1. Imaging the itinerant-to-localized transmutation of electrons across the metal-to-insulator transition in V$_2$O$_3$
- Author
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Juan Trastoy, Franck Fortuna, Silke Biermann, Yoav Kalcheim, Patrick Le Fèvre, Ivan K. Schuller, Maximilian Thees, Hiroshi Kumigashira, Min Han Lee, Marcelo J. Rozenberg, Emmanouil Frantzeskakis, Koji Horiba, Alexandre Zimmers, Andrés F. Santander-Syro, Rosa Luca Bouwmeester, Emma David, Pedro H. Rezende-Gonçalves, Nicolás Vargas, Interfaces and Correlated Electron Systems, and MESA+ Institute
- Subjects
Materials science ,Photoemission spectroscopy ,Binding energy ,FOS: Physical sciences ,Angle-resolved photoemission spectroscopy ,Electronic structure ,Electron ,01 natural sciences ,010305 fluids & plasmas ,Metal ,symbols.namesake ,Condensed Matter - Strongly Correlated Electrons ,0103 physical sciences ,Dispersion (optics) ,Physical and Materials Sciences ,010306 general physics ,Condensed Matter::Quantum Gases ,Condensed Matter - Materials Science ,Multidisciplinary ,Condensed matter physics ,Strongly Correlated Electrons (cond-mat.str-el) ,Physics ,Fermi level ,Materials Science (cond-mat.mtrl-sci) ,SciAdv r-articles ,3. Good health ,visual_art ,symbols ,visual_art.visual_art_medium ,Condensed Matter::Strongly Correlated Electrons ,Research Article - Abstract
Description, This work shows how itinerant electrons localize due to increased interactions across the Mott metal-insulator transition., 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 V2O3, 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.
- Published
- 2022