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简化化学交换饱和传递(CEST)成像评估:局部偏移频率和 CEST 效应。

Simplified assessment for chemical exchanged saturation transfer (CEST) imaging: local offset frequency and CEST effect.

机构信息

Brain Attack Center Ota Memorial Hospital, 3-6-28 Okinogami, Fukuyama, Hiroshima, 7200825, Japan.

Institute of Biomedical Sciences, Tokushima University Graduate School, 3-18-15 Kuramoto-Cyo, Toksuhima, 7708503, Japan.

出版信息

Radiol Phys Technol. 2024 Mar;17(1):93-102. doi: 10.1007/s12194-023-00752-z. Epub 2023 Oct 28.

Abstract

The aim of this study is to develop a novel phantom for the evaluation of clinical CEST imaging settings, e.g., B and B field inhomogeneities, CEST contrast, and post-processing. We made a phantom composed of two slice sections: a grid section for local offset frequency evaluation and a sample section for CEST effect evaluation using different concentrations of an egg white albumin solution. On a 3 Tesla MR scanner, a phantom study was performed using CEST imaging; the mean B amplitudes were set at 1.2 and 1.9 µT, and CEST images with and without B corrections were acquired. Next, region of interest (ROI) analysis was performed for each slice. Then, CEST images with and without B corrections were compared at each B amplitude. The B corrected Z-spectrums at each local region in the grid section showed a shifting of the curve bottom to 0 ppm. Z-spectrum at B = 1.9 µT showed a broader curve shape than that at 1.2 µT. Moreover, MTR values at 3.5 ppm for each albumin sample at B = 1.9 µT were about two times higher than those at 1.2 µT. Our phantom enabled us to evaluate and optimize B inhomogeneity and the CEST effect at the B amplitude.

摘要

本研究旨在开发一种新型的体模,用于评估临床 CEST 成像设置,例如 B 和 B 场不均匀性、CEST 对比度和后处理。我们制作了一个由两个切片组成的体模:一个用于局部偏移频率评估的网格切片和一个用于使用不同浓度的卵清白蛋白溶液评估 CEST 效应的样本切片。在 3T MR 扫描仪上,使用 CEST 成像进行了体模研究;平均 B 幅度设置为 1.2 和 1.9 µT,并采集了有和没有 B 校正的 CEST 图像。然后,对每个切片进行了感兴趣区域(ROI)分析。然后,比较了每个 B 幅度的有和没有 B 校正的 CEST 图像。网格切片中每个局部区域的 B 校正 Z 谱显示曲线底部向 0 ppm 移动。B = 1.9 µT 的 Z 谱显示出比 B = 1.2 µT 更宽的曲线形状。此外,B = 1.9 µT 时每个白蛋白样本在 3.5 ppm 处的 MTR 值约为 B = 1.2 µT 时的两倍。我们的体模使我们能够评估和优化 B 不均匀性和 CEST 效应在 B 幅度下的效果。

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