An analytical solution is given for amplitudes and phases of adiabatic decoupling sidebands as a function of spin inversion time . Since all the adiabatic decoupling phases (t, ) refocus at two periods (2T) of the decoupling pulse, the sidebands are located at n/2T rather than at n/T as observed in
Synchronized Adiabatic Decoupling
β Scribed by Shanmin Zhang; David G Gorenstein
- Book ID
- 102602229
- Publisher
- Elsevier Science
- Year
- 2000
- Tongue
- English
- Weight
- 100 KB
- Volume
- 147
- Category
- Article
- ISSN
- 1090-7807
No coin nor oath required. For personal study only.
β¦ Synopsis
A new decoupling scheme termed "synchronized adiabatic decoupling" is developed for use in the indirectly detected dimension. After each increment, the decoupling sequence is replaced by another one with different period T or different initial period T(ini) so that sampling always occurs at the end of a complete decoupling period. The effects of J coupling are therefore completely averaged out for all data points. As a result, all decoupling sidebands disappear and the center band increases correspondingly. Since the synchronized adiabatic decoupling does not require conventional editing techniques to cancel the sidebands, it is useful in high-field gradient-enhanced multidimensional experiments with only a single scan per increment.
π SIMILAR VOLUMES
RF pulse sequences applied to IS spin systems may produce decoupling scheme (4), recently introduced as a method for substantial transverse antiphase S magnetization coupled to anticanceling ordinary sidebands resulting from in-phase magnephase I magnetization, just prior to detection of the S signa
A vector model of adiabatic decoupling is enunciated for an IS-coupled system of two spin-1 2 heteronuclei in the high-power limit of ideal adiabatic pulses. The observed S-spin magnetization evolves according to a time-dependent coupling that scales as the z component of an I-spin vector which evol