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Proposition 21.13.2849A9A66B3A4D

Proposition 21.13.28.49A9A66B3A4D Let $\varphi \in \mathrm{PSH}_{\mathrm{tor}}(X,\theta )$. Then

04F5C34B36CA 21.13.29
\begin{equation} \operatorname{Trop}_* \left(\theta |_{T(\mathbb {C})}+\mathrm{dd}^{\mathrm{c}}\varphi |_{T(\mathbb {C})} \right)^ n=\operatorname{MA}_{\mathbb {R}}\left(F_{\varphi }\right). \end{equation}

In particular,

5FCC3FDF4C75 21.13.30
\begin{equation} \int _ X \theta _{\varphi }^ n =n! \operatorname{vol}\Delta (\theta ,\varphi ) \end{equation}

Proof. Let $F_0$ be a smooth convex function on $N_{\mathbb {R}}$ such that $\mathrm{dd}^{\mathrm{c}}\operatorname{Trop}^* F_0$ can be extended to a Kähler form on $X$. For example, Guillemin's construction (21.12.9) with respect to a suitable Delzant polytope gives such an example.

Write $\omega $ for a Kähler form on $X$ extending $\mathrm{dd}^{\mathrm{c}}\operatorname{Trop}^*F_0$. Then for any large enough $C>0$, $\theta +C\omega $ is a Kähler form. So we conclude from proposition 21.12.24 that

\[ \operatorname{Trop}_* \left((\theta +C\omega )|_{T(\mathbb {C})}+\mathrm{dd}^{\mathrm{c}}\varphi |_{T(\mathbb {C})} \right)^ n=\operatorname{MA}_{\mathbb {R}}(F_{\varphi }+CF_0). \]

By the multi-linearity of the non-pluripolar product proposition 13.11.4 6, the left-hand side is a polynomial in $C$. By the expansion formula for the mixed real Monge–Ampère measure theorem 21.11.58 1, the right-hand side is also a polynomial in $C$. We conclude that the same holds for $C=0$. Therefore, (21.13.29) follows.

(21.13.30) is a direct consequence of (21.13.29). $\square$

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