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MgO 纳米管的电子结构。一项从头量子力学研究。

The electronic structure of MgO nanotubes. An ab initio quantum mechanical investigation.

机构信息

Equipe de Chimie physique, IPREM UMR 5254, Technopole Hélioparc, 2 avenue du Président Pierre Angot, 64053 Pau Cedex 09, France.

出版信息

Phys Chem Chem Phys. 2013 Aug 28;15(32):13296-303. doi: 10.1039/c3cp50979f.

Abstract

The structural, vibrational and response properties of the (n,0) and (m,m) MgO nanotubes are computed by using a Gaussian type basis set, a hybrid functional (B3LYP) and the CRYSTAL09 code. Tubes in the range 6 ≤ n ≤ 140 and 3 ≤ m ≤ 70 were considered, being n = 2 × m the number of MgO units in the unit cell (so, the maximum number of atoms is 280). Tubes are built by rolling up the fully relaxed 2-D conventional cell (2 MgO units, with oxygen atoms protruding from the Mg plane alternately up and down by 0.38 Å). The relative stability of the (n,0) with respect to the (m,m) family, the relaxation energy and equilibrium geometry, the band gap, the IR vibrational frequencies and intensities, and the electronic and ionic contributions to the polarizability are reported. All these properties are shown to converge smoothly to the monolayer values. Absence of negative vibrational frequencies confirms that the tubes have a stable structure. The parallel component of the polarizability α(∥) converges very rapidly to the monolayer value, whereas α(⊥) is still changing at n = 140; however, when extrapolated to very large n values, it coincides with the monolayer value to within 1%. The electronic contribution to α is in all cases (α(∥) and α(⊥); 6 ≤ n ≤ 140) smaller than the vibrational contribution by about a factor of three, at variance with respect to more covalent tubes such as the BN ones, for which the ratio between the two contributions is reversed.

摘要

采用高斯型基组、杂化泛函(B3LYP)和 CRYSTAL09 代码,计算了(n,0)和(m,m)MgO 纳米管的结构、振动和响应特性。考虑了 6≤n≤140 和 3≤m≤70 的纳米管,其中 n=2×m 是单元晶胞中 MgO 单元的数量(因此,最大原子数为 280)。纳米管是通过将完全弛豫的二维常规单元(2MgO 单元,氧原子沿 Mg 平面交替向上和向下突出 0.38Å)卷起而构建的。报告了(n,0)相对于(m,m)族的相对稳定性、弛豫能和平衡几何形状、能带隙、IR 振动频率和强度以及对极化率的电子和离子贡献。所有这些特性都被证明可以平滑地收敛到单层值。不存在负振动频率表明纳米管具有稳定的结构。极化率的平行分量 α(∥)迅速收敛到单层值,而 α(⊥)在 n=140 时仍在变化;然而,当外推到非常大的 n 值时,它与单层值在 1%以内重合。在所有情况下(α(∥)和 α(⊥);6≤n≤140),电子对 α 的贡献都小于振动贡献,大约是振动贡献的三分之一,与 BN 等更共价的纳米管相反,对于 BN 等纳米管,这两种贡献的比值是相反的。

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