Pome

Proposition 14.9.1CA9F2EF1D149

Proposition 14.9.1.CA9F2EF1D149 For every smooth real $F$ on this threefold,

028038652BCC 14.9.2
\begin{align} \mathrm{e}^{D(F)}& =1+\int _ X|(u_ F)_ w|^2\, \mathrm{d}\nu , \\ \| u_ F-Au_ F\| _{L^2(X,\nu )}^2 & \leq 4\bigl (\mathrm{e}^{D(F)}-1\bigr ). \tag{14.9.3} \end{align}

Thus $D(F)\geq 0$, with equality if and only if $F=\pi ^*H$ for some $H\in C^\infty (\mathbb P^2,\mathbb R)$.

Proof. Integration of the equation and (23.1.5) give

\[ \mathrm{e}^{D(F)}=\frac16\int _ X(\omega +\mathrm{dd}^{\mathrm{c}}u_ F)^3 =1+\int _ X|(u_ F)_ w|^2\, \mathrm{d}\nu . \]

Substituting the first equality into (23.1.39) proves (14.9.3).

If $D(F)=0$, then $(u_ F)_ w=0$ everywhere, because $u_ F$ is smooth. Since $u_ F$ is real, it is constant on each connected fiber, so it descends to a smooth real function $q$ on $\mathbb P^2$, and $\omega _{\mathrm{FS}}+\mathrm{dd}^{\mathrm{c}}q>0$ as in the proof of proposition 23.1.38. Since $\beta ^2=0$ and $\omega =\pi ^*\omega _{\mathrm{FS}}+\beta $, we have

\[ (\omega +\mathrm{dd}^{\mathrm{c}}\pi ^*q)^3 =3\pi ^*(\omega _{\mathrm{FS}}+\mathrm{dd}^{\mathrm{c}}q)^2\wedge \beta . \]

Dividing by $\omega ^3=3\pi ^*\omega _{\mathrm{FS}}^2\wedge \beta $ and taking logarithms proves that $F$ is a smooth base pullback.

Conversely, suppose $F=\pi ^*H$. Apply theorem 14.2.1 on $(\mathbb P^2,\omega _{\mathrm{FS}})$ to obtain a smooth real $q$ and a scalar $c$ with

\[ \omega _{\mathrm{FS}}+\mathrm{dd}^{\mathrm{c}}q>0,\qquad (\omega _{\mathrm{FS}}+\mathrm{dd}^{\mathrm{c}}q)^2=\mathrm{e}^{H+c}\omega _{\mathrm{FS}}^2. \]

Since the base form is closed, Stokes' theorem gives $\mathrm{e}^ c\int _{\mathbb P^2}\mathrm{e}^ H\omega _{\mathrm{FS}}^2=1$. The preceding cube identity shows that $\pi ^*q$, after subtraction of its $\nu $-mean, solves the equation on $X$ with scalar $c$, and uniqueness gives $b(F)=c$. Since the base measure of $\nu $ is $\omega _{\mathrm{FS}}^2$, it follows that $D(F)=0$. $\square$

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