J4 ›› 2015, Vol. 32 ›› Issue (6): 740-750.

• 半导体光电 • 上一篇    下一篇

平面正六边形晶格振动的色散关系

陈志远,吴 涛,周文良   

  1. 1.湖北科技学院 核技术与化学生物学院, 湖北 咸宁 437100;2.咸宁职业技术学院 机电工程系, 湖北 咸宁 437100; 3.湖北科技学院 电子与信息工程学院, 湖北 咸宁 437100
  • 收稿日期:2015-05-04 修回日期:2015-07-01 出版日期:2015-11-28 发布日期:2015-11-05
  • 通讯作者: 陈志远(1972-),博士,教授,从事半导体光电性能研究. E-mail:czy2004hust@163.com
  • 基金资助:

    国家自然科学基金项目(51272072);湖北省自然科学基金项目(2013CFC013)

Dispersion Relations of Two-dimensional Equilateral Hexagonal Lattice Vibration

Chen Zhi-yuan, Wu Tao, Zhou Wen-liang   

  1. 1.School of Nuclear Technology and Chemistry﹠Biology, Hubei University of Science and Technology, Xianning 437100, China; 2. Department of Mechanical and Electronic Engineering, Xianning Vocational Technology College, Xianning 437100,China; 3. School of Electronic and Information Engineering, Hubei University of Science and Technology, Xianning 437100, China
  • Received:2015-05-04 Revised:2015-07-01 Published:2015-11-28 Online:2015-11-05

摘要:

基于晶格动力学理论推导了平面正六边形晶格振动的色散关系,得到第一布里渊区中沿 -M、M-K和 -K三个对称方向的色散关系表达式,沿每一对称方向有四支格波,其中两支声学波和两支光学波。分析讨论了只考虑最近邻原子间作用时和计及次近邻原子间作用下的色散关系,结果表明:只考虑最近邻原子间作用时, 点两声学模频率为零、两光学模频率简并, 点高频声学支与低频光学支频率简并,而 点声子频率非简并;沿三个对称方向都存在一支频率为零的声学波和一支频率不变的无色散光学波,并且 方向的声学波和光学波间具有频隙,另外两个方向的格波间无频隙。当计及次近邻原子间作用时,晶格振动的频率升高,三个对称方向的四支格波都表现出明显的色散性,沿 方向声学支与光学支间的频隙减小,由此可见次近邻原子间作用对色散关系有显著影响,但是对 点声子频率的大小和简并无影响,对 点声子频率的简并也无影响。

关键词: 光电子学, 色散关系, 晶格动力学, 平面正六边形晶格, 次近邻原子间作用

Abstract:

Based on lattice dynamics, the dispersion relations of two-dimensional equilateral hexagonal lattice were derived, and the expressions of the dispersion relations along -M、M-Kand -K three symmetry directions were obtained in the first Brillouin zone. There are four pieces of lattice waves in each direction, where two branches are acoustic waves and other two are optical waves. The effects of the nearest neighbor and secondary neighbor coupling to the dispersion relations were discussed. The results show that, in only nearest neighbor coupling, the eigen frequencies of two acoustic modes are zero and other two non-zero values which correspond to optical modes are degenerate at point. One high frequency acoustic branch and one low frequency optical branch are degenerate at K point, and all four branches are nondegenerate at M point. One of the acoustic branches has totally zero frequencies and one optical branch is dispersionless over the entire symmetry directions. There is a frequency gap between acoustic branches and optical branches along -M direction, and no frequency gap in other directions. With the enhancement of the secondary neighbor coupling, the phonon frequencies are increased, and all four branches are displaied distinct dispersion along three directions, and the frequency gap is narrowed along -M direction. The above results indicate that the dispersion relations are remarkably affected by the secondary neighbor coupling. But the phonon frequencies are still degenerate at and points, further they remain unchanged at point.

Key words: optoelectronics, dispersion relation, lattice dynamics, equilateral hexagonal Lattice, secondary neighbor coupling

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