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Experimental study of photon-counting CT neural network material decomposition under conditions of pulse pileup

Purpose: We investigated the performance of a neural network (NN) material decomposition method under varying pileup conditions. Approach: Experiments were performed at tube current settings that provided count rates incident on the detector through air equal to 9%, 14%, 27%, 40%, and 54% of the max...

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Autores principales: Jenkins, Parker J. B., Schmidt, Taly Gilat
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Society of Photo-Optical Instrumentation Engineers 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7797008/
https://www.ncbi.nlm.nih.gov/pubmed/33447645
http://dx.doi.org/10.1117/1.JMI.8.1.013502
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author Jenkins, Parker J. B.
Schmidt, Taly Gilat
author_facet Jenkins, Parker J. B.
Schmidt, Taly Gilat
author_sort Jenkins, Parker J. B.
collection PubMed
description Purpose: We investigated the performance of a neural network (NN) material decomposition method under varying pileup conditions. Approach: Experiments were performed at tube current settings that provided count rates incident on the detector through air equal to 9%, 14%, 27%, 40%, and 54% of the maximum detector count rate. An NN was trained for each count-rate level using transmission measurements through known thicknesses of basis materials (PMMA and aluminum). The NN trained for each count-rate level was applied to x-ray transmission measurements through test materials and to CT data of a rod phantom. Material decomposition error was evaluated as the distance in basis material space between the estimated thicknesses and ground truth. Results: There was no clear trend between count-rate level and material decomposition error for all test materials except neoprene. As an example result, Teflon error was 0.33 cm at the 9% count-rate level and 0.12 cm at the 54% count-rate level for the x-ray transmission experiments. Decomposition error increased with count-rate level for the neoprene test case, with 0.65-cm error at 9% count-rate level and 1.14-cm error at the 54% count-rate level. In the CT study, material decomposition error decreased with increasing incident count rate. For example, the material decomposition error for Teflon was 0.089, 0.066, 0.054 at count-rate levels of 14%, 27%, and 40%, respectively. Conclusions: Results demonstrate over a range of incident count-rate levels that an NN trained at a specific count-rate level can learn the relationship between photon-counting spectral measurements and basis material thicknesses.
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spelling pubmed-77970082022-01-09 Experimental study of photon-counting CT neural network material decomposition under conditions of pulse pileup Jenkins, Parker J. B. Schmidt, Taly Gilat J Med Imaging (Bellingham) Physics of Medical Imaging Purpose: We investigated the performance of a neural network (NN) material decomposition method under varying pileup conditions. Approach: Experiments were performed at tube current settings that provided count rates incident on the detector through air equal to 9%, 14%, 27%, 40%, and 54% of the maximum detector count rate. An NN was trained for each count-rate level using transmission measurements through known thicknesses of basis materials (PMMA and aluminum). The NN trained for each count-rate level was applied to x-ray transmission measurements through test materials and to CT data of a rod phantom. Material decomposition error was evaluated as the distance in basis material space between the estimated thicknesses and ground truth. Results: There was no clear trend between count-rate level and material decomposition error for all test materials except neoprene. As an example result, Teflon error was 0.33 cm at the 9% count-rate level and 0.12 cm at the 54% count-rate level for the x-ray transmission experiments. Decomposition error increased with count-rate level for the neoprene test case, with 0.65-cm error at 9% count-rate level and 1.14-cm error at the 54% count-rate level. In the CT study, material decomposition error decreased with increasing incident count rate. For example, the material decomposition error for Teflon was 0.089, 0.066, 0.054 at count-rate levels of 14%, 27%, and 40%, respectively. Conclusions: Results demonstrate over a range of incident count-rate levels that an NN trained at a specific count-rate level can learn the relationship between photon-counting spectral measurements and basis material thicknesses. Society of Photo-Optical Instrumentation Engineers 2021-01-09 2021-01 /pmc/articles/PMC7797008/ /pubmed/33447645 http://dx.doi.org/10.1117/1.JMI.8.1.013502 Text en © 2021 The Authors https://creativecommons.org/licenses/by/4.0/ Published by SPIE under a Creative Commons Attribution 4.0 Unported License. Distribution or reproduction of this work in whole or in part requires full attribution of the original publication, including its DOI.
spellingShingle Physics of Medical Imaging
Jenkins, Parker J. B.
Schmidt, Taly Gilat
Experimental study of photon-counting CT neural network material decomposition under conditions of pulse pileup
title Experimental study of photon-counting CT neural network material decomposition under conditions of pulse pileup
title_full Experimental study of photon-counting CT neural network material decomposition under conditions of pulse pileup
title_fullStr Experimental study of photon-counting CT neural network material decomposition under conditions of pulse pileup
title_full_unstemmed Experimental study of photon-counting CT neural network material decomposition under conditions of pulse pileup
title_short Experimental study of photon-counting CT neural network material decomposition under conditions of pulse pileup
title_sort experimental study of photon-counting ct neural network material decomposition under conditions of pulse pileup
topic Physics of Medical Imaging
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7797008/
https://www.ncbi.nlm.nih.gov/pubmed/33447645
http://dx.doi.org/10.1117/1.JMI.8.1.013502
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