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Theorem 20.4.26400A4F39FD56

Theorem 20.4.26.400A4F39FD56 For a smooth compact modification $g:Z'\to Z$ over $Y$, there is a unique finite effective real divisor $E_ g$ supported on the exceptional locus of $g$ such that

D5C95521E68E 20.4.27
\begin{equation} S_{Z'}=g^*S_ Z+[E_ g]. \end{equation}

For a further smooth compact modification $h:Z''\to Z'$, these divisors satisfy

398DC29813C5 20.4.28
\begin{equation} E_{g\circ h}=E_ h+h^*E_ g. \end{equation}

Their coefficients are additive and positively homogeneous in the ambient potential $u$.

For every $m$, the analytic-ideal divisors on the two models differ by a finite effective divisor $E_{m,g}$ supported on the exceptional locus:

\[ [E_{m,g}]=D_{m,Z'}-g^*D_{m,Z}. \]

For every Gauduchon metric $\gamma '$ on $Z'$, the measures

\[ [E_{m,g}]\wedge (\gamma ')^{r-1} \longrightarrow [E_ g]\wedge (\gamma ')^{r-1} \]

converge in total variation.

Proof. Step 1: the exceptional divisor. Enumerate the prime divisors on $Z$ with positive trace coefficient. By theorem 20.4.5, the pullback of every finite partial sum of $S_ Z$ is at most $S_{Z'}$, and corollary 20.4.24 identifies the increasing limit of these pullbacks with $g^*S_ Z$. Thus $S_{Z'}-g^*S_ Z$ is a positive closed divisorial current. The two currents have equal coefficients along the strict transform of every prime divisor on $Z$, because these coefficients are computed by the same valuation. Every other prime divisor on $Z'$ is exceptional for $g$, and the exceptional analytic set has only finitely many irreducible components on the compact manifold $Z'$. Hence the difference is the integration current of a finite effective real divisor $E_ g$ supported on its divisorial components, and the coefficients of integration currents determine $E_ g$ uniquely.

Step 2: the cocycle identity. Pullback of positive closed $(1,1)$-currents is functorial, since it is defined by composing local plurisubharmonic potentials. Using (20.4.27) for $h$ and for $g$ gives

\[ S_{Z''}=h^*S_{Z'}+[E_ h] =(g\circ h)^*S_ Z+[h^*E_ g]+[E_ h], \]

and uniqueness gives (20.4.28). Additivity and positive homogeneity follow from the same properties of the trace coefficients and the linearity of pullback.

Step 3: approximation. For fixed $m$, apply (20.4.6) to the finitely many prime divisors in the support of the image ideal on $Z$. After division by $m$, it gives $D_{m,Z'}-g^*D_{m,Z}\geq 0$. The coefficients along strict transforms vanish, so this difference is the integration current of an effective real divisor $E_{m,g}$ supported on the exceptional locus.

Choose also a Gauduchon metric $\gamma $ on $Z$. By theorem 20.4.2, the currents $S_ Z-D_{m,Z}$ and $S_{Z'}-D_{m,Z'}$ are positive, and their trace masses tend to zero. Subtracting the two identities for the exceptional currents gives

\[ [E_{m,g}]-[E_ g] =-(S_{Z'}-D_{m,Z'})+g^*(S_ Z-D_{m,Z}), \]

where both $S_{Z'}-D_{m,Z'}$ and $g^*(S_ Z-D_{m,Z})$ are positive. By (20.4.23), the total variation of the signed measure $([E_{m,g}]-[E_ g])\wedge (\gamma ')^{r-1}$ is therefore at most

\[ \int _{Z'}(S_{Z'}-D_{m,Z'})\wedge (\gamma ')^{r-1} +C_ g\int _ Z(S_ Z-D_{m,Z})\wedge \gamma ^{r-1}. \]

Both terms tend to zero, which proves convergence in total variation. $\square$

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