Let ΩΩ be an annulus. We prove that the mean field equation −Δψ=e\sp−βψ∫\sbΩe\sp−βψ−Δψ=∫\sbΩe\sp−βψe\sp−βψ admits a solution with zero boundary for β∈(−16π,−8π)β∈(−16π,−8π). This is a supercritical case for the Moser-Trudinger inequality.
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