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Revealing Phosphorus Nitrides up to the Megabar Regime: Synthesis of α′‐P(3)N(5,) δ‐P(3)N(5) and PN(2)

Non‐metal nitrides are an exciting field of chemistry, featuring a significant number of compounds that can possess outstanding material properties. These properties mainly rely on maximizing the number of strong covalent bonds, with crosslinked XN(6) octahedra frameworks being particularly attracti...

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Detalles Bibliográficos
Autores principales: Laniel, Dominique, Trybel, Florian, Néri, Adrien, Yin, Yuqing, Aslandukov, Andrey, Fedotenko, Timofey, Khandarkhaeva, Saiana, Tasnádi, Ferenc, Chariton, Stella, Giacobbe, Carlotta, Bright, Eleanor Lawrence, Hanfland, Michael, Prakapenka, Vitali, Schnick, Wolfgang, Abrikosov, Igor A., Dubrovinsky, Leonid, Dubrovinskaia, Natalia
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9827839/
https://www.ncbi.nlm.nih.gov/pubmed/35997073
http://dx.doi.org/10.1002/chem.202201998
Descripción
Sumario:Non‐metal nitrides are an exciting field of chemistry, featuring a significant number of compounds that can possess outstanding material properties. These properties mainly rely on maximizing the number of strong covalent bonds, with crosslinked XN(6) octahedra frameworks being particularly attractive. In this study, the phosphorus–nitrogen system was studied up to 137 GPa in laser‐heated diamond anvil cells, and three previously unobserved phases were synthesized and characterized by single‐crystal X‐ray diffraction, Raman spectroscopy measurements and density functional theory calculations. δ‐P(3)N(5) and PN(2) were found to form at 72 and 134 GPa, respectively, and both feature dense 3D networks of the so far elusive PN(6) units. The two compounds are ultra‐incompressible, having a bulk modulus of K (0)=322 GPa for δ‐P(3)N(5) and 339 GPa for PN(2). Upon decompression below 7 GPa, δ‐P(3)N(5) undergoes a transformation into a novel α′‐P(3)N(5) solid, stable at ambient conditions, that has a unique structure type based on PN(4) tetrahedra. The formation of α′‐P(3)N(5) underlines that a phase space otherwise inaccessible can be explored through materials formed under high pressure.