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Coulomb problem in nanostructures. E.M. Kazaryan, H.A. Sarkisyan Russian-Armenian University Yerevan State University. k. B A B. B A B. Types of nanostructures. 3D systems. 2D systems. A. B. 1D systems. 0D systems. The idea of size-quantisation. Kane’s disperssion law.
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E.M. Kazaryan, H.A. Sarkisyan Russian-Armenian University Yerevan State University
k B A B B A B Types of nanostructures 3D systems 2D systems
A B 1D systems 0D systems
E(k) G6 G8 Eg k 0 V1 G7 V2 V3 InS Experimental realization of InSb quantum dots K.D. Moiseev et al, Tech. Phys. Lett. (2007) InSb band structure
h + e _ Two dimensional Kane’s excitonE.M. Kazaryan, L.S. Petrosyan, H.A. Sarkisyan, Physica E (2008). InSb Fig.11. Kane’s exciton in the InSb QW.
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Nanoscale rings GaInAs quantum rings (Lorke et all. Phys. Rev. Lett. (2000)). Chakraborty-Pietilainen model:
R2 R1 R2 R1 Quantum ring L Confining potential Spherical nanolayer Cylindrical nanolayer R1 R2 Simple models layerednanostructures
Importance! The importance of realization of that kind of geometry is in confirmation of Aaronov-Bom effect for bound states (the model of two-dimensional rotator in magnetic field).
R1 R2 On radial direction we ignore the Coulomb interaction and suppose that both electrons are in the ground radial state.
R1 R2 R1 R2
Difference between approximated and exact functions of Coulomb interaction. Approximated (1) and exact (2) functions of Coulomb interaction.
Oscillation character Harmonic Anharmonic Libration
Harmonic R1 R2
Anharmonic R1 R2
Libration R1 R2