Simplifying proton NMR spectra by instant homonuclear broadband decoupling.
Simplifying proton NMR spectra by instant homonuclear broadband decoupling.
复制标题
DOI:
10.1002/anie.201300129
复制
发表时间:
2013-07-08
影响因子:
16.6
通讯作者:
Zangger, Klaus
中科院分区:
文献类型:
--
作者:
Meyer, N. Helge;Zangger, Klaus
NMR spectroscopy is a versatile tool to determine structural, chemical, and physical properties of molecules. One-dimensional 1H NMR spectra probably represent the most often acquired type of NMR data. However, compared to other NMR detectable nuclei, 1H spectra typically suffer from low resolution and severe signal overlap, mainly arising from extensive scalar coupling between protons. Homonuclear broadband decoupling, which leads to a collapse of 1H signals into singlets, has been suggested to be a solution to overcome the problem of poor signal dispersion in 1H NMR spectroscopy. Indeed, it was recently shown that the gain in resolution obtained in 1H spectra by broadband proton decoupling is comparable with the theoretical signal dispersion of regular spectra measured at several GHz.[1] Over the last 30years several methods have been developed which achieve homonuclear broadband decoupling.[2–14] However, these techniques have not been widely used, since they are insensitive and usually complicated processing schemes have to be applied to achieve the desired homonuclear decoupling. Recently, the slice-selective broadband-decoupling during a weak gradient field (also called Zangger–Sterk or ZS method)[14] has been rediscovered and improved to become a more general way to record pure shift spectra.[1, 7, 15]The ZS-method employs the concept of slice-selective excitation by a weak magnetic gradient field to decouple all spins: Different parts of the NMR sample experience different magnetic field strengths when a linear gradient is applied. Therefore, a location-dependent frequency shift Δw= g* G* s across the sample volume over a length of s is established, with the gyromagnetic ratio of the observed nucleus g and the gradient strength G. While the gradient is active, a selective pulse thus excites the whole spectrum. However, different
登录
查看更多内容
影响因子:
4.9
作者:
Nilsson, Mathias;Morris, Gareth A.
通讯作者:
Morris, Gareth A.
影响因子:
2.2
作者:
Lupulescu, Adonis;Olsen, Gregory L.;Frydman, Lucio
通讯作者:
Frydman, Lucio
影响因子:
3.5
作者:
ANDREU, D;UBACH, J;BOMAN, HG
通讯作者:
BOMAN, HG
影响因子:
2.2
作者:
Sakhaii, Peyman;Haase, Burkhard;Bermel, Wolfgang
通讯作者:
Bermel, Wolfgang
影响因子:
2.2
作者:
GEEN, H;FREEMAN, R
通讯作者:
FREEMAN, R