Luminescent characterization of solution oligomerization process mediated gold-gold interactions. DTF calculations on [Au2Ag2R4L2]n moieties.

The optical properties of [Au2Ag2(C6F5)4(OCMe2)2](n) (1) have been studied in the solid state at room temperature and at 77 K and in acetone solution (5 x 10-4 M). The crystal structure of 1, analyzed by X-ray diffraction, consists of polymeric chains formed by repetition of Au2Ag2 moieties linked t...

Descripción completa

Detalles Bibliográficos
Autores: Fernández, E.J. [0000-0002-6501-744X], Gimeno, M.C. [0000-0003-0553-0695], Laguna, A. [0000-0003-1984-7538], López-De-Luzuriaga, J.M. [0000-0001-5767-8734], Monge, M. [0000-0002-9672-8279], Pyykkö, P., Sundholm, D.
Tipo de recurso: artículo
Estado:Versión publicada
Fecha de publicación:2000
País:España
Institución:Universidad de La Rioja (UR)
Repositorio:RIUR. Repositorio Institucional de la Universidad de La Rioja
OAI Identifier:oai:portal.dialnet.es:doc/5bbc683fb750603269e8054e
Acceso en línea:https://investigacion.unirioja.es/documentos/5bbc683fb750603269e8054e
Access Level:acceso abierto
Descripción
Sumario:The optical properties of [Au2Ag2(C6F5)4(OCMe2)2](n) (1) have been studied in the solid state at room temperature and at 77 K and in acetone solution (5 x 10-4 M). The crystal structure of 1, analyzed by X-ray diffraction, consists of polymeric chains formed by repetition of Au2Ag2 moieties linked through short gold - gold interactions. The emission profile observed for 1 in dilute acetone solution (5 x 10-4 M) is assignable to pentafluorophenyl localized ππ* excited states or from π-MMCT transitions, and in the solid-state arises from metal-centered (dσ*)1(pσ)1 or (dδ*)1(pσ)1 excited states. When the absorption and emission spectra of compound 1 in acetone are registered at different concentrations, they display a band that does not obey the Lambert - Beer law. This deviation is consistent with molecular aggregation in solution through gold - gold interactions, and a clear correlation between the emission wavelength and the structure of 1 in the solid state and in solution is shown. DFT calculations accord with the observed experimental behavior and show the nature of the orbitals involved in each transition.