Evidence for a bulk complex order parameter in Y0. 9Ca0. 1Ba2Cu3O7− δ thin films
Europhysics Letters, 2004•iopscience.iop.org
We have measured the penetration depth of overdoped Y 0.9 Ca 0.1 Ba 2 Cu 3 O 7− δ (Ca-
YBCO) thin films using two different methods. The change of the penetration depth as a
function of temperature has been measured using the parallel-plate resonator (PPR), while
its absolute value was obtained from a quasi-optical transmission measurement. Both sets of
measurements are compatible with an order parameter of the form Δ dx 2− y 2+ iδ d xy, with
Δ= 14.5±1.5 meV and δ= 1.8 meV, indicating a finite gap at low temperature. Below 15 K, the …
YBCO) thin films using two different methods. The change of the penetration depth as a
function of temperature has been measured using the parallel-plate resonator (PPR), while
its absolute value was obtained from a quasi-optical transmission measurement. Both sets of
measurements are compatible with an order parameter of the form Δ dx 2− y 2+ iδ d xy, with
Δ= 14.5±1.5 meV and δ= 1.8 meV, indicating a finite gap at low temperature. Below 15 K, the …
Abstract
We have measured the penetration depth of overdoped Y 0.9 Ca 0.1 Ba 2 Cu 3 O 7− δ (Ca-YBCO) thin films using two different methods. The change of the penetration depth as a function of temperature has been measured using the parallel-plate resonator (PPR), while its absolute value was obtained from a quasi-optical transmission measurement. Both sets of measurements are compatible with an order parameter of the form Δ d x 2− y 2+ iδ d xy, with Δ= 14.5±1.5 meV and δ= 1.8 meV, indicating a finite gap at low temperature. Below 15 K, the drop of the scattering rate of uncondensed carriers becomes steeper in contrast to a flattening observed for optimally doped YBCO films. This decrease supports our results on the penetration depth temperature dependence. The findings are in agreement with tunneling measurements on similar Ca-YBCO thin films.
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