An investigation of the parametric amplification and its coherent control in a semiconductor microcavity is presented. The time and angle resolved pump and probe experiments show that several ps after pumping parametric scattering is still phase coherent. The experimental data are in qualitative agreement with the numerical data obtained from a relatively simple theoretical model based on three polarisation components, pump, probe, and idler. This model also predicts that under particular circumstances, the polaritons can scatter back from the signal and idler to the pump.1. Introduction Ten years ago the strong coupling regime between quantum well (QW) excitons (Xs) and microcavity (MC) photons has been observed [1]. Since then, Fabry-Perot semiconductor MCs have been intensively investigated [2]. The mixed Xphoton states, the polaritons, can be excited optically by external photons sent to the planar structure. It has not been straightforward to understand the linear optical properties of MCs [3,4]. The MCs were initially strongly affected by disorder in the mirror and QW structures. The latter leads to inhomogeneous X broadening, which of course strongly influences the polariton spectra and in extreme cases even destroys the strong coupling regime [5][6][7]. Moreover, this disorder causes also Rayleigh scattering in the MC, whereby the part due to the QWs is resonant [8][9][10]. The spread of the polaritons, after resonant excitation by light with oblique incidence, along a ring in the wavevector plane parallel to the QW, is one of the most spectacular features of resonant Rayleigh scattering [11,12]. It is directly related to the strong coupling regime and the particularities of the polariton dispersion that ensue. The particular shape of the polariton dispersion is also at the origin of the observed very long polariton dephasing times [13]. Thorough experimental and theoretical investigations were needed to understand the interplay of strong coupling, disorder effects, and the combination of both [14, 15] on the optical properties and polariton dynamics in MCs.The effects of strong excitation in MCs, which are featuring a very rich phenomenology, can be divided into two groups. The first one concerns excitonic non-linearities