2-DIMENSIONAL DEUTERIUM MAGIC-ANGLE-SPINNING NUCLEAR-MAGNETIC-RESONANCE OF PARAMAGNETIC COMPOUNDS - SEPARATION OF PARAMAGNETIC AND QUADRUPOLE INTERACTIONS

Citation
Tp. Spaniol et al., 2-DIMENSIONAL DEUTERIUM MAGIC-ANGLE-SPINNING NUCLEAR-MAGNETIC-RESONANCE OF PARAMAGNETIC COMPOUNDS - SEPARATION OF PARAMAGNETIC AND QUADRUPOLE INTERACTIONS, The Journal of chemical physics, 106(13), 1997, pp. 5393-5405
Citations number
56
Categorie Soggetti
Physics, Atomic, Molecular & Chemical
ISSN journal
00219606
Volume
106
Issue
13
Year of publication
1997
Pages
5393 - 5405
Database
ISI
SICI code
0021-9606(1997)106:13<5393:2DMN>2.0.ZU;2-T
Abstract
A new two-dimensional H-2 magic-angle-spinning NMR experiment to study paramagnetic compounds is presented. It can be carried out by the two -pulse sequence (90 degrees)-(t(1))-(180 degrees) -(t(2), acquisition) or the three-pulse sequence (90 degrees)-(t(1))-(54.7 degrees)-(tau)- (125.3 degrees)-(t(2), acquisition). The latter has the advantages ove r the former in that pure-absorption spectra can be obtained, and also finite pulse-width effects are less apparent. The intensities of the two-dimensionally spread sidebands are calculated as a function of the paramagnetic and the quadrupole coupling parameters, the time-evoluti on of the spin system during the rf pulse being involved. The method i s applied to paramagnetic coordination compounds with selectively deut erated acetate groups: Mn2O(O2CCD3)(2){(C3H3N2)(2)BH}(2) and Pr(O2CCD3 )(3) . H2O. The principal values of the two interaction tensors can be separately estimated from the projections of the two-dimensional spec trum onto the corresponding diagonals. These values are further refine d by simulations of the two-dimensional spinning sideband pattern, whi ch also allows us to determine the mutual orientation of the two tenso rs. The paramagnetic shift tensors are calculated on the basis of the crystal structures and are compared with those obtained by the experim ents. The effect of the bulk magnetic susceptibility on the observed p aramagnetic shift tensor is discussed. Some methods to remove this eff ect are suggested. (C) 1997 American Institute of Physics.