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  • 21
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 1554-1565 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 22
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 2953-2958 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 23
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 9617-9624 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 24
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 16136-16143 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 25
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 7379-7380 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: It is elucidated that, for nanostructures in which the electron states are filled though the energy range of a transmission or reflection peak (quasilevel resonance), the electron pair distribution has a variety of the Fermi exchange hole in which, to a good approximation, just half of the electron pairs contribute to the Coulomb interaction energy. The displacement of current characteristics due to the space-charge interaction should be calculated with this 1/2 factor. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 26
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 79 (1996), S. 7381-7382 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: It is shown, by analysis in terms of the eigenvalues of the S matrix, that the Fano type of transmission resonance in nanostructures has the same space-charge property as applies to the simple Lozentzian resonances. The total space charge in the structure enclosed by the leads, due to filling all electron states (of one spin state) over the energy range of a narrow resonance, is equal to just one electron charge. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 27
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 109 (1998), S. 6390-6395 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Molecular dynamics simulation has been used to explore the nature of solvation dynamics for an excess electron in methanol and in water. We perform the analysis within the linear response theory and show that nonlinear corrections are small in both cases. The response function characterizing solvent relaxation after electron photoexcitation and that following the subsequent nonradiative transition are modeled and found to behave very similarly in methanol, in contrast to water. For methanol, each is comprised of an extremely short Gaussian inertial component of small amplitude and a bi-exponential diffusive decay. A relatively fast ∼1 ps exponential accounts for approximately half of the solvent relaxation and is followed by a slower ∼7 ps relaxation of comparable magnitude, a solvation response that is rather similar to that reported previously for relatively large molecules in methanol. Spectral densities of energy gap fluctuations for the equilibrium ground and excited state trajectories show that translational motion dominates solvation. Relaxational processes in methanol have been compared with the results for water. In contrast to methanol, librational motions of solvent molecules significantly influence aqueous solvation dynamics, especially following excited state decay. This difference is reflected in the relaxational processes, which are an order of magnitude slower in methanol than in water. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 28
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 107 (1997), S. 5863-5878 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The impact of quantum decoherence and zero point motion on non-adiabatic transition rates in condensed matter systems is studied in relation to non-adiabatic (NA) molecular dynamics (MD) techniques. Both effects, and decoherence in particular, strongly influence the transition rate, while neither is accounted for by straightforward quantum-classical approaches. Quantum corrections to the quantum-classical results are rigorously introduced based on Kubo's generating function formulation of Fermi's Golden rule and the frozen Gaussian approximation for the nuclear wave functions. The development provides a one-to-one correspondence between the decoherence function and the Franck–Condon factor. The decoherence function defined in this paper corrects an error in our previous work [J. Chem. Phys. 104, 5942 (1996)]. The relationship between the short time approach and the real time NA MD is investigated and a specific prescription for incorporating quantum decoherence into NA simulations is given. The proposed scheme is applied to the hydrated electron. The rate of excited state non-radiative relaxation is found to be very sensitive to the decoherence time. Quantum coherence decays about 50% faster in H2O than in D2O, providing a theoretical rationalization for the lack of experimentally observed solvent isotope effect on the relaxation rate. Microscopic analysis of solvent mode contributions to the coherence decay shows that librational degrees of freedom are primarily responsible, due to the strong coupling between the electron and molecular rotations and to the small widths of the wave packets describing these modes. Zero point motion of the O–H bonds decreases the life time of the excited state of the hydrated electron by a factor of 1.3–1.5. The implications of the use of short time approximations for the NA transition rate and for the evolution of the nuclear wave functions are considered. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 29
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 106 (1997), S. 9659-9667 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The extraction of the true Kohn-Sham exchange-correlation potential from near-exact electronic densities is demonstrated, with particular reference to the two-electron systems He and H2. It is shown that if the reference density is obtained from a standard configuration interaction calculation, very large orbital basis sets are required to obtain convergence in the resulting exchange-correlation potential. The correlation contribution to molecular bonding is analysed in terms of contributions from the potential in different regions of real space. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 30
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 104 (1996), S. 9651-9653 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We present a new technique for the evaluation of hydrodynamic densities (for example mass, energy or momentum densities) at planes in molecular dynamics simulations. This technique employs an easily computed expression for the density at a plane that is formally exact, unlike other expressions such as histogram approximations. We present simple examples of applications of this procedure to the calculation of mass and momentum densities, and hence the streaming velocity, at planes in a fluid undergoing planar Poiseuille flow, and show how the temperature profile can be obtained by the same procedure. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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