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Computational modelling of the vortex state in high temperature superconductors

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Figure

Figure 2.1:Spatial variation of the Cooper pairpercurrentnetic induction drops to zero over the length scalegiven by the London penetration depth,density |ψ|2, the magnetic induction B, and the su- js around the vortex centre
Figure 2.7: Static phase diagram suggested by LeDoussal and Giamarchi (1998) for the elastic man-ifolds in a random potential
Figure 2.8: Schematic representation of the re-sults of Koshelev and Vinokur (1994) on the dy-namic phase diagram for a system with a fixedmagnetic field and varying Lorentz force andtemperature.
Figure 2.9:Schematic representation of the phase diagram for three-dimensional systemsthis depins and becomes a moving Bragg glass
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