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首页> 外文期刊>The Journal of Chemical Physics >Geometries, stabilities, and electronic properties of different-sized ZrSin (n=1-16) clusters: A density-functional investigation
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Geometries, stabilities, and electronic properties of different-sized ZrSin (n=1-16) clusters: A density-functional investigation

机译:不同大小的ZrSin(n = 1-16)团簇的几何,稳定性和电子性质:密度泛函研究

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The ZrSin (n=1-16) clusters with different spin configurations have been systematically investigated by using the density-functional approach. The total energies, equilibrium geometries, growth-pattern mechanisms, natural population analysis, etc., are discussed. The equilibrium structures of different-sized ZrSin clusters can be determined by two evolution patterns. Theoretical results indicate that the most stable ZrSin (n=1-7) geometries, except ZrSi3, keep the analogous frameworks as the lowest-energy or the second lowest-energy Sin+1 clusters. However, for large ZrSin (n=8-16) clusters, Zr atom obviously disturbs the framework of silicon clusters, and the localized position of the transition-metal (TM) Zr atom gradually varies from the surface insertion site to the concave site of the open silicon cage and to the encapsulated site of the sealed silicon cage. It should be mentioned that the lowest-energy sandwichlike ZrSi12 geometry is not a sealed structure and appears irregular as compared with other TM@Si-12 (TM=Re,Ni). The growth patterns of ZrSin (n=1-16) clusters are concerned showing the Zr-encapsulated structures as the favorable geometries. In addition, the calculated fragmentation energies of the ZrSin (n=1-16) clusters manifest that the magic numbers of stabilities are 6, 8, 10, 14, and 16, and that the fullerenelike ZrSi16 is the most stable structure, which is in good agreement with the calculated atomic binding energies of ZrSin (n=8-16) and with available experimental and theoretical results. Natural population analysis shows that the natural charge population of Zr atom in the most stable ZrSin (n=1-16) structures exactly varies from positive to negative at the critical-sized ZrSi8 cluster; furthermore, the charge distribution around the Zr atom appears clearly covalent in character for the small- or middle-sized clusters and metallic in character for the large-sized clusters. Finally, the properties of frontier orbitals and polarizabilities of ZrSin are also discussed. (C) 2005 American Institute of Physics.
机译:通过使用密度泛函方法,系统地研究了具有不同自旋构型的ZrSin(n = 1-16)团簇。讨论了总能量,平衡几何形状,增长模式机制,自然种群分析等。不同大小的ZrSin团簇的平衡结构可以通过两种演化模式来确定。理论结果表明,除了ZrSi3之外,最稳定的ZrSin(n = 1-7)几何形状都将类似框架保留为最低能量或次最低能量的Sin + 1簇。然而,对于较大的ZrSin(n = 8-16)团簇,Zr原子明显干扰了硅团簇的结构,过渡金属(TM)Zr原子的局部位置从表面插入位置到凹入位置逐渐变化。打开硅笼,并到达密封硅笼的封装部位。应该提到的是,最低能量的三明治状ZrSi12几何形状不是密封结构,与其他TM @ Si-12(TM = Re,Ni)相比显得不规则。 ZrSin(n = 1-16)团簇的生长模式受到关注,显示出Zr封装的结构是有利的几何形状。此外,计算得出的ZrSin(n = 1-16)团簇的碎片能表明,稳定的魔术数为6、8、10、14和16,而富勒烯状ZrSi16是最稳定的结构,即与计算得出的ZrSin的原子结合能(n = 8-16)以及现有的实验和理论结果高度吻合。自然种群分析表明,在临界尺寸的ZrSi8团簇中,最稳定的ZrSin(n = 1-16)结构中Zr原子的自然电荷种群正负完全不同。此外,Zr原子周围的电荷分布在中小型簇中表现出明显的共价特征,在大型簇中表现出金属特征。最后,还讨论了ZrSin的前沿轨道性质和极化率。 (C)2005美国物理研究所。

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