Abstract

We use a recently developed interpretable and unsupervised machine-learning method, the tensorial kernel support vector machine (TK-SVM), to investigate the low-temperature classical phase diagram of a generalized Heisenberg-Kitaev-$\Gamma$ ($J$-$K$-$\Gamma$) model on a honeycomb lattice. Aside from reproducing phases reported by previous quantum and classical studies, our machine finds a hitherto missed nested zigzag-stripy order and establishes the robustness of a recently identified modulated $S_3 \times Z_3$ phase, which emerges through the competition between the Kitaev and $\Gamma$ spin liquids, against Heisenberg interactions. The results imply that, in the restricted parameter space spanned by the three primary exchange interactions -- $J$, $K$, and $\Gamma$, the representative Kitaev material $\alpha$-${\rm RuCl}_3$ lies close to the boundaries of several phases, including a simple ferromagnet, the unconventional $S_3 \times Z_3$ and nested zigzag-stripy magnets. A zigzag order is stabilized by a finite $\Gamma^{\prime}$ and/or $J_3$ term, whereas the four magnetic orders may compete in particular if $\Gamma^{\prime}$ is anti-ferromagnetic.

Highlights

  • Machine learning (ML) is quickly developing into a powerful tool in modern day physics research [1,2]

  • Aside from reproducing phases reported by previous quantum and classical studies, our machine finds a hitherto missed nested zigzag-stripy order and establishes the robustness of a recently identified modulated S3 × Z3 phase, which emerges through the competition between the Kitaev and spin liquids, against Heisenberg interactions

  • We focus on the machine-learned phase diagram for the pure Heisenberg-Kitaev- model and save the discussion on the effects of the and J3 terms for Sec

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Summary

INTRODUCTION

Machine learning (ML) is quickly developing into a powerful tool in modern day physics research [1,2]. We use our recently developed tensorialkernel support vector machine (TK-SVM) [56,57,58] to investigate the phase diagram of a generalized Heisenberg-Kitaevmodel on a honeycomb lattice This method is interpretable and unsupervised, equipped with a tensorial kernel and graph partitioning. Heisenberg-Kitaev- (J-K- ) model as well as the effect of the and third-nearest-neighbor Heisenberg (J3) terms, which are subleading exchange terms commonly encountered in the class of Kitaev materials From our findings it follows that in the parameter space spanned by J, K, and , the representative Kitaev material α-RuCl3 lies close to several competing phases, including a hitherto missed nested zigzag-stripy magnet, a previously identified S3 × Z3 magnet, a ferromagnet, and a possibly correlated paramagnet (Sec. III). A brief summary of TK-SVM and details about the training procedure and Monte Carlo simulations are provided in Appendixes

HONEYCOMB J-K- - -J3 Model
J-K- PHASE DIAGRAM
Finite
Finite J3 and
IMPLICATION TO MATERIALS
SUMMARY
Decision function
Graph partitioning
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