Three‐frequency RF coil designed for optimized imaging of hyperpolarized, 13 C‐labeled compounds
Imaging exams involving hyperpolarized, 13 C‐labeled compounds require novel RF coils for efficient signal utilization. While 13 C coils are required for mapping the spatial distribution of the hyperpolarized compounds, imaging/pulsing at different frequencies is also needed for scan setup steps pri...
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Veröffentlicht in: | Magnetic resonance in medicine 2008-10, Vol.60 (4), p.928-933 |
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Hauptverfasser: | , , , , , , , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Imaging exams involving hyperpolarized,
13
C‐labeled compounds require novel RF coils for efficient signal utilization. While
13
C coils are required for mapping the spatial distribution of the hyperpolarized compounds, imaging/pulsing at different frequencies is also needed for scan setup steps prior to the image acquisition. Imaging/pulsing at the
1
H frequency is typically used for anatomical localization and shimming. Flip angle (FA) calibration, which is difficult or impossible to achieve at the
13
C frequency, can be accurately performed at the
23
Na frequency using the natural abundance signal that exists in any living tissue. We demonstrate here a single RF resonant structure that is capable of operating linearly at the
1
H and
23
Na frequencies for scan setup steps, and in quadrature at the
13
C frequency for imaging. Images at the three resonant frequencies of this coil are presented from an exam involving hyperpolarized
13
C compounds in vivo. Magn Reson Med 60:928–933, 2008. © 2008 Wiley‐Liss, Inc. |
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ISSN: | 0740-3194 1522-2594 |
DOI: | 10.1002/mrm.21698 |