Image resonance in the many-body density of states at a metal surface
arXiv:cond-mat/0305678 · doi:10.1103/PhysRevB.68.195404
Abstract
The electronic properties of a semi-infinite metal surface without a bulk gap are studied by a formalism able to account for the continuous spectrum of the system. The density of states at the surface is calculated within the approximation of many-body perturbation theory. We demonstrate the presence of an unoccupied surface resonance peaked at the position of the first image state. The resonance encompasses the whole Rydberg series of image states and cannot be resolved into individual peaks. Its origin is the shift in spectral weight when many-body correlation effects are taken into account.
5 pages, 6 figures
References in corpus (2)
Cited by in corpus (9)
- Resolution-of-identity approach to Hartree-Fock, hybrid density functionals, RPA, MP2, and \textit{GW} with numeric atom-centered orbital basis functions
- The GW compendium: A practical guide to theoretical photoemission spectroscopy
- Combining GW calculations with exact-exchange density-functional theory: An analysis of valence-band photoemission for compound semiconductors
- Screening in 2D: GW calculations for surfaces and thin films using the repeated-slab approach
- Dielectric anisotropy in the GW space-time method
- Image states in metal clusters
- Many-body approach to infinite non-periodic systems: application to the surface of semi-infinite jellium
- Resolubility of Image-Potential Resonances
- Mean-field approximation of the Hubbard model expressed in a many-body basis