Moderate Magic Angle Spinning Research Articles

High-resolution solid-state NMR of anisotropically mobile molecules under very low-power 1H decoupling and moderate magic-angle spinning

We show that for observing high-resolution heteronuclear NMR spectra of anisotropically mobile systems with order parameters less than 0.25, moderate magic-angle spinning (MAS) rates of ∼11 kHz combined with 1H decoupling at 1–2 kHz are sufficient. Broadband decoupling at this low 1H nutation frequency is achieved by composite pulse sequences such as WALTZ-16. We demonstrate this moderate MAS low-power decoupling technique on hydrated POPC lipid membranes, and show that 1 kHz 1H decoupling yields spectra with the same resolution and sensitivity as spectra measured under 50 kHz 1H decoupling when the same acquisition times (∼50 ms) are used, but the low-power decoupled spectra give higher resolution and sensitivity when longer acquisition times (>150 ms) are used, which are not possible with high-power decoupling. The limits of validity of this approach are explored for a range of spinning rates and molecular mobilities using more rigid membrane systems such as POPC/cholesterol mixed bilayers. Finally, we show 15N and 13C spectra of a uniaxially diffusing membrane peptide assembly, the influenza A M2 transmembrane domain, under 11 kHz MAS and 2 kHz 1H decoupling. The peptide 15N and 13C intensities at low-power decoupling are 70–80% of the high-power decoupled intensities. Therefore, it is possible to study anisotropically mobile lipids and membrane peptides using liquid-state NMR equipment, relatively large rotors, and moderate MAS frequencies.

Enhanced Sensitivity and Resolution in 1H Solid-State NMR Spectroscopy of Paramagnetic Complexes under Very Fast Magic Angle Spinning

High-resolution NMR spectroscopy for paramagnetic complexes in solids has been rarely performed because of its limited sensitivity and resolution due to large paramagnetic shifts and associated technical difficulties. The present study demonstrates that magic angle spinning (MAS) at speeds exceeding 20 kHz provides unusually high sensitivity and excellent resolution in 1H solid-state NMR (SSNMR) for paramagnetic systems. Spinning-speed dependence of 1H MAS spectra showed that very fast MAS (VFMAS) at 24-28 kHz enhanced sensitivity by a factor of 12-18, compared with the sensitivity of 1H SSNMR spectra under moderate MAS at 10 kHz, for Cu(dl-alanine)2.H2O and Mn(acac)3, for which the spectral ranges due to 1H paramagnetic shifts reach 200 and 1000 ppm, respectively. It was theoretically and experimentally confirmed that the absolute sensitivity of 1H VFMAS for small paramagnetic complexes such as Cu(dl-alanine)2 can be an order of magnitude higher than that of equimolar diamagnetic ligands because of short 1H T1 ( approximately 1 ms) of the paramagnetic systems and improved sensitivity under VFMAS. On the basis of this demonstrated high sensitivity, 1H SSNMR micro analysis of paramagnetic systems in a nanomole scale is proposed. Applications were performed on two polymorphs of Cu(II)(8-quinolinol)2, which is a suppressor of human cancer cells. It was demonstrated that 1H VFMAS SSNMR spectra accumulated for 20 nmol of the polycrystalline samples in 10 min enabled one to distinguish alpha- and beta-forms of Cu(II)(8-quinolinol)2 on the basis of shift positions and line widths.

Homonuclear chemical shift correlation in rotating solids via RN?n symmetry-based adiabatic RF pulse schemes

The efficacy of RN(nu) (n) symmetry-based adiabatic Zero-Quantum (ZQ) dipolar recoupling schemes for obtaining chemical shift correlation data at moderate magic angle spinning frequencies has been evaluated. RN(nu) (n) sequences generally employ basic inversion elements that correspond to a net 180 degrees rotation about the rotating frame x-axis. It is shown here via numerical simulations and experimental measurements that it is also possible to achieve efficient ZQ dipolar recoupling via RN(nu) (n) schemes employing adiabatic pulses. Such an approach was successfully used for obtaining (13)C chemical shift correlation spectra of a uniformly labelled sample of (CUG)(97) - a triplet repeat expansion RNA that has been implicated in the neuromuscular disease myotonic dystrophy. An analysis of the (13)C sugar carbon chemical shifts suggests, in agreement with our recent (15)N MAS-NMR studies, that this RNA adopts an Alpha-helical conformation.

Heteronuclear decoupling in rotating solids via symmetry-based adiabatic RF pulse schemes

The performance of symmetry-based adiabatic RF pulse schemes for 1H decoupling at moderate magic angle spinning (MAS) frequencies has been evaluated via numerical simulations and experimentally compared with other decoupling techniques. Our studies reveal that in MAS solid state NMR studies of polycrystalline specimens, in contrast to symmetry-based RF pulse schemes involving rectangular RF pulses, adiabatic decoupling sequences can be effectively implemented to make use of all the available decoupling RF field strength and to eliminate the deleterious effects of H 1 inhomogeneity and resonance offset. Symmetry-based adiabatic decoupling sequences lead to improved decoupling performance compared to a continuous train of adiabatic inversion pulses that are phase cycled as in solution state NMR studies.

REDOR: an assessment of the efficacy of dipolar recoupling with adiabatic inversion pulses.

A numerical assessment of the efficacy of REDOR recoupling of heteronuclear dipolar interactions employing adiabatic dephasing pulses has been carried out by considering an isolated dipolar coupled spin 1/2 I-S system. At moderate magic angle spinning frequencies in the range of 3-6 kHz and when the CSA of the dephased spins is large, it is shown that efficient broadband heteronuclear dipolar recoupling and reliable distance estimates can be achieved even under conditions where a significant fraction of the rotor period is occupied by the adiabatic pulse. The efficacy of REDOR with adiabatic inversion pulses has been demonstrated experimentally in two model 15N-13C spin systems, (13C',15N) Aib-(15N) Aib-NH2 (Aib = alpha-aminoisobutyric acid) and (1-13C,15N) glycine.