首页> 外文期刊>Journal of the Physical Society of Japan >Stabilization of Long-Range Order by Additional Anisotropic Spins in Two-Dimensional Isotropic Heisenberg Antiferromagnets - A Possible Model of an Organic Compound with Magnetic Anions
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Stabilization of Long-Range Order by Additional Anisotropic Spins in Two-Dimensional Isotropic Heisenberg Antiferromagnets - A Possible Model of an Organic Compound with Magnetic Anions

机译:二维各向同性海森堡反铁磁体中通过附加各向异性自旋来稳定远距离有序-含磁性阴离子的有机化合物的可能模型

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We examine a two-dimensional (2D) coupled antiferromagnetic (AF) Heisenberg model that consists of two subsystems: an isotropic S = 1/2 spin subsystem with strong AF exchange interactions (main system), and a uniaxial S = 5/2 spin subsystem with weak exchange interactions. This model is an example in which additional semiclassical degrees of freedom affect a quantum system; it also describes a possible stabilization mechanism of AF long-range order (LRO) in the 2D organic compound lambda-(BETS)(2)FeCl4, where BETS stands for bis(ethylenedithio)tetraselenafulvalene. Previous experimental studies have revealed that 3d spins on FeCl4 anions passively follow the AF LRO of the pi-electron system in the BETS layers, although the AF LRO is stabilized by the 3d spins themselves. To explain this paradoxical behavior, we examine a scenario in which the uniaxial anisotropy of the 3d spins stabilizes the AF LRO on an isotropic 2D pi-spin system. We extend Green's function theory, called the Tyablikov approximation, to the present system, which describes spin-wave excitations and is consistent with the Mermin-Wagner theorem. It is shown that even extremely weak interactions with the uniaxial subsystem efficiently stabilize the AF LRO in the main system, even in the absence of AF exchange interactions in the uniaxial subsystem. The AF LRO is triggered by the uniaxial subsystem, but the sublattice magnetization remains smaller than that of the main system in the high-temperature region. These results are consistent with experimental data for lambda-(BETS)(2)FeCl4 and lambda-(BETS)(2)GaCl4; the latter does not have the 3d spins and does not exhibit the AF LRO.
机译:我们研究了二维(2D)耦合反铁磁(AF)Heisenberg模型,该模型由两个子系统组成:各向同性S = 1/2自旋子系统,具有很强的AF交换相互作用(主系统),以及单轴S = 5/2自旋子系统之间的交互作用较弱。该模型是一个示例,其中附加的半经典自由度影响量子系统。它还描述了二维有机化合物lambda-(BETS)(2)FeCl4中AF远程有序(LRO)的可能稳定机制,其中BETS代表双(亚乙基二硫代)四硒富勒烯。先前的实验研究表明,在FeCl4阴离子上的3d自旋会被动地跟随BETS层中pi电子系统的AF LRO,尽管AF LRO由3d自旋本身稳定了。为了解释这种自相矛盾的行为,我们检查了3d自旋的单轴各向异性使各向同性2D pi-spin系统上的AF LRO稳定的情况。我们将格林函数理论(称为Tyablikov逼近)扩展到本系统,该系统描述了自旋波激励,并且与Mermin-Wagner定理一致。结果表明,即使在单轴子系统中不存在AF交换相互作用的情况下,即使与单轴子系统的相互作用极弱,也可以有效地稳定主系统中的AF LRO。 AF LRO由单轴子系统触发,但在高温区域,亚晶格磁化强度仍小于主系统的磁化强度。这些结果与lambda-(BETS)(2)FeCl4和lambda-(BETS)(2)GaCl4的实验数据一致。后者没有3d自旋,也没有AF LRO。

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