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Quantum spin state stabilized by coupling with classical spins

H. Yamaguchi1,*, T. Okubo2, A. Matsuo3, T. Kawakami4, Y. Iwasaki5, T. Takahashi1, Y. Hosokoshi1, and K. Kindo3

  • 1Department of Physics, Osaka Metropolitan University, Osaka 599-8531, Japan
  • 2Department of Physics, the University of Tokyo, Tokyo 113-0033, Japan
  • 3Institute for Solid State Physics, the University of Tokyo, Chiba 277-8581, Japan
  • 4Department of Chemistry, Osaka University, Toyonaka, Osaka 560-0043, Japan
  • 5Department of Physics, College of Humanities and Sciences, Nihon University, Tokyo 156-8550, Japan

  • *Corresponding author: h_yamaguchi@omu.ac.jp

Phys. Rev. B 109, L100404 – Published 15 March, 2024

DOI: https://doi.org/10.1103/PhysRevB.109.L100404

Abstract

We introduce a model compound featuring a spin-1/2 frustrated square lattice partially coupled by spin-5/2. A significant magnetization plateau exceeding 60 T could be observed, indicating a quantum state formed by S=1/2 spins in the square lattice. The remaining S=5/2 spins exhibited paramagnetic behavior in the low-field regions. The numerical analysis confirmed that the observed quantum state is a many-body entangled state based on the dominant antiferromagnetic interactions and is strongly stabilized by coupling with spin-5/2. The stabilization of this quantum state can be attributed to a compensation effect similar to magnetic field-induced superconductivity, which serves as a strategy to control the stability of quantum spin states in magnetic fields.

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