首页> 美国卫生研究院文献>Scientific Reports >Effect of divalent Ba cation substitution with Sr on coupled‘multiglass’ state in the magnetoelectric multiferroic compoundBa3NbFe3Si2O14
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Effect of divalent Ba cation substitution with Sr on coupled‘multiglass’ state in the magnetoelectric multiferroic compoundBa3NbFe3Si2O14

机译:Sr取代二价Ba阳离子对偶联的影响磁电多铁化合物中的多玻璃状态Ba3NbFe3Si2O14

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摘要

(Ba/Sr)3NbFe3Si2O14 is a magneto-electric multiferroic with an incommensurate antiferromagnetic spiral magnetic structure which induces electric polarization at 26 K. Structural studies show that both the compounds have similar crystal structure down to 6 K. They exhibit a transition, TN at 26 K and 25 K respectively, as indicated by heat capacity and magnetization, into an antiferromagnetic state. Although Ba and Sr are isovalent, they exhibit very different static and dynamic magnetic behaviors. The Ba-compound exhibits a glassy behavior with critical slowing dynamics with a freezing temperature of ~35 K and a critical exponent of 3.9, a value close to the 3-D Ising model above TN, in addition to the invariant transition into an antiferromagnetic state. The Sr-compound however does not exhibit any dispersive behavior except for the invariant transition at TN. The dielectric constant reflects magnetic behavior of the two compounds: the Ba-compound has two distinct dispersive peaks while the Sr-compound has a single dispersive peak. Thus the compounds exhibit coupled ‘multiglass’ behavior. The difference in magnetic properties between the two compounds is found to be due tomodifications to super exchange path angle and length as well as anti-site defectswhich stabilize either ferromagnetic or antiferromagnetic interactions.
机译:(Ba / Sr)3NbFe3Si2O14是具有不相称的反铁磁螺旋磁性结构的磁电多铁性化合物,在26 K时感应极化。如热容量和磁化强度所示,分别为26 K和25 K进入反铁磁状态。尽管Ba和Sr是等价的,但它们表现出非常不同的静态和动态磁行为。 Ba化合物表现出玻璃态行为,具有临界减慢动力学,冻结温度约为35 K,临界指数为3.9,该值接近于TN以上的3-D Ising模型,并且始终不变地转变为反铁磁态。然而,Sr-化合物除了在TN处的不变转变外,没有表现出任何分散行为。介电常数反映了这两种化合物的磁行为:Ba化合物具有两个不同的色散峰,而Sr化合物具有一个单独的色散峰。因此,这些化合物表现出耦合的“多玻璃”行为。发现这两种化合物之间的磁性能差异是由于修改超级交换路径的角度和长度以及抗位缺陷可以稳定铁磁或反铁磁相互作用。

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