ScalingStacks

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

In particular, we can represent the Calabi-Yau metric ωC​Y,s\omega_{CY,s} on XsX_{s} by a potential φC​Y,s\varphi_{CY,s}. The Calabi-Yau condition is

ωC​Y,sn=as​s−n​d​μs,\omega_{CY,s}^{n}=a_{s}s^{-n}d\mu_{s}, (20)

where the normalising constant

as=∫Xs[Δ]n∫Xsd​μs→a∞=∫Xs[Δ]nVol​(∂Δλ∨)a_{s}=\frac{\int_{X_{s}}[\Delta]^{n}}{\int_{X_{s}}d\mu_{s}}\to a_{\infty}=\frac{\int_{X_{s}}[\Delta]^{n}}{\text{Vol}(\partial\Delta_{\lambda}^{\vee})} (21)

as s→+∞s\to+\infty (cf. Prop. 3.14).

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