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Fast and equilibrium CEST imaging of brain tumor patients at 3T
Chemical exchange saturation transfer (CEST) MRI, versatile for detecting endogenous mobile proteins and tissue pH, has proved valuable in tumor imaging. However, CEST MRI scans are often performed under non-equilibrium conditions, which confound tissue characterization. This study proposed a quasi-...
Autores principales: | , , , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Elsevier
2021
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8645967/ https://www.ncbi.nlm.nih.gov/pubmed/34864285 http://dx.doi.org/10.1016/j.nicl.2021.102890 |
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author | Wu, Yin Liu, Zhou Yang, Qian Zou, Liyan Zhang, Fan Qian, Long Liu, Xin Zheng, Hairong Luo, Dehong Sun, Phillip Zhe |
author_facet | Wu, Yin Liu, Zhou Yang, Qian Zou, Liyan Zhang, Fan Qian, Long Liu, Xin Zheng, Hairong Luo, Dehong Sun, Phillip Zhe |
author_sort | Wu, Yin |
collection | PubMed |
description | Chemical exchange saturation transfer (CEST) MRI, versatile for detecting endogenous mobile proteins and tissue pH, has proved valuable in tumor imaging. However, CEST MRI scans are often performed under non-equilibrium conditions, which confound tissue characterization. This study proposed a quasi-steady-state (QUASS) CEST MRI algorithm to standardize fast and accurate tumor imaging at 3 T. The CEST signal evolution was modeled by longitudinal relaxation rate during relaxation delay (Td) and spinlock relaxation during RF saturation time (Ts), from which the QUASS CEST effect is derived. Numerical simulation and human MR imaging experiments (7 healthy volunteers and 19 tumor patients) were conducted at 3 T to compare the CEST measurements obtained under two representative experimental conditions. In addition, amide proton transfer (APT), combined magnetization transfer (MT) and nuclear overhauser enhancement (NOE) effects, and direct water saturation were isolated using a 3-pool Lorentzian fitting in white matter and gray matter of healthy volunteers and for patients in the contralateral normal-appearing white matter and tumor regions. Finally, the student's t-test was performed between conventional and QUASS CEST measurements. The routine APT and combined MT & NOE measures significantly varied with Ts and Td (P < .001) and were significantly smaller than the corresponding QUASS indices (P < .001). In contrast, the results from the QUASS reconstruction showed little dependence on the scan protocol (P > .05), indicating the accuracy and robustness of QUASS CEST MRI for tumor imaging. To summarize, the QUASS CEST reconstruction algorithm enables fast and accurate tumor CEST imaging at 3 T, promising to expedite and standardize clinical CEST MRI. |
format | Online Article Text |
id | pubmed-8645967 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2021 |
publisher | Elsevier |
record_format | MEDLINE/PubMed |
spelling | pubmed-86459672021-12-15 Fast and equilibrium CEST imaging of brain tumor patients at 3T Wu, Yin Liu, Zhou Yang, Qian Zou, Liyan Zhang, Fan Qian, Long Liu, Xin Zheng, Hairong Luo, Dehong Sun, Phillip Zhe Neuroimage Clin Regular Article Chemical exchange saturation transfer (CEST) MRI, versatile for detecting endogenous mobile proteins and tissue pH, has proved valuable in tumor imaging. However, CEST MRI scans are often performed under non-equilibrium conditions, which confound tissue characterization. This study proposed a quasi-steady-state (QUASS) CEST MRI algorithm to standardize fast and accurate tumor imaging at 3 T. The CEST signal evolution was modeled by longitudinal relaxation rate during relaxation delay (Td) and spinlock relaxation during RF saturation time (Ts), from which the QUASS CEST effect is derived. Numerical simulation and human MR imaging experiments (7 healthy volunteers and 19 tumor patients) were conducted at 3 T to compare the CEST measurements obtained under two representative experimental conditions. In addition, amide proton transfer (APT), combined magnetization transfer (MT) and nuclear overhauser enhancement (NOE) effects, and direct water saturation were isolated using a 3-pool Lorentzian fitting in white matter and gray matter of healthy volunteers and for patients in the contralateral normal-appearing white matter and tumor regions. Finally, the student's t-test was performed between conventional and QUASS CEST measurements. The routine APT and combined MT & NOE measures significantly varied with Ts and Td (P < .001) and were significantly smaller than the corresponding QUASS indices (P < .001). In contrast, the results from the QUASS reconstruction showed little dependence on the scan protocol (P > .05), indicating the accuracy and robustness of QUASS CEST MRI for tumor imaging. To summarize, the QUASS CEST reconstruction algorithm enables fast and accurate tumor CEST imaging at 3 T, promising to expedite and standardize clinical CEST MRI. Elsevier 2021-11-27 /pmc/articles/PMC8645967/ /pubmed/34864285 http://dx.doi.org/10.1016/j.nicl.2021.102890 Text en © 2021 Published by Elsevier Inc. https://creativecommons.org/licenses/by-nc-nd/4.0/This is an open access article under the CC BY-NC-ND license (http://creativecommons.org/licenses/by-nc-nd/4.0/). |
spellingShingle | Regular Article Wu, Yin Liu, Zhou Yang, Qian Zou, Liyan Zhang, Fan Qian, Long Liu, Xin Zheng, Hairong Luo, Dehong Sun, Phillip Zhe Fast and equilibrium CEST imaging of brain tumor patients at 3T |
title | Fast and equilibrium CEST imaging of brain tumor patients at 3T |
title_full | Fast and equilibrium CEST imaging of brain tumor patients at 3T |
title_fullStr | Fast and equilibrium CEST imaging of brain tumor patients at 3T |
title_full_unstemmed | Fast and equilibrium CEST imaging of brain tumor patients at 3T |
title_short | Fast and equilibrium CEST imaging of brain tumor patients at 3T |
title_sort | fast and equilibrium cest imaging of brain tumor patients at 3t |
topic | Regular Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC8645967/ https://www.ncbi.nlm.nih.gov/pubmed/34864285 http://dx.doi.org/10.1016/j.nicl.2021.102890 |
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