Rotary-resonance condition

Recently a new type of proton assisted recoupling experiments has been developed for coherence transfer where rf irradiation is taking place on all involved rf channels. This embraces the homonuclear proton assisted recoupling (PAR) [45, 140, 141] and the later resonant second-order transfer (RESORT) [142] experiments, as well as the heteronuclear proton assisted insensitive nuclei (PAIN) cross polarization [44] experiments. In PAR and PAIN, spin-lock CW irradiation is applied on both passive ( H) and active spins (13C, 15N) without matching rotary resonance conditions. In RESORT a phase alternation irradiation scheme for the passive spins is used. 

Finally, we should also mention that assisted spin recoupling is by no means restricted to 1H, 13C, and 15N spin species but may also be used to facilitate H and 2H to low- spin transfers. This may be exploited in extensively deuterated samples using rf fields on JH and 2H which are matched to a rotary resonance condition to facilitate spin-diffusion between 13C spins in a longitudinal mixing process. This was recently demonstrated by van Rossum and coworkers in terms of the doublenucleus enhanced recoupling (DONER) experiment [143]. 

Rotary resonance recoupling of heteronuclear C- H dipolar interactions in NMR spectra (recorded under conditions of H decoupling at frequency vi and MAS at frequency Vr) has been studied for three examples of molecular solids (adamantane, ferrocene and hexamethylbenzene) in which substantial molecular motion is known to occur. It has been shown that when rotary resonance conditions are satisfied (i.e. l Vr = , for n = 1 or 2), the recoupling can lead to motionally averaged Pake-like powder patterns from which information on C- H intemuclear distances and/or molecular motion can be derived. 

While the Ur — 2uj DQ-HORROR condition selectively recouples dipolar interactions, the homonuclear rotary resonance condition = leads to single-quantum and double-quantum recoupling, including recoupling of CSA. Accordingly, the homonuclear n = I condition with Wr = has also been called MSD-HORROR (mixed single- and double quantum HORROR) " and has been employed to determine the orientation of the two C chemical shielding tensors in 2,3- C2-labelled L-alanine. However, the homonuclear resonance condition simultaneously represents a heteronuclear n = 1... 

Fig. 21. (a) H-decoupled NMR spectrum of polycrystalline N-labelled N-methyldiphenylphosphoiamidate, without sample rotation. The P-shielding anisotropy and asymmetry parameters are -21.24 kHz and 0.19, respectively, (b) With ma c-angle sample rotation at 1.5 kHz. (c)-(e) indicate when an r.f. irradiation is on at the N-15 isotropic shift frequency. The irradiation intensity fulfils the rotary resonance conditions [Pg.82]

S. Paul, V.S. Mithu, N.D. Kurur, P.K. Madhu, Efficient heteronuclear dipolar decoupling in solid-state nuclear magnetic resonance at rotary resonance conditions, J. Magn. Reson. 203 (1) (2010) 199-202. 

R -HMQC spectra ofHA and tHA, presented in Fig. 4.16. The N=2 rotary-resonance condition (cOrp = 2(0 was chosen rather than the N= I condition to avoid recoupling of homonuclear recouphng. 

Dipolar recoupling may also be accomplished using continuous rf irradiation as demonstrated in the heteronuclear and homonuclear case by the CP at MAS conditions (or for low-y heteronuclear spins called double-cross-polarization, DCP [103]) and HORROR (homonuclear rotary resonance) [26] experiments, respectively. These experiments may easily be described by transforming the description into the interaction frame of the rf irradiation using (14a) exploiting... 

It is known that, at the HORROR condition, homonuclear dipolar couplings between xHs are reintroduced, leading to partial removal of the heteronuclear coupling.28 29 It is worth noting that at 60 and 120 kHz the proton decoupling is insufficient due to the rotary resonance effect. It has been shown theoretically by Emsley and co-workers,19 that the first and second rotary resonances are partially quenched by the presence of homonuclear couplings. 

Thus, the occurrence of broad C resonances under H high-power decoupling and MAS conditions should neither lead to the automatic conclusion of lack of crystallinity of the sample, nor be considered a nuisance in contrast line broadening mechanisms under MAS are a valuable source of information for the extraction of kinetic parameters and activation energies of thermally activated processes. It should also be mentioned that further line broadening effects may arise from interference between ooi and the MAS frequency, leading to so-called rotary-resonance recoupling of dipolar... 

A new scheme for heteronuclear decoupling, phase-inverted supercycled sequence for attenuation of rotary resonance (PISSARRO), designed for fast MAS has been reported. " Its efficiency compares favourably with CW, TPPM, SPINAL and XiX decoupling methods at medium and high rf amplitudes, particularly under conditions where the efficiency of decoupling is affected by undesired rotary resonance effects. 

Thus cooling-warming cycles, suitably induced, allowed temporal resolution of the reaction, step by step. The absorption, optical rotary dispersion, and electron spin resonance (ESR) spectra of pure compounds I and II were then recorded and found to be similar to those obtained under fast-reaction conditions (Douzou et al., 1970 Douzou and Leter-rier, 1970). Additional interesting observations were made possible by the low-temperature technique for instance, instead of making the time scale of reactions feasible exp>erimentally by increasing the substrate concentrations as in fast techniques, reactions at low temperatures could be performed with stoichiometric concentrations of enzyme. Such con-... 

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