Proposition 12.36.1.3A78333ED147 The divisorial threshold is $\tau _\omega (H)=1$. For $\mu _0=\omega ^3/6$ and $0\leq a\leq 1$,
\[ \mathcal V_{\mu _0}(\omega ;aH)=6(1-a)^2. \]
For $a<1$ this is the scalar of the equation solved, as in theorem 12.35.4, by $a\sigma _ H$ plus a smooth function. At $a=1$ the residual background is nef, and the logarithmic potential $\sigma _ H$ has zero non-pluripolar Monge–Ampère measure. For $a<1$, every residual background has infinite upper mass.
Proof.
The residual background is
\[ R_ a=(1-a)\alpha +\zeta . \]
It is positive for $0\leq a<1$ and semipositive for $a=1$, so every coefficient $a\leq 1$ is feasible. For the reverse inequality, consider the metrics $\gamma _ t=\alpha +t\zeta $, $t>0$. They are Gauduchon, since
\[ \mathrm{dd}^{\mathrm{c}}(\gamma _ t^2)=-2t\alpha ^3=0. \]
Using $\zeta ^2=0$, we obtain
\[ \frac{\int _ X\omega \wedge \gamma _ t^2}{\deg _{\gamma _ t}H} =\frac{1+2t}{2t}\longrightarrow 1\qquad (t\to \infty ), \]
and the threshold formula gives $\tau _\omega (H)=1$.
For $a<1$,
\[ R_ a^3=3(1-a)^2\alpha ^2\wedge \zeta =(1-a)^2\omega ^3=6(1-a)^2\mu _0. \]
Hence the zero potential solves the residual smooth equation, and uniqueness of the scalar gives the volume. At $a=1$, the form $R_1=\zeta $ is nef, because $\zeta +\epsilon \omega >0$ for $\epsilon >0$, and the same computation gives
\[ \mathcal V_{\mu _0}(\zeta +\epsilon \omega ) =6\epsilon ^2(1+\epsilon )\longrightarrow 0. \]
By theorem 12.11.1, the residual volume at $a=1$ is zero. Moreover $\omega +\mathrm{dd}^{\mathrm{c}}\sigma _ H=[H]+\zeta $, so the non-pluripolar measure of $\sigma _ H$ is $\zeta ^3=0$.
Finally, fix $a<1$ and choose $0<\delta \leq \min \{ 1-a,1\} $, so that $R_ a-\delta \omega \geq 0$. For the smooth functions $V_ j$ of theorem 23.1.1,
\[ R_ a+\mathrm{dd}^{\mathrm{c}}(\delta V_ j) =(R_ a-\delta \omega )+\delta (\omega +\mathrm{dd}^{\mathrm{c}}V_ j)>0. \]
Monotonicity of the determinant on positive matrices bounds the mass of this form below by $\delta ^3\int _ X(\omega +\mathrm{dd}^{\mathrm{c}}V_ j)^3$, which tends to infinity. Thus a finite residual volume and an explicit divisorial threshold coexist with unbounded upper mass.
$\square$
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