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核磁共振中的选择性粒子数反转

Selective population inversion in NMR.

作者信息

Silver M S, Joseph R I, Chen C N, Sank V J, Hoult D I

出版信息

Nature. 1984;310(5979):681-3. doi: 10.1038/310681a0.

Abstract

Population inversion of a selected region of a spectrum is a concept which has wide application in both NMR spectroscopy and imaging. While inversion of population at any one frequency is a trivial matter, ensuring an accurate inversion over a specified bandwidth, with negligible perturbation of the magnetization outside that bandwidth, is a major problem. However, by using as a driving function a complex radiofrequency (r.f.) pulse with an envelope of the form (sech beta t)1+5i where 1/beta is the temporal width and t is time, we have found that above a critical r.f. power threshold, magnetization is accurately inverted over a very sharply defined bandwidth, while outside that region, magnetization is returned to its initial position, and population is unaffected. Within the broad limits imposed by our equipment, we have also discovered that the phenomenon is independent of the incident r.f. power.

摘要

光谱选定区域的粒子数反转是一个在核磁共振光谱学和成像中都有广泛应用的概念。虽然在任何一个频率上实现粒子数反转是一件简单的事情,但要确保在指定带宽上进行精确反转,同时使该带宽之外的磁化强度受到的扰动可忽略不计,却是一个主要问题。然而,通过使用一个包络形式为(sech βt)^(1 + 5i)的复射频(r.f.)脉冲作为驱动函数,其中1/β是时间宽度,t是时间,我们发现,在高于一个临界射频功率阈值时,磁化强度在一个非常明确界定的带宽上被精确反转,而在该区域之外,磁化强度回到其初始位置,且粒子数不受影响。在我们设备所施加的宽泛限制范围内,我们还发现该现象与入射射频功率无关。

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