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arXiv 1503.07328cond-mat.str-el
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(LaNiO3)n/(LaMnO3)2超晶格光谱重分布的光谱研究

Spectral weight redistribution in (LaNiO3)n/(LaMnO3)2 superlattices from optical spectroscopy

P. Di Pietro, J. Hoffman, A. Bhattacharya, S. Lupi, A. Perucchi

摘要:

研究了SrTiO $_3$衬底上的四种(LaNiO $_3$)$_n$ /(LaMnO $_3$)$_2$超晶格(SL)($n$ =2,3,4,5)的光学性质。我们测量了20 K到400 K温度范围内的反射率,并通过基于Kramers-Kronig一致的Lorentz-Drude模型的拟合过程提取了光学电导率。随着LaNiO $_3$厚度的增加,SL经历绝缘体-金属转变(IMT),其伴随着光谱权重从高频到低频的转移。然而,宽的中红外带的存在表明(LaNiO $_3$)$_n$ /(LaMnO $_3$)$_2$ SL的光学电导率不是LaMnO $_3$和LaNiO $_3$电导率的线性组合。我们的观察表明,界面电荷转移导致IMT由于在Mn和Ni网站的价态的变化。

英文摘要:

We have studied the optical properties of four (LaNiO$_3$)$_n$/(LaMnO$_3$)$_2$ superlattices (SL) ($n$=2, 3, 4, 5) on SrTiO$_3$ substrates. We have measured the reflectivity at temperatures from 20 K to 400 K, and extracted the optical conductivity through a fitting procedure based on a Kramers-Kronig consistent Lorentz-Drude model. With increasing LaNiO$_3$ thickness, the SLs undergo an insulator-to-metal transition (IMT) that is accompanied by the transfer of spectral weight from high to low frequency. The presence of a broad mid-infrared band, however, shows that the optical conductivity of the (LaNiO$_3$)$_n$/(LaMnO$_3$)$_2$ SLs is not a linear combination of the LaMnO$_3$ and LaNiO$_3$ conductivities. Our observations suggest that interfacial charge transfer leads to an IMT due to a change in valence at the Mn and Ni sites.

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