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See Ref. 2 for growth on Si. See Ref. 4 for growth on GaAs. For growth on high-temperature superconductors, see
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See Ref. 2 for growth on Si. See Ref. 4 for growth on GaAs. For growth on high-temperature superconductors, see T. R. Ohno, Y.-N. Yang, G. H. Kroll, K. Krause, L. D. Schmidt, J. H. Weaver, Y. Kimachi, Y. Hidaka, S. H. Pan, and A. L. de Lozanne, Phys. Rev. B 44, 2430 (1991);
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A. Zangwill, Physics at Surfaces (Cambridge University Press, Cambridge, England, 1988).
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85039000888
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The rare-gas buffer is always solid. The equilibrium melting temperature of Xe is 161 K, and an adsorbed rare-gas monolayer remains crystalline below 0.6ε/k [where ε is the interatomic potential (Ref. 31)] or 139 K for Xe. At this temperature, the buffer has completely sublimed in our experiments
-
The rare-gas buffer is always solid. The equilibrium melting temperature of Xe is 161 K, and an adsorbed rare-gas monolayer remains crystalline below 0.6ε/k [where ε is the interatomic potential (Ref. 31)] or 139 K for Xe. At this temperature, the buffer has completely sublimed in our experiments.
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14
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0000999716
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references therein
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Z. L. Wang, J. Phys. Chem. B 104, 1153 (2000), and references therein.
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85039030583
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The reduction reflects the fact that nearby clusters grow together and that energy released from atom capture can make small clusters mobile
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The reduction reflects the fact that nearby clusters grow together and that energy released from atom capture can make small clusters mobile.
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23
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33646656817
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F. Family, B. Sapoval, P. Meabin, and R. Wool MRS Symposia Proceedings No. 367 (Materials Research Society, Pittsburgh)
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St. C. Pencea and M. Dumitrascu, in Fractal Aspects of Materials edited by F. Family, B. Sapoval, P. Meabin, and R. Wool MRS Symposia Proceedings No. 367 (Materials Research Society, Pittsburgh), p. 373.
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26
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85039003346
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The effect should be even more pronounced on Ar. It would be observable if the sample were cold enough to produce a smooth buffer surface. At 20 K, however, Ar buffers have inhomogeneous thicknesses and cluster densities
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The effect should be even more pronounced on Ar. It would be observable if the sample were cold enough to produce a smooth buffer surface. At 20 K, however, Ar buffers have inhomogeneous thicknesses and cluster densities.
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27
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2442635618
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A recent study has demonstrated that the relaxation time of shape equilibration increases exponentially with crystallite size
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A recent study has demonstrated that the relaxation time of shape equilibration increases exponentially with crystallite size [Nicolas Combe, Pablo Jensen, and Alberto Pimpinelli, Phys. Rev. Lett. 85, 110 (2000)].
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34
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85038990048
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In this model, friction was assumed to arise from the excitation of lattice vibration modes during the sliding of the two surfaces
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In this model, friction was assumed to arise from the excitation of lattice vibration modes during the sliding of the two surfaces.
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36
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85039024926
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The binding energy of single Xe, Kr, or Ar atoms to polycrystalline Au is within several percent of the cohesive energy of the corresponding rare-gas solid (see Ref. 24)
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The binding energy of single Xe, Kr, or Ar atoms to polycrystalline Au is within several percent of the cohesive energy of the corresponding rare-gas solid (see Ref. 24).
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37
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0010545961
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T. R. Ohno, J. C. Patrin, U. S. Ayyala, and J. H. Weaver, Phys. Rev. B 44, 1891 (1991).
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