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Advances in Differential Equations Volume 9, Numbers 5-6, May/June 2004, Pages 563–586 ON AN EVOLUTION SYSTEM DESCRIBING SELF-GRAVITATING FERMI–DIRAC PARTICLES Piotr Biler Instytut Matematyczny, Uniwersytet Wroc!lawski pl. Grunwaldzki 2/4, 50–384 Wroc!law, Poland Philippe Laurençot Mathématiques pour l’Industrie et Physique, CNRS UMR 5640 Université Paul Sabatier – Toulouse 3, 118 route de Narbonne F–31062 Toulouse cedex 4, France Tadeusz Nadzieja Instytut Matematyki, Uniwersytet Zielonogórski ul. Szafrana 4a, 65–516 Zielona Góra, Poland (Submitted by: Herbert Amann) Abstract. The global-in-time existence of solutions for a system describing the interaction of gravitationally attracting particles that obey the Fermi–Dirac statistics is proved. Stationary solutions of that system are also studied. 1. Introduction and derivation of the system Our aim in this paper is to study a nonlinear, nonlocal, parabolic system with nonlinear diffusion describing the evolution of a cloud of self-gravitating particles that obey the Fermi–Dirac statistics. This model has been introduced in [14] on the basis of considerations of kinetic equations, and has been studied in [13, 10]. Unlike the models of interacting particles where the particles are subject to linear Brownian diffusion (see, e.g., [7, 4, 5, 6, 23, 24]), the assumption that the density 0 ≤ f = f (x, v, t) of particles at the point (x, t) ∈ Ω × R+ , Ω ⊂ Rd , moving at the velocity v ∈ Rd is bounded by, say η0 > 0, leads to mathematically completely different models. They involve nonlinear diffusion resembling that for fast-diffusing gases (at large densities). The plan of this paper is following: after discussing the derivation of the system of partial differential equations in Section 1 and properties of Accepted for publication: January 2004. AMS Subject Classifications: 35Q, 35K60, 35B40, 82C21. 563