Metastable Bound States of the Two-Dimensional Bimagnetoexcitons in the Lowest Landau Levels Approximation
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MOSKALENKO, Sveatoslav; KHADZHI, Peter; PODLESNY, Igor; DUMANOV, Evgheni; LIBERMAN, Michael; ZUBAC, Ion. Metastable Bound States of the Two-Dimensional Bimagnetoexcitons in the Lowest Landau Levels Approximation. In: Semiconductors. 2018, nr. 14(52), pp. 1801-1805. ISSN 1063-7826.
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Semiconductors
Numărul 14(52) / 2018 / ISSN 1063-7826

Metastable Bound States of the Two-Dimensional Bimagnetoexcitons in the Lowest Landau Levels Approximation


DOI: 10.1134/S1063782618140208
Pag. 1801-1805

Moskalenko Sveatoslav1, Khadzhi Peter1, Podlesny Igor1, Dumanov Evgheni1, Liberman Michael2, Zubac Ion1
 
1 Institute of Applied Physics,
2 Nordic Institute for Theoretical Physics (NORDITA) KTH
 
Disponibil în IBN: 21 iunie 2019


Rezumat

Abstract: The possible existence of the bound states of the interacting two-dimensional (2D) magnetoexcitons in the lowest Landau levels (LLLs) approximation was investigated using the Landau gauge description. The magnetoexcitons taking part in the formation of the bound state with resultant wave vector k = 0 have opposite in-plane wave vectors k and k and look as two electric dipoles with the arms oriented in-plane perpendicularly to the corresponding wave vectors. The bound state of two antiparallel dipoles moving with equal probability in any direction of the plane with equal but antiparallel wave vectors is characterized by the variational wave function of the relative motion ϕn(k) depending on the modulus |k|. The spins of two electrons and the effective spins of two holes forming the bound states were combined separately in the symmetric or in the antisymmetric forms (↑↓ + η↓↑) with the same parameter η = ±1 for electrons and holes. In the case of the variational wave function ϕ2(k) = (8α3)1/2k2I0 22exp[−αk2I0 2] the maximum density of the magnetoexcitons in the momentum space representation is concentrated on the in-plane ring with the radius kr = 1/( αl0). The stable bound states of the bimagnetoexciton molecule do not exist for both spin orientations. Instead of them, a deep metastable bound state with the activation barrier comparable with the ionization potential I1 of the magnetoexciton with k=0 was revealed in the case η = 1 and α = 0.5. In the case η = −1 and α = 3.4 only a shallow metastable bound state can appear.