Proof.
Let $s_ D$ be the canonical section of $\mathcal O_ X(D)$, with zero divisor $D$. For a real parameter $t>0$, define a smooth Hermitian metric on this line bundle by prescribing the norm of $s_ D$:
\[ |s_ D|_ t^2=(1+t|v|^2)^{-1}\quad \hbox{on }X\setminus D. \]
To check that it extends smoothly, use the coordinate $\xi =1/w$ near $D$. The squared norm of a local nonvanishing frame is
\[ \bigl (|\xi |^2+t|1-(\operatorname {Im}z)\xi |^2\bigr )^{-1}, \]
which is smooth and positive. The prescribed norm is invariant under the transformations on the complement of $D$, so these local extensions define a global metric. Its curvature form is
\[ \theta _ t=\mathrm{dd}^{\mathrm{c}}\log (1+t|v|^2) \quad \hbox{on }X\setminus D. \]
Set $\theta =\theta _1$, and let $\sigma =\sigma _0/\pi $ on $E$, where the denominator is the number $\pi $.
We now estimate the curvature from below. Put $r=|v|^2$ and let $H$ be the complex Hessian of $\log (1+tr)$ in the coordinates $(z,w)$. Direct differentiation gives
\[ \begin{split} H_{w\bar w}& =\frac{t}{(1+tr)^2},\\ H_{z\bar w}& =\frac{\mathrm i t(1-tv^2)}{2(1+tr)^2},\\ H_{z\bar z}& =\frac{t}{2(1+tr)} -\frac{t^2(\operatorname {Re}v)^2}{(1+tr)^2}. \end{split} \]
Consequently
\[ H_{z\bar z}-\frac{|H_{z\bar w}|^2}{H_{w\bar w}} =\frac{t(1-tr)}{4(1+tr)}\geq -\frac t4. \]
Completing the square gives $\theta _ t\geq -(t/4)\pi ^*\sigma $ on $X\setminus D$, and by continuity this inequality extends across $D$. The restriction of $\theta _ t$ to every fiber is a positive Fubini–Study form, including at infinity. Thus $\theta _ t+A\pi ^*\sigma $ is strictly positive off $D$ whenever $A>t/4$. At $\xi =0$, its coefficient matrix, with the common factor $\mathrm i/(2\pi )$ omitted, is
\[ \begin{pmatrix} A
& \mathrm i/2
\\ -\mathrm i/2
& 1/t
\end{pmatrix}. \]
Its vertical coefficient is positive and its Schur complement is $A-t/4>0$, so the form is strictly positive along $D$ as well. In particular, $\kappa =\theta +\pi ^*\sigma _0$ is Kähler.
The function
\[ f_ t=\log \frac{1+t|v|^2}{1+|v|^2} \]
extends smoothly across $D$ and satisfies $\theta _ t=\theta +\mathrm{dd}^{\mathrm{c}}f_ t$. Letting $t\downarrow 0$ in the curvature lower bound shows that the class of $\theta $ is nef in the sense of subsection 20.4.16.
Write $\psi _ D=\log |s_ D|_1^2$. By the Poincaré–Lelong formula, $\theta +\mathrm{dd}^{\mathrm{c}}\psi _ D=[D]$. Let $u\in \mathrm{PSH}(X,\theta )$. Then $u-\psi _ D$ is plurisubharmonic on $X\setminus D$. Its lift $\Phi (z,w)$ to $\mathbb C^2$ is invariant under the two deck transformations and, since $u$ is bounded above on the compact surface $X$, satisfies
\[ \Phi (z,w)\leq C+\log \bigl (1+|w-\operatorname {Im}z|^2\bigr ) \]
for some real constant $C$. For each fixed $w$, the function $z\mapsto \Phi (z,w)$ is either identically $-\infty $ or subharmonic. It is $1$-periodic and has logarithmic upper growth, so lemma 5.24.6 makes it constant. Thus $\Phi (z,w)=\phi (w)$, where $\phi $ is a subharmonic function of $w$, not identically $-\infty $. The second deck transformation gives $\phi (w+1)=\phi (w)$, and the bound at $z=0$ gives logarithmic growth, so the same lemma makes $\phi $ constant. Therefore $u=\psi _ D+C$ off $D$, and lemma 5.24.3 extends this equality across $D$. Hence $\theta +\mathrm{dd}^{\mathrm{c}}u=[D]$.
$\square$
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