TY - JOUR
T1 - Unshielded bent folded-end dipole 9.4 T human head transceiver array decoupled using modified passive dipoles
AU - Avdievich, Nikolai I.
AU - Solomakha, Georgiy
AU - Ruhm, Loreen
AU - Henning, Anke
AU - Scheffler, Klaus
N1 - Funding Information:
Financial support by the Max Planck Society, German Research Foundation (Reinhart Koselleck Project, DFG SCHE 658/12), European Union (European Research Council [ERC] Starting Grant, SYNAPLAST MR, grant number: 679927; ERC Advanced Grant, Spread MRI, grant number 834940), and Cancer Prevention and Research Institute of Texas (grant number: RR180056) are gratefully acknowledged. S.G. acknowledges Russian Science Foundation (Project 19‐75‐10104) for support of numerical simulations.
Funding Information:
Supported by the Max Planck Society, German Research Foundation (Reinhart Koselleck Project, DFG SCHE 658/12); the European Union (European Research Council [ERC] Starting Grant, SYNAPLAST MR, grant number: 679927); the ERC Advanced Grant, Spread MRI, grant number 834940); and the Cancer Prevention and Research Institute of Texas (CPRIT), (grant number: RR180056); Russian Science Foundation (Project 19‐75‐10104)
Publisher Copyright:
© 2021 The Authors. Magnetic Resonance in Medicine published by Wiley Periodicals LLC on behalf of International Society for Magnetic Resonance in Medicine.
PY - 2021/7
Y1 - 2021/7
N2 - Purpose: To develop an unshielded dipole transceiver array for human head imaging at 9.4 Tesla and to improve decoupling of adjacent dipole elements, a novel array design with modified passive dipole antennas was developed, evaluated, and tested. Methods: The new array consisted of 8 bent folded-end dipole elements placed in a single row and surrounding the head. Adjacent elements of RF transceiver arrays are usually decoupled by introducing circuits electrically connected to elements. These methods are difficult to use for dipole arrays because of the distant location of the adjacent antennas. A recently developed decoupling technique using passive dipoles is simple and does not require any electrical connection. However, common parallel passive dipoles can produce destructive interference with the RF field of the array itself. To minimize this interference, we placed the passive dipoles perpendicularly to the active dipoles and positioned them at the ends of the array. We also evaluated the effect of different passive dipoles on the array transmit performance. Finally, we optimized the array transmit performance by varying the length of the dipole folded portion. Results: By rotating the passive dipoles 90º and moving them toward the ends of the array, we minimized the destructive interference to an acceptable level without compromising decoupling and the transmit efficiency. Conclusion: While keeping the benefits of the passive dipole decoupling method, the new modified dipoles produce substantially less destructive interference with the RF field of the array than the common design. The constructed transceiver array demonstrated good decoupling and whole-brain coverage.
AB - Purpose: To develop an unshielded dipole transceiver array for human head imaging at 9.4 Tesla and to improve decoupling of adjacent dipole elements, a novel array design with modified passive dipole antennas was developed, evaluated, and tested. Methods: The new array consisted of 8 bent folded-end dipole elements placed in a single row and surrounding the head. Adjacent elements of RF transceiver arrays are usually decoupled by introducing circuits electrically connected to elements. These methods are difficult to use for dipole arrays because of the distant location of the adjacent antennas. A recently developed decoupling technique using passive dipoles is simple and does not require any electrical connection. However, common parallel passive dipoles can produce destructive interference with the RF field of the array itself. To minimize this interference, we placed the passive dipoles perpendicularly to the active dipoles and positioned them at the ends of the array. We also evaluated the effect of different passive dipoles on the array transmit performance. Finally, we optimized the array transmit performance by varying the length of the dipole folded portion. Results: By rotating the passive dipoles 90º and moving them toward the ends of the array, we minimized the destructive interference to an acceptable level without compromising decoupling and the transmit efficiency. Conclusion: While keeping the benefits of the passive dipole decoupling method, the new modified dipoles produce substantially less destructive interference with the RF field of the array than the common design. The constructed transceiver array demonstrated good decoupling and whole-brain coverage.
KW - RF head array
KW - decoupling of the transmit dipoles
KW - folded-end dipole antenna
KW - transceiver array
KW - ultra-high field MRI
KW - whole-brain coverage
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U2 - 10.1002/mrm.28711
DO - 10.1002/mrm.28711
M3 - Article
C2 - 33629436
AN - SCOPUS:85101531065
SN - 0740-3194
VL - 86
SP - 581
EP - 597
JO - Magnetic resonance in medicine
JF - Magnetic resonance in medicine
IS - 1
ER -