APS March Meeting 2015
Volume 60, Number 1
Monday–Friday, March 2–6, 2015;
San Antonio, Texas
Session Q13: Focus Session: Complex Oxide Interfaces - LaAlO3/SrTiO3 II
2:30 PM–5:30 PM,
Wednesday, March 4, 2015
Room: 007D
Sponsoring
Unit:
DMP
Chair: Sohraib Ismail-Beigi, Yale University
Abstract ID: BAPS.2015.MAR.Q13.1
Abstract: Q13.00001 : Combining Mott insulators and ferroelectrics
2:30 PM–3:06 PM
Preview Abstract
Abstract
Author:
Agn`es Barthelemy
(Unit\'e Mixte de Physique CNRS/Thales)
We investigated the properties of high quality heterostructures consisting
of a Mott insulator, (Ca,Ce)MnO$_{3}$ (CCMO) and a
ferroelectric, BiFeO$_{3}$ in the supertetragonal phase (T-BFO)
materials. In particular, we studied the electrical response induced by
ferroelectric switching in both planar and vertical devices.
In the planar geometry, we used thick T-BFO films to explore the possibility
to electrically tune the properties of the CCMO compound in a ferroelectric
field-effect device with a CCMO channel and a T-BFO gate. Upon polarization
reversal of the T-BFO ferroelectric gate, the CMO channel exhibits a
nonvolatile resistance switching by a factor of 4 around room temperature,
and up to a factor of 10 at 200 K [1].
We also studied Ferroelectric tunnel junctions (FTJs) composed of an
ultrathin ferroelectric tunnel barrier of T-BFO sandwiched between a CCMO
electrode and a Co/Pt counter-electrode. In these junctions, the tunneling
current significantly depends on the orientation of the ferroelectric
polarization, resulting in large electroresistance enabling a simple
nondestructive readout of the ferroelectric state [2]. FTJs based on
ultrathin T-BFO films show fast, stable multistate switching with very high
resistance ratios of up to four orders of magnitude [3]. Combined
piezoresponse force microscopy (PFM) and electrical measurements give a
clear correlation between ferroelectric domain configurations and multiple
resistance states They also provide insights into the switching dynamics in
response to trains of nanosecond pulses. Additionnaly, we demonstrated the
very good endurance and retention characteristics of these FTJs [4].
\\[4pt]
[1] H Yamada et al., Scientific Reports 3, 2834 (214)\\[0pt]
[2] V. Garcia et al, Nature 460, 81 (2009)\\[0pt]
[3] H Yamada et al., ACS Nano 7, 53855390 (2013)\\[0pt]
[4] S. Boyn et al., Appl. Phys Lett. 104, 052909 (2014)
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2015.MAR.Q13.1