The cyclic irradiation sidebands appearing in homonuclear adiabatic decoupling are calculated in detail, which reveals the origin of the antisymmetric sidebands. The sidebands can be inverted by inserting an initial decoupling with a different period, but the same f 1rms as the main decoupling that
“Double-WURST” Decoupling for15N- and13C-Double-Labeled Proteins in a High Magnetic Field
✍ Scribed by Shanmin Zhang; Jian Wu; David G. Gorenstein
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 204 KB
- Volume
- 123
- Category
- Article
- ISSN
- 1064-1858
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✦ Synopsis
A ''Double-WURST'' decoupling sequence is constructed for sitogether with suitable phase cycles, mainly to compensate multaneously decoupling the 13 CO and 13 C a regions in 15 N/ 13 C-doupulse imperfections.
ble-labeled proteins. It uses frequency-shifted WURST decoupling
The early design of broadband decoupling sequences is combined with standard WURST decoupling. The power can be based on Fourier analysis, which is quite intuitive but not reduced by two-thirds compared to conventional WURST decoualways successful since the spin system is, by nature, not a pling, which decouples the entire 13 C region including the unneeded linear system. A general decoupling theory was presented region between 13 CO and 13 C a . Well-decoupled spectra are acquired by Waugh (6) based on coherent average-Hamiltonian theusing the Double-WURST decoupling sequence with a test 15 N/ 13 Cory (7). A good broadband decoupling sequence must have double-labeled peptide sample and 8 and 19.6 kDa 15 N/ 13 C-doublean average Hamiltonian labeled proteins. It has also been shown that adiabatic decoupling, WURST, for example, has already reached its highest decoupling index n (Å2) defined in a relation of decouple range D f versus RF
where l is a constant. For n greater than 2, the energy conservation law would be violated, and for offsets D f from zero to as large as possible and a RF therefore is not possible.
📜 SIMILAR VOLUMES
A Gaussian-shaped, offset-independent adiabatic decoupling is adopted to decouple 13CO from 13C alpha or vice versa for 13C- and 15N-double-labeled proteins, together with a compensating decoupling applied on the opposite side of the 13C alpha resonance frequency. In a quite broad range, the double-
A number of heteronuclear 3D techniques have been de-constant-time period of 26-28 ms [2l / 2T(CO)] follows, veloped in recent years to obtain the complete assignment which allows optimum refocusing of the Ca, Cb coupling of 15 N, 13 C-labeled proteins (1). An experiment that often and also allows t
HCN, a new 3D NMR technique for stepwise coherence transfer rarely sufficient to establish the mechanism through which from 1 H to 13 C to 15 N and reverse through direct spin couplings it participates in the protein's function. The structure may 1 J CH and 1 J CN , is presented as a method for dete