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.
Example 12.10.29E97964925666
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. $\square$
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