Layer-by-layer pulsed-laser deposition has been used to grow ultrathin superconducting (Ba(0.9)Nd(0.1))CuO(2+x)/CaCuO(2) artificial structures with various thicknesses of the two constituent layers. Superconductivity was observed in the ultrathin structure consisting of a single CaCuO(2) superconducting block sandwiched between two (Ba(0.9)Nd(0.1))CuO(2+x) blocks. The results obtained allowed an experimental demonstration of the currently accepted structural model for high T(C) superconductivity, which requires the presence in the same structure of two blocks with different functional properties: the superconducting infinite layer block and the nonsuperconducting charge reservoir block. (C) 2001 American Institute of Physics.
Superconductivity in ultrathin artificial cuprate structures
POrgiani;
2001
Abstract
Layer-by-layer pulsed-laser deposition has been used to grow ultrathin superconducting (Ba(0.9)Nd(0.1))CuO(2+x)/CaCuO(2) artificial structures with various thicknesses of the two constituent layers. Superconductivity was observed in the ultrathin structure consisting of a single CaCuO(2) superconducting block sandwiched between two (Ba(0.9)Nd(0.1))CuO(2+x) blocks. The results obtained allowed an experimental demonstration of the currently accepted structural model for high T(C) superconductivity, which requires the presence in the same structure of two blocks with different functional properties: the superconducting infinite layer block and the nonsuperconducting charge reservoir block. (C) 2001 American Institute of Physics.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
