Exploring the Irreducible Support

B. Brames
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Abstract

The phase problem confronts one with the task obtaining a function having a specified autocorrelation (or Fourier modulus) which is also consistent with a limited number of object constraints. In many case of interest it is known that the object has compact support; indeed, in two dimensions this is often sufficient to uniquely define it [1]. Nonetheless, one can usually find an autocorrelation such that some object defined on the same compact support is but one of a multitude of functions having that autocorrelation. However, if the object happens to be defined on Eisenstein's support, it has been shown that the object is always uniquely described by its autocorrelation [2]. We shall call supports of the Eisenstein-type irreducible supports. Unfortunately, variations on Eisenstein's support are the only ones to have been shown to be irreducible, and the method of proof for Eisenstein's support does not lend itself to ready generalization. Herein the irreducible support will be defined in a wider sense, and a method of testing an arbitrary convex support for irreducibility will be presented.
探索不可约支持
相位问题面临的任务是获得具有特定自相关(或傅立叶模)的函数,该函数也与有限数量的目标约束一致。在许多感兴趣的情况下,我们知道物体有紧密的支撑;事实上,在二维中,这通常足以唯一地定义它[1]。尽管如此,人们通常可以找到自相关,这样在同一紧凑支持上定义的某些对象只是具有自相关的众多函数之一。然而,如果对象恰好是在爱森斯坦的支持下定义的,则已经证明对象总是由其自相关来唯一描述[2]。我们称爱森斯坦型的支撑为不可约支撑。不幸的是,爱森斯坦支持的变体是唯一被证明是不可约的,而爱森斯坦支持的证明方法并不适合于现成的推广。本文将在更广泛的意义上定义不可约支撑,并给出一种检验任意凸支撑不可约性的方法。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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