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Disorder Effects on Electron Transport in Nanocrystal Assemblies and Topological Insulators

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Figure 1.2: (a) Energy band structure of undoped Bi 2 Se 3 measured by ARPES. The top and bottom are the conduction and valence band of the bulk, respectively; in the middle are the gapless surface states that have a dirac-cone like band structure
Figure 1.3: (Color online) Phase diagram indicating regimes of activated and ES re- re-sistivity as a function of doping level ν and the dimensionless quantum energy gap
Figure 1.4: (Color online) The DOGS of a regular 3d array of monodisperse NCs, where ε = E/(e 2 /2C 0 ) is the dimensionless single-particle energy and g ∗ (ε) = (e 2 D d /2C 0 )g(ε) is the dimensionless DOGS, where D is the NC diameter
Figure 1.5: (Color online) Single electron and pair DOGS, g 1 ∗ (ε) and g ∗ 2 (ε), of a regular 2d array of monodisperse metallic grains as a function of the dimensionless electron energy ε = E/E c at different values of the superconducting gap ∆ ∗ = ∆ 0 /E
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Outline

Model of NC arrays with random number of dopants Computer modeling Results and discussion Gating of a NC array by an ionic liquid Model Tunneling experiments Introduction The model, pseudoground state, and density of states

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