Origin of morphotropic phase boundaries in ferroelectrics

A piezoelectric material is one that generates a voltage in response to a mechanical strain (and vice versa). The most useful piezoelectric materials display a transition region in their composition phase diagrams, known as a morphotropic phase boundary, where the crystal structure changes abruptly and the electromechanical properties are maximal. As a result, modern piezoelectric materials for technological applications are usually complex, engineered, solid solutions, which complicates their manufacture as well as introducing complexity in the study of the microscopic origins of their properties. Here we show that even a pure compound, in this case lead titanate, can display a morphotropic phase boundary under pressure. The results are consistent with first-principles theoretical predictions, but show a richer phase diagram than anticipated; moreover, the predicted electromechanical coupling at the transition is larger than any known. Our results show that the high electromechanical coupling in solid solutions with lead titanate is due to tuning of the high-pressure morphotropic phase boundary in pure lead titanate to ambient pressure. We also find that complex microstructures or compositions are not necessary to obtain strong piezoelectricity. This opens the door to the possible discovery of high-performance, pure-compound electromechanical materials, which could greatly decrease costs and expand the utility of piezoelectric materials.

[1]  G. Shirane,et al.  Phase diagram of the ferroelectric relaxor (1-x)PbMg1/3Nb2/3O3-xPbTiO3 , 2002, cond-mat/0203422.

[2]  P. Bouvier,et al.  High-pressure phases in highly piezoelectric PbZr0.52Ti0.48O3 , 2003, cond-mat/0309705.

[3]  H. Mao,et al.  Energy dispersive x-ray diffraction of charge density waves via chemical filtering , 2005 .

[4]  U. V. Waghmare,et al.  Ab initio statistical mechanics of the ferroelectric phase transition in PbTiO 3 , 1997 .

[5]  R. Cohen Materials science: Relaxors go critical , 2006, Nature.

[6]  P. Bouvier,et al.  Ferroelectricity of perovskites under pressure. , 2005, Physical review letters.

[7]  David J. Singh,et al.  Interplay between A -site and B -site driven instabilities in perovskites , 2005 .

[8]  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 .

[9]  Gonzalo,et al.  Pressure dependence of free-energy expansion coefficients in PbTiO3 and BaTiO3 and tricritical-point behavior. , 1990, Physical review. B, Condensed matter.

[10]  G. Burns,et al.  High-pressure Raman study of zone-center phonons in PbTi O 3 , 1983 .

[11]  G. Shirane,et al.  Phase diagram of the relaxor ferroelectric Ñ1¿xÖPbÑZn 1'3 Nb 2'3 ÖO 3 -xPbTiO 3 , 2002 .

[12]  Guo,et al.  Origin of the high piezoelectric response in PbZr1-xTixO3 , 1999, Physical review letters.

[13]  Matthieu Verstraete,et al.  First-principles computation of material properties: the ABINIT software project , 2002 .

[14]  B. Noheda,et al.  Phase diagram of the relaxor ferroelectric (1-x)Pb(Zn1/3Nb2/3)O3-xPbTiO3 , 2002 .

[15]  V. M. Goldschmidt,et al.  Crystal structure and chemical constitution , 1929 .

[16]  Ronald E. Cohen,et al.  Polarization rotation mechanism for ultrahigh electromechanical response in single-crystal piezoelectrics , 2000, Nature.

[17]  Ronald E. Cohen,et al.  Origin of ferroelectricity in perovskite oxides , 1992, Nature.

[18]  V. Struzhkin,et al.  Raman spectroscopy of metals, high‐temperature superconductors and related materials under high pressure , 2003 .

[19]  Raymond Jeanloz,et al.  The equation of state of the gold calibration standard , 1984 .

[20]  Xavier Gonze,et al.  The ABINIT software project , 2001 .

[21]  Yu U. Wang,et al.  Microstructures of coherent phase decomposition near morphotropic phase boundary in lead zirconate titanate , 2007 .

[22]  R. Roth,et al.  Piezoelectric Properties of Lead Zirconate‐Lead Titanate Solid‐Solution Ceramics , 1954 .

[23]  G. Burns,et al.  Raman Studies of Underdamped Soft Modes in PbTi O 3 , 1970 .

[24]  H. Mao,et al.  Single-domain electromechanical constants for Pb(Zn1/3Nb2/3)O3-4.5%PbTiO3 from micro-Brillouin scattering , 2006 .

[25]  D. Viehland,et al.  Conformal miniaturization of domains with low domain-wall energy: monoclinic ferroelectric states near the morphotropic phase boundaries. , 2003, Physical review letters.

[26]  D. Vanderbilt,et al.  Monoclinic and triclinic phases in higher-order Devonshire theory , 2000, cond-mat/0009337.

[27]  G. Jennings,et al.  Diffractometer for high energy X-rays at the APS , 2000 .

[28]  Stability of the monoclinic phase in the ferroelectric perovskite PbZr1-xTixO3 , 2000, cond-mat/0006152.

[29]  Pressure-induced anomalous phase transitions and colossal enhancement of piezoelectricity in PbTiO3. , 2005, Physical review letters.