2014
DOI: 10.4028/www.scientific.net/ddf.353.292
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Self-Diffusion on Pd(111) from the Point of View of the Band Model of Diffusion

Abstract: In this article we present a different view on the results of experimental investigation of the self - diffusion on Pd (111) published in „Surface Science“ [1]. Our consideration is based on the band model of diffusion. This model is able to explain the Meyer-Neldel rule (MNR) and to clarify “puzzles” mentioned in [1]. The aim of this article is also to familiarize the readers with this model, to the band model of diffusion.

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Cited by 2 publications
(3 citation statements)
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“…In transverse excitation, the relative contributions of ERS and SERS scale by the spectral dependence of scattering and β, as discussed above. The clearest signature of ERS is the anti-Stokes branch of the continuum, which decays exponentially as a function of Raman shift. It perfectly fits the Fermi–Dirac distribution of hole states, which serve as the thermally occupied terminal states in ERS (see Figure ii). The fit of the anti-Stokes ERS to the Fermi Dirac distribution yields the temperature of the nantenna, and its dependence on excitation intensity yields the heating rate, which limits the tolerable average irradiation intensity (see below).…”
Section: Systemmentioning
confidence: 93%
“…In transverse excitation, the relative contributions of ERS and SERS scale by the spectral dependence of scattering and β, as discussed above. The clearest signature of ERS is the anti-Stokes branch of the continuum, which decays exponentially as a function of Raman shift. It perfectly fits the Fermi–Dirac distribution of hole states, which serve as the thermally occupied terminal states in ERS (see Figure ii). The fit of the anti-Stokes ERS to the Fermi Dirac distribution yields the temperature of the nantenna, and its dependence on excitation intensity yields the heating rate, which limits the tolerable average irradiation intensity (see below).…”
Section: Systemmentioning
confidence: 93%
“…Let us now restrict our attention to the aS background of the SER spectra in Figure . SERS background arises mostly from inelastic light scattering off electrons in the plasmonic metal. Other factors, like molecular vibrations or photoluminescence, also contribute to the background, yet they are of secondary importance in our case. The reader is referred to the work of Mahajan et al that explains the contribution of molecular vibrations to the SERS background (which is evident in the Stokes part of the spectra), and to the papers by Huang et al and Liu et al that explain how luminescence arises in plasmonic nanostructures.…”
mentioning
confidence: 99%
“…It was also observed (but not commented) by Hugall and Baumberg (see Figure b in ref ), who used continuous wave illumination at 785 nm. On the contrary, a strictly single-exponential aS background was observed by Xie et al on arrays of plasmonic nanostructures, and by Banik on a single nanodumbell . Understanding and quantification of the extra component in the aS background is a matter of current debate in the field.…”
mentioning
confidence: 99%