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Motion and magnetic field inhomogeneity correction techniques for chemical exchange saturation transfer (CEST) MRI : A contemporary review

Simegn, Gizeaddis Lamesgin ; Sun, Phillip Zhe ; Zhou, Jinyuan ; Kim, Mina ; Reddy, Ravinder ; Zu, Zhongliang ; Zaiss, Moritz ; Yadav, Nirbhay Narayan ; Edden, Richard A E and van Zijl, Peter C M , et al. (2025) In NMR in Biomedicine 38(1).
Abstract

Chemical exchange saturation transfer (CEST) magnetic resonance imaging (MRI) has emerged as a powerful imaging technique sensitive to tissue molecular composition, pH, and metabolic processes in situ. CEST MRI uniquely probes the physical exchange of protons between water and specific molecules within tissues, providing a window into physiological phenomena that remain invisible to standard MRI. However, given the very low concentration (millimolar range) of CEST compounds, the effects measured are generally only on the order of a few percent of the water signal. Consequently, a few critical challenges, including correction of motion artifacts and magnetic field (B
0 and B
1
+) inhomogeneities, have to be addressed in... (More)

Chemical exchange saturation transfer (CEST) magnetic resonance imaging (MRI) has emerged as a powerful imaging technique sensitive to tissue molecular composition, pH, and metabolic processes in situ. CEST MRI uniquely probes the physical exchange of protons between water and specific molecules within tissues, providing a window into physiological phenomena that remain invisible to standard MRI. However, given the very low concentration (millimolar range) of CEST compounds, the effects measured are generally only on the order of a few percent of the water signal. Consequently, a few critical challenges, including correction of motion artifacts and magnetic field (B
0 and B
1
+) inhomogeneities, have to be addressed in order to unlock the full potential of CEST MRI. Motion, whether from patient movement or inherent physiological pulsations, can distort the CEST signal, hindering accurate quantification. B
0 and B
1
+ inhomogeneities, arising from scanner hardware imperfections, further complicate data interpretation by introducing spurious variations in the signal intensity. Without proper correction of these confounding factors, reliable analysis and clinical translation of CEST MRI remain challenging. Motion correction methods aim to compensate for patient movement during (prospective) or after (retrospective) image acquisition, reducing artifacts and preserving data quality. Similarly, B
0 and B
1
+ inhomogeneity correction techniques enhance the spatial and spectral accuracy of CEST MRI. This paper aims to provide a comprehensive review of the current landscape of motion and magnetic field inhomogeneity correction methods in CEST MRI. The methods discussed apply to saturation transfer (ST) MRI in general, including semisolid magnetization transfer contrast (MTC) and relayed nuclear Overhauser enhancement (rNOE) studies.

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publishing date
type
Contribution to journal
publication status
published
subject
in
NMR in Biomedicine
volume
38
issue
1
publisher
John Wiley & Sons Inc.
external identifiers
  • scopus:85208795593
  • pmid:39532518
ISSN
0952-3480
DOI
10.1002/nbm.5294
language
English
LU publication?
no
additional info
© 2024 John Wiley & Sons Ltd.
id
3ad38956-80fb-4e4b-9471-14f4b2ad3e39
date added to LUP
2024-11-23 01:29:33
date last changed
2025-07-05 23:22:01
@article{3ad38956-80fb-4e4b-9471-14f4b2ad3e39,
  abstract     = {{<p>Chemical exchange saturation transfer (CEST) magnetic resonance imaging (MRI) has emerged as a powerful imaging technique sensitive to tissue molecular composition, pH, and metabolic processes in situ. CEST MRI uniquely probes the physical exchange of protons between water and specific molecules within tissues, providing a window into physiological phenomena that remain invisible to standard MRI. However, given the very low concentration (millimolar range) of CEST compounds, the effects measured are generally only on the order of a few percent of the water signal. Consequently, a few critical challenges, including correction of motion artifacts and magnetic field (B<br>
 0 and B<br>
 1 <br>
 +) inhomogeneities, have to be addressed in order to unlock the full potential of CEST MRI. Motion, whether from patient movement or inherent physiological pulsations, can distort the CEST signal, hindering accurate quantification. B<br>
 0 and B<br>
 1 <br>
 + inhomogeneities, arising from scanner hardware imperfections, further complicate data interpretation by introducing spurious variations in the signal intensity. Without proper correction of these confounding factors, reliable analysis and clinical translation of CEST MRI remain challenging. Motion correction methods aim to compensate for patient movement during (prospective) or after (retrospective) image acquisition, reducing artifacts and preserving data quality. Similarly, B<br>
 0 and B <br>
 1 <br>
 + inhomogeneity correction techniques enhance the spatial and spectral accuracy of CEST MRI. This paper aims to provide a comprehensive review of the current landscape of motion and magnetic field inhomogeneity correction methods in CEST MRI. The methods discussed apply to saturation transfer (ST) MRI in general, including semisolid magnetization transfer contrast (MTC) and relayed nuclear Overhauser enhancement (rNOE) studies.<br>
 </p>}},
  author       = {{Simegn, Gizeaddis Lamesgin and Sun, Phillip Zhe and Zhou, Jinyuan and Kim, Mina and Reddy, Ravinder and Zu, Zhongliang and Zaiss, Moritz and Yadav, Nirbhay Narayan and Edden, Richard A E and van Zijl, Peter C M and Knutsson, Linda}},
  issn         = {{0952-3480}},
  language     = {{eng}},
  number       = {{1}},
  publisher    = {{John Wiley & Sons Inc.}},
  series       = {{NMR in Biomedicine}},
  title        = {{Motion and magnetic field inhomogeneity correction techniques for chemical exchange saturation transfer (CEST) MRI : A contemporary review}},
  url          = {{http://dx.doi.org/10.1002/nbm.5294}},
  doi          = {{10.1002/nbm.5294}},
  volume       = {{38}},
  year         = {{2025}},
}