Abstract
The depression of the order parameter at grain boundaries in high critical temperature superconducting oxides is determined using two formulations. First, we use the Bardeen-Cooper-Schrieffer formulation and assume formation of Cooper pairs by an attractive interaction potential. The spatial variation of the density of energy states at the Fermi level near the boundary, estimated as a function of hydrostatic stress field, is used to determine the depression of the order parameter. Second, the proximity-effect formulation is used in the form of a boundary condition on the order parameter at the interface. The boundary conditions are solved taking into account the spatial variation of the density of energy states. The depression of the order parameter from the two formulations is used in conjunction with atomic modeling to determine the critical current density associated with the grain boundaries. The model correctly predicts dependence of the critical current density across grain boundaries on the misorientation angle and temperature, in good agreement with experimental observations.
Highlights
The transparent tin dioxide (SnO:) films when deposited by chemical vapor deposition methods canbehighly conductive ( 104 [2-1 cm-1 ), they may not be adequately conductiveorwhheasn deposited attempted by to d.c. sputtering investigate the various problems associated with the SnO films and the sputtering process
The d.c. glow discharge sputtering, hereafter referred to as "sputtering", is characterized with an objective of relating the deposition parameters to the properties of the Sb-doped SnO2 films, referred to as "the films". This should enable one to understand how to control the conductivity and the transparency of the films and obtain reproducible films run after run
This paper briefly discusses some of the problems incurred in achieving reliable and reproducible thin films of tin dioxide
Summary
The transparent tin dioxide (SnO:) films when deposited by chemical vapor deposition methods canbehighly conductive ( 104 [2-1 cm-1 ), they may not be adequately conductive (pr
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