Ab initio atomistic description of temperature-induced phase changes: The cases of zirconia and Ti-Y-co-doped zirconia

• Autores: Negreiros Ribeiro, Fábio; Ribeiro Ricci Lazar, Dolores; Ussui, Valter; De Lima, Nelson Batista; Marchi, Juliana; Dalpian, Gustavo Martini
• Año de publicación: 2021
• Idioma: inglés
• Tipo de recurso: artículo
• Materia: DFT; Zirconia; Phase-Changes
• Institución: Consejo Nacional de Investigaciones Científicas y Técnicas

Zirconium dioxide, or zirconia, is a common and useful ceramic with a wide range of applications, from fuel cells to odontology. Its phase diagram is simple and well understood, having a structure which is monoclinic at temperatures up to 1500 K, tetragonal up to 2700 K and cubic up to 3000 K. Zirconia is rarely used in its pure form, being typically doped with Y2O3, MgO or TiO2, and in this regime its phase diagram becomes much more complex. In this context, ab initio molecular dynamics (AIMD) can provide a detailed atomistic description of the phase diagram of this system, accurately describing its stable phases and transition regions. In this work, 3 mol-% Y2O3 (3YSZ) crystals doped with different Ti contents were studied at the density-functional level. For Ti contents varying from 0 to 30 at%, a global search algorithm was first used to explore the 0 K potential-energy surface and determine the most stable sites for the added Ti atoms. It was found that, at low Ti compositions XTi, small TiO2 clusters form, followed by TiO2 channels and infinite TiO2 planes at larger XTi values, and that the highest stability is achieved at 9% Ti. AIMD simulations within the isothermal-isobaric NPT ensemble were then performed to characterize the temperature-dependent phase changes as a function of the Ti content, where it was found that the Ti-doped structures presented considerably smaller volume changes near the phase-change critical temperatures. These findings suggest that YSZ materials doped with a small amount of Ti are both energetically and kinetically more stable than the undoped counterparts, in the ideal proportion of 3% TiO2 for every 1% Y2O3 doping.
Fil: Negreiros Ribeiro, Fábio. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Córdoba. Instituto de Investigaciones en Físico-química de Córdoba. Universidad Nacional de Córdoba. Facultad de Ciencias Químicas. Instituto de Investigaciones en Físico-química de Córdoba; Argentina
Fil: Ribeiro Ricci Lazar, Dolores. Comissao Nacional de Energia Nuclear. Centro de Lasers e Aplicacoes. Instituto de Pesquisas Energéticas e Nucleares; Brasil
Fil: Ussui, Valter. Comissao Nacional de Energia Nuclear. Centro de Lasers e Aplicacoes. Instituto de Pesquisas Energéticas e Nucleares; Brasil
Fil: De Lima, Nelson Batista. Comissao Nacional de Energia Nuclear. Centro de Lasers e Aplicacoes. Instituto de Pesquisas Energéticas e Nucleares; Brasil
Fil: Marchi, Juliana. Universidad Federal do Abc; Brasil
Fil: Dalpian, Gustavo Martini. Universidad Federal do Abc; Brasil