论文标题

Na-K合金簇的铁磁状态在低硫酸沸石中

Ferrimagnetic States of Na-K Alloy Clusters in Zeolite Low-Silica X

论文作者

Nakano, Takehito, Araki, Shingo, Kien, Luu Manh, Nam, Nguyen Hoang, Hanh, Duong Thi, Owaki, Akihiro, Goto, Ken, Matsuo, Akira, Kindo, Koichi, Nozue, Yasuo

论文摘要

在沸石低硫酸X(LSX)中,内径约为7 aa {}的β型盘以钻石结构排列。其中,通过与内径约为8 aa {}的内径共享窗口,形成了大约13 aa {}内径的超级尺寸。本研究中使用的沸石LSX的化学公式由Na $ _ {x} $ k $ _ {12-x} $ al $ _ {12} $ _ {12} $ si $ _ {12} $ _ {12} $ o $ $ $ $ _ {48} $ per supercage(或beta cage) Al $ _ {12} $ si $ _ {12} $ o $ _ {48} $分别是Zeolite LSX的可交换阳离子和铝硅酸盐框架。 Na-k合金簇通过$ n $ k原子的每个超级售价(或beta-cage)加载在这些笼子中。已经观察到$ n = 7.8 $,$ x = 4 $,已观察到n'eel的N型铁磁性。在本文中,详细研究了光学,磁性和电气性能,主要是$ x = 4 $。 $ 6.5 <n <8.5 $,观察到铁磁特性。同时,居里常数突然增加。根据Curie常数的突然增加,观察到$ n> 6.5 $的beta笼簇的光学反射带。电阻率表示金属值在$ n $ gtrapprox 6处,因为金属状态在超级式簇的能带中实现。铁磁性是通过超级式群体在巡回电子铁磁群的磁性转带和β型群簇处的局部矩之间的抗铁磁相互作用来解释的。 $ n = 8.2 $ $ x = 4 $的铁磁样品中的电阻率在非常低的温度下升高,例如$ 10^6 $倍的$ 10^6 $倍于较高温度下的值。在电阻率中观察到的异常类似于近托绝缘子,但是超舱簇的窄能带的巡回电子是铁磁。

In zeolite low-silica X (LSX), beta-cages with the inside diameter of approx 7 AA{} are arrayed in a diamond structure. Among them, supercages with the inside diameter of approx 13 AA{} are formed and arrayed in a diamond structure by the sharing of windows with the inside diameter of approx 8 AA{}. The chemical formula of zeolite LSX used in the present study is given by Na$_{x}$K$_{12-x}$Al$_{12}$Si$_{12}$O$_{48}$ per supercage (or beta-cage), where Na$_{x}$K$_{12-x}$ and Al$_{12}$Si$_{12}$O$_{48}$ are the exchangeable cations of zeolite LSX and the aluminosilicate framework, respectively. Na-K alloy clusters are incorporated in these cages by the loading of guest K metal at $n$K atoms per supercage (or beta-cage). A N'eel's N-type ferrimagnetism has been observed at $n = 7.8$ for $x = 4$. In the present paper, optical, magnetic and electrical properties are studied in detail mainly for $x = 4$. Ferrimagnetic properties are observed at $6.5 < n < 8.5$. At the same time, the Curie constant suddenly increases. An optical reflection band of beta-cage clusters at 2.8 eV is observed at $n > 6.5$ in accordance with the sudden increase in the Curie constant. An electrical resistivity indicates metallic values at $n$ gtrapprox 6, because a metallic state is realized in the energy band of supercage clusters. The ferrimagnetism is explained by the antiferromagnetic interaction between the magnetic sublattice of itinerant electron ferromagnetism at supercage clusters and that of localized moments at beta-cage clusters. The electrical resistivity in ferrimagnetic samples at $n = 8.2$ for $x = 4$ increases extraordinarily at very low temperatures, such as approx $10^6$ times larger than the value at higher temperatures. Observed anomalies in the electrical resistivity resembles the Kondo insulator, but itinerant electrons of narrow energy band of supercage clusters are ferromagnetic.

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