APS March Meeting 2012
Volume 57, Number 1
Monday–Friday, February 27–March 2 2012;
Boston, Massachusetts
Session D28: Focus Session: Dopants and Defects in Semiconductors - Oxides and Interfaces
2:30 PM–5:30 PM,
Monday, February 27, 2012
Room: 258C
Sponsoring
Unit:
DMP
Chair: Michael Stavola, Lehigh University
Abstract ID: BAPS.2012.MAR.D28.1
Abstract: D28.00001 : Interdiffusion, Unintentional Doping and Electronic Reconstruction at Polar/nonpolar Oxide Interfaces*
2:30 PM–3:06 PM
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Abstract
Author:
Scott Chambers
(Pacific Northwest National Laboratory)
The observation of conductivity at the interface of insulating polar and
non-polar perovskites (general form ABO$_{3})$ has sparked considerable
interest worldwide, with much of the work to date being focused on the
LaAlO$_{3}$/SrTiO$_{3}$(001) heterojunction. Many attribute the interface
conductivity to an electronic reconstruction alleviating the polar
discontinuity via a film-to-interface charge transfer. However, the
possibility of dopant- and/or defect-mediated conductivity cannot be ruled
out, especially when the interfaces are not atomically abrupt. Electronic
reconstruction requires an electric field within the film to facilitate the
charge transfer process. However, x-ray photoemission spectroscopy studies
reveal little or no electric field in the LAO film either above or below the
critical thickness for conductivity, calling into question the validity of
the electronic reconstruction model. In order to gain deeper insight into
the electronic properties, it is worthwhile to manipulate the interface by
changing the B-site cation in the polar perovskite. There are no low-lying
$d$--derived bands in LaAlO$_{3}$ Therefore, if conductivity occurs, it ought
to be driven by either the wholesale transfer of charge from the LaAlO$_{3}$
O2$p$-derived band into the STO (i.e. electronic reconstruction), or
unintentional doping and/or defect creation. By replacing Al with a
transition metal cation, we inject a new degree of freedom into the band
structure -- partially occupied $d $orbitals -- and, thus, enable other
mechanisms of charge redistribution. We have explored this concept by
placing Cr(III) at the B-site and describe the electronic properties of
epitaxial LaCrO$_{3}$/STO(001) heterojunctions. To minimize defect creation,
the films were deposited using molecular beam epitaxy (MBE), in which the
incoming atom energies are very low ($<$0.1 eV). Core-level and valence-band
x-ray photoemission spectra measured for MBE-grown
LaCrO$_{3}$/SrTiO$_{3}$(001) yield band offsets and potential gradients
within the LaCrO$_{3}$ sufficient to trigger an electronic reconstruction to
alleviate the polarity mismatch. Yet, the interface is insulating. Based on
first principles calculations, we attribute this unexpected result to
interfacial cation mixing combined with charge redistribution within
CrO$_{2}$ layers, enabled by low-lying $d$ states within LaCrO$_{3}$, which suppresses an electronic reconstruction.
*This work was supported by the U.S. Department of Energy, Office of Science, Division of Materials Sciences and Engineering under Award \#10122 (film growth) and Division of Chemical Sciences under Award \#48526 (photoemission measurements and modeling).
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2012.MAR.D28.1