Superconducting Sr$_{1-x}$La$_{x}$CuO$_{2}$ thin films have been grown on GdScO$_{3}$ substrates by reflection high-energy electron diffraction calibrated layer-by-layer molecular-beam epitaxy. X-ray diffraction analysis has confirmed the infinite layer structure after an in-situ vacuum annealing step. In-situ photoemission spectroscopy indicates that the vacuum annealing step employed immediately after film growth to achieve superconducting films results in oxygen loss from the films. The superconducting critical temperature depends on the La content $x$, with the highest value obtained for $x \sim 0.10$. Resistivity as a function of temperature $\rho(T)$ curves of optimally doped samples show a T$^{2}$ temperature dependence characteristic of a scattering process where electron-electron interactions dominate.

Layer-by-layer shuttered molecular-beam epitaxial growth of superconducting Sr1-xLaxCuO2 thin films

POrgiani;
2013

Abstract

Superconducting Sr$_{1-x}$La$_{x}$CuO$_{2}$ thin films have been grown on GdScO$_{3}$ substrates by reflection high-energy electron diffraction calibrated layer-by-layer molecular-beam epitaxy. X-ray diffraction analysis has confirmed the infinite layer structure after an in-situ vacuum annealing step. In-situ photoemission spectroscopy indicates that the vacuum annealing step employed immediately after film growth to achieve superconducting films results in oxygen loss from the films. The superconducting critical temperature depends on the La content $x$, with the highest value obtained for $x \sim 0.10$. Resistivity as a function of temperature $\rho(T)$ curves of optimally doped samples show a T$^{2}$ temperature dependence characteristic of a scattering process where electron-electron interactions dominate.
2013
Istituto Superconduttori, materiali innovativi e dispositivi - SPIN
Superconducting films and low-dimensional structures
Molecular beam epitaxy
Cuprate superconductors
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/21258
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