Abstract

Several explicitly solvable models of electron tunnelling in a system of single and double two-dimensional periodic arrays of quantum dots with two laterally coupled leads in a homogeneous magnetic field are constructed. First, a model of single layer formed by periodic array of zero-range potentials is described. The Landau operator (the Schrodinger operator with a magnetic field) with point-like interactions is the system Hamiltonian. We deal with two types of the layer lattices: square and honeycomb. The periodicity condition gives one an invariance property for the Hamiltonian in respect to magnetic translations group. The consideration of double quantum layer reduces to the replacement of the basic cell for the single layer by a cell including centers of different layers. Two variants of themodel for the double layer are suggested: with direct tunneling between the layers and with the connecting channels (segments in the model) between the layers. The theory of self-adjoint extensions of symmetric operators is a mathematical background of the model. The third stage of the construction is the description of leads connection. It is made by the operator extensions theory method too. Electron tunneling from input lead to the output lead through the double quantum layer is described. Energy ranges with extremely small (practically, zero) transmission were found. Dependencies of the transmission coefficient (particularly, “zero transmission bands” positions) on the magnetic field, the energy of electron and the distance between layers are investigated. The results are compared with the corresponding single-layer transmission.

Highlights

  • Electron tunnelling through periodic array of quantum dots in a homogeneous magnetic field has been intensively investigated over the last few years because it can be significant for nanotechnology applications [1,2,3,4,5,6]

  • In this paper zero-range potential model [8-10] based on the theory of self-adjoint extensions of symmetric operators is used [11]

  • We start from the Hamiltonian of a single particle in constant homogeneous magnetic field B

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Summary

Introduction

Electron tunnelling through periodic array of quantum dots in a homogeneous magnetic field has been intensively investigated over the last few years because it can be significant for nanotechnology applications [1,2,3,4,5,6]. One deals with the ballistic regime of electron transport In this case the Landauer-Buttiker formalism can be used to derive the conductivity V for the nanostructure with several leads from the transmission coefficient T (E) |E=EF (here EF is the Fermi energy). We study the influence of the magnetic field and tunnelling electron energy on the transmission coefficient and compare our results with the tunnelling through the corresponding single-layer periodic arrays researched earlier [14-15]

Model of single-layer array
Model of tunnelling between layers
Model of tunnelling
Results and discussion
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