Baishya Bikash, Suryaprakash N
Solid State and Structural Chemistry Unit, Indian Institute of Science, Bangalore 560012, India.
J Chem Phys. 2007 Dec 7;127(21):214510. doi: 10.1063/1.2803900.
In the present work we demonstrate a novel method for spectral simplification and determination of the relative signs of the scalar couplings using a spin selective multiple quantum NMR experiment. A spin selective excitation of double quantum coherence of A and M spins in a weakly coupled three spin system of the type AMX, results in a doublet in the double quantum dimension whose separation corresponds to the sum of couplings of the active spins to the passive spin X. One component of the doublet has the passive spin X in mid R:alpha state while the other component has the passive spin X in mid R:beta state. The spin selective conversion of double quantum coherence to single quantum coherence does not disturb the spin states of the passive spin thereby providing the spin state selection. There will be two domains of single quantum transitions in single quantum dimension at the chemical shift positions of A and M spins. The mid R:alpha domain of A spin is a doublet because of mid R:alpha and mid R:beta states of M spin only, while that of mid R:beta domain is another doublet in a different cross section of the spectra. The scalar coupling J(AM) can be extracted from any of the mid R:alpha and mid R:beta domain transitions while the relative displacements of the two doublets between the two domains at the two chemical shifts provides the magnitude and sign of the scalar coupling J(AX) relative to the coupling J(MX). Similar result is obtained for zero quantum studies on AMX spin system. The proposed technique is discussed theoretically using product operator approach. The new spin state selective double quantum J-resolved sequence has also been developed. The methodology is confirmed experimentally on a homonuclear weakly coupled three spin system and applied to two different heteronuclear five spin systems.
在本工作中,我们展示了一种新颖的方法,用于光谱简化以及使用自旋选择性多量子核磁共振实验确定标量耦合的相对符号。在AMX型弱耦合三自旋系统中,对A和M自旋的双量子相干进行自旋选择性激发,会在双量子维度上产生一个双峰,其间距对应于活性自旋与被动自旋X的耦合之和。双峰的一个分量中被动自旋X处于中R:α态,而另一个分量中被动自旋X处于中R:β态。双量子相干到单量子相干的自旋选择性转换不会干扰被动自旋的自旋状态,从而实现自旋状态选择。在单量子维度上,A和M自旋的化学位移位置会有两个单量子跃迁域。A自旋的中R:α域只是由于M自旋的中R:α和中R:β态而成为一个双峰,而中R:β域在光谱的不同截面中是另一个双峰。标量耦合J(AM)可以从任何一个中R:α和中R:β域跃迁中提取,而两个域在两个化学位移处的两个双峰的相对位移提供了相对于耦合J(MX)的标量耦合J(AX)的大小和符号。对于AMX自旋系统的零量子研究也得到了类似结果。使用乘积算符方法从理论上讨论了所提出的技术。还开发了新的自旋状态选择性双量子J分辨序列。该方法在同核弱耦合三自旋系统上通过实验得到了证实,并应用于两个不同的异核五自旋系统。