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Structures, and electronic and spectral properties of single-atom transition metal-doped boron clusters MB(24)(−) (M = Sc, Ti, V, Cr, Mn, Fe, Co, and Ni)

A theoretical study of geometrical structures, electronic properties, and spectral properties of single-atom transition metal-doped boron clusters MB(24)(−) (M = Sc, Ti, V, Cr, Mn, Fe, Co, and Ni) is performed using the CALYPSO approach for the global minimum search, followed by density functional t...

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Detalles Bibliográficos
Autores principales: Li, Shi-Xiong, Yang, Yue-Ju, Chen, De-Liang, Long, Zheng-Wen
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9169616/
https://www.ncbi.nlm.nih.gov/pubmed/35754907
http://dx.doi.org/10.1039/d2ra02500k
Descripción
Sumario:A theoretical study of geometrical structures, electronic properties, and spectral properties of single-atom transition metal-doped boron clusters MB(24)(−) (M = Sc, Ti, V, Cr, Mn, Fe, Co, and Ni) is performed using the CALYPSO approach for the global minimum search, followed by density functional theory calculations. The global minima obtained for the MB(24)(−) (M = Sc, Ti, V, and Cr) clusters correspond to cage structures, and the MB(24)(−) (M = Mn, Fe, and Co) clusters have similar distorted four-ring tubes with six boron atoms each. Interestingly, the global minima obtained for the NiB(24)(−) cluster tend to a quasi-planar structure. Charge population analyses and valence electron density analyses reveal that almost one electron on the transition-metal atoms transfers to the boron atoms. The electron localization function (ELF) of MB(24)(−) (M = Sc, Ti, V, Cr, Mn, Fe, Co, and Ni) indicates that the local delocalization of MB(24)(−) (M = Sc, Ti, V, Cr, and Ni) is weaker than that of MB(24)(−) (M = Mn, Fe, and Co), and there is no obvious covalent bond between doped metal and B atoms. The spin density and spin population analyses reveal that open-shell MB(24)(−) (M = Ti, Cr, Fe, and Ni) has different spin characteristics which are expected to lead to interesting magnetic properties and potential applications in molecular devices. The polarizability of MB(24)(−) (M = Sc, Ti, V, Cr, Mn, Fe, Co, and Ni) shows that MB(24)(−) (M = Mn, Fe, and Co) has larger first hyperpolarizability, indicating that MB(24)(−) (M = Mn, Fe, and Co) has a strong nonlinear optical response. Hence, MB(24)(−) (M = Mn, Fe, and Co) might be considered as a promising nonlinear optical boron-based nanomaterial. The calculated spectra indicate that MB(24)(−) (M = Sc, Ti, V, Cr, Mn, Fe, Co, and Ni) has different and meaningful characteristic peaks that can be compared with future experimental values and provide a theoretical basis for the identification and confirmation of these single-atom transition metal-doped boron clusters. Our work enriches the database of geometrical structures of doped boron clusters and can provide an insight into new doped boron clusters.