Computational Characterisation of Gold Nanocluster Structures by Andrew James Logsdail
Author:Andrew James Logsdail
Language: eng
Format: epub
Publisher: Springer International Publishing, Cham
Results of adsorption on an HOPG substrate with and without surface vacancies, with C atoms unconstrained within 7.0 Å of the cluster, are given in Appendix C.5. General trends are as previously observed for adsorption on to a surface with an unconstrained distance of 3.5 Å (Table 4.1). The increased freedom of the C atoms results in minimal changes to the range of , and thus the hierarchy of the different cluster-substrate interactions. The only relational difference is the decrease in for (111) face adsorption on GR2-2h when compared to GR2-h, which is noted as being due to distortion of the starting -symmetry geometry. (X) increases throughout due to the greater area of C free movement, directly leading to decreased (Au) values as the vertical displacement of the top HOPG layers increases. Though an Au atom still sits in plane for calculations on GR2-2h and GR2-3h, there is an increased bending in the topmost HOPG layer; and thus greater displacement. The increased planar bending also effects , with values more negative across the board (GR2, GR2-h, GR2-2h and GR2-3h). Calculated interlayer distances and (X) for the isolated HOPG systems with both 3.5 and 7.0 Å of unconstrained C atoms are given in Appendix C.5, reaffirming the observation that the surface bending is predominantly a cluster-induced effect.Table 4.2Structural analysis of cluster on HOPG graphite with and without multiple surface defects as defined for 4.1
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