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Exciton fine structure in interfacial quantum dots
Author(s) -
Phillips R. T.,
Steffan A. G.,
Newton S. R.,
Reinecke T. L.,
Kotlyar R.
Publication year - 2003
Publication title -
physica status solidi (b)
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.51
H-Index - 109
eISSN - 1521-3951
pISSN - 0370-1972
DOI - 10.1002/pssb.200303184
Subject(s) - quantum dot , exciton , zeeman effect , condensed matter physics , hamiltonian (control theory) , fine structure , biexciton , diamagnetism , physics , photoluminescence , zeeman energy , spin (aerodynamics) , atomic physics , magnetic field , quantum mechanics , optics , mathematical optimization , mathematics , thermodynamics
We have studied, by ‘micro‐magneto‐photoluminescence’, the eigenstates of excitons localised in the interfacial potential of narrow GaAs/Al 0.31 Ga 0.69 As quantum wells. These behave in many respects as quantum dot excitons, and give narrow emission lines that permit direct resolution of Zeeman splittings. Some dots show small zero‐field splitting (<100 μeV), varying down to below the limit of resolution of our technique (≈25 μeV). For these dots the excitonic g ‐factor depends on well‐width, and also shows variation with the applied field B . The variation with B is related to the band mixing which is more prominent in these weakly‐confined dots than in, for example, typical Stranski–Krastanow dots. The magnitude of the term linear in B can be calculated in a simplified model of the confined state, which gives a method of estimating the lateral extent of the confining potential. For particular transitions which are found at the extreme low‐energy end of the emission from wells of 2 nm and 3 nm width, a different behaviour is found. These show much larger zero‐field splitting of around 1 meV, and much smaller diamagnetic shift than that in the more usual dots with small zero‐field splitting. The measured spin fine structure of these states is compared with that calculated from a spin Hamiltonian for a heavy‐hole exciton, which gives a unique determination of the full three‐dimensional g ‐factor for a single quantum dot.