Electric-field-induced phase transformation at a lead-free morphotropic phase boundary: Case study in a 93%(Bi0.5Na0.5)TiO3–7% BaTiO3 piezoelectric ceramic

The electric-field-induced strain in 93%(Bi0.5Na0.5)TiO3–7%BaTiO3 polycrystalline ceramic is shown to be the result of an electric-field-induced phase transformation from a pseudocubic to tetragonal symmetry. High-energy x-ray diffraction is used to illustrate the microstructural nature of the transformation. A combination of induced unit cell volumetric changes, domain texture, and anisotropic lattice strains are responsible for the observed macroscopic strain. This strain mechanism is not analogous to the high electric-field-induced strains observed in lead-based morphotropic phase boundary systems. Thus, systems which appear cubic under zero field should not be excluded from the search for lead-free piezoelectric compositions.

[1]  Tadashi Takenaka,et al.  (Bi1/2Na1/2)TiO3-BaTiO3 System for Lead-Free Piezoelectric Ceramics , 1991 .

[2]  M. Drakopoulos,et al.  High-energy X-ray diffraction using the Pixium 4700 flat-panel detector. , 2009, Journal of synchrotron radiation.

[3]  Qing Xu,et al.  Structure and electrical properties of (Na0.5Bi0.5)1−xBaxTiO3 piezoelectric ceramics , 2008 .

[4]  W. Jo,et al.  Acoustic emission study of domain wall motion and phase transition in (1 − x − y)Bi0.5Na0.5TiO3–xBaTiO3–yK0.5Na0.5NbO3 lead-free piezoceramics , 2009 .

[5]  W. Jo,et al.  Perspective on the Development of Lead‐free Piezoceramics , 2009 .

[6]  Yu U. Wang Diffraction theory of nanotwin superlattices with low symmetry phase: Application to rhombohedral nanotwins and monoclinic M{sub A} and M{sub B} phases , 2007 .

[7]  Dragan Damjanovic Contributions to the Piezoelectric Effect in Ferroelectric Single Crystals and Ceramics , 2005 .

[8]  Jacob L. Jones,et al.  Domain texture distributions in tetragonal lead zirconate titanate by x-ray and neutron diffraction , 2005 .

[9]  J. Daniels Determination of directionally dependent structural and microstructural information using high-energy X-ray diffraction , 2008 .

[10]  Jacob L. Jones,et al.  High-throughput evaluation of domain switching in piezoelectric ceramics and application to PbZr0.6Ti0.4O3 doped with La and Fe , 2008 .

[11]  G. Rossetti,et al.  Ferroelectric solid solutions with morphotropic boundaries: Vanishing polarization anisotropy, adaptive, polar glass, and two-phase states , 2008 .

[12]  A. Steuwer,et al.  Texture of poled tetragonal PZT detected by synchrotron X-ray diffraction and micromechanics analysis , 2005 .

[13]  R. Ranjan,et al.  Structure and dielectric properties of (Na0.50Bi0.50)1 -xBaxTiO3 : 0≤x≤0.10 , 2005 .

[14]  H. Kungl,et al.  Nanodomain structure of Pb[Zr 1-x Ti x ]O 3 at its morphotropic phase boundary: Investigations from local to average structure , 2007 .

[15]  Hajime Nagata,et al.  Phase diagrams and electrical properties of (Bi1/2Na1/2)TiO3-based solid solutions , 2008 .

[16]  Chuin-Shan Chen,et al.  Switching characteristics of MPB compositions of (Bi0.5Na0.5)TiO3–BaTiO3–(Bi0.5K0.5)TiO3 lead-free ferroelectric ceramics , 2007 .

[17]  C. Tai,et al.  Influence of short-range and long-range order on the evolution of the morphotropic phase boundary in Pb Zr[sub 1−x]Ti[sub x] O₃ , 2004 .

[18]  Q. Yin,et al.  Electrical properties of Na1/2Bi1/2TiO3–BaTiO3 ceramics , 2002 .