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arXiv:2404.08099 · Physical review. B./Physical review. B

Comparing quantum fluctuations in the spin- 1 2 and spin-1 XXZ Heisenberg models on the square and honeycomb lattices

Masahiro Kadosawa, Masaaki Nakamura, Y. Ohta, Satoshi Nishimoto

Published Oct 10, 2024• 6 citations
arXivHTMLPDF

Abstract

We present a detailed investigation of the XXZ Heisenberg model for spin-$1/2$ and spin-1 systems on square and honeycomb lattices. Utilizing the density-matrix renormalization group method, complemented by spiral boundary conditions (SBCs) for mapping two-dimensional (2D) clusters onto one-dimensional chains, we meticulously explore the evolution of staggered magnetization and spin gaps across a broad spectrum of easy-axis anisotropies. Our study reveals that despite the lower site coordination number of the honeycomb lattice, which intuitively suggests increased quantum fluctuations in its N\'eel phase compared to the square lattice, the staggered magnetization in the honeycomb structure exhibits only a marginal reduction. Furthermore, our analysis demonstrates that the dependence of staggered magnetization on the XXZ anisotropy $\mathrm{\ensuremath{\Delta}}$, except in close proximity to $\mathrm{\ensuremath{\Delta}}=1$, aligns with series expansion predictions up to the 12th order. Notably, for the $S=1/2$ honeycomb lattice, deviations from the 10th-order series expansion predictions near the isotropic Heisenberg limit emphasize the critical influence of quantum fluctuations on the spin excitation in its N\'eel state. Additionally, our findings are numerically consistent with the singular behavior of the spin gap near the isotropic Heisenberg limit as forecasted by spin-wave theory. The successful implementation of SBCs marks a methodological advancement, streamlining the computational complexity involved in analyzing 2D models and paving the way for more precise determinations of physical properties in complex lattice systems.

DOI
10.1103/physrevb.110.134418

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We present a detailed investigation of the XXZ Heisenberg model for spin-1/21/21/2 and spin-1 systems on square and honeycomb lattices. Utilizing the density-matrix renormalization group method, complemented by spiral boundary conditions (SBCs) for mapping two-dimensional (2D) clusters onto one-dimensional chains, we meticulously explore the evolution of staggered magnetization and spin gaps across a broad spectrum of easy-axis anisotropies. Our study reveals that despite the lower site coordination number of the honeycomb lattice, which intuitively suggests increased quantum fluctuations in its N'eel phase compared to the square lattice, the staggered magnetization in the honeycomb structure exhibits only a marginal reduction. Furthermore, our analysis demonstrates that the dependence of staggered magnetization on the XXZ anisotropy \ensuremathΔ\mathrm{\ensuremath{\Delta}}\ensuremathΔ, except in close proximity to \ensuremathΔ=1\mathrm{\ensuremath{\Delta}}=1\ensuremathΔ=1, aligns with series expansion predictions up to the 12th order. Notably, for the S=1/2S=1/2S=1/2 honeycomb lattice, deviations from the 10th-order series expansion predictions near the isotropic Heisenberg limit emphasize the critical influence of quantum fluctuations on the spin excitation in its N'eel state. Additionally, our findings are numerically consistent with the singular behavior of the spin gap near the isotropic Heisenberg limit as forecasted by spin-wave theory. The successful implementation of SBCs marks a methodological advancement, streamlining the computational complexity involved in analyzing 2D models and paving the way for more precise determinations of physical properties in complex lattice systems.
We propose an efficient numerical method to obtain local order parameter in two-dimensional systems using spiral boundary conditions. As a benchmark, we first estimate the magnitude of staggered magnetization for the S=1/2S=1/2S=1/2 XXZ Heisenberg model on a square lattice in the whole range of the XXZ anisotropy by density-matrix renormalization group technique. The validity of our method is confirmed by comparing our results with the previous analytical and numerical studies. Then, as further demonstration, we apply our method to obtain the staggered magnetization for the higher-spin cases from S=1S=1S=1 to S=6S=6S=6. The accuracy of the obtained results is validated using the series expansion and the spin-wave theory.
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We study the ground state of the 1D Kitaev-Heisenberg (KH) model using the density-matrix renormalization group and Lanczos exact diagonalization methods. We obtain a rich ground-state phase diagram as a function of the ratio between Heisenberg (J = cosϕ) and Kitaev (K = sinϕ) interactions. Depending on the ratio, the system exhibits four long-range ordered states: ferromagnetic-z, ferromagnetic-xy, staggered-xy, Néel-z, and two liquid states: Tomonaga-Luttinger liquid and spiral-xy. The two Kitaev points ϕ=π2 and φ=3π2 are singular. The ϕ-dependent phase diagram is similar to that for the 2D honeycomb-lattice KH model. Remarkably, all the ordered states of the honeycomb-lattice KH model can be interpreted in terms of the coupled KH chains. We also discuss the magnetic structure of the K-intercalated RuCl3, a potential Kitaev material, in the framework of the 1D KH model. Furthermore, we demonstrate that the low-lying excitations of the 1D KH Hamiltonian can be explained within the combination of the known six-vertex model and spin-wave theory.
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