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Quantifying pulmonary perfusion from noncontrast computed tomography

PURPOSE: Computed tomography (CT)‐derived ventilation methods compute respiratory induced volume changes as a surrogate for pulmonary ventilation. Currently, there are no known methods to derive perfusion information from noncontrast CT. We introduce a novel CT‐Perfusion (CT‐P) method for computing...

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Autores principales: Castillo, Edward, Nair, Girish, Turner‐Lawrence, Danielle, Myziuk, Nicholas, Emerson, Scott, Al‐Katib, Sayf, Westergaard, Sarah, Castillo, Richard, Vinogradskiy, Yevgeniy, Quinn, Thomas, Guerrero, Thomas, Stevens, Craig
Formato: Online Artículo Texto
Lenguaje:English
Publicado: John Wiley and Sons Inc. 2021
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8252085/
https://www.ncbi.nlm.nih.gov/pubmed/33608933
http://dx.doi.org/10.1002/mp.14792
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author Castillo, Edward
Nair, Girish
Turner‐Lawrence, Danielle
Myziuk, Nicholas
Emerson, Scott
Al‐Katib, Sayf
Westergaard, Sarah
Castillo, Richard
Vinogradskiy, Yevgeniy
Quinn, Thomas
Guerrero, Thomas
Stevens, Craig
author_facet Castillo, Edward
Nair, Girish
Turner‐Lawrence, Danielle
Myziuk, Nicholas
Emerson, Scott
Al‐Katib, Sayf
Westergaard, Sarah
Castillo, Richard
Vinogradskiy, Yevgeniy
Quinn, Thomas
Guerrero, Thomas
Stevens, Craig
author_sort Castillo, Edward
collection PubMed
description PURPOSE: Computed tomography (CT)‐derived ventilation methods compute respiratory induced volume changes as a surrogate for pulmonary ventilation. Currently, there are no known methods to derive perfusion information from noncontrast CT. We introduce a novel CT‐Perfusion (CT‐P) method for computing the magnitude mass changes apparent on dynamic noncontrast CT as a surrogate for pulmonary perfusion. METHODS: CT‐Perfusion is based on a mass conservation model which describes the unknown mass change as a linear combination of spatially corresponding inhale and exhale HU estimated voxel densities. CT‐P requires a deformable image registration (DIR) between the inhale/exhale lung CT pair, a preprocessing lung volume segmentation, and an estimate for the Jacobian of the DIR transformation. Given this information, the CT‐P image, which provides the magnitude mass change for each voxel within the lung volume, is formulated as the solution to a constrained linear least squares problem defined by a series of subregional mean magnitude mass change measurements. Similar to previous robust CT‐ventilation methods, the amount of uncertainty in a subregional sample mean measurement is related to measurement resolution and can be characterized with respect to a tolerance parameter [Formula: see text]. Spatial Spearman correlation between single photon emission CT perfusion (SPECT‐P) and the proposed CT‐P method was assessed in two patient cohorts via a parameter sweep of [Formula: see text]. The first cohort was comprised of 15 patients diagnosed with pulmonary embolism (PE) who had SPECT‐P and 4DCT imaging acquired within 24 h of PE diagnosis. The second cohort was comprised of 15 nonsmall cell lung cancer patients who had SPECT‐P and 4DCT images acquired prior to radiotherapy. For each test case, CT‐P images were computed for 30 different uncertainty parameter values, uniformly sampled from the range [0.01, 0.125], and the Spearman correlation between the SPECT‐P and the resulting CT‐P images were computed. RESULTS: The median correlations between CT‐P and SPECT‐P taken over all 30 test cases ranged between 0.49 and 0.57 across the parameter sweep. For the optimal tolerance τ = 0.0385, the CT‐P and SPECT‐P correlations across all 30 test cases ranged between 0.02 and 0.82. A one‐sample sign test was applied separately to the PE and lung cancer cohorts. A low Spearmen correlation of 15% was set as the null median value and two‐sided alternative was tested. The PE patients showed a median correlation of 0.57 (IQR = 0.305). One‐sample sign test was statistically significant with 96.5 % confidence interval: 0.20–0.63, P < 0.00001. Lung cancer patients had a median correlation of 0.57(IQR = 0.230). Again, a one‐sample sign test for median was statistically significant with 96.5 percent confidence interval: 0.45–0.71, P < 0.00001. CONCLUSION: CT‐Perfusion is the first mechanistic model designed to quantify magnitude blood mass changes on noncontrast dynamic CT as a surrogate for pulmonary perfusion. While the reported correlations with SPECT‐P are promising, further investigation is required to determine the optimal CT acquisition protocol and numerical method implementation for CT‐P imaging.
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spelling pubmed-82520852021-07-07 Quantifying pulmonary perfusion from noncontrast computed tomography Castillo, Edward Nair, Girish Turner‐Lawrence, Danielle Myziuk, Nicholas Emerson, Scott Al‐Katib, Sayf Westergaard, Sarah Castillo, Richard Vinogradskiy, Yevgeniy Quinn, Thomas Guerrero, Thomas Stevens, Craig Med Phys QUANTITATIVE IMAGING AND IMAGE PROCESSING PURPOSE: Computed tomography (CT)‐derived ventilation methods compute respiratory induced volume changes as a surrogate for pulmonary ventilation. Currently, there are no known methods to derive perfusion information from noncontrast CT. We introduce a novel CT‐Perfusion (CT‐P) method for computing the magnitude mass changes apparent on dynamic noncontrast CT as a surrogate for pulmonary perfusion. METHODS: CT‐Perfusion is based on a mass conservation model which describes the unknown mass change as a linear combination of spatially corresponding inhale and exhale HU estimated voxel densities. CT‐P requires a deformable image registration (DIR) between the inhale/exhale lung CT pair, a preprocessing lung volume segmentation, and an estimate for the Jacobian of the DIR transformation. Given this information, the CT‐P image, which provides the magnitude mass change for each voxel within the lung volume, is formulated as the solution to a constrained linear least squares problem defined by a series of subregional mean magnitude mass change measurements. Similar to previous robust CT‐ventilation methods, the amount of uncertainty in a subregional sample mean measurement is related to measurement resolution and can be characterized with respect to a tolerance parameter [Formula: see text]. Spatial Spearman correlation between single photon emission CT perfusion (SPECT‐P) and the proposed CT‐P method was assessed in two patient cohorts via a parameter sweep of [Formula: see text]. The first cohort was comprised of 15 patients diagnosed with pulmonary embolism (PE) who had SPECT‐P and 4DCT imaging acquired within 24 h of PE diagnosis. The second cohort was comprised of 15 nonsmall cell lung cancer patients who had SPECT‐P and 4DCT images acquired prior to radiotherapy. For each test case, CT‐P images were computed for 30 different uncertainty parameter values, uniformly sampled from the range [0.01, 0.125], and the Spearman correlation between the SPECT‐P and the resulting CT‐P images were computed. RESULTS: The median correlations between CT‐P and SPECT‐P taken over all 30 test cases ranged between 0.49 and 0.57 across the parameter sweep. For the optimal tolerance τ = 0.0385, the CT‐P and SPECT‐P correlations across all 30 test cases ranged between 0.02 and 0.82. A one‐sample sign test was applied separately to the PE and lung cancer cohorts. A low Spearmen correlation of 15% was set as the null median value and two‐sided alternative was tested. The PE patients showed a median correlation of 0.57 (IQR = 0.305). One‐sample sign test was statistically significant with 96.5 % confidence interval: 0.20–0.63, P < 0.00001. Lung cancer patients had a median correlation of 0.57(IQR = 0.230). Again, a one‐sample sign test for median was statistically significant with 96.5 percent confidence interval: 0.45–0.71, P < 0.00001. CONCLUSION: CT‐Perfusion is the first mechanistic model designed to quantify magnitude blood mass changes on noncontrast dynamic CT as a surrogate for pulmonary perfusion. While the reported correlations with SPECT‐P are promising, further investigation is required to determine the optimal CT acquisition protocol and numerical method implementation for CT‐P imaging. John Wiley and Sons Inc. 2021-03-11 2021-04 /pmc/articles/PMC8252085/ /pubmed/33608933 http://dx.doi.org/10.1002/mp.14792 Text en © 2021 The Authors. Medical Physics published by Wiley Periodicals LLC on behalf of American Association of Physicists in Medicine. https://creativecommons.org/licenses/by-nc-nd/4.0/This is an open access article under the terms of the http://creativecommons.org/licenses/by-nc-nd/4.0/ (https://creativecommons.org/licenses/by-nc-nd/4.0/) License, which permits use and distribution in any medium, provided the original work is properly cited, the use is non‐commercial and no modifications or adaptations are made.
spellingShingle QUANTITATIVE IMAGING AND IMAGE PROCESSING
Castillo, Edward
Nair, Girish
Turner‐Lawrence, Danielle
Myziuk, Nicholas
Emerson, Scott
Al‐Katib, Sayf
Westergaard, Sarah
Castillo, Richard
Vinogradskiy, Yevgeniy
Quinn, Thomas
Guerrero, Thomas
Stevens, Craig
Quantifying pulmonary perfusion from noncontrast computed tomography
title Quantifying pulmonary perfusion from noncontrast computed tomography
title_full Quantifying pulmonary perfusion from noncontrast computed tomography
title_fullStr Quantifying pulmonary perfusion from noncontrast computed tomography
title_full_unstemmed Quantifying pulmonary perfusion from noncontrast computed tomography
title_short Quantifying pulmonary perfusion from noncontrast computed tomography
title_sort quantifying pulmonary perfusion from noncontrast computed tomography
topic QUANTITATIVE IMAGING AND IMAGE PROCESSING
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8252085/
https://www.ncbi.nlm.nih.gov/pubmed/33608933
http://dx.doi.org/10.1002/mp.14792
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