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THE GEOMETRY OF THE DIRICHLET ETA FUNCTION

机译:dirichlet eta函数的几何形状

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This paper presents a geometric interpretation of the Dirichlet eta function, and presents an analysis of the zeros of the eta function in that context. As the sum of a series of products, the eta function is recognized as two dot products involving three high-dimensional vectors. Two of these vectors, corresponding to the imaginary part of input value s, define a plane; the third vector corresponds to the real part of s. At a zero of the eta function, both of the dot products must be zero, meaning that the corresponding vectors are orthogonal. An analysis of the geometric properties of the curve traced by the vector corresponding to the real part of s as it varies from 0 to 1, and the geometric properties of the space perpendicular to the plane corresponding to the imaginary part of s leads to the conclusion that these elements can only intersect once for any given non-zero imaginary value of s. The implication is that there is only one zero of the eta function over that range of real values of s for a given non-zero imaginary value of s.
机译:本文介绍了Dirichlet ETA函数的几何解释,并在这种情况下介绍了ETA函数零的分析。作为一系列产品的总和,ETA函数被认为是涉及三个高维矢量的两种点产物。这些向量中的两个,与输入值s的假想部分相对应,定义了一个平面。第三个向量对应于s的实际部分。在ETA函数的零下,两个点产物必须为零,这意味着相应的向量是正交的。对矢量所追踪的曲线的几何特性的分析,与S的实际部分相对应,因为它从0到1不等,并且垂直于与S的假想部分相对的平面的空间的几何特性导致结论对于任何给定的非零假想值s,这些元素只能相交一次。这意味着,对于给定的s的非零假想值,s的真实值范围内只有一个零一个零函数。

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