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Sb(2)Se(3) under pressure

Selected members of the A(2)B(3) (A = Sb, Bi; B = Se, Te) family are topological insulators. The Sb(2)Se(3) compound does not exhibit any topological properties at ambient conditions; a recent high-pressure study, however, indicated that pressure transforms Sb(2)Se(3) from a band insulator into a to...

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Detalles Bibliográficos
Autores principales: Efthimiopoulos, Ilias, Zhang, Jiaming, Kucway, Melvin, Park, Changyong, Ewing, Rodney C., Wang, Yuejian
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2013
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3776230/
https://www.ncbi.nlm.nih.gov/pubmed/24045363
http://dx.doi.org/10.1038/srep02665
Descripción
Sumario:Selected members of the A(2)B(3) (A = Sb, Bi; B = Se, Te) family are topological insulators. The Sb(2)Se(3) compound does not exhibit any topological properties at ambient conditions; a recent high-pressure study, however, indicated that pressure transforms Sb(2)Se(3) from a band insulator into a topological insulator above ~2 GPa; in addition, three structural transitions were proposed to occur up to 25 GPa. Partly motivated by these results, we have performed x-ray diffraction and Raman spectroscopy investigations on Sb(2)Se(3) under pressure up to 65 GPa. We have identified only one reversible structural transition: the initial Pnma structure transforms into a disordered cubic bcc alloy above 51 GPa. On the other hand, our high-pressure Raman study did not reproduce the previous results; we attribute the discrepancies to the effects of the different pressure transmitting media used in the high-pressure experiments. We discuss the structural behavior of Sb(2)Se(3) within the A(2)B(3) (A = Sb, Bi; B = Se, Te) series.