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  • Letter
  • Open Access

Coexisting Kondo hybridization and itinerant f-electron ferromagnetism in UGe2

Ioannis Giannakis1, Divyanshi Sar1, Joel Friedman1, Chang-Jong Kang2,3, Marc Janoschek4,*, Pinaki Das4,†, Eric D. Bauer4, Gabriel Kotliar2,5, and Pegor Aynajian1,‡

  • 1Department of Physics, Applied Physics and Astronomy, Binghamton University, Binghamton, New York 13902, USA
  • 2Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854, USA
  • 3Department of Physics, Chungnam National University, Daejeon 34134, South Korea
  • 4Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
  • 5Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA

  • *Present address: Laboratory for Neutron and Muon Instrumentation, Paul Scherrer Institute, Villigen PSI, Switzerland.
  • †Present address: Advanced Photon Source, Argonne National Laboratory, 9700 S. Cass Ave, Lemont, IL 60439.
  • ‡Corresponding author: aynajian@binghamton.edu

Phys. Rev. Research 4, L022030 – Published 6 May, 2022

DOI: https://doi.org/10.1103/PhysRevResearch.4.L022030

Abstract

Kondo hybridization in partially filled f-electron systems conveys a significant amount of electronic states sharply near the Fermi energy leading to various instabilities from superconductivity to exotic electronic orders. UGe2 is a 5f heavy fermion system, where the Kondo hybridization is interrupted by the formation of two ferromagnetic phases below a second order transition Tc∼52K and a crossover transition Tx∼32K. These two ferromagnetic phases are concomitantly related to a spin-triplet superconductivity that only emerges and persists inside the magnetically ordered phase at high pressure. The origin of the two ferromagnetic phases and how they form within a Kondo-lattice remain ambiguous. Using scanning tunneling microscopy and spectroscopy, we probe the spatial electronic states in the UGe2 as a function of temperature. We find a Kondo resonance and sharp 5f-electron states near the chemical potential that form at high temperatures above Tc in accordance with our density functionaltheory+Gutzwiller calculations. As temperature is lowered below Tc, the resonance narrows and eventually splits below Tx dumping itinerant f-electron spectral weight right at the Fermi energy. Our findings suggest a Stoner mechanism forming the highly polarized ferromagnetic phase below Tx that itself sets the stage for the emergence of unconventional superconductivity at high pressure.

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