Abstract

A Gabor system generated by a window function ϕϕ and a rectangular lattice aZ×Z/ba \Z\times \Z/b is given by G(ϕ,aZ×Z/b):={e−2πint/bϕ(t−ma): (m,n)∈Z×Z}.{\mathcal G}(ϕ, a \Z\times \Z/b):=\{e^{-2πi n t/b} ϕ(t- m a):\ (m, n)\in \Z\times \Z\}. One of fundamental problems in Gabor analysis is to identify window functions ϕϕ and time-frequency shift lattices aZ×Z/ba \Z\times \Z/b such that the corresponding Gabor system G(ϕ,aZ×Z/b){\mathcal G}(ϕ, a \Z\times \Z/b) is a Gabor frame for L2(R)L^2(\R), the space of all square-integrable functions on the real line R\R. In this paper, we provide a full classification of triples (a,b,c)(a,b,c) for which the Gabor system G(χI,aZ×Z/b){\mathcal G}(χ_I, a \Z\times \Z/b) generated by the ideal window function χIχ_I on an interval II of length cc is a Gabor frame for L2(R)L^2(\R). For the classification of such triples (a,b,c)(a, b, c) (i.e., the abcabc-problem for Gabor systems), we introduce maximal invariant sets of some piecewise linear transformations and establish the equivalence between Gabor frame property and triviality of maximal invariant sets. We then study dynamic system associated with the piecewise linear transformations and explore various properties of their maximal invariant sets. By performing holes-removal surgery for maximal invariant sets to shrink and augmentation operation for a line with marks to expand, we finally parameterize those triples (a,b,c)(a, b, c) for which maximal invariant sets are trivial. The novel techniques involving non-ergodicity of dynamical systems associated with some novel non-contractive and non-measure-preserving transformations lead to our arduous answer to the abcabc-problem for Gabor systems.

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