Cargando…

Chiral Inversion of Thiolate-Protected Gold Nanoclusters via Core Reconstruction without Breaking a Au–S Bond

[Image: see text] On the basis of density functional theory computations of the well-known chiral Au(38)(SR)(24) nanocluster and its Pd- and Ag-doped derivatives, we propose here a mechanism for chiral inversion that does not require the breaking of a metal–sulfur bond at the metal–ligand interface...

Descripción completa

Detalles Bibliográficos
Autores principales: Malola, Sami, Häkkinen, Hannu
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2019
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6727375/
https://www.ncbi.nlm.nih.gov/pubmed/30889350
http://dx.doi.org/10.1021/jacs.9b01204
Descripción
Sumario:[Image: see text] On the basis of density functional theory computations of the well-known chiral Au(38)(SR)(24) nanocluster and its Pd- and Ag-doped derivatives, we propose here a mechanism for chiral inversion that does not require the breaking of a metal–sulfur bond at the metal–ligand interface but features a collective rotation of the gold core. The calculated energy barriers for this mechanism for Au(38) and Pd-doped Au(38) are in the range of 1–1.5 eV, significantly lower than barriers involving the breakage of Au–S bonds (2.5 eV). For Ag-doped Au(38), barriers for both mechanisms are similar (1.3–1.5 eV). Inversion barriers for a larger chiral Au(144)(SR)(60) are much higher (2.5−2.8 eV). Our computed barriers are in good agreement with racemization barriers estimated from existing experiments for bare and doped Au(38). These results highlight the sensitivity of chiral inversion to the size, structure, and metal composition of the metal core and sensitivity to the detailed structure of the metal–thiolate interface. Our work also predicts that enantiopure Au(144)(SR)(60) clusters would be promising materials for applications requiring high resistance to chiral inversion.