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Layer-controlled orbital-selective Mott transition in monolayer nickelate

  • Byungmin Sohn*
  • , Minjae Kim
  • , Sangjae Lee
  • , Wenzheng Wei
  • , Juan Jiang
  • , Fengmiao Li
  • , Sergey Gorovikov
  • , Marta Zonno
  • , Tor Pedersen
  • , Sergey Zhdanovich
  • , Ying Liu
  • , Huikai Cheng
  • , Ke Zou
  • , Yu He
  • , Sohrab Ismail-Beigi
  • , Frederick J. Walker
  • , Charles H. Ahn
  • *Corresponding author for this work
  • Yale University
  • Sungkyunkwan University
  • University of British Columbia
  • University of Saskatchewan
  • Thermo Fisher Scientific, Inc.

Research output: Contribution to journalJournal articlepeer-review

Abstract

Dimensionality and electronic correlations are crucial elements of many quantum material properties. An example is the change of the electronic structure accompanied by the loss of quasiparticles when a metal is reduced from three dimensions to a lower dimension, where the Coulomb interaction between carriers becomes poorly screened. Here, using angle-resolved photoemission spectroscopy, we report an orbital-selective decoherence of spectral density in the perovskite nickelate LaNiO3 toward the monolayer limit. The spectral weight of the dz2 band vanishes much faster than that of the dx2-y2 band as the thickness of the LaNiO3 layer is decreased to a single unit cell, indicating a stronger correlation effect for the former upon dimensional confinement. Dynamical mean-field theory calculations show an orbital-selective Mott transition largely due to the localization of dz2 electrons along the c axis in the monolayer limit. This orbital-selective correlation effect underpins many macroscopic properties of nickelates, such as metal-to-insulator transition and superconductivity, where most theories are built upon a dx2-y2-dz2 two-band model.

Original languageEnglish
Article number043132
JournalPhysical Review Research
Volume7
Issue number4
DOIs
StatePublished - 2025.10

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