1,727,053 research outputs found

    Synthesis and luminescence behavior of rhenium(I) triynyl complexes. X-ray crystal structures of [Re(CO)3(tBu2bpy)(C=C-C=C-C=CPh)]and [Re(CO)3(Me2bpy)(C=C-C=C-C=CSiMe3)]

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    Luminescent rhenium(I) triynyl complexes [Re(CO)3(tBu2bpy)(C-C-C=C-C=CPh)] 1, [Re(CO)3(tBu2bpy)(C=C-C=C-C=CSiMe3)] 2, and [Re(CO)3(Me2bpy)(C=C-C=C-C= CSiMe3)] 3, were synthesized and their photophysical and electrochemical properties studied. The X-ray crystal structures of 1 and 3 have also been determined. A comparison study of their emission properties to that of their mono- and diynyl analogues was made and their emission origin suggested and supported by EHMO studies. © 2000 American Chemical Society.link_to_subscribed_fulltex

    Heptahexaenylidene Complexes:  Synthesis and Characterization of the First Complexes with an MCCCCCCCR<sub>2</sub> Moiety (M = Cr, W)

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    Silica-induced elimination of dimethylamide from [(CO)5M(C⋮C)3C(NMe2)3]- [M = Cr (4a), W (4b)] affords the first isolated and characterized heptahexaenylidene complexes [(CO)5MCCCCCCC(NMe2)2] (5a,b). Complexes 4a,b were generated by sequential reaction of Me3Si(C⋮C)3SiMe3 with LiMe·LiBr, [(Me2N)3C]+Cl-, LiBu, and [(CO)5M(thf)]. Complex 5b is inert in methanol, but adds dimethylamine across the C5C6 bond to give [(CO)5WCCCCC{CHC(NMe2)2}NMe2]. The reaction of 5a,b with LiMe·LiBr and SiO2 generates the heptahexaenylidene complexes [(CO)5MCCCCCCC(Me)NMe2] (8a,b). Trapping of 8b with HNMe2 yields pentatetraenylidene complex [(CO)5WCCCCC{CHC(Me)NMe2}NMe2]

    Microwave Spectra of Four New Perfluoromethyl Polyyne Chains:  Trifluoropentadiyne, CF<sub>3</sub>C⋮CC⋮CH, Trifluoroheptatriyne, CF<sub>3</sub>C⋮CC⋮CC⋮CH, Tetrafluoropentadiyne, CF<sub>3</sub>C⋮CC⋮CF, and Trifluoromethylcyanoacetylene, CF<sub>3</sub>C⋮CC⋮N

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    Four fluoromethyl polyynes, 5,5,5-trifluoro-1,3-pentadiyne, CF3C⋮CC⋮CH, 7,7,7-trifluoro-1,3,5-heptatriyne, CF3C⋮CC⋮CC⋮CH, 1,5,5,5-tetrafluoro-1,3-pentadiyne, CF3C⋮CC⋮CF, and 4,4,4-trifluoro-1-nitrile-2-butyne, CF3C⋮CC⋮N, were studied by pulsed-jet Fabry Perot Fourier transform microwave spectroscopy. The molecules were produced by pulsed high voltage discharges of dilute mixtures of precursor gases such as trifluoropropyne in an argon carrier pulsed jet. The carbon-13 and deuterium substituted isotopomers of trifluoropentadiyne were studied, and the molecular structure was determined

    Cationic and Neutral [4]-Cumulenes CCCCC with Five Cumulated Carbons and Three to Four Ferrocenyl Termini

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    Starting from 1,1-diferrocenyl-1-methoxypropyne, the first air-stable C5-cumulenium salt (Fc)2CCCCC(Fc)+BF4- (Fc = ferrocenyl) can be synthesized by a metalation, iodination, cross-coupling, and dehydration sequence. Attempted nucleophilic attack of ferrocenyl carbanion affords only radical decomposition products and none of the desired tetraferrocenyl-C5-cumulene (Fc)2CCCCC(Fc)2. In contrast, reaction with phenyllithium yields the nucleophilic addition product (Fc)2CCC(R)C⋮CFc (R = C6H5) with 100% regioselectivity. Starting from diferrocenyl ketone, the first air-stable protonated C5-cumulenium salt (Fc)2CCHCCC(Fc)2+BF4- is prepared by stepwise substitution of propyne with diferrocenyl(methoxy)methyl groups and subsequent 2-fold dehydration. Addition of methoxide affords (Fc)2CCC(R)CΗC(Fc)2 (R = OCH3); attempted conversion to tetraferrocenyl-C5-cumulene (Fc)2CCCCC(Fc)2 by thermal elimination of methanol in vacuo fails but yields an unusual cyclobutene dimer with eight ferrocenyl substituents. Finally, deprotonation of (Fc)2CCHCCC(Fc)2+BF4- with “super base” n-BuLi/t-BuOK gives access to tetraferrocenyl-C5-cumulene (Fc)2CCCCC(Fc)2, one of the very few C5-cumulenes known. IR, Raman, UV−vis, MS, NMR, Mössbauer spectroscopy, cyclic voltammetry, and X-ray crystallography are used for a detailed characterization of these metallocenylcumulene compounds

    Cationic and Neutral [4]-Cumulenes CCCCC with Five Cumulated Carbons and Three to Four Ferrocenyl Termini

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    Starting from 1,1-diferrocenyl-1-methoxypropyne, the first air-stable C5-cumulenium salt (Fc)2CCCCC(Fc)+BF4- (Fc = ferrocenyl) can be synthesized by a metalation, iodination, cross-coupling, and dehydration sequence. Attempted nucleophilic attack of ferrocenyl carbanion affords only radical decomposition products and none of the desired tetraferrocenyl-C5-cumulene (Fc)2CCCCC(Fc)2. In contrast, reaction with phenyllithium yields the nucleophilic addition product (Fc)2CCC(R)C⋮CFc (R = C6H5) with 100% regioselectivity. Starting from diferrocenyl ketone, the first air-stable protonated C5-cumulenium salt (Fc)2CCHCCC(Fc)2+BF4- is prepared by stepwise substitution of propyne with diferrocenyl(methoxy)methyl groups and subsequent 2-fold dehydration. Addition of methoxide affords (Fc)2CCC(R)CΗC(Fc)2 (R = OCH3); attempted conversion to tetraferrocenyl-C5-cumulene (Fc)2CCCCC(Fc)2 by thermal elimination of methanol in vacuo fails but yields an unusual cyclobutene dimer with eight ferrocenyl substituents. Finally, deprotonation of (Fc)2CCHCCC(Fc)2+BF4- with “super base” n-BuLi/t-BuOK gives access to tetraferrocenyl-C5-cumulene (Fc)2CCCCC(Fc)2, one of the very few C5-cumulenes known. IR, Raman, UV−vis, MS, NMR, Mössbauer spectroscopy, cyclic voltammetry, and X-ray crystallography are used for a detailed characterization of these metallocenylcumulene compounds

    On the Way to Heptahexaenylidene Complexes:  Trapping of an Intermediate with the Novel MCCCCCCCR<sub>2</sub> Moiety

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    Sequential treatment of the in situ generated heptatriyne Me3SiC⋮CC⋮CC⋮CC(NMe2)3 with n-BuLi, (CO)5W[THF], and BF3·OEt2 affords the first alkenyl-substituted pentatetraenylidene complex, (CO)5WC CCCC(NMe2)C(H)C(NMe2)2 (4), via addition of dimethylamine to the CεCζ bond of the intermediate heptahexaenylidene complex (CO)5WCαCβCγCδ CεCζCη(NMe2)2. In addition, the alkynyl(butatrienyl)carbene complex (CO)5WC(C⋮CSiMe3)C(Bu)C CC(NMe2)2 (5) is formed

    Preparation of Phosphorescent Iridium(III) Complexes with a Dianionic C,C,C,C-Tetradentate Ligand

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    The preparation and photophysical properties of heteroleptic iridium­(III) complexes containing a dianionic C,C,C,C-tetradentate ligand and a cyclometalated phenylpyridine group are described. Complex [Ir­(μ-OMe)­(COD)]2 (1, COD = 1,5-cyclooctadiene) reacts with 1,1-diphenyl-3,3-butylenediimidazolium iodide ([PhIm­(CH2)4­ImPh]­I2), in the presence NaOtBu, to give [Ir­(μ-I)­{κ4-C,C,C,C-[C6H4Im­(CH2)4­ImC6H4]}]2 (2), which leads to {[Ir­{κ4-C,C,C,C-[C6H4Im­(CH2)4­ImC6H4]}]2­(μ-OH)­(μ-OMe)} (3) by treatment first with silver trifluoromethanesulfonate (AgOTf) in acetone–dichloromethane and subsequently with KOH in methanol. The reaction of 2 with AgOTf and acetonitrile affords the bis­(solvento) complex [Ir­{κ4-C,C,C,C-[C6H4Im­(CH2)4­ImC6H4]}­(CH3CN)2]­OTf (4). The latter promotes the pyridyl-supported heterolytic ortho-CH bond activation of the phenyl group of 2-phenylpyridine, 2-(2,4-difluorophenyl)­pyridine, 2-(p-tolyl)­pyridine, and 5-methyl-2-phenylpyridine to yield Ir­{κ4-C,C,C,C-[C6H4Im­(CH2)4­ImC6H4]}­{κ2-C,N-[Ar-py]} (Ar-py = C6H4-py (5), C6H2F2-py (6), C6H3Me-py (7), C6H4-Mepy (8)) using (piperidinomethyl)­polystyrene as an external base. Complexes 5–8 are blue-green emitters, which display short lifetimes (0.6–4.8 μs) and quantum yields close to unity in both doped poly­(methyl methacrylate) films at 5 wt % and in 2-methyltetrahydrofuran at room temperature

    Synthesis and Luminescence Behavior of Rhenium(I) Triynyl Complexes. X-ray Crystal Structures of [Re(CO)<sub>3</sub>(<sup>t</sup>Bu<sub>2</sub>bpy)(C⋮C−C⋮C−C⋮CPh)] and [Re(CO)<sub>3</sub>(Me<sub>2</sub>bpy)(C⋮C−C⋮C−C⋮CSiMe<sub>3</sub>)]

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    Luminescent rhenium(I) triynyl complexes [Re(CO)3(tBu2bpy)(C⋮C−C⋮C−C⋮CPh)] 1, [Re(CO)3(tBu2bpy)(C⋮C−C⋮C−C⋮CSiMe3)] 2, and [Re(CO)3(Me2bpy)(C⋮C−C⋮CC⋮CSiMe3)] 3, were synthesized and their photophysical and electrochemical properties studied. The X-ray crystal structures of 1 and 3 have also been determined. A comparison study of their emission properties to that of their mono- and diynyl analogues was made and their emission origin suggested and supported by EHMO studies

    Synthesis and Luminescence Behavior of Rhenium(I) Triynyl Complexes. X-ray Crystal Structures of [Re(CO)<sub>3</sub>(<sup>t</sup>Bu<sub>2</sub>bpy)(C⋮C−C⋮C−C⋮CPh)] and [Re(CO)<sub>3</sub>(Me<sub>2</sub>bpy)(C⋮C−C⋮C−C⋮CSiMe<sub>3</sub>)]

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    Luminescent rhenium(I) triynyl complexes [Re(CO)3(tBu2bpy)(C⋮C−C⋮C−C⋮CPh)] 1, [Re(CO)3(tBu2bpy)(C⋮C−C⋮C−C⋮CSiMe3)] 2, and [Re(CO)3(Me2bpy)(C⋮C−C⋮CC⋮CSiMe3)] 3, were synthesized and their photophysical and electrochemical properties studied. The X-ray crystal structures of 1 and 3 have also been determined. A comparison study of their emission properties to that of their mono- and diynyl analogues was made and their emission origin suggested and supported by EHMO studies

    The rotational spectre of cyanoacetylene dimer, H-C-C-C-N ••• H-C-C-C-N

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    \begin{wrapfigure}{r}{0pt} \includegraphics[scale=0.09]{Big23c2.eps} \end{wrapfigure} The rotational spectra of H-C-C-C-N ••• H-C-C-C-N, cyanoacetylene dimer,were recorded using Balle-Flygare type Fourier transform microwave (FTMW) spectrometers at Wesleyan and Arizona. The low-J transitions were measured down to 1.3 GHz at very high resolution, FWHM ~1 kHz using a large-cavity spectrometer. The spectral hyperfine structure due to the 14^{14}N nuclear quadrupole coupling interactions is well-resolved below 4 GHz using a low frequency spectrometer at the University of Arizona. The experimental spectroscopic constants were fitted as: B0_0 = 339.292331(8) MHz, DJ_J = 32.15(8) Hz, H = -0.0015(2) Hz, eqQ(14^{14}N1_1) = -3.990(1) MHz, and eqQ(14^{14}N2_2) = -4.171(1) MHz. The vibrationally averaged dimer configuration is \\ H-C-C-C-N1_1 ••• H-C-C-C-N2_2. Using a simple linear model, the vibrational ground state and the equilibrium hydrogen bond lengths are determined to be: r0_0(N ••• H) = 2.2489(3) \AA and re_e(N ••• H) = 2.2315 \AA. The equilibrium center-of-mass distance between the two HCCCN subunits is = 7.0366 \AA. Using the rigid precession model, the vibrational ground state center-of-mass distance and the pivot angles which HCCCN subunits make with the a-axis of H-C-C-C-N1_1 ••• H-C-C-C-N2_2 are = 7.0603 \AA, θ\theta1_1 = 1313^{\circ}, and θ\theta2_2 = 8.78.7^{\circ}, respectively. The calculated hydrogen bond energy of H-C-C-C-N ••• H-C-C-C-N is 1466 cm1^{-1} using the MP2/aug-cc-PVTZ method in present work.Made available in DSpace on 2017-01-26T21:39:30Z (GMT). No. of bitstreams: 3 license.txt: 4848 bytes, checksum: 96035ab3f5e1c23cc7138a224ce498bd (MD5) 1543.pdf: 5478808 bytes, checksum: 9f3b641657a387cdb721764a9153ca17 (MD5) 566281.pptx: 9191050 bytes, checksum: 687c35db25e867a8f7f76b69d5887416 (MD5) Previous issue date: 2016-06-2
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