Clean two-dimensional Fermi liquids are now known to exhibit an intermediate tomographic regime, between ballistic and Navier-Stokes transport, caused by the anomalously slow relaxation of parity-odd multipolar deformations of the Fermi surface. Here, we show that this anomaly extends to the dynamical realm. Starting from a microscopic numerical evaluation of the linearized electron-electron collision operator, we find that the finite-frequency nonlocal conductivity is controlled at low frequency by a single hydrodynamic pole, $\sigma (q,\omega )=\mathcal{D}(q)/(i\omega +{\eta }_{\star }{q}^z)$, with dynamical exponent $z=4/3$ and superdiffusive viscosity ${\eta }_{\star }$. Remarkably, the pole residue itself is scale dependent and obeys $\mathcal{D}(q)\sim q^{-\alpha }$ with $\alpha =1/3$, so the dynamical properties are described by two separate exponents rather than one. We interpret the residue suppression using a Krylov-chain description of current relaxation: As $q$ increases, the longest-lived quasinormal mode ceases to be a nearly pure current excitation and spreads over higher odd angular harmonics. Finally, we show that ac transport in narrow channels provides a direct experimental probe of these phenomena.

Close

PrevNext

View figure in article

• Electrical conductivity
• Strongly correlated systems
• Two-dimensional electron system
• Boltzmann theory
• Hydrodynamics