S. Lavanga

Superconducting properties of [ BaCuO x ] 2 / [ CaCuO 2 ] n artificial structures with ultrathick CaCuO 2 blocks

The electrical transport properties of

Superconducting properties of [BaCuO_x]_2/[CaCuO_2]_n artificial structures with ultrathick CaCuO_2 blocks

[{\mathrm{BaCuO}}_{x}{]}_{2}/[{\mathrm{CaCuO}}_{2}{]}_{n}(\mathrm{C}\mathrm{B}\mathrm{C}\mathrm{C}\mathrm{O}\ensuremath{-}2\ifmmode\times\else\texttimes\fi{}n)

Superconductivity in ultrathin artificial cuprate structures

underdoped high-temperature superconducting superlattices grown by pulsed laser deposition have been investigated. Starting from the optimally doped

Transport measurements, vortex dynamics and anisotropy in artificially layered (BaCuO2)2/(CaCuO2)2 superconducting films

\mathrm{C}\mathrm{B}\mathrm{C}\mathrm{C}\mathrm{O}\ensuremath{-}2\ifmmode\times\else\texttimes\fi{}2

Reflection high-energy electron diffraction oscillations during epitaxial growth of artificially layered films of (BaCuOx)m/(CaCuO2)n

superlattice, having three

Superconductivity and interlayer coupling in ultrathin artificially layered cuprates

{\mathrm{CuO}}_{2}

Artificial high-temperature superconducting structures

planes and

Strain effect on transport properties of SrRuO 3 films grown by laser MBE

{T}_{c}

Interlayer coupling in ultrathin high- T c artificial structures

around 80 K, we have systematically increased the number n up to 15 moving toward the underdoped region and hence decreasing

Very large purely intralayer critical current density in ultrathin cuprate artificial structures.

{T}_{c}.