Proton assisted recoupling and protein structure determination

Abstract
We introduce a homonuclear version of third spin assisted recoupling, a second-order mechanism that can be used for polarization transfer between C13 or N15 spins in magic angle spinning (MAS) NMR experiments, particularly at high spinning frequencies employed in contemporary high field MAS experiments. The resulting sequence, which we refer to as proton assisted recoupling (PAR), relies on a cross-term between H1C13 (or H1N15 ) couplings to mediate zero quantum C13C13 (or N15N15 recoupling). In particular, using average Hamiltonian theory we derive an effective Hamiltonian for PAR and show that the transfer is mediated by trilinear terms of the form C1±C2HZ for C13C13 recoupling experiments (or N1±N2HZ for N15N15 ). We use analytical and numerical simulations to explain the structure of the PAR optimization maps and to delineate the PAR matching conditions. We also detail the PAR polarization transfer dependence with respect to the local molecular geometry and explain the observed reduction in dipolar truncation. Finally, we demonstrate the utility of PAR in structural studies of proteins with C13C13 spectra of uniformly C13 , N15 labeled microcrystalline Crh, a 85 amino acid model protein that forms a domain swapped dimer (MW=2×10.4kDa) . The spectra, which were acquired at high MAS frequencies (ωr2π>20kHz) and magnetic fields (750–900 MHz H1 frequencies) using moderate rf fields, exhibit numerous cross peaks corresponding to long (up to 67Å ) C13C13 distances which are particularly useful in protein structure determination. Using results from PAR spectra we calculate the structure of the Crh protein.