IntroductionThe term 'polarization conversions' appeared in mid-1990s with regard to the polarization phenomena observed at the conditions of optical pumping of GaAs/(Al,Ga)As layered nanostructures.1,2 In particular, the external magnetic field applied along the growth axis caused the appearance of the circularly polarized component of the photoluminescence (PL) at a linearly polarized optical excitation or, vice versa, appearance of the linearly polarized component of the PL at a circularly polarized excitation. The 'linear-to-linear conversion', i.e., merely the rotation of the plane of polarization of the PL with respect to that of the excitation light, was also observed. 2 Taking a broader view of things, one can consider as 'conversions' all the collection of the exciton-mediated relationships between the three polarization parameters of the excitation light and the three polarization parameters of the PL. With such an interpretation, well-known effects of optical orientation and optical alignment of excitons 3 are particular forms of the conversions.Later on, the conversions effect was reported for quantum dot layers.
Models and resultsWe shall calculate optical polarization responses of a layer of uncharged quantum dots where neutral excitons are created by the polarized optical excitation. We consider two-step models of the exciton evolution, and the relaxation is not taken into account. We allow for random orientations of the principal axes of the QDs' lower (ground) state potential (in-plane 'elongations' of QDs, where the inhomogeneous in-plane strain distribution can add to the QD shape effect 15,16 ). Confirmed by various ensemble and single-QD experiments, the directional scatter is a well-established reality for many epitaxial QD systems. We shall describe it by a probability density function, where where capital Θ s refer to the upper, small θ s -to the lower state. Together with the parameters β α , of the angular function Eq.(2) they form the full parameter system of the problem.We searched for all the polarization components of the luminescence for the cases of linearly where i specifies the incoming-, j -the outgoing polarization, ' L stands for the linear polarization degree in the axes rotated by 45° with respect to the vertical direction, coefficients ij C are functions of B but not of ϕ . Table are marked (corr). By this model we have in mind large QDs (each of them contains several exciton levels) being excited by photons whose energy exceed the PL energy only slightly. Second, a fully non-correlated conversion (marked n/corr), i.e., the excited-state potential has arbitrary direction of the in-plane elongation with no relationship to the ground-state elongation. Third, an almost non-correlated conversion (marked n/corr*), i.e., the excited-state potential is elongated parallel to [110] for all the QDs with no relationship to the ground-state elongation. The latter two models can be compared to the case of small QDs as emitting states and the excitons being generated in the wetting ...