Session P36: Focus
Session: X-ray and Neutron Instrumentation and Science
8:00 AM–10:48 AM,
Wednesday, March 12, 2008
Morial Convention Center - 228
Sponsoring Unit: GIMS
Chair: George Srajer, Argonne National Laboratory
Abstract: P36.00009 :
Identification of Mn site in Pb(Zr,Ti)O$_{3}$
10:00 AM–10:12 AM
Preview Abstract
Authors:
A. Boonchun
(School of Physics, Suranaree University of
Technology, Thailand)
M.F. Smith
(School of Physics, Suranaree University of
Technology, Thailand)
S. Rujirawat
(School of Physics, Suranaree University of
Technology, Thailand)
B. Cherdhirunkorn
(School of Physics, Suranaree University of
Technology, Thailand)
S. Limpijumnong
(School of Physics, Suranaree University of
Technology, Thailand)
The impurity Mn in
PbTiO$_{3}$ and PbZrO$_{3}$ has been studied by mean of
first-principles spin density functional theory.[1] It is found that
the Mn atom energetically prefers to substitute on the Ti/Zr site over
other sites (i.e., Pb site, O site or interstitial) under all
equilibrium growth conditions. The calculations predict that a majority
of Mn atoms substitute for Ti/Zr and have neutral-charge state each
with a total electron spin of M$_{z}$ = 3/2. This prediction is
supported by the combination of x-ray absorption near edge structure
(XANES) experiment and first-principles simulation of the spectrum. [2]
The measured XANES of the Mn-doped Pb(Ti,Zr)O$_
{3}$ within the concentration range of 0.5 - 2.0 at.\% yield the exact
same features, indicating that the location of Mn in the crystal is
independent of Mn concentration. The measured XANES is consistent with
the partial density of states simulation of Mn atom on the Ti/Zr site
and inconsistent with the simulations of Mn atom on other
sites.\newline
[1] A. Boonchun, M. F. Smith, B. Cherdhirunkorn, and S. Limpijumnong,
J. Appl. Phys. 101, 043521 (2007).
[2] S. Limpijumnong, S. Rujirawat, A. Boonchun, M.F. Smith, B.
Cherdhirunkorn, Appl. Phys. Lett. 90, 103113 (2007).