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Antiferromagnetic order of the Co$$^{2+}$$ high-spin state with a large orbital angular momentum in La$$_{1.5}$$Ca$$_{0.5}$$CoO$$_{4}$$

層状ペロブスカイト型コバルト酸化物La$$_{1.5}$$Ca$$_{0.5}$$CoO$$_{4}$$の大きい軌道磁気モーメントを持つ高スピン状態における反強磁性

岡本 淳*; 中尾 裕則*; 山崎 裕一*; 和達 大樹*; 田中 新*; 久保田 正人; 堀金 和正*; 村上 洋一*; 山田 和芳*

Okamoto, Jun*; Nakao, Hironori*; Yamasaki, Yuichi*; Wadachi, Hiroki*; Tanaka, Arata*; Kubota, Masato; Horigane, Kazumasa*; Murakami, Yoichi*; Yamada, Kazuyoshi*

The antiferromagnetic insulator La$$_{1.5}$$Ca$$_{0.5}$$CoO$$_{4}$$ has been investigated by Co L$$_{2,3}$$-edge and O K-edge X-rayabsorption spectroscopy (XAS) measurements and Co L$$_{2,3}$$-edge resonant soft X-ray magnetic scattering (RXMS)measurement to determine the Co electronic structures associated with magnetic ordering. Co L$$_{2,3}$$-edge linear-dichroicXAS shows that Co$$^{2+}$$ takes a high-spin (HS) state and Co$$^{3+}$$ takes a low-spin (LS) state. Using Co L$$_{2,3}$$-edge RXMS, wedirectly determined that an antiferromagnetic order is formed with a HS state of Co$$^{2+}$$ ions. Moreover, the spin andorbital angular momenta of the Co$$^{2+}$$ HS state are quantitatively estimated to be 1.1$$pm$$0.1 and 1.0$$pm$$0.1, respectively,and to align parallel in the ab plane by utilizing the cluster model calculation. The large orbital angular momentum of the Co$$^{2+}$$ HS state originates from the small $$D_{4h}$$-symmetry crystal field splitting of $$t_{2g}$$ levels, which is comparable with the spin-orbit coupling constant of the Co 3$$d$$ orbital.

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パーセンタイル:38.92

分野:Physics, Multidisciplinary

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