Diffusion conjecture for the almost Mathieu–Markovian equation

Let gRg\in\mathbb{R}, let θ,α[0,1]\theta,\alpha\in[0,1], and consider the almost Mathieu–Markovian equation on 2(Z)\ell^2(\mathbb{Z}) with potential 2gcos2π(θ+xα)2g\cos 2\pi(\theta+x\alpha) and disorder coupling λ\lambda.

Almost Mathieu diffusion conjecture. For almost every θ,α[0,1]\theta,\alpha\in[0,1], the equation has a diffusion constant D(g,λ)(0,)D(g,\lambda)\in(0,\infty) that is smooth for all (g,λ)R×R+(g,\lambda)\in\mathbb{R}\times\mathbb{R}^+. Moreover, D(g,λ)O(λ2)D(g,\lambda)\sim O(\lambda^2) for all g>1|g|>1 and D(g,λ)O(λ2)D(g,\lambda)\sim O(\lambda^{-2}) for all g<1|g|<1.

This conjecture applies the expected relation between diffusion and the transport regime of the unperturbed almost Mathieu operator: the localized regime g>1|g|>1 and the ballistic regime g<1|g|<1 are predicted to produce opposite small-coupling scalings. The critical case g=1|g|=1 is not covered by the statement.

Sources & referencesView supporting material

Primary source

Jeffrey Schenker, F. Zak Tilocco and Shiwen Zhang, “Diffusion in the mean for a periodic Schrödinger equation perturbed by a fluctuating potential”, arXiv:1901.06598 (2019).

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