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.
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Phillips et al. (2003) studied this question.
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