Under the right conditions, cavity polaritons form a macroscopic condensate in the ground state. The fascinating nonlinear behaviour of this condensate is largely dictated by the strength of polariton-polariton interactions. In inorganic semiconductors, these result principally from the Coulomb interaction between Wannier-Mott excitons. Such interactions are considerably weaker for the tightly bound Frenkel excitons characteristic of organic semiconductors and were notably absent in the first reported demonstration of organic polariton lasing. In this work, we demonstrate the realization of an organic polariton condensate, at room temperature, in a microcavity containing a thin film of 2,7-bis[9,9-di(4-methylphenyl)-fluoren-2-yl]-9,9-di(4-methylphenyl)fluorene. Upon reaching threshold, we observe the spontaneous formation of a linearly polarized condensate, which exhibits a superlinear power dependence, long-range order and a power dependent blue shift: a clear signature of Frenkel polariton interactions.
2The last decade has seen the study of the quantum fluidic behaviour of light flourish. 1 One branch of this field has focused on exploiting the properties of cavity polaritons:hybrid light-matter quasiparticles formed in semiconductor microcavities. 2 The substantial interest in strongly coupled semiconductor microcavities stems principally from the possibility to impart weakly interacting cavity photons with a strongly interacting matter component inherited from the exciton. On one hand, this matter component enhances energetic relaxation towards the polariton ground state by allowing interactions with phonons and other polaritons. 3,4 On the other hand, the nonlinearity inherited from the exciton gives rise to the hydrodynamic behaviour of polaritons. 5,6, 7,8,9,10,11 Polaritons have a finite lifetime, determined principally by their photonic component, beyond which they decay through the cavity mirrors. If relaxation is efficient enough, however, a macroscopic population can be accumulated in a single state-often the ground state-via bosonic final state stimulation. 12, 13,14 The threshold corresponding to this process, termed polariton lasing, can be significantly below that required for conventional photon lasing. The resulting macroscopically occupied state then behaves as a non-equilibrium Bose-Einstein condensate of polaritons. 15,16 Although polariton lasing has been mainly observed at low temperature due to the small binding energy typical of Wannier-Mott excitons, 13 recent developments have led to room temperature demonstrations in III-nitrides and ZnO. 17,18,19,20 Frenkel excitons possess binding energies of ~ 1 eV and are thus highly stable at room temperature. 21 Organic polariton lasing was first demonstrated in microcavities containing anthracene single-crystals. 22,23 3The nonlinear character of polariton condensates leads to a wealth of fascinating phenomena such as superfluidity and the formation of dark solitons and vortices. 7,8,9,10,11 This nonlinearity, which in a microscopic pi...