Global phase diagram and momentum distribution of single-particle excitations in Kondo insulators

J. H. Pixley, Rong Yu, Silke Paschen, and Qimiao Si
Phys. Rev. B 98, 085110 – Published 7 August 2018
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Abstract

Kondo insulators are emerging as a simplified setting to study both magnetic and insulator-to-metal quantum phase transitions. Here, we study the half-filled Anderson lattice model defined on a magnetically frustrated Shastry-Sutherland geometry. We determine a “global” phase diagram that applies to both the local-moment and intermediate-valence regimes. This provides the theoretical basis for understanding how tuning a Kondo insulator by external parameters can close its hybridization gap, liberate the local-moment spins from the conduction electrons, and lead to a magnetically correlated metal. We also calculate the momentum distribution of the single-particle excitations in the Kondo insulating state, and show how Fermi-surface-like features emerge as a precursor to the actual Fermi surfaces of the Kondo-destroyed metals. The implications for an incipient Fermi surface and quantum phase transitions of Kondo insulators including SmB6 are discussed.

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  • Received 23 September 2015
  • Revised 10 June 2016

DOI:https://doi.org/10.1103/PhysRevB.98.085110

©2018 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

J. H. Pixley1,2, Rong Yu3, Silke Paschen4, and Qimiao Si5

  • 1Department of Physics and Astronomy, Center for Materials Theory, Rutgers University, Piscataway, NJ 08854, USA
  • 2Condensed Matter Theory Center and Joint Quantum Institute, Department of Physics, University of Maryland, College Park, Maryland 20742-4111, USA
  • 3Department of Physics, Renmin University of China, Beijing 100872, China
  • 4Institute of Solid State Physics, Vienna University of Technology, Wiedner Hauptstraße 8-10, 1040 Vienna, Austria
  • 5Department of Physics & Astronomy, Rice University, Houston, Texas 77005, USA

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Issue

Vol. 98, Iss. 8 — 15 August 2018

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