4.6 Article

Phase stability of TiO2 polymorphs from diffusion Quantum Monte Carlo

Journal

NEW JOURNAL OF PHYSICS
Volume 18, Issue -, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.1088/1367-2630/18/11/113049

Keywords

titanium dioxide; phase stability; finite temperature; lattice dynamics; density functional theory; electronic structure; quantum Monte Carlo

Funding

  1. Argonne Leadership Computing Facility
  2. DOE Office of Science User Facility [DE-AC02-06CH11357]
  3. Office of Science of the U.S. Department of Energy [DE-AC05-00OR22725]
  4. U.S. Department of Energy's National Nuclear Security Administration [DE-AC04-94AL85000]
  5. Predictive Theory and Modeling for Materials and Chemical Science program by the U.S. Department of Energy Office of Science, Basic Energy Sciences (BES)
  6. U.S. Department of Energy, Office of Science [DE-AC02-06CH11357]
  7. U.S Department of Energy [DE-AC05-00OR22725, DE-AC04-94AL85000]
  8. DOE Public Access Plan

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Titanium dioxide, TiO2, has multiple applications in catalysis, energy conversion and memristive devices because of its electronic structure. Most of these applications utilize the naturally existing phases: rutile, anatase and brookite. Despite the simple form of TiO2 and its wide uses, there is long-standing disagreement between theory and experiment on the energetic ordering of these phases that has never been resolved. We present the first analysis of phase stability at zero temperature using the highly accurate many-body fixed node diffusion Quantum Monte Carlo (QMC) method. We also include the effects of temperature by calculating the Helmholtz free energy including both internal energy and vibrational contributions from density functional perturbation theory based quasi harmonic phonon calculations. Our QMC calculations find that anatase is the most stable phase at zero temperature, consistent with many previous mean-field calculations. However, at elevated temperatures, rutile becomes the most stable phase. For all finite temperatures, brookite is always the least stable phase.

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