Abstract:Abstract. Using a combined quantum mechanical/classical method, we study the dynamics of deposition of small Na clusters on Ar(001) surface. We work out basic mechanisms by systematic variation of substrate activity, impact energy, cluster orientations, cluster sizes, and charges. The soft Ar material is found to serve as an extremely efficient shock absorber which provides cluster capture in a broad range of impact energies. Reflection is only observed in combination with destruction of the substrate. The kin… Show more
“…Enhancing the impact energy further to force reflection leads into a regime where a whole surface area is destroyed. This is similar to our findings for deposition of Na clusters [26].…”
We study deposition dynamics of Na and Na$_2$ on an Ar substrate, both
species neutral as well as charged. The system is modeled by a hierarchical
approach describing the Na valence electrons by time-dependent
density-functional theory while Na core, Ar atoms and their dynamical
polarizability are treated by molecular dynamics. We explore effects of Na
charge and initial kinetic energy of the impinging Na system. We find that
neutral Na is captured into a loosely bound adsorbate state for sufficiently
low impact energy. The charged monomers are more efficiently captured and the
cation Na$^+$ even penetrates the surface layer. For charged dimers, we come to
different final configurations depending on the process, direct deposit of
Na$_2^+$ as a whole, or sequential deposit. In any case, charge dramatically
amplifies the excitation of the matrix, in particular at the side of the Ar
dipoles. The presence of a charge also enhances the binding to the surface and
favours accumulation of larger compounds.Comment: 8 figures, to be published in Surf. Sci. (2008
“…Enhancing the impact energy further to force reflection leads into a regime where a whole surface area is destroyed. This is similar to our findings for deposition of Na clusters [26].…”
We study deposition dynamics of Na and Na$_2$ on an Ar substrate, both
species neutral as well as charged. The system is modeled by a hierarchical
approach describing the Na valence electrons by time-dependent
density-functional theory while Na core, Ar atoms and their dynamical
polarizability are treated by molecular dynamics. We explore effects of Na
charge and initial kinetic energy of the impinging Na system. We find that
neutral Na is captured into a loosely bound adsorbate state for sufficiently
low impact energy. The charged monomers are more efficiently captured and the
cation Na$^+$ even penetrates the surface layer. For charged dimers, we come to
different final configurations depending on the process, direct deposit of
Na$_2^+$ as a whole, or sequential deposit. In any case, charge dramatically
amplifies the excitation of the matrix, in particular at the side of the Ar
dipoles. The presence of a charge also enhances the binding to the surface and
favours accumulation of larger compounds.Comment: 8 figures, to be published in Surf. Sci. (2008
“…The collision process produces a sudden local heating of cluster and matrix, followed by a rapid dissipation of the heat in the matrix, 33,34 which can result in the coexistence of different low energy isomers in the rare-gas matrix. 35 Finally, it has to be noted that the relative stability of different embedded isomers has to account for their insertion energy into the matrix ͑that can be important in Ref.…”
We present a joint theoretical and experimental investigation of the absorption spectra of silver clusters Ag n ͑4 Յ n Յ 22͒. The experimental spectra of clusters isolated in an Ar matrix are compared with the calculated ones in the framework of the time-dependent density functional theory. The analysis of the molecular transitions indicates that the s-electrons are responsible for the optical response of small clusters ͑n Յ 8͒ while the d-electrons play a crucial role in the optical excitations for larger n values.
“…Thus Ar substrates are very efficient soft stopper materials. In the former analysis, 33,47 we had run a similar series of impact energies as above and we also found soft deposition for energies up to at least E kin 0 / N ion = 0.272 eV. An attempt to reach a reflection regime by further increasing the impact energy then led to a significant destruction of the substrate.…”
Section: Mgo Versus Ar Substratementioning
confidence: 72%
“…Recently, we have investigated deposition dynamics of Na clusters on Ar͑001͒ surface. 33,35,36 The aim of this paper is to continue these theoretical studies now considering deposition dynamics of Na clusters on a much "harder" surface than Ar, namely, MgO͑001͒ insulator surfaces. The structural properties and optical response of Na n on MgO have already been studied in great detail in using the present computational approach.…”
We investigate the dynamics of deposition of small Na clusters on MgO͑001͒ surface. A hierarchical modeling is used combining quantum mechanical with molecular mechanical description. Full time-dependent density-functional theory is used for the cluster electrons while the substrate atoms are treated at a classical level. We consider Na 6 and Na 8 at various impact energies. We analyze the dependence on cluster geometry, trends with impact energy, and energy balance. We compare the results with deposit on the much softer Ar͑001͒ surface.
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