The renormalization of the electron g factor by the confining potential in semiconductor nanostructures is considered. A new effective k·p Hamiltonian for the electronic states in III--V semiconductor nanostructures in the presence of an external magnetic field is introduced. The mesoscopic spin-orbit (Rashba type) and Zeeman interactions are taken into account on an equal footing. It is then solved analytically for the electron effective g factor in symmetric quantum wells (gQW*). Comparison with different spin quantum beat measurements in GaAs and InGaAs structures demonstrates the accuracy and utility of the theory. The quantum size effects in gQW* are easily understood and its anisotropy ΔgQW* (i.e., the difference between the in-plane and perpendicular configurations) is shown to be given by a mesoscopic spin-orbit effect having the same origin as the Rashba one.
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Sandoval et al. (2012) studied this question.
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