首页> 外文期刊>International Journal of Quantum Chemistry >Unexpected Spin-Glass Behavior of the Mixed Sulfide-Selenide Chalcogenides TlCr_5S_(8-y)Se_y (y = 1-7) Mediated by the Nonmagnetic Sublattice
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Unexpected Spin-Glass Behavior of the Mixed Sulfide-Selenide Chalcogenides TlCr_5S_(8-y)Se_y (y = 1-7) Mediated by the Nonmagnetic Sublattice

机译:非磁性亚晶格介导的混合硫化物-硒化物硫族化物TlCr_5S_(8-y)Se_y(y = 1-7)的意外自旋玻璃行为

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Spin0glass behavior in the series TlCr_5S_(8-y)Se_y is mediated by the nonmagnetic anionic sublattice. The magnetic susceptibilities of compounds with 1 <- y <- 8 follow a Curie-Weiss law in the high temperature region above 300 K. As the Se content increases, the magnitude of the Weiss constant #theta# drastically decreases from about - 499(3) K for TlCr_5S_7Se to - 180(3) K for TlCr_5Se_8. Substitution of S by Se leads to structural alterations and stronger ferromagnetic exchange interactions according to the well-established Goodenough-Kanamori rules. In the low-temperature region, zero field cooled and field cooled susceptibility curves split below a characteristic freezing temperature T_f, which increases with rising Se content from 23 to 46 K for TlCr_5SeS_7 to TlCr_5Se_7S, respectively. Using an Ising spin model, the magnetic frustration and the observed spin-glass behavior can be explained by considering different ferromagnetic and antiferromagnetic exchange paths. Neutron diffraction patterns at 5 K show no long-range magnetic order. Analyses of broad humps of magnetic scattering in the diffraction patterns in terms of real space distribution functions show that the antiferromagnetic exchange becomes weaker at the expense of increasing ferromagnetic correlations between 120 and 5 K. Nonlinear changes of #theta#, T_f, and the effective magnetic moment per Cr(III) across the TlCr_5S_(8-y)Se_y series, but linear dependencies of T_f and #theta# on composition within the two regions 1 <- y <- 4 and 4 <- y <- 7 in the low and high temperature regimes, respectively, indicate that a critical Cr-Cr interatomic distance is reached at y #approx =#4.
机译:TlCr_5S_(8-y)Se_y系列中的Spin0glass行为是由非磁性阴离子亚晶格介导的。具有1 <-y <-8的化合物的磁化率在300 K以上的高温区域遵循居里·韦斯定律。随着Se含量的增加,Weiss常数#theta的幅度从大约-499()急剧降低。 3)对于TlCr_5S_7Se为K,对于-TlCr_5Se_8为180(3)K。根据公认的Goodenough-Kanamori规则,Se取代S会导致结构改变和更强的铁磁交换相互作用。在低温区域,零磁场冷却和磁场冷却的磁化率曲线在特征冻结温度T_f以下分裂,随着Se含量从23 K增加到46 K(对于TlCr_5SeS_7到TlCr_5Se_7S),其增加。使用Ising自旋模型,可以通过考虑不同的铁磁和反铁磁交换路径来解释磁挫折和观察到的自旋玻璃行为。 5 K的中子衍射图没有长程磁序。根据实际空间分布函数对衍射图谱中的宽散射峰进行分析,结果表明,反铁磁交换变弱了,但代价是增加了120 K和5 K之间的铁磁相关性。 TlCr_5S_(8-y)Se_y系列上每个Cr(III)的磁矩,但是T_f和#theta#对两个区域1 <-y <-4和4 <-y <-7内的成分的线性依赖性低温和高温状态分别表明在y #approx =#4处达到了临界Cr-Cr原子间距离。

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