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首页> 外文期刊>Magnetic resonance in medical sciences: MRMS : an official journal of Japan Society of Magnetic Resonance in Medicine >Investigation of the asymmetric distributions of RF transmission and reception fields at high static field
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Investigation of the asymmetric distributions of RF transmission and reception fields at high static field

机译:高静电场下射频发射与接收场的不对称分布研究

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摘要

When radiofrequency (RF) transmission field represents B 1 +, the reception field represents B 1 -*. The distribution of those maps demonstrates asymmetric features at high field magnetic resonance (MR) imaging. Both maps are in mirror symmetry to one another. Almost symmetric distribution of the B1 field was expected on the laboratory frame in a symmetric sample loaded inside the RF coil designed to achieve a homogeneous B 1 field. Then, a simple change was made in the coordinate transformation equation of RF fields between the rotating and laboratory frames in both linear and quadrature modes to investigate the source of this feature of asymmetry. The magnitude of rotating frame components, B 1 + and B 1 -, consists of the magnitude and the phase difference of the laboratory frame components. The rotating frame components differ in the sign of the sinusoidal phase difference. B 1 + is equal to B 1 - at lower field because phase changes that depend on position can be ignored. At higher fields, the magnitude component has a symmetric profile, and distribution in the phase component is antisymmetric. Thus, the distributions of B 1 + and B 1 - maps demonstrate mirror symmetry. Maps of magnitude and phase components were examined in the laboratory frame. Their maps were computed from B 1 + and B 1 - maps of the human brain and of a spherical saline phantom measured at 4.7T. It was concluded from these analytical and experimental results that the asymmetric and mirror symmetric distributions in B 1 + and B 1 - are derived from the phase difference in the laboratory frame.
机译:当射频(RF)发送字段表示B 1 +时,接收字段表示B 1-*。这些图的分布在高场磁共振(MR)成像中显示出不对称特征。两张地图彼此镜像对称。预期在实验室框架上的对称样品中B1场几乎对称分布,该对称样品加载到设计成实现均匀B 1场的RF线圈中。然后,对线性和正交模式下旋转和实验室框架之间的射频场的坐标变换方程进行了简单的更改,以研究这种不对称特征的来源。旋转框架组件的大小B 1 +和B 1-由实验室框架组件的大小和相位差组成。旋转框架组件的正弦相位差符号不同。 B 1 +等于B 1-在下半场,因为取决于位置的相位变化可以忽略。在较高的磁场中,幅度分量具有对称轮廓,并且相位分量中的分布是反对称的。因此,B 1 +和B 1-图的分布证明是镜像对称的。在实验室框架中检查了幅度和相位分量图。他们的图谱是根据人脑的B 1 +和B 1-图谱以及在4.7T下测得的球形盐体模绘制的。从这些分析和实验结果可以得出结论,B 1 +和B 1-中的不对称和镜像对称分布是由实验室框架中的相位差得出的。

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