阿贝尔微分和相对极值长度理论及其在极值缝映射中的应用

Hisao Mizumoto
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引用次数: 13

摘要

设R是任意开放黎曼曲面R是它的Kerekjarto-Stoilow紧化。划分理想边界_??_ (R)分为三个不相交的集合f¿,ƒÀ和ƒÁ。考虑R上具有有限Dirichlet范数的调和微分dU•adU•aR<•‡满足ƒÀ和ƒÁ上的边界条件:U是dU的一个积分,在ƒÀ的每个分量ƒÀ'上都是常数,其常数的选择使得•çƒÀ' dU*=0, dU*是dU的共轭微分,并且dU*=0沿ƒÁ。设An为这样的微分dU的空间。对于这样的空间,我们首先推导出一些结果,这些结果可以归结为众所周知的微分理论(例如。参见Nevanlinna [34], Ahlfors和Sario[5]),如果我们取整个理想边界J为δ¿。设f¶是R的一个子区域,它不是相对紧凑的。在f¶上的归一化函数u被定义为一个单值调和函数,它在f´上的边界值为0,并且具有与在ƒÀ和ƒÁ上的dU•o´Ah相同的边界行为。在•1中,我们将建立极大极小原理(定理1.1和1.2)、格林公式(引理1.4)和同调定理(推论1.3)等。进一步,我们将证明对于一个归一化函数u和dU•` ` Ah(` `¶)的方程
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Theory of Abelian differentials and relative extremal length with applications to extremal slit mappings
Let R be an arbitrary open Riemann surface and R be its Kerekjarto-Stoilow compactification. Partition the ideal boundary _??_ of R into three disjoint sets ƒ¿ , ƒÀ and ƒÁ . Consider a harmonic differential dU on R with finite Dirichlet norm •adU•aR<•‡ satisfying the boundary conditions on ƒÀ and ƒÁ: U , an integral of dU, is constant on each component ƒÀ' of ƒÀ with the constant so chosen that •çƒÀ' dU*=0 , dU* being the conjugate differential of dU, and dU*=0 along ƒÁ. Let An be the space of such differentials dU. For such the space Ah we shall first derive some consequences which are reduced to the well known theory of differentials (e. g . see Nevanlinna [34], and Ahlfors and Sario [5]) if we take the whole ideal boundary J as ƒ¿. Let ƒ¶ be a subregion of R which is not relatively compact . A normalized function u on ƒ¶ is defined as a single-valued harmonic function which takes the boundary value 0 on ƒ¿ and has the same boundary behaviors as dU• ̧Ah on ƒÀ and ƒÁ . In • ̃1, we shall establish the maximum-minimum principles (THEOREMS 1.1 and 1.2) , Green's formula (LEMMA 1.4) and the homology theorem (COROLLARY 1.3), etc. Further we shall show that for a normalized function u on ƒ¶ and dU• ̧Ah (ƒ¶) the equation
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