7 tesla MRI with RF power and field homogeneity comparable to 4 tesla using computational electromagnetics

被引:0
|
作者
Tang, L. [3 ,4 ]
Ibrahim, T. S. [1 ,2 ,3 ,4 ]
机构
[1] Univ Pittsburgh, Dept Radiol, Pittsburgh, PA 15260 USA
[2] Univ Pittsburgh, Dept Bioengn, Pittsburgh, PA 15260 USA
[3] Univ Oklahoma, Sch Elect & Comp Engn, Norman, OK 73019 USA
[4] Univ Oklahoma, Ctr Bioengn, Norman, OK 73019 USA
关键词
MRI; RF coil; transmit array; FDTD; optimization; RF power; B-1; field; coupling; high filed;
D O I
暂无
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
In ultrahigh (>= 7 Tesla) field magnetic resonance imaging (MRI), the electromagnetic interactions between the coil, its excitation sources, and the biological load become more significant compared to low MRI applications. Computational electromagnetic (CEM) techniques are currently playing a major role in the evaluation of MRI radiofrequency (RF) coils (commonly now, within ultrahigh field context, referred to as transmit arrays). This work compares the RF power requirements in 4 and 7 Tesla human MRI using CEM. Furthermore, we demonstrate that at ultrahigh MRI, high-quality/homogenous RF excitation fields could be obtained simultaneously with total RF power deposition lower than that achieved at lower field strengths. These results dispel what has been widely accepted from quasistatic approximations, namely that pushing the envelope of MRI field strength results in more RF power requirements and therefore, more RF power absorption in human tissue. This study is presented using the finite difference time domain (FDTD) method and a gradient-based optimization method.
引用
收藏
页码:70 / 75
页数:6
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