容量负载分环的磁感应元表面用于7T核磁共振鸟中的局部场均化:一个模拟研究研究
Manuel J Freire1, Ricardo Marqués1, Jesús Tornero2
1Department of Electronics and Electromagnetism, University of Seville, Spain.
Journal of magnetic resonance (San Diego, Calif. : 1997)
|November 9, 2023
概括
由导电环组成的元表面可以使7T鸟MRI扫描仪中的传输场B1+均化. 这些阵列支持磁电感应波,提高场均性,而无需调节扫描仪的传输和接收.
科学领域:
- 磁共振成像 (MRI) 是一种磁共振成像技术.
- 电磁主义 电磁主义
- 超材料是指一种超材料.
背景情况:
- 在7台特斯拉 (T) 鸟磁共振成像 (MRI) 扫描仪中的发射场B1+显著不均.
- 这种不均性源于波长效应与生物组织相互作用,限制了图像质量和定量准确性.
- 现有的B1+场均质化方法通常是复杂的或集成到扫描仪设计中.
研究的目的:
- 为了研究使用超表面在7T鸟MRI扫描仪中使B1+场均质化.
- 评估使用这些超表面与商业MRI系统进行传输和接收的可行性.
主要方法:
- 设计和实施的超表面包括容量负载导电环的二维平面阵列.
- 在患者的头部和鸟线圈之间放置了超表面.
- 分析了由于相互的感应合而导致的超表面阵列内静止磁电感应波的激发.
主要成果:
- 超表面通过静态磁感应波成功产生了强大的局部场,从而促进了B1+场的均质化.
- 超表面的存在并没有导致鸟共振器的显著脱调.
- 拟议的解决方案与现有的商业鸟线圈兼容,用于发射和接收操作.
结论:
- 超表面提供了一种可行的,非侵入性的方法,用于提高高场MRI中的B1+场均性.
- 这种方法可以提高7TMRI系统的性能,而不需要对商业扫描仪进行硬件修改.
- 超表面的磁感应波特性是实现局部化场均质化的关键.
相关概念视频
Magnetic Field Of A Current Loop
4.6K
Consider a circular loop with a radius a, that carries a current I. The magnetic field due to the current at an arbitrary point P along the axis of the loop can be calculated using the Biot-Savart law.
4.6K
Induced Electric Fields: Applications
1.7K
An important distinction exists between the electric field induced by a changing magnetic field and the electrostatic field produced by a fixed charge distribution. Specifically, the induced electric field is nonconservative because it does not work in moving a charge over a closed path. In contrast, the electrostatic field is conservative and does no net work over a closed path. Hence, electric potential can be associated with the electrostatic field but not the induced field. The following...
1.7K
Diamagnetic Shielding of Nuclei: Local Diamagnetic Current
877
An applied magnetic field causes the electrons present in the molecule to circulate, setting up a local diamagnetic current within the molecule. The local diamagnetic current arising from circulating sigma-bonding electrons induces a magnetic field, Blocal that opposes the applied magnetic field, B0. The effective magnetic field experienced by these nuclei is given by the difference between the applied and local magnetic fields in a phenomenon called local diamagnetic shielding. Essentially,...
877


