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Singularities in the lineshape of a second-order perturbed quadrupolar nucleus and their use in data fitting
Affiliation:1. Department of Electrical and Computer Engineering, McMaster University, Hamilton, ON, Canada L8S 4L8;2. Department of Chemistry and Chemical Biology, McMaster University, Hamilton, ON, Canada L8S 4M1;1. Max Planck Institute for Biophysical Chemistry, Am Fassberg 11, 37077 Göttingen, Germany;2. German Center for Neurodegenerative Diseases (DZNE), Göttingen, Germany;3. Centre for Nanoscale Microscopy and Molecular Physiology of the Brain (CNMPB), Göttingen, Germany;1. Geography Section, Department of Geography and Geology, University of Turku, 20014 Turku, Finland;2. Department of Physical Geography, Stockholm University, 10691 Stockholm, Sweden;1. Univ. Grenoble Alpes, INAC, SCIB, F-38000 Grenoble, France;2. CEA, INAC, SCIB, F-38000 Grenoble, France;3. CNRS, SCIB, F-38000 Grenoble, France;1. TIFR Centre for Interdisciplinary Sciences, Tata Institute of Fundamental Research, 21 Brundavan Colony, Narsingi, Hyderabad 500 075, India;2. Department of Chemical Sciences, Tata Institute of Fundamental Research, Homi Bhabha Road, Colaba, Mumbai 400 005, India
Abstract:Even for large quadrupolar interactions, the powder spectrum of the central transition for a half-integral spin is relatively narrow, because it is unperturbed to first order. However, the second-order perturbation is still orientation dependent, so it generates a characteristic lineshape. This lineshape has both finite step discontinuities and singularities where the spectrum is infinite, in theory. The relative positions of these features are well-known and they play an important role in fitting experimental data. However, there has been relatively little discussion of how high the steps are, so we present explicit formulae for these heights. This gives a full characterization of the features in this lineshape which can lead to an analysis of the spectrum without the usual laborious powder average.The transition frequency, as a function of the orientation angles, shows critical points: maxima, minima and saddle points. The maxima and minima correspond to the step discontinuities and the saddle points generate the singularities. Near a maximum, the contours are ellipses, whose dimensions are determined by the second derivatives of the frequency with respect to the polar and azimuthal angles. The density of points is smooth as the contour levels move up and down, but then drops to zero when a maximum is passed, giving a step. The height of the step is determined by the Hessian matrix—the matrix of all partial second derivatives. The points near the poles and the saddle points require a more detailed analysis, but this can still be done analytically. The resulting formulae are then compared to numerical simulations of the lineshape.We expand this calculation to include a relatively simple case where there is chemical shielding anisotropy and use this to fit experimental 139La spectra of La2O3.
Keywords:Second-order perturbation  Quadrupolar nuclei  Powder patterns  Critical points  Line shapes
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