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On the structure of the Gram matrix for Gabor systems generated by B-splines

Martin Buck, Christina Frederick, Kasso Okoudjou, Alexander Stangl

Abstract

We consider the Gabor system $\mathcal{G}(g,a\mathbb{Z}\times b\mathbb{Z})$ generated by a continuous, compactly supported function $g$ over the time-frequency lattice generated by the parameters $a$ and $b$. We show that, under an appropriate ordering of the Gabor elements, certain submatrices of the Gram matrix of $\mathcal{G}(g,a\mathbb{Z}\times b\mathbb{Z})$ exhibit a block-Toeplitz structure. This structural property enables us to derive spectral results for finite sub-blocks of the Gram matrix by appealing to the spectral theory of Toeplitz matrices. In particular, we apply our results to the Gram matrix of Gabor systems generated by the $N$th-order B-spline.

On the structure of the Gram matrix for Gabor systems generated by B-splines

Abstract

We consider the Gabor system generated by a continuous, compactly supported function over the time-frequency lattice generated by the parameters and . We show that, under an appropriate ordering of the Gabor elements, certain submatrices of the Gram matrix of exhibit a block-Toeplitz structure. This structural property enables us to derive spectral results for finite sub-blocks of the Gram matrix by appealing to the spectral theory of Toeplitz matrices. In particular, we apply our results to the Gram matrix of Gabor systems generated by the th-order B-spline.
Paper Structure (14 sections, 17 theorems, 78 equations, 5 figures)

This paper contains 14 sections, 17 theorems, 78 equations, 5 figures.

Key Result

Lemma 3.1

Let $s, t \in \mathbb{R}$ and define the shifted set: and the corresponding Gabor atoms Then, for any $(j,k), (j',k') \in \Lambda_n$, the new Gram matrix $\tilde{G}_n$ has entries The shifting factor $s$$(s=1/ab)$ can be chosen so that $\tilde{G}_n=G_n$ is unchanged. Furthermore, the spectra of $G_n$ and $\tilde{G}_n$ are identical.

Figures (5)

  • Figure 1: Top: The magnitude and phase of the finite Gram matrix $G_{15} \in \mathbb{C}^{115 \times 115}$ with blocks $G_{15}^{[\ell]} \in \mathbb{C}^{15 \times 15}$ Bottom: The magnitude of the matrix $T_{15}$ with Toeplitz blocks $T^{[\ell]}_{15}$ and the phase of the matrix $H_{15}$ with Hankel blocks $H_{15}^{[\ell]}$ in the decomposition \ref{['eqn:gram:toeplitz-dot-hankel']} for $a=.25, b=1.5, n=15$.
  • Figure 2: The Laurent polynomials $t^{[\ell]}(x) \in W$ associated to the Toeplitz blocks $T_{\infty}^{[\ell]} \in \mathcal{B}(l^p(\mathbb{Z}))$, $\ell=0, \hdots, 4$. The spectrum of $T_{\infty}^{[\ell]}$ is the interval $[\min t^{[\ell]}(x), \max t^{[\ell]}(x)]$. Here, $a=.3, .4, .5$ and the shades of blue correspond to different values of $b\in [1.5, 1.98]$.
  • Figure 3: Width of spectrum of $t^{[\ell]}(x)$ for $a=.23$, $b=1.7$ corresponding to the $N$th order B-spline. The dashed lines show the corresponding $N$th order decay proved in Lemma \ref{['lem:decay']}.
  • Figure 4: Plots of $\lambda_1(G_n)$ (top left), $\min t^{[0]}(x)$ (top right), $\lambda_n(G_n)$ (bottom left), and $\max t^{[0]}(x)$ (bottom right) for $n=15$ demonstrate the results of Corollary \ref{['corr: eigs']}.
  • Figure 5: Lemma \ref{['lem:circeigconv']} gives the convergence of eigenvalues of the Toeplitz block $T_n^{[\ell]}$ to those of the circulant matrix $C_n^{[\ell]}$. Here, $T_n^{[\ell]}$ correspond to the subblocks $G_n^{[\ell]}$ of the Gram matrices $G_n$ for $\mathcal{G}(s_2,\Lambda_n)$.

Theorems & Definitions (26)

  • Lemma 3.1
  • proof
  • Lemma 3.2
  • proof
  • Theorem 3.3
  • proof
  • Corollary 3.3.1
  • proof
  • Corollary 3.3.2
  • Proposition 3.4
  • ...and 16 more