Abstract

ObjectiveTo evaluate the transmit efficiency and specific absorption rate (SAR) efficiency of a new eight‐element passively fed meander‐dipole antenna array designed for body MRI at 7 T, and to compare these values with a conventional directly fed meander‐dipole array.MethodsThe main radiating element of the passively fed dipole is printed on one side of a dielectric substrate and is capacitively coupled to a shorter feeding element (connected to the coaxial cable) printed on the opposite side of the substrate. The transmit (B1 +) field and SAR were simulated on a phantom and on a human voxel model for both a passively fed and a directly fed single element. Two eight‐channel arrays containing, respectively, directly and passively fed meander dipoles were then simulated, and experimental B1 + maps and T2‐weighted spin echo images of the prostate were obtained in vivo for four healthy volunteers.ResultsIn simulations, the mean transmit efficiency (B1 + per square root input power) value in the prostate was ~ 12.5% lower, and the maximum 10 g average SAR was 44% lower for the array containing passively fed dipoles, resulting in ~ 15% higher SAR efficiency for the passively fed array. In vivo RF‐shimmed turbo spin echo images were acquired from both arrays, and showed image SNRs within 5% of one another.ConclusionA passive‐feeding network for meander‐dipole antennas has been shown to be a simple method to increase the SAR efficiency of a multi‐element array used for body imaging at high fields. We hypothesize that the main reason for the increase in SAR efficiency is the storage of the strong conservative electric field in the dielectric between the feeding element and the radiating element of the dipole. The passive‐feeding approach can be generalized to other dipole geometries and configurations.

Highlights

  • Human MRI at high field strengths is challenging due to significant inhomogeneities in the transmit (B1+) fields that occur as a result of the relatively short RF wavelength in tissue compared with the dimensions of the human body

  • The reference point for the measurements was the feed point, ie the short feeding dipole was at the same distance from the phantom as the feed point of the directly fed dipole

  • The results show that the transmit efficiency of a passively fed dipole or dipole array is reduced by ~ 15% at penetration depths of ~ 10–15 cm, whereas the SAR10g, max is reduced by more than 40% and the specific absorption rate (SAR) efficiency is increased by ~ 15%

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Summary

Introduction

Human MRI at high field strengths is challenging due to significant inhomogeneities in the transmit (B1+) fields that occur as a result of the relatively short RF wavelength in tissue compared with the dimensions of the human body. This is evident in body applications at field strengths of 7 T and higher,[1,2] which has led to the use of transmit arrays consisting of multiple (typically 8–32 elements) transmit antennas.[3,4,5,6,7,8,9] This approach uses individually controlled transmit channel phases and/or magnitudes. Dipoles have been shown both theoretically 18,19 and experimentally[20,21,22,23] to be efficient transmit elements for body imaging at 7 T in particular, and have recently been used at 10.5 T.24

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