Dielectric response of Anderson and pseudogapped insulators
arXiv:1711.05972 · doi:10.1088/1367-2630/aac0d7
Abstract
Using a combination of analytic and numerical methods, we study the polarizability of a (non-interacting) Anderson insulator in one, two, and three dimensions and demonstrate that, in a wide range of parameters, it scales proportionally to the square of the localization length, contrary to earlier claims based on the effective-medium approximation. We further analyze the effect of electron-electron interactions on the dielectric constant in quasi-1D, quasi-2D and 3D materials with large localization length, including both Coulomb repulsion and phonon-mediated attraction. The phonon-mediated attraction (in the pseudogapped state on the insulating side of the Superconductor-Insulator Transition) produces a correction to the dielectric constant, which may be detected from a linear response of a dielectric constant to an external magnetic field.
9 pages
References in corpus (5)
- Localization of preformed Cooper-pairs in disordered superconductors
- Eigenfunction fractality and pseudogap state near superconductor-insulator transition
- Microwave-induced excess quasiparticles in superconducting resonators measured through correlated conductivity fluctuations
- Correlations of the local density of states in quasi-one-dimensional wires
- Low-energy dynamical response of an Anderson insulator with local attraction
Cited by in corpus (7)
- Mott, Floquet, and the response of periodically driven Anderson insulators
- Overactivated transport in the localized phase of the superconductor-insulator transition
- Characterizing dielectric properties of ultra-thin films using superconducting coplanar microwave resonators
- Electron-phonon cooling power in Anderson insulators
- Anyon superconductivity and plateau transitions in doped fractional quantum anomalous Hall insulators
- Mean-field theory of first-order quantum superconductor-insulator transition
- Atomically Thin Amorphous Carbon with an Ultralow Dielectric Constant