Reconstruction algorithms for a class of restricted ray transforms without added singularities

preprint2016arXivOpen access

Abstract

Let XX and X∗X^* denote a restricted ray transform along curves and a corresponding backprojection operator, respectively. Theoretical analysis of reconstruction from the data XfXf is usually based on a study of the composition X∗DXX^* D X, where DD is some local operator (usually a derivative). If X∗X^* is chosen appropriately, then X∗DXX^* D X is a Fourier Integral Operator (FIO) with singular symbol. The singularity of the symbol leads to the appearance of artifacts (added singularities) that can be as strong as the original (or, useful) singularities. By choosing DD in a special way one can reduce the strength of added singularities, but it is impossible to get rid of them completely. In the paper we follow a similar approach, but make two changes. First, we replace DD with a nonlocal operator D~\tilde D that integrates XfXf along a curve in the data space. The result D~Xf\tilde D Xf resembles the generalized Radon transform RR of ff. The function D~Xf\tilde D Xf is defined on pairs (x0,Θ)∈U×S2(x_0,Θ)\in U\times S^2, where U⊂R3U\subset\mathbb R^3 is an open set containing the support of ff, and S2S^2 is the unit sphere in R3\mathbb R^3. Second, we replace X∗X^* with a backprojection operator R∗R^* that integrates with respect to ΘΘ over S2S^2. It turns out that if D~\tilde D and R∗R^* are appropriately selected, then the composition R∗D~XR^* \tilde D X is an elliptic pseudodifferential operator of order zero with principal symbol 1. Thus, we obtain an approximate reconstruction formula that recovers all the singularities correctly and does not produce artifacts. The advantage of our approach is that by inserting D~\tilde D we get access to the frequency variable ΘΘ. In particular, we can incorporate suitable cut-offs in R∗R^* to eliminate bad directions ΘΘ, which lead to added singularities.

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