Incollection,

Statistical mechanics of random lasers: a glassy scenario

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Abstract Book of the XXIII IUPAP International Conference on Statistical Physics, Genova, Italy, (9-13 July 2007)

Abstract

The electromagnetic field in nonlinear disordered active media, i.e. random lasers, can be described by coupled-mode equations for the complex field amplitudes introducing an Hamiltonian with many-body interaction terms among overlapping modes. Within the quenched-amplitudes approximation, the relevant variables are the mode-phases which interact through quenched disordered couplings $J$: equation H = - \sum_spqr J_spqr ( \varphi_s+\varphi_p-\varphi_q-\varphi_r) \nonumber equation Statistical mechanics methods can be applied to study the thermodynamics of the model. In the weakly disordered case (couplings fluctuation negligible with respect to their mean values) a paramagnetic-ferromagnetic phase transition is predicted, corresponding to phase-mode locking transition in multimode lasers. In the opposite regime (strongly disordered case) a glassy behaviour emerges: a one-step replica symmetry breaking glass transition is present at a given temperature (or pumping rate, i.e. stored energy in the modes), corresponding to a random mode-locking transition in random lasers. In the intermediate regime (couplings fluctuation comparable with mean values) a reach phase diagram is expected to hold, with the presence of paramagnetic, ferromagnetic and glassy phases. Implications on numerical and real experiments will be discussed.\\ \\ References: 1. L.~Angelani, C.~Conti, G.~Ruocco, and F.~Zamponi, Phys. Rev. Lett. 96, 065702 (2006), Phys. Rev. B 74, 104207 (2006). 2. L.~Angelani, C.~Conti, L.~Prignano, G.~Ruocco, and F.~Zamponi, Phys. Rev. B (submitted); cond-mat/0612024.

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