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nabokoite家族高阻挫装饰型正方形kagomé晶格反铁磁体中的共线与非共线反铁磁有序

Collinear and noncollinear antiferromagnetic ordering in a highly frustrated decorated square kagomé lattice antiferromagnets of the nabokoite family

V. N. Glazkov, Ya V. Rebrov, M. A. Dubovitskii, M. M. Markina, K. V. Zakharov, A. F. Murtazoev, P. S. Berdonosov, A. N. Vasiliev

arXiv 2608.29330首次发表:更新:

发表机构

P.L. Kapitza Institute for Physical Problems, RAS; National Research University “HSE”; M.V. Lomonosov Moscow State University; National University of Science and Technology “MISiS”(俄罗斯科学院P.L.卡皮察物理问题研究所; 国立研究型大学高等经济大学; 莫斯科罗蒙诺索夫国立大学; 国立科技大学米西斯大学)

机构由 AI 辅助整理,请以论文原文为准。

AI 中文总结

本研究通过实验与建模,揭示nabokoite家族中轻、重碱金属化合物的磁有序存在质的差异,重碱金属呈共线反铁磁有序,轻碱金属经铁电相变后形成两步相变的非共线磁有序。

AI 中文摘要

nabokoite家族化合物ACu$_7$(TeO$_4$)(SO$_4$)$_5$X(A=Na、K、Rb、Cs;X=Cl、Br)包含由额外层间磁性离子修饰的阻挫二维正方形kagomé晶格层。本研究通过多频电子自旋共振光谱及热力学测量(比热、磁化强度、介电常数)探究nabokoite的磁有序。研究表明,轻碱金属离子(K、Na)化合物与重碱金属离子(Rb、Cs)化合物的低温基态选择存在质的差异:重碱金属nabokoite呈现具有易轴各向异性的常规共线反铁磁模式,其有序反铁磁态参数在整个重碱金属亚族中非常接近;轻碱金属nabokoite则展现出更为复杂的有序态形成路径:首先在25-90K发生铁电相变以解除阻挫,从而预准备低温有序;随后通过两步相变形成异常非共线磁有序,第一步相变温度T$_{c1}$≃5-6K,第二步相变温度T$_{c2}$≃3-4K,非共线有序通过特征性非拉莫尔反铁磁共振模式的观测得到证实。轻碱金属nabokoite的自旋动力学以三个零场磁振子能隙和两个自旋重取向场为特征,不同化合物的磁振子能隙与临界场值差异显著。结合nabokoite结构的金字塔结构块的有限尺寸团簇建模表明,nabokoite交换耦合参数与金字塔结构块不同量子基态边界的临界接近度,可能是轻、重碱金属nabokoite选择质的不同有序态的关键。

英文摘要

Nabokoite family compounds ACu$_7$(TeO$_4$)(SO4)$_5$X (A=Na, K, Rb, Cs; X=Cl, Br) host frustrated 2D square kagom'{e} lattice layers decorated by additional inter-layer magnetic ions. We study magnetic order in nabokoites with multi-frequency electron spin resonance spectroscopy and thermodynamic measurement (specific heat, magnetization and dielectric permittivity). Our study reveals that the choice of the low-temperature ground state is qualitatively different in light-alkali-ion (K, Na) and heavy-alkali-ion (Rb, Cs) compounds. Heavy-alkali-ion nabokoites order in conventional collinear antiferromagnetic pattern with easy-axis anisotropy. The parameters of the ordered antiferromagnetic state are very close for all heavy-alkali-ion subfamily. Light-alkali-ion members of nabokoite family demonstrate much more complicated route to the ordered state: firstly, a ferroelectric transition at 25-90K lifts the frustration and thus pre-cooks the low-temperature ordering; secondly, an unusual noncollinear magnetic order develops via two-step phase transition with first transition temperature $T_{c1}\simeq 5-6$K and the second transition at $T_{c2}\simeq 3-4$K. Noncollinear order is evidenced by observation of characteristic non-Larmor antiferromagnetic resonance mode. Spin dynamics of light-alkali-ion nabokoites is characterized by three zero-field magnon gaps and two spin-reorientation fields, the values of magnon gaps and critical fields are quite different for different compounds. The finite-size cluster modeling of pyramidal structural block of nabokoite structure combined suggests that the critical closeness of the nabokoite exchange coupling parameters to the border-line between the different quantum ground state of pyramidal building block of nabokoite structure could be the clue to the choice of qualitatively different ordered state in light- and heavy-alkali-ion nabokoites.

Comments22 pages, 16 figures

论文原文

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