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  • Letter

Scaling of the disorder operator at (3+1)D O(3) quantum criticality

Xuyang Liang1, Xiao-Chuan Wu2,3,*, Zenan Liu4,5,6, Zhe Wang5,6, Zheng Yan5,6,†, and Dao-Xin Yao1,‡

  • 1Guangdong Provincial Key Laboratory of Magnetoelectric Physics and Devices, State Key Laboratory of Optoelectronic Materials and Technologies, Institute of Neutron Science and Technology, School of Physics, Sun Yat-Sen University, Guangzhou 510275, China
  • 2Department of Physics, Princeton University, Princeton, New Jersey 08544, USA
  • 3Leinweber Institute for Theoretical Physics, University of Chicago, Chicago, Illinois 60637, USA
  • 4Department of Physics, South China University of Technology, Guangzhou 510640, China
  • 5Department of Physics, School of Science and Research Center for Industries of the Future, Westlake University, Hangzhou 310030, China
  • 6Institute of Natural Sciences, Westlake Institute for Advanced Study, Hangzhou 310024, China

  • *Contact author: xw0618@princeton.edu
  • †Contact author: zhengyan@westlake.edu.cn
  • ‡Contact author: yaodaox@mail.sysu.edu.cn

Phys. Rev. B 114, L111104 – Published 10 August, 2026

DOI: https://doi.org/10.1103/8nq1-q47x

Abstract

The disorder operator, as an easily measured nonlocal observable, displays great potential in detecting intrinsic information of field theories. It has been systematically studied in one- and two-dimensional (1D and 2D) quantum systems, while the knowledge of 3D is still limited. The disorder operator associated with U(1) global symmetry exhibits rich geometric dependence on the shape of the spatial region at a quantum critical point, meanwhile, (3+1)D is the upper critical dimension for O(N) criticality, both of which pose a challenge for exploring the disorder operator in high dimensions. In this Letter, we investigate the scaling behaviors of disorder operators in (3+1)D O(3) models through a large-scale quantum Monte Carlo simulation combined with a theoretical analysis. Although the upper critical dimension introduces logarithmic corrections in correlations, we analytically prove and numerically demonstrate that the corrections do not modify the universal trihedral-corner contribution of the disorder operator. The universal contributions, such as the current central charge, have been revealed in our calculation, which establishes a concrete link between lattice simulations and continuum field theory. This work opens promising directions for the experimental and numerical exploration of universal properties at quantum critical points in (3+1)D models.

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