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Superiorization-based multi-energy CT image reconstruction. (English) Zbl 1367.65033

In multi-energy computer-tomography (CT) image reconstruction one has to find the image \(X\) by minimizing the objective function \(\phi(X)=\|X\|_*+\lambda r(X)\), subject to \(AX=G\) where \(r\) is a total variation (TV) term for smoothing purpose and the norm is the nuclear norm. The prior rank intensity and sparsity model (PRISM) essentially assumes that \(X\) is a superposition of a low rank and a sparse matrix. The simultaneous algebraic reconstruction technique (SART) is an iterative method to solve \(AX=G\) using a relaxation parameter to control the step size. In a superiorizated version of an iterative algorithm, the usual iterations are perturbed to get better performance. Inspired by Y. Censor et al. [J. Optim. Theory Appl. 160, No. 3, 730–747 (2014; Zbl 1298.90104)], this paper proposes a superiorized version of the SART subject to the PRISM prior. The superiorization consists in modifying the iteration by adding an appropriate matrix to the SART iterate \(X^{(k)}\) to force a descend of the objective function \(\phi\). The method is compared numerically with the split-Bregman algorithm (see [T. Goldstein and S. Osher, SIAM J. Imaging Sci. 2, No. 2, 323–343 (2009; Zbl 1177.65088)]).

MSC:

65D18 Numerical aspects of computer graphics, image analysis, and computational geometry
68U10 Computing methodologies for image processing
94A08 Image processing (compression, reconstruction, etc.) in information and communication theory

References:

[1] Allmendinger T 2014 X-ray CT scanning and dual-source CT system United States Patent Application US 14/183,579
[2] Andersen A H and Kak A C 1984 Simultaneous algebraic reconstruction technique (SART): a superior implementation of the ART algorithm Ultrason. Imaging6 81–94
[3] Avron H, Kale S, Kasiviswanathan S and Sindhwani V 2012 Efficient and practical stochastic subgradient descent for nuclear norm regularization (arXiv: 1206.6384)
[4] Beister M, Kolditz D and Kalender W A 2012 Iterative reconstruction methods in X-ray CT Phys. Med.28 94–108
[5] Bouman C A and Sauer K 1996 A unified approach to statistical tomography using coordinate descent optimization IEEE Trans. Image Process.5 480–92
[6] Butnariu D, Davidi R, Herman G T and Kazantsev I G 2007 Stable convergence behavior under summable perturbations of a class of projection methods for convex feasibility and optimization problems IEEE. Sel. Top. Signal Process.1 540–7
[7] Censor Y, Davidi R and Herman G T 2010 Perturbation resilience and superiorization of iterative algorithms Inverse Problems26 065008 · Zbl 1193.65019
[8] Censor Y, Davidi R, Herman G T, Schulte R W and Tetruashvili L 2014 Projected subgradient minimization versus superiorization J. Optim. Theory Appl.160 730–47 · Zbl 1298.90104
[9] Chambolle A and Pock T 2011 A first-order primal-dual algorithm for convex problems with applications to imaging J. Math. Imaging Vis.40 120–45 · Zbl 1255.68217
[10] Chu J, Cong W, Li L and Wang G 2013 Combination of current-integrating/photon-counting detector modules for spectral CT Phys. Med. Biol.58 7009
[11] Davidi R, Herman G and Censor Y 2009 Perturbation-resilient block-iterative projection methods with application to image reconstruction from projections Int. Trans. Oper. Res.16 505–24 · Zbl 1191.94013
[12] Elbakri I A and Fessler J A 2002 Statistical image reconstruction for polyenergetic x-ray computed tomography IEEE Trans. Med. Imaging21 89–99
[13] Feuerlein S, Roessl E, Proksa R, Martens G, Klass O, Jeltsch M, Rasche V, Brambs H-J, Hoffmann M H and Schlomka J-P 2008 Multienergy photon-counting K-edge imaging: potential for improved luminal depiction in vascular imaging 1 Radiology249 1010–6
[14] Fornaro J, Leschka S, Hibbeln D, Butler A, Anderson N, Pache G, Scheffel H, Wildermuth S, Alkadhi H and Stolzmann P 2011 Dual-and multi-energy CT: approach to functional imaging Insights Imaging2 149–59
[15] Garduno E and Herman G T 2014 Superiorization of the ML-EM algorithm IEEE Trans. Nucl. Sci.61 162–72
[16] Gao H, Yu H, Osher S and Wang G 2011 Multi-energy CT based on a prior rank, intensity and sparsity model (PRISM) Inverse problems27 115012 · Zbl 1230.92024
[17] Goldstein T and Osher S 2009 The split Bregman method for L1-regularized problems SIAM J. Imaging Sci.2 323–43 · Zbl 1177.65088
[18] Goldstein T, O’Donoghue B, Setzer S and Baraniuk R 2014 Fast alternating direction optimization methods SIAM J. Imaging Sci.7 1588–623
[19] Gordon R, Bender R and Herman G 1970 Algebraic reconstruction techniques (ART) for three-dimensional electron microscopy and x-ray photography J. Theor. Biol.29 471–81
[20] Heismann B J, Schmidt B T and Flohr T 2012 Spectral Computed Tomography (Bellingham, WA: SPIE)
[21] Herman G T, Garduño E, Davidi R and Censor Y 2012 Superiorization: an optimization heuristic for medical physics Med. Phys.39 5532–46
[22] Holt K M 2014 Total nuclear variation and jacobian extensions of total variation for vector fields IEEE Trans. Image Process.23 3975–89 · Zbl 1374.94140
[23] Jia X, Lou Y, Li R, Song W Y and Jiang S B 2010 GPU-based fast cone beam CT reconstruction from undersampled and noisy projection data via total variation Med. Phys.37 1757–60
[24] Jiang M and Wang G 2003 Convergence studies on iterative algorithms for image reconstruction IEEE Trans. Med. Imaging22 569–79
[25] Lefkimmiatis S, Roussos A, Unser M and Maragos P 2013 Convex generalizations of total variation based on the structure tensor with applications to inverse problems Int. Conf. on Scale Space and Variational Methods in Computer Vision pp 48–60
[26] Langan D A, Tkaczyk J E, LeBlanc J W, Wilson C R, Wu X, Xu D, Benson T M and Pack J D 2010 System and method of fast kVp switching for dual energy CT US Patent 12/558,248
[27] Luo S and Zhou T 2014 Superiorization of EM algorithm and its application in single-photon emission computed tomography (SPECT) Inverse Problems Imaging8 223–46 · Zbl 1301.92043
[28] Pan D, Schirra C O, Senpan A, Schmieder A H, Stacy A J, Roessl E, Thran A, Wickline S A, Proska R and Lanza G M 2012 An early investigation of ytterbium nanocolloids for selective and quantitative ’multicolor’ spectral CT imaging ACS Nano6 3364–70
[29] Rigie D S and La Rivière P J 2015 Joint reconstruction of multi-channel, spectral CT data via constrained total nuclear variation minimization Phys. Med. Biol.60 1741
[30] Sawatzky A, Xu Q, Schirra C O and Anastasio M A 2014 Proximal ADMM for multi-channel image reconstruction in spectral x-ray CT IEEE Trans. Med. Imaging33 1657–68
[31] Shikhaliev P M 2008 Computed tomography with energy-resolved detection: a feasibility study Phys. Med. Biol.53 1475
[32] Sidky E Y, Kao C M and Pan X 2006 Accurate image reconstruction from few-views and limited-angle data in divergent-beam CT J. X-ray Sci. Technol.14 119–39
[33] Tian Z, Jia X, Yuan K, Pan T and Jiang S B 2011 Low-dose CT reconstruction via edge-preserving total variation regularization Phys. Med. Biol.56 5949
[34] Walsh M F, Opie A M T, Ronaldson J P, Doesburg R M N, Nik S J, Mohr J L, Ballabriga R, Butler A P H and Butler P H 2011 First CT using Medipix3 and the MARS-CT-3 spectral scanner J. Instrum.6 C01095
[35] Wang X, Meier D, Mikkelsen S, Maehlum G E, Wagenaar D J, Tsui B M W, Patt B E and Frey E C 2011 MicroCT with energy-resolved photon-counting detectors Phys. Med. Biol.56 2791–816
[36] Yu H and Wang G 2009 Compressed sensing based interior tomography Phys. Med. Biol.54 2791
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