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Reentrance of interface superconductivity in a high-T(c) cuprate heterostructure

Increasing the carrier density in a Mott insulator by chemical doping gives rise to a generic superconducting dome in high temperature superconductors. An intriguing question is whether a second superconducting dome may exist at higher dopings. Here we heavily overdope La(2-x)Sr(x)CuO(4) (0.45 ≤ x ≤...

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Detalles Bibliográficos
Autores principales: Shen, J. Y., Shi, C. Y., Pan, Z. M., Ju, L. L., Dong, M. D., Chen, G. F., Zhang, Y. C., Yuan, J. K., Wu, C. J., Xie, Y. W., Wu, J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10638369/
https://www.ncbi.nlm.nih.gov/pubmed/37949854
http://dx.doi.org/10.1038/s41467-023-42903-1
Descripción
Sumario:Increasing the carrier density in a Mott insulator by chemical doping gives rise to a generic superconducting dome in high temperature superconductors. An intriguing question is whether a second superconducting dome may exist at higher dopings. Here we heavily overdope La(2-x)Sr(x)CuO(4) (0.45 ≤ x ≤ 1.0) and discover an unprecedented reentrance of interface superconductivity in La(2-x)Sr(x)CuO(4) /La(2)CuO(4) heterostructures. As x increases, the superconductivity is weakened and completely fades away at x = 0.8; but it revives at higher doping and fully recovers at x = 1.0. This is shown to be correlated with the suppression of the interfacial charge transfer around x = 0.8 and the weak-to-strong localization crossover in the La(2-x)Sr(x)CuO(4) layer. We further construct a theoretical model to account for the sophisticated relation between charge localization and interfacial charge transfer. Our work advances both the search for and control of new superconducting heterostructures.