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Competing magnetic and topological orders in the spin-1 Kitaev-Heisenberg chain with single-ion anisotropy

Sahinur Reja1 and Satoshi Nishimoto2,3

Phys. Rev. B 114, 084406 – Published 10 August, 2026

DOI: https://doi.org/10.1103/z6xd-4697

Abstract

We investigate the ground-state phase diagram of the spin-1 Kitaev–Heisenberg (KH) chain in the presence of uniaxial single-ion anisotropy Dz using the density-matrix renormalization-group method. The relative strength of the Heisenberg and Kitaev interactions is parametrized by a coupling angle ϕ, defined by J=cosϕ and K=sinϕ. By combining energy-based diagnostics with finite-size extrapolations of order parameters and correlation functions, we obtain a comprehensive phase diagram as a function of ϕ and Dz. The phase diagram contains ferromagnetic and Néel ordered phases, collinear states with four-site spin modulation, magnetically disordered or critical regimes, two Kitaev-dominated spin-liquid-like regions, and a topological Haldane phase near the Heisenberg limit. We find that the Kitaev-dominated disordered regions acquire finite parameter widths in the spin-1 model, whereas the Haldane phase is fragile against Kitaev-type anisotropy, especially for Dz<0. Positive Dz generally suppresses magnetic order and expands nonmagnetic regimes, while negative Dz enhances Ising-like magnetic order. At Dz=0, we also identify an exactly solvable point at tanϕ=−2(ϕ/π≃1.6476), which gives rise to a first-order transition between the Néel-z state and a four-site collinear state. We further contrast these findings with the spin-1/2 KH chain and with the spin-1 honeycomb KH model, highlighting the distinct roles of single-ion anisotropy and dimensionality in Kitaev-type magnets.

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