The Origin of Ferroelectricity in Hf$_{x}$ Zr$_{1-x}$ O$_2$: A Computational Investigation and a Surface Energy Model

Robin Materlik; Christopher Künneth; Alfred Kersch

doi:10.1063/1.4916707

paper

The Origin of Ferroelectricity in Hf $_{x}$ Zr $_{1 - x}$ O $_{2}$ : A Computational Investigation and a Surface Energy Model

arXiv:1507.00588 · doi:10.1063/1.4916707

Abstract

The structural, thermal, and dielectric properties of the ferroelectric phase of HfO $_{2}$ , ZrO $_{2}$ and Hf $_{0.5}$ Zr $_{0.5}$ O $_{2}$ (HZO) are investigated with carefully validated density functional computations. We find, that the free bulk energy of the ferroelectric orthorhombic Pca2 $_{1}$ phase is unfavorable compared to the monoclinic P2 $_{1}$ /c and the orthorhombic Pbca phase for all investigated stoichiometries in the Hf $_{χ}$ Zr $_{1 - χ}$ O $_{2}$ system. To explain the existence of the ferroelectric phase in nanoscale thin films we explore the Gibbs / Helmholtz free energies as a function of stress and film strain and find them unlikely to become minimal in HZO films for technological relevant conditions. To assess the contribution of surface energy to the phase stability we parameterize a model, interpolating between existing data, and find the Helmholtz free energy of ferroelectric grains minimal for a range of size and stoichiometry. From the model we predict undoped HfO $_{2}$ to be ferroelectric for a grain size of about 4 nm and epitaxial HZO below 5 nm. Furthermore we calculate the strength of an applied electric field necessary to cause the antiferroelectric phase transformation in ZrO $_{2}$ from the P4 $_{2}$ /nmc phase as 1 MV/cm in agreement with experimental data, explaining the mechanism of field induced phase transformation.

The Origin of Ferroelectricity in Hf $_{x}$ Zr $_{1 - x}$ O $_{2}$ : A Computational Investigation and a Surface Energy Model

Abstract

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The Origin of Ferroelectricity in Hf $_{x}$ Zr $_{1 - x}$ O $_{2}$ : A Computational Investigation and a Surface Energy Model