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Possibility of ferro-octupolar order in Ba$$_2$$CaOsO$$_6$$ assessed by X-ray magnetic dichroism measurements

芝田 悟朗 ; 藤森 淳; 他10名*

Shibata, Goro; Fujimori, Atsushi; 10 of others*

We studied the cubic double perovskite Ba$$_{2}$$CaOsO$$_{6}$$ containing the Os$$^{6+}$$ ($$5d^2$$) ions, which exhibits a phase transition to a `hidden order' below $$T^{*} sim 50$$ K, by X-ray absorption spectroscopy (XAS) and X-ray magnetic circular dichroism (XMCD) at the Os $$L_{2,3}$$ edge. The cubic ligand-field splitting between the $$t_{2g}$$ and $$e_g$$ levels of Os $$5d$$ was deduced by XAS to be $$sim 4$$ eV. The temperature dependence of the XMCD spectra was consistent with a $$sim 18$$ meV residual cubic splitting of the lowest $$J_mathrm{eff} = 2$$ multiplet state into the non-Kramers $$E_g$$ doublet ground state and the $$T_{2g}$$ triplet excited state. Ligand-field (LF) multiplet calculation under fictitious strong magnetic fields indicated that the exchange interaction between nearest-neighbor octupoles should be as strong as $$sim 1.5$$ meV if a ferro-octupole order is stabilized in the `hidden-ordered' state, consistent with the exchange interaction of $$sim 1$$ meV previously predicted theoretically using model and density functional theory calculations.

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