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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    Inorganic chemistry 30 (1991), S. 4130-4135 
    ISSN: 1520-510X
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    Medical microbiology and immunology 9 (1890), S. 218-234 
    ISSN: 1432-1831
    Source: Springer Online Journal Archives 1860-2000
    Topics: Medicine
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Amsterdam : Elsevier
    Chemical Physics Letters 163 (1989), S. 455-460 
    ISSN: 0009-2614
    Source: Elsevier Journal Backfiles on ScienceDirect 1907 - 2002
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 106 (1997), S. 6806-6812 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Vibrational predissociation spectra of hydrazine (N2H4)n clusters have been measured from the dimer to the tetramer using a linetunable, isotopically substituted CO2-laser in order to fill the frequency gap between 990 and 1010 cm−1. The clusters are size selected in a scattering experiment with helium atoms. The large blue shifts of the asymmetric NH2 wag mode at 937 cm−1 are completely interpreted by calculations based on a recently determined systematic model potential. The gross shifts of 60 cm−1 for the dimer, 80 cm−1 for the trimer, and 110 cm−1 for the larger clusters are explained by the different structures: Cyclic arrangements with two hydrogen bonds per molecule for the dimer, rings with one hydrogen bond per molecule for the trimer, and three-dimensional structures for the larger ones. The peaks in the spectra are caused by characteristic vibrations to which more than one isomer contributes. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 98 (1993), S. 9425-9431 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Infrared photodissociation spectra of the mixed complexes C2H4–CH3COCH3 and C2H4–(CH3COCH3)2 have been observed after size selecting them by scattering from a helium beam combined with mass spectrometric detection. The excitation of the ν7-out of plane symmetric wagging mode of ethene near its gas phase frequency at 949.3 cm−1 with a cw-CO2 laser leads to a characteristic depletion of the cluster beam. The dissociation spectrum of the 1:1 complex can be explained by two peaks at 950.8 and 961.6 cm−1. Calculations of minimum energy configurations and band shifts based on an empirical site–site potential show that these frequencies can be attributed to the absorption of two different isomers. They correspond to the two different binding patterns of the H atoms of ethene to the O atom of acetone and those of acetone to the C–C group of ethene, respectively. For the 1:2 complex, a large peak at 958.5 cm−1 and a smaller one around 940.5 cm−1 are found which can be explained in a similar manner by several isomers found in the structure calculations.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 28 (1993), S. 331-337 
    ISSN: 1434-6079
    Keywords: 36.40.+d ; 33.20.Ea
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Infrared photodissociation spectra of (CH3OH) n clusters (n=2, 3 and 6) and the mixed dimer C2H4 · CH3COCH3 are presented. The clusters are generated in a supersonic jet expansion and size selected by scattering from a helium atomic beam combined with mass spectrometric detection. Continuous CO2-lasers are used to vibrationally excite the molecules in the cluster leading to rapid dissociation of the complex. Various dissociation peaks that are found in single-laser dissociation spectra can be assigned unambigously in a pump-probe experiment with two lasers to either different isomers (acetone-ethene dimer) or splitted lines of one isomer (methanol hexamer). For size distributions, the method is able to select contributions of single masses which is demonstrated for mixtures of methanol dimers and trimers.
    Type of Medium: Electronic Resource
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  • 7
    ISSN: 1434-6079
    Keywords: 36.40 ; 82.50.F
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Infrared photodissociation spectra of (CH3NH2) n clusters were measured fromn=2 ton=6 near the monomer absorption of the C-N stretching mode at 1044 cm−1 using a cw-CO2 laser. The clusters were size-selected by scattering from a helium beam. The spectrum of cold dimers shows a red (1038 cm−1) and a blue (1048 cm−1) shifted peak which is attributed to the non-equivalent position of the C-N in the open dimer structure. The larger clusters exhibit only one peak between 1045.4 cm−1 and 1046.0 cm−1 caused by the equivalent position of the C-N in the cyclic structures of the larger clusters. Structure calculations confirm these results. Secondly, the mixed complexes C2H4-CH3COCH3 and C2H4-(CH3COCH3)2 were investigated. The dimer spectrum, measured around the monomer frequency of the out-of-plane bending mode of C2H4 at 949 cm−1, shows two peaks at 946.2 cm−1 and 961.3 cm−1. This splitting is attributed to two different isomers that are found in configuration calculations. A similar behaviour is found for the trimer.
    Type of Medium: Electronic Resource
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  • 8
    ISSN: 1434-6079
    Keywords: 36.40 ; 34.80.G
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The hydrogen-bonded (N2H4) n clusters and the van der Waals (OCS) n clusters are size selected in a scattering experiment with a He beam up to the cluster sizen=6. By measuring the angular distributions of the scattered clusters the complete fragmentation pattern of electron impact ionization is obtained. For Hydrazine the two main fragment masses are the protonated species (N2H4) n−1H+ and with somewhat weaker intensities also the nominal ion mass (N2H4) n + . The largest intensity is observed for the monomer ion N2H 4 + to which clusters up ton=5 fragment. For carbonylsulfide, completely different results are obtained. Aside from the fragments of the OCS monomer and the van der Waals cluster fragments (OCS) 2 + and (OCS) 3 + signals at mass S 2 + , S 3 + and S2OCS+ are detected. This indicates a fast chemical reaction in the cluster according to: S + OCS → CO + S2 which occurs for clusters of sizen ≥ 2. Peaks at S 3 + and S2OCS+ are seen for the first time forn ≥ 5 according to a further reaction of S2 in the cluster.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Fresenius' Zeitschrift für analytische Chemie 40 (1901), S. 430-431 
    ISSN: 1618-2650
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 10
    ISSN: 0044-2313
    Keywords: Chemistry ; Inorganic Chemistry
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Description / Table of Contents: Cyclic Diazastannylenes. XXVIII. Inorganic Polycyclic Compounds from the Reaction of Bis(amino)stannylene or Iminostannylene with SnCl2, SnBr2, and tert-Butoxitin(II) Chloride or BromideThe cyclic bis(amino)stannylene 1 may react with tert-butoxitin(II) chloride or bromide yielding a Lewis acid-base adduct 4 resp. 5, in which the two molecules are held together via N→Sn (233.8(3) pm) and O→Sn (215.1(2) pm) bonds. The resulting adduct 4 contains therefore two four membered rings sharing one common edge as found by X-ray structure determination. If 1 is allowed to react with SnCl2 or SnBr2, the salts Me2Si(NtBu)2Sn2Br+Sn2Br5- (7) are formed. Structure analysis reveals the cations in 6 and 7 to be very similar: SnCl+ and SnBr+ are coordinated by the “trihapto ligand” 1 in a way resulting a polycyclic SiN2Sn2X-arrangement. To a central Sn2N2 tetrahedron Si and halogen X are added occupying and bridging two opposite edges (mean values: N—Sn = 232(5) (6), N—Sn = 230(2) (7), Sn—C1 = 265(1), Sn- Br = 275(1) pm). The reaction intermediate (SnNtBu)2 adds to SnCl2 to form the crystalline polymer ( tBuN)2Sn3C12 (8). X-ray structure determination reveals the solid to be built up by one-dimensional chains of polycyclic Sn3(NtBu)2C13 sharing two chlorine atoms with neighbouring units. The unit Sn3(NtBu)2C13 can be visualized as an equilateral triangle of chlorine atoms, on which a smaller triangle of tin atoms is superimposed; the corners of the smaller triangle being located in the middle of the larger triangle's edges. The tin atoms are bipyramidally coordinated by two N- tBu-groups thus forming a nearly perfect Sn3N2s trigonal bipyramide (Sn—N = 222.7(3) pm). Two chlorine atoms of the triangle are connected to neighbouring units, the chlorine atoms thus attain an unusual nearly square-planar coordination sphere (Sn—Cl(mean) = 308(5) pm). The tertbutyl groups at the nitrogen atoms “screen” the inorganic part of the structure leading to a layer structure.
    Notes: Das cyclische Bis(amino)stannylen 1 reagiert mit tert-Butoxizinn(II)-chlorid oder -bromid zu einem Lewis-Säure-Base-Addukt 4 bzw. 5, in dem die beiden Moleküle über N→Sn- (233,8(3) pm) und O→Sn- (215,1(2) pm) Bindungen zusammengehalten werden, was zur Bildung zweier anellierter Vierringe führt (Röntgenstrukturanalyse von 4). Setzt man 1 hingegen mit SnCl2 oder SnBr2 um, so entstehen die “Salze” Me2Si(NtBu)2Sn2Br+Sn2Br5- (7). Gemäß Strukturanalysen sind die Kationen in 6 und 7 strukturell nahe verwandt: SnCl+ bzw. SnBr+ werden von dem “Trihaptoliganden” 1 so koordiniert, daß eine polycyclische SiN2Sn2X-Einheit mit einem N2Sn2-Tetraeder und kantenüberbrückenden Si und Halogen (X) entsteht (Mittelwerte : N—Sn = 232(2) (6), 230(2) (7), Sn—Cl = 265(1), Sn—Br = 275(1) pm). (tBuNSn)2, eine kurzlebige Zwischenstufe, addiert sich an SnCl2 unter Bildung eines kristallinen Polymers (tBuN)2Sn3Cl2 (8). Der Festkörper besteht nach Röntgenstrukturanalyse aus einer unendlichen Kette von (tBuN)2Sn3Cl3-Polycyclen, die sich mit benachbarten Einheiten jeweils zwei Chloratome teilen. (tBuN)2Sn3Cl3 bildet ein gleichseitiges Dreieck aus Chloratomen, auf dessen Kantenmitten ein zweites gleichseitigtes Dreieck aus Zinnatomen hineingestellt ist. Diese sind ihrerseits durch (NtBu)-Gruppen trigonal bipyramidal verknüpft. Die verbrückenden Chloratome besitzen eine ungewöhnliche planare, fast quadratische Koordination (Sn—Cl(Mittel) = 308(5) pm). Der mittlere Sn3N2-Polycyclus der Figur kann als nahezu perfekte trigonale Bipyramide beschrieben werden (Sn—N = 222,7(3) pm). Die tert-Butylgruppen an den Stickstoffatomen schirmen den anorganischen Teil der Struktur so ab, daß eine Schichtstruktur entsteht.
    Additional Material: 7 Ill.
    Type of Medium: Electronic Resource
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