Fractal superconductivity near localization threshold
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If you have a question about this talk, please contact Dr Jonathan Keeling.
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I will present a theory of a pseudogap state appearing near the
superconductor-insulator transition in strongly disordered metals with
attractive interaction. Such an interaction combined with the fractal
nature of the single particle wave functions near the mobility edge leads
to an anomalously large single particle gap in the superconducting state
near SI transition that persists and even increases in the insulating
state long after the superconductivity is destroyed. Analytic expressions
for the value of the pseudogap in terms of the inverse participation ratio
of the corresponding localization problem.
This talk is part of the Theory of Condensed Matter series.
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