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首页> 外文期刊>Materials Chemistry Frontiers >Field tunable magnetic transitions of CsCo2(MoO4)2(OH): a triangular chain structure with a frustrated geometry
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Field tunable magnetic transitions of CsCo2(MoO4)2(OH): a triangular chain structure with a frustrated geometry

机译:CsCo2(MoO4)2(OH)的磁场可调磁跃迁:具有受挫几何形状的三角链结构

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The sawtooth chain compound CsCo2(MoO4)2(OH) is a complex magnetic system and here, we present a comprehensive series of magnetic and neutron scattering measurements to determine its magnetic phase diagram. The magnetic properties of CsCo2(MoO4)2(OH) exhibit a strong coupling to the crystal lattice and its magnetic ground state can be easily manipulated by applied magnetic fields. There are two unique Co2+ ions, base and vertex, with Jbb and Jbv magnetic exchange. The magnetism is highly anisotropic with the b-axis (chain) along the easy axis and the material orders antiferromagnetically at TN = 5 K. There are two successive metamagnetic transitions, the first at Hc1 = 0.2 kOe into a ferrimagnetic structure, and the other at Hc2 = 20 kOe to a ferromagnetic phase. Heat capacity measurements in various fields support the metamagnetic phase transformations, and the magnetic entropy value is intermediate between S = 3/2 and 1/2 states. The zero field antiferromagnetic phase contains vertex magnetic vectors (Co(1)) aligned parallel to the b-axis, while the base vectors (Co(2)) are canted by 34° and aligned in an opposite direction to the vertex vectors. The spins in parallel adjacent chains align in opposite directions, creating an overall antiferromagnetic structure. At a 3 kOe applied magnetic field, adjacent chains flip by 180° to generate a ferrimagnetic phase. An increase in field gradually induces the Co(1) moment to rotate along the b-axis and align in the same direction with Co(2) generating a ferromagnetic structure. The antiferromagnetic exchange parameters are calculated to be Jbb = 0.028 meV and Jbv = 0.13 meV, while the interchain exchange parameter is considerably weaker at Jch = (0.0047/Nch) meV. Our results demonstrate that the CsCo2(MoO4)2(OH) is a promising candidate to study new physics associated with sawtooth chain magnetism and it encourages further theoretical studies as well as the synthesis of other sawtooth chain structures with different magnetic ions.
机译:锯齿链化合物CsCo2 (MoO4) 2(哦)复杂的磁系统,在这里,我们提出一个全面的一系列磁和中子散射测量,以确定其磁性相图。CsCo2 (MoO4) 2 (OH)表现出的强耦合晶格和磁基态能很容易被应用磁场。有两个独特的Co2 +离子,基地和顶点,与Jbb Jbv磁交换。与b轴高度各向异性(链)沿易轴和材料订单antiferromagnetically TN = 5 K。连续metamagnetic转换,第一用盐酸= 0.2 kOe成亚铁磁性结构,另一个在Hc2 = 20 kOe铁磁阶段。字段支持metamagnetic阶段转换和磁熵值介于S = 3/2和1/2。包含零场反铁磁性的阶段顶点磁向量(Co(1)平行对齐b轴,而基向量(Co (2))34°和一致的倾斜的相反顶点向量方向。平行相邻链排列相反方向,创建一个整体的反铁磁性的结构。生成一个相邻链翻转180°亚铁磁的阶段。逐渐引起Co(1)旋转沿着b轴对齐在同一个方向有限公司(2)生成一个铁磁结构。反铁磁性的交易所参数计算Jbb = 0.028兆电子伏,Jbv = 0.13兆电子伏,而跨链交换参数相当弱Jch = (0.0047 / Nch)兆电子伏。我们的研究结果表明,CsCo2 (MoO4) 2(哦)是一种很有前途的候选人为研究新的物理吗与锯齿链磁性和它联系在一起鼓励进一步的理论研究以及其他锯齿链结构的合成不同的磁性离子。

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