1 Introduction Quantum light sources exhibiting one-and two-photon emission are the key requirement for quantum cryptography ultimately leading to truly secure data transmission [1]. Physical realization can be obtained by parametric down-conversion [2], atomic [3], or defect related transitions [4,5] and quantum dot (QD) luminescence [6,7]. Tailoring the electronic structure of a highly integrable [8] semiconductor QD even leads to tunability of the resulting photon streams [9] based on variation of vital parameters as the exciton fine-structure splitting [10][11][12] and the biexciton binding energy [13][14][15][16].Hence, the precise determination of such parameters is mandatory for the design of quantum light sources, but the emission linewidth broadening due to spectral diffusion can make such task a tough challenge. The general phenomenon of spectral diffusion was first described in nu-