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arXiv:2601.22924 · Physical review. B./Physical review. B

Spiral phase and phase diagram of the S = 1 2 XXZ model on the Shastry-Sutherland lattice

Zhengpeng Yuan, Muwei Wu, Dao‐Xin Yao, Han-Qing Wu

Published Apr 1, 2026• 0 citations
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Abstract

We investigate the ground-state phase diagram of the $S$=1/2 XXZ model on the two-dimensional Shastry-Sutherland lattice using exact diagonalization (ED), density-matrix renormalization group (DMRG), and cluster mean-field theory (CMFT) with DMRG as a solver. In the isotropic case ($Δ=1$), CMFT results reveal an intermediate empty plaquette (EP) phase that has a lower energy than the full plaquette (FP) phase. However, due to mean-field artifacts, CMFT alone is not suitable for accurately determining phase boundaries. Therefore, we combined three methods to map out the reliable phase diagram. Our calculations show that the EP phase narrows as $Δ$ deviates from unity and eventually vanishes. More importantly, we identify a spiral phase at small $Δ$, which has not been reported in previous studies. This phase is clearly captured by DMRG simulations on long cylindrical geometries. The competition between the EP, spiral, and $xy$-AFM phases near their boundaries provides a plausible explanation for the emergent spin-liquid-like behavior in RE$_2$Be$_2$GeO$_2$, while shedding new light on the role of XXZ anisotropy in the Shastry-Sutherland XXZ model.

DOI
10.1103/9ys7-hz3x

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We investigate the ground-state phase diagram of the SSS=1/2 XXZ model on the two-dimensional Shastry-Sutherland lattice using exact diagonalization (ED), density-matrix renormalization group (DMRG), and cluster mean-field theory (CMFT) with DMRG as a solver. In the isotropic case (Δ=1Δ=1Δ=1), CMFT results reveal an intermediate empty plaquette (EP) phase that has a lower energy than the full plaquette (FP) phase. However, due to mean-field artifacts, CMFT alone is not suitable for accurately determining phase boundaries. Therefore, we combined three methods to map out the reliable phase diagram. Our calculations show that the EP phase narrows as ΔΔΔ deviates from unity and eventually vanishes. More importantly, we identify a spiral phase at small ΔΔΔ, which has not been reported in previous studies. This phase is clearly captured by DMRG simulations on long cylindrical geometries. The competition between the EP, spiral, and xyxyxy-AFM phases near their boundaries provides a plausible explanation for the emergent spin-liquid-like behavior in RE2_22​Be2_22​GeO2_22​, while shedding new light on the role of XXZ anisotropy in the Shastry-Sutherland XXZ model.
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The ground state phase diagram of the Shastry-Sutherland model remains controversial. In particular, the nature of the transition between the plaquette valence bond solid (PVBS) phase and the Néel antiferromagnetic (AFM) phase is still under debate. While some studies suggest a direct transition between the two phases, others propose the existence of a narrow intermediate quantum spin liquid regime. To address this issue, we perform large-scale Density Matrix Renormalization Group calculations to determine the Néel AFM phase boundary in the Shastry-Sutherland model. By applying staggered boundary pinning fields and directly measuring the bulk staggered magnetization, and through systematic extrapolations with respect to truncation error as well as careful finite-size scaling, we find that the staggered magnetization remains finite across the controversial region 0.78≲J1/J2≤0.810.78 \lesssim J_{1}/J_{2} \leq 0.810.78≲J1​/J2​≤0.81, which was suggested to host a quantum spin liquid phase in some studies. Together with the previously established consensus placing the PVBS phase boundary at J1/J2≈0.78J_{1}/J_{2} \approx 0.78J1​/J2​≈0.78, these results provide evidence against the existence of an intermediate quantum spin liquid phase and support a direct PVBS--Néel AFM transition in the Shastry-Sutherland model.
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