Gabor's signal expansion and the Gabor transform based on a non-orthogonal sampling geometry

M. J. Bastiaans, A. J. V. Leest
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引用次数: 6

Abstract

Gabor's (1946) signal expansion and the Gabor transform are formulated on a non-orthogonal time-frequency lattice instead of on the traditional rectangular lattice. The reason for doing so is that a non-orthogonal sampling geometry might be better adapted to the form of the window functions (in the time-frequency domain) than an orthogonal one. Oversampling in the Gabor scheme, which is required to have mathematically more attractive properties for the analysis window, then leads to better results in combination with less oversampling. The new procedure presented in this paper is based on considering the non-orthogonal lattice as a sub-lattice of a denser orthogonal lattice that is oversampled by a rational factor. In doing so, Gabor's signal expansion on a non-orthogonal lattice can be related to the expansion on an orthogonal lattice (restricting ourselves, of course, to only those sampling points that are part of the non-orthogonal sub-lattice), and all the techniques that have been derived for rectangular sampling can be used, albeit in a slightly modified form.
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基于非正交采样几何的Gabor信号展开和Gabor变换
Gabor(1946)的信号展开和Gabor变换是在非正交时频晶格上而不是在传统的矩形晶格上表述的。这样做的原因是,非正交采样几何可能比正交采样几何更适合于窗函数的形式(在时频域)。Gabor方案中的过采样,需要在数学上对分析窗口具有更有吸引力的属性,然后与更少的过采样相结合,导致更好的结果。本文提出的新方法是把非正交格看作是被有理因子过采样的稠密正交格的子格。这样,Gabor在非正交晶格上的信号展开可以与在正交晶格上的展开相关联(当然,限制我们自己只使用那些属于非正交子晶格的采样点),并且可以使用所有为矩形采样导出的技术,尽管形式略有修改。
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