SAR reduction in 7T C‐spine imaging using a “dark modes” transmit array strategy

Local specific absorption rate (SAR) limits many applications of parallel transmit (pTx) in ultra high‐field imaging. In this Note, we introduce the use of an array element, which is intentionally inefficient at generating spin excitation (a “dark mode”) to attempt a partial cancellation of the electric field from those elements that do generate excitation. We show that adding dipole elements oriented orthogonal to their conventional orientation to a linear array of conventional loop elements can lower the local SAR hotspot in a C‐spine array at 7 T.

[1]  Lawrence L. Wald,et al.  Local specific absorption rate (SAR), global SAR, transmitter power, and excitation accuracy trade‐offs in low flip‐angle parallel transmit pulse design , 2014, Magnetic resonance in medicine.

[2]  G. Metzger,et al.  Local B1+ shimming for prostate imaging with transceiver arrays at 7T based on subject‐dependent transmit phase measurements , 2008, Magnetic resonance in medicine.

[3]  Julien Cohen-Adad,et al.  Nineteen‐channel receive array and four‐channel transmit array coil for cervical spinal cord imaging at 7T , 2014, Magnetic resonance in medicine.

[4]  Elfar Adalsteinsson,et al.  Local SAR in parallel transmission pulse design , 2011, Magnetic resonance in medicine.

[5]  Thoralf Niendorf,et al.  Design, evaluation and application of an eight channel transmit/receive coil array for cardiac MRI at 7.0 T. , 2013, European journal of radiology.

[6]  Thoralf Niendorf,et al.  Design and Evaluation of a Hybrid Radiofrequency Applicator for Magnetic Resonance Imaging and RF Induced Hyperthermia: Electromagnetic Field Simulations up to 14.0 Tesla and Proof-of-Concept at 7.0 Tesla , 2013, PloS one.

[7]  Yudong Zhu,et al.  Parallel excitation with an array of transmit coils , 2004, Magnetic resonance in medicine.

[8]  J. Lagendijk,et al.  SAR and power implications of different RF shimming strategies in the pelvis for 7T MRI , 2009, Journal of magnetic resonance imaging : JMRI.

[9]  Steen Moeller,et al.  A 32‐channel lattice transmission line array for parallel transmit and receive MRI at 7 tesla , 2010, Magnetic resonance in medicine.

[10]  Thoralf Niendorf,et al.  Two‐Dimensional sixteen channel transmit/receive coil array for cardiac MRI at 7.0 T: Design, evaluation, and application , 2012, Journal of magnetic resonance imaging : JMRI.

[11]  Lawrence L. Wald,et al.  An Automated Framework to Decouple pTx Arrays with Many Channels , 2012 .

[12]  Gabriele Eichfelder,et al.  Local specific absorption rate control for parallel transmission by virtual observation points , 2011, Magnetic resonance in medicine.

[13]  Y. Rahmat-Samii,et al.  Particle swarm optimization in electromagnetics , 2004, IEEE Transactions on Antennas and Propagation.

[14]  Kawin Setsompop,et al.  Slice‐selective RF pulses for in vivo B  1+ inhomogeneity mitigation at 7 tesla using parallel RF excitation with a 16‐element coil , 2008, Magnetic resonance in medicine.

[15]  Matthew D Robson,et al.  Automated tuning of an eight-channel cardiac transceive array at 7 tesla using piezoelectric actuators , 2014, Magnetic resonance in medicine.

[16]  C A T van den Berg,et al.  Design of a radiative surface coil array element at 7 T: The single‐side adapted dipole antenna , 2011, Magnetic resonance in medicine.