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Relative Populations and IR Spectra of Cu(38) Cluster at Finite Temperature Based on DFT and Statistical Thermodynamics Calculations

The relative populations of Cu(38) isomers depend to a great extent on the temperature. Density functional theory and nanothermodynamics can be combined to compute the geometrical optimization of isomers and their spectroscopic properties in an approximate manner. In this article, we investigate ent...

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Detalles Bibliográficos
Autores principales: Buelna-García, Carlos Emiliano, Castillo-Quevedo, Cesar, Quiroz-Castillo, Jesus Manuel, Paredes-Sotelo, Edgar, Cortez-Valadez, Manuel, Martin-del-Campo-Solis, Martha Fabiola, López-Luke, Tzarara, Utrilla-Vázquez, Marycarmen, Mendoza-Wilson, Ana Maria, Rodríguez-Kessler, Peter L., Vazquez-Espinal, Alejandro, Pan, Sudip, de Leon-Flores, Aned, Mis-May, Jhonny Robert, Rodríguez-Domínguez, Adán R., Martínez-Guajardo, Gerardo, Cabellos, Jose Luis
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Frontiers Media S.A. 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8921525/
https://www.ncbi.nlm.nih.gov/pubmed/35300385
http://dx.doi.org/10.3389/fchem.2022.841964
Descripción
Sumario:The relative populations of Cu(38) isomers depend to a great extent on the temperature. Density functional theory and nanothermodynamics can be combined to compute the geometrical optimization of isomers and their spectroscopic properties in an approximate manner. In this article, we investigate entropy-driven isomer distributions of Cu(38) clusters and the effect of temperature on their IR spectra. An extensive, systematic global search is performed on the potential and free energy surfaces of Cu(38) using a two-stage strategy to identify the lowest-energy structure and its low-energy neighbors. The effects of temperature on the populations and IR spectra are considered via Boltzmann factors. The computed IR spectrum of each isomer is multiplied by its corresponding Boltzmann weight at finite temperature. Then, they are summed together to produce a final temperature-dependent, Boltzmann-weighted spectrum. Our results show that the disordered structure dominates at high temperatures and the overall Boltzmann-weighted spectrum is composed of a mixture of spectra from several individual isomers.