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Structural changes of silver terrace domains in aqueous perchloric acid solution at constant anodic current density (j) and room temperature were followed by in situ scanning tunneling microscopy sequential imaging. For j15 {μ}A cm^-2 silver electrodissolution proceeds at step edges without roughening. Conversely, for j{}15 {μ}A cm^-2 the silver surface becomes progressively rougher to attain, after a certain critical time, a steady roughness. In this case, the dynamic scaling theory applied to STM images indicates that the dissolving silver surface can be described as a self-affine fractal surface with a static roughening exponent {α}=0.90±{}0.06, and a dynamic roughening exponent {β}=0.36±{}0.08. The value of {α} is consistent with the relevant role played by surface diffusion in the silver electrodissolution mechanism, whereas the value of {β} is slightly higher than those derived from growth models incorporating surface diffusion. The difference in the value of {β} would reflect the influence of either the electric field or energetic barriers at step edges on the rate of roughness development. {} 1996 The American Physical Society.
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Vela et al. (1996) studied this question.
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