Abstract

Small amplitude motion in the chaotic maser model with finite temperature is studied in the context of a mean field approximation. The equilibrium state is constructed for both the normal and superradiant phases. The linear response of the model is obtained in these two cases and analytical expressions for the variation of the corresponding frequencies with temperature are derived. Their behaviour both in the integrable and chaotic limit is discussed. Sum rules are shown to be fulfilled and relative percentages turn out to be temperature dependent. Finally the authors obtain the dynamical stability conditions for the chaotic maser model at finite temperature.

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