Abstract
A semiconductor microcavity is an optical resonator, where the mirrors consist of alternating layers of two different semiconductors with different refractive indices, e.g., GaAs and AlAs, which have thicknesses of a quarter wavelength each. The resonator itself is called spacer, and has a thickness of a few half wavelengths. The electric fields of the light waves, and hence the light–matter interaction can be modified significantly inside a microcavity. In the past decades, a number of sophisticated experiments have been reported that took advantage of the strongly enhanced electric field inside the spacer of a planar semiconductor microcavity. A prominent example is the enhanced exciton–photon coupling, resulting in an enlarged Rabi splitting, in planar microcavities containing undoped quantum wells [1]. Subsequently, a wealth of theoretical and experimental work on exciton polaritons in semiconductor microcavities, e.g., about the influence of a magnetic field [2], or coupling between different microcavities [3], followed.
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Schüller, C. (2006). Inelastic Light Scattering in Microcavities. In: Inelastic Light Scattering of Semiconductor Nanostructures. Springer Tracts in Modern Physics, vol 219. Springer, Berlin, Heidelberg . https://doi.org/10.1007/3-540-36526-5_8
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DOI: https://doi.org/10.1007/3-540-36526-5_8
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