Let Ω∉0G be a plane region
and let λΩ(z) be its Poincaré metric. Let EΩ be the complement of Ω and write
α(ζ) = α(ζ : Ω) = {π−1∫EΩ|z − ζ|−4dσ(z)}1∕2, where dσ(z) = dxdy and ζ ∈ Ω.
λΩ(z) = α(z : Ω) for all z ∈ Ω only when Ω is a disk less (possibly) a closed subset
of inner capacity zero. Let ϕ be holomorphic and univalent in Ω and let
Sϕ(z, ζ) = −6(∂2∕∂z∂ζ) ×log(ϕ(z) −ϕ(ζ))∕(z −ζ). Here Sϕ(z,z) is the Schwarzian
derivative of ϕ. We show