Fermi Edge Singularities: Boundstates and Finite Size Effects
arXiv:cond-mat/9704248 · doi:10.1088/0305-4470/30/16/017
Abstract
Fermi edge adsorption singularities (FES) are studied using a combination of conformal field theory (CFT), an exact sum rule and numerical work on a tight binding model which is shown to exhibit remarkable simplifying features. The relationship between FES and Anderson orthogonality exponent is established in great generality, using CFT, including the case where the core hole potential produces a boundstate. Universal results on the adsorption intensity in a finite sized sample are obtained. Various predictions are checked numerically and the evolution of the adsorption intensity with electron density is studied.
21 pages, 7 figures (included)
Cited by in corpus (12)
- Local quantum quenches in critical one-dimensional systems: entanglement, the Loschmidt echo, and light-cone effects
- Andreev scattering and Josephson current in a one-dimensional electron liquid
- Equilibrium and time-dependent Josephson current in one-dimensional superconducting junctions
- Entanglement evolution across defects in critical anisotropic Heisenberg chains
- Logarithmic corrections to the free energy from sharp corners with angle
- Exact full counting statistics for the staggered magnetization and the domain walls in the XY spin chain
- Fermi Edge Singularities in the Mesoscopic Regime: I. Anderson Orthogonality Catastrophe
- Tunneling singularities in the open Hubbard chain
- Fermi Edge Singularities in the Mesoscopic Regime: II. Photo-absorption Spectra
- Orthogonality catastrophe beyond bosonization from post-selection
- Finite-size energy of non-interacting Fermi gases
- Ground-state-energy universality of noninteracting fermionic systems