2020
DOI: 10.1140/epjb/e2020-10178-2
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Electronic properties of α − 𝒯3 quantum dots in magnetic fields

Abstract: We address the electronic properties of quantum dots in the two-dimensional α − 𝒯3 lattice when subjected to a perpendicular magnetic field. Implementing an infinite mass boundary condition, we first solve the eigenvalue problem for an isolated quantum dot in the low-energy, long-wavelength approximation where the system is described by an effective Dirac-like Hamiltonian that interpolates between the graphene (pseudospin 1/2) and Dice (pseudospin 1) limits. Results are compared to a full numerical (finite-ma… Show more

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Cited by 6 publications
(3 citation statements)
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“…A number of properties of finite size dice lattice quantum dots were studied in recent years. Among them are the description of distributions of edge currents in quantum dots [31], prediction appearance of Majorana corner states in the presence of Rashba coupling [32], size dependence of Landau levels formed in the ring made of α − T 3 lattice [33], analysis of the role of atomic effects in narrow zigzag ribbons [34], valley filtering [35,36] and dynamical formation of bound states by external driving [37] in α − T 3 lattice quantum dots. The formation of pseudo-Landau levels in nonuniform strain for triangular shaped quantum dots was discussed in [38].…”
Section: Introductionmentioning
confidence: 99%
“…A number of properties of finite size dice lattice quantum dots were studied in recent years. Among them are the description of distributions of edge currents in quantum dots [31], prediction appearance of Majorana corner states in the presence of Rashba coupling [32], size dependence of Landau levels formed in the ring made of α − T 3 lattice [33], analysis of the role of atomic effects in narrow zigzag ribbons [34], valley filtering [35,36] and dynamical formation of bound states by external driving [37] in α − T 3 lattice quantum dots. The formation of pseudo-Landau levels in nonuniform strain for triangular shaped quantum dots was discussed in [38].…”
Section: Introductionmentioning
confidence: 99%
“…There are also several suggestions for an optical α-T 3 lattice that would allow a tuning of α by dephasing one pair of the three counter-propagating laser beams [28,30]. Under external electromagnetic fields, the flat band and α-dependent Berry phase have striking consequences on the Landau level quantization [28,31], the quantum Hall effect [32,33], Klein tunneling [34][35][36][37] and Weiss oscillations [38]. While the flat band has zero group ve-locity and therefore zero conductivity, it is predicted to play an important role for the transport by its nontrivial topology [29,44], the coupling to propagating bands [39][40][41], or interaction effects [42][43][44][45].…”
Section: Introductionmentioning
confidence: 99%
“…The combination of strain, Dirac-cone physics, and flat-band physics in a modified α-T 3 lattice structure is an interesting case to study, not only because the flat band then crosses the nodal Dirac points with peculiar consequences for the Berry phase [18], Klein tunneling [19], Weiss oscillations [20], or LL quantization [21], but also regarding the interplay between the local inversion symmetry breaking by strain and the global one by α. In the α-T 3 structure one of the inequivalent sites of the honeycomb lattice is connected to a site located in the center of the hexagons with strength α, i.e., in a certain sense this system interpolates between graphene (α = 0) and dice (α = 1) lattices [22].…”
Section: Introductionmentioning
confidence: 99%