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Normal state properties of high angle grain boundaries in (Y,Ca)Ba2Cu3O7-delta
Submitted to Physical Review B
Normal state properties of high angle grain boundaries in (Y,Ca)Ba2Cu3O7-δ
S.H. Mennema, J.H.T. Ransley, G. Burnell, J.L. MacManus-Driscoll, E.J. Tarte, M.G. Blamire
Department for Materials Science and Metallurgy, University of Cambridge, Pembroke Street, CB2
3QZ, Cambridge, United Kingdom.
By lithographically fabricating an optimised Wheatstone bridge geometry, we have been able to make
accurate measurements of the resistance of grain boundaries in Y1-xCaxBa2Cu3O7-δ between the
superconducting transition temperature, Tc, and room temperature. Below Tc the normal state
properties were assessed by applying sufficiently high currents. The behaviour of the grain boundary
resistance versus temperature and of the conductance versus voltage are discussed in the framework
charge transport through a tunnel barrier. The influence of misorientation angle, oxygen content, and
calcium doping on the normal state properties is related to changes of the height and shape of the grain
boundary potential barrier.
I. INTRODUCTION
Grain boundaries in high-Tc cuprates have become a subject of intensive study after it became clear
that these defects are the cause of severe reduction of the attainable critical currents in polycrystalline
materials.1-4 Elucidating the electronic properties of grain boundaries is of great importance for the
development of recipes to enhance their transport properties for the purpose of multigrain applications,
like coated conductors. A widely discussed framework to describe the exponential decrease of critical
current density and normal state conductivity with misorientation angle is the so-called model of band
bending, as proposed by Mannhart et al.5,6 Band bending at the grain boundary is expected to occur as
a result of work-function differences, charging, and Fermi-level pinning at interface states, and leads to
hole-depleted layers in the superconducting electrodes next to the boundary. Acco
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