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Published byBirger Aas Modified over 5 years ago
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Topological states of matter – from the quantum Hall effect to Majorana fermions
Ady Stern (Weizmann) The quantum Hall effects – introduction Unavoidable conclusions
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The quantum Hall effects
Introduction
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Landau level filling factor = density of electrons
The Hall effect I B Electrons in two dimensions Classically, Hall resistivity longitudinal resistivity - unchanged by B. Quantum mechanically degenerate harmonic oscillator spectrum Landau levels Landau level filling factor = density of electrons density of flux quanta
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The quantum Hall effect
zero longitudinal resistivity - no dissipation quantized Hall resistivity to amazing precision Integer quantum Hall effect - integer n Fractional quantum Hall effect
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Single particle spectrum – highly degenerate Landau levels
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The original sample of the FQHE:
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