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Schulich Faculty of Chemistry, Technion - Israel Institute of Technology, Haifa, 3200003, Israel.
Phys Chem Chem Phys. 2017 Feb 15;19(7):5222-5229. doi: 10.1039/c6cp07597e.
ESR spectroscopy can be efficiently used to acquire the distance between two spin labels placed on a macromolecule by measuring their mutual dipolar interaction frequency, as long as the distance is not greater than ∼10 nm. Any hope to significantly increase this figure is hampered by the fact that all available spin labels have a phase memory time (T), restricted to the microseconds range, which provides a limited window during which the dipolar interaction frequency can be measured. Thus, due to the inverse cubic dependence of the dipolar frequency over the labels' separation distance, evaluating much larger distances, e.g. 20 nm, would require to have a T that is ∼200 microsecond, clearly beyond any hope. Here we propose a new approach to greatly enhancing the maximum measured distance available by relying on another type of dipole interaction-mediated mechanism called spin diffusion. This mechanism operates and can be evaluated during the spin lattice relaxation time, T (commonly in the milliseconds range), rather than only during T. Up until recently, the observation of spin diffusion in solid electron spin systems was considered experimentally impractical. However, recent developments have enabled its direct measurement by means of high sensitivity pulsed ESR that employs intense short magnetic field gradients, thus opening the door to the subsequent utilization of these capabilities. The manuscript presents the subject of spin diffusion, the ways it can be directly measured, and a theoretical discussion on how intramolecular spin-pair distance, even in the range of 20-30 nm, could be accurately extracted from spin diffusion measurements.
只要两个自旋标记之间的距离不大于约10纳米,电子顺磁共振(ESR)光谱就可以通过测量它们的相互偶极相互作用频率,有效地用于获取放置在大分子上的两个自旋标记之间的距离。但任何显著增加这一距离的希望都受到阻碍,因为所有可用的自旋标记都有一个限于微秒范围的相位记忆时间(T),这就提供了一个有限的窗口,在此期间可以测量偶极相互作用频率。因此,由于偶极频率与标记间分离距离呈立方反比关系,要评估大得多的距离,例如20纳米,就需要一个约为200微秒的T,这显然是不可能的。在此,我们提出一种新方法,通过依赖另一种称为自旋扩散的偶极相互作用介导机制,极大地增加可测量的最大距离。这种机制在自旋晶格弛豫时间T(通常在毫秒范围内)期间起作用且可以被评估,而不只是在T期间。直到最近,在固体电子自旋系统中观察自旋扩散在实验上还被认为是不切实际的。然而,最近的进展使得通过采用强短磁场梯度的高灵敏度脉冲ESR直接测量自旋扩散成为可能,从而为随后利用这些能力打开了大门。本文阐述了自旋扩散的主题、直接测量它的方法,以及关于如何从自旋扩散测量中准确提取分子内自旋对距离(即使在20 - 30纳米范围内)的理论讨论。