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Spin-chirality-driven ferroelectricity on a perfect triangular lattice antiferromagnet
Magnetic field (B) variation of the electrical polarization P(c) (∥c) of the perfect triangular lattice antiferromagnet RbFe(MoO(4))(2) is examined up to the saturation point of the magnetization for B⊥c. P(c) is observed only in phases for which chirality is predicted in the in-plane magnetic struc...
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Published in: | Physical review letters 2014-10, Vol.113 (14), p.147202-147202, Article 147202 |
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container_title | Physical review letters |
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creator | Mitamura, H Watanuki, R Kaneko, K Onozaki, N Amou, Y Kittaka, S Kobayashi, R Shimura, Y Yamamoto, I Suzuki, K Chi, S Sakakibara, T |
description | Magnetic field (B) variation of the electrical polarization P(c) (∥c) of the perfect triangular lattice antiferromagnet RbFe(MoO(4))(2) is examined up to the saturation point of the magnetization for B⊥c. P(c) is observed only in phases for which chirality is predicted in the in-plane magnetic structures. No strong anomaly is observed in P(c) at the field at which the spin modulation along the c axis, and hence the spin helicity, exhibits a discontinuity to the commensurate state. These results indicate that the ferroelectricity in this compound originates predominantly from the spin chirality, the explanation of which would require a new mechanism for magnetoferroelectricity. The obtained field-temperature phase diagram of ferroelectricity agree well with those theoretically predicted for the spin chirality of a Heisenberg spin triangular lattice antiferromagnet. |
doi_str_mv | 10.1103/physrevlett.113.147202 |
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(ORNL), Oak Ridge, TN (United States). High Flux Isotope Reactor (HFIR)</creatorcontrib><title>Spin-chirality-driven ferroelectricity on a perfect triangular lattice antiferromagnet</title><title>Physical review letters</title><addtitle>Phys Rev Lett</addtitle><description>Magnetic field (B) variation of the electrical polarization P(c) (∥c) of the perfect triangular lattice antiferromagnet RbFe(MoO(4))(2) is examined up to the saturation point of the magnetization for B⊥c. P(c) is observed only in phases for which chirality is predicted in the in-plane magnetic structures. No strong anomaly is observed in P(c) at the field at which the spin modulation along the c axis, and hence the spin helicity, exhibits a discontinuity to the commensurate state. These results indicate that the ferroelectricity in this compound originates predominantly from the spin chirality, the explanation of which would require a new mechanism for magnetoferroelectricity. 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(ORNL), Oak Ridge, TN (United States). High Flux Isotope Reactor (HFIR)</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Physical review letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Mitamura, H</au><au>Watanuki, R</au><au>Kaneko, K</au><au>Onozaki, N</au><au>Amou, Y</au><au>Kittaka, S</au><au>Kobayashi, R</au><au>Shimura, Y</au><au>Yamamoto, I</au><au>Suzuki, K</au><au>Chi, S</au><au>Sakakibara, T</au><aucorp>Oak Ridge National Lab. (ORNL), Oak Ridge, TN (United States). High Flux Isotope Reactor (HFIR)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Spin-chirality-driven ferroelectricity on a perfect triangular lattice antiferromagnet</atitle><jtitle>Physical review letters</jtitle><addtitle>Phys Rev Lett</addtitle><date>2014-10-01</date><risdate>2014</risdate><volume>113</volume><issue>14</issue><spage>147202</spage><epage>147202</epage><pages>147202-147202</pages><artnum>147202</artnum><issn>0031-9007</issn><eissn>1079-7114</eissn><abstract>Magnetic field (B) variation of the electrical polarization P(c) (∥c) of the perfect triangular lattice antiferromagnet RbFe(MoO(4))(2) is examined up to the saturation point of the magnetization for B⊥c. P(c) is observed only in phases for which chirality is predicted in the in-plane magnetic structures. 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subjects | Antiferromagnetism Chirality CLASSICAL AND QUANTUM MECHANICS, GENERAL PHYSICS Discontinuity Ferroelectricity Helicity Lattices Modulation Phase diagrams |
title | Spin-chirality-driven ferroelectricity on a perfect triangular lattice antiferromagnet |
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