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Hydrogen segregation and its roles in structural stability and metallization: silane under pressure

We present results from first-principles calculations on silane (SiH(4)) under pressure. We find that a three dimensional P-3 structure becomes the most stable phase above 241 GPa. A prominent structural feature, which separates the P-3 structure from previously observed/predicted SiH(4) structures,...

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Detalles Bibliográficos
Autores principales: Cui, Wenwen, Shi, Jingming, Liu, Hanyu, Yao, Yansun, Wang, Hui, Iitaka, Toshiaki, Ma, Yanming
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group 2015
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC4533316/
https://www.ncbi.nlm.nih.gov/pubmed/26266340
http://dx.doi.org/10.1038/srep13039
Descripción
Sumario:We present results from first-principles calculations on silane (SiH(4)) under pressure. We find that a three dimensional P-3 structure becomes the most stable phase above 241 GPa. A prominent structural feature, which separates the P-3 structure from previously observed/predicted SiH(4) structures, is that a fraction of hydrogen leaves the Si-H bonding environment and forms segregated H(2) units. The H(2) units are sparsely populated in the system and intercalated with a polymeric Si-H framework. Calculations of enthalpy of formation suggest that the P-3 structure is against the decomposition into Si-H binaries and/or the elemental crystals. Structural stability of the P-3 structure is attributed to the electron-deficient multicenter Si-H-Si interactions when neighboring silicon atoms are linked together through a common hydrogen atom. Within the multicenter bonds, electrons are delocalized and this leads to a metallic state, possibly also a superconducting state, for SiH(4). An interesting outcome of the present study is that the enthalpy sum of SiH(4) (P-3 structure) and Si (fcc structure) appears to be lower than the enthalpy of disilane (Si(2)H(6)) between 200 and 300 GPa (for all previously predicted crystalline forms of Si(2)H(6)), which calls for a revisit of the stability of Si(2)H(6) under high pressure.