Abstract

The development of novel multiple-element transmit-receive arrays is an essential factor for improving B1+ field homogeneity in cardiac MRI at ultra-high magnetic field strength (B0 > = 7.0T). One of the key steps in the design and fine-tuning of such arrays during the development process is finding the default driving phases for individual coil elements providing the best possible homogeneity of the combined B1+-field that is achievable without (or before) subject-specific B1+-adjustment in the scanner. This task is often solved by time-consuming (brute-force) or by limited efficiency optimization methods. In this work, we propose a robust technique to find phase vectors providing optimization of the B1-homogeneity in the default setup of multiple-element transceiver arrays. The key point of the described method is the pre-selection of starting vectors for the iterative solver-based search to maximize the probability of finding a global extremum for a cost function optimizing the homogeneity of a shaped B1+-field. This strategy allows for (i) drastic reduction of the computation time in comparison to a brute-force method and (ii) finding phase vectors providing a combined B1+-field with homogeneity characteristics superior to the one provided by the random-multi-start optimization approach. The method was efficiently used for optimizing the default phase settings in the in-house-built 8Tx/16Rx arrays designed for cMRI in pigs at 7T.

Highlights

  • The implementation of MRI-scanners, operating at ultra-high field static magnetic fields

  • With Nstart = 1000 starting vectors and N = 8 optimized phase components the random multi-start optimization using the cost function based on the coefficient-ofvariation may lead to the relative gradient which is by factor 10 higher compared to the one achieved in the optimized multi-start

  • We propose a time-efficient technique for the calculation of globally optimized hardware phases to be used for the construction and the subsequent optimization of transceiver arrays for UHF MRI

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Summary

Introduction

The implementation of MRI-scanners, operating at ultra-high field static magnetic fields (UHF of B0 7T, promises a significant increase of both SNR and the spatial resolution (up to ~200μm in-plane) [1] of clinical MR-images. At the Larmor frequency of protons 300MHz (B0 7T) and electrical permittivity of muscle tissue (ε 60), the wavelength of Bþ1 À field (1012cm) is smaller than the dimensions of a human thorax. This leads to the establishment of a standing wave regime and creates interferences of a B1+-field across an imaged field-of-view (FOV).

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