Quadratic Fermi node in a 3D strongly correlated semimetal

Strong spin–orbit coupling fosters exotic electronic states such as topological insulators and superconductors, but the combination of strong spin–orbit and strong electron–electron interactions is just beginning to be understood. Central to this emerging area are the 5d transition metal iridium oxi...

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Bibliographic Details
Main Author: Kondo, Takeshi (author)
Other Authors: Nakayama, M. (author), Chen, R. (author), Ishikawa, J. J. (author), Moon, E.-G. (author), Yamamoto, T. (author), Ota, Y. (author), Malaeb, W. (author), Kanai, H. (author), Nakashima, Y. (author), Ishida, Y. (author)
Format: article
Published: 2015
Online Access:http://hdl.handle.net/10725/16683
https://doi.org/10.1038/ncomms10042
http://libraries.lau.edu.lb/research/laur/terms-of-use/articles.php
https://www.nature.com/articles/ncomms10042
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Summary:Strong spin–orbit coupling fosters exotic electronic states such as topological insulators and superconductors, but the combination of strong spin–orbit and strong electron–electron interactions is just beginning to be understood. Central to this emerging area are the 5d transition metal iridium oxides. Here, in the pyrochlore iridate Pr2Ir2O7, we identify a non-trivial state with a single-point Fermi node protected by cubic and time-reversal symmetries, using a combination of angle-resolved photoemission spectroscopy and first-principles calculations. Owing to its quadratic dispersion, the unique coincidence of four degenerate states at the Fermi energy, and strong Coulomb interactions, non-Fermi liquid behaviour is predicted, for which we observe some evidence. Our discovery implies that Pr2Ir2O7 is a parent state that can be manipulated to produce other strongly correlated topological phases, such as topological Mott insulator, Weyl semimetal, and quantum spin and anomalous Hall states.