journal article·2022-12-19

Perfect kagome-lattice antiferromagnets with Jeff=12 : The Co2+ analogs of the copper minerals volborthite and vesignieite

Yuya Haraguchi, Takehiro Ohnoda, Akira Matsuo, Koichi Kindo, Hiroko Aruga Katori

Physical Review B· Volume 106· Issue 21
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Abstract

We report the synthesis, crystal structure, and magnetic properties of ${\mathrm{Co}}2+$ kagome magnets ${\mathrm{Co}}3{\mathrm{V}}2{\mathrm{O}}7{(\mathrm{OH})}2\ifmmode\cdot\else\textperiodcentered\fi{}2{\mathrm{H}}2\mathrm{O}$ and ${\mathrm{BaCo}}3$(${\mathrm{VO}}4{)}2{(\mathrm{OH})}2$, which can be recognized as Co analogs of the intensively researched quantum kagome magnet volborthite ${\mathrm{Cu}}3{\mathrm{V}}2{\mathrm{O}}7{(\mathrm{OH})}2\ifmmode\cdot\else\textperiodcentered\fi{}2{\mathrm{H}}2\mathrm{O}$ and vesignieite ${\mathrm{BaCu}}3$(${\mathrm{VO}}4{)}2{(\mathrm{OH})}2$. For each compound, the ground state is seemingly $A$-type antiferromagnetic order. At low temperatures, applying a magnetic field causes a metamagneticlike transition described by the transition in which antiferromagnetically aligned canted moments change to ferromagnetically aligned ones. These ground and field-induced states include a canted ferromagnetic component perpendicular to the kagome planes favored by Dzyaloshinskii-Moriya interactions. These magnetic properties are well characterized by the ${J}_{\mathrm{eff}}=\frac{1}{2}$ physics. Our findings will be a step toward clarifying the ${J}_{\mathrm{eff}}=\frac{1}{2}$ kagome physics, which has not been thoroughly studied experimentally or theoretically.
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OpenAlex topics: Advanced Condensed Matter Physics · Physics of Superconductivity and Magnetism · Multiferroics and related materials

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