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Disorder-induced topological phases in a two-dimensional Chern insulator with strong magnetic disorder

Devesh Vaish1,* and Michael Potthoff1,2,†

  • *Contact author: devesh.r.vaish@jyu.fi
  • †Contact author: michael.potthoff@uni-hamburg.de

Phys. Rev. Research 8, 023312 – Published 17 June, 2026

DOI: https://doi.org/10.1103/fjnq-k1wq

Abstract

Strong directional disorder in local magnetic moments coupled to a Chern insulator gives rise to topological phases that cannot be realized in any clean system and are therefore genuinely disorder driven. We demonstrate this in a spinful Qi-Wu-Zhang model of a two-dimensional Chern insulator coupled to disordered classical spins of unit length. The topological phase diagram is computed numerically using two complementary approaches: twisted boundary conditions and the topological Hamiltonian technique. Our results show that strong disorder can act as a fundamental topological mechanism rather than merely a perturbation. For strong exchange coupling, tuning the mass parameter reveals a transition between phases with different Chern numbers C. Remarkably, this transition is driven by zeros, rather than poles, of the disorder-averaged Green’s function crossing the chemical potential, and has no analog in any clean system. We further identify a strong-coupling phase with C=0 that is nonetheless topologically nontrivial, characterized by a distinct Chern number C(S)≠0 over the manifold of classical spin configurations. This phase is also disorder driven, as C(S)=0 in the clean limit.

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