Dual pairs of Gabor frames for trigonometric generators without the partition of unity property (Q2892237)

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scientific article; zbMATH DE number 6047353
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Dual pairs of Gabor frames for trigonometric generators without the partition of unity property
scientific article; zbMATH DE number 6047353

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    18 June 2012
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    Gabor frames
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    dual frame
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    Dual pairs of Gabor frames for trigonometric generators without the partition of unity property (English)
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    The aim of this paper is to provide explicit constructions of dual pairs of frames having Gabor structure. To be more precise, let us denote by \(T_a\) and \(E_b\) the translation and modulation operators on \(L^2({\mathbb R})\) defined by \((T_af)(x) = f(x-a)\) and \((E_bf)(x) = e^{2\pi i b x}f(x).\) Let \(g\in L^2({\mathbb R})\) and \(a, b > 0\) be given. The system \(\{E_{mb}T_{na}g\}_{m,n\in {\mathbb Z}}\) is called a Gabor frame if there exist constants \(A,B > 0\) such that NEWLINE\[NEWLINE A||f||^2 \leq \sum_{m,n\in {\mathbb Z}}|\left<f, E_{mb}T_{na}g\right>|^2 \leq B||f||^2\;\;\forall f\in L^2({\mathbb R}).NEWLINE\]NEWLINE A typical result of the article is as follows. Let \(\eta \in {\mathbb N}, a = 1, b\in ]0, \frac{1}{5}]\) and consider the function \(g(x) = \sin^\eta(\frac{1}{3}\pi x)\chi_{[0,3]}(x).\) Then \(\{E_{mb}T_{na}g\}_{m,n\in {\mathbb Z}}\) is a Gabor frame admitting a dual Gabor frame \(\{E_{mb}T_{na}h\}_{m,n\in {\mathbb Z}}\) for some \(h\) of the form \(h(x) = (\frac{4}{3})^\eta b (Cg(x) + Dg(x+1) + Eg(x+2))\) if and only if \(\eta < 6\).NEWLINENEWLINE This is part of Theorem 2.2, which also contains a discussion of the concrete expression for \(h\) in the case \(\eta < 6.\) Frames generated by \(g(x) = \sin(\frac{\eta}{3}\pi x)\chi_{[0,3]}(x)\) are also considered.
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