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Compactly supported Gabor orthonormal bases

Published 28 May 2026 in math.FA | (2605.29984v1)

Abstract: We characterize all lattices ΛR<sup>2Λ\subset \mathbb{R}<sup>2 and all compactly supported functions gL<sup>2(R)g \in L<sup>2(\mathbb{R}) for which the Gabor system $\left { e<sup>{2πi</sup> s x} g(x-t) : (t,s) \in Λ\right }$ forms an orthonormal basis for L<sup>2(R)L<sup>2(\mathbb{R}). The characterization is given in geometric terms through translation tilings and discreteness properties of lattice projections. In particular, this resolves a conjecture of Han and Wang on the non-existence of Gabor bases along specific irrational lattices. Finally, we construct Gabor bases that cannot be realized by any product set, answering a problem of Iosevich and Mayeli.

Authors (1)

Summary

  • The paper completely characterizes lattice-based Gabor orthonormal bases with compactly supported windows, showing existence exactly when the lattice has density 1 and a discrete first-coordinate projection.
  • It proves that every admissible window has magnitude a scaled indicator function of a bounded measurable set that tiles the real line, while irrational shear lattices cannot support compactly supported Gabor bases.
  • It answers the Iosevich–Mayeli question affirmatively by using fractional Fourier transforms to construct a Gabor basis with no product-set realization, necessarily employing a window with unbounded support.

This paper by Lukas Liehr resolves two long-standing problems concerning Gabor orthonormal bases with compactly supported windows: it proves a conjecture of Han and Wang on the non-existence of such bases along irrational lattices, and it answers a question of Iosevich and Mayeli by constructing Gabor bases that cannot be realized along any product set (2605.29984). The main contribution is a complete geometric characterization of all lattices ΛR2\Lambda \subset \mathbb{R}^2 and all compactly supported windows gL2(R)g \in L^2(\mathbb{R}) for which the Gabor system G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\} forms an orthonormal basis (ONB) for L2(R)L^2(\mathbb{R}). This problem is often called the Fuglede–Gabor problem, in analogy with Fuglede's spectral set problem.

Main characterization

The central result gives necessary and sufficient conditions on the lattice alone. For every full-rank lattice ΛR2\Lambda \subset \mathbb{R}^2, there exists a compactly supported gg such that G(g,Λ)\mathbf{G}(g,\Lambda) is an ONB if and only if:

  1. the lattice density satisfies D(Λ)=1D(\Lambda)=1, and
  2. the projection onto the first coordinate π1(Λ)\pi_1(\Lambda) equals aZa\mathbb{Z} for some gL2(R)g \in L^2(\mathbb{R})0, i.e., is discrete.

The density condition was already known to be necessary; the discreteness of the projection is the new obstruction, and it is sharp. When both conditions hold, a second theorem characterizes all admissible windows: gL2(R)g \in L^2(\mathbb{R})1 is an ONB exactly when

gL2(R)g \in L^2(\mathbb{R})2

for a bounded measurable set gL2(R)g \in L^2(\mathbb{R})3 that tiles the line by gL2(R)g \in L^2(\mathbb{R})4-translates. Thus, remarkably, the admissible windows are determined up to phase by measurable translational tilings — no smoothness or regularity of gL2(R)g \in L^2(\mathbb{R})5 beyond compact support enters the characterization. In particular, the classical system gL2(R)g \in L^2(\mathbb{R})6 is recovered as the special case gL2(R)g \in L^2(\mathbb{R})7, gL2(R)g \in L^2(\mathbb{R})8.

An immediate consequence is the resolution of the Han–Wang conjecture: for the shear lattice gL2(R)g \in L^2(\mathbb{R})9 with G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\}0 and G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\}1, one has G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\}2, which is dense in G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\}3. Hence no compactly supported window generates an ONB along G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\}4. Since Bekka's result guarantees some (necessarily non-compactly-supported) window exists for every lattice, the conjecture isolates compact support as precisely the property destroyed by irrational shears.

Proof strategy for the Han–Wang conjecture

The proof proceeds by contradiction and combines harmonic analysis on fibres with a complex-analytic rigidity argument. Assuming G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\}5 is an ONB with G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\}6 supported in a compact set G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\}7, the author introduces a weighted Zak-type transform

G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\}8

interpreted as an G(g,Λ)={e2πisxg(xt):(t,s)Λ}\mathbf{G}(g,\Lambda) = \{e^{2\pi i s x} g(x-t) : (t,s)\in\Lambda\}9-Fourier series in L2(R)L^2(\mathbb{R})0. Orthonormality forces the autocorrelations of the coefficient sequence to be Kronecker deltas, whence L2(R)L^2(\mathbb{R})1 almost everywhere, together with the quasi-periodicity relation

L2(R)L^2(\mathbb{R})2

The key structural lemma shows that for almost every fixed L2(R)L^2(\mathbb{R})3, the distributional Fourier transform of L2(R)L^2(\mathbb{R})4 is supported in L2(R)L^2(\mathbb{R})5: this follows because testing against L2(R)L^2(\mathbb{R})6 yields Fourier coefficients proportional to inner products of L2(R)L^2(\mathbb{R})7 with translates of L2(R)L^2(\mathbb{R})8, which vanish by disjointness of supports; a separability argument removes the dependence of the null set on the test function.

A second ingredient is a rigidity lemma of independent interest: if L2(R)L^2(\mathbb{R})9 is unimodular almost everywhere and its distributional Fourier transform has compact support, then ΛR2\Lambda \subset \mathbb{R}^20 for some unimodular constant ΛR2\Lambda \subset \mathbb{R}^21 and some frequency ΛR2\Lambda \subset \mathbb{R}^22 in the support of ΛR2\Lambda \subset \mathbb{R}^23. The proof uses Paley–Wiener–Schwartz to represent ΛR2\Lambda \subset \mathbb{R}^24 as an entire function of exponential type, forms the entire function ΛR2\Lambda \subset \mathbb{R}^25, which equals ΛR2\Lambda \subset \mathbb{R}^26 on ΛR2\Lambda \subset \mathbb{R}^27 and hence identically, so ΛR2\Lambda \subset \mathbb{R}^28 is zero-free; Hadamard factorization then forces ΛR2\Lambda \subset \mathbb{R}^29 to be a pure exponential.

Combining these, one obtains gg0 with measurable gg1 and gg2 (measurability extracted via injectivity of gg3 on the compact set gg4). The quasi-periodicity relation then implies gg5 almost everywhere. Here irrationality enters decisively: since gg6 is bounded and measurable and invariant under the irrational rotation by gg7, ergodicity forces gg8 to be constant. The remaining functional equation for gg9 becomes G(g,Λ)\mathbf{G}(g,\Lambda)0, whose Fourier coefficients satisfy G(g,Λ)\mathbf{G}(g,\Lambda)1 for all G(g,Λ)\mathbf{G}(g,\Lambda)2; any nonzero coefficient would violate square-summability, so G(g,Λ)\mathbf{G}(g,\Lambda)3, contradicting G(g,Λ)\mathbf{G}(g,\Lambda)4 almost everywhere. The contradiction establishes non-existence.

Reduction to the standard lattice

With the Han–Wang conjecture in hand, the general classification follows from a chirp-modulation/dilation invariance: for G(g,Λ)\mathbf{G}(g,\Lambda)5, the unitary G(g,Λ)\mathbf{G}(g,\Lambda)6 maps G(g,Λ)\mathbf{G}(g,\Lambda)7 to G(g,Λ)\mathbf{G}(g,\Lambda)8 while preserving compact support. If G(g,Λ)\mathbf{G}(g,\Lambda)9 and D(Λ)=1D(\Lambda)=10 is not discrete, the generator matrix factors as a lower triangular matrix times the shear matrix defining D(Λ)=1D(\Lambda)=11, reducing to the irrational case. Conversely, if D(Λ)=1D(\Lambda)=12 is discrete, a unimodular change of basis brings D(Λ)=1D(\Lambda)=13 into lower triangular form D(Λ)=1D(\Lambda)=14 with D(Λ)=1D(\Lambda)=15, and the chirp invariance reduces the problem to the integer lattice, where the classical characterization due to Liu applies: D(Λ)=1D(\Lambda)=16 is an ONB if and only if D(Λ)=1D(\Lambda)=17 for a bounded measurable set tiling D(Λ)=1D(\Lambda)=18 by integer translates. Pulling back through D(Λ)=1D(\Lambda)=19 yields the stated window characterization.

Non-product Gabor bases and the Iosevich–Mayeli question

Iosevich and Mayeli asked whether there exist π1(Λ)\pi_1(\Lambda)0 and π1(Λ)\pi_1(\Lambda)1 such that π1(Λ)\pi_1(\Lambda)2 is an ONB while π1(Λ)\pi_1(\Lambda)3 fails to be an ONB for every choice of sets π1(Λ)\pi_1(\Lambda)4. The preceding classification shows that compactly supported windows cannot furnish such an example in the lattice setting: whenever π1(Λ)\pi_1(\Lambda)5 is an ONB with π1(Λ)\pi_1(\Lambda)6 compactly supported, the same π1(Λ)\pi_1(\Lambda)7 works along the product set π1(Λ)\pi_1(\Lambda)8.

The paper nevertheless answers the question affirmatively using fractional Fourier transforms. Let π1(Λ)\pi_1(\Lambda)9 and aZa\mathbb{Z}0 with aZa\mathbb{Z}1. Since the fractional Fourier transform diagonalizes on the Hermite basis and implements rotation of the time-frequency plane, aZa\mathbb{Z}2 is an ONB. Suppose aZa\mathbb{Z}3 were also an ONB for some aZa\mathbb{Z}4. Rotating back via Lemma (fractional invariance), aZa\mathbb{Z}5 would be an ONB, so by the Gabardo–Lai–Wang structure theory, aZa\mathbb{Z}6 must tile aZa\mathbb{Z}7, forcing aZa\mathbb{Z}8 to equal one of two explicit "staircase" sets of upper Beurling density aZa\mathbb{Z}9. But the tiling structure forces gL2(R)g \in L^2(\mathbb{R})00 and gL2(R)g \in L^2(\mathbb{R})01 each to lie inside arithmetic progressions with spacings gL2(R)g \in L^2(\mathbb{R})02 and gL2(R)g \in L^2(\mathbb{R})03 respectively, giving

gL2(R)g \in L^2(\mathbb{R})04

contradicting the required density gL2(R)g \in L^2(\mathbb{R})05. Hence no product realization exists. Note that gL2(R)g \in L^2(\mathbb{R})06 necessarily has unbounded support when gL2(R)g \in L^2(\mathbb{R})07, as follows from the integral representation of gL2(R)g \in L^2(\mathbb{R})08; this is consistent with, and forced by, the compact-support classification above.

Limitations and open questions

The characterization is specific to the lattice setting in gL2(R)g \in L^2(\mathbb{R})09; extensions to higher dimensions, to non-lattice countable index sets, or to frames rather than orthonormal bases are not addressed. The window characterization permits arbitrary measurable tiling sets gL2(R)g \in L^2(\mathbb{R})10, so it does not classify regular (e.g., interval-based or continuous) windows within the admissible class. The construction answering the Iosevich–Mayeli question relies essentially on unbounded support, and the paper leaves open whether non-product examples can exist with windows of controlled decay. Finally, the rigidity lemma on compactly supported Fourier transforms of unimodular functions is proved only in one dimension, and its applicability in several variables is not discussed.

Conclusion

The paper delivers a complete solution to the Fuglede–Gabor problem for compactly supported windows over lattices in gL2(R)g \in L^2(\mathbb{R})11: existence holds exactly for unit-density lattices with discrete first projection, and the admissible windows are precisely scaled indicators of measurable translational tiling sets. The proof of the Han–Wang conjecture introduces a weighted Zak transform combined with a distributional Paley–Wiener and Hadamard factorization argument, yielding a rigidity principle for unimodular functions with compactly supported spectra that may prove useful elsewhere. The affirmative answer to the Iosevich–Mayeli question via rotated integer lattices demonstrates that product-set realizations fail in general, but only outside the compactly supported class.

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