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Ferroelectricity induced by a combination of crystallographic chirality and axial vector

結晶学的キラリティーと軸性ベクトルの組み合わせによって誘起される強誘電性

永井 隆之*; 萩原 雅人   ; 横井 里江*; 森分 博紀*; 木村 剛*

Nagai, Takayuki*; Hagihara, Masato; Yokoi, Rie*; Moriwake, Hiroki*; Kimura, Tsuyoshi*

Ferroelectric materials compatible with magnetism and/or conductive properties provide a platform for exploring unconventional phenomena, such as the magnetoelectric effect, nonreciprocal responses, and nontrivial superconductivity. Though recent studies on multiferroics have offered several approaches, the search for magnetic and/or conducting ferroelectric materials is still a challenging issue under the traditional "d$$^{0}$$-ness" rule, refusing active d electrons. Here, we propose the emergence of ferroelectricity through a combination of crystallographic chirality and axial vector, accepting even non-d$$^{0}$$ magnetic ions. This proposal is demonstrated in quasi-one-dimensional magnetic systems SrM$$_{2}$$V$$_{2}$$O$$_{8}$$ (M = Ni, Mg, and Co). The ferroelectric phase transition is observed by measurements of neutron powder diffraction and dielectric properties in all compositions. Structural analyses and first-principles calculations indicate that these magnetic compounds are identified as proper-type ferroelectrics whose ferroelectric phase transition is achieved by spiral motions of crystallographic screw chains formed by edge-shared MO6 octahedra, considered as the combination of locally defined chirality and axial vector. Computationally predicted magnitude of spontaneous polarization of SrM$$_{2}$$V$$_{2}$$O$$_{8}$$ reaches $$sim$$10$$^{circ}$$$$mu$$C/cm$$^{2}$$, comparable to that of conventional ferroelectrics, despite the incorporation of non-d$$^{0}$$ magnetic elements. The mechanism proposed in this study offers a unique approach to the exploration of new ferroelectrics beyond the traditional paradigms.

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パーセンタイル:16.13

分野:Chemistry, Multidisciplinary

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