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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 116 (2002), S. 1748-1748 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    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 115 (2001), S. 5498-5506 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The 19F–1H coupling constants were calculated on the multiconfiguration self-consistent field (MCSCF) level in several systems, ranging from covalently bonded HF, hydrogen bonded FHF− and (HF)2 complexes to weak van der Waals complex CH4–HF. The sign of the 19F–1H coupling varies in this sequence, and its absolute value decreases. Still, it is sizable even for CH4–HF. The distance dependence of 19F–1H coupling is essentially the same in all systems under study, and the calculations for FHF− with distorted geometry suggest that the value of 19F–1H coupling is determined mainly by molecular geometry. 19F–19F coupling constants were also analyzed. 19F–19F intermolecular coupling in (HF)2 is substantial but has the opposite sign to that in FHF− and its counterpart in (H2O)2. © 2001 American Institute of Physics.
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 101 (1994), S. 6800-6809 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The potential energy surface of the ground state He+Cl2(1Σg) is calculated by using the perturbation theory of intermolecular forces and supermolecular Møller–Plesset perturbation theory approach. The potential energy surface of the first excited triplet He+Cl2(3Πu) was evaluated using the supermolecular unrestricted Møller–Plesset perturbation theory approach. In the ground state two stable isomers are found which correspond to the linear He–Cl–Cl structure (a primary minimum, De=45.1 cm−1, Re=4.25 A(ring)) and to the T-shaped structure with He perpendicular to the molecular axis (a secondary minimum, De=40.8 cm−1, Re=3.5 A(ring)). The small difference between these geometries is mainly due to the induction effect which is larger for the linear form. The results obtained for the T-shaped minimum are in good agreement with the excitation spectroscopy experiments which observed only the T-shaped form [Beneventi et al., J. Chem. Phys. 98, 178 (1993)]. In the lowest triplet states correlating with Cl2(3Πu), 3A' and 3A‘, the same two isomers correspond to minima. Now, however, the T-shaped form is lower in energy. The 3A' and 3A‘ states correspond to (De,Re) of (19.9 cm−1, 3.75 A(ring)) and (30.3 cm−1, 3.50 A(ring)), respectively, whereas the linear form is characterized by (19.8 cm−1, 5.0 A(ring)). The binding energy for the T form in the lower 3A‘ state is in good agreement with the experimental value of Beneventi et al.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 109 (1998), S. 3919-3927 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The supermolecular Moller–Plesset perturbation theory (MPPT) is applied to calculate and analyze selected portions of the potential-energy surface (PES) of the H2O(centered ellipsis)CO2 complex. Two kinds of minima have been found. The global minimum, which corresponds to the T-shaped structure with the C atom bonded to the O atom, and the local minimum for the H-bonded arrangement OCO(centered ellipsis)HOH. The global minimum was estimated to be 920 cm−1 deep at the fourth order of MPPT combined with the extended spdf-quality basis set supplemented with bond functions. At the same level of theory the optimal H-bonded structure is 357 cm−1 higher in energy, and reveals a small 10° departure from the collinear arrangement OCO(centered ellipsis)H–O. Both the T-shaped and H-bonded forms are primarily bound by the electrostatic term, which is twice as large as the dispersion component. One-dimensional sections of the potential-energy surface were subsequently used to calculate vibrational energy levels for the wagging motion of the water moiety in the T-shaped and H-bonded forms. Two-dimensional cuts of the PES along the intermolecular Jacobi coordinates, r and θ, were employed to simulate the dynamics of the stretch–bend coupling close to the minima. © 1998 American Institute of Physics.
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 6569-6576 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The ab initio potential energy surface of the ArCO2 cluster is calculated using the supermolecular Møller–Plesset perturbation theory (S-MPPT) and dissected into its fundamental components; electrostatic, exchange, induction, and dispersion energies. The surface contains a single minimum for the perpendicular approach of Ar toward the C atom which has a well depth of ∼210 cm−1 at R=6.5 a0. This value is obtained using an extended basis set supplied with the bond functions and the fourth order supermolecular Møller–Plesset calculations, and is expected to be accurate to within ±5%. The areas of the surface corresponding to the collinear approach of Ar to CO2 contain an extended plateau. The saddle point in this region for R=9.0 a0 is stabilized by 117 cm−1. The analytical pair potential for Ar–CO2 obtained by fitting to the individual interaction components is provided. The three-body effects in the related cluster, Ar2CO2, are examined for two configurations of the Ar2CO2 cluster. The overall nonadditivity is dominated by the three-body dispersion effect; however, the exchange nonadditivity is the most anisotropic. The sources of this anisotropy are discussed. © 1996 American Institute of Physics.
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  • 6
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 75 (1971), S. 3581-3585 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    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 99 (1993), S. 5211-5218 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The potential energy surface of the H2CO–Ar complex is calculated at the second-order Møller–Plesset perturbation theory and analyzed using the perturbation theory of intermolecular forces. The equilibrium geometry (De=171 cm−1) involves a T-shape structure with the Ar atom nearly perpendicular to the C–O bond of H2CO and in the molecular plane of H2CO. The equilibrium configuration results from a minimum in the exchange repulsion. It is conceivable that H2CO undegoes a hindered internal rotation in the complex. A barrier to such a motion is estimated at 32 cm−1. The potential energy surface is very complex. The anisotropy of the surface involving the in-plane motion of Ar is very high and resembles that of the Ar–H2O complex. The anisotropy involving motion of Ar perpendicular to the molecular plane of H2CO is much weaker, and it is strikingly similar to that of the Ar–CO complex.
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 99 (1993), S. 3700-3706 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The analysis of the potential energy surface of the Ar–ClF complex is performed using the perturbation theory of intermolecular forces. The three minima on the potential energy surface correspond to the linear Ar—Cl–F configuration (global minimum De=233 cm−1), the linear Ar—F–Cl configuration (De=133 cm−1), and the T structure in which the Ar atom is nearly perpendicular to the molecular axis of Cl–F (De=146 cm−1). The calculated parameters of the minima are in full accord with the recent ab initio study by Tao and Klemperer [J. Chem. Phys. 97, 440 (1992)]. The absolute minimum results from the attractive dispersion and polarization energies which help overcome a considerable exchange repulsion. The secondary linear minimum Ar—F–Cl, is due, in large measure, to the dispersion energy accompanied by a weaker exchange repulsion. The T configuration is characterized by the weakest repulsion and the dispersion energy roughly equal to that in Ar—F–Cl. The analysis of the angular behavior of the Heitler–London interaction energy leads us to believe that the charge distribution of the Cl–F molecule possesses a concave shape along the molecular axis at the Cl end of the molecule. This indentation in the charge cloud allows subsystems to approach close to one another in the linear Ar—Cl–F arrangement, and also causes an appreciable stiffness of the Ar–Cl–F bending mode.
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Theoretical chemistry accounts 76 (1989), S. 173-185 
    ISSN: 1432-2234
    Keywords: Hydrogen bonding ; CO2-HF complex ; N2O-HF complex
    Source: Springer Online Journal Archives 1860-2000
    Topics: Chemistry and Pharmacology
    Notes: Summary Quantum chemical ab initio calculations have been performed for the complex CO2⋯HF and N2O⋯HF. The interaction energies were computed through fourth order MBPT and were corrected for basis set superposition errors. Extended polarized basis sets were used which are constructed to give accurate values for electric moments and polarizabilities. The complex NNO⋯HF was found to be bent, while OCO⋯HF is linear, in agreement with experiment. The MBPT calculations give evidence for a second linear isomeric structure FH⋯NNO, a possibility which has also been suggested by recent experimental data. The computed binding energies are: 2.5 kcal/mol for OCO⋯HF, 2.4 kcal/mol for NNO⋯HF, and 3.0 kcal/mol for FH⋯NNO. At the SCF level, the FH⋯NNO complex is less stable than NNO⋯HF, but correlation has a large effect on the geometry and energetics of the latter complex. The NNO⋯HF complex seems to be a system where the positive intramolecular correlation correction prevails over the negative intermolecular component.
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  • 10
    Electronic Resource
    Electronic Resource
    New York, NY : Wiley-Blackwell
    International Journal of Quantum Chemistry 46 (1993), S. 623-634 
    ISSN: 0020-7608
    Keywords: Computational Chemistry and Molecular Modeling ; Atomic, Molecular and Optical Physics
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: The structure and energetics of the complexes formed between SCO/He and SCO/N2 were investigated using ab initio wave functions at both the SCF and correlated levels of theory with a medium-sized polarized basis set. The energy of the T-structure for SCO⃛He was found to be lower than the energy of the corresponding linear complexes with He bonded to the oxygen or sulfur atoms. Two linear structures for SCO⃛ He were found to be nearly isoenergetic. There is only a small difference in energy between the T-structure for SCO⃛N2 and the OCS⃛N—N colinear structure, with the T-structure being the lowest. The electron correlation contributions to the interaction energy were calculated using Möller-Plesset perturbation theory at the MP2, MP3 and SDTQ-MP4 levels. Analysis shows the importance of the triple excitations in these complexes. © 1993 John Wiley & Sons, Inc.
    Additional Material: 3 Ill.
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