Inorg Chem. 2019 Sep 16;58(18):11941-11948. doi: 10.1021/acs.inorgchem.9b01110. Epub 2019 Aug 8.
Kagomé lattice magnets have emerged as a versatile platform on which to discover and explore the underlying physics of quantum-spin liquids and related states of matter, although experimental examples of ideal kagomé lattices remain rare. Here we report that NaTiCl is an ideal realization of an insulating = 1 kagomé magnet. This material undergoes a discrete two-step trimerization upon cooling, transforming from a centrosymmetric, paramagnetic high-temperature (HT) 3 phase to noncentrosymmetric, polar, and trimerized intermediate- (IT) and low-temperature (LT) 3 phases via two successive first-order phase transitions. Symmetry mode decomposition analysis shows that trimerization requires activation of the proper polar order parameter Γ and that this mode becomes active at the HT → IT phase transition. The magnitude of this order parameter approximately doubles at the IT → LT transition, with possible activation of a second polar mode, corresponding to Na and TiCl displacing layers toward each other, at the IT → LT transition. Specific heat measurements reveal comparable changes in entropy between the LT → IT transition, 18.6(1.0) J (mol of f.u.) K, and the IT → LT transition, 16.8(1.0) J (mol of f.u.) K, demonstrating loss of the magnetic degrees of freedom and constraining possible models for the magnetic and electronic structures of the IT and LT phases. Thus, NaTiCl demonstrates a novel mechanism to obtain polar structures driven by geometrically frustrated lattices and metal-metal bonding and highlights the rich physics arising from kagomé lattice materials.
菱方晶格磁体已成为发现和探索量子自旋液体和相关物质状态的基本物理性质的通用平台,尽管理想菱方晶格的实验实例仍然很少。在这里,我们报告 NaTiCl 是绝缘 = 1 菱方磁体的理想实现。该材料在冷却时经历离散的两步三聚化,通过两个连续的一级相变从中心对称、顺磁高温 (HT) 3 相转变为非中心对称、极性和三聚体化的中间 (IT) 和低温 (LT) 3 相。对称模态分解分析表明三聚化需要激活适当的极有序参数 Γ,并且该模态在 HT → IT 相变时变得活跃。该有序参数的幅度在 IT → LT 相变时大约增加一倍,可能在 IT → LT 相变时激活第二个极性模态,对应于 Na 和 TiCl 相互朝向对方的层位移。比热测量显示 LT → IT 转变和 IT → LT 转变之间的熵发生相当大的变化,分别为 18.6(1.0) J (mol 的 f.u.) K 和 16.8(1.0) J (mol 的 f.u.) K,证明了磁自由度的丧失,并限制了 IT 和 LT 相的磁和电子结构的可能模型。因此,NaTiCl 展示了一种由几何上受挫的晶格和金属-金属键驱动获得极性结构的新机制,并突出了菱方晶格材料所带来的丰富物理性质。