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In situ study of the crystal symmetry changes in lithium titanate spinel by X-ray diffraction and Raman spectroscopy

Natasa Jovic 1Milica Vucinic-Vasic 2Bratislav Antic 1Aleksandar Kremenovic 3Volker Kahlenberg 4

1. VINCA Institute, POB 522, Belgrade 11001, Serbia
2. Faculty of Technical Sciences, University of Novi Sad, Trg D. Obradovica 6, Novi Sad 21000, Serbia
3. Faculty of Mining and Geology, Laboratory for Crystallography, University of Belgrade, Djusina 7, Belgrade 11000, Serbia
4. Institute of Mineralogy and Petrography, University of Innsbruck, Innrain 52, Innsbruck A-6020, Austria

Abstract

Li1.33Ti1.67O4 spinel exhibits a special interest as negative electrode material. The effect on electrochemistry by a partial substitution of lithium and/or titanium ions with transition metal ions has been studied. In the present work we have investigated the microstructure and crystal structure evolution of LiZn0.5Ti1.5O4 obtained by high energy ball milling from an appropriate mixture of Li2CO3, ZnO and TiO2 powders. For as-synthesized material the powder X-ray diffraction pattern confirms disordered spinel structure (Fd -3m). Determined cation distribution, (Li0.28Zn0.19Ti0.53)[Li0.72Zn0.31Ti0.97], is in discrepancy with the known cation site preferences and can be classified as metastable one. Microstructural size-strain analysis has been done using the FullProf computer program. The average apparent size of sample was found to be 187(12) Å, and the average apparent strain is 26(4) 10-4. After annealing sample at 650 °C for 3 hours and slowly cooling down to room temperature, the superstructure reflections have been observed, indicating cation ordering at octahedral, (Oh) sublattice (P4332). The order-disorder phase transition in the annealed sample was studied by in-situ XRD experiment. The extinction of superstructure reflections was observed between 1020 °C and 1040 °C. Disorder began with the cation migration of Li+ and Zn2+ ions between the tetrahedral, 8c and octahedral, 4b sites, but the main mechanism was cation mixing inside Oh sublattice. At the temperatures higher than 1030 °C, crystal structure refinements were performed in disordered phase (Fd-3 m). The linear increase of the lattice parameter, a, with the temperature rise was observed, with discontinuity at the phase transition temperature. Landau theory of phase transition was used to analyze the mechanisms of the phase transitions. Analysis of the topology of the order parameter vector space could indicate biquadratic coupling between Q1 and Q2 parameters. In the temperature stability range of the ordered phase (P4332), there is a linear relationship between Q1 and Q2, therefore linear-quadratic coupling is not excluded. The phase transition in LiZn0.5Ti1.5O4 spinel has also been studied by Raman spectroscopy. Raman spectra were recorded between 500 and 1200 ºC in heating and cooling, as well as at room temperature (RT) before and after thermal treatment. Raman spectra recorded at RT shows a presence of more than five Raman mode of vibrations, as a consequence of 1:3 ordering at Oh sublattice.

 

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Related papers

Presentation: Poster at 11th European Powder Diffraction Conference, Poster session, by Natasa Jovic
See On-line Journal of 11th European Powder Diffraction Conference

Submitted: 2008-04-20 16:42
Revised:   2009-06-07 00:48