arXiv subjects

M. Potthoff

Publications and source records attributed to M. Potthoff.

39 records · Page 3Linked to original sources

arXiv1997

Interpolating self-energy of the infinite-dimensional Hubbard model: Modifying the iterative perturbation theory

We develop an analytical expression for the self-energy of the infinite-dimensional Hubbard model that is correct in a number of different limits. The approach represents a generalization of the iterative perturbation theory to arbitrary fillings. In the weak-coupling regime perturbation theory to second order in the interaction U is recovered. The theory is exact in the atomic limit. The high-energy behavior of the self-energy up to order (1/E)**2 and thereby the first four moments of the spectral density are reproduced correctly. Referring to a standard strong-coupling moment method, we analyze the limit of strong U. Different modifications of the approach are discussed and tested by comparing with the results of an exact diagonalization study.

cond-mat.str-el↗

arXiv1997

One-step model of photoemission for non-local potentials

The one-step model of valence-band photoemission and inverse photoemission from single-crystal surfaces is reformulated for generalized (non-local, complex and energy-dependent) potentials. Thereby, it becomes possible to account for self-energy corrections taken from many-body electronic-structure calculations. The original formulation due to Pendry and co-workers employs the KKR multiple-scattering theory for the calculation of the initial state. This prevents a straightforward generalization of the one-step model to non-local potentials. We therefore consider the Dyson equation which is set up within a muffin-tin-orbitals representation as an alternative to obtain the initial-state Green function. This approach requires a revision of the transition-matrix elements which is carried out in detail. The final state is considered as a time-reversed LEED state as usual. The proposed generalization of the one-step model allows to distinguish between the bare photocurrent reflecting the (quasi-particle) band structure and the secondary effects due to the (dipole) selection rules and due to the wave-vector and energy dependence of the transition-matrix elements.

cond-mat.str-el↗

arXiv1997

Weak-coupling approach to the semi-infinite Hubbard model: Non-locality of the self-energy

The Hubbard model on a semi-infinite three-dimensional lattice is considered to investigate electron-correlation effects at single-crystal surfaces. The standard second-order perturbation theory in the interaction U is used to calculate the electronic self-energy and the quasi-particle density of states (QDOS) in the bulk as well as in the vicinity of the surface. Within a real-space representation we fully account for the non-locality of the self-energy and examine the quality of the local approximation. Numerical results are presented and discussed for the three different low-index surfaces of the simple-cubic lattice. Compared with the bulk significant differences can be found for the top-layer local self-energy, the imaginary part of which is energetically narrowed and has a reduced total weight. The non-local parts of the self-energy Sigma(ij)(E) decrease with increasing distance between the sites i and j. At the surface and for the three-dimensional bulk their decrease is faster than for a two-dimensional lattice. For all surfaces considered the effects of the non-local parts of the self-energy on the QDOS are found to be qualitatively the same as for the bulk: The weight of the quasi-particle resonance at the Fermi energy is lowered while the high-energy charge-excitation peaks become more pronounced. The main structures in the layer-dependent spectra are already recovered within the local approximation; taking into account the nearest-neighbor non-local parts turns out to be an excellent approximation. Due to the reduced coordination number for sites at the very surface, the top-layer QDOS is narrowed. Contrary to the the free (U=0) system, quasi-particle damping results in a comparatively weak layer dependence of the QDOS generally.

cond-mat.str-el↗