2009
DOI: 10.1103/physrevb.79.035107
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Lattice Green’s function approach to the solution of the spectrum of an array of quantum dots and its linear conductance

Abstract: In this paper we derive general relations for the band-structure of an array of quantum dots and compute its transport properties when connected to two perfect leads. The exact lattice Green's functions for the perfect array and with an attached adatom are derived. The expressions for the linear conductance for the perfect array as well as for the array with a defect are presented. The calculations are illustrated for a dot made of three atoms. The results derived here are also the starting point to include th… Show more

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Cited by 10 publications
(7 citation statements)
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“…The conductance can be evaluated from the transmission probabilities of up and down spin electrons following the Landauer definition, whereas spin-dependent transmission probabilities are computed with the help of the well known non-equilibrium Green’s function (NEGF) technique [ 80 ]. In the NEGF approach, the effects of the side attached electrodes are incorporated through finite dimensional self-energy matrices, and the effective Green’s functions are [ 80 , 81 , 82 , 83 , 84 ] where E is the energy of an incident electron and I represents the identity matrix. All of the matrices in Equation ( 7 ) are of the dimension .…”
Section: Magnetoresistance Setup and Theoretical Frameworkmentioning
confidence: 99%
“…The conductance can be evaluated from the transmission probabilities of up and down spin electrons following the Landauer definition, whereas spin-dependent transmission probabilities are computed with the help of the well known non-equilibrium Green’s function (NEGF) technique [ 80 ]. In the NEGF approach, the effects of the side attached electrodes are incorporated through finite dimensional self-energy matrices, and the effective Green’s functions are [ 80 , 81 , 82 , 83 , 84 ] where E is the energy of an incident electron and I represents the identity matrix. All of the matrices in Equation ( 7 ) are of the dimension .…”
Section: Magnetoresistance Setup and Theoretical Frameworkmentioning
confidence: 99%
“…where U k (x) denote the Chebyshev polynomials of the second kind. [20][21][22] This expression holds for k ≤ m, for m > k we just have to interchange the indices. An alternative calculation can be performed using the functional integral formalism.…”
Section: Basics: 1d Tight-binding Chainmentioning
confidence: 99%
“…At first sight, Eq. ( 33) does not look like the surface Green's function of a semi-infinite one-dimensional chain (that is because we used two atoms per unit cell for the metal) [20], however simple algebraic manipulations show that (G + RR ) 11 can be put in the known form…”
Section: Local Electronic Properties At Equilibriummentioning
confidence: 99%