In this note we explore the structure of the diffusion metric of Coifman-Lafon determined by fractional dyadic Laplacians. The main result is that, for each \(t> 0\), the diffusion metric is a function of the dyadic distance, given in \(R^+\) by \(δ(x,y) = inf\{|I| I is a dyadic interval containing x and y\}\). Even if these functions of \(δ\) are not equivalent to \(δ\), the families of balls are the same, to wit, the dyadic intervals.
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Acosta et al. (2024) studied this question.
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