Let Ω be an annulus. We prove that the mean field equation
-\Delta\psi=\frac{e\sp{-\beta\psi}}{\int\sb{\Omega}e\sp{-\beta\psi}} admits
a solution with zero boundary for β∈(−16π,−8π). This is a
supercritical case for the Moser-Trudinger inequality.Comment: Filling a gap in the argument and adding 2 referrence