Markov 谱与 Lagrange 谱在 $3$ 附近的分形维数
数论
2023-11-07 v2 动力系统
摘要
Lagrange 谱 L \mathcal{L} L 与 Markov 谱 M \mathcal{M} M 是实直线的子集,具有复杂的分形性质,自然出现于丢番图逼近的研究中。已知这些集合与任意半直线的交集的 Hausdorff 维数相同,即对每个 t ≥ 0 t \geq 0 t ≥ 0 有 d i m H ( L ∩ ( − ∞ , t ) ) = d i m H ( M ∩ ( − ∞ , t ) ) : = d ( t ) \mathrm{dim}_{\mathrm{H}}(\mathcal{L} \cap (-\infty, t)) = \mathrm{dim}_{\mathrm{H}}(\mathcal{M} \cap (-\infty, t)):= d(t) dim H ( L ∩ ( − ∞ , t )) = dim H ( M ∩ ( − ∞ , t )) := d ( t ) 。还已知 d ( 3 ) = 0 d(3)=0 d ( 3 ) = 0 且对每个 ε > 0 \varepsilon>0 ε > 0 有 d ( 3 + ε ) > 0 d(3+\varepsilon)>0 d ( 3 + ε ) > 0 。我们证明,对足够小的 ε > 0 \varepsilon > 0 ε > 0 ,有近似 d ( 3 + ε ) = 2 ⋅ W ( e c 0 ∣ log ε ∣ ) ∣ log ε ∣ + O ( log ∣ log ε ∣ ∣ log ε ∣ 2 ) d(3+\varepsilon) = 2\cdot\frac{W(e^{c_0}|\log \varepsilon|)}{|\log \varepsilon|}+\mathrm{O}\left(\frac{\log |\log \varepsilon|}{|\log \varepsilon|^2}\right) d ( 3 + ε ) = 2 ⋅ ∣ l o g ε ∣ W ( e c 0 ∣ l o g ε ∣ ) + O ( ∣ l o g ε ∣ 2 l o g ∣ l o g ε ∣ ) ,其中 W W W 表示 Lambert 函数(即 f ( x ) = x e x f(x)=xe^x f ( x ) = x e x 的逆)且 c 0 = − log log ( ( 3 + 5 ) / 2 ) ≈ 0.0383 c_0=-\log\log((3+\sqrt{5})/2) \approx 0.0383 c 0 = − log log (( 3 + 5 ) /2 ) ≈ 0.0383 。我们还证明该结果对用“合理”函数近似 d ( 3 + ε ) d(3+\varepsilon) d ( 3 + ε ) 是最优的,即在如下意义下:若 F ( t ) F(t) F ( t ) 是一个 C 2 C^2 C 2 函数使得 d ( 3 + ε ) = F ( ε ) + o ( log ∣ log ε ∣ ∣ log ε ∣ 2 ) d(3+\varepsilon) = F(\varepsilon) + \mathrm{o}\left(\frac{\log |\log \varepsilon|}{|\log \varepsilon|^2}\right) d ( 3 + ε ) = F ( ε ) + o ( ∣ l o g ε ∣ 2 l o g ∣ l o g ε ∣ ) ,则其二阶导数 F ′ ′ ( t ) F''(t) F ′′ ( t ) 在 t t t 趋于 0 0 0 时变号无穷多次。
引用
@article{arxiv.2208.14830,
title = {Fractal dimensions of the Markov and Lagrange spectra near $3$},
author = {Harold Erazo and Carlos Gustavo Moreira and Rodolfo Gutiérrez-Romo and Sergio Romaña},
journal= {arXiv preprint arXiv:2208.14830},
year = {2023}
}
备注
65 pages, one appendix. Major revision containing many more details and fixing mistakes