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扩展用于异核偶极弛豫的固态T1rho实验的频率范围。

Expanding the frequency range of the solid-state T1rho experiment for heteronuclear dipolar relaxation.

作者信息

Krushelnitsky Alexey, Kurbanov Rauf, Reichert Detlef, Hempel Guenter, Schneider Horst, Fedotov Vladimir

机构信息

Kazan Institute of Biochemistry and Biophysics, PO Box 30, Kazan 420111, Russia.

出版信息

Solid State Nucl Magn Reson. 2002 Dec;22(4):423-38. doi: 10.1006/snmr.2002.0071.

Abstract

Solid-state spin-lattice relaxation in the rotating frame permits the investigation of dynamic processes with correlation times in the range of microseconds. The relaxation process in organic solids is driven by the fluctuation of the local magnetic field due to the dipole-dipole interaction of the probe nuclei (13C,15N) with 1H in close proximity. However, its effect is often hidden by a competing relaxation process due to the contact between the rotating frame 13C/15N Zeeman and 1H dipolar reservoirs. In most cases the latter process becomes superior for the commonly applied low and moderate spin-lock fields and practically does not provide information about the molecular dynamics. To suppress this undesired process and to expand the dynamic range of T1rho experiments, we present two approaches. The first one uses a resonance offset of the frequency of the spin-lock irradiation, which leads to a significant enhancement of the effective spin-lock frequency without the application of destructive high transmitter powers. We derive the theory and demonstrate the applicability of the method on various model compounds. The second approach utilizes heteronuclear 1H decoupling during the 13C/15N spin-lock irradiation which disrupts the contact between the 13C/15N Zeeman and 1H dipolar reservoirs. We demonstrate the method and discuss the results qualitatively.

摘要

旋转坐标系中的固态自旋 - 晶格弛豫使得能够研究相关时间在微秒范围内的动态过程。有机固体中的弛豫过程是由探测核((^{13}C)、(^{15}N))与附近的(^{1}H)之间的偶极 - 偶极相互作用导致的局部磁场波动所驱动的。然而,由于旋转坐标系中的(^{13}C/^{15}N)塞曼与(^{1}H)偶极库之间的接触,其效应常常被一个竞争性的弛豫过程所掩盖。在大多数情况下,对于常用的低和中等自旋锁定场,后一种过程占主导,实际上无法提供有关分子动力学的信息。为了抑制这种不期望的过程并扩大(T1rho)实验的动态范围,我们提出了两种方法。第一种方法使用自旋锁定辐照频率的共振偏移,这在不施加高功率破坏性发射机功率的情况下显著提高了有效自旋锁定频率。我们推导了该理论并证明了该方法在各种模型化合物上的适用性。第二种方法在(^{13}C/^{15}N)自旋锁定辐照期间利用异核(^{1}H)去耦,这破坏了(^{13}C/^{15}N)塞曼与(^{1}H)偶极库之间的接触。我们展示了该方法并定性地讨论了结果。

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