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Resolution analysis of inverting the generalized NN-dimensional Radon transform in Rn\mathbb R^n from discrete data

Published 17 Feb 2021 in math.NA and cs.NA | (2102.09035v1)

Abstract: Let R\mathcal R denote the generalized Radon transform (GRT), which integrates over a family of NN-dimensional smooth submanifolds Sy~⊂U\mathcal S_{\tilde y}\subset\mathcal U, 1≤N≤n−11\le N\le n-1, where an open set U⊂R<sup>n\mathcal U\subset\mathbb R<sup>n is the image domain. The submanifolds are parametrized by points y~⊂V~\tilde y\subset\tilde{\mathcal V}, where an open set V~⊂R<sup>n\tilde{\mathcal V}\subset\mathbb R<sup>n is the data domain. The continuous data are g=Rfg={\mathcal R} f, and the reconstruction is fˇ=R<sup>∗</sup>Bg\check f=\mathcal R<sup>*\mathcal</sup> B g. Here R<sup>∗\mathcal R<sup>* is a weighted adjoint of R\mathcal R, and B\mathcal B is a pseudo-differential operator. We assume that ff is a conormal distribution, supp(f)⊂U\text{supp}(f)\subset\mathcal U, and its singular support is a smooth hypersurface S⊂U\mathcal S\subset\mathcal U. Discrete data consists of the values of gg on a lattice y~<sup>j\tilde y<sup>j with the step size O(ϵ)O(\epsilon). Let fˇϵ=R<sup>∗</sup>Bgϵ\check f_\epsilon=\mathcal R<sup>*\mathcal</sup> B g_\epsilon denote the reconstruction obtained by applying the inversion formula to an interpolated discrete data gϵ(y~)g_\epsilon(\tilde y). Pick a generic pair (x0,y~0)(x_0,\tilde y_0), where x0∈Sx_0\in\mathcal S, and Sy~0\mathcal S_{\tilde y_0} is tangent to S\mathcal S at x0x_0. The main result of the paper is the computation of the limit f0(xˇ):=lim⁡ϵ→0ϵ<sup>κ</sup>fˇϵ(x0+ϵxˇ). f_0(\check x):=\lim_{\epsilon\to0}\epsilon<sup>\kappa</sup> \check f_\epsilon(x_0+\epsilon\check x). Here κ≥0\kappa\ge 0 is selected based on the strength of the reconstructed singularity, and xˇ\check x is confined to a bounded set. The limiting function f0(xˇ)f_0(\check x), which we call the discrete transition behavior, allows computing the resolution of reconstruction.

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