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A strong ferroelectric ferromagnet created by means of spinlattice coupling

Source: Nature 466, 954 (2010); doi:10.1038/nature09331

Issue Date: 30 August 2010

PUBLICATION DATA
ISSN:
1553-9644 (online)
Publisher:
AIP is a member of CrossRef NATURE
June Hyuk Lee
[1] Department of Materials Science and Engineering, Cornell University, Ithaca, New York 14853-1501, USA [2] Department of Materials Science and Engineering, Pennsylvania State University, University Park, Pennsylvania 16802-5005, USA

Lei Fang
[1] Department of Physics, Ohio State University, Columbus, Ohio 43210-1117, USA [2] These authors contributed equally to this work.

Eftihia Vlahos
[1] Department of Materials Science and Engineering, Pennsylvania State University, University Park, Pennsylvania 16802-5005, USA [2] These authors contributed equally to this work.

Xianglin Ke
[1] Department of Physics and Materials Research Institute, Pennsylvania State University, University Park, Pennsylvania 16802, USA [2] These authors contributed equally to this work.

Young Woo Jung
Department of Physics, Ohio State University, Columbus, Ohio 43210-1117, USA

Lena Fitting Kourkoutis
School of Applied and Engineering Physics, Cornell University, Ithaca, New York 14853, USA

Jong-Woo Kim
Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA

Philip J. Ryan
Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA

Tassilo Heeg
Department of Materials Science and Engineering, Cornell University, Ithaca, New York 14853-1501, USA

Martin Roeckerath
Institute of Bio and Nanosystems, JARA-Fundamentals of Future Information Technologies, Research Centre Jlich, D-52425 Jlich, Germany

Veronica Goian
Institute of Physics ASCR, Na Slovance 2, 182 21 Prague 8, Czech Republic

Margitta Bernhagen
Leibniz Institute for Crystal Growth, Max-Born-Strae 2, D-12489 Berlin, Germany

Reinhard Uecker
Leibniz Institute for Crystal Growth, Max-Born-Strae 2, D-12489 Berlin, Germany

P. Chris Hammel
Department of Physics, Ohio State University, Columbus, Ohio 43210-1117, USA

Karin M. Rabe
Department of Physics and Astronomy, Rutgers University, Piscataway, New Jersey 08854-8019, USA

Stanislav Kamba
Institute of Physics ASCR, Na Slovance 2, 182 21 Prague 8, Czech Republic

Jrgen Schubert
Institute of Bio and Nanosystems, JARA-Fundamentals of Future Information Technologies, Research Centre Jlich, D-52425 Jlich, Germany

John W. Freeland
Advanced Photon Source, Argonne National Laboratory, Argonne, Illinois 60439, USA

David A. Muller
[1] School of Applied and Engineering Physics, Cornell University, Ithaca, New York 14853, USA [2] Kavli Institute at Cornell for Nanoscale Science, Ithaca, New York 14853, USA

Craig J. Fennie
School of Applied and Engineering Physics, Cornell University, Ithaca, New York 14853, USA

Peter Schiffer
Department of Physics and Materials Research Institute, Pennsylvania State University, University Park, Pennsylvania 16802, USA

Venkatraman Gopalan
Department of Materials Science and Engineering, Pennsylvania State University, University Park, Pennsylvania 16802-5005, USA

Ezekiel Johnston-Halperin
Department of Physics, Ohio State University, Columbus, Ohio 43210-1117, USA

Darrell G. Schlom
Department of Materials Science and Engineering, Cornell University, Ithaca, New York 14853-1501, USA
Ferroelectric ferromagnets are exceedingly rare, fundamentally interesting multiferroic materials that could give rise to new technologies in which the low power and high speed of field-effect electronics are combined with the permanence and routability of voltage-controlled ferromagnetism. Furthermore, the properties of the few compounds that simultaneously exhibit these phenomena are insignificant in comparison with those of useful ferroelectrics or ferromagnets: their spontaneous polarizations or magnetizations are smaller by a factor of 1,000 or more. The same holds for magnetic- or electric-field-induced multiferroics. Owing to the weak properties of single-phase multiferroics, composite and multilayer approaches involving strain-coupled piezoelectric and magnetostrictive components are the closest to application today. Recently, however, a new route to ferroelectric ferromagnets was proposed by which magnetically ordered insulators that are neither ferroelectric nor ferromagnetic are transformed into ferroelectric ferromagnets using a single control parameter, strain. The system targeted, EuTiO3, was predicted to exhibit strong ferromagnetism (spontaneous magnetization, 7 Bohr magnetons per Eu) and strong ferroelectricity (spontaneous polarization, 10Ccm2) simultaneously under large biaxial compressive strain. These values are orders of magnitude higher than those of any known ferroelectric ferromagnet and rival the best materials that are solely ferroelectric or ferromagnetic. Hindered by the absence of an appropriate substrate to provide the desired compression we turned to tensile strain. Here we show both experimentally and theoretically the emergence of a multiferroic state under biaxial tension with the unexpected benefit that even lower strains are required, thereby allowing thicker high-quality crystalline films. This realization of a strong ferromagnetic ferroelectric points the way to high-temperature manifestations of this spinlattice coupling mechanism. Our work demonstrates that a single experimental parameter, strain, simultaneously controls multiple order parameters and is a viable alternative tuning parameter to composition for creating multiferroics. ©2010

(As supplied by publisher.)

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