Abstract

To overcome challenges of inhomogeneous transmit B1 distribution and high specific energy absorption rate (SAR) in MRI, we compare slice-selective array-optimized composite pulse and RF shimming designed to both improve B1 uniformity and reduce SAR using an 8-channel transmit head array loaded with a head model at various RF pulse excitation times, and compare results with standard quadrature voltage distribution at 3T (128 MHz) and 7T (300 MHz). The excitation uniformity was estimated throughout the 3D brain region and SAR was calculated for the whole head. The optimized composite pulse could produce significantly better homogeneity and significantly better homogeneity when SAR was not constrained, and both significantly better homogeneity and lower SAR when the pulse duration was allowed to be twice that of the quadrature or RF shimmed pulse. When the total pulse durations were constrained to the same length, the relative advantages of the optimized composite pulse for producing better homogeneity and lower SAR simultaneously were diminished. Using the optimization results, the slice-selective composite pulse sequence was implemented on a 3D MRI simulator currently under development, and showed both effective slice selection and improvement in excitation uniformity compared to a conventional quadrature driving method.

Highlights

  • High field (3T and greater) magnetic resonance imaging (MRI) systems are used increasingly in clinical diagnosis and scientific research because of high Signal-to-Noise Ratio (SNR) and versatile soft tissue contrast

  • The slice-selective composite pulse sequence was implemented on a 3D MRI simulator currently under development, and showed both effective slice selection and improvement in excitation uniformity compared to a conventional quadrature driving method

  • The most recent IEC guidelines [18] clarify the distinction between suggested specific energy absorption rate (SAR) limits for volume transmit coils and those for local transmit coils with no local (10 g) SAR limits given for volume transmit coils

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Summary

Introduction

High field (3T and greater) magnetic resonance imaging (MRI) systems are used increasingly in clinical diagnosis and scientific research because of high Signal-to-Noise Ratio (SNR) and versatile soft tissue contrast. Higher main magnetic field (B0) strengths require a higher frequency RF magnetic (B1) field resulting in more dramatic perturbations of the B1 field and more power absorbed by the human body or a sample for a given B1 field strength. The wavelength inside the human body will be shorter at the higher field strengths, and much shorter in tissue than in free space. Because the human body has complex geometry consisting of highly inhomogeneous and lossy materials, strong electromagnetic interactions between the RF fields and the human body are expected. These interactions can lead to non-uniform, asymmetric, and complex current distributions on the RF coils as well as the inside of the human body. The distortions of the B1 field and increased absorbed power present significant challenges to the further advancement of MR

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