测量自旋-自旋弛豫时间的最优采样策略

J.A. Jones , P. Hodgkinson , A.L. Barker , P.J. Hore
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引用次数: 109

摘要

说明了如何利用cram - rao理论来确定测量核磁共振自旋-自旋弛豫时间T2的最佳采样模式。这些结果也可以应用于任何其他指数衰减的测量,包括一些用于测量自旋晶格弛豫时间T1的脉冲序列。最佳采样模式包括将22%的样本点置于0时间,将其余78%的样本点置于1.28T2,或者,更实际且几乎同样准确地,将一个点置于0时间,四个点置于1.30T2时间。这些抽样模式与常用的抽样模式大不相同。cram - rao结果与实验测量和计算机模拟进行了比较。描述了该方法的一些局限性,并讨论了将其扩展到同时测量2个值范围的问题。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Optimal Sampling Strategies for the Measurement of Spin–Spin Relaxation Times

It is shown how Cramér–Rao theory may be used to determine the optimal sampling pattern for measuring the NMR spin–spin relaxation time,T2. The results may also be applied to the measurement of any other exponential decay, including some pulse sequences for measuring the spin–lattice relaxation time,T1. The optimal sampling pattern involves placing 22% of the sample points at zero time and the remaining 78% at 1.28T2, or, more practically and almost as accurately, one point at zero and four at 1.30T2. These sampling patterns are very different from those commonly used. The Cramér–Rao results are compared with experimental measurements and computer simulations. Some limitations of the method are described, and its extension to the simultaneous measurement of a range ofT2values is addressed.

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