Theorem 18.28.49.EA3E101DCA5E Suppose that $\varphi \in \mathrm{PSH}(X,\theta )_{>0}$. Then
A6F9F2DF4A0D
18.28.50
EA3E101DCA5ETheorem 18.28.49.EA3E101DCA5E Suppose that $\varphi \in \mathrm{PSH}(X,\theta )_{>0}$. Then
A6F9F2DF4A0D
18.28.50
Proof of theorem 18.28.49. By 18.28.15 and proposition 16.6.11, the three potentials below have the same multiplier ideals. Hence
This allows us to replace $\varphi $ with $P_{\theta ,K}[\varphi ]_{\mathcal{I}}(v)$.
By 13.13.47, there exists a sequence $(\varphi _ j)_ j$ in $\mathrm{PSH}(X,\theta )$ such that $\varphi _ j\nearrow \varphi $ a.e. and $\theta _{\varphi _ j}$ is a Kähler current for each $j\geq 1$. This gives
Let $\tau $ be the weak limit of a subsequence of $(\beta ^ k_{v,\varphi ,\mu })_ k$. Then by proposition 18.28.74,
By proposition 18.28.35 and corollary 13.13.12, we have
Hence,
8FD19D2B07C7
18.28.78
A comparison of total masses using (18.28.48) gives that equality holds in (18.28.78). As $\tau $ is arbitrary, we obtain (18.28.50). $\square$
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