Abstract
Motivated by recent structural data questioning the adequacy of the charge order (CO) or disorder picture for the Verwey transition (at ) in magnetite, we reinvestigate this issue within a new theoretical picture. Using the local density mean-field theory () method, we show that the nontrivial interplay between octahedral distortions and strong, multiorbital electronic correlations in the half-metallic state is a necessary ingredient for a proper quantitative understanding of the physical responses across . While weak CO is found to have very small effects on the low- spectral function, the low- charge gap and the resistivity jump across are quantitatively reproduced only upon inclusion of CO in the local spin density scheme. Our results strongly suggest that the Verwey transition is dominantly driven by multiorbital electronic correlations with associated Jahn-Teller distortions on the sublattice, and constitutes a nontrivial advance in attempts to understand the physics of .
- Received 12 June 2006
DOI:https://doi.org/10.1103/PhysRevB.74.064425
©2006 American Physical Society