Free-standing boron nanocages or borospherenes have been observed recently for B40(-) and B40. There is evidence that a family of borospherenes may exist. However, the smallest borospherene is still not known. Here, we report experimental and computational evidence of a seashell-like borospherene cage for B28(-) and B28. Photoelectron spectrum of B28(-) indicated contributions from different isomers. Theoretical calculations showed that the seashell-like B28(-) borospherene is competing for the global minimum with a planar isomer and it is shown to be present in the cluster beam, contributing to the observed photoelectron spectrum. The seashell structure is found to be the global minimum for neutral B28 and the B28(-) cage represents the smallest borospherene observed to date. It is composed of two triangular close-packed B15 sheets, interconnected via the three corners by sharing two boron atoms. The B28 borospherene was found to obey the 2(n + 1)(2) electron-counting rule for spherical aromaticity.
A planar, elongated B15(+) cationic cluster is shown to be structurally fluxional and functions as a nanoscale tank tread on the basis of electronic structure calculations, bonding analyses, and molecular dynamics simulations. The outer B11 peripheral ring behaves like a flexible chain gliding around an inner B4 rhombus core, almost freely at the temperature of 500 K. The rotational energy barrier is only 1.37 kcal mol(-1) (0.06 eV) at the PBE0/6-311+G* level, further refined to 1.66 kcal mol(-1) (0.07 eV) at the single-point CCSD(T)/6-311G*//CCSD/6-311G* level. Two soft vibrational modes of 166.3 and 258.3 cm(-1) are associated with the rotation, serving as double engines for the system. Bonding analysis suggests that the "island" electron clouds, both σ and π, between the peripheral ring and inner core flow and shift continuously during the intramolecular rotation, facilitating the dynamic fluxionality of the system with a small rotational barrier. The B15(+) cluster, roughly 0.6 nm in dimension, is the first double-axle nanoscale tank tread equipped with two engines, which expands the concepts of molecular wheels, Wankel motors, and molecular tanks.
Gas-phase clusters are deemed to be σ-aromatic when they satisfy the 4n+2 rule of aromaticity for delocalized σ electrons and fulfill other requirements known for aromatic systems. While the range of n values was shown to be quite broad when applied to short-lived clusters found in molecular-beam experiments, stability of all-metal cluster-like fragments isolated in condensed phase was previously shown to be mainly ascribed to two electrons (n=0). In this work, the applicability of this concept is extended towards solid-state compounds by demonstrating a unique example of a storable compound, which was isolated as a stable [K([2.2.2]crypt)] salt, featuring a [Au Sb ] cluster core possessing two all-metal aromatic AuSb fragments with six delocalized σ electrons each (n=1). This discovery pushes the boundaries of the original idea of Kekulé and firmly establishes the usefulness of the σ-aromaticity concept as a general idea for both small clusters and solid-state compounds.
Boron oxide clusters offer intriguing molecular models for the electron-deficient system, in which the boronyl (BO) group plays a key role and the interplay between the localized BO triple bond and the multicenter electron delocalization dominates the chemical bonding. Here we report the structural, electronic, and bonding properties of the B4O4(+) cationic cluster on the basis of unbiased Coalescence Kick global-minimum searches and first-principles electronic structural calculations at the B3LYP and single-point CCSD(T) levels. The B4O4(+) cluster is shown to possess a Cs (1, (2)A') global minimum. It represents the smallest boron oxide species with a hexagonal boroxol (B3O3) ring as the core, terminated by a boronyl group. Chemical bonding analyses reveal double (π and σ) aromaticity in Cs B4O4(+), which closely mimics that in the 3,5-dehydrophenyl cation C6H3(+) (D3h, (1)A1'), a prototypical molecule with double aromaticity. Alternative D2h (2, (2)B3g) and C2v (3, (2)A1) isomeric structures of B4O4(+) are also analyzed, which are relevant to the global minima of B4O4 neutral and B4O4(-) anion, respectively. These three structural motifs vary drastically in terms of energetics upon changing the charge state, demonstrating an interesting case in which every electron counts. The calculated ionization potentials and electron affinities of the three corresponding neutral isomers are highly uneven, which underlie the conformational changes in the B4O4(+/0/-) series. The current work presents the smallest boron oxide species with a boroxol ring, establishes an analogy between boron oxides and the 3,5-dehydrophenyl cation, and enriches the chemistry of boron oxides and boronyls.
The bowl-shaped C B cluster with a central hexagon hole is considered an ideal molecular model for low-dimensional boron-based nanosystems. Owing to the electron deficiency of boron, chemical bonding in the B cluster is intriguing, complicated, and has remained elusive despite a couple of papers in the literature. Herein, a bonding analysis is given through canonical molecular orbitals (CMOs) and adaptive natural density partitioning (AdNDP), further aided by natural bond orbital (NBO) analysis and orbital composition calculations. The concerted computational data establish the idea of concentric double π aromaticity for the B cluster, with inner 6π and outer 18π electron counting, which both conform to the (4n+2) Hückel rule. The updated bonding picture differs from existing knowledge of the system. A refined bonding model is also proposed for coronene, of which the B cluster is an inorganic analogue. It is further shown that concentric double π aromaticity in the B cluster is retained and spatially fixed, irrespective of the migration of the hexagonal hole; the latter process changes the system energetically. The hexagonal hole is a destabilizing factor for σ/π CMOs. The central hexagon hole affects substantially fewer CMOs, thus making the bowl-shaped C B cluster the global minimum.
The concept of boronyl (BO) and the BO/H isolobal analogy build an interesting structural link between boron oxide clusters and hydrocarbons. Based upon global-minimum searches and first-principles electronic structural calculations, we present here the perfectly planar C2v B5O5 (+) (1, (1)A1), C2v B5O5 (2, (2)A1), and tetrahedral Cs B5O5 (-) (3, (1)A') clusters, which are the global minima of the systems. Structural and molecular orbital analyses indicate that C2v B5O5 (+) (1) [B3O3(BO)2 (+)] and C2v B5O5 (2) [B3O3(BO)2] feature an aromatic six-membered boroxol (B3O3) ring as the core with two equivalent boronyl terminals, similar to the recently reported boronyl boroxine D3h B6O6 [B3O3(BO)3]; whereas Cs B5O5 (-) (3) [B(BO)3(OBO)(-)] is characterized with a tetrahedral B(-) center, terminated with three BO groups and one OBO unit, similar to the previously predicted boronyl methane Td B5O4 (-) [B(BO)4 (-)]. Alternatively, the 1-3 clusters can be viewed as the boron oxide analogs of phenyl cation C6H5 (+), phenyl radical C6H5, and chloromethane CH3Cl, respectively. Chemical bonding analyses also reveal a dual three-center four-electron (3c-4e) π hyperbond in Cs B5O5 (-) (3). The infrared absorption spectra of B5O5 (+) (1), B5O5 (2), and B5O5 (-) (3) and anion photoelectron spectrum of B5O5 (-) (3) are predicted to facilitate their forthcoming experimental characterizations. The present work completes the BnOn (+/0/-) series for n = 1-6 and enriches the analogous relationship between boron oxides and hydrocarbons.
Gas-phase clusters are deemed to be s-aromatic when they satisfy the 4n + 2rule of aromaticity for delocalized s electrons and fulfill other requirements knownf or aromatic systems.W hile the range of nvalues was shown to be quite broad when applied to short-lived clusters found in molecularbeam experiments,s tability of all-metal cluster-like fragments isolated in condensed phase was previously shown to be mainly ascribed to two electrons (n = 0). In this work, the applicability of this concept is extended towards solid-state compounds by demonstrating au nique example of as torable compound, which was isolated as astable [K([2.2.2]crypt)] + salt, featuring a[ Au 2 Sb 16 ] 4À cluster core possessing two all-metal aromatic AuSb 4 fragments with six delocalized s electrons each (n = 1). This discovery pushes the boundaries of the original idea of KekulØ and firmly establishes the usefulness of the s-aromaticity concept as ag eneral idea for both small clusters and solid-state compounds.Although the original concept of aromaticity in chemistry was put forward by August KekulØ [1] more than 150 years ago, it currently occupies am assive niche in modern chemistry. [2] Theconcepts of p aromaticity/antiaromaticity were primarily used to explain chemical bonding in organic compounds. Today,t hese terms are well used for av ariety of molecules, including inorganic compounds.A longside,t hese concepts have also gained huge popularity as more and more chemical species are being discovered, where delocalized bonding is used to describe the structures.I n1 995, Robinson and coworkers reported [3] thes ynthesis of Na 2 [[(2,4,6-Me 3 C 6 H 2 ) 2 C 6 H 3 ]Ga] 3 with two p electrons delocalized over the three gallium atoms that make the system p-aromatic according to the Hückel rule.Recently,the first solid-state allmetal p-antiaromatic compounds [Ln(h 4 -Sb 4 ) 3 ] 3À (Ln = La, Y, Ho,E r, Lu) were synthesized and characterized. [4] The [U@Bi 12 ] 3À anion with similar geometry was reported very recently by Dehnen and co-workers. [5] Thea romaticity/ antiaromaticity concept was also extended to bare metal clusters found in the gas phase. [6] Fort he first time,t he saromaticity concept was shown to be applicable to small alkali metal and alkaline earth metal clusters. [7] Modern developments on aromaticity in various aromatic/antiaromatic chemical species composed of main-group elements and transition metals have been extensively reviewed elsewhere. [8][9][10][11] Fora ll all-metal aromatic fragments that have been synthesized in the solid state up to date,t here were only two delocalized electrons responsible for the s-aromaticity of the compounds,asexemplified by the cases of Pd 3 + ,Au 3 + ,and TiSn 2 clusters. [12][13][14] Thus far,w ea re not aware of any solidstate compounds containing two all-metal s-aromatic fragments involving six delocalized electrons each. Hence,the 6s-electron aromatic fragments found in the [Au 2 Sb 16 ] 4À cluster in this study expand the family of storable aromatic metal clusters thus solidifying ...
In a recent communication, an all-metal aromatic sandwich [Sb3Au3Sb3](3-) was synthesized and characterized. We report herein a density-functional theory (DFT) study on the chemical bonding of this unique cluster, which makes use of a number of computational tools, including the canonical molecular orbital (CMO), adaptive natural density partitioning (AdNDP), Wiberg bond index, and orbital composition analyses. The 24-electron, triangular prismatic sandwich is intrinsically electron-deficient, being held together via six Sb-Sb, three Au-Au, and six Sb-Au links. A standard, qualitative bonding analysis suggests that all CMOs are primarily located on the three Sb3/Au3/Sb3 layers, three Au 6s based CMOs are fully occupied, and the three extra charges are equally shared by the two cyclo-Sb3 ligands. This bonding picture is referred to as the zeroth order model, in which the cluster can be formally formulated as [Sb3(1.5+)Au3(3-)Sb3(1.5+)](3-) or [Sb3(0)Au3(3-)Sb3(0)]. However, the system is far more complex and covalent than the above picture. Seventeen CMOs out of 33 in total involve remarkable Sb → Au electron donation and Sb ← Au back-donation, which are characteristic of covalent bonding and effectively redistribute electrons from the Sb3 and Au3 layers to the interlayer edges. This effect collectively leads to three Sb-Au-Sb three-center two-electron (3c-2e) σ bonds as revealed in the AdNDP analyses, despite the fact that not a single such bond can be identified from the CMOs. Orbital composition analyses for the 17 CMOs allow a quantitative understanding of how electron donation and back-donation redistribute the charges within the system from the formal Sb3(0)/Au3(3-) charge states in the zeroth order model to the effective Sb3(1.5-)/Au3(0) charge states, the latter being revealed from the natural bond orbital analysis.
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