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A linear fit of the width w (τ) at the transition time τ, as a function of the spatial periodicity, gives [w (τ)] (qn) =a qn +b, with a=0.547 (4) and b=0.8 (2). The times τ 's and the relative widths w (τ) 's have been determined by fitting the subdiffusive behavior of the incommensurate case and the linear behaviors of the commensurate cases and finding the intersection points between these two fits.
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When λ>2 and the interaction strength β is of the order of or larger than the upper bound found by energy conservation arguments, we find that the self-trapping can be so strong to suppress also the growth of the width w (t) (see also).
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When λ>2 and the interaction strength β is of the order of or larger than the upper bound found by energy conservation arguments, we find that the self-trapping can be so strong to suppress also the growth of the width w (t) (see also).
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