Abstract
Epitaxial YBa2Cu3O7−δ/PrBa2Cu3O7−δ (YBCO/PBCO) superlattices are tools for systematic, fundamental studies of high-temperature superconductivity. The variation of T c in YBCO/PBCO superlattices can be understood as arising from changes in the interlayer phase coupling between YBCO layers that are highly two-dimensional when they are very thin (∼1–2 c-axis unit cells) and completely isolated from each other. Single-cell-thick YBCO layers, containing isolated pairs of Cu02 planes, are found to be superconducting at T c ∼ 20 K, in a PBCO matrix. The resistance in the superconducting transition region scales with temperature as expected for the (flux flow) resistance produced by thermally generated 2D vortices, or for a 2D array of superconducting weak links. Relative to both thin-film and singlecrystal HTSc specimens, the thin superconducting layers in YBCO/PBCO superlattices exhibit a greatly expanded temperature range over which characteristic 2D dissipation can be observed, as a consequence of the enhanced anisotropy and reduced dimensionality of the YBCO layers. Scanning tunneling microscope studies reveal that YBCO films and YBCO/PBCO superlattices grow unit cell-by-unit cell by a terraced-island growth mechanism. On miscut, near-(001) substrates the terraces are epitaxially aligned with the substrate crystal lattice and spiral growth structures (screw dislocation-mediated growth) are not seen. These observations explain the steps or “kinks” that are seen in cross-section Z-contrast TEM images of YBCO/PBCO superlattices. The kinks may correspond physically to regions where the supercurrent must tunnel along the c-axis, and thus may be weak-link barriers.
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Lowndes, D.H., Norton, D.P., Zhu, S., Zheng, XY. (1992). Superconducting Properties and Microstructure of YBa2Cu3O7−δ/PrBa2Cu3O7−δ Superlattices. In: Hayakawa, H., Koshizuka, N. (eds) Advances in Superconductivity IV. Springer, Tokyo. https://doi.org/10.1007/978-4-431-68195-3_5
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DOI: https://doi.org/10.1007/978-4-431-68195-3_5
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