Condensation of cavity polaritons in a disordered environment

A model for direct two band excitons in a disordered quantum well coupled to light in a cavity is investigated. In the limit in which the exciton density is high, we assess the impact of weak "pair-breaking" disorder on the feasibility of condensation of cavity polaritons. The mean-field phase diagram shows a "lower density" region, where the condensate is dominated by electronic excitations and where disorder tends to close the condensate and quench coherence. Increasing the density of excitations in the system, partially due to the screening of Coulomb interaction, the excitations contributing to the condensate become mainly photonlike and coherence is re-established for any value of disorder. In contrast, in the photon dominated region of the phase diagram, the energy gap of the quasiparticle spectrum still closes when the disorder strength is increased. Above mean-field, thermal, quantum, and fluctuations induced by disorder are considered and the spectrum of the collective excitations is evaluated. In particular, it is shown that the angle resolved photon intensity exhibits an abrupt change in its behavior, going from the condensed to the noncondensed region.