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Super-resolution of positive near-colliding point sources

Published 1 Dec 2022 in eess.IV and eess.SP | (2212.00536v1)

Abstract: In this paper, we analyze the capacity of super-resolution of one-dimensional positive sources. In particular, we consider the same setting as in [arXiv:1904.09186v2 [math.NA]] and generalize the results there to the case of super-resolving positive sources. To be more specific, we consider resolving dd positive point sources with p⩽dp \leqslant d nodes closely spaced and forming a cluster, while the rest of the nodes are well separated. Similarly to [arXiv:1904.09186v2 [math.NA]], our results show that when the noise level ϵ≲SRF<sup>−2</sup>p+1\epsilon \lesssim \mathrm{SRF}<sup>{-2</sup> p+1}, where SRF=(ΩΔ)<sup>−1\mathrm{SRF}=(\Omega \Delta)<sup>{-1} with Ω\Omega being the cutoff frequency and Δ\Delta the minimal separation between the nodes, the minimax error rate for reconstructing the cluster nodes is of order 1ΩSRF<sup>2</sup>p−2ϵ\frac{1}{\Omega} \mathrm{SRF}<sup>{2</sup> p-2} \epsilon, while for recovering the corresponding amplitudes $\left{a_j\right}$ the rate is of order SRF<sup>2</sup>p−1ϵ\mathrm{SRF}<sup>{2</sup> p-1} \epsilon. For the non-cluster nodes, the corresponding minimax rates for the recovery of nodes and amplitudes are of order ϵΩ\frac{\epsilon}{\Omega} and ϵ\epsilon, respectively. Our numerical experiments show that the Matrix Pencil method achieves the above optimal bounds when resolving the positive sources.

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