Abstract

Pb(Zr1-xTix)O3 single crystal with a low titanium content (x = 4%) was studied by the piezoresponse force microscopy (PFM) and X-ray diffraction (XRD). The XRD studies showed that the crystal faces are orthogonal to the principal cubic axes and confirmed the existence of an intermediate phase between the high-temperature paraelectric (PE) phase and the low-temperature antiferroelectric (AFE) one. A significant temperature hysteresis of phase transitions was observed by the XRD: On heating, the AFE state transforms into the intermediate one at about 373 K and the PE phase appears at 508 K, whereas on cooling the intermediate phase forms at 503 K and persists down to at least 313 K. The PFM investigation was focused on the intermediate phase and involved measurements of both out-of-plane and in-plane electromechanical responses of the (001)-oriented crystal face. The PFM images revealed the presence of polarization patterns switchable by an applied electric field, which confirms the ferroelectric character of the intermediate phase. Importantly, two types of regular domain structures were found, which differ by the spatial orientation of domain walls. The reconstruction of polarization configurations in the observed domain structures showed that one of them is a purely ferroelectric 180° structure with domain walls orthogonal to the crystal surface and parallel to one of the ⟨111⟩ pseudocubic directions. Another one is a ferroelectric-ferroelastic domain structure with the 71° walls parallel to the {101} or {011} crystallographic planes. Remarkably, this domain structure shows correlated out-of-plane and in-plane polarization reorientations after the poling with the aid of the microscope tip.

Highlights

  • The Pb(Zr1-xTix)O3 (PZT) solid solution is one of the most actively studied ferroic material systems

  • We studied PZT-4% single crystal with the dimensions 1500×300×200 μm grown by the method of alloy crystallization.[9]

  • Spatial directions of crystallographic axes were determined by X-ray diffraction (XRD) using SuperNova diffractometer (Oxford Diffraction, UK), and the crystal faces were found to be orthogonal to the principal cubic axes

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Summary

Introduction

The Pb(Zr1-xTix)O3 (PZT) solid solution is one of the most actively studied ferroic material systems. The phase diagram of PZT, first synthesized already in 1952,1 is distinguished by the presence of nearly vertical boundary between the rhombohedral and tetragonal ferroelectric phases (morphotropic phase boundary – MPB) at x ≈ 0.48.2 PZT compounds with compositions in the MPB region were the subject of intensive studies due to their exceptional piezoelectric properties useful for electromechanical applications.[3] At the same time, there is a growing interest in PZT solutions with high Zr content, which have extremely rich phase diagram comprising an antiferroelectric state characteristic of PbZrO3.4,5 This interest is driven by strongly increased attention to anitiferroelectrics,[6] motivated by their practical importance for the energy storage applications[7] resulting from favorable combination of high electric permittivity and low dielectric losses. The domain switching in applied electric fields, which is of primary importance for practical applications of FE materials, has not been investigated yet

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