Author
Listed:
- Takeshi Kondo
(ISSP, University of Tokyo)
- M. Nakayama
(ISSP, University of Tokyo)
- R. Chen
(University of California
University of California
Molecular Foundry, Lawrence Berkeley National Laboratory)
- J. J. Ishikawa
(ISSP, University of Tokyo)
- E.-G. Moon
(University of California
Korea Advanced Institute of Science and Technology)
- T. Yamamoto
(ISSP, University of Tokyo)
- Y. Ota
(ISSP, University of Tokyo)
- W. Malaeb
(ISSP, University of Tokyo
Faculty of Science, Beirut Arab University, P. O. Box 11-5020)
- H. Kanai
(ISSP, University of Tokyo)
- Y. Nakashima
(ISSP, University of Tokyo)
- Y. Ishida
(ISSP, University of Tokyo)
- R. Yoshida
(ISSP, University of Tokyo)
- H. Yamamoto
(ISSP, University of Tokyo)
- M. Matsunami
(UVSOR Facility, Institute for Molecular Science
Energy Materials Laboratory, Toyota Technological Institute)
- S. Kimura
(UVSOR Facility, Institute for Molecular Science
Graduate School of Frontier Biosciences, Osaka University)
- N. Inami
(Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK))
- K. Ono
(Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK))
- H. Kumigashira
(Institute of Materials Structure Science, High Energy Accelerator Research Organization (KEK))
- S. Nakatsuji
(ISSP, University of Tokyo
PRESTO, Japan Science and Technology Agency (JST))
- L. Balents
(Kavli Institute for Theoretical Physics)
- S. Shin
(ISSP, University of Tokyo)
Abstract
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.
Suggested Citation
Takeshi Kondo & M. Nakayama & R. Chen & J. J. Ishikawa & E.-G. Moon & T. Yamamoto & Y. Ota & W. Malaeb & H. Kanai & Y. Nakashima & Y. Ishida & R. Yoshida & H. Yamamoto & M. Matsunami & S. Kimura & N. , 2015.
"Quadratic Fermi node in a 3D strongly correlated semimetal,"
Nature Communications, Nature, vol. 6(1), pages 1-8, December.
Handle:
RePEc:nat:natcom:v:6:y:2015:i:1:d:10.1038_ncomms10042
DOI: 10.1038/ncomms10042
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Citations
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Cited by:
- Lun-Hui Hu & Rui-Xing Zhang, 2023.
"Topological superconducting vortex from trivial electronic bands,"
Nature Communications, Nature, vol. 14(1), pages 1-10, December.
- Taiki Uehara & Takumi Ohtsuki & Masafumi Udagawa & Satoru Nakatsuji & Yo Machida, 2022.
"Phonon thermal Hall effect in a metallic spin ice,"
Nature Communications, Nature, vol. 13(1), pages 1-8, December.
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