ScalingStacks

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2.1 Skoda inequality

An upper semicontinuous L1L^{1}-function ϕ\phi on a coordinate ball is called plurisubharmonic (psh) if −1​∂∂¯​ϕ≥0\sqrt{-1}\partial\bar{\partial}\phi\geq 0. The basic intuition is that regularity properties for psh functions in general dimensions are analogous to subharmonic functions on Riemann surfaces. This is captured by the basic version of the Skoda inequality:

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Theorem 2.1. (cf. [40, Thm 3.1]) If ϕ\phi is psh on B2⊂ℂnB_{2}\subset\mathbb{C}^{n}, with ∫B2|ϕ|​ωEn≤1\int_{B_{2}}|\phi|\omega_{E}^{n}\leq 1 with respect to the standard Euclidean metric ωE\omega_{E}, then there are dimensional constants α\alpha, CC, such that

log∫B1e−α​ϕωEn≤C.\log\int_{B_{1}}e^{-\alpha\phi}\omega_{E}^{n}\leq C.
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Remark 2.2. If instead ∫B2|ϕ|​ωEn≤C′\int_{B_{2}}|\phi|\omega_{E}^{n}\leq C^{\prime} for some constant C′C^{\prime}, then we can apply Thm 2.1 to a scaling of ϕ\phi, to get a Skoda inequality with modified α,C\alpha,C.

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Remark 2.3. Assuming an L1L^{1}-bound on ϕ\phi, then we can take a suitable cutoff function χ\chi, and via integration by parts,

∫B1−1​∂∂¯​ϕ∧ωEn−1≤∫B2χ​−1​∂∂¯​ϕ∧ωEn−1=∫B2ϕ​−1​∂∂¯​χ∧ωEn−1≤‖χ‖C2​‖ϕ‖L1≤C.\int_{B_{1}}\sqrt{-1}\partial\bar{\partial}\phi\wedge\omega_{E}^{n-1}\leq\int_{B_{2}}\chi\sqrt{-1}\partial\bar{\partial}\phi\wedge\omega_{E}^{n-1}=\int_{B_{2}}\phi\sqrt{-1}\partial\bar{\partial}\chi\wedge\omega_{E}^{n-1}\leq\left\lVert\chi\right\rVert_{C^{2}}\left\lVert\phi\right\rVert_{L^{1}}\leq C.

This simple idea is a basic version of the Chern-Levine inequality, which is another fundamental reason why psh functions are much more regular than the subharmonic functions in general dimensions.

The basic Skoda inequality immediately implies a global version. On a compact Kähler manifold (X,ω)(X,\omega), we say an upper semicontinuous L1L^{1}-function ϕ∈P​S​H​(X,ω)\phi\in PSH(X,\omega) if ωϕ=ω+−1​∂∂¯​ϕ≥0\omega_{\phi}=\omega+\sqrt{-1}\partial\bar{\partial}\phi\geq 0. This is the generalised notion of Kähler potentials.

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Theorem 2.4. On a fixed (X,ω)(X,\omega), there are positive constants α\alpha, CC depending only on X,ωX,\omega, such that

∫Xe−α​ϕ​ωXn≤C,∀ϕ∈P​S​H​(X,ω)​ with ​supϕ=0.\int_{X}e^{-\alpha\phi}\omega_{X}^{n}\leq C,\quad\forall\phi\in PSH(X,\omega)\text{ with }\sup\phi=0.
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Remark 2.5. Here ∫X|ϕ|​ωXn\int_{X}|\phi|\omega_{X}^{n} is automatically bounded using the Harnak inequality, because Δ​ϕ≥−n\Delta\phi\geq-n for ϕ∈P​S​H​(X,ω)\phi\in PSH(X,\omega).

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Remark 2.6. The supremum of all such α\alpha is known as Tian’s alpha invariant.

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