A general procedure for the calculation of theoretical nuclear magnetic resonance second moments in dipolar solids; application to oxalic acid dihydrate (original) (raw)
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Journal of magnetic resonance, 1979
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Chemical Physics Letters, 1997
. The use of ab initio Hartree-Fock techniques for the calculation of H quadrupole coupling constants DQCCs in hydrogen bonded molecular crystals has been assessed for the a and b polymorphs of oxalic acid dihydrate. Results demonstrate the importance of considering the full periodic structure, rather than a single molecule or a small cluster of molecules. Intramolecular contributions to the DQCCs and contributions arising from the first shell of neighbouring molecules and from outer shells are quantified. The influence of the size of basis set on the calculated DQCCs is investigated; the 6-31G ) ) basis set is found to give good agreement with experiment. Correlations between the calculated DQCCs and geometrical parameters are investigated. q 1997 Elsevier Science B.V. 14 molecules 9-11 , showing that the EFG at the N nucleus is dominated by the intramolecular contribu-0009-2614r97r$17.00 q 1997 Elsevier Science B.V. All rights reserved.
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Freezing of molecular rotation in a paramagnetic crystal studied by <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML">mml:mmultiscripts<mml:mi mathvariant="normal">P<mml:mprescripts /><mml:none />mml:mn31 NMR
Physical review, 2021
We present a detailed 31 P nuclear magnetic resonance (NMR) study of the molecular rotation in the compound [Cu(pz)2(2-HOpy)2](PF6)2, where pz = C4H4N2 and 2-HOpy = C5H4NHO. Here, a freezing of the PF6 rotation modes is revealed by several steplike increases of the temperaturedependent second spectral moment, with accompanying broad peaks of the longitudinal and transverse nuclear spin-relaxation rates. An analysis based on the Bloembergen-Purcell-Pound (BPP) theory quantifies the related activation energies as Ea/kB = 250 and 1400 K. Further, the anisotropy of the second spectral moment of the 31 P absorption line was calculated for the rigid lattice, as well as in the presence of several sets of PF6 reorientation modes, and is in excellent agreement with the experimental data. Whereas the anisotropy of the frequency shift and enhancement of nuclear spin-relaxation rates is driven by the molecular rotation with respect to the dipole fields stemming from the Cu ions, the second spectral moment is determined by the intramolecular interaction of nuclear 19 F and 31 P moments in the presence of the distinct rotation modes.