Thermodynamics of oxygen defective TiO2-x : The Magneli phases.

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Presentation transcript:

Thermodynamics of oxygen defective TiO2-x : The Magneli phases. Leandro Liborio Giuseppe Mallia Nicholas Harrison Computational Materials Science Group

Magneli Phases TnO2n-1 composition, .Oxygen defects in {121} planes. Figure 1a Figure 1b TnO2n-1 composition, .Oxygen defects in {121} planes. Ti4O7 at T<154K insulator with 0.29eV band gap(1). T4O7 Metal-insulator transition at 154K, with sharp decrease of the magnetic susceptibility. (3) P. Waldner and G. Eriksson, Calphad Vol. 23, No. 2, pp. 189-218, 1999. ( 2) W. Masayuki et al., J. of Luminiscence, Vol. 122-123, pp. 393-395, 2007. (1) K. Kobayashi et al., Europhysics Lett., Vol. 59, pp. 868-874, 2002.

Magneli Phases: T4O7 crystalline structure Figure 3a Figure 3b Figure 3c Rutile unit cell View along the a lattice parameter View of Hexagonal oxygen arrangement Figure 3e Figure 3d View of Hexagonal oxygen network Metal nets in antiphase. (121)r Cristallographic shear plane.

Technical details of the calculations CASTEP CRYSTAL Local density functional: LDA Ultrasoft pseudopotentials replacing core electrons Plane waves code Supercell approach Simulated systems: Oxygen point-defective supercell, Magneli phases supercells, Titanium bulk metal. Hybrid density functional: B3LYP, GGA Exchange GGA Correlation 20% Exact Exchange All electron code. No pseudopotentials Local basis functions: atom centred Gaussian type functions. Ti: 27 atomic orbitals, O: 18 atomic orbitals Supercell approach Simulated systems: Oxygen point-defective supercell, Magneli phases supercells, Oxygen molecule.

Defect Formation Energies: Thermodynamical Formalism Figure 5a TiO2 bulk T, pO2 Initial state nDef oxygen atoms TiO2-x or TinO2n-1 + Final state Phonon contribution pV contribution

Defect Formation Energies: Oxygen chemical potential Limits for the oxygen chemical potential: Hard limit Soft limit Assuming the oxygen behaves as an ideal gas: Oxygen molecule’s total energy at 0K Oxygen molecule’s standard chemical potential at T=298K and pO2=1atm Expression (5) allows the calculation of 0O2(T,pO2) at any T and pO2

Oxygen chemical potential CASTEP CRYSTAL E0 and the 0K total energy of the oxygen atom are calculated with CRYSTAL. MxOy: ZnO, Anatase, Rutile, Ti4O7, Ti3O5 Exp. PW-GGA (4) CRYSTAL Binding energy [eV] 2.56 3.6 2.53 Bond length [ang] 1.21 1.22 1.23 0O2(T0, p0O2)= mean +/-  Now E0 has to be calculated Now 0O2 has to be calculated T>298K and pO2=1atm T>0K and any pO2 (4) W. Li et al., PRB, Vol. 65, pp. 075407-075419, 2002.

Results for the Magneli phases Figure 8a Isolated defects Magneli phases Figure 8b

Results for the Magneli phases 1 2 Equilibrium point 1: Equilibrium point 2: Relationship between pO2 and T in the phase equilibrium.

Results for the Magneli phases Figure 10a 1 2 3 1 2 3 Ti3O5 Ti4O7 Ti5O9 Figure 10b Forbidden region (1) P. Waldner and G. Eriksson, Calphad Vol. 23, No. 2, pp. 189-218, 1999.

CASTEP Results for the Magneli phases Figure 10a Figure 10b Figure 10c Figure 10d Forbidden region Forbidden region (1) P. Waldner and G. Eriksson, Calphad Vol. 23, No. 2, pp. 189-218, 1999.

CRYSTAL Results for the Magneli phases Figure 12a Figure 12b Figure 12c P. Waldner and G. Eriksson, Calphad Vol. 23, No. 2, pp. 189-218, 1999.

Formation mechanism for an oxygen-defective plane Cation + anion (100) layer Ti L. Bursill and B. Hyde, Prog. Sol. State Chem. Vol. 7, pp. 177, 1972. S. Andersson and A. D. Waldsey, Nature Vol. 211, pp. 581, 1966.

Formation mechanism for an oxygen-defective plane Final stages a) d) c) b) e) f) Antiphase boundaries (dislocation) acts as high conductivity paths for titanium. Dislocations are needed No long-range diffusion Formation of Ti interstitials.

Conclusions The thermodynamics of rutile’s higher oxides has been investigated by first principles calculations. First principles thermodynamics reproduce the experimental observations reasonably well. Spin does not affect the thermodynamics. At a high concentration of oxygen defects and low oxygen chemical potential, oxygen defects prefer to form Magneli phases. But, at low concentration of oxygen defects and low oxygen chemical potential, titanium interstitials proved to be the stable point defects. These results support the mechanism proposed by Andersson and Waldsey for the production the crystalline shear planes in rutile.

Prof. Nic Harrison Dr. Giuseppe Mallia Dr. Barbara Montanari Acknowledgements Prof. Nic Harrison Dr. Giuseppe Mallia Dr. Barbara Montanari Dr Keith Refson