The most characteristic feature of planar π-aromatics is the ability to sustain a long-range shielding cone under a magnetic field oriented in a specific direction. In this article, we showed that similar magnetic responses can be found in σ-aromatic and spherical aromatic systems. For [Au 13 ] 5+ , long-range characteristics of the induced magnetic field in the bare icosahedral core are revealed, which are also found in the ligand protected [Au 25 (SH) 18 ] − model, proving its spherical aromatic properties, also supported by the AdNDP analysis. Such properties are given by the 8-ve of the structural core satisfying the Hirsch 2( N + 1) 2 rule, which is also found in the isoelectronic [M@Au 12 ] 4+ core, a part of the [MAu 24 (SR) 18 ] 2− (M = Pd, Pt) cluster. This contrasts with the [M@Au 12 ] 6+ core in [MAu 24 (SR) 18 ] 0 (M = Pd, Pt), representing 6-ve superatoms, which exhibit characteristics of planar σ-aromatics. Our results support the spherical aromatic character of stable superatoms, whereas the 6-ve intermediate electron counts satisfy the 4 N + 2 rule (applicable for both π- and σ-aromatics), showing the reversable and controlled interplay between 3D spherical and 2D σ-aromatic clusters. 
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                            Ligand exchange on Au 38 (SR) 24 : substituent site effects of aromatic thiols
                        
                    
    
            Understanding the critical roles of ligands ( e.g. thiolates, SR) in the formation of metal nanoclusters of specific sizes has long been an intriguing task since the report of ligand exchange-induced transformation of Au 38 (SR) 24 into Au 36 (SR′) 24 . Herein, we conduct a systematic study of ligand exchange on Au 38 (SC 2 H 4 Ph) 24 with 21 incoming thiols and reveal that the size/structure preference is dependent on the substituent site. Specifically, ortho -substituted benzenethiols preserve the structure of Au 38 (SR) 24 , while para - or non-substituted benzenethiols cause its transformation into Au 36 (SR) 24 . Strong electron-donating or -withdrawing groups do not make a difference, but they will inhibit full ligand exchange. Moreover, the crystal structure of Au 38 (SR) 24 (SR = 2,4-dimethylbenzenethiolate) exhibits distinctive π⋯π stacking and “anagostic” interactions (indicated by substantially short Au⋯H distances). Theoretical calculations reveal the increased energies of frontier orbitals for aromatic ligand-protected Au 38 , indicating decreased electronic stability. However, this adverse effect could be compensated for by the Au⋯H–C interactions, which improve the geometric stability when ortho -substituted benzenethiols are used. Overall, this work reveals the substituent site effects based on the Au 38 model, and highlights the long-neglected “anagostic” interactions on the surface of Au-SR NCs which improve the structural stability. 
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                            - PAR ID:
- 10172598
- Date Published:
- Journal Name:
- Nanoscale
- Volume:
- 12
- Issue:
- 17
- ISSN:
- 2040-3364
- Page Range / eLocation ID:
- 9423 to 9429
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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