Department of Physics, Utah Center for Advanced Imaging Research, University of Utah, Salt Lake City, Utah 84108, USA.
Magn Reson Med. 2010 Sep;64(3):734-42. doi: 10.1002/mrm.22367.
The conventional stimulated-echo NMR sequence only measures the longitudinal component while discarding the transverse component, after tipping up the prepared magnetization. This transverse magnetization can be used to measure a spin echo, in addition to the stimulated echo. Two-dimensional single-shot spin- and stimulated-echo-planar imaging (ss-SESTEPI) is an echo-planar-imaging-based single-shot imaging technique that simultaneously acquires a spin-echo-planar image and a stimulated-echo-planar image after a single radiofrequency excitation. The magnitudes of the spin-echo-planar image and stimulated-echo-planar image differ by T(1) decay and diffusion weighting for perfect 90 degrees radiofrequency and thus can be used to rapidly measure T(1). However, the spatial variation of amplitude of radiofrequency field induces uneven splitting of the transverse magnetization for the spin-echo-planar image and stimulated-echo-planar image within the imaging field of view. Correction for amplitude of radiofrequency field inhomogeneity is therefore critical for two-dimensional ss-SESTEPI to be used for T(1) measurement. We developed a method for amplitude of radiofrequency field inhomogeneity correction by acquiring an additional stimulated-echo-planar image with minimal mixing time, calculating the difference between the spin echo and the stimulated echo and multiplying the stimulated-echo-planar image by the inverse functional map. Diffusion-induced decay is corrected by measuring the average diffusivity during the prescanning. Rapid single-shot T(1) mapping may be useful for various applications, such as dynamic T(1) mapping for real-time estimation of the concentration of contrast agent in dynamic contrast enhancement MRI.
传统的激发回波 NMR 序列仅在翻转准备好的磁化后测量纵向分量,而丢弃横向分量。这种横向磁化可用于测量自旋回波,除了激发回波之外。二维单次激发自旋和激发回波平面成像(ss-SESTEPI)是一种基于回波平面成像的单次激发成像技术,在单次射频激发后同时采集自旋回波平面图像和激发回波平面图像。自旋回波平面图像和激发回波平面图像的幅度因 T(1) 衰减和扩散加权而有所不同,对于完美的 90 度射频,可以快速测量 T(1)。然而,射频场幅度的空间变化会导致成像视野内的自旋回波平面图像和激发回波平面图像的横向磁化不均匀分裂。因此,对于二维 ss-SESTEPI 用于 T(1) 测量,射频场幅度不均匀性的校正至关重要。我们通过获取具有最小混合时间的额外激发回波平面图像来开发一种射频场幅度不均匀性校正方法,计算自旋回波和激发回波之间的差异,并将激发回波平面图像乘以逆函数图。通过在预扫描期间测量平均扩散率来校正扩散引起的衰减。快速单次 T(1) 映射可能对各种应用有用,例如用于实时估计动态对比增强 MRI 中对比剂浓度的动态 T(1) 映射。