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Thermoelectric transport in the Quantum Hall regime

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Figure 1.3: Energy levels of a semiconductor heterostructure interface (a) before,and (b) after the charge transfer.EEC is the energy of the conduction band, EV the energy of the valence band, andF the Fermi energy
Figure 1.4: The graphical results obtained by Klaus von Klitzing in 1980, showinghow the Hall resistance and the dissipative resistance quantises in the quantum Hallregime of low temperatures and high magnetic fields [1]
Figure 1.5: The relationship between the Landau energy levels and the densityof states in a 2DEG with (a) a non-doped system, and (b) a system containingimpurities.
Figure 1.6: A sketch of the trajectories of the particles in both localised and extendedstates [2].Therefore it can be seen how those in the localised areas move aroundthe peaks and troughs, while those in the extended areas move freely through thematerial.
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System with a Symmetric Top Hat Probability Distribution Defining the Chemical Potential Inclusion of Tunnelling

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