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Competing magnetic and structural states in multiferroic<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>YM</mml:mi><mml:msub><mml:mi mathvariant="normal">n</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>5</mml:mn></mml:msub></mml:mrow></mml:math>at high pressure

Д. П. КозленкоFrank Laboratory of Neutron Physics, Joint Institute for Nuclear Research, 141980 Dubna, RussiaN. T. DangInstitute of Research and Development, Duy Tan University, 550000 Da Nang, Viet NamС. Е. КичановFrank Laboratory of Neutron Physics, Joint Institute for Nuclear Research, 141980 Dubna, RussiaЕ. В. ЛукинFrank Laboratory of Neutron Physics, Joint Institute for Nuclear Research, 141980 Dubna, RussiaA. M. PashayevNational Aviation Academy, AZ1045, Baku, AzerbaijanА. И. МаммадовLaboratory of Non-Standard Control and Diagnostics, Institute of Physics, ANAS, AZ-1143, Baku, AzerbaijanS. H. JabarovBayerisches Geoinstitut, Universität Bayreuth, D-95440 Bayreuth, GermanyLeonid DubrovinskyBayerisches Geoinstitut, Universität Bayreuth, D-95440 Bayreuth, GermanyHanns‐Peter LiermannPhoton Sciences, Deutsches Elektronen Synchrotron, D-22607 Hamburg, GermanyW. MorgenrothInstitute of Geosciences, University of Frankfurt, D-60438 Frankfurt, GermanyR. Z. MehdiyevaLaboratory of Non-Standard Control and Diagnostics, Institute of Physics, ANAS, AZ-1143, Baku, AzerbaijanV. G. SmotrakovPhysics Research Institute, Southern Federal University, 344090, Rostov-on-Don, RussiaБ. Н. СавенкоFrank Laboratory of Neutron Physics, Joint Institute for Nuclear Research, 141980 Dubna, Russia
2015lv
ABI

Аннотация

The magnetic, structural, and vibrational properties of $\mathrm{YM}{\mathrm{n}}_{2}{\mathrm{O}}_{5}$ multiferroic have been studied by means of neutron, x-ray powder diffraction, and Raman spectroscopy at pressures up to 6 and $30\phantom{\rule{0.28em}{0ex}}\mathrm{GPa}$, respectively. Application of high pressure, $P&gt;1\phantom{\rule{0.28em}{0ex}}\mathrm{GPa}$, leads to a gradual suppression of the commensurate and incommensurate antiferromagnetic (AFM) phases with a propagation vector $q=(1/2,0,{q}_{z}\ensuremath{\sim}1/4)$ and appearance of the commensurate AFM phase with $q=(1/2,0,1/2)$. This observation is sharply contrasting to general trend towards stabilization of commensurate AFM phase with $q=(1/2,0,1/4)$ found in other $R\mathrm{M}{\mathrm{n}}_{2}{\mathrm{O}}_{5}$ compounds upon lattice compression. At $P\ensuremath{\sim}16\phantom{\rule{0.28em}{0ex}}\mathrm{GPa}$ a structural phase transformation accompanied by anomalies in lattice compression and pressure behavior of vibrational modes was observed. The comparative analysis of high-pressure and $R$-cation radius variation effects clarified a role of particular magnetic interactions in the formation of the magnetic states of $R\mathrm{M}{\mathrm{n}}_{2}{\mathrm{O}}_{5}$ compounds.

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