Bulletin of the American Physical Society
APS March Meeting 2018
Volume 63, Number 1
Monday–Friday, March 5–9, 2018; Los Angeles, California
Session C09: Dielectric and Ferroic Oxides - Elastic Phenomena
2:30 PM–5:54 PM,
Monday, March 5, 2018
LACC
Room: 301A
Sponsoring
Unit:
DMP
Chair: Muhtar Ahart, Carnegie Institute of Washington
Abstract ID: BAPS.2018.MAR.C09.10
Abstract: C09.00010 : Macroscopic polarization in ferroelastic SrTiO3 via gradient-mediated couplings*
5:06 PM–5:18 PM
Presenter:
Andrea Schiaffino
(Institut de Ciència de Materials de Barcelona (ICMAB-CSIC))
Authors:
Andrea Schiaffino
(Institut de Ciència de Materials de Barcelona (ICMAB-CSIC))
Massimiliano Stengel
(ICREA-Institució Catalana de Recerca i Estudis Avançats)
the polarity of ferroelastic twin boundaries (TBs) in tetragonal SrTiO3.
We carry out our investigation by using a new multiscale approach that starts from
the first-principles results, and uses them in order to build an effective
continuum Hamiltonian by taking the long-wavelength limit of the
relevant lattice-dynamical data.
Such a methodology has allowed us to identify three main gradient-mediated
mechanisms for polarity:
(i) flexoelectricity, which originates from the strain gradient at the TB;
(ii) a "rotopolar" coupling, which comes directly from the gradients of the
octahedral tilts;
(iii) a previously overlooked tri-linear coupling, which is mediated
by an antiferroelectric displacement of the Ti atoms.
Remarkably, the rotopolar coupling bears a strong analogy with the
mechanism that generates a polarization in cycloidal magnets, thereby
allowing for a macroscopic breakdown of inversion symmetry even in a
periodic sequence of parallel twins.
*MINECO-Spain Grants No. FIS2013-48668-C2-2-P, No. MAT2016-77100-C2-2-P, and No. SEV-2015-0496;
Generalitat de Catalunya Grant No. 2014 SGR301;
European Research Council (ERC) Grant Agreement No. 724529;
Supercomputing Center of Galicia (CESGA)
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.MAR.C09.10
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