Abstract
In this paper we develop a Nash-Moser iteration type reducibility approach to prove the (inverse) localization for some d-dimensional discrete almost-periodic operators with power-law long-range hopping. We also provide a quantitative lower bound on the regularity of the hopping. As an application, some results of Sarnak (Comm Math Phys 84(3):377–401, 1982), Pöschel (Comm Math Phys 88(4):447–463, 1983), Craig (Comm Math Phys 88(1):113–131, 1983) and Bellissard et al. (Comm Math Phys 88(4):465–477, 1983) are generalized to the power-law hopping case.
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The exponential scale of smoothing operator was first introduced by Klainerman [Kla80].
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This work was supported by the NSFC (No. 12271380). The author would like to thank the editor and referees for their helpful suggestions.
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Appendix A
Appendix A
In this appendix we prove Lemma 3.1.
Proof of Lemma 3.1
The proof is standard and is based on the Hölder inequality. For any \(X\in \mathcal {M}^s\), recall that
We first show if \(Z=XY,\) then
In fact, we have
which implies (A.1).
Next, from (2.2), we obtain since (A.1)
where in the last equality we use the translation invariance of \(\mathfrak {B}\). Let \(a_\textbf{k}=\Vert X_\textbf{k}\Vert _\mathfrak {B},\ b_{\textbf{k}}=\Vert Y_{\textbf{k}}\Vert _\mathfrak {B}\). It suffices to study the sum \( \left( \sum _{\textbf{j}\in \mathbb Z^d}a_\textbf{j}b_{\textbf{k}-\textbf{j}}\right) ^2\langle \textbf{k}\rangle ^{2\,s}. \) We have the following two cases.
- Case 1.:
-
\(\textbf{j}\in \mathcal {I}_\textbf{k}:=\{\textbf{j}\in \mathbb Z^d:\ {\langle \textbf{k}\rangle ^{2\,s}}{\langle \textbf{k}-\textbf{j}\rangle ^{-2\,s}}\le 10\}.\) In this case we have
$$\begin{aligned} {\langle \textbf{k}\rangle ^{2s}}{\langle \textbf{k}-\textbf{j}\rangle ^{-2s}}\langle \textbf{j}\rangle ^{-2\alpha _0}\le 10\langle \textbf{j}\rangle ^{-2\alpha _0}. \end{aligned}$$(6.7)Hence we have by using the Hölder inequality
$$\begin{aligned} \sum _{\textbf{k}\in \mathbb Z^d}\left( \sum _{\textbf{j}\in \mathcal {I}_\textbf{k}}a_\textbf{j}b_{\textbf{k}-\textbf{j}}\right) ^2\langle \textbf{k}\rangle ^{2s}&\le \sum _{\textbf{k}\in \mathbb Z^d}\left( \sum _{\textbf{j}\in \mathcal {I}_\textbf{k}}a_\textbf{j}^2\langle \textbf{j}\rangle ^{2\alpha _0}\right) \left( \sum _{\textbf{j}\in \mathcal {I}_\textbf{k}}b_{\textbf{k}-\textbf{j}}^2\langle \textbf{j}\rangle ^{-2\alpha _0}\right) \langle \textbf{k}\rangle ^{2s}\\&\le \Vert X\Vert _{\alpha _0}^2\sum _{\textbf{k}\in \mathbb Z^d}\left( \sum _{\textbf{j}\in \mathcal {I}_\textbf{k}}b_{\textbf{k}-\textbf{j}}^2\langle \textbf{k}-\textbf{j}\rangle ^{2s}\langle \textbf{j}\rangle ^{-2\alpha _0}\langle \textbf{k}\rangle ^{2s}\langle \textbf{k}-\textbf{j}\rangle ^{-2s}\right) \\&\le 10\Vert X\Vert _{\alpha _0}^2\sum _{\textbf{k}\in \mathbb Z^d}\left( \sum _{\textbf{j}\in \mathcal {I}_\textbf{k}}b_{\textbf{k}-\textbf{j}}^2\langle \textbf{k}-\textbf{j}\rangle ^{2s}\langle \textbf{j}\rangle ^{-2\alpha _0}\right) \ (\mathrm{since (A.2)})\\&\le 10\Vert X\Vert _{\alpha _0}^2\sum _{\textbf{j}\in \mathbb Z^d}\langle \textbf{j}\rangle ^{-2\alpha _0}\left( \sum _{\textbf{k}\in \mathbb Z^d}b_{\textbf{k}-\textbf{j}}^2\langle \textbf{k}-\textbf{j}\rangle ^{2s}\right) \\&\le M_0^2\Vert X\Vert _{\alpha _0}^2\Vert Y\Vert _{s}^2, \end{aligned}$$where \(M_0=\sqrt{10\sum \limits _{\textbf{k}\in \mathbb Z^d}\langle \textbf{k}\rangle ^{-2\alpha _0}}<\infty \) since \(\alpha _0>d/2.\)
- Case 2.:
-
\(\textbf{j}\notin \mathcal {I}_\textbf{k}.\) In this case we must have \(\textbf{k}\ne \textbf{0}.\) Then
$$\begin{aligned} \langle \textbf{k}\rangle&>10^{\frac{1}{2s}}\langle \textbf{k}-\textbf{j}\rangle >10^{\frac{1}{2s}}|\textbf{k}-\textbf{j}|\ge 10^{\frac{1}{2s}}(|\textbf{k}|-|\textbf{j}|)\ge 10^{\frac{1}{2s}}(\langle \textbf{k}\rangle -\langle \textbf{j}\rangle ), \end{aligned}$$which yields
$$\begin{aligned} \langle \textbf{j}\rangle ^{-2s}\le (1-10^{-\frac{1}{2s}})^{-2s}\langle \textbf{k}\rangle ^{-2s}. \end{aligned}$$(A.1)Thus using again the Hölder inequality implies
$$\begin{aligned} \sum _{\textbf{k}\in \mathbb Z^d}\left( \sum _{\textbf{j}\notin \mathcal {I}_{\textbf{k}}}a_\textbf{j}b_{\textbf{k}-\textbf{j}}\right) ^2\langle \textbf{k}\rangle ^{2s}&\le \sum _{\textbf{k}\in \mathbb Z^d}\left( \sum _{\textbf{j}\in \mathbb Z^d}b_{\textbf{k}-\textbf{j}}^2\langle \textbf{k}-\textbf{j}\rangle ^{2\alpha _0}\right) \left( \sum _{\textbf{j}\notin \mathcal {I}_\textbf{k}}a_{\textbf{j}}^2\langle \textbf{k}-\textbf{j}\rangle ^{-2\alpha _0}\right) \langle \textbf{k}\rangle ^{2s}\\&\le \Vert Y\Vert _{\alpha _0}^2\sum _{\textbf{k}\in \mathbb Z^d}\left( \sum _{\textbf{j}\notin \mathcal {I}_\textbf{k}}a_{\textbf{j}}^2\langle \textbf{j}\rangle ^{2s}\langle \textbf{k}-\textbf{j}\rangle ^{-2\alpha _0}\langle \textbf{j}\rangle ^{-2s}\langle \textbf{k}\rangle ^{2s}\right) \\&\le (1-10^{-\frac{1}{2s}})^{-2s}\Vert Y\Vert _{\alpha _0}^2\sum _{\textbf{k}\in \mathbb Z^d}\left( \sum _{\textbf{j}\in \mathbb Z^d}a_{\textbf{j}}^2\langle \textbf{j}\rangle ^{2s}\langle \textbf{k}-\textbf{j}\rangle ^{-2\alpha _0}\right) \ (\mathrm{since (A.3)})\\&\le (1-10^{-\frac{1}{2s}})^{-2s}\Vert Y\Vert _{\alpha _0}^2\sum _{\textbf{j}\in \mathbb Z^d}a_{\textbf{j}}^2\langle \textbf{j}\rangle ^{2s}\left( \sum _{\textbf{k}\in \mathbb Z^d}\langle \textbf{k}-\textbf{j}\rangle ^{-2\alpha _0}\right) \\&\le M_1^2(s)\Vert Y\Vert _{\alpha _0}^2\Vert X\Vert _{s}^2, \end{aligned}$$where \(M_1(s)=(1-10^{-\frac{1}{2\,s}})^{-s}\sqrt{\sum \limits _{\textbf{k}\in \mathbb Z^d}\langle \textbf{k}\rangle ^{-2\alpha _0}}<\infty \) since \(\alpha _0>d/2.\)
Combining Case 1 and Case 2 implies
which proves Lemma 3.1, where \(K_0=\sqrt{2}M_0,\ K_1(s)=\sqrt{2}M_1(s).\)
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Shi, Y. Localization for Almost-Periodic Operators with Power-law Long-range Hopping: A Nash-Moser Iteration Type Reducibility Approach. Commun. Math. Phys. 402, 1765–1806 (2023). https://doi.org/10.1007/s00220-023-04756-z
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DOI: https://doi.org/10.1007/s00220-023-04756-z