{"title":"Magnetoplasma-Reflectivity of Pb1-XGeXTe","authors":"J. Burkhart, G. Bauer, W. Jantsch, A. Lopez‐Otero","doi":"10.1109/ICSWA.1979.9335446","DOIUrl":null,"url":null,"abstract":"Pb<inf>1-X</inf>Ge<inf>X</inf>Te exhibits a structural phase transition from the cubic NaCl(O<inf>h</inf>) to the rhombohedral As-like structure (C<inf>3v</inf>) at low lattice temperatures [1]. The transition temperature T<inf>C</inf> is a steep function of the Ge content. The infrared active mode of the cubic structure is split into an A<inf>1</inf>-mode and a double degenerate E-mode. These modes are both infrared and Raman active. A<inf>1</inf> is observable for the polarization <sup>→</sup>E‖ c-axis [2,3]. In the cubic phase, electrons or holes are located in four equivalent L-valleys. Below T<inf>C</inf>, there are three equivalent L-valleys, and along the direction of the c-axis a T-valley.","PeriodicalId":216123,"journal":{"name":"1979 International Conference on Submillimeter Waves and Their Applications","volume":"15 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1979-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"1979 International Conference on Submillimeter Waves and Their Applications","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ICSWA.1979.9335446","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
Pb1-XGeXTe exhibits a structural phase transition from the cubic NaCl(Oh) to the rhombohedral As-like structure (C3v) at low lattice temperatures [1]. The transition temperature TC is a steep function of the Ge content. The infrared active mode of the cubic structure is split into an A1-mode and a double degenerate E-mode. These modes are both infrared and Raman active. A1 is observable for the polarization →E‖ c-axis [2,3]. In the cubic phase, electrons or holes are located in four equivalent L-valleys. Below TC, there are three equivalent L-valleys, and along the direction of the c-axis a T-valley.