Phase competition and negative piezoelectricity in interlayer-sliding ferroelectric ZrI$_2$

TL;DR

This study explores the phase competition and negative piezoelectricity in bulk ZrI$_2$, revealing tunable ferroelectric phases and the unique origin of negative piezoelectricity linked to interlayer-sliding ferroelectricity.

Contribution

It provides the first detailed analysis of phase competition and negative piezoelectricity in bulk ZrI$_2$, highlighting the role of interlayer-sliding ferroelectricity.

Findings

ZrI$_2$ has two competitive phases with different polarization characteristics.

Negative longitudinal piezoelectricity in ZrI$_2$ is mainly due to enhanced layer dipoles.

Hydrostatic pressure and uniaxial strain can tune the ground state phase.

Abstract

The so-called interlayer-sliding ferroelectricity was recently proposed as an unconventional route to pursuit electric polarity in van der Waals multi-layers, which was already experimentally confirmed in WTe$_2$ bilayer even though it is metallic. Very recently, another van der Waals system, i.e., the ZrI$_2$ bilayer, was predicted to exhibit the interlayer-sliding ferroelectricity with both in-plane and out-of-plane polarizations [Phys. Rev. B \textbf{103}, 165420 (2021)]. Here the ZrI$_2$ bulk is studied, which owns two competitive phases ($\alpha$ \textit{vs} $\beta$), both of which are derived from the common parent $s$-phase. The $\beta$-ZrI$_2$ owns a considerable out-of-plane polarization ($0.39$ $\mu$C/cm$^2$), while its in-plane component is fully compensated. Their proximate energies provide the opportunity to tune the ground state phase by moderate hydrostatic pressure and uniaxial strain. Furthermore, the negative longitudinal piezoelectricity in $\beta$-ZrI$_2$ is dominantly contributed by the enhanced dipole of ZrI$_2$ layers as a unique characteristic of interlayer-sliding ferroelectricity, which is different from many other layered ferroelectrics with negative longitudinal piezoelectricity like CuInP$_2$S$_6$.