Imaging the itinerant-to-localized transmutation of electrons across the metal-to-insulator transition in VO
arXiv:2207.04287 · doi:10.1126/sciadv.abj1164
Abstract
In solids, strong repulsion between electrons can inhibit their movement and result in a "Mott" metal-to-insulator transition (MIT), a fundamental phenomenon whose understanding has remained a challenge for over 50 years. A key issue is how the wave-like itinerant electrons change into a localized-like state due to increased interactions. However, observing the MIT in terms of the energy- and momentum-resolved electronic structure of the system, the only direct way to probe both itinerant and localized states, has been elusive. Here we show, using angle-resolved photoemission spectroscopy (ARPES), that in VO the temperature-induced MIT is characterized by the progressive disappearance of its itinerant conduction band, without any change in its energy-momentum dispersion, and the simultaneous shift to larger binding energies of a quasi-localized state initially located near the Fermi level.
Main Text (4 figures) and Supplementary Information (12 figures)
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Cited by in corpus (6)
- The fate of quasiparticles at high-temperature
- Disentangling structural and electronic properties in VO thin films: a genuine non-symmetry breaking Mott transition
- Electronic band structure of Ti2O3 thin films studied by angle-resolved photoemission spectroscopy
- Interface-induced collective phase transition in VO2-based bilayers studied by layer selective spectroscopy
- Self-Consistent Coulomb Interactions from Constrained Dynamical Mean-Field Theory
- Confinement-Induced Isosymmetric Metal-Insulator Transition in Ultrathin Epitaxial V2O3 Films