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On the distribution of zeros of the Hermite-Pade polynomials for three algebraic functions $1,f,f^2$ and the global topology of the Stokes lines for some differential equations of the third order

机译:关于Hermite-pade多项式零点的三维分布   代数函数$ 1,f,f ^ 2 $和斯托克斯线的全局拓扑   一些三阶微分方程

摘要

The paper presents some heuristic results about the distribution of zeros ofHermite-Pade polynomials of first kind for the case of three functions$1,f,f^2$, where $f$ has the form $f(z): = \prod\limits_ {j = 1 } ^3 (z-a_j) ^{\alpha_j} $, $\alpha_j \in \mathbb C\setminus \mathbb Z $, $ \sum \limits_ {j= 1 } ^ 3 \alpha_j = 0 $, $ f (\infty) = 1 $. Answers are given in termsrelated to the problem of extreme minimum capacity of a plane Nuttallcondenser, two plates of which intersect ("hooked" for each other) in a fivepoints: the branch points $ a_1, a_2, a_3 $ of function $ f $, at $ v_1 = v $,where $ v = v (a_1, a_2, a_3) $ the Chebotarev point corresponding to triplepoints $ a_1, a_2, a_3 $, and another "unknown" at $ v_2 \neq v_1, a_1, a_2,a_3 $ (see Fig1-Fig3). The connection between the distribution of zeros of Hermite-Pade polynomialsand global topology of the Stokes lines and the asymptotic behavior ofLiouville-Green solutions of a class of homogeneous linear differentialequations of the third order containing a large parameter is the free term isestablished. The basic idea of the new and still heuristic approach is to reduce at firstsome theoretical potential vector equilibrium problem to the scalar problemwith the external field, and then use the general method of Gonchar-Rakhmanovdeveloped in 1987 for solving the Varga problem "about $ 1/9 $". It is supposed that in the general case of an arbitrary algebraic function $f $ it is imposible to constract the Nuttall condenser for a set of threefunctions $ 1, f, f ^ 2 $ without the knowledge of the structure of the Stahlcompact for function $ f $. Namely, the Nuttall condenser is constructed usingGreen's function $ g_ {D} (z, \infty) $ for the Stahl domain $ D $ and "core"of Stahl compact, which consists of "effective" branch points of $ f $ andcorresponding Chebotarev points.
机译:对于三个函数$ 1,f,f ^ 2 $,其中$ f $的形式为$ f(z):= \ prod \,本文提供了一些启发式结果,这些启发式结果涉及第一类Herrmite-Pade多项式的零点分布。 Limits_ {j = 1} ^ 3(z-a_j)^ {\\ alpha_j} $,$ \ alpha_j \ in \ mathbb C \ setminus \ mathbb Z $,$ \ sum \ limits_ {j = 1} ^ 3 \ alpha_j = 0 $,$ f(\ infty)= 1 $。给出的答案与平面Nuttallcondenser的极小最小容量问题有关,该平面的两块板在五个点上相交(彼此“钩接”):分支点$ a_1,a_2,a_3 $函数$ f $,在$ v_1 = v $,其中$ v = v(a_1,a_2,a_3)$对应于三点$ a_1,a_2,a_3 $的Chebotarev点,以及在$ v_2 \ neq v_1,a_1,a_2处的另一个“未知”点, a_3 $(请参见图1-图3)。建立了自由项,建立了Hermite-Pade多项式的零分布和Stokes线的整体拓扑与一类三阶包含大参数的齐次线性微分方程的Liouville-Green解的渐近行为的联系。新的仍然启发式方法的基本思想是首先将一些理论上的势矢量平衡问题简化为具有外部场的标量问题,然后使用1987年开发的Gonchar-Rakhmanov的一般方法来求解Varga问题“大约$ 1 / 9 $”。假定在任意代数函数$ f $的一般情况下,在不知道函数Stahlcompact的结构$的情况下,不可能针对一组三个函数$ 1,f,f ^ 2 $约束Nuttall凝聚器。 f $。即,Nuttall冷凝器是针对Stahl域$ D $和Stahl契约的“核心”,使用格林函数$ g_ {D}(z,\ infty)$和Stahl契约的“核心”构造而成的,后者由$ f $的“有效”分支点和相应的Chebotarev点。

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  • 作者

    Suetin, Sergey;

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  • 年度 2013
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  • 原文格式 PDF
  • 正文语种 {"code":"ru","name":"Russian","id":37}
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