Pome

12.10.28 Two attained instances244D24A4396B

Example 12.10.29.E97964925666 On the Hopf surface $X=(\mathbb C^2\setminus \{ 0\} )/\langle z\mapsto 2z\rangle $, the background $\omega =|z|^{-2}\mathrm{dd}^{\mathrm{c}}|z|^2$ satisfies $\mathrm{dd}^{\mathrm{c}}\omega =0$, so its Monge–Ampère mass is invariant. There are smooth densities whose threshold solutions are smooth and nonconstant and whose maximizing tests are smooth strictly positive forms.

Proof. The form is invariant under $z\mapsto 2z$, so it descends to $X$, and it is positive. For $s=|z|^2$ and $F(s)=s^{-1}$, the identity $sF''+2F'=0$ gives $\mathrm{dd}^{\mathrm{c}}\omega =\mathrm{dd}^{\mathrm{c}}(s^{-1})\wedge \mathrm{dd}^{\mathrm{c}}s=0$, while $\omega $ is not closed. Choose a nonconstant smooth real $q$ and small nonzero $\varepsilon $ such that $A=\omega +\mathrm{dd}^{\mathrm{c}}(\varepsilon q)>0$. Put $V=\int _ X\omega ^2$, $\mathrm{d}V=\omega ^2/V$, $f=A^2/\mathrm{d}V$ and $u=\varepsilon q-\sup _ X\varepsilon q$. Invariance of the mass gives $\int _ Xf\, \mathrm{d}V=\int _ XA^2=V$, hence $b_\omega (f)=1$ by theorem 12.10.23.

The form $T=A/V$ satisfies $\mathrm{dd}^{\mathrm{c}}T=0$, $\int _ X\omega \wedge T=1$ and $D_{\sqrt f}(T)=1$. For every smooth strictly positive $Q\in \mathscr G_\omega $, the arithmetic–geometric mean inequality and Stokes' theorem give $D_{\sqrt f}(Q)\leq \int _ XA\wedge Q=1$. Thus $T$ is a smooth strictly positive maximizer, and since $u$ is a threshold solution with supremum zero, corollary 12.10.12 gives $\Phi _ f=u$. This is a bounded nonconstant example. $\square$

Example 12.10.30.4C03E42B184D Let $n\geq 3$, and view the smooth quadric of dimension $n$ as a double cover of $\mathbb P^ n$. For the restricted Fubini–Study form and a suitable smooth density, the maximizing test is a smooth semipositive form whose smooth root has rank at least two everywhere and degenerates along the ramification divisor.

Proof. Let

\[ X=\{ [w:z_0:\cdots :z_ n]:w^2=\textstyle \sum _{i=0}^ nz_ i^2\} \subset \mathbb P^{n+1},\qquad F([w:z])=[z]. \]

The quadratic form is nonsingular, and $F$ is finite of degree two, with smooth ramification divisor $Z=\{ w=0\} $. Local branch coordinates show that $\mathrm dF$ has rank $n-1$ on $Z$ and $n$ elsewhere. Let $\omega $ be the restriction to $X$ of the normalized Fubini–Study form of $\mathbb P^{n+1}$, and let $A=F^*\omega _{\mathrm{FS}}$, where $\omega _{\mathrm{FS}}$ is the normalized Fubini–Study form of $\mathbb P^ n$. Then

\[ u=\log \frac{\sum _ i|z_ i|^2}{|w|^2+\sum _ i|z_ i|^2} \]

is a smooth function on $X$ with $-\log 2\leq u\leq 0$, $\sup _ Xu=0$ and $A=\omega +\mathrm{dd}^{\mathrm{c}}u$. The change of variables for the branched cover gives $\int _ XA^ n=2$, and Stokes' theorem gives $V=\int _ X\omega ^ n=2$.

Set $\mathrm{d}V=\omega ^ n/V$, $f=A^ n/\mathrm{d}V$, $T=A^{n-1}/V$ and $\gamma =A/V^{1/(n-1)}$. Since $\omega $ is closed, theorem 12.10.23 gives $b_\omega (f)=V/\int _ Xf\, \mathrm{d}V=1$. Stokes' theorem gives $\mathrm{dd}^{\mathrm{c}}T=0$ and $\int _ X\omega \wedge T=1$, and computing the determinant density gives $D_{f^{1/n}}(T)=1$. The arithmetic–geometric mean inequality, which remains valid for semipositive $A$, bounds $D_{f^{1/n}}(Q)$ by $\int _ XA\wedge Q=1$ for every smooth strictly positive $Q\in \mathscr G_\omega $. Thus $T$ is a maximizer, strictly positive off the proper analytic set $Z$, and theorem 12.10.17 gives $\Phi _ f=u$. Its root $\gamma $ has rank $n-1\geq 2$ on $Z$ and is positive elsewhere, as required. $\square$

The invariant-mass and sublinear conditions settle the envelope condition only in special situations. We do not know whether general moment or entropy bounds imply either of them, or the hypothesis on the smooth root.

Corollary 12.10.31.2A3A58A80CB4 Under the hypotheses of theorem 12.10.17, suppose in addition that $f\in L^ p(\mathrm{d}V)$ for some $p>1$. Then the normalized threshold solution $u_0$ is continuous, and the normalized greatest exponential solutions converge uniformly to $u_0$ as the exponent tends to zero.

Proof. By proposition 15.28.7, the constant $c$ for which $\mathrm{MA}_\omega (v)=cf\, \mathrm{d}V$ has a continuous solution is $b_\omega (f)$. The continuous normalized solution is therefore a threshold solution, and it equals $u_0$ by the uniqueness in theorem 12.10.17. For $L^ p$ data the greatest exponential solution coincides with the bounded solution, as explained after theorem 15.35.2. By proposition 15.20.1, applied with the trivial group, the normalized family is uniformly precompact, and every cluster limit solves the threshold equation. Uniqueness identifies every cluster limit with $u_0$, which proves uniform convergence of the whole family. $\square$

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