A SAR Prediction Concept for Parallel Transmission MRI

The speci c absorption rate (SAR) is a limiting factor in higheld MR. SAR estimation is typically performed by numerical simulations using generic human body models. However, SAR concepts for single-channel RF transmission cannot be directly applied for multi-channel systems. In this study, a novel and comprehensive SAR prediction concept for parallel RF transmission MRI is presented, based on pre-calculated B1 and electric elds obtained from EM simulations of multiple numerical body models. The application of so-called Q-matrices and further computational optimizations allow for real-time SAR prediction prior to scanning. This SAR prediction concept was fully integrated into an 8-channel whole body MRI system and facilitates selection of di erent body models and body positions. Experimental validation of the global SAR in phantoms showed good qualitative and quantitative agreement. Also an initial in vivo validation showed good qualitative agreement between simulated and measured B1. The feasibility and practicability of this SAR prediction concept was shown, paving the way for safe parallel RF transmission in higheld MR.

[1]  Peter Börnert,et al.  Specific absorption rate reduction in parallel transmission by k‐space adaptive radiofrequency pulse design , 2011, Magnetic resonance in medicine.

[2]  R. Luebbers,et al.  The Finite Difference Time Domain Method for Electromagnetics , 1993 .

[3]  Herbert Rinneberg,et al.  Patient safety concept for multichannel transmit coils , 2007, Journal of magnetic resonance imaging : JMRI.

[4]  K. Uğurbil,et al.  Temperature and SAR calculations for a human head within volume and surface coils at 64 and 300 MHz , 2004, Journal of magnetic resonance imaging : JMRI.

[5]  P. Röschmann Radiofrequency penetration and absorption in the human body: limitations to high-field whole-body nuclear magnetic resonance imaging. , 1987, Medical physics.

[6]  Peter Börnert,et al.  Patient Adapted SAR Calculation on a Parallel Transmission System , 2011 .

[7]  Christopher M Collins,et al.  Calculation of SAR for Transmit Coil Arrays. , 2007, Concepts in magnetic resonance. Part B, Magnetic resonance engineering.

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

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

[10]  F. Bardati,et al.  SAR optimization in a phased array radiofrequency hyperthermia system , 1995, IEEE Transactions on Biomedical Engineering.

[11]  K. Caputa,et al.  An algorithm for computations of the power deposition in human tissue , 1999 .

[12]  E. Adalsteinsson,et al.  Magnitude least squares optimization for parallel radio frequency excitation design demonstrated at 7 Tesla with eight channels , 2008, Magnetic resonance in medicine.

[13]  Douglas C Noll,et al.  Small tip angle three‐dimensional tailored radiofrequency slab‐select pulse for reduced B1 inhomogeneity at 3 T , 2005, Magnetic resonance in medicine.

[14]  C Gabriel,et al.  The dielectric properties of biological tissues: I. Literature survey. , 1996, Physics in medicine and biology.

[15]  Peter Börnert,et al.  Eigenmode analysis of transmit coil array for tailored B1 mapping , 2010, Magnetic resonance in medicine.

[16]  Jan J W Lagendijk,et al.  Simultaneous B  1+ homogenization and specific absorption rate hotspot suppression using a magnetic resonance phased array transmit coil , 2007, Magnetic resonance in medicine.

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

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

[19]  Douglas C Noll,et al.  Spatial domain method for the design of RF pulses in multicoil parallel excitation , 2006, Magnetic resonance in medicine.

[20]  Dirk Diehl,et al.  Evaluation of maximum local SAR for parallel transmission (pTx) pulses based on pre-calculated field data using a selected subset of "Virtual Observation Points" , 2010 .

[21]  Lawrence L Wald,et al.  Simultaneous z‐shim method for reducing susceptibility artifacts with multiple transmitters , 2009, Magnetic resonance in medicine.

[22]  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.

[23]  Klaas P Pruessmann,et al.  Optimal design of multiple‐channel RF pulses under strict power and SAR constraints , 2010, Magnetic resonance in medicine.

[24]  C. Collins,et al.  Calculations ofB1 distribution, specific energy absorption rate, and intrinsic signal-to-noise ratio for a body-size birdcage coil loaded with different human subjects at 64 and 128 MHz , 2005, Applied magnetic resonance.

[25]  Zhi-Pei Liang,et al.  Variable slew‐rate spiral design: Theory and application to peak B1 amplitude reduction in 2D RF pulse design , 2007, Magnetic resonance in medicine.