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High-resolution creatine mapping of mouse brain at 11.7 T using non-steady-state chemical exchange saturation transfer
被引:28
作者:
Chen, Lin
[1
,2
]
Wei, Zhiliang
[1
,2
]
Cai, Shuhui
[3
]
Li, Yuguo
[1
,2
]
Liu, Guanshu
[1
,2
]
Lu, Hanzhang
[1
,2
]
Weiss, Robert G.
[1
,4
]
van Zijl, Peter C. M.
[1
,2
]
Xu, Jiadi
[1
,2
]
机构:
[1] Johns Hopkins Univ, Sch Med, Russell H Morgan Dept Radiol & Radiol Sci, Baltimore, MD USA
[2] Kennedy Krieger Res Inst, FM Kirby Res Ctr Funct Brain Imaging, Baltimore, MD USA
[3] Xiamen Univ, Fujian Prov Key Lab Plasma & Magnet Resonance, Dept Elect Sci, Xiamen, Fujian, Peoples R China
[4] Johns Hopkins Univ, Sch Med, Dept Med, Div Cardiol, Baltimore, MD 21205 USA
基金:
中国国家自然科学基金;
关键词:
chemical exchange saturation transfer (CEST);
creatine;
magnetization transfer;
polynomial and Lorentzian line-shape fitting (PLOF);
QUANTITATIVE PULSED CEST;
IN-VIVO;
NEUROCHEMICAL PROFILE;
RAT-BRAIN;
H-1-NMR SPECTROSCOPY;
ROTATING-FRAME;
TRANSFER MRI;
SPIN-LOCK;
RELAXATION;
QUANTIFICATION;
D O I:
10.1002/nbm.4168
中图分类号:
Q6 [生物物理学];
学科分类号:
071011 ;
摘要:
The current study aims to optimize the acquisition scheme for the creatine chemical exchange saturation transfer weighted (CrCESTw) signal on mouse brain at 11.7 T, in which a strong magnetization transfer contrast (MTC) is present, and to further develop the polynomial and Lorentzian line-shape fitting (PLOF) method for quantifying CrCESTw signal with a non-steady-state (NSS) acquisition scheme. Studies on a Cr phantom with cross-linked bovine serum albumin (BSA) as well as on mouse brain demonstrated that the maximum CrCESTw signal was reached with a short saturation time determined by the rotating frame relaxation time of the MTC pool instead of the steady-state saturation. The saturation power for the maximal signal was around 1-1.5 mu T for Cr with 20% cross-linked BSA and in vivo applications, but 2 mu T was found to be most practical for signal stability. For the CrCEST acquisition with strong MTC interference, the optimal saturation power and length are completely different from those on Cr solution alone. This observation could be explained well using R-1 rho theory by incorporating the strong MTC pool. Finally, a high-resolution Cr map was obtained on mouse brain using the PLOF method with the NSS CEST acquisition and a cryogenic coil. The Cr map obtained by CEST showed homogenous intensity across the mouse brain except for regions with cerebrospinal fluid.
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页数:16
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