Lemma 19.4.44.F3D0645BDF93 Assume that $\theta _{\varphi }$ is a Kähler current. Then as $\mathbb {Q}\ni \beta \to 0+$, we have
Lemma 19.4.44F3D0645BDF93
Proof. By proposition 19.4.33 and proposition 19.4.28, we have
for any small enough $\beta \in \mathbb {Q}_{>0}$. In particular, if $\Delta '$ is the Hausdorff limit of a subnet of $(\Delta ((1-\beta )\theta ,\varphi ))_{\beta }$, then $\Delta '\subseteq \Delta _{\nu }(\theta ,\varphi )$. But
Since we have not developed the theory of nef b-divisors yet, we give a direct proof as well. Take a Kähler form $\omega $ so that $\theta _{\varphi }\geq \omega $. Let $\psi =P_{\theta -\omega }[\varphi ]_{\mathcal{I}}$. Then $\varphi \sim _{\mathcal{I}}\psi $. In order to establish the last equality, we may replace $\varphi $ by $\psi $ and hence assume that $\varphi $ is $\mathcal{I}$-good. For small enough $\beta >0$, the form $(1-\beta )\theta -(\theta -\omega )=\omega -\beta \theta $ is Kähler, so this remains true in the class $(1-\beta )\{ \theta \} $ by 18.1.8. Thus the equality of masses in an $\mathcal{I}$-equivalence class reduces the desired equality to
which is obvious.
It follows that $\Delta '=\Delta _{\nu }(\theta ,\varphi )$. We conclude by theorem 19.7.4. $\square$
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