Anharmonic line shift and linewidth of the Raman mode in covalent semiconductors

被引:76
|
作者
Lang, G [1 ]
Karch, K
Schmitt, M
Pavone, P
Mayer, AP
Wehner, RK
Strauch, D
机构
[1] Univ Regensburg, Inst Theoret Phys, D-93040 Regensburg, Germany
[2] Univ Jena, Inst Festkorpertheorie & Theoret Opt, D-07743 Jena, Germany
[3] Max Planck Inst Phys Komplexer Syst, D-01187 Dresden, Germany
[4] Univ Munster, Inst Theoret Festkorperphys, D-48149 Munster, Germany
来源
PHYSICAL REVIEW B | 1999年 / 59卷 / 09期
关键词
D O I
10.1103/PhysRevB.59.6182
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Combining density-functional perturbation theory with the frozen-phonon approach, the anharmonic shift of the Raman frequency of the covalent semiconductors diamond and silicon are determined ab initio. The temperature dependence of the Raman frequency and the contribution of zero-point motion are calculated as well as the Raman linewidth. Corresponding results for germanium have been obtained with the assumption that the quartic anharmonic force constants may be approximated by those of silicon. [S0163-1829(99)13305-8].
引用
收藏
页码:6182 / 6188
页数:7
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