$$L^p$$ Teichmüller 理论:临界点的存在性和规律性

IF 4.6 Q2 MATERIALS SCIENCE, BIOMATERIALS ACS Applied Bio Materials Pub Date : 2024-02-02 DOI:10.1007/s00205-023-01955-9
Gaven Martin, Cong Yao
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引用次数: 0

摘要

我们研究 p-共形能量函数的最小值,$$\begin{aligned}(开始{aligned})。textsf{E}_p(f):=int _{\mathbb {D}}{mathbb {K}}^p(z,f)\,text {d}z,\quad f|_{\mathbb {S}=f_0|_{\mathbb {S}}, \end{aligned}$$定义为自映射 \(f.z),\quad f|_{\mathbb {S}=f_0|_{\mathbb {S}}, \end{aligned}$$:f: {\mathbb {D}\rightarrow {\mathbb {D}}\) 具有有限失真和规定边界值 \(f_0\)。这里 $$\begin{aligned} {\mathbb {K}}(z,f) = \frac\{Vert Df(z)\Vert ^2}{J(z,f)} = \frac{1+|\mu _f(z)|^2}{1-|\mu _f(z)|^2}\我们证明,对于准对称边界数据,极限情形 \(p\rightarrow \infty \) 恢复了极值准共形映射的经典 Teichmüller 理论(部分是 Ahlfors 的结果),而对于 \(p\rightarrow 1\) 则恢复了调和映射理论。(textsf{E}_p\)的临界点总是满足内变分布方程 $$\begin{aligned} 2p\int _{\mathbb {D}}{\mathbb {K}}^p\;\frac{overline\{mu _f}}{1+|\mu _f|^2}\varphi _{overline{z}}\; \text {d}z=\int _{mathbb {D}}{mathbb {K}}^p \; \varphi _z\; \text {d}z, \quad \forall \varphi \ in C_0^\infty ({\mathbb {D}}).\end{aligned}$We establish the existence of minimisers in the a priori regularity class \(W^{1、\frac{2p}{p+1}}({\mathbb {D}})中存在最小化函数,并证明这些最小化函数有一个伪反--一个连续的 \(W^{1,2}({\mathbb {D}})的 \({\mathbb {D}}) 与 \((h\circ f)(z)=z\) 的投射几乎无处不在。然后我们给出一个充分条件来确保分布方程的解的平滑性。例如 \({\mathbb {K}}(z,f)\in L^{p+1}_{loc}({\mathbb {D}}) 就足以暗示分布方程的解是局部衍射。此外,L^1({\mathbb {D}})\({\mathbb {K}}(w,h)\in L^1({\mathbb {D}}))将暗示 h 是同构的,而这些结果共同产生了一个差分最小化。我们将证明这种更高的正则性假设对于内变分方程的临界点是必要的。
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The \(L^p\) Teichmüller Theory: Existence and Regularity of Critical Points

We study minimisers of the p-conformal energy functionals,

$$\begin{aligned} \textsf{E}_p(f):=\int _{\mathbb {D}}{\mathbb {K}}^p(z,f)\,\text {d}z,\quad f|_{\mathbb {S}}=f_0|_{\mathbb {S}}, \end{aligned}$$

defined for self mappings \(f:{\mathbb {D}}\rightarrow {\mathbb {D}}\) with finite distortion and prescribed boundary values \(f_0\). Here

$$\begin{aligned} {\mathbb {K}}(z,f) = \frac{\Vert Df(z)\Vert ^2}{J(z,f)} = \frac{1+|\mu _f(z)|^2}{1-|\mu _f(z)|^2} \end{aligned}$$

is the pointwise distortion functional and \(\mu _f(z)\) is the Beltrami coefficient of f. We show that for quasisymmetric boundary data the limiting regimes \(p\rightarrow \infty \) recover the classical Teichmüller theory of extremal quasiconformal mappings (in part a result of Ahlfors), and for \(p\rightarrow 1\) recovers the harmonic mapping theory. Critical points of \(\textsf{E}_p\) always satisfy the inner-variational distributional equation

$$\begin{aligned} 2p\int _{\mathbb {D}}{\mathbb {K}}^p\;\frac{\overline{\mu _f}}{1+|\mu _f|^2} \varphi _{\overline{z}}\; \text {d}z=\int _{\mathbb {D}}{\mathbb {K}}^p \; \varphi _z\; \text {d}z, \quad \forall \varphi \in C_0^\infty ({\mathbb {D}}). \end{aligned}$$

We establish the existence of minimisers in the a priori regularity class \(W^{1,\frac{2p}{p+1}}({\mathbb {D}})\) and show these minimisers have a pseudo-inverse - a continuous \(W^{1,2}({\mathbb {D}})\) surjection of \({\mathbb {D}}\) with \((h\circ f)(z)=z\) almost everywhere. We then give a sufficient condition to ensure \(C^{\infty }({\mathbb {D}})\) smoothness of solutions to the distributional equation. For instance \({\mathbb {K}}(z,f)\in L^{p+1}_{loc}({\mathbb {D}})\) is enough to imply the solutions to the distributional equation are local diffeomorphisms. Further \({\mathbb {K}}(w,h)\in L^1({\mathbb {D}})\) will imply h is a homeomorphism, and together these results yield a diffeomorphic minimiser. We show such higher regularity assumptions to be necessary for critical points of the inner variational equation.

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来源期刊
ACS Applied Bio Materials
ACS Applied Bio Materials Chemistry-Chemistry (all)
CiteScore
9.40
自引率
2.10%
发文量
464
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