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Density and location of resonances for convex co-compact hyperbolic surfaces

机译:共凸双曲曲面的共振密度和位置

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Let X = Γ H~2 be a convex co-compact hyperbolic surface and let δ be the Hausdorff dimension of the limit set. Let Δ_X be the hyperbolic Laplacian. We show that the density of resonances of the Laplacian Δ_X in rectangles{σ ≤ Re(s) ≤ δ, |Im(s)| ≤ T }is less than O(T ~(1+τ(σ))) in the limit T →∞, where τ(σ)<δ as long as σ >δ/2. This improves the previous fractal Weyl upper bound of Zworski (Invent. Math. 136(2):353-409, 1999) and goes in the direction of a conjecture stated in Jakobson and Naud (Geom. Funct. Anal. 22(2):352-368, 2012).
机译:令X =Γ H〜2为凸协紧双曲曲面,令δ为极限集的Hausdorff维数。令Δ_X为双曲型拉普拉斯算子。我们显示矩形中的拉普拉斯算子Δ_X的共振密度{σ≤Re(s)≤δ,| Im(s)| ≤T}在极限T→∞内小于O(T〜(1 +τ(σ))),只要σ>δ/ 2,则τ(σ)<δ。这改善了Zworski的先前分形Weyl上限(Invent。Math。136(2):353-409,1999),并朝着Jakobson和Naud(Geom。Funct。Anal。22(2))中所述的猜想方向发展。 :352-368,2012)。

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