Abstract

Crystalline materials with broken inversion symmetry can exhibit a spontaneous electric polarization, which originates from a microscopic electric dipole moment. Long-range polar or anti-polar order of such permanent dipoles gives rise to ferroelectricity or antiferroelectricity, respectively. However, the recently discovered antiferroelectrics of fluorite structure (HfO2 and ZrO2) are different: A non-polar phase transforms into a polar phase by spontaneous inversion symmetry breaking upon the application of an electric field. Here, we show that this structural transition in antiferroelectric ZrO2 gives rise to a negative capacitance, which is promising for overcoming the fundamental limits of energy efficiency in electronics. Our findings provide insight into the thermodynamically forbidden region of the antiferroelectric transition in ZrO2 and extend the concept of negative capacitance beyond ferroelectricity. This shows that negative capacitance is a more general phenomenon than previously thought and can be expected in a much broader range of materials exhibiting structural phase transitions.

Highlights

  • Crystalline materials with broken inversion symmetry can exhibit a spontaneous electric polarization, which originates from a microscopic electric dipole moment

  • The non-linear permittivity and capacitance of a material is proportional to (d2G/dP2)−1, which means that at the antiferroelectric transition the capacitance of the material would become negative if stabilized in a larger system[17,18]

  • Grazing incidence X-ray diffraction (GIXRD) measurement results presented in Supplementary Fig. 1 confirm that the crystalline ZrO2 layer is in the non-polar tetragonal P42/nmc phase in the as fabricated capacitors

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Summary

Introduction

Crystalline materials with broken inversion symmetry can exhibit a spontaneous electric polarization, which originates from a microscopic electric dipole moment. The current understanding of the origin of antiferroelectricity in ZrO2 is that the non-polar tetragonal P42/nmc phase undergoes a first-order structural phase transition into the polar orthorhombic Pca[21] phase by application of an electric field of around 2-3 MV cm−1 25,26.

Results
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