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The compound bis(acetylacetonato)dichlorotin(IV) [Sn(acac)2Cl2] forms a distorted octahedral structure involving both oxygen atoms of the acetylacetone group. The two chlorides occupy the cis position, with Sn-Cl distances of Sn1-Cl1 = 2.380(2) Å, Sn1-O1 = 2.043(2) Å and Sn1-O2 = 2.093(2) Å. We report here a new and simple method for the synthesis of Sn(acac)2Cl2, its spectroscopic characterization and, for the first time, we report its crystal structure. 相似文献
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Wenzel Davidsohn Bernard R. LaliberteCharles M. Goddard Malcolm C. Henry 《Journal of organometallic chemistry》1972
Dimethyl- and diphenylbis(p-hydroxyphenyl) Group IV metal compounds have been synthesized. Scope and limitations of the following methods were investigated: (a) reaction of the halogen-metal exchange product of p-bromophenol and n-butyllithium with organometallic dihalides; (b) protection of the phenolic group with trimethyl or benzyl groups and subsequent hydrolysis or hydrogenolysis. 相似文献
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Silver J Frampton CS Fern GR Davies DA Miller JR Sosa-Sanchez JL 《Inorganic chemistry》2001,40(21):5434-5439
Three newly elucidated crystal structures of group IV phthalocyaninato complexes are reported, along with data for two further SiPc carboxylate complexes. In one of these crystal structures, bis(undecylcarboxylate)Sn(IV) phthalocyanine, the tin ion is seven coordinate, which is a unique finding for this atom in phthalocyanine ring coordination. Comparison of these structures with other group IV phthalocyaninato and related structures reveals differences, illustrating features significant in the chemistries of Si(IV) and Sn(IV) ions. These differences are thought to originate from their differing sizes and polarizabilities. The structures show that the Sn(IV) ion can only occupy an in-plane location in the phthalocyaninato ring where it elongates toward the two axial ligands. When the axial ligands do not facilitate this elongation cis coordination is preferred and the Sn(IV) ion sits above the phthalocyaninato ring plane. In contrast, the Si(IV) structures, with smaller, harder (i.e., less polarizable) Si(IV) ions, are six coordinate with the Si(IV) ion in the phthalocyaninato ring plane in a distorted octahedral symmetry. The electronic spectra and cyclic voltammetry of some of the Si compounds indicate that on the electrode the oxidized/reduced species behave as though they are in a solid film, rather than a soluble freely diffusing species. 相似文献
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Conclusions The barriers of rotation around the C-N bond in the amides C5H5CoB9H9C2HCON(CH3)2, 1-(CH3)2NCO-1, 2-B10C2H11 and 1-(CH3)2NCO-1,7-B10C2H11 are substantially lower than in ordinary amides.Translated from Izvestiya Akademii Nauk SSSR, Seriya Khimicheskaya, No. 9, pp. 2119–2120, September, 1977. 相似文献
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A distorted octahedron C2S4 geometry is found for the tin atom in the title compound; C? Sn? C is 136.61(19)°. Copyright © 2004 John Wiley & Sons, Ltd. 相似文献
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Alexandru T. Balaban Cornelia Uncuţ/a Mihai Elian Filip Chiraleu Antonie Dinculescu 《Tetrahedron》1984,40(13):2547-2553
Pairwise chemical shift nonequivalence of the 2,6-methyl and 3,5-protons in 1H NMR spectra, as well as of the 2,6-methyl, 2,6-ring and 3,5-ring carbons in 13C NMR spectra, was observed for N-alkyl-2,4,6-trimethylpyridinium salts 2. Dynamic NMR spectroscopy demonstrates appreciably higher activation free energies ΔG# for rotation around the N(sp2)-C(sp3 bond than ΔG# for the analogously substituted mesityl derivatives, in agreement with the shorter N-C bond distance than for the C-C bond. 相似文献
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《Journal of Inorganic and Nuclear Chemistry》1978,40(4):607-611
Bis(acetylacetonato)oxovanadium(IV), VO(acac)2, reacts with 1,10-phenanthroline in methanol to afford an adduct VO(acac)2(phen) · 2CH3OH (1). The IR and electronic spectra of 1 show a close resemblance to those of the corresponding α- and β-naphthoquinoline adducts, and 1 is assumed to have a trans octahedral structure containing the phenanthroline molecule as a unidentate ligand. Although 1 attains a reversible dissociation equilibrium in dichloromethane, the trifluoroacetylacetonato complex VO(tfac)2(phen) (2) is quite stable even in solution. The cis octahedral structure is assigned to 2 and also to the corresponding pyridine, α- and β-naphthoquinoline adducts VO(tfac)2L on the basis of IR data. 相似文献
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Pere M. Deyà Antonio Frontera Guillem A. Suñer David Quiñonero Carolina Garau Antoni Costa Pau Ballester 《Theoretical chemistry accounts》2002,108(3):157-167
The structural and energetic changes associated with C–N bond rotation in a squaric acid derivative as well as in formamide,
3-aminoacrolein and vinylamine have been studied theoretically using ab initio molecular orbital methods. Geometry optimizations
at the MP2(full)/6-31+G* level confirmed an increase in the C–N bond length and a smaller decrease in the C=O length on going
from the equilibrium geometry to the twisted transition state. Other geometrical changes are also discussed. Energies calculated
at the QCISD(T)/6-311+G** level, including zero-point-energy correction, show barrier heights decreasing in the order formamide,
squaric acid derivative, 3-aminoacrolein and vinylamine. The origin of the barriers were examined using the atoms-in-molecules
approach of Bader and the natural bond orbital population analysis. The calculations agree with Pauling's resonance model,
and the main contributing factor of the barrier is assigned to the loss of conjugation on rotating the C–N bond. Finally,
molecular interaction potential calculations were used to study the changes in the nucleophilicity of N and O (carbonyl) atoms
upon C–N rotation, and to obtain a picture of the abilities of the molecules to act in nonbonded interactions, in particular
hydrogen bonds. The molecular interaction potential results confirm the suitability of squaramide units for acting as binding
units in host–guest chemistry.
Received: 13 March 2002 / Accepted: 23 June 2002 / Published online: 21 August 2002 相似文献
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Silver J Marsh PJ Symons MC Svistunenko DA Frampton CS Fern GR 《Inorganic chemistry》2000,39(13):2874-2881
The crystal structure of the title compound is presented and shown to be one of a class of low-spin iron porphyrin complexes having a ground-state electronic configuration of (dxy)2(dxz)2(dyz)1. If their Fe-N bond lengths (average N-porphyrin plotted against average N-axial) are considered, this class of low-spin iron(III) porphyrins of general formula [Fe(III)Por(L)2]+X- and of 2B ground state is shown to be distinctly different crystallographically from a similar class of compounds with the same general formula but with a 2E or a (dxy)2(dxz,dyz)3 ground state. A third group of compounds with the same general formula have a (dxz,dyz)4(d)1 ground state and again are in a different region of the plot. Compounds showing intermediate properties can be forecast from the simple relationship presented in this work. The electron paramagenetic resonance data are shown to be dependent on the ground state, and those of configuration (dxy)2(dxz,dyz)3 and the 2B ground state obey a correlation previously suggested in the literature. 相似文献
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