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Background suppressed magnetization transfer MRI
Author(s) -
Gelderen Peter,
Duyn Jeff H.
Publication year - 2020
Publication title -
magnetic resonance in medicine
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.696
H-Index - 225
eISSN - 1522-2594
pISSN - 0740-3194
DOI - 10.1002/mrm.27978
Subject(s) - magnetization , magnetization transfer , signal (programming language) , nuclear magnetic resonance , excitation , pulse (music) , chemistry , pulse sequence , subtraction , physics , biological system , magnetic resonance imaging , magnetic field , computer science , optics , mathematics , medicine , radiology , biology , arithmetic , quantum mechanics , detector , programming language
Purpose Up to 30% of the hydrogen atoms in brain tissue are part of molecules (“semisolids”) other than water. In MRI, their magnetization is typically not observed directly, but can influence the water magnetization through magnetization transfer (MT). Comparison of MRI scans differentially sensitized to MT allows estimation of the semisolid fraction and potential changes with disease. Here, we present an approach designed to improve this estimate by measuring the size of the MT effect in a single scan. Methods A stimulated echo sequence was used to generate a spatial pattern in the longitudinal water magnetization, which was then given time to exchange with semisolids. After saturating the remaining water magnetization, reverse exchange was allowed to partly re‐establish the original water magnetization pattern. The third excitation pulse then formed a stimulated echo out of this pattern. Results MT data were obtained on 10 human subjects at 7 T with varying exchange times. The images showed the expected time dependence of signal associated with the forward and reverse exchange processes. Excellent suppression of non‐exchanging background signal was achieved. As expected, this suppression came at the price of a substantial reduction in exchange‐related signal (by ~75% compared to the signal in saturation recovery MT), in part because of the reliance on a 2‐step exchange process. Conclusion The results demonstrate an MT signal can be observed in a single acquisition without subtraction. This may be advantageous for MT measurements when signal instabilities related to motion and physiological variations exceed thermal noise sources.