首页> 外文期刊>Inorganic Chemistry: A Research Journal that Includes Bioinorganic, Catalytic, Organometallic, Solid-State, and Synthetic Chemistry and Reaction Dynamics >Comparison of the crystal structures and magnetic properties of the low- and high-temperature forms of AgCuPO4: Crystal structure determination, magnetic susceptibility measurements, and spin dimer analysis
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Comparison of the crystal structures and magnetic properties of the low- and high-temperature forms of AgCuPO4: Crystal structure determination, magnetic susceptibility measurements, and spin dimer analysis

机译:AgCuPO4低温和高温形式的晶体结构和磁性的比较:晶体结构确定,磁化率测量和自旋二聚体分析

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摘要

The crystal structure of the low-temperature form of AgCuPO4 (i.e., alpha-AgCuPO4) was determined by powder X-ray diffraction and was compared with that of the high-temperature form of AgCuPO4 (i.e. beta-AgCuPO4). The magnetic properties of the two forms were examined by measuring their magnetic susceptibilities and evaluating the relative strengths of their spin-exchange interactions on the basis of spin-dimer analysis. Both forms of AgCuPO4 have layers of Cu2P2O8 alternating with silver-atom double layers; beta-AgCuPO4 has two Cu2P2O8 layers per unit cell, while alpha-AgCuPO4 has one. The coordinate environment of each Cu2+ ion is close to being a distorted square pyramid in alpha-AgCuPO4, but it is close to being a distorted trigonal bipyramid in beta-AgCuPO4. The magnetic susceptibilities of alpha- and beta-AgCuPO4 are well simulated by an antiferromagnetic alternating-chain model, which leads to J/K-B = -146.1 K and alpha J/K-B = -75.8 K for alpha-AgCuPO4, and J/K-B = -82.6 K and alpha J/K-B = -31.7 K for beta-AgCuPO4 (with the convention in which the spin-exchange parameter between two adjacent spin sites is written as 2J). The spin gaps, Delta/K-B, obtained from these parameters are 93.7 K for alpha-AgCuPO4 and 62.3 K for beta-AgCuPO4. The strongest spin exchange in both forms of AgCuPO4 comes from a super-superexchange path, and this interaction is stronger for R-AgCuPO4 than for beta-AgCuPO4 by a factor of similar to 2, in good agreement with the experiment. Our analysis supports the use of this model for beta-AgCuPO4 and indicates that the spin lattice of alpha-AgCuPO4 would be better described by a two-dimensional net made up of weakly interacting alternating chains.
机译:通过粉末X射线衍射确定低温形式的AgCuPO 4(即,α-AgCuPO4)的晶体结构,并将其与AgCuPO 4的高温形式(即β-AgCuPO4)的晶体结构进行比较。通过测量自旋二聚体的磁化率并评估自旋交换相互作用的相对强度,检查了这两种形式的磁性。两种形式的AgCuPO4均具有交替的Cu2P2O8层和银原子双层。 beta-AgCuPO4每单位晶胞具有两层Cu2P2O8,而alpha-AgCuPO4有一层。每个Cu2 +离子的配位环境在α-AgCuPO4中接近于扭曲的方形金字塔,但在β-AgCuPO4中接近于扭曲的三角锥体。通过反铁磁交替链模型很好地模拟了α-和β-AgCuPO4的磁化率,这导致α/ AgCuPO4的J / KB = -146.1 K和alpha J / KB = -75.8 K,并且J / KB =对于β-AgCuPO4,-82.6 K和alpha J / KB = -31.7 K(惯例是两个相邻的自旋位点之间的自旋交换参数写为2J)。从这些参数获得的自旋间隙Delta / K-B对于α-AgCuPO4是93.7 K,对于β-AgCuPO4是62.3K。两种形式的AgCuPO4中最强的自旋交换来自超级交换通道,R-AgCuPO4的相互作用比β-AgCuPO4的相互作用强2倍,与实验相符。我们的分析支持将这种模型用于beta-AgCuPO4,并表明通过由弱相互作用的交替链组成的二维网络可以更好地描述alpha-AgCuPO4的自旋晶格。

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