydrodynamic shear viscosity in graphene
- Theoretical prediction of a strongly correlated Dirac metal
- Hydrodynamic description of transport in strongly correlated electron systems
- Planckian dissipation, minimal viscosity and the transport in cuprate strange metals
- The Shear Viscosity to Entropy Ratio: A Status Report
- Viscous electron fluids
- Electron hydrodynamics dilemma: whirlpools or no whirlpools
- Holographic turbulence
- Wannier Function Approach to Realistic Coulomb Interactions in Layered Materials and Heterostructures
- Out-of-bounds hydrodynamics in anisotropic Dirac fluids
- Electron doping of proposed quantum spin liquid kagomé Zn-Cu hydroxyl-halides produces localized states in the band gap
- Dynamo Effect and Turbulence in Hydrodynamic Weyl Metals
- Prospects for the detection of electronic pre-turbulence in graphene
- Bond order wave instabilities in doped frustrated antiferromagnets: "Valence bond solids" at fractional filling
- Strongly coupled electron fluids in the Poiseuille regime
- Critical Viscosity of a Fluctuating Superconductor
Cited by in corpus (27)
- Topological kagome magnets and superconductors
- Nature of unconventional pairing in the kagome superconductors AVSb
- Direct observation of vortices in an electron fluid
- Optical detection of charge-density-wave instability in the non-magnetic kagome metal KVSb
- Hydrodynamic approach to two-dimensional electron systems
- Observation of current whirlpools in graphene at room temperature
- Flat band separation and robust spin-Berry curvature in bilayer kagome metals
- Chiral hydrodynamics in strong external magnetic fields
- Dynamics and Resilience of the Charge Density Wave in a bilayer kagome metal
- Kagome metals
- Para-hydrodynamics from weak surface scattering in ultraclean thin flakes
- Gibbons-Hawking-York boundary terms and the generalized geometrical trinity of gravity
- Emergent chiral spin ordering and anomalous Hall effect of kagome lattice at 1/3 filling
- Strong suppression of electron convection in Dirac and Weyl semimetals
- Electric conductivity in non-Hermitian holography
- Anomalous Gurzhi effect
- Hall viscosity and hydrodynamic inverse Nernst effect in graphene
- Shear viscosity expression for a graphene system in relaxation time approximation
- Hydrodynamics of the electronic Fermi liquid: a pedagogical overview
- Chiral symmetry breaking through spontaneous dimerization in kagomé metals
- Stray magnetic field and stability of time-dependent viscous electron flow
- Concurrence of topological electrons and magnons in the Kagome ferromagnet CoCu3(OH)6Cl2
- Novel semi-circle law and Hall sliding in a strongly interacting electron liquid
- Wiedemann-Franz law violation domain for graphene and nonrelativistic systems
- Graphene is neither Relativistic nor Non-Relativistic case: Thermodynamics Aspects
- Relativistic Wind Farm Effect: Possibly Turbulent Flow of a Charged, Massless Relativistic Fluid in Graphene
- Torsional Hall Viscosity of Massive Chern Insulators: Magnetic Field and Momentum Deformations