2020/12/16 by Ze-Yi Song, Xiu-Cai Jiang, Yu-Zhong Zhang +1
Materials Science · Physics and Astronomy · #Advanced Condensed Matter Physics #Atomic orbital #Condensed matter physics #Coulomb #Coupling (piping) #Electron #Fermi level #Fermi liquid theory #Hubbard model #Magnetic and transport properties of perovskites and related materials #Materials science #Metal #Mott insulator #Mott transition #Physics #Physics of Superconductivity and Magnetism #Quantum mechanics #Spin–orbit interaction #Superconductivity #cond-mat.str-el
paper · pdf · doi:10.1103/physrevb.102.245124
published as Phys. Rev. B 102, 245124 (2020) · 12 pages, 8 figures
openalex publication_date 2020/12/16 · openalex created_date 2020/12/21 · arxiv created 2021/07/01 · arxiv updated 2021/07/02 · openalex updated_date 2026/08/05
We show that spin-orbit coupling (SOC) plays Janus-faced roles on the orbitally selective Mott transitions in a three-orbital Hubbard model with crystal field splitting at a specific filling of 2/3, which is a minimal Hamiltonian for ruthenates. While the SOC favors the metallic state due to enhancement of orbital hybridization at smaller on-site Coulomb repulsions, it stabilizes the Mott-insulating state ascribed to the lifting of orbital degeneracies and enhancement of band polarizations at larger electronic interaction. Moreover, an orbitally selective non-Fermi liquid (OSNFL), where breakdown and retention of the Fermi liquid coexist in different orbitals, emerges between the orbitally selective Mott phase and the Fermi-liquid state. This novel state can be used to account for the exotic metallic behavior observed in 4d materials, such as Ca1.8Sr0.2RuO4, Ba2RuO4 under strain, and Sr2RuO4 under uniaxial pressure. We propose that orbitally selective Kondo breakdown may account for the OSNFL.