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Condensed Matter > Strongly Correlated Electrons

Title: Unveiling the phase diagram of a bond-alternating spin-$\frac12$ $K$-$Γ$ chain

Abstract: The key to unraveling intriguing phenomena observed in various Kitaev materials lies in understanding the interplay of Kitaev ($K$) interaction and a symmetric off-diagonal $\Gamma$ interaction. To provide insight into the challenging problems, we study the quantum phase diagram of a bond-alternating spin-$1/2$ $g_x$-$g_y$ $K$-$\Gamma$ chain by density-matrix renormalization group method where $g_x$ and $g_y$ are the bond strengths of the odd and even bonds, respectively. The phase diagram is dominated by even-Haldane ($g_x > g_y$) and odd-Haldane ($g_x < g_y$) phases where the former is topologically trivial while the latter is a symmetry-protected topological phase. Near the antiferromagnetic Kitaev limit, there are two gapped $A_x$ and $A_y$ phases characterized by distinct nonlocal string correlators. In contrast, the isotropic ferromagnetic (FM) Kitaev point serves as a multicritical point where two topological phase transitions meet. The remaining part of the phase diagram contains three symmetry-breaking magnetic phases. One is a six-fold degenerate FM$_{U_6}$ phase where all the spins are parallel to one of the $\pm \hat{x}$, $\pm \hat{y}$, and $\pm \hat{z}$ axes in a six-site spin rotated basis, while the other two have more complex spin structures with all the three spin components being finite. Existence of a rank-2 spin-nematic ordering in the latter is also discussed.
Comments: 12+4 pages, 14+4 figures. For a subsequent spin-1 analogy, see arXiv:2104.10725
Subjects: Strongly Correlated Electrons (cond-mat.str-el)
Journal reference: Phys. Rev. B 103, 144423 (2021)
DOI: 10.1103/PhysRevB.103.144423
Cite as: arXiv:2012.03382 [cond-mat.str-el]
  (or arXiv:2012.03382v2 [cond-mat.str-el] for this version)

Submission history

From: Qiang Luo [view email]
[v1] Sun, 6 Dec 2020 21:44:48 GMT (744kb,D)
[v2] Tue, 13 Jul 2021 22:03:20 GMT (771kb,D)

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