ScalingStacks

Verified tagged author-source HTML · 1912.02360v1 · cited publication edition alignment unverified.

A general (singular) Kähler metric ωφ\omega_{\varphi} on XsX_{s} in the polarisation class s−1​[Δ]s^{-1}[\Delta] is given by a potential φ∈P​S​H​(Xs,s−1​ωF​S)\varphi\in PSH(X_{s},s^{-1}\omega_{FS}). The normalising factor s−1s^{-1} is aimed at extracting nontrivial limits as s→∞s\to\infty. We can completely analogous define the local potentials:

{φ0=φ+(n+2)2​s​log⁡(∑m′∈v​e​r​t​e​x​(Δ)e2n+2​⟨m′,Log​(z)⟩),φm=φ+(n+2)2​s​log⁡(∑m′∈v​e​r​t​e​x​(Δ)e2n+2​⟨m′,Log​(z)⟩)−⟨m,Logs​(z)⟩,\begin{cases}\varphi_{0}=\varphi+\frac{(n+2)}{2s}\log(\sum_{m^{\prime}\in vertex{(\Delta)}}e^{\frac{2}{n+2}\langle m^{\prime},\text{Log}(z)\rangle}),\\ \varphi_{m}=\varphi+\frac{(n+2)}{2s}\log(\sum_{m^{\prime}\in vertex{(\Delta)}}e^{\frac{2}{n+2}\langle m^{\prime},\text{Log}(z)\rangle})-\langle m,\text{Log}_{s}(z)\rangle,\end{cases} (19)

which are by definition psh on respective regions.

Original mathematics by the credited authors. Source collection and HTML conversion remain in progress.