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Properties of percolation channels in planar memristive structures based on epitaxial films of a YBa <sub/>2</sub> Cu <sub/>3</sub> O <sub/> 7? <i>δ</i> </sub> high temperature superconductor

DOI:10.1088/1361-6668/aae966 期刊:Superconductor Science and Technology 出版年份:2019 更新时间:2025-09-09 09:28:46
摘要: The transport properties of the percolation channels of memristive structures based on YBa2Cu3O7?δ epitaxial ?lms were studied. Molecular electronics and Andreev re?ection spectroscopy were utilised, and the in?uence of the superconductive transition of electrodes on resistive switching effects in these structures was examined. Based on the analysis of the conductivity mechanisms in the obtained heterostructures, it is assumed that percolation channels form through a chain of domains disordered by oxygen about 10 nm in diameter, with a maximum Tc of 60 K. Zero-bias anomalies of the dynamic resistance of the studied structures display temperature dependence of the critical current of typical superconductor—normal—superconductor weak links within the framework of Kulik–Omel’yanchuk theory in the dirty limit. A simulation was used to determine the physical parameters of the studied heterostructures.
作者: N A Tulina,A N Rossolenko,I M Shmytko,A A Ivanov,V V Sirotkin,I Yu Borisenko,V A Tulin
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Studying the transport properties of the percolation channels of the memristive structures based on YBCO epitaxial ?lms in order to ?nd the mechanism of the formation of such channels.

The high-resistive OFF state in memristive YBCO heterostructures is determined by the barrier properties of a structure. The heterogeneous distribution of the electric field near the electrodes creates areas with higher electric field intensity, characterized by the motion and the redistribution of oxygen defects in the surface layer of the film and a change in the resistive properties of all the structures. The percolation channel is formed by a chain of oxygen-disordered domains under the action of several processes: the formation of tunnel channels on electrodes of the structure and oxygen electro-diffusion to oxygen vacancies. The critical temperature of the superconductive transition of this channel can be controlled by the current conducted through the structure, and it fits the range 0 K–60 K.

The study does not provide an ultimate conclusion regarding the Josephson character of weak links in the percolation channel, and hence additional studies are necessary.

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