TY - JOUR
T1 - Bent folded-end dipole head array for ultrahigh-field MRI turns “dielectric resonance” from an enemy to a friend
AU - Avdievich, Nikolai I.
AU - Solomakha, Georgiy
AU - Ruhm, Loreen
AU - Bause, Jonas
AU - Scheffler, Klaus
AU - Henning, Anke
N1 - Funding Information:
The authors gratefully acknowledge the financial support of the Max Planck Society, German Research Foundation (Reinhart Koselleck Project DFG SCHE 658/12), European Union (ERC Starting Grant SYNAPLAST MR [679927]), the Cancer Prevention and Research Institute of Texas (RR180056), the Russian Foundation for Basic Research (19-29-10038), and the Russian Ministry of Science and Higher Education (8.13464.2019/13.2).
Funding Information:
The authors gratefully acknowledge the financial support of the Max Planck Society, German Research Foundation (Reinhart Koselleck Project DFG SCHE 658/12), European Union (ERC Starting Grant SYNAPLAST MR [679927]), the Cancer Prevention and Research Institute of Texas (RR180056), the Russian Foundation for Basic Research (19‐29‐10038), and the Russian Ministry of Science and Higher Education (8.13464.2019/13.2).
Publisher Copyright:
© 2020 The Authors. Magnetic Resonance in Medicine published by Wiley Periodicals LLC on behalf of International Society for Magnetic Resonance in Medicine
PY - 2020/12/1
Y1 - 2020/12/1
N2 - Purpose: To provide transmit whole-brain coverage at 9.4 T using an array with only eight elements and improve the specific absorption rate (SAR) performance, a novel dipole array was developed, constructed, and tested. Methods: The array consists of eight optimized bent folded-end dipole antennas circumscribing a head. Due to the asymmetrical shape of the dipoles (bending and folding) and the presence of an RF shield near the folded portion, the array simultaneously excites two modes: a circular polarized mode of the array itself, and the TE mode (“dielectric resonance”) of the human head. Mode mixing can be controlled by changing the length of the folded portion. Due to this mixing, the new dipole array improves longitudinal coverage as compared with unfolded dipoles. By optimizing the length of the folded portion, we can also minimize the peak local SAR (pSAR) value and decouple adjacent dipole elements. Results: The new array improves the SEE (' (Formula presented.) '/√pSAR) value by about 50%, as compared with the unfolded bent dipole array. It also provides better whole-brain coverage compared with common single-row eight-element dipole arrays, or even to a more complex double-row 16-element surface loop array. Conclusion: In general, we demonstrate that rather than compensating for the constructive interference effect using additional hardware, we can use the “dielectric resonance” to improve coverage, transmit field homogeneity, and SAR efficiency. Overall, this design approach not only improves the transmit performance in terms of the coverage and SAR, but substantially simplifies the common surface loop array design, making it more robust, and therefore safer.
AB - Purpose: To provide transmit whole-brain coverage at 9.4 T using an array with only eight elements and improve the specific absorption rate (SAR) performance, a novel dipole array was developed, constructed, and tested. Methods: The array consists of eight optimized bent folded-end dipole antennas circumscribing a head. Due to the asymmetrical shape of the dipoles (bending and folding) and the presence of an RF shield near the folded portion, the array simultaneously excites two modes: a circular polarized mode of the array itself, and the TE mode (“dielectric resonance”) of the human head. Mode mixing can be controlled by changing the length of the folded portion. Due to this mixing, the new dipole array improves longitudinal coverage as compared with unfolded dipoles. By optimizing the length of the folded portion, we can also minimize the peak local SAR (pSAR) value and decouple adjacent dipole elements. Results: The new array improves the SEE (' (Formula presented.) '/√pSAR) value by about 50%, as compared with the unfolded bent dipole array. It also provides better whole-brain coverage compared with common single-row eight-element dipole arrays, or even to a more complex double-row 16-element surface loop array. Conclusion: In general, we demonstrate that rather than compensating for the constructive interference effect using additional hardware, we can use the “dielectric resonance” to improve coverage, transmit field homogeneity, and SAR efficiency. Overall, this design approach not only improves the transmit performance in terms of the coverage and SAR, but substantially simplifies the common surface loop array design, making it more robust, and therefore safer.
KW - RF head array
KW - RF shimming
KW - TE mode of a human head
KW - folded-end dipole
KW - ultrahigh-field MRI
KW - whole-brain coverage
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U2 - 10.1002/mrm.28336
DO - 10.1002/mrm.28336
M3 - Article
C2 - 32627916
AN - SCOPUS:85087316001
SN - 0740-3194
VL - 84
SP - 3453
EP - 3467
JO - Magnetic Resonance in Medicine
JF - Magnetic Resonance in Medicine
IS - 6
ER -