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首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Crystal Structures of Heavily Na-Loaded Low-Silica X (LSX) Zeolites in Insulating and Metallic States
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Crystal Structures of Heavily Na-Loaded Low-Silica X (LSX) Zeolites in Insulating and Metallic States

机译:处于绝缘状态和金属状态的重载Na的低硅X(LSX)沸石的晶体结构

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Crystal structures of sodium clusters incorporated in LSX zeolite [Na_(12)Al_(12)Si_(12)O_(48) (2 = 8)] with FAU-type topology are analyzed by powder X-ray diffraction. The two different Na-loaded samples, Na_(9.4)/Na_(12)-LSX and Na_(16.7)/Na_(12)- LSX, show insulating and metallic states, respectively. The insulating state is changed to the metallic state upon increasing the loading density of Na atoms. The two samples have the space group Fd3 attributed to cubic symmetry and lattice constants of a = 2.49646(3) nm for Na_(9.4)/Na_(12)LSX and a = 2.495060(11) nm for Na_(16.7)/Na_(12)-LSX. In both samples, three cation sites at the centers of two types of 6-ring of the sod-cage and the centers of the d6r prism are fully occupied by Na ions. In addition, a large number of Na cations forming Na clusters are distributed in the cavity (supercage), and Na distribution inside the cavity is disorderly, which is represented by several independent sites with low site occupancy. Electron-density distribution analysis clearly reveals the covalent bond of Si(Al)-O and disordered Na distribution in the cavity. In addition, electron densities based on the orbital hybridization between a Na cation and framework oxygen atom are observed around the 12-ring. In Na_(16.7)/Na_(12)-LSX, the formation of the chain-like Na cation distribution, which connects between the second neighboring cavities, is represented. However, this Na-Na connectivity is not formed in Na_(9.4)/Na_(12)-LSX. It was identified that the total number of Na cations in the cavity in Na_(16.7)/Na_(12)-LSX is much larger than that in Na_(9.4)/Na_(12)-LSX. The cation sites can be classified into two types of character: (a) close to the inner wall of cavity and (b) around the center of cavity and/or at the center of 12-ring pore window. In the domain (b), the number of cations remarkably increases with the increase in n. This change must be strongly related to the insulator-to-metal transition.
机译:通过粉末X射线衍射分析了LSX沸石[Na_(12)Al_(12)Si_(12)O_(48)(2 = 8)]中掺入的钠簇的晶体结构。 Na_(9.4)/ Na_(12)-LSX和Na_(16.7)/ Na_(12)-LSX这两个不同的Na加载样品分别显示出绝缘状态和金属状态。随着Na原子的负载密度的增加,绝缘状态变为金属状态。这两个样本具有归因于立方对称性的空间群Fd3,晶格常数对于Na_(9.4)/ Na_(12)LSX为a = 2.49646(3)nm,对于Na_(16.7)/ Na_(a = 2.495060(11)nm) 12)-LSX。在这两个样品中,草皮笼的两种类型的6环中心和d6r棱镜中心的三个阳离子位点被Na离子完全占据。另外,形成Na簇的大量Na阳离子分布在空腔(超笼)中,并且空腔内部的Na分布是无序的,其表现为几个独立的位点,具有较低的位点占有率。电子密度分布分析清楚地揭示了Si(Al)-O的共价键和空腔中无序的Na分布。另外,在12环附近观察到基于Na阳离子与骨架氧原子之间的轨道杂化的电子密度。在Na_(16.7)/ Na_(12)-LSX中,表示了连接第二个相邻腔之间的链状Na阳离子分布的形成。但是,在Na_(9.4)/ Na_(12)-LSX中未形成此Na-Na连接。可以确定,Na_(16.7)/ Na_(12)-LSX中空腔中的Na阳离子总数远大于Na_(9.4)/ Na_(12)-LSX中的空腔。阳离子位点可分为两种类型:(a)靠近腔体的内壁和(b)围绕腔体的中心和/或在12环孔窗口的中心。在区域(b)中,阳离子的数量随着n的增加而显着增加。这种变化必须与绝缘子到金属的转变密切相关。

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