Abstract

We develop a primal-dual algorithm that allows for one-step inversion of spectral CT transmission photon counts data to a basis map decomposition. The algorithm allows for image constraints to be enforced on the basis maps during the inversion. The derivation of the algorithm makes use of a local upper bounding quadratic approximation to generate descent steps for non-convex spectral CT data discrepancy terms, combined with a new convex-concave optimization algorithm. Convergence of the algorithm is demonstrated on simulated spectral CT data. Simulations with noise and anthropomorphic phantoms show examples of how to employ the constrained one-step algorithm for spectral CT data.

Highlights

  • The recent research activity in photon-counting detectors has motivated a resurgence in the investigation of spectral computed tomography (CT)

  • We demonstrate the algorithm with the use of total variation (TV) constraints, but the framework allows for other constraints such as non-negativity, upper bounds, and sum bounds applied to either the basis maps or to a composite image such as an estimated mono-chromatic attenuation map

  • We have developed a constrained minimization algorithm for inverting spectral CT transmission data directly to basis material maps

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Summary

Introduction

The recent research activity in photon-counting detectors has motivated a resurgence in the investigation of spectral computed tomography (CT). Photon-counting detectors detect individual x-ray quanta and the electronic pulse signal generated by these quanta has a peak amplitude proportional to the photon energy (Taguchi and Iwanczyk 2013). Thresholding these amplitudes allows for coarse energy resolution of the x-ray photons, and the transmitted flux of x-ray photons can be measured simultaneously in a number of energy windows. For photon-counting detectors where the number of energy windows can be three or greater, the new advantage with respect to quantitative imaging is the ability to image contrast agents that possess a K-edge in the diagnostic x-ray energy range (Roessl and Proksa 2007, Schlomka et al 2008, Cormode et al 2010, Roessl et al 2011a, 2011b, Schirra et al 2013)

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