Resonant inductive decoupling (RID) for transceiver arrays to compensate for both reactive and resistive components of the mutual impedance

被引:65
作者
Avdievich, Nikolai I. [1 ]
Pan, Jullie W. [1 ]
Hetherington, Hoby P. [1 ]
机构
[1] Yale Univ, Dept Neurosurg, New Haven, CT 06520 USA
基金
美国国家卫生研究院;
关键词
RF head coil; transceiver arrays; array decoupling; high-field MRI; mutual resistance; PHASED-ARRAY; HUMAN BRAIN; 7; T; TRANSMIT SENSE; RF COIL; MRI; 8-CHANNEL; TESLA;
D O I
10.1002/nbm.2989
中图分类号
Q6 [生物物理学];
学科分类号
071011 ;
摘要
Transceiver surface coil arrays improve transmit performance (B-1/kW) and B-1 homogeneity for head imaging up to 9.4T. To further improve reception performance and parallel imaging, the number of array elements must be increased with a corresponding decrease in their size. With a large number of small interacting antennas, decoupling is one of the most challenging aspects in the design and construction of transceiver arrays. Previously described decoupling techniques using geometric overlap, inductive or capacitive decoupling have focused on the elimination of the reactance of the mutual impedance only, which can limit the obtainable decoupling to -10dB as a result of residual mutual resistance. A novel resonant inductive decoupling (RID) method, which allows compensation for both reactive and resistive components of the mutual impedance between the adjacent surface coils, has been developed and verified experimentally. This method provides an easy way to adjust the decoupling remotely by changing the resonance frequency of the RID circuit through the adjustment of a variable capacitor. As an example, a single-row (1x16) 7-T transceiver head array of n=16 small overlapped surface coils using RID decoupling between adjacent coils was built. In combination with overlapped coils, the RID technique achieved better than -24dB of decoupling for all adjacent coils. Copyright (c) 2013 John Wiley & Sons, Ltd.
引用
收藏
页码:1547 / 1554
页数:8
相关论文
共 28 条
[1]  
Aal-Braij R., 2009, P 17 ANN M ISMRM HON, P2974
[2]   Transmit and receive transmission line arrays for 7 tesla parallel imaging [J].
Adriany, G ;
Van de Moortele, PF ;
Wiesinger, F ;
Moeller, S ;
Strupp, JP ;
Andersen, P ;
Snyder, C ;
Zhang, XL ;
Chen, W ;
Pruessmann, KP ;
Boesiger, P ;
Vaughan, T ;
Ugurbil, K .
MAGNETIC RESONANCE IN MEDICINE, 2005, 53 (02) :434-445
[3]   A 32-Channel Lattice Transmission Line Array for Parallel Transmit and Receive MRI at 7 Tesla [J].
Adriany, Gregor ;
Auerbach, Edward J. ;
Snyder, Carl J. ;
Gozubuyuk, Ark ;
Moeller, Steen ;
Ritter, Johannes ;
Van de Moortele, Pierre-Francois ;
Vaughan, Tommy ;
Ugurbil, Kamil .
MAGNETIC RESONANCE IN MEDICINE, 2010, 63 (06) :1478-1485
[4]  
Avdievich N., 2012, P 20 ANN M ISMRM MEL, P2806
[5]   Short Echo Spectroscopic Imaging of the Human Brain at 7T Using Transceiver Arrays [J].
Avdievich, N. I. ;
Pan, J. W. ;
Baehring, J. M. ;
Spencer, D. D. ;
Hetherington, H. P. .
MAGNETIC RESONANCE IN MEDICINE, 2009, 62 (01) :17-25
[6]   Transceiver-Phased Arrays for Human Brain Studies at 7 T [J].
Avdievich, Nikolai I. .
APPLIED MAGNETIC RESONANCE, 2011, 41 (2-4) :483-506
[7]   Tissue-equivalent phantoms for high frequencies [J].
Beck, BL ;
Jenkins, KA ;
Rocca, JR ;
Fitzsimmons, JR .
CONCEPTS IN MAGNETIC RESONANCE PART B-MAGNETIC RESONANCE ENGINEERING, 2004, 20B (01) :30-33
[8]   A conformal transceive array for 7 T neuroimaging [J].
Gilbert, Kyle M. ;
Belliveau, Jean-Guy ;
Curtis, Andrew T. ;
Gati, Joseph S. ;
Klassen, L. Martyn ;
Menon, Ravi S. .
MAGNETIC RESONANCE IN MEDICINE, 2012, 67 (05) :1487-1496
[9]   RADIATIVE LOSSES OF A BIRDCAGE RESONATOR [J].
HARPEN, MD .
MAGNETIC RESONANCE IN MEDICINE, 1993, 29 (05) :713-716
[10]   Insight into RF power requirements and B1 field homogeneity for human MRI via rigorous FDTD approach [J].
Ibrahim, Tamer S. ;
Tang, Lin .
JOURNAL OF MAGNETIC RESONANCE IMAGING, 2007, 25 (06) :1235-1247