Structural phase transition and dielectric relaxation in Pb(Zn1/3Nb2/3)O3 single crystals

TL;DR

This study investigates the structural phases and dielectric relaxation behavior of Pb(Zn1/3Nb2/3)O3 single crystals, revealing phase coexistence, diffuse phase transition, and relaxor characteristics through advanced diffraction and spectroscopy techniques.

Contribution

It provides new insights into the phase coexistence and dielectric properties of PZN, comparing its relaxor behavior with Pb(Mg1/3Nb2/3)O3 and highlighting the effects of electric field and poling.

Findings

Coexistence of rhombohedral and ferroelectric phases at low temperatures.

Diffuse phase transition with no dielectric anomalies.

Frequency-dependent dielectric maximum fitting Vogel-Fulcher relation.

Abstract

The structure and the dielectric properties of Pb(Zn1/3Nb2/3)O3 (PZN) crystal have been investigated by means of high-resolution synchrotron x-ray diffraction (with an x-ray energy of 32 keV) and dielectric spectroscopy (in the frequency range of 100 Hz - 1 MHz). At high temperatures, the PZN crystal exhibits a cubic symmetry and polar nanoregions inherent to relaxor ferroelectrics are present, as evidenced by the single (222) Bragg peak and by the noticeable tails at the basis of the peak. At low temperatures, in addition to the well-known rhombohedral phase, another low-symmetry, probably ferroelectric, phase is found. The two phases coexist in the form of mesoscopic domains. The para- to ferroelectric phase transition is diffused and observed between 325 and 390 K, where the concentration of the low-temperature phases gradually increases and the cubic phase disappears upon cooling. However, no dielectric anomalies can be detected in the temperature range of diffuse phase transition. The temperature dependence of the dielectric constant show the maximum at higher temperature (Tm = 417 - 429 K, depending on frequency) with the typical relaxor dispersion at T < Tm and the frequency dependence of Tm fitted to the Vogel-Fulcher relation. Application of an electric field upon cooling from the cubic phase or poling the crystal in the ferroelectric phase gives rise to a sharp anomaly of the dielectric constant at T 390 K and diminishes greatly the dispersion at lower temperatures, but the dielectric relaxation process around Tm remains qualitatively unchanged. The results are discussed in the framework of the present models of relaxors and in comparison with the prototypical relaxor ferroelectric Pb(Mg1/3Nb2/3)O3.