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9.4 T double‐tuned 13 C/ 1 H human head array using a combination of surface loops and dipole antennas
Author(s) -
Avdievich Nikolai I.,
Solomakha Georgiy,
Ruhm Loreen,
Henning Anke,
Scheffler Klaus
Publication year - 2021
Publication title -
nmr in biomedicine
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.278
H-Index - 114
eISSN - 1099-1492
pISSN - 0952-3480
DOI - 10.1002/nbm.4577
Subject(s) - dipole , dipole antenna , human head , ultra high frequency , physics , electromagnetic coil , antenna (radio) , antenna array , phased array , bent molecular geometry , nuclear magnetic resonance , optics , materials science , electrical engineering , absorption (acoustics) , engineering , quantum mechanics , composite material
MRI at ultra‐high field (UHF, ≥7 T) provides a natural strategy for improving the quality of X‐nucleus magnetic resonance spectroscopy and imaging due to the intrinsic benefit of increased signal‐to‐noise ratio. Considering that RF coils require both local transmission and reception at UHF, the designs of double‐tuned coils, which often consist of several layers of transmit and receive resonant elements, become quite complex. A few years ago, a new type of RF coil, ie a dipole antenna, was developed and used for human body and head imaging at UHF. Due to the mechanical and electrical simplicity of dipole antennas, combining an X‐nucleus surface loop array with 1 H dipoles can substantially simplify the design of a double‐tuned UHF human head array coil. Recently, we developed a novel bent folded‐end dipole transceiver array for human head imaging at 9.4 T. The new eight‐element dipole array demonstrated full brain coverage, and transmit efficiency comparable to that of the substantially more complex 16‐element surface loop array. In this work, we developed, constructed and evaluated a double‐tuned 13 C/ 1 H human head 9.4 T array consisting of eight 13 C transceiver surface loops and eight 1 H transceiver bent folded‐end dipole antennas all placed in a single layer. We showed that interaction between loops and dipoles can be minimized by placing four 1 H traps into each 13 C loop. The presented double‐tuned RF array coil substantially simplifies the design as compared with the common double‐tuned surface loop arrays. At the same time, the coil demonstrated an improved 1 H longitudinal coverage and good transmit efficiency.