LDA+DMFT study for $La_{1-x}Sr_{x}TiO_{3}$
| dc.creator | Zoelfl, M. B. | |
| dc.creator | Pruschke, Th. | |
| dc.creator | Keller, J. | |
| dc.creator | Poteryaev, A. I. | |
| dc.creator | Nekrasov, I. A. | |
| dc.creator | Anisimov, V. I. | |
| dc.date | 1999-09-24 | |
| dc.date.accessioned | 2026-07-07T03:14:38Z | |
| dc.date.available | 2026-07-07T03:14:38Z | |
| dc.description | The dynamical mean-field theory together with the non-crossing approximation is used to set up a novel scheme to study the electronic structure of strongly correlated electron systems. The non-interacting band structure is obtained from a density functional calculation within the local density approximation. With this method the doped Mott insulator $\rm La_{1-x}Sr_x Ti O_3$ is studied. Starting from first-principle calculations for a cubic and an orthorhombic system we determined the one-particle spectrum. Both one-particle spectra show a lower Hubbard band (seen as $d^1 \to d^o$ transitions in photo emission experiments), a Kondo resonance near the Fermi energy and the upper Hubbard band ($d^1\to d^2$ transitions in an inverse photoemission experiment). The upper Hubbard band develops a multipeak structure, a consequence of the consideration of all local two-particle correlations, which leads to the full multiplet structure in the atomic limit. The calculation for the orthorhombic system shows qualitative good agreement when compared with experimental photoemission spectra. | |
| dc.description | 6 pages, 4 figures | |
| dc.identifier | https://arxiv.org/abs/cond-mat/9909359 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/9909359 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/29748 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.subject | Materials Science | |
| dc.title | LDA+DMFT study for $La_{1-x}Sr_{x}TiO_{3}$ | |
| dc.type | text |