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We present the results of first-principles-derived Monte Carlo simulations of H adatom diffusion on the Si(100)-2×{}1 surface. We developed an analytical Si/H potential which was fit to the results of first-principles electronic-structure calculations of H adatom adsorption and diffusion on embedded silicon clusters designed to model Si(100)-2×{}1. With this interaction potential, we calculated the rate constants for a H adatom hopping from one site to another, both parallel and perpendicular to the silicon dimer rows, using Monte Carlo simulations to extract exact classical transition-state-theory rate constants. The diffusion constants for H adatoms moving parallel and perpendicular to the surface dimer rows both were found to obey an Arrhenius temperature dependence (over the temperature range T=700--900 K) with preexponential factors and activation energies of D₀^∥=4.0×{}10^±0.5 cm² s^-1, Eₐ^∥=38.1±{}1.7 kcal/mol, and D₀^⊥=4.8×{}10^-1.0±1.8 cm² s^-1, Eₐ^⊥=62.8±{}6.4 kcal/mol, respectively. These results confirm our previous suggestion that anisotropic diffusion of H adatoms on the Si(100)-2×{}1 surface will occur preferentially along the edges of silicon dimer rows. However, these predicted H adatom diffusion rates are orders of magnitude faster (along the dimer rows) or slower (across the dimer rows) than measured values for the rates of H₂ desorption from Si(100)-2×{}1-H. Thus these results suggest that diffusion of hydrogen atoms may not be involved in the rate-limiting step for hydrogen desorption from Si(100).
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Wu et al. (1994) studied this question.
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