Misra Sushil K, Borbat Peter P, Freed Jack H
Physics Department, Concordia University, Montreal, Quebec H3G 1M8, Canada.
Appl Magn Reson. 2009 Dec 1;36(2-4):237-258. doi: 10.1007/s00723-009-0023-5.
The double quantum coherence (DQC) echo signal for two coupled nitroxides separated by distances ≳10 Å, is calculated rigorously for the six-pulse sequence. Successive application of six pulses on the initial density matrix, with appropriate inter-pulse time evolution and coherence pathway selection leaves only the coherent pathways of interest. The amplitude of the echo signal following the last π pulse can be used to obtain a one-dimensional dipolar spectrum (Pake doublet), and the echo envelope can be used to construct the two-dimensional DQC spectrum. The calculations are carried out using the product space spanned by the two electron-spin magnetic quantum numbers m(1), m(2) and the two nuclear-spin magnetic quantum numbers M(1), M(2), describing e.g. two coupled nitroxides in bilabeled proteins. The density matrix is subjected to a cascade of unitary transformations taking into account dipolar and electron exchange interactions during each pulse and during the evolution in the absence of a pulse. The unitary transformations use the eigensystem of the effective spin-Hamiltonians obtained by numerical matrix diagonalization. Simulations are carried out for a range of dipolar interactions, D, and microwave magnetic field strength B for both fixed and random orientations of the two (14)N (and (15)N) nitroxides. Relaxation effects were not included. Several examples of one- and two-dimensional Fourier transforms of the time domain signals vs. dipolar evolution and spin-echo envelope time variables are shown for illustration. Comparisons are made between 1D rigorous simulations and analytical approximations. The rigorous simulations presented here provide insights into DQC ESR spectroscopy, they serve as a standard to evaluate the results of approximate theories, and they can be employed to plan future DQC experiments.
对于间距≳10 Å的两个耦合氮氧化物,严格计算了六脉冲序列的双量子相干(DQC)回波信号。对初始密度矩阵连续施加六个脉冲,并进行适当的脉冲间时间演化和相干路径选择,仅留下感兴趣的相干路径。最后一个π脉冲之后的回波信号幅度可用于获得一维偶极谱(帕克双峰),回波包络可用于构建二维DQC谱。计算使用由两个电子自旋磁量子数m(1)、m(2)和两个核自旋磁量子数M(1)、M(2)所跨越的乘积空间进行,例如描述双标记蛋白质中的两个耦合氮氧化物。考虑每个脉冲期间以及无脉冲演化期间的偶极和电子交换相互作用,对密度矩阵进行一系列酉变换。酉变换使用通过数值矩阵对角化获得的有效自旋哈密顿量的本征系统。针对两个(14)N(和(15)N)氮氧化物的固定和随机取向,在一系列偶极相互作用D和微波磁场强度B下进行了模拟。未包括弛豫效应。给出了时域信号与偶极演化和自旋回波包络时间变量的一维和二维傅里叶变换的几个示例,用于说明。对一维严格模拟和解析近似进行了比较。这里给出的严格模拟为DQC ESR光谱学提供了见解,它们可作为评估近似理论结果的标准,并且可用于规划未来的DQC实验。