拉曼光谱
声子
拉曼散射
非谐性
材料科学
大气温度范围
热膨胀
凝聚态物理
锗
分子束外延
激光线宽
分析化学(期刊)
外延
化学
硅
光学
纳米技术
热力学
激光器
光电子学
图层(电子)
冶金
物理
色谱法
作者
Tao Liu,Yuanhao Miao,Liming Wang,Guangjian Zhu,Huiyong Hu,Zhenyang Zhong,Xinju Yang,Zuimin Jiang
摘要
Abstract Temperature dependence of Raman scattering from Ge 0.95 Sn 0.05 and Ge 0.92 Sn 0.08 films, grown on Ge (001) substrates by low temperature molecular beam epitaxy, was studied over the temperature range of 90 to 850 K. Nonlinear temperature dependencies in the Raman shift of Ge‐Ge and Ge‐Sn modes have been observed. Although they could be well described by an empirical formula, much different values were found in first‐order temperature coefficient of the Raman shift for the Ge‐Ge mode in bulk Ge, the Ge 0.95 Sn 0.05 , and Ge 0.92 Sn 0.08 films, being 1.7, 2.4, and 2.7 × 10 −2 cm −1 /K, respectively. Two factors, phonon–phonon coupling and thermal expansion, contribute to the temperature dependence of Raman shift. Detailed analysis shows that the thermal expansion contribution increases slightly with the Sn content, whereas the phonon–phonon coupling contribution increases markedly with the Sn content. In other words, the anharmonic decay process is much enhanced by the alloy perturbation in GeSn alloys. In addition, an abrupt change was observed at temperature of 650 K in Raman shift and linewidth of Ge‐Ge mode for the Ge 0.92 Sn 0.08 film, which is caused by Sn segregation, concomitant lattice relaxation, and crystallization as well.
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