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Spectroscopies and simulations to understand materials properties
NMR and simulations of NMR spectra version française

 

People involved in the subject:
Florent BOUCHER (CR), Nicolas DUPRE (CR), Christophe PAYEN (Pr), Michaël PARIS (IR), Lionel TRUFLANDIER (Thèse 2007)

Overview

In the field of materials science, it is of paramount importance to achieve a chemical and structural characterization as complete as possible before studying the evolution of physico-chemical properties as functions of various parameters such as composition, temperature, pressure, oxidation state. XRD is the reference tool that comes to mind for structural characterization. However, when crystalline domains shrink (nanomaterials) or in the case of disordered materials (batteries materials), limitations are reached as far as this technique is concerned. It becomes then very interesting to use local or selective probes such as XAS, EELS, RAMAN, IR or NMR. In order to widen its range of characterization methods, IMN acquired few years back a 500 MHz Bruker NMR spectrometer and MAS probes. This spectroscopy is an extremely selective probe, very sensitive to the evolutions of atomic local environments: site distortions, changes in bonds length, evolution of the iono-covalent character of interatomic forces. Moreover, thanks to its local character, solid state NMR can be applied to crystallized materials as well as glasses or amorphous compounds.
Still, NMR spectra interpretation is a delicate step and, in numerous cases, the assignments of resonances cannot be done without the help of simulation methods. By setting tools allowing the simulation of NMR parameters, our aim is to contribute to the development of this technique and to shed light on the complementarity simulation/NMR experiment.
Prior to the work done by Pickard and Mauri [1] who introduced the GIPAW (Gauge-Including Projector Augmented-Wave) approach, NMR parameters simulation on periodic systems was performed using "clusters" approach, inappropriate for an meaningful description of solids. The GIPAW concept, now implemented in the NMR CASTEP code, permits this type of simulations for complex compounds with several hundreds of atoms per lattice. Nevertheless, up to now, no GIPAW simulation had been reported for transition metals of the first period, such as titanium or vanadium, interesting for various applications: pigments, catalysis, photovoltaic, lithium batteries electrode...Thus it seemed important to validate the GIPAW approach for transition metals. Within the Ph.D research project carried by Lionel Truflandier (2004/2007), we focused on the simulation of 51V NMR parameters, namely chemical shift anisotropy (CSA) and electrical field gradient (EFG) tensors.

  • (1) C. J. Pickard and F. Mauri Phys. Rev. B (2001), 63, 245101

 

Results

The first studies introducing chemical shift calculations for 3d metals using the GIPAW method have just been published on the AlVO4 compound, giving new insights on its structure. Recent EFG calculations performed on this compound allowed the assignments of the NMR resonances to the three distinct vanadium sites found in the structure. Moreover, our work, yielding CSA tensor parameters, permitted first, to confirm this attribution and second, to obtain accurate values of Euler angles describing the relative orientation of the two CSA and EFG tensors.

L. Truflandier, M. Paris, C. Payen and F. Boucher J. Phys. Chem. B (2006), 110, 21403-21407.

 

 

Figure 1: Experimental and theoretical eigenvalues obtained by the GIPAW method for the CSA tensor of the three vanadium sites in AlVO4

 

 

 

 

 

 

 

 

 

 

 

 

Figure 2 Correlation between isotropic values of the shielding tensor and the chemical shift for different 51V sites found in numerous molecular extended systems.

 

 

Before the finalization of these first studies, a comprehensive work was however, necessary from the building of an efficient pseudo-potential for the vanadium atom to its validation in the case of chemical shift calculation and finally to its application on numerous molecular extended systems. This body of work can be found in PRB (ref http://link.aps.org/abstract/PRB/v76/e035102). We show that it is possible to predict the isotropic chemical shift for 51V with an error margin within 30 ppm for a chemical shift range wider than 800 ppm. Concerning the assignment of vanadium resonances in a particular structure, acceptable error margins would have to be narrowed, with an order of magnitude smaller than 10 ppm.
Based on these results, we started a collaboration with Nathalie Steunou et Christian Bonhomme (Université Pierre et Marie Curie, Paris) aiming at guiding the analysis of complex NMR spectra acquired for some of their compounds. We focused in particular, on Cs4(H2V10O28),4H2O displaying 5 distinct vanadium sites with very similar chemical shifts. Since this compound is used as a precursor in sol-gel syntheses of functionalized materials, it was of paramount importance to gather information on the alkalinity and then the reactivity of the different anionic sites within the structure. The attribution of the 51V resonances permitted to make progress in this direction. By coupling geometry optimization based on DFT and chemical shifts calculations based on the GIPAW method, we are able to propose a complete and accurate crystallographic structure including well defined protons positions. It is now also possible to assign, without any doubt, the five observed NMR resonances to the five non-equivalent vanadium crystallographic sites, thanks to the accurate calculations of the EFG and CSA tensors parameters. These results will be soon submitted for publication.

Our attention was also held by the family of the VOPO4 compounds, studied during the Ph.D work of Maxence Launay, in which several phases display structural ambiguities: polymorphism problems, metastability, stacking faults. MAS NMR coupled with simulation should allow to shed light on some of these unsolved problems. This is a work in progress.

Publications

1- L. Truflandier, M. Paris, C. Payen and F. Boucher J. Phys. Chem. B (2006), 110, 21403-21407

2- L. Truflandier, M. Paris, and F. Boucher :Phys. Rev. B 76, 035102 (2007)

 

 
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Updated on spetember, 20th 2007