[1] Jiang X, Rodriguez-Molina B, Nazarian N, et al. Rotation of a bulky triptycene in the solid state: toward engineered nanoscale artificial molecular machines[J]. J Am Chem Soc, 2014, 136: 8 871-8 874.[2] Walaszek B, Adamczyk A, Pery T, et al. 2H solid-state NMR of ruthenium complexes[J]. J Am Chem Soc, 2008, 130: 17 502-17 508.[3] Tardy-Laporte C, Arnold A A, Genard B, et al. A 2H solid-state NMR study of the effect of antimicrobial agents on intact Escherichia coli without mutating[J]. Biochim Biophys Acta, 2013, 1828: 614-622.[4] Heaton N J, Vold R R, Vold R L. Deuterium quadrupole-echo NMR spectroscopy. IV. Inversion of full width deuterium powder patterns[J]. J Magn Reson, 1988, 77(1 969): 572-576.[5] Greenfield M S, Ronemus A D, Vold R L, et al. Deuterium quadrupole-echo NMR spectroscopy. III. Practical aspects of lineshape calculations for multiaxis rotational processes[J]. J Magn Reson, 1987, 72(1 969): 89-107.[6] Barbara T M, Greenfield M S, Vold R L, et al. Deuterium quadrupole echo NMR spectroscopy. I. Effects of chemical exchange during single and composite pulses[J]. J Magn Reson, 1986, 69(1 969): 311-330.[7] Ronemus A D, Vold R L, Vold R R. Deuterium quadrupole echo NMR spectroscopy II. Artifact suppression[J]. J Magn Reson, 1986, 70(1 969): 416-426.[8] Iijima T, Shimizu T, Nishimura K. 2H NMR pure-quadrupole spectra for paramagnetic solids[J]. J Magn Reson, 2015, 251: 57-64.[9] Sun C, Boutis G S. Simulation studies of instrumental artifacts on spin I = 1 double quantum filtered NMR spectroscopy[J]. J Magn Reson, 2010, 205: 102-108.[10] Rosal I d, Gutmann T, Maron L, et al. DFT 2H quadrupolar coupling constants of ruthenium complexes: a good probe of the coordination of hydrides in conjuction with experiments[J]. Phys Chem Chem Phys, 2009, 11: 5 657-5 663.[11] Michal C A, Wehman J C, Jelinski L W. Deuterium quadrupole-coupling and chemical-shielding tensors in the model dipeptide glycylglycine monohydrochloride monohydrate[J]. J Magn Reson (Series B), 1996, 111: 31-39.[12] Shen M, Roopchand R, Mananga E N S, et al. Revisiting NMR composite pulses for broadband 2H excitation[J]. Solid State Nucl Magn Reson, 2015, 66–67: 45-48.[13] Mananga E S, Rumala Y S, Boutis G S. Finite pulse width artifact suppression in spin-1 quadrupolar echo spectra by phase cycling[J]. J Magn Reson, 2006, 181: 296-303.[14] Haeberlen U, Waugh J S. Coherent averaging effects in magnetic resonance[J]. Phys Rev, 1968, 175: 453-467.[15] Vega S, Pines A. Operator formalism for double quantum NMR[J]. J Chem Phys, 1977, 66: 5 624.[16] Bak M, Rasmussen J T, Nielsen N C. SIMPSON: A general simulation program for solid-state NMR spectroscopy[J]. J Magn Reson, 2000, 147: 296-330. [17] Alderman D W, Solum M S, Grant D M. Methods for analyzing spectroscopic line shapes. NMR solid powder patterns[J]. J Chem Phys, 1986, 84: 3 717.[18] Siminovitch D J, Raleigh D P, Olejniczak E T, et al. Composite pulse excitation in quadrupole echo spectroscopy[J]. J Chem Phys, 1986, 84: 2 556.[19] Bain A D, Dumont R S. Introduction to Floquet theory: The calculation of spinning sideband intensities in magic-angle spinning NMR[J]. Concept Magn Reson, 2001, 13: 159-170. |