Ghosh Sayandeep, Joshi Deep Chandra, Pramanik Prativa, Jena Suchit K, Pittala Suresh, Sarkar Tapati, Seehra Mohindar S, Thota Subhash
Department of Physics, Indian Institute of Technology, Guwahati-781039, Assam, India.
Department of Materials Science and Engineering, Uppsala University, Box 534, SE-751 21 Uppsala, Sweden.
J Phys Condens Matter. 2020 Sep 8;32(48). doi: 10.1088/1361-648X/aba6a6.
Static and dynamic magnetic properties of normal spinel CoRuO= (Co)A[Co3+Ru3+]BO4are reported based on our investigations of the temperature (), magnetic field () and frequency () dependence of the ac-magnetic susceptibilities and dc-magnetization () covering the temperature range= 2 K-400 K and H up to 90 kOe. These investigations show that CoRuOexhibits an antiferromagnetic (AFM) transition at∼ 15.2 K, along with a spin-glass state at slightly lower temperature () near 14.2 K. It is argued thatis mainly governed by the ordering of the spins of Coions occupying the-site, whereas the exchange interaction between the Coions on the-site and randomly distributed Ruon the-site triggers the spin-glass phase, Coions on the-site being in the low-spin non-magnetic state. Analysis of measurements of(,) for
基于我们对交流磁化率和直流磁化强度在温度(T)、磁场(H)和频率(f)方面的依赖性的研究,报道了正常尖晶石CoRuO₄(Co)A[Co³⁺Ru³⁺]BO₄的静态和动态磁性,研究涵盖的温度范围为T = 2 K - 400 K,磁场高达90 kOe。这些研究表明,CoRuO₄在约15.2 K处表现出反铁磁(AFM)转变,同时在略低温度(T₀)约14.2 K附近存在自旋玻璃态。据认为,M主要由占据A位的Co离子的自旋有序性决定,而A位上的Co离子与B位上随机分布的Ru之间的交换相互作用引发了自旋玻璃相,A位上的Co离子处于低自旋非磁性状态。对T < T₀时χ(T,H)测量值的分析用于构建相图,结果表明T随H变化向低温移动,这符合自旋玻璃态的预期,而χ₀几乎与H无关。对于T > T₀,顺磁磁化率(χ)与T数据的分析符合修正的居里-外斯定律,χ = χ₀ + C /(T + θ),其中χ₀ = 0.0015 emu·mol⁻¹·Oe⁻¹,得到θ = 53 K,C = 2.16 emu·K·mol⁻¹·Oe⁻¹,后者得出有效磁矩μeff = 4.16 μB,与每个CoRuO₄预期的μeff = 4.24 μB值相当。利用该结果以及高温级数,估计了A位上Co之间的主导交换常数J / kB ∼ 6 K。对T₀附近的交流磁化率分析得出动态临界指数z = 5.2和微观自旋弛豫时间τ₀ ∼ 1.16 × 10⁻⁸ s,这是团簇自旋玻璃的特征,并且观察到的M(T)的时间依赖性支持了自旋玻璃态。对于场冷样品,低温下的大回线不对称以及巨大的交换偏置效应(约1.8 kOe)和矫顽力(约7 kOe)进一步支持了这种有趣尖晶石的混合磁相性质。在T₀以下观察到的负磁热效应被解释为是由于AFM和SG有序化。有人认为,在CoRuO₄中观察到的从T > T₀时的正磁热效应(MCE)到T < T₀时的逆MCE的变化(之前在其他系统中也有报道)与(∂M / ∂T)对T数据符号的变化有关。