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ABSTRACT: The effects of the electronic and geometric factors on the global minimum structures of MB9 (-) (M = V, Nb, Ta) are investigated using photoelectron spectroscopy and ab initio calculations. Photoelectron spectra are obtained for MB9 (-) at two photon energies, and similar spectral features are observed for all three species. The structures for all clusters are established by global minima searches and confirmed by comparison of calculated and experimental vertical electron detachment energies. The VB9 (-) cluster is shown to have a planar C2v V©B9 (-) structure, whereas both NbB9 (-) and TaB9 (-) are shown to have Cs M©B9 (-) type structures with the central metal atom slightly out of plane. Theoretical calculations suggest that the V atom fits perfectly inside the B9 ring forming a planar D9h V©B9 (2-) structure, while the lower symmetry of V©B9 (-) is due to the Jahn-Teller effect. The Nb and Ta atoms are too large to fit in the B9 ring, and they are squeezed out of the plane slightly even in the M©B9 (2-) dianions. Thus, even though all three M©B9 (2-) dianions fulfill the electronic design principle for the doubly aromatic molecular wheels, the geometric effect lowers the symmetry of the Nb and Ta clusters.
The Journal of chemical physics 04/2013; 138(13):134315. · 3.09 Impact Factor
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ABSTRACT: The structural and electronic properties for di-tantalum boride clusters Ta(2)B(x) (-) (x = 2-5) were investigated using photoelectron spectroscopy and density functional calculations. The photoelectron spectra for Ta(2)B(x) (-) (x = 2-5) are obtained at several photon energies with rich spectral features. Density functional theory calculations are performed at the BP86 level to search for the global minima of both the anionic and neutral clusters. The calculated vertical electron detachment energies for the global minimum and low-lying isomers are compared with the experimental data. Strong boron-boron bonding is found to dominate the lowest energy structures of Ta(2)B(x) (-) and Ta(2)B(x) (x = 2-5), which are shown to be bipyramidal with the boron atoms forming an equatorial belt around the Ta-Ta dimer. Strong Ta-Ta bonding is observed in Ta(2)B(x) (-) and Ta(2)B(x) for x = 2-4, whereas the Ta-Ta distance is increased significantly in Ta(2)B(5) (-) and Ta(2)B(5).
The Journal of chemical physics 01/2013; 138(3):034308. · 3.09 Impact Factor
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ABSTRACT: We performed a joint photoelectron spectroscopy and ab initio study of two carbon-doped boron clusters, CB(9) (-) and C(2)B(8) (-). Unbiased computational searches revealed similar global minimum structures for both clusters. The comparison of the experimentally observed and theoretically calculated vertical detachment energies revealed that only the global minimum structure is responsible for the experimental spectra of CB(9) (-), whereas the two lowest-lying isomers of C(2)B(8) (-) contribute to the experimental spectra. The planar "distorted wheel" type structures with a single inner boron atom found for CB(9) (-) and C(2)B(8) (-) are different from the quasi-planar structure of B(10) (-), which consists of two inner atoms and eight peripheral boron atoms. The adaptive natural density partitioning chemical bonding analysis revealed that CB(9) (-) and C(2)B(8) clusters exhibit π aromaticity and σ antiaromaticity, which is consistent with their planar distorted structures.
The Journal of chemical physics 12/2012; 137(23):234306. · 3.09 Impact Factor
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Journal of Organometallic Chemistry 12/2012; 721–722:148-154. · 2.38 Impact Factor
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ABSTRACT: Atomic clusters have intermediate properties between that of individual atoms and bulk solids, which provide fertile ground for the discovery of new molecules and novel chemical bonding. In addition, the study of small clusters can help researchers design better nanosystems with specific physical and chemical properties. From recent experimental and computational studies, we know that small boron clusters possess planar structures stabilized by electron delocalization both in the σ and π frameworks. An interesting boron cluster is B(9)(-), which has a D(8h) molecular wheel structure with a single boron atom in the center of a B(8) ring. This ring in the D(8h)-B(9)(-) cluster is connected by eight classical two-center, two-electron bonds. In contrast, the cluster's central boron atom is bonded to the peripheral ring through three delocalized σ and three delocalized π bonds. This bonding structure gives the molecular wheel double aromaticity and high electronic stability. The unprecedented structure and bonding pattern in B(9)(-) and other planar boron clusters have inspired the designs of similar molecular wheel-type structures. But these mimics instead substitute a heteroatom for the central boron. Through recent experiments in cluster beams, chemists have demonstrated that transition metals can be doped into the center of the planar boron clusters. These new metal-centered monocyclic boron rings have variable ring sizes, M©B(n) and M©B(n)(-) with n = 8-10. Using size-selected anion photoelectron spectroscopy and ab initio calculations, researchers have characterized these novel borometallic molecules. Chemists have proposed a design principle based on σ and π double aromaticity for electronically stable borometallic cluster compounds, featuring a highly coordinated transition metal atom centered inside monocyclic boron rings. The central metal atom is coordinatively unsaturated in the direction perpendicular to the molecular plane. Thus, chemists may design appropriate ligands to synthesize the molecular wheels in the bulk. In this Account, we discuss these recent experimental and theoretical advances of this new class of aromatic borometallic compounds, which contain a highly coordinated central transition metal atom inside a monocyclic boron ring. Through these examples, we show that atomic clusters can facilitate the discovery of new structures, new chemical bonding, and possibly new nanostructures with specific, advantageous properties.
Accounts of Chemical Research 12/2012; · 21.64 Impact Factor
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ABSTRACT: Clusters of boron atoms exhibit intriguing size-dependent structures and chemical bonding that are different from bulk boron and may lead to new boron-based nanostructures. We report a combined photoelectron spectroscopic and ab initio study of the 22- and 23-atom boron clusters. The joint experimental and theoretical investigation shows that B(22)(-) and B(23)(-) possess quasi-planar and planar structures, respectively. The quasi-planar B(22)(-) consists of fourteen peripheral atoms and eight interior atoms in a slightly buckled triangular lattice. Chemical bonding analyses of the closed-shell B(22)(2-) species reveal seven delocalized π orbitals, which are similar to those in anthracene. B(23)(-) is a perfectly planar and heart-shaped cluster with a pentagonal cavity and a π-bonding pattern similar to that in phenanthrene. Thus, B(22)(-) and B(23)(-), the largest negatively charged boron clusters that have been characterized experimentally to date, can be viewed as all-boron analogues of anthracene and phenanthrene, respectively. The current work shows not only that boron clusters are planar at very large sizes but also that they continue to yield surprises and novel chemical bonding analogous to specific polycyclic aromatic hydrocarbons.
Journal of the American Chemical Society 10/2012; · 9.91 Impact Factor
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ABSTRACT: A class of transition-metal-centered aromatic boron wheels (D(nh)-M©B(n)(q-)) have been recently produced and characterized according to an electronic design principle. Here we investigate the interplay between electronic and geometric requirements for the molecular wheels using the case of VB(10)(-), which is isoelectronic to the decacoordinated molecular wheels, Ta©B(10)(-) and Nb©B(10)(-). Photoelectron spectra of VB(10)(-) are observed to be broad and complicated with relatively low electron binding energies, in contrast to the simple and high electron binding energies observed for the molecular wheels of its heavier congeners. An unbiased global minimum search found the most stable isomer of VB(10)(-) to be a singlet "boat"-like structure (C(2)), in which the V atom is coordinated to a quasi-planar B(10) unit. A similar triplet C(2v) boat-like isomer is found to be almost degenerate to the C(2) structure, whereas the beautiful molecular wheel structure, D(10h)-V©B(10)(-), is significantly higher in energy on the potential energy surface. Therefore, even though the VB(10)(-) system fulfills the electronic requirement to form a D(10h)-M©B(10)(-) aromatic molecular wheel, the V atom is too small to stabilize the ten-membered boron ring.
Physical Chemistry Chemical Physics 09/2012; 14(39):13663-9. · 3.57 Impact Factor
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ABSTRACT: Dihydrogenated boron clusters, H(2)B(n)(-) (n = 7-12), were produced and characterized using photoelectron spectroscopy and computational chemistry to have ladderlike structures terminated by a hydrogen atom on each end. The two rows of boron atoms in the dihydrides are bonded by delocalized three-, four-, or five-center σ and π bonds. The π bonding patterns in these boron nanoladders bear similarities to those in conjugated alkenes: H(2)B(7)(-), H(2)B(8), and H(2)B(9)(-), each with two π bonds, are similar to butadiene, while H(2)B(10)(2-), H(2)B(11)(-), and H(2)B(12), each with three π bonds, are analogous to 1,3,5-hexatriene. The boron cluster dihydrides can thus be considered as polyene analogues, or "polyboroenes". Long polyboroenes with conjugated π bonds (analogous to polyacetylenes), which may form a new class of molecular wires, should exist.
Journal of the American Chemical Society 07/2012; 134(32):13228-31. · 9.91 Impact Factor
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ABSTRACT: The structures and chemical bonding of the B(21)(-) cluster have been investigated by a combined photoelectron spectroscopy and ab initio study. The photoelectron spectrum at 193 nm revealed a very high adiabatic electron binding energy of 4.38 eV for B(21)(-) and a congested spectral pattern. Extensive global minimum searches were conducted using two different methods, followed by high-level calculations of the low-lying isomers. The global minimum of B(21)(-) was found to be a quasiplanar structure with the next low-lying planar isomer only 1.9 kcal/mol higher in energy at the CCSD(T)/6-311-G* level of theory. The calculated vertical detachment energies for the two isomers were found to be in good agreement with the experimental spectrum, suggesting that they were both present experimentally and contributed to the observed spectrum. Chemical bonding analyses showed that both isomers consist of a 14-atom periphery, which is bonded by classical two-center two-electron bonds, and seven interior atoms in the planar structures. A localized two-center two-electron bond is found in the interior of the two planar isomers, in addition to delocalized multi-center σ and π bonds. The structures and the delocalized bonding of the two lowest lying isomers of B(21)(-) were found to be similar to those in the two lowest energy isomers in B(19)(-).
The Journal of chemical physics 03/2012; 136(10):104310. · 3.09 Impact Factor
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ABSTRACT: Molecular wheels: Decacoordinated molecular wheels, Ta©B(10) (-) and Nb©B(10) (-) , showing the highest coordination number for the central atom in a planar environment at present, were produced in a laser-vaporization supersonic molecular beam and characterized by photoelectron spectroscopy and ab initio calculations. The highly symmetric Ta©B(10) (-) and Nb©B(10) (-) anions are doubly aromatic with six delocalized π electrons and ten delocalized σ electrons.
Angewandte Chemie International Edition 02/2012; 51(9):2101-5. · 13.45 Impact Factor
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The Journal of Chemical Physics. 01/2012; 137(23):234306.
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ABSTRACT: We report the observation of two transition-metal-centered nine-atom boron rings, RhⓒB(9)(-) and IrⓒB(9)(-). These two doped-boron clusters are produced in a laser-vaporization supersonic molecular beam and characterized by photoelectron spectroscopy and ab initio calculations. Large HOMO-LUMO gaps are observed in the anion photoelectron spectra, suggesting that neutral RhⓒB(9) and IrⓒB(9) are highly stable, closed shell species. Theoretical calculations show that RhⓒB(9) and IrⓒB(9) are of D(9h) symmetry. Chemical bonding analyses reveal that these complexes are doubly aromatic, each with six completely delocalized π and σ electrons, which describe the bonding between the central metal atom and the boron ring. This work establishes firmly the metal-doped B rings as a new class of novel aromatic molecular wheels.
Journal of the American Chemical Society 12/2011; 134(1):165-8. · 9.91 Impact Factor
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ABSTRACT: The structures and the electronic properties of two aluminum-doped boron clusters, AlB(7)(-) and AlB(8)(-), were investigated using photoelectron spectroscopy and ab initio calculations. The photoelectron spectra of AlB(7)(-) and AlB(8)(-) are both broad, suggesting significant geometry changes between the ground states of the anions and the neutrals. Unbiased global minimum searches were carried out and the calculated vertical electron detachment energies were used to compare with the experimental data. We found that the Al atom does not simply replace a B atom in the parent B(8)(-) and B(9)(-) planar clusters in AlB(7)(-) and AlB(8)(-). Instead, the global minima of the two doped-clusters are of umbrella shapes, featuring an Al atom interacting ionically with a hexagonal and heptagonal pyramidal B(7) (C(6v)) and B(8) (C(7v)) fragment, respectively. These unique umbrella-type structures are understood on the basis of the special stability of the quasi-planar B(7)(3-) and planar B(8)(2-) molecular wheels derived from double aromaticity.
The Journal of chemical physics 09/2011; 135(10):104301. · 3.09 Impact Factor
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Angewandte Chemie International Edition 08/2011; 50(40):9334-7. · 13.45 Impact Factor
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ABSTRACT: The structures and the electronic properties of two Al-doped boron clusters, AlB(9)(-) and AlB(10)(-), were investigated via joint photoelectron spectroscopy and high-level ab initio study. The photoelectron spectra of both anions are relatively broad and have no vibrational structure. The geometrical structures were established by unbiased global minimum searches using the Coalescence Kick method and comparison between the experimental and calculated vertical electron detachment energies. The results show that both clusters have quasi-planar structures and that the Al atom is located at the periphery. Chemical bonding analysis revealed that the global minimum structures of both anions can be described as doubly (σ- and π-) aromatic systems. The nona-coordinated wheel-type structure of AlB(9)(-) was found to be a relatively high-lying isomer, while a similar structure for the neutral AlB(9) cluster was previously shown to be either a global minimum or a low-lying isomer.
The Journal of Physical Chemistry A 08/2011; 115(38):10391-7. · 2.95 Impact Factor
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ABSTRACT: Small boron clusters have been shown to be planar from a series of combined photoelectron spectroscopy and theoretical studies. However, a number of boron clusters are quasiplanar, such as B(7)(-) and B(12)(-). To elucidate the nature of the nonplanarity in these clusters, we have investigated the electronic structure and chemical bonding of two isoelectronic Al-doped boron clusters, AlB(6)(-) and AlB(11)(-). Vibrationally resolved photoelectron spectra were obtained for AlB(6)(-), resulting in an accurate electron affinity (EA) for AlB(6) of 2.49 ± 0.03 eV. The photoelectron spectra of AlB(11)(-) revealed the presence of two isomers with EAs of 2.16 ± 0.03 and 2.33 ± 0.03 eV, respectively. Global minimum structures of both AlB(6)(-) and AlB(11)(-) were established from unbiased searches and comparison with the experimental data. The global minimum of AlB(6)(-) is nearly planar with a central B atom and an AlB(5) six membered ring, in contrast to that of B(7)(-), which possesses a C(2v) structure with a large distortion from planarity. Two nearly degenerate structures were found for AlB(11)(-) competing for the global minimum, in agreement with the experimental observation. One of these isomers with the lower EA can be viewed as substituting a peripheral B atom by Al in B(12)(-), which has a bowl shape with a B(9) outer ring and an out-of-plane inner B(3) triangle. The second isomer of AlB(11)(-) can be viewed as an Al atom interacting with a B(11)(-) cluster. Both isomers of AlB(11)(-) are perfectly planar. It is shown that Al substitution of a peripheral B atom in B(7)(-) and B(12)(-) induces planarization by slightly expanding the outer ring due to the larger size of Al.
Journal of the American Chemical Society 06/2011; 133(22):8646-53. · 9.91 Impact Factor
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ABSTRACT: In this joint experimental and theoretical work we present a novel type of structural transition occurring in the series of C(x)B(8-x)(-) (x=1-8) mixed clusters upon increase of the carbon content from x=2 to x=3. The wheel to ring transition is surprising because it is rather planar-to-linear type of transition to be expected in the series since B(8), B(8)(-), B(8)(2-) and CB(7)(-) are known to possess wheel-type global minimum structures while C(8) is linear.
Physical Chemistry Chemical Physics 05/2011; 13(19):8805-10. · 3.57 Impact Factor
