Effects of Compression on the Iodine Local Environment in Dipotassium Zinc Tetraiodate(V) Dihydrate K2Zn(IO3)4·2H2O

[EN] Combining X-ray diffraction with density-functional theory and electron topology calculations, we found that pressure substantially modifies the bonding in K2Zn(IO3)42H2O. We discovered that under compression, there is a progressive change from primary covalent I-O bonds and secondary halogen I...

Descripción completa

Detalles Bibliográficos
Autores: Errandonea, Daniel; Turnbull, Robin; Osman, Hussien H. H.; Hebboul, Zoulikha; Botella, Pablo; Bura, Neha; Zang, Peijie; Rodrigo-Ramon, Jose Luis; Sanchez-Martin, Josu; Popescu, Catalin; Manjón, Francisco-Javier|||0000-0002-3926-1705
Tipo de documento: Artículo
Fecha de publicación:2025
País:España
Institución:Universitat Politècnica de València (UPV)
Repositorio:RiuNet. Repositorio Institucional de la Universitat Politécnica de Valéncia
Lenguaje:Inglés
OAI Identifier:oai:dnet:riunet______::cf953561371dc675c83ddee3a654589a
Acceso en línea:https://riunet.upv.es/handle/10251/233996
Nivel de acceso:Acceso abierto
Palabra clave:High-pressure crystallography
Iodates
Multicenter bonding
Iodine hypercoordination
Electron topology
Band gap
Descripción
Sumario:[EN] Combining X-ray diffraction with density-functional theory and electron topology calculations, we found that pressure substantially modifies the bonding in K2Zn(IO3)42H2O. We discovered that under compression, there is a progressive change from primary covalent I-O bonds and secondary halogen IO interactions toward O-I-O electron-deficient multicenter bonds. Because of this, iodine hypercoordination converts IO3 trigonal pyramids toward IO6 units. The formation of these IO6 units breaks the typical isolation of iodate molecules, forming an infinite two-dimensional iodate network. Hypercoordination influences the hydrogen atoms too, such that multicenter O-H-O bonds are also promoted with increasing pressure. We have determined that K2Zn(IO3)42H2O is one of the most compressible iodates studied to date, with a bulk modulus of 22(3) GPa. The pressure-induced structural changes strongly modify the electronic structure as shown by optical-absorption measurements and band-structure calculations. The band gap energy closes from 4.2(1) eV at ambient pressure to 3.4(1) eV at 20 GPa.