APS March Meeting 2011
Volume 56, Number 1
Monday–Friday, March 21–25, 2011;
Dallas, Texas
Session L33: Focus Session: Dielectric, Ferroelectric, and Piezoelectric Oxides: Lattice Dynamics, Polarons, and Structure
2:30 PM–5:30 PM,
Tuesday, March 22, 2011
Room: C143/149
Sponsoring
Units:
DMP DCOMP
Chair: Matt Dawber, Stony Brook University
Abstract ID: BAPS.2011.MAR.L33.7
Abstract: L33.00007 : A Neutron Study of the Structure and Lattice Dynamics of Single Crystal PZT
3:42 PM–4:18 PM
Preview Abstract
Abstract
Author:
Peter Gehring
(National Institute of Standards and Technology)
The outstanding piezoelectric properties of
PbZr$_{1-x}$Ti$_{x}$O$_{3}$
(PZT) perovskite ceramics have long been exploited in numerous
device
applications, making PZT arguably the most technologically important
ferroelectric material in use today. Efforts to understand the
piezoelectric
mechanism have inspired a plethora of structural studies spanning
decades,
but solving the PZT phase diagram has proven to be famously
problematic
because single crystals have not been available save for Zr- and
Ti-rich
compositions that lie very near the end members PbZrO$_{3}$ and
PbTiO$_{3}$,
where the piezoelectricity is weakest. Thus, whereas PZT has been
the
subject of thousands of powder and ceramic investigations, no
consensus
regarding the crystal structures of PZT exists. We report the
first neutron
diffraction study of single-crystal PZT with compositions x =
0.325 and
0.460 [1]. Our data refute the thesis that the ferroelectric
phases of PZT
within this composition range, all of which are highly
piezoelectric, are
purely monoclinic (Cc or Cm). The broadening of certain Bragg
peaks can be
interpreted in terms of coexisting rhombohedral and monoclinic
domains,
whereby monoclinic order is enhanced by Ti-doping. This is
consistent with
the theoretical proposal that the tendency to form macroscopic
monoclinic
phases facilitates the mechanism of polarization rotation by
reducing the
energy required to reorient the electric polarization.
Dispersions of the
lowest energy TO and TA phonon modes were measured on a single
crystal of
PZT with x = 0.325 in the paraelectric phase at 650 K [2]. The TO
mode
energy drops at small wave-vectors suggesting that it is a soft mode
associated with the ferroelectric phase transition at 590 K.
Evidence of a
second soft-mode, corresponding to a phase transition at 370 K at
the
R-point, is provided based on the redistribution of spectral
weight as a
function of temperature.
\\[4pt]
[1] D. Phelan \textit{et al}., Phys. Rev. Lett. \textbf{105},
207601 (2010).
\\[0pt]
[2] D. Phelan \textit{et al}., submitted.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2011.MAR.L33.7