Abstract

The temperature dependence of the superfluid density ρ_{s}(T) has been measured for a series of ultrathin MBE-grown DyBa_{2}Cu_{3}O_{7-δ} superconducting (SC) films by submillimeter wave interferometry combined with time-domain terahertz spectroscopy and IR ellipsometry. We find that all films 10u.c. and thicker show the same universal temperature dependence of ρ_{s}(T), which follows the critical behavior characteristic of single crystal YBa_{2}Cu_{3}O_{7-δ} as T approaches T_{c}. In 7u.c. thick films, ρ_{s}(T) declines steeply upon approaching T_{c}, as expected for the Berezinskii-Kosterlitz-Thouless vortex unbinding transition. Our analysis provides evidence for a sharply defined 4u.c. non-SC interfacial layer, leaving a quasi-2D SC layer on top. We propose that the SC state in this interfacial layer is suppressed by competing (possibly charge) order.

Highlights

  • The temperature dependence of the superfluid density ρsðTÞ has been measured for a series of ultrathin molecular beam epitaxy (MBE)-grown DyBa2Cu3O7-δ superconducting (SC) films by submillimeter wave interferometry combined with time-domain terahertz spectroscopy and IR ellipsometry

  • The commonality of the layered CuO2 plane structure to all families of copper oxide high-Tc superconductors (HTSCs) implies that understanding the effect of reduced dimensionality on superconductivity in the cuprates is key to elucidating the mechanism of HTSC

  • In this Letter, we report the temperature and thickness dependence of ρs in a series of near-optimally doped DyBCO ultrathin films grown by molecular beam epitaxy (MBE)

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Summary

Published by the American Physical Society

(LaAlO3Þ0.3ðSr2AlTaO6Þ0.7 (LSAT) substrates of dimensions 10 × 10 mm by ozone-assisted atomic-layer-bylayer oxide MBE, and the high crystal structure quality of the films was confirmed by x-ray diffraction and transmission electron microscopy measurements, as reported elsewhere [16]. The results reported here are primarily based on measurements of the complex transmission obtained with a tabletop quasioptical submillimeter-wave Mach-Zehnder interferometer. These measurements were supplemented by broadband measurements of the complex dielectric function via combined time-domain terahertz spectroscopy and far-infrared-to-UV ellipsometry [17]

The real part of the conductivity shows a maximum below
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