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Articles

A new projection-based iterative image reconstruction algorithm for dual-energy computed tomography

, ORCID Icon & ORCID Icon
Pages 1030-1047 | Received 15 Mar 2015, Accepted 26 Sep 2015, Published online: 28 Oct 2015

Figures & data

Figure 1. A validation test for reconstructing the coefficients ac and ap: The first and second rows are the reconstruction results of ac and ap for the Compton scatter and the photoelectric case, respectively. The first column refers the reference values of ac and ap. The second and third columns are the results reconstructed from sinogram without and with noise, respectively.

Figure 1. A validation test for reconstructing the coefficients ac and ap: The first and second rows are the reconstruction results of ac and ap for the Compton scatter and the photoelectric case, respectively. The first column refers the reference values of ac and ap. The second and third columns are the results reconstructed from sinogram without and with noise, respectively.

Figure 2. Relative L2-error of the results reconstructed from An and An+1 with respect to the number of iteration: blue and red lines are the errors in a logarithmic scale for the Compton scatter and the photoelectric cases, respectively.

Figure 2. Relative L2-error of the results reconstructed from An and An+1 with respect to the number of iteration: blue and red lines are the errors in a logarithmic scale for the Compton scatter and the photoelectric cases, respectively.

Figure 3. A synthetic human abdomen model for experiments: (a) The reference image of the human abdomen anatomy. (b) The log–log plot of the attenuation coefficients for the five materials of fat, muscle, blood, soft tissue and bone.

Figure 3. A synthetic human abdomen model for experiments: (a) The reference image of the human abdomen anatomy. (b) The log–log plot of the attenuation coefficients for the five materials of fat, muscle, blood, soft tissue and bone.

Figure 4. Dual-energy spectra and the corresponding sinograms: (Top) two different energy spectra for 80 kVp and 140 kVp, denoted by S80 ()and S140 (). (Bottom Left) The simulated sinogram for the low-energy spectrum S80. (Bottom Right) The simulated sinogram for the high-energy spectrum S140.

Figure 4. Dual-energy spectra and the corresponding sinograms: (Top) two different energy spectra for 80 kVp and 140 kVp, denoted by S80 (∙)and S140 (∘). (Bottom Left) The simulated sinogram for the low-energy spectrum S80. (Bottom Right) The simulated sinogram for the high-energy spectrum S140.

Figure 5. Compton and photoelectric images: the first row is the reconstruction results for the Compton scatter case and the second row is the reconstruction results for the photoelectric case. (a) and (d) are reconstructed by the proposed iterative method. (b) and (e) are the first-order method. (c) and (f) are the second-order methods.

Figure 5. Compton and photoelectric images: the first row is the reconstruction results for the Compton scatter case and the second row is the reconstruction results for the photoelectric case. (a) and (d) are reconstructed by the proposed iterative method. (b) and (e) are the first-order method. (c) and (f) are the second-order methods.

Figure 6. Performance comparison of three algorithms at photon energy 40 keV; (a) is the reference image of μ(r,40). (b-1), (c-1) and (d-1) are reconstructed images by the iterative method, the first-order method and the second-order method, respectively. (b-2), (c-2) and (d-2) are difference images of (b-1), (c-1) and (d-1) from (a), respectively.

Figure 6. Performance comparison of three algorithms at photon energy 40 keV; (a) is the reference image of μ(r,40). (b-1), (c-1) and (d-1) are reconstructed images by the iterative method, the first-order method and the second-order method, respectively. (b-2), (c-2) and (d-2) are difference images of (b-1), (c-1) and (d-1) from (a), respectively.

Figure 7. Performance comparison of three algorithms at photon energy 80 keV; (a) is the reference image of μ(r,80). (b-1), (c-1) and (d-1) are reconstructed images by the iterative method, the first-order method and the second-order method, respectively. (b-2), (c-2) and (d-2) are difference images of (b-1), (c-1) and (d-1) from (a), respectively.

Figure 7. Performance comparison of three algorithms at photon energy 80 keV; (a) is the reference image of μ(r,80). (b-1), (c-1) and (d-1) are reconstructed images by the iterative method, the first-order method and the second-order method, respectively. (b-2), (c-2) and (d-2) are difference images of (b-1), (c-1) and (d-1) from (a), respectively.

Table 1. Comparison of relative errors for reconstruction results by the first-order, the second-order and the iterative methods. The values are represented in %.

Table 2. Computational time of the proposed algorithm under the parallelization.

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