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A multienergy computed tomography method without image segmentation or prior knowledge of X-ray spectra or materials
Many methods have been proposed for multienergy computed tomography (CT) imaging based on traditional CT systems. Usually, either prior knowledge of the X-ray spectra distribution or materials or the segmentation of the projection or reconstructed image is needed. To avoid these requirements, a mult...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Elsevier
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9674550/ https://www.ncbi.nlm.nih.gov/pubmed/36411882 http://dx.doi.org/10.1016/j.heliyon.2022.e11584 |
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author | Wei, Jiaotong Chen, Ping Liu, Bin Han, Yan |
author_facet | Wei, Jiaotong Chen, Ping Liu, Bin Han, Yan |
author_sort | Wei, Jiaotong |
collection | PubMed |
description | Many methods have been proposed for multienergy computed tomography (CT) imaging based on traditional CT systems. Usually, either prior knowledge of the X-ray spectra distribution or materials or the segmentation of the projection or reconstructed image is needed. To avoid these requirements, a multienergy CT method is proposed in this paper. A CT image can be seen as a linear combination of energy-dependent components and spatially dependent components. The latter components are the base images, while the former components are the coefficients. A blind decomposition model is constructed to decompose the multivoltage projections to obtain the base images and the energies. Multienergy CT images are computationally synthesized with the base images and the energies. Multivoltage projections can be acquired based on one scan with stepped voltages. X-ray scattering is considered an important factor in imaging errors and appears as a low-frequency signal. The variance is used to describe the low-frequency features and is minimized as the optimized objective function of the decomposition model. The solution of the model uses Karush–Kuhn–Tucker (KKT) conditions. In the experiments, the images reconstructed with the proposed method exhibit weak beam-hardening artifacts. Additionally, the X-ray energies of the different materials represented have small relative errors. Therefore, the reconstructed images have narrow energy intervals. This shows the effectiveness of the proposed method. |
format | Online Article Text |
id | pubmed-9674550 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | Elsevier |
record_format | MEDLINE/PubMed |
spelling | pubmed-96745502022-11-20 A multienergy computed tomography method without image segmentation or prior knowledge of X-ray spectra or materials Wei, Jiaotong Chen, Ping Liu, Bin Han, Yan Heliyon Research Article Many methods have been proposed for multienergy computed tomography (CT) imaging based on traditional CT systems. Usually, either prior knowledge of the X-ray spectra distribution or materials or the segmentation of the projection or reconstructed image is needed. To avoid these requirements, a multienergy CT method is proposed in this paper. A CT image can be seen as a linear combination of energy-dependent components and spatially dependent components. The latter components are the base images, while the former components are the coefficients. A blind decomposition model is constructed to decompose the multivoltage projections to obtain the base images and the energies. Multienergy CT images are computationally synthesized with the base images and the energies. Multivoltage projections can be acquired based on one scan with stepped voltages. X-ray scattering is considered an important factor in imaging errors and appears as a low-frequency signal. The variance is used to describe the low-frequency features and is minimized as the optimized objective function of the decomposition model. The solution of the model uses Karush–Kuhn–Tucker (KKT) conditions. In the experiments, the images reconstructed with the proposed method exhibit weak beam-hardening artifacts. Additionally, the X-ray energies of the different materials represented have small relative errors. Therefore, the reconstructed images have narrow energy intervals. This shows the effectiveness of the proposed method. Elsevier 2022-11-15 /pmc/articles/PMC9674550/ /pubmed/36411882 http://dx.doi.org/10.1016/j.heliyon.2022.e11584 Text en © 2022 The Authors. Published by Elsevier Ltd. https://creativecommons.org/licenses/by/4.0/This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Research Article Wei, Jiaotong Chen, Ping Liu, Bin Han, Yan A multienergy computed tomography method without image segmentation or prior knowledge of X-ray spectra or materials |
title | A multienergy computed tomography method without image segmentation or prior knowledge of X-ray spectra or materials |
title_full | A multienergy computed tomography method without image segmentation or prior knowledge of X-ray spectra or materials |
title_fullStr | A multienergy computed tomography method without image segmentation or prior knowledge of X-ray spectra or materials |
title_full_unstemmed | A multienergy computed tomography method without image segmentation or prior knowledge of X-ray spectra or materials |
title_short | A multienergy computed tomography method without image segmentation or prior knowledge of X-ray spectra or materials |
title_sort | multienergy computed tomography method without image segmentation or prior knowledge of x-ray spectra or materials |
topic | Research Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9674550/ https://www.ncbi.nlm.nih.gov/pubmed/36411882 http://dx.doi.org/10.1016/j.heliyon.2022.e11584 |
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