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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Fresenius' journal of analytical chemistry 364 (1999), S. 367-375 
    ISSN: 1432-1130
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology
    Notes: Abstract An overview is given about the new developments in GDMS, both with respect to the glow discharge source as to the coupling with various kinds of mass spectrometers. Moreover, as for every analytical technique, methodological and fundamental research is being carried out to improve the analytical results of GDMS, and some of the new developments in these fields will be discussed as well. Finally, the various analytical applications of GDMS will be presented.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 91 (1989), S. 4425-4426 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The dissociation energy of boron hydride has been calculated ab initio using a very accurate theoretical model, with an expected accuracy of ±0.2 kcal mol−1. The values of 85.7 and 82.4 kcal mol−1 for De and D0, respectively, confirm the conclusion of Curtiss and Pople [J. Chem. Phys. 90, 2522 (1989)], that the predissociation limit of 82.6±0.4 kcal mol−1 might be close to the actual dissociation energy, and that an earlier proposed De of 78.9 kcal mol−1 is in error.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 6655-6667 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The spectroscopic properties of the three lowest-lying states X 3Π, A 3∑−, and a 1∑+ of SiC have been computed accurately using augmented coupled cluster methods and different basis sets. Partition functions have been set up, accounting for anharmonicity, rotation–vibration coupling, centrifugal distortion, and isotope effects. Thermodynamic properties are tabulated in JANAF style from 100 to 6000 K. A critical analysis of the effects of the various contributions is made, as well as an error analysis.
    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 90 (1989), S. 6469-6485 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: For a number of different structures and states of B3, B2N, BN2, and N3, optimum geometries and harmonic spectra were obtained at the HF/6-31G* level. The relative stability of the isomers was determined using full fourth-order Møller–Plesset theory, both with and without spin projection, as well as coupled cluster methods. Estimates for the dissociation energies are based on scaled CCD+ST(CCD) binding energies. Koopmans' vertical ionization potentials and Mulliken charge distributions, both at the UHF/6-31G* level, are quoted for the most stable isomers. B3 is found to be an equilateral triangle in its 2A'1 ground state. B2N has a symmetric linear arrangement in its 2Σ+u ground state with an extremely low bending frequency (73 cm−1), and an unusually low vertical ionization potential (6.75 eV). Its asymmetric stretching (2021 cm−1) is found to be extremely intense (8782 km mol−1). BN2 has four rather closely spaced states, of which an isosceles triangle is the absolute minimum (2A1 state). However, at high temperatures, an asymmetric linear arrangement (2Π state) is found to have equal importance, whereas a 4Σ− state plays a role there too. The same theoretical methods correctly predict for N3 a symmetric linear arrangement in the 2Πg ground state; the spectroscopic constants are found to be in reasonable agreement with experiment. Estimated dissociation energies (expected accuracy ±4 kcal mol−1) are: B3 197.9, B2N 265.0, BN2 224.9, N3 210.1 kcal mol−1. From a statistical thermodynamical analysis, B3 is stable against dissociation to B2 and B up to very high temperatures, B2N is extraordinarily stable, whereas BN2 and N3 dissociate spontaneously to B+N2 and N+N2 at all temperatures. From these results, the presence of B2N+ and B+3, the high abundance of B2N+, as well as the absence of BN+2 and N+3 in laser mass spectra of boron nitride is explained.
    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 96 (1992), S. 7633-7645 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The anharmonic potential energy surface of water has been computed ab initio using an augmented coupled cluster method and various basis sets. Whereas the Pople 6–311 G family is manifestly unsatisfactory, Huzinaga–Dunning basis sets perform quite well. The [5s4p2d1f,3s2p] surface reproduces harmonic frequencies and anharmonicity constants to better than about 2 and 1 cm−1, respectively. For quantitative agreement with experiment, both f functions on oxygen and inclusion of core correlation seem to be prerequisite. Comparison with various experimentally derived force fields reveals that the ab initio force field is of comparable quality. From the best computed force field, a set of spectroscopic constants has been derived for all important isotopomers of water. Using a hybrid analytic/direct summation method recently developed by the present authors, the thermodynamic functions gef(T), hcf(T), S0, and Cp are computed including exact account of anharmonicity and rovibrational coupling, and very good analytical approximations to centrifugal distortion and quantum rotation effects. The computed functions substantially revise previous literature results at high temperatures. Differences between thermodynamic functions from various computed force fields are an order of magnitude smaller than these errors. Thermodynamic tables in JANAF style from 100 to 3000 K, as well as a full set of rovibrational spectroscopic constants, are presented. It is concluded that obtaining force fields of near-spectroscopic accuracy, and thermodynamic tables of very high accuracy, is presently feasible for small polyatomic molecules.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 4485-4487 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The dissociation energy of N3 has been computed ab initio using coupled cluster techniques and large basis sets. Our best theoretical estimates (accuracy ±2 kcal/mol) are ∑De=234.0, ∑D0=228.4, ΔH0 f =109.3, and ΔH0 f,298=108.4 kcal/mol. These values are in excellent agreement with an ICR determination of ΔH0 f=112±5 kcal/mol. Very large basis set effects are observed.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 8850-8861 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The harmonic frequencies, infrared intensities, and isotopic substitution bands of C6 have been evaluated at the MP2/6-31G* level. They confirm previous assignments of the 1952 and 1197 cm−1 matrix IR bands to C6. Isotopic substitution spectra at the MP2/6-31G* and HF/4-21G levels, as well as those with a newly developed ad hoc modified neglect of diatomic overlap (MNDO) method are shown to be in good agreement with experiment for C4, C5, and C6. On the basis of RHF/4-21G, RHF/6-31G*, MP2/4-21G, MP2/6-31G*, and ad hoc MNDO data, including theoretical frequencies, IR intensities, and isotopic substitution spectra, it is shown with virtual certainty that the 2128 and 1893 cm−1 matrix IR bands belong to C7. A recent assignment of the very intense 1997 cm−1 matrix IR feature to C8 is contradicted on the same grounds, and an alternative assignment to C9 put forward.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 94 (1991), S. 3753-3761 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The lowest-lying 1Ag and 3Σ−g states of C4 have been studied using basis sets including f functions, quadratic configuration interaction, and full fourth-order Møller–Plesset perturbation theory with multiple spin projection. Basis set effects on the linear-cyclic separation have been found to be fairly significant. Use of the 6-311G* and [5s3p1d] basis sets leads to qualitatively different conclusions; this problem is remedied by expansion of the polarization space. At the highest level of theory considered, the cyclic structure lies about 1 kcal/mol below the linear structure. A G1-type estimate of its heat of formation at 0 K of 249.6 kcal/mol is proposed. This value is in disagreement with the generally quoted experimental values, but in good agreement with third-law values by Drowart et al. [J. Chem. Phys. 31, 1131 (1959)] corrected for improved partition functions. Geometries and harmonic frequencies are reported. It is tentatively suggested that a matrix ir band at 1284 cm−1 may belong to cyclic C4; to aid experimentalists in confirming or rejecting this assignment, theoretical isotope shifts are reported.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 93 (1990), S. 5037-5045 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The potential energy surface of the C+3 cation has been investigated using coupled cluster techniques and large basis sets. The results are particularly sensitive towards the level of electron correlation. Spin contamination even produces a "false stationary point'' at the UHF/6-31G* level. C+3 has a cyclic 2B2 ground state with predicted geometry r=1.3242 A(ring), θ=73.06° (MP2/6-311G*, empirically corrected bond distance). At the highest level of theory considered, the linear structure (2Σ+u state) lies about 2 kcal/mol above the ground state: this might imply quasilinearity. There is also a low barrier towards degenerate isomerization: at high temperatures, C+3 will be extremely floppy. Harmonic frequencies (UHF/6-31G*) as well as double-harmonic IR and Raman intensities are given for various structures of C+3. Interesting analogies of C+3 with B3 and B2N are pointed out. The heat of formation at 298.15 K, vertical and adiabatic ionization potentials of C3 are predicted as 194.9±2 kcal/mol, 11.92±0.1 eV, and 11.84±0.1 eV, respectively.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 3403-3405 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The geometry and infrared spectrum of C5 have been computed ab initio using the MP2/6-31G* theoretical model. The inner and outer bond lengths are 1.291 and 1.300 A(ring), respectively. A very intense (1243 km mol−1) ∑+u band is predicted at 2193 cm−1, while another ∑+u mode at 1368 cm−1 is found to be much less intense (64 km mol−1). The results confirm the assignment of the experimental infrared (IR) frequencies of C4 and C5 suggested by Bernholdt et al. [J. Chem. Phys. 89, 3612 (1988)].
    Type of Medium: Electronic Resource
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