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Theorem 19.4.4176132CC6940C

Theorem 19.4.41.76132CC6940C As $k\to \infty $, we have

958BCE448264 19.4.42
\begin{equation} \Delta _{k,T}(\theta ,\varphi )\xrightarrow {d_{\mathrm{Haus}}} \Delta _{\nu }(\theta ,\varphi ). \end{equation}

Proof of theorem 19.4.41. Fix a very ample line bundle $H$ on $X$ and a Kähler form $\omega \in c_1(H)$ such that $\omega \geq \theta $.

Step 1. We first handle the case where $\theta _{\varphi }$ is a Kähler current, say $\theta _{\varphi }\geq 2\delta \omega $ for some $\delta \in (0,1)$. Take a quasi-equisingular approximation $(\varphi _ j)_ j$ of $\varphi $ in $\mathrm{PSH}(X,\theta )$. We may assume that $\theta _{\varphi _ j}\geq \delta \omega $ for all $j\geq 1$. After adding constants, we also assume that $\varphi \leq 0$ and $\varphi _ j\leq 0$ for all $j$.

Let $\Delta '$ be a limit of a subsequence of $(\Delta _{k,T}(\theta ,\varphi ))_ k$. Let us say the indices of the subsequence are $k_1<k_2<\cdots $. By theorem 19.7.4, it suffices to show that $\Delta '=\Delta _{\nu }(\theta ,\varphi )$.

Observe that for each $j\geq 1$, we have $\Delta '\subseteq \Delta _{\nu }(\theta ,\varphi _ j)$ by 19.4.43. Letting $j\to \infty $, we find $\Delta '\subseteq \Delta _{\nu }(\theta ,\varphi )$ as a consequence of theorem 19.4.30. Therefore, it suffices to prove that

\[ \operatorname{vol}\Delta '\geq \operatorname{vol}\Delta _{\nu }(\theta ,\varphi ). \]

Fix an integer $N>\delta ^{-1}$. Observe that for any $j\geq 1$, we have $\varphi _ j\in \mathrm{PSH}(X,(1-N^{-1})\theta )$. Similarly, $\varphi \in \mathrm{PSH}(X,(1-N^{-1})\theta )$. By 19.4.44, it suffices to argue that

6A18B89932A8 19.4.45
\begin{equation} \operatorname{vol}\Delta '\geq \operatorname{vol}\Delta _{\nu }\left((1-N^{-1})\theta ,\varphi \right). \end{equation}

Step 1.1. We first reduce to the case where $N|k_ i$ for all $i$.

We are free to replace $(k_ i)_ i$ by a subsequence, so we may assume that $k_ i\equiv a$ modulo $N$ for all $i\geq 1$, where $a\in \{ 0,1,\ldots ,N-1\} $. We write $k_ i=g_ i N+a$. Observe that for each $i\geq 1$,

\[ \mathrm{H}^0\left(X,T\otimes L^{k_ i}\otimes \mathcal{I}(k_ i\varphi )\right)\supseteq \mathrm{H}^0\left(X,T\otimes L^{-N+a}\otimes L^{g_ i N+ N}\otimes \mathcal{I}\left((g_ iN+N)\varphi \right)\right). \]

Up to replacing $T$ by $T\otimes L^{-N+a}$, we may therefore assume that $a=0$, so that $k_ i=g_ i N$.

Step 1.2. Write $k_ i=g_ i N$ for all $i$. We prove (19.4.45).

Since

\[ \int _ X\theta _{\varphi _ j}^ n\to \int _ X\theta _{P_\theta [\varphi ]_{\mathcal I}}^ n, \]

we can apply 13.13.30 to find $j'\in \mathbb {Z}_{>0}$ such that for all $j\geq j'$, there is $\psi _ j\in \mathrm{PSH}(X,\theta )_{>0}$ satisfying

8D5878FDF4FD 19.4.46
\begin{equation} P_{\theta }[\varphi ]_{\mathcal{I}}\geq \left(1-N^{-1}\right)\varphi _ j+N^{-1} \psi _ j. \end{equation}

Fix $j\geq j'$. It suffices to show that

DA123199D17C 19.4.47
\begin{equation} \Delta _{\nu }\left((1-N^{-1})\theta ,\varphi _{j}\right)+v'\subseteq \Delta ' \end{equation}

for some $v'\in \mathbb {R}^ n$. In fact, if this is true, we have

\[ \operatorname{vol}\Delta '\geq \operatorname{vol}\Delta _{\nu }\left((1-N^{-1})\theta ,\varphi _ j\right). \]

Letting $j\to \infty $ and applying corollary 16.9.36 and theorem 19.4.30, we conclude (19.4.45).

It remains to prove (19.4.47).

By 13.13.48, there is $g'>0$ such that for any $g\geq g'$, we can find a non-zero section

\[ s_ g\in \mathrm{H}^0\left(X,L^ g\otimes \mathcal I(g\psi _ j)\right). \]

By 5.18.15, after possibly increasing $g'$, for all $g\geq g'$,

\[ \mathcal I\left(gN\varphi _ j\right)\subseteq \mathcal I_\infty \left(g(N-1)\varphi _ j\right). \]

Moreover, the inequality (19.4.46) gives that for $g\geq g'$,

\[ \begin{aligned} \mathcal I(gN\varphi _ j)\cdot \mathcal I(g\psi _ j)\subseteq & \mathcal I_\infty \left(g(N-1)\varphi _ j\right)\cdot \mathcal I(g\psi _ j)\\ \subseteq & \mathcal I\Bigl (g(N-1)\varphi _ j+g\psi _ j\Bigr )\\ \subseteq & \mathcal I\Bigl (gN P_\theta [\varphi ]_{\mathcal I}\Bigr )\\ =& \mathcal I(gN\varphi ), \end{aligned} \]

where the second inclusion follows directly from the definition of $\mathcal I_\infty $. Thus multiplication by $s_ g$ gives an injective linear map

\[ \mathrm{H}^0\left(X,T\otimes L^{g(N-1)}\otimes \mathcal I(gN\varphi _ j)\right) \xrightarrow {\times s_ g} \mathrm{H}^0\left(X,T\otimes L^{gN}\otimes \mathcal I(gN\varphi )\right). \]

In particular, when $g=g_ i$ for some $i$ large enough, we then find

\[ \Delta _{g_ i,T}\left((N-1)\theta ,N\varphi _{j}\right)+(g_ i)^{-1}\nu (s_{g_ i})\subseteq N\Delta _{k_ i,T}(\theta ,\varphi ). \]

We observe that the $(g_ i)^{-1}\nu (s_{g_ i})$'s are bounded, since both convex bodies appearing in this equation remain bounded as $i$ varies. After passing to a subsequence, we may assume that $(g_ i)^{-1}\nu (s_{g_ i})$ converges. Then 19.4.43, followed by division by $N$, gives a vector $v'\in \mathbb {R}^ n$ such that (19.4.47) holds.

Step 2. Next we handle the general case.

Let $\Delta '$ be the Hausdorff limit of a subsequence of $(\Delta _{k,T}(\theta ,\varphi ))_ k$, say the subsequence with indices $k_1<k_2<\cdots $. By theorem 19.7.4, it suffices to prove that $\Delta '=\Delta _{\nu }(\theta ,\varphi )$.

Take $\psi \in \mathrm{PSH}(X,\theta )$ such that $\theta _{\psi }$ is a Kähler current and $\psi \leq \varphi $. The existence of $\psi $ follows from 13.13.47.

Then for any $\epsilon \in \mathbb {Q}\cap (0,1)$,

\[ \Delta _{k,T}(\theta ,\varphi )\supseteq \Delta _{k,T}\Bigl (\theta ,(1-\epsilon )\varphi +\epsilon \psi \Bigr ) \]

for all $k\geq 1$. It follows from Step 1 that

\[ \Delta ' \supseteq \Delta _{\nu }\Bigl (\theta ,(1-\epsilon )\varphi +\epsilon \psi \Bigr ). \]

As $\epsilon \to 0+$, we have

\[ (1-\epsilon )\varphi +\epsilon \psi \xrightarrow {d_ S}\varphi \]

by 16.9.25. Hence theorem 19.4.30 gives

\[ \Delta _{\nu }\Bigl (\theta ,(1-\epsilon )\varphi +\epsilon \psi \Bigr )\to \Delta _{\nu }(\theta ,\varphi ) \]

in the Hausdorff metric. It follows that $\Delta ' \supseteq \Delta _{\nu }(\theta ,\varphi )$.

It remains to establish that

CFA7D4F4C2EB 19.4.48
\begin{equation} \operatorname{vol}\Delta '\leq \operatorname{vol}\Delta _{\nu }(\theta ,\varphi ). \end{equation}

Fix an integer $N>0$, it suffices to argue that

05403B615855 19.4.49
\begin{equation} \operatorname{vol}\Delta '\leq \frac{1}{n!} \int _ X \left(N^{-1}\omega +\theta +\mathrm{dd}^{\mathrm{c}}P_{N^{-1}\omega +\theta }[\varphi ]_{\mathcal{I}}\right)^ n. \end{equation}

Assuming this, letting $N\to \infty $ and using 18.1.31 together with proposition 18.1.27 6, we conclude (19.4.48).

After adding a constant to $\varphi $, which does not change the multiplier ideals or the current $\theta +\mathrm{dd}^{\mathrm{c}}\varphi $, we may assume that $\varphi \leq 0$.

Step 2.1. We first reduce to the case $N|k_ i$ for all $i$.

For this purpose, we are free to replace $k_1<k_2<\cdots $ by a subsequence. We may then assume that $k_ i\equiv a$ modulo $N$ for all $i\geq 1$ for some $a\in \{ 0,1,\ldots ,N-1\} $. We write $k_ i=g_ iN +a$. Observe that

\[ \mathrm{H}^0\left(X,T\otimes L^{k_ i}\otimes \mathcal{I}(k_ i \varphi )\right)\subseteq \mathrm{H}^0\left(X, T\otimes L^ a \otimes L^{g_ i N}\otimes \mathcal{I}(g_ i N \varphi ) \right). \]

Up to replacing $T$ by $T\otimes L^ a$, we may assume that $a=0$.

Step 2.2. We write $k_ i=g_ i N$ for all $i$.

Take a non-zero section $s\in \mathrm{H}^0(X,H)$.

We have an injective linear map

\[ \mathrm{H}^0\left(X,T\otimes L^{gN}\otimes \mathcal{I}(gN\varphi )\right)\xrightarrow {\times s^ g}\mathrm{H}^0\left(X,T\otimes H^ g\otimes L^{gN}\otimes \mathcal{I}(gN\varphi )\right) \]

for each $g\geq 1$. In particular, for each $i\geq 1$,

\[ k_ i\Delta _{k_ i,T}(\theta ,\varphi )+g_ i\nu (s)\subseteq g_ i\Delta _{g_ i,T}\left(\omega +N\theta ,N\varphi \right). \]

Letting $i\to \infty $, by Step 1, we have

\[ N\Delta ' + \nu (s) \subseteq \Delta _{\nu }(\omega +N\theta ,N\varphi ). \]

So

\[ \operatorname{vol}\Delta '\leq \operatorname{vol}\Delta _{\nu }\left(N^{-1}\omega +\theta ,\varphi \right)=\frac{1}{n!}\int _ X \left(N^{-1}\omega +\theta +\mathrm{dd}^{\mathrm{c}}P_{N^{-1}\omega +\theta }[\varphi ]_{\mathcal{I}}\right)^ n. \]

This completes the proof. $\square$

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