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Demonstration of accurate multi-pool chemical exchange saturation transfer MRI quantification-Quasi-steady-state reconstruction empowered quantitative CEST analysis
被引:6
|作者:
Sun, Phillip Zhe
[1
,2
,3
]
机构:
[1] Emory Univ, Primate Imaging Ctr, Emory Natl Primate Res Ctr, Atlanta, GA USA
[2] Emory Univ, Sch Med, Dept Radiol & Imaging Sci, Atlanta, GA USA
[3] Emory Univ, Sch Med, Primate Imaging Ctr, Emory Natl Primate Res Ctr,Dept Radiol & Imaging S, 954 Gatewood Rd NE, Atlanta, GA 30329 USA
关键词:
Chemical exchange saturation transfer;
(CEST);
Quantitative CEST (qCEST);
Quasi-steady-state (QUASS);
Spinlock;
PROTON-TRANSFER APT;
TRANSFER QCEST MRI;
PH-WEIGHTED MRI;
MAGNETIZATION-TRANSFER;
IMAGING SIGNAL;
OMEGA PLOT;
AMIDE;
RELAXATION;
SPILLOVER;
OPTIMIZATION;
D O I:
10.1016/j.jmr.2023.107379
中图分类号:
Q5 [生物化学];
学科分类号:
071010 ;
081704 ;
摘要:
Chemical exchange saturation transfer (CEST) MRI is sensitive to dilute labile protons and microenviron-ment properties, yet CEST quantification has been challenging. This difficulty is because the CEST mea-surement depends not only on the underlying CEST system but also on the scan protocols, including RF saturation amplitude, duration, and repetition time. In addition, T1 normalization is not straightfor-ward under non-equilibrium conditions. Recently, a quasi-steady-state (QUASS) algorithm was estab-lished to reconstruct the desired equilibrium state from experimental measurements. Our study aimed to determine the accuracy of spinlock-model-based multi-pool CEST quantification using numerical sim-ulations and phantom experiments. In short, CEST Z-spectra were simulated for a representative 3-pool model, and CEST amplitudes were solved with spinlock model-based multi-pool fitting and assessed as a function of RF saturation time (Ts), repetition time (TR), and T1. Although the apparent CEST signals showed significant T1 dependence, such relationships were not observed following QUASS reconstruc-tion. To test the accuracy of T1 correction, a multi-vial phantom of nicotinamide and creatine was doped with manganese chloride, resulting in T1 ranging from 1 s to beyond 2 s. The multi-labile signals deter-mined from the routine measurements showed significant dependence on Ts, TR, and T1. In contrast, CEST signals from the QUASS reconstruction showed consistent quantification independent of such variables. To summarize, our study demonstrated that accurate CEST quantification is feasible in multi-pool CEST systems with the spinlock-model-based fitting of QUASS CEST MRI. (c) 2023 Elsevier Inc. All rights reserved.
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