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3
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11
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0000791158
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0000634932
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D. R. Bowler, J H G. Owen, K. Miki, and G A D. Briggs, Phys. Rev. B57, 8790 (1998).
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Miki, K.3
Briggs, G.A.D.4
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14
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0000445753
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Goringe, C.M.3
Horsfield, A.P.4
Pettifor, D.G.5
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16
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85037912433
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The third, higher energy diffusive channel is between dimer rows
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The third, higher energy diffusive channel is between dimer rows.
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19
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30544439683
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B. S. Swartzentruber, Y W. Mo, M B. Webb, and M G. Lagally, J. Vac. Sci. Technol. A7, 2901 (1989).
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Mo, Y.W.2
Webb, M.B.3
Lagally, M.G.4
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22
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0002407010
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The fitting algorithm (York’s method) ensures that the parameters and their uncertainties correctly reflect the uncertainties in both the rates and the temperatures
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B. C. Reed, Am. J. Phys.60, 59 (1992). The fitting algorithm (York’s method) ensures that the parameters and their uncertainties correctly reflect the uncertainties in both the rates and the temperatures.
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Am. J. Phys.
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Reed, B.C.1
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23
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85037895045
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Temperature uncertainties reflect uncertainties in the corresponding H diffusion rates as well as uncertainties in the H attempt frequency and activation energy
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Temperature uncertainties reflect uncertainties in the corresponding H diffusion rates as well as uncertainties in the H attempt frequency and activation energy.
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24
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85037905343
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The uncertainties of the (formula presented) ratio reflect the dependence of the (formula presented) measurement on (formula presented) through the use of (formula presented) in determining the temperatures
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The uncertainties of the (formula presented) ratio reflect the dependence of the (formula presented) measurement on (formula presented) through the use of (formula presented) in determining the temperatures.
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25
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85037883792
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The agreement between activation energies, in spite of the disagreement between attempt frequencies, can be attributed to a ∼40 K temperature offset between the two experiments
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The agreement between activation energies, in spite of the disagreement between attempt frequencies, can be attributed to a ∼40 K temperature offset between the two experiments.
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30
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85037899221
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Estimating a temperature limit is complicated by the 0.3-eV raising of the diffusion barrier for H atoms when they become paired on a single Si dimer
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Estimating a temperature limit is complicated by the 0.3-eV raising of the diffusion barrier for H atoms when they become paired on a single Si dimer.
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31
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0000541655
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See Refs. 12, 27, or, and
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See Refs. 12, 27, or A. Vittadini, A. Selloni, and M. Casarin, Phys. Rev. B49, 11 191 (1994).
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Phys. Rev. B
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Vittadini, A.1
Selloni, A.2
Casarin, M.3
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33
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0001217212
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The bend mode values used are the average of values for symmetric and antisymmetric bending of H on a monohydride terminated dimer
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H. Froitzheim, U. Köhler, and H. Lammering, Surf. Sci.149, 537 (1985). The bend mode values used are the average of values for symmetric and antisymmetric bending of H on a monohydride terminated dimer.
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Surf. Sci.
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Froitzheim, H.1
Köhler, U.2
Lammering, H.3
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34
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85037900540
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(private communication)
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U. Hansen (private communication).
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Hansen, U.1
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