Burger C, Buchli R, McKinnon G, Meier D, Boesiger P
Institute of Biomedical Engineering and Medical Informatics, University of Zurich, Switzerland.
Magn Reson Med. 1992 Aug;26(2):218-30. doi: 10.1002/mrm.1910260204.
When performing volume-localized spectroscopy measurements, the amount of spatial contamination is an important quality criterion. With the ISIS localization technique contamination cannot only arise from the transition regions around the volume of interest, but also from remote regions of the sample. The latter contamination component is a consequence of inhomogeneous excitation pulses, if short repetition times TR are used. Its severity depends both on the order of the eight phase cycling experiments needed for an ISIS measurement, and on the ratio TR/T1. Here it is theoretically discussed from which regions of the sample contamination can arise for a specific phase cycling order. For the worst orders the contaminating regions are almost three times as large as for the optimal orders. The ratio for the effectively measured contamination, however, can be moderated in real experiments, because cancellation effects occur due to the phase distribution of the contaminating signals. 31P phantom experiments clearly demonstrate that contamination is present even if adiabatic excitation pulses are applied and that spatial contamination can be reduced to about a third by an optimal choice of the phase cycling order.
在进行体积定位光谱测量时,空间污染量是一项重要的质量标准。使用ISIS定位技术时,污染不仅可能源于感兴趣体积周围的过渡区域,还可能来自样品的远程区域。如果使用短重复时间TR,后一种污染成分是不均匀激发脉冲的结果。其严重程度既取决于ISIS测量所需的八步相位循环实验的阶数,也取决于TR/T1的比值。本文从理论上讨论了对于特定的相位循环阶数,样品的哪些区域会产生污染。对于最差的阶数,污染区域几乎是最优阶数的三倍。然而,在实际实验中,有效测量的污染比值可以得到控制,因为污染信号的相位分布会产生抵消效应。31P体模实验清楚地表明,即使应用绝热激发脉冲,污染仍然存在,并且通过最佳选择相位循环阶数,空间污染可以减少到大约三分之一。