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

preprint2021arXivOpen access

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⊂Rn\mathcal U\subset\mathbb R^n is the image domain. The submanifolds are parametrized by points y~⊂V~\tilde y\subset\tilde{\mathcal V}, where an open set V~⊂Rn\tilde{\mathcal V}\subset\mathbb R^n is the data domain. The continuous data are g=Rfg={\mathcal R} f, and the reconstruction is fˇ=R∗Bg\check f=\mathcal R^*\mathcal B g. Here R∗\mathcal R^* 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~j\tilde y^j with the step size O(ε)O(ε). Let fˇε=R∗Bgε\check f_ε=\mathcal R^*\mathcal B g_ε denote the reconstruction obtained by applying the inversion formula to an interpolated discrete data gε(y~)g_ε(\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→0εκfˇε(x0+εxˇ). f_0(\check x):=\lim_{ε\to0}ε^κ\check f_ε(x_0+ε\check x). Here κ≥0κ\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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