Dynamical CPA and Tight-Binding LMTO Approach to Correlated Electron System
| dc.creator | Kakehashi, Y. | |
| dc.creator | Shimabukuro, T. | |
| dc.creator | Tamashiro, T | |
| dc.creator | Nakamura, T. | |
| dc.date | 2008-07-05 | |
| dc.date.accessioned | 2026-07-07T09:48:41Z | |
| dc.date.available | 2026-07-07T09:48:41Z | |
| dc.description | Dynamical Coherent-Potential Approximation (CPA) to correlated electrons has been extended to a system with realistic Hamiltonian which consists of the first-principles tight-binding Linear Muffintin Orbital (LMTO) bands and intraatomic Coulomb interactions. Thermodynamic potential and self-consistent equations for Green function are obtained on the basis of the functional integral method and the harmonic approximation which neglects the mode-mode couplings between the dynamical potentials with different frequency. Numerical calculations have been performed for Fe and Ni within the 2nd-order dynamical corrections to the static approximation. The band narrowing of the quasiparticle states and the 6 eV satellite are obtained for Ni at finite temperatures. The theory leads to the Curie-Weiss law for both Fe and Ni. Calculated effective Bohr magneton numbers are 3.0 $μ_{\rm B}$ for Fe and 1.2 $μ_{\rm B}$ for Ni, explaining the experimental data. But calculated Curie temperatures are 2020 K for Fe and 1260 K for Ni, being still overestimated by a factor of two as compared with the experimental ones. Dynamical effects on electronic and magnetic properties are discussed by comparing with those in the static approximations. | |
| dc.description | To be published in J. Phys. Soc. Jpn. 77 No.9 (2008) | |
| dc.identifier | https://arxiv.org/abs/0807.0847 | |
| dc.identifier | http://arxiv.org/abs/0807.0847 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/164308 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.subject | Materials Science | |
| dc.title | Dynamical CPA and Tight-Binding LMTO Approach to Correlated Electron System | |
| dc.type | text |