Hafnia <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi>HfO</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math> is a proper ferroelectric
Aldo Raeliarijaona, R. E. Cohen
Abstract
We clarify the nature of hafnia as a proper ferroelectric and show that there is a shallow double well involving a single soft polar mode as in well-known classic ferroelectrics. Using symmetry analysis, density functional theory structural optimizations with and without epitaxial strain, and density functional perturbation theory, we examine several important possible hafnia structures derived ultimately from the cubic fluorite structure, including baddeleyite $(P{2}_{1}/c)$, tetragonal antiferroelectric $P{4}_{2}nmc$, $Pbca$ (nonpolar and brookite), ferroelectric rhombohedral $(R3m--\mathrm{and}--R3)$, $Pmn{2}_{1}$, and $Pca{2}_{1}$ structures. The latter is considered to be the most likely ferroelectric phase seen experimentally and has an antiferroelectric parent with space group $Pbcn$, with a single unstable polar mode and a shallow double well with a well depth of 24 meV/atom. Strain is not required for switching or other ferroelectric properties, nor is coupling of the soft mode with any other modes within the ferroelectric $Pca{2}_{1}$, $Pmn{2}_{1}$, $R3m$, or $R3$ phases.