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Layer-controlled orbital-selective Mott transition in monolayer nickelate

Byungmin Sohn1,2,*,†, Minjae Kim3,4,*, Sangjae Lee1,*, Wenzheng Wei1, Juan Jiang1, Fengmiao Li5, Sergey Gorovikov6, Marta Zonno6, Tor Pedersen6 et al.

Sergey Zhdanovich6, Ying Liu7, Huikai Cheng7, Ke Zou5, Yu He1, Sohrab Ismail-Beigi1, Frederick J. Walker1, and Charles H. Ahn1,8

  • *These authors contributed equally to this work.
  • †Contact author: bsohn@skku.edu

Phys. Rev. Research 7, 043132 – Published 4 November, 2025

DOI: https://doi.org/10.1103/n92p-xrhl

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.

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