RF encoding using a multielement parallel transmit system

Radiofrequency (RF) encoding using spatially variant RF transmission fields represents an alternative to the conventional signal‐encoding techniques applied in MRI, which are based on main field gradients. Thus, RF encoding might allow omitting the use of all main field gradients, alleviating acoustic noise and other main field gradient‐related problems. This study investigates the potential of RF transmit encoding using spatially nonlinear RF fields generated by an eight‐channel parallel transmit system equipped with the corresponding transmit array. Appropriate spatial encoding functions are determined iteratively by randomized superposition of the array element sensitivities and judging their performance. Besides RF amplitude‐based signal encoding, the possibility of RF phase‐dominated encoding is investigated to allow future fast imaging applications. The theoretical background is given and experimental phantom results are compared with predictions from corresponding simulations to prove the basic feasibility of the approach for low‐resolution MRI. Deviations of roughly 10–15% between main field and RF encoded images were found for an in‐plane resolution of 5 × 5 mm2. The approach of RF encode MRI does not seem to be able to replace standard main field gradient encoding completely, but a suitable combination of both concepts could find promising applications. Magn Reson Med 63:1463–1470, 2010. © 2010 Wiley‐Liss, Inc.

[1]  Scott B King,et al.  MRI using radiofrequency magnetic field phase gradients , 2010, Magnetic resonance in medicine.

[2]  A. Maudsley Fourier imaging using rf phase encoding , 1986, Magnetic Resonance in Medicine.

[3]  Christina Triantafyllou,et al.  A 128‐channel receive‐only cardiac coil for highly accelerated cardiac MRI at 3 Tesla , 2008, Magnetic resonance in medicine.

[4]  J Perlo,et al.  Echo-planar rotating-frame imaging. , 2003, Journal of magnetic resonance.

[5]  D. Blezek,et al.  128‐channel body MRI with a flexible high‐density receiver‐coil array , 2008, Journal of magnetic resonance imaging : JMRI.

[6]  Spatially resolved NQR. , 1992, Magnetic resonance imaging.

[7]  Daniel Canet,et al.  Slice selection in NMR imaging by use of the B1 gradient along the axial direction of a saddle-shaped coil , 1991 .

[8]  M. L. Wood,et al.  Spoiling of transverse magnetization in steady‐state sequences , 1991, Magnetic resonance in medicine.

[9]  P Wach,et al.  Imaging of the active B1 field in vivo , 1996, Magnetic resonance in medicine.

[10]  Kay Nehrke,et al.  On the steady‐state properties of actual flip angle imaging (AFI) , 2009, Magnetic resonance in medicine.

[11]  M. Weiner,et al.  Detection of motion using B1 gradients , 1988, Magnetic resonance in medicine.

[12]  A. Morelli Inverse Problem Theory , 2010 .

[13]  Kawin Setsompop,et al.  Parallel RF transmission with eight channels at 3 Tesla , 2006, Magnetic resonance in medicine.

[14]  Delalande,et al.  Single-coil surface imaging using a radiofrequency field gradient , 2000, Journal of magnetic resonance.

[15]  D I Hoult Rotating frame zeugmatography. , 1980, Philosophical transactions of the Royal Society of London. Series B, Biological sciences.

[16]  F. Franconi,et al.  Radiofrequency map of an NMR coil by imaging. , 1993, Magnetic resonance imaging.

[17]  P Röschmann,et al.  Eight‐channel transmit/receive body MRI coil at 3T , 2007, Magnetic resonance in medicine.

[18]  Jürgen Hennig,et al.  Experimental analysis of parallel excitation using dedicated coil setups and simultaneous RF transmission on multiple channels , 2005, Magnetic resonance in medicine.

[19]  Vasily L Yarnykh,et al.  Actual flip‐angle imaging in the pulsed steady state: A method for rapid three‐dimensional mapping of the transmitted radiofrequency field , 2007, Magnetic resonance in medicine.

[20]  Ingmar Graesslin,et al.  Whole Body 3T MRI System with Eight Parallel RF Transmission Channels , 2006 .