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钙钛矿型 CaCuO2 和 SrTiO3 绝缘氧化物界面处的高温超导现象。

High-T(c) Superconductivity at the Interface between the CaCuO2 and SrTiO3 Insulating Oxides.

机构信息

Dipartimento di Ingegneria Civile e Ingegneria Informatica, Università di Roma Tor Vergata, Via del Politecnico 1, I-00133 Roma, Italy.

CNR-SPIN, Università di Roma Tor Vergata, Roma I-00133, Italy.

出版信息

Phys Rev Lett. 2015 Oct 2;115(14):147001. doi: 10.1103/PhysRevLett.115.147001. Epub 2015 Sep 28.

DOI:10.1103/PhysRevLett.115.147001
PMID:26551817
Abstract

At interfaces between complex oxides it is possible to generate electronic systems with unusual electronic properties, which are not present in the isolated oxides. One important example is the appearance of superconductivity at the interface between insulating oxides, although, until now, with very low T(c). We report the occurrence of high T(c) superconductivity in the bilayer CaCuO(2)/SrTiO(3), where both the constituent oxides are insulating. In order to obtain a superconducting state, the CaCuO(2)/SrTiO(3) interface must be realized between the Ca plane of CaCuO(2) and the TiO(2) plane of SrTiO(3). Only in this case can oxygen ions be incorporated in the interface Ca plane, acting as apical oxygen for Cu and providing holes to the CuO(2) planes. A detailed hole doping spatial profile can be obtained by scanning transmission electron microscopy and electron-energy-loss spectroscopy at the O K edge, clearly showing that the (super)conductivity is confined to about 1-2 CaCuO(2) unit cells close to the interface with SrTiO(3). The results obtained for the CaCuO(2)/SrTiO(3) interface can be extended to multilayered high T(c) cuprates, contributing to explaining the dependence of T(c) on the number of CuO(2) planes in these systems.

摘要

在复杂氧化物的界面处,可以生成具有非常规电子特性的电子系统,这些特性在孤立的氧化物中并不存在。一个重要的例子是在绝缘氧化物的界面处出现超导性,尽管到目前为止,其超导转变温度(T(c))非常低。我们报告了在双层 CaCuO(2)/SrTiO(3)中出现高温超导性,其中两个组成氧化物都是绝缘的。为了获得超导状态,必须在 CaCuO(2)的 Ca 平面和 SrTiO(3)的 TiO(2)平面之间实现 CaCuO(2)/SrTiO(3)界面。只有在这种情况下,氧离子才能掺入界面的 Ca 平面中,作为 Cu 的顶点氧,并向 CuO(2)平面提供空穴。通过扫描透射电子显微镜和电子能量损失光谱在 O K 边,可以获得详细的空穴掺杂空间分布,清楚地表明超导性局限于大约 1-2 个靠近与 SrTiO(3)界面的 CaCuO(2)单元。在 CaCuO(2)/SrTiO(3)界面上获得的结果可以扩展到多层高温超导铜酸盐,有助于解释这些系统中 T(c)对 CuO(2)平面数量的依赖性。

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