English
 
Help Privacy Policy Disclaimer
  Advanced SearchBrowse

Item

ITEM ACTIONSEXPORT

Released

Meeting Abstract

Novel Splittable N-Tx/2N-Rx Transceiver Phased Array to Optimize both SNR and Transmit Efficiency at 9.4T

MPS-Authors
/persons/resource/persons133464

Avdievich,  NI
Department High-Field Magnetic Resonance, Max Planck Institute for Biological Cybernetics, Max Planck Society;

/persons/resource/persons192635

Giapitzakis,  IA
Department High-Field Magnetic Resonance, Max Planck Institute for Biological Cybernetics, Max Planck Society;

/persons/resource/persons84402

Henning,  A
Department High-Field Magnetic Resonance, Max Planck Institute for Biological Cybernetics, Max Planck Society;

Fulltext (restricted access)
There are currently no full texts shared for your IP range.
Fulltext (public)
There are no public fulltexts stored in PuRe
Supplementary Material (public)
There is no public supplementary material available
Citation

Avdievich, N., Giapitzakis, I., & Henning, A. (2015). Novel Splittable N-Tx/2N-Rx Transceiver Phased Array to Optimize both SNR and Transmit Efficiency at 9.4T. Magnetic Resonance Materials in Physics, Biology and Medicine, 28(Supplement 1), S57-S57.


Cite as: https://hdl.handle.net/11858/00-001M-0000-002A-4463-E
Abstract
Purpose/Introduction: Ultra-high field (UHF) (C7 T) tight fit transceiver head phased arrays improve Tx-efficiency (1, 2) in comparison to larger Tx-only arrays (3). However, increasing the number of elements above 16 is difficult due to decoupling problems and the limited number of Tx-channels. The number of Rx-elements needs to be higher to improve SNR and parallel Rx-perfomance (3). In this work, we developed and constructed a novel splittable transceiver array at 9.4 T (400 MHz). The array doubles the number of Rxelements while keeping both Tx- and Rx-elements at the same distance to a subject. Both Tx and Rx-performance are optimized using this technology. Subjects and Methods: The array (Fig. 1) consists of 4 Tx-loops (8 9 9 cm). Each loop can be split into two smaller Rx-loops (Fig. 1b). Splitting is provided by 4 PIN diode switches, S1, S2. During transmission four larger loops are produced by shortening S1 and opening S2 switches. Open S1 and shortened S2 switches produce two Rx-loops during reception. All switches are connected in series and driven by 100 mA current. The array can also be used in 4-channel mode without splitting. In both modes a 4-way splitter with 1008 phase shift between the loops was used during transmission. B1 + maps were obtained using the AFI sequence (4) and a rectangular phantom (26 9 20 9 12 cm) matching tissue properties (3). SNR and g-factor maps were obtained using non-accelerated and GRAPPA accelarated GREs (3). Data were acquired on the Siemens Magnetom Discussion/Conclusion: Both SNR and parallel reception were substantially improved by doubling the number of Rx-elements. Arrangement of elements can be adapted to future head or body applications. The direction of splitting can be chosen depending on the most beneficial direction of acceleration. Tx-elements splittable into a larger number of Rx-elements (4, 8) would allow acceleration in both directions. As a proof of concept we developed a novel splittable transceiver phased array. Both Tx- and Rx-performance are optimized using this method.