Conformal metrics on the complex plane

Let MM be a Riemannian manifold with metric gg, recall the Laplace-Beltrami operator of the metric is the elliptic operator defined as

Δgf=1gi(ggijjf).\Delta_g f = \frac{1}{\sqrt{|g|}} \partial_i \left( \sqrt{|g|} g^{ij} \partial_j f\right).

In the previous equation we use the Einstein convention of summing over repeated indexes in covariant and contravariant position. If the manifold is an open region in the complex plane, the Theorem of Liouville asserts that there exists a positive function λ\lambda, such that under a suitable change of coordinates, g=λ2dzdzˉg = \lambda^2 dz d\bar{z}, the curvature of this metric can be computed as

κ=Δglog(λ)=1λ2Δlog(λ),\kappa = - \Delta_g \log(\lambda) = -\frac{1}{\lambda^2} \Delta \log (\lambda),

where Δg\Delta_g is the Laplace-Beltrami operator of the metric and Δ=4zzˉ=x2+y2\Delta = 4 \partial_z\bar{\partial_z} = \partial^2_x + \partial^2_y is the flat Laplacian.