C.J. Gorter Center for High Field MRI, Department of Radiology, Leiden University Medical Center, Leiden, The Netherlands.
Imaging Division, University Medical Centre Utrecht, Utrecht, The Netherlands.
NMR Biomed. 2019 Aug;32(8):e4106. doi: 10.1002/nbm.4106. Epub 2019 May 27.
To 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.
The 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 (B ) 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 B maps and T -weighted spin echo images of the prostate were obtained in vivo for four healthy volunteers.
In simulations, the mean transmit efficiency (B 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.
A 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.
评估为 7T 体部 MRI 设计的新型八元无源曲折偶极子天线阵列的传输效率和比吸收率(SAR)效率,并将这些值与传统的直接馈电曲折偶极子阵列进行比较。
无源偶极子的主要辐射元件印制在介电基板的一侧,并与印制在基板另一侧的较短馈电元件(与同轴电缆相连)电容耦合。在体模和人体体素模型上对无源和直接馈电单兀的传输(B)场和 SAR 进行了模拟。然后对包含无源和直接馈电曲折偶极子的两个八通道阵列进行了模拟,并在四名健康志愿者体内获得了实验性 B 映射和 T -加权自旋回波图像。
在模拟中,前列腺内的平均传输效率(B 与平方根输入功率之比)值低约 12.5%,并且包含无源偶极子的阵列的最大 10g 平均 SAR 低 44%,导致无源偶极子阵列的 SAR 效率提高约 15%。从两个阵列都获得了 RF 整形的涡轮自旋回波图像,并且图像 SNR 彼此相差在 5%以内。
已经证明,曲折偶极子天线的无源馈电网络是一种在高场用于体部成像的多兀阵列提高 SAR 效率的简单方法。我们假设 SAR 效率提高的主要原因是在馈电元件和偶极子的辐射元件之间的介电质中存储了强保守电场。无源馈电方法可以推广到其他偶极子几何形状和配置。