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論文

Crystal structure, photomagnetic and dielectric properties of a cyanido-bridged Cu-Mo assembly film

池田 侑典*; 松村 大樹; 辻 卓也; 生井 飛鳥*; 井元 健太*; 所 裕子*; 中林 耕二*; 大越 慎一*

Inorganica Chimica Acta, 550, p.121434_1 - 121434_8, 2023/03

https://doi.org/10.1016/j.ica.2023.121434
 被引用回数：0 パーセンタイル：0.01(Chemistry, Inorganic & Nuclear)

A film of a cyanido-bridged Cu-Mo assembly Cu$$_{2}$$[Mo(CN)$$_{8}$$]$$cdot$$8H$$_{2}$$O (CuMo-film) was electrochemically synthesized. Unlike analogs with a formula of M$$_{2}$$[Mo(CN)$$_{8}$$]$$cdot$$zH$$_{2}$$O (M = Mn, Fe, Co), which show tetragonal crystal structures, the CuMo-film shows a monoclinic structure in the C2/m space group with cell parameters of a = 17.2461 $AA, b = 11.1681 AA, c = 11.2618 AA, $beta$$ = 125.1089$$^{circ}$$, and V = 1774.44 $AA$^{3}$$. Extended X-ray absorption fine structure analysis traced the bond distances around the Cu site as 1.93-2.30 $r{A}$ for Cu-N and 2.01-2.40 $r{A}$ for Cu-O. CuMo-film exhibits photo-switchable magnetization with T$$_{C}$$ = 18 K and dielectric relaxation related to the hydrogen bond network. The change of activation energy (E$$_{a}$$) of the dielectric relaxation around 157 K (from E$$_{a}$$ = 49.9 kJ mol$$^{-1}$$ to E$$_{a}$$ = 27.3 kJ mol$$^{-1}$$ on cooling) suggests that the development of the hydrogen bond network occurs below 157 K.

論文

Electronic structure and correlation in $$beta$$-Ti$$_3$$O$$_5$$ and $$lambda$$-Ti$$_3$$O$$_5$$ studied by hard X-ray photoelectron spectroscopy

小林 啓介*; 田口 宗孝*; 小畠 雅明; 田中 健司*; 所 裕子*; 大門 寛*; 岡根 哲夫; 山上 浩志; 池永 英司*; 大越 慎一*

Physical Review B, 95(8), p.085133_1 - 085133_7, 2017/02

AA2017-0038.pdf:0.98MB

https://doi.org/10.1103/PhysRevB.95.085133
 被引用回数：15 パーセンタイル：56.08(Materials Science, Multidisciplinary)

We have conducted hard X-ray photoelectron spectroscopy investigations of the electronic structure changes and electron correlation phenomena which take place upon the photoinduced reversible phase transition between $$beta$$- and $$lambda$$-Ti$$_3$$O. From valence band spectra of $$beta$$- and $$lambda$$-Ti$$_3$$O$$_5$$, we have identified the bipolaron caused by the $$sigma$$-type bonding of $$d_{xy}$$ orbitals in $$beta$$-Ti$$_3$$O$$_5$$ and the $$pi$$ stacking between the $$d_{xy}$$ orbitals between different Ti sites in $$lambda$$-Ti$$_3$$O$$_5$$, previously predicted by $textit{ab initio}$ calculations. On the other hand, the Ti $$2p$$ and Ti $$1s$$ core level spectra exhibit nonlocal screening satellite features, which are typical spectroscopic signs of strong electron correlation in the coherent Ti $$t_{2g}$$ states. Correlation in the valence band also manifests to reduce the plasmon energy, which results in an enhancement of the valence electron mass by a factor of 2.7.

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