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  • 2000-2004  (3)
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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 88 (2000), S. 6897-6901 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We calculate the potential energy curves for H adsorption on and absorption in Cu(111), Pt(111), and Pd(111) within the density functional theory. We show stronger dependence of the potential energies on the lateral position of the H atom at the position further from the surface in the case of Pt(111) than one in the case of Pd(111), and no lateral position dependence in the case of Cu(111). Contrary to this, when the H atom comes close to and adsorbs on the surface, the dependence of its adsorption energy (a depth of potential well outside the surface) on the lateral position in the case of Cu(111) is stronger than one in the case of Pd(111), and such dependencies are hardly seen, and the adsorption energies are nearly the same in the case of Pt(111). When the H atom penetrates the first layer of the surface, the activation barrier at a so-called face-centered-cubic hollow site in the case of Pd(111) is the lowest in three surfaces. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 91 (2002), S. 1855-1859 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The quantum mechanical behavior of an H atom adsorbed on Cu(111) and on Pt(111) is investigated. The potential energy curves (PECs) for the H atom motion on these surfaces are calculated within the density functional theory, and the adiabatic three-dimensional potential energy surfaces (PESs) are constructed based on the obtained PECs. The wave functions and their energies for the H atom motion on the PESs are calculated within the framework of the variation method. The results show that, in the case of Cu(111), the ground state wave function is strongly localized around the fcc hollow site, the first-excited state wave function is strongly localized around the hcp hollow site, and these states almost energetically degenerate. On the other hand, the second-excited state wave function is delocalized and extends from the fcc hollow site to the bridge site and further to the hcp hollow site. Then, there is a significant energy gap between the first- excited and the second-excited state. In the case of Pt(111), the ground and the first-excited state wave functions are delocalized and extend from the hollow site to the bridge site. The second-excited state wave function further extends over the top site. The energy differences between the ground and the first-excited state, and between the first-excited and the second-excited state are very small. Thus, the H atom adsorbed on Pt(111) has a delocalized nature. © 2000 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    ISSN: 1476-4687
    Source: Nature Archives 1869 - 2009
    Topics: Biology , Chemistry and Pharmacology , Medicine , Natural Sciences in General , Physics
    Notes: [Auszug] Many superconductors do not entirely expel magnetic flux—rather, magnetic flux can penetrate the superconducting state in the form of vortices. Moving vortices create resistance, so they must be ‘pinned’ to permit dissipationless current flow. This is a particularly ...
    Type of Medium: Electronic Resource
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