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
Hauptverfasser: Hancu, Ileana, Wood, S. James, Piel, Joseph, Whitt, David B., Fish, Kenneth M., Rutt, Brian K., Tropp, James, Dixon, W. Thomas
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.
ISSN:0740-3194
1522-2594
DOI:10.1002/mrm.21698