Local electronic structure of dicarba-closo-dodecarboranes C2B10H12

We report nonresonant inelastic X-ray scattering (NRIXS) measurement of core-shell excitations from both B 1s and C 1s initial states in all three isomers of the dicarba-closo-dodecarboranes C2B10H12. First, these data yield an experimental determination of the angular-momentum-projected final local density of states (l-DOS). We find low-energy resonances with distinctive local s- or p-type character, providing a more complete experimental characterization of bond hybridization than is available from dipole-transition limited techniques, such as X-ray absorption spectroscopies. This analysis is supported by independent density functional theory and real-space full multiple scattering calculation of the l-DOS which yield a clear distinction between tangential and radial contributions. Second, we investigate the isomer sensitivity of the NRIXS signal and compare and contrast these results with prior electron energy loss spectroscopy measurements. This work establishes NRIXS as a valuable tool for borane chemistry, not only for the unique spectroscopic capabilities of the technique but also through its compatibility with future studies in solution or in high-pressure environments. In addition, this work also establishes the real-space full multiple scattering approach as a useful alternative to traditional approaches for excited states calculations of aromatic polyhedral boranes and related systems.     

The electronic structure ofα-B12, B12P2 and B12AS2

The electronic band structures of the rhombohedral-based boron compounds -B₁₂, B₁₂P₂ and B₁₂ As₂ have been investigated along all symmetry directions. The calculations show that the band gap, in all cases, is of the order of 2 eV, which correlates with the known color of -rhombohedral boron. The materials should be intrinsic semi-conductors, as has recently been shown experimentally. The states around the band gap in -B₁₂ are dominated by the boron 2p atomic states. The bonding in the icosahedra, as illuminated by cluster calculations, is shown to be rather similar to that in the isolated B₁₂ icosahedron. Of the intericosahedron interactions, those between B(2) and B(2) atoms are the strongest and have a bond index just above unity. In B₁₂P₂ the orbitals of the P₂ moiety make a significant contribution to the valence band edge states and the conduction band edge states also incorporate considerable (55%) phosphorus 3d orbital character. In B₁₂As₂ the arsenic 4d orbitals do not have as much effect in that crystal as do the 3d orbitals in B₁₂P₂.     

Thermal transformations of B10H12(NH3)2, B10H12(C5H5N)2, and B10H12(C9H7N)2

Conclusions For B₁₀H₁₂L₂, where L=NH₃, C₅H₅N, or C₉H₇N, features of thermal transformations in the range 25–850°C and the composition of the pyrolysis products are determined. The latter are x-ray amorphous phases, containing nitride, carbide, boron carbide, boron, and carbon.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya, No. 11, pp. 2481–2484, November, 1988.     

ChemInform Abstract: Structures of arachno‐ and hypho‐B10 Clusters and Stability of Their Possible Lewis Base Adducts ([B10H12]2‐, [B10H12×L]2‐, [B10H12×2L]2‐, [B10H13]‐, [B10H13×L]‐, [B10H12×2L]). An ab initio/IGLO/NMR Investigation.

ChemInform is a weekly Abstracting Service, delivering concise information at a glance that was extracted from about 100 leading journals. To access a ChemInform Abstract of an article which was published elsewhere, please select a “Full Text” option. The original article is trackable via the “References” option.     

Crown compounds for anions: sandwich and half-sandwich complexes of cyclic trimetric perfluoro-o-phenylenemercury with polyhedral closo-[B10H10]2- and closo-[B12H12]2- anions

It has been shown by IR and NMR spectroscopy that cyclic trimeric perfluoro-o-phenylenemercury (o-C6F4-Hg)3 (1) is capable of binding closo-[B10H10]2- and closo-[B12H12]2- anions to form complexes [[(o-C6F4Hg)3](B10-H10)]2- (2), [[(o-C6F4Hg)3]2(B10H10)]2-(3), [[(o-C6F4Hg)3](B12H12)]2- (4), and [[(o-C6F4Hg)3]2(B12H12)]2- (5). According to IR data, the bonding of the [B10H10]2- and [B12H12]2- ions to the macrocycle in these complexes is accomplished through the formation of B-H-Hg bridges. Complexes 2, 3, and 5 have been isolated in analytically pure form and have been characterized by spectroscopic means. X-ray diffraction studies of 3 and 5 have revealed that these compounds have unusual sandwich structures, in which the polyhedral di-anion is located between the planes of two molecules of 1 and is bonded to each of them through two types of B-H-Hg bridges. One type is the simultaneous coordination of a B-H group to all three Hg atoms of the macrocycle. The other type is the coordination of a B-H group to a single Hg atom of the cycle. According to X-ray diffraction data, complex 2 has an analogous but half-sandwich structure. The obtained complexes 2-5 are quite stable; their stability constants in THF/acetone (1:1) at 20 degrees C have been determined as 1.0 x 10(2)Lmol(-1), 2.6 x 10(3)L(2)mol(2), 0.7 x 10(2)Lmol(-1), and 0.98 x 10(3)L(2)mol(-2), respectively.     

The electronic structure of the B2H 5 + ion

The B₂H ₅ ⁺ ion has been studied using theab initio SCF method employing a basis set of Gaussian orbitals and various semi-empirical methods. The most stable structure appears to be a planar structure with two vacantp orbitals rather than a triply bridged structure suggested by analogy with acetylene with which it is isoelectronic. The semi-empirical results reinforce earlier conclusions that inclusion of charges from neighbouring atoms in iterative Extended Hückel methods is necessary to satisfactorily treat ionic molecules.

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Zusammenfassung Das B₂H ₅ ⁺ -Ion ist mit Hilfe derab initio SCF-Methode unter Benutzung eines Basissatzes von Gaußorbitalen und mit verschiedenen semiempirischen Methoden untersucht worden. Die stabilste Struktur scheint eine planare Struktur mit zwei leerenp-Orbitalen und nicht eine dreifach verbrückte Struktur zu sein, wie sie durch Analogiebetrachtungen am Acetylen nahegelegt wird. Durch die semiempirischen Resultate werden die bereits früher erhaltenen Ergebnisse bestätigt, daß zur zufriedenstellenden Behandlung von Molekülionen mit iterativen erweiterten Hückel-Methoden die Berücksichtigung der Ladungen benachbarter Atome nötig ist.

     

The structures of MeP(C2B10H10)2CH2 and MeAs(C2B10H10)2, compounds containing o-carborane ring carbon atoms in the heterocycle

Conclusions Crystal and molecular structures have been determined for 1-methylphospha-2,3,5,6-bis-o-carboranocyclohexane and 1-methylarsa-2,3,4,5-bis-o-carboranocyclopentane.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya, No. 7, pp. 1523–1528, July, 1979.     

Molecular and electronic structure of Br2O

Br₂O has been studied with the aid of ab initio calculation and an extended basis set. The calculated geometry is in good agreement with the experimental one measured in the condensed phase. A qualitative analysis of chemical bonding and ionization energies is given and dipole moment predicted for a free molecule.     

Crystal structure of di (1-n-dodecylpyridine) decahydro-closo-decaborate(2-) (C5H5N-C12H25)2[B10H10]

Using X-ray analysis, we have determined the crystal structure of di(1-n-dodecylpyridine) decahydrocloso-decaborate(2-), (py-C₁₂H₂₅)₂[B₁₀H₁₀] (I), a yellow salt-like substance obtained by reaction of (py-C₁₂H₂₅)Br and K₂[B₁₀H₁₀] in an aqueous solution. Compound I melts at 125⁰ without decomposition and luminesces under ultraviolet radiation (λ_max=555 nm at 298 K). In I, quaternary pyridine bases, containing a hydrocarbon radical with the C₁₂ chain, are combined with the closo-cluster hydroborate anion [B₁₀H₁₀]^2-. This results in a charge transfer structure having shortened nonvalent (equatorial B) H.…H(C of pyridine) contacts of 2.41(8) Å. Crystals I are orthorhombic with a=8.584 (1), b=7.739(1), c=31.183(5) Å, V_cell=2071.4(5) ų, space group Pnmm, Z=2, d_calc=0.986 g/cm³ (a Syntex P2₁ automatic diffractometer, λCUK_α, N_msd/used=1654/711, R_aniso=0.076, R_w=0.080, w=1/(σ(F_obs)²+0.0007·F _obs ² ). Substantial changes are observed in the vibration range of the valent B?H bonds in the IR spectrum of I as compared to that of pure ionic K₂[B₁₀H₁₀], confirming the interaction.