Abstract

The origin of the ferroelectricity in HfO 2 is considered to be the formation of the non-centrosymmetric polar orthorhombic phase. The double-well energy landscape as a function of the polarization for orthorhombic HfO 2 is obtained using density functional computations. Our calculation shows that the orthorhombic HfO 2 has the remnant polarization of $66.25 \mu \mathrm{C}$ cm $^{-2}$ and a barrier height of 77.4 meV atom $^{-1}$ for polarization switching. Two methods (doping with Zr and applying biaxial strain) are theoretically investigated to adjust the ferroelectricity of the orthorhombic HfO 2 . Moreover, both single- and double-domain HfO 2 structures are calculated and discussed in this work. We found the ferroelectricity of HfO 2 could be stabilized under tensile strain.

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