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Gold(i) sulfide: unusual bonding and an unexpected computational challenge in a simple solid

We report the experimental high-pressure crystal structure and equation of state of gold(i) sulfide (Au(2)S) determined using diamond-anvil cell synchrotron X-ray diffraction. Our data shows that Au(2)S has a simple cubic structure with six atoms in the unit cell (four Au in linear, and two S in tet...

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Detalles Bibliográficos
Autores principales: Santamaría-Pérez, D., Daisenberger, D., Ruiz-Fuertes, J., Marqueño, T., Chulia-Jordan, R., Muehle, C., Jansen, M., Rodriguez-Hernandez, P., Muñoz, A., Johnson, Erin R., Otero-de-la-Roza, A.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Royal Society of Chemistry 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6610519/
https://www.ncbi.nlm.nih.gov/pubmed/31341598
http://dx.doi.org/10.1039/c9sc00371a
Descripción
Sumario:We report the experimental high-pressure crystal structure and equation of state of gold(i) sulfide (Au(2)S) determined using diamond-anvil cell synchrotron X-ray diffraction. Our data shows that Au(2)S has a simple cubic structure with six atoms in the unit cell (four Au in linear, and two S in tetrahedral, coordination), no internal degrees of freedom, and relatively low bulk modulus. Despite its structural simplicity, Au(2)S displays very unusual chemical bonding. The very similar and relatively high electronegativities of Au and S rule out any significant metallic or ionic character. Using a simple valence bond (Lewis) model, we argue that the Au(2)S crystal possesses two different types of covalent bonds: dative and shared. These bonds are distributed in such a way that each Au atom engages in one bond of each kind. The multiple arrangements in space of dative and shared bonds are degenerate, and the multiplicity of configurations imparts the system with multireference character, which is highly unusual for an extended solid. The other striking feature of this system is that common computational (DFT) methods fail quite spectacularly to describe it, with 20% and 400% errors in the equilibrium volume and bulk modulus, respectively. We explain this by the poor treatment of static correlation in common density-functional approximations. The fact that the solid is structurally very simple, yet presents unique chemical bonding and is unmodelable using current DFT methods, makes it an interesting case study and a computational challenge.