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-...
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Elsevier
2022
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oai:doaj.org-article:14971f3d4d8344f7864e16771618e8862021-12-04T04:33:59ZFast and equilibrium CEST imaging of brain tumor patients at 3T2213-158210.1016/j.nicl.2021.102890https://doaj.org/article/14971f3d4d8344f7864e16771618e8862022-01-01T00:00:00Zhttp://www.sciencedirect.com/science/article/pii/S221315822100334Xhttps://doaj.org/toc/2213-1582Chemical 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.Yin WuZhou LiuQian YangLiyan ZouFan ZhangLong QianXin LiuHairong ZhengDehong LuoPhillip Zhe SunElsevierarticleAmide proton transferChemical exchange saturation transferQuasi-steady-state (QUASS)TumorComputer applications to medicine. Medical informaticsR858-859.7Neurology. Diseases of the nervous systemRC346-429ENNeuroImage: Clinical, Vol 33, Iss , Pp 102890- (2022) |
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DOAJ |
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Amide proton transfer Chemical exchange saturation transfer Quasi-steady-state (QUASS) Tumor Computer applications to medicine. Medical informatics R858-859.7 Neurology. Diseases of the nervous system RC346-429 |
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Amide proton transfer Chemical exchange saturation transfer Quasi-steady-state (QUASS) Tumor Computer applications to medicine. Medical informatics R858-859.7 Neurology. Diseases of the nervous system RC346-429 Yin Wu Zhou Liu Qian Yang Liyan Zou Fan Zhang Long Qian Xin Liu Hairong Zheng Dehong Luo Phillip Zhe Sun Fast and equilibrium CEST imaging of brain tumor patients at 3T |
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 |
article |
author |
Yin Wu Zhou Liu Qian Yang Liyan Zou Fan Zhang Long Qian Xin Liu Hairong Zheng Dehong Luo Phillip Zhe Sun |
author_facet |
Yin Wu Zhou Liu Qian Yang Liyan Zou Fan Zhang Long Qian Xin Liu Hairong Zheng Dehong Luo Phillip Zhe Sun |
author_sort |
Yin Wu |
title |
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_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_sort |
fast and equilibrium cest imaging of brain tumor patients at 3t |
publisher |
Elsevier |
publishDate |
2022 |
url |
https://doaj.org/article/14971f3d4d8344f7864e16771618e886 |
work_keys_str_mv |
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