Pome

18.7 Limits of analytic envelopesE69A0F80536C

E69A0F80536C

By the curve construction of theorem 18.6.4, convergence of potentials alone does not determine the limit of their ideal envelopes. Two further conditions do: a common lower bound in the multiplier-ideal order, and convergence of all divisorial Lelong numbers. Together they force every cluster value of the envelopes to have the multiplier ideals of the limiting potential, and maximality of the envelope then identifies the cluster value. The dyadic analytic approximants satisfy both conditions.

In this section, $\theta $ is again an arbitrary smooth real $(1,1)$-form. We fix $u\in \mathrm{PSH}(X,\theta )$ and a Hermitian form $h$ on $X$, which will absorb the curvature errors of the approximants. Recall from section 5.38 that a local divisor $E$ over $X$ is a prime divisor on a smooth modification $\pi $ of a coordinate neighborhood in $X$, and that $\nu _ E(u)=\nu (u\circ \pi ,E)$ is the generic Lelong number of the pullback of $u$ along $E$.

Proposition 18.7.1.B727D2CB45A6 Let $\epsilon _ j\geq 0$ tend to zero, and let $a_ j\in \mathrm{PSH}(X,\theta +\epsilon _ jh)$ satisfy

\[ u\preceq _{\mathcal I}a_ j,\qquad \nu _ E(a_ j)\longrightarrow \nu _ E(u) \quad \text{for every local divisor }E\text{ over }X. \]

Then

\[ P_{\theta +\epsilon _ jh}[a_ j]_{\mathcal I} \longrightarrow P_\theta [u]_{\mathcal I} \quad \text{in }L^1. \]

If the $a_ j$ have analytic singularities, their ordinary envelopes converge to $P_\theta [u]$ in $L^1$ if and only if $P_\theta [u]=P_\theta [u]_{\mathcal I}$.

Proof. Set $p=P_\theta [u]_{\mathcal I}$ and $q_ j=P_{\theta +\epsilon _ jh}[a_ j]_{\mathcal I}$. Projection and the ideal order give

\[ p\leq P_{\theta +\epsilon _ jh}[p]_{\mathcal I}\leq q_ j\leq 0. \]

The first inequality holds because $p$ is a competitor in the larger background, and the second follows from proposition 18.4.6, since $p\sim _{\mathcal I}u\preceq _{\mathcal I}a_ j$. All $q_ j$ have supremum zero and belong to $\mathrm{PSH}(X,\theta +Ch)$ for a fixed $C\geq \sup _ j\epsilon _ j$. By normalized compactness, every subsequence therefore has a further subsequence converging in $L^1$. Let $q$ be such a limit. Passing to the limit in the current inequalities gives $q\in \mathrm{PSH}(X,\theta )$, and lemma 5.24.3 gives $p\leq q\leq 0$.

Fix a local modification $\pi :Z\to U$ and a prime divisor $E\subset Z$. By lemma 5.43.19, the chosen subsequence still converges in $L^1_{\mathrm{loc}}$ after pullback. Since $q_ j\sim _{\mathcal I}a_ j$, the two functions have the same divisorial Lelong numbers, and the pointwise semicontinuity in lemma 5.38.7 yields

\[ \nu _ E(q)\geq \limsup _ j\nu _ E(q_ j) =\lim _ j\nu _ E(a_ j)=\nu _ E(u). \]

Indeed, at every point of $E$ the pullback of each $q_ j$ has Lelong number at least $\nu _ E(q_ j)$; it remains to apply the pointwise inequality at a point of $E$ where the pullback of $q$ has Lelong number $\nu _ E(q)$. On the other hand, $p\leq q$ gives $\nu _ E(q)\leq \nu _ E(p)=\nu _ E(u)$. Thus $q$ and $u$ have the same Lelong numbers along all local divisors. Blowing up a point of any local modification recovers the pointwise Lelong number there as a generic divisorial number; on a curve the point is already a divisor. By theorem 5.37.3, $q\sim _{\mathcal I}u$.

Consequently $q$ is a competitor for $p$, so $q\leq p$. Every cluster value is therefore $p$, which proves convergence of the whole sequence. For analytic $a_ j$, proposition 18.4.8 identifies the ordinary and ideal envelopes, and the last assertion follows from uniqueness of $L^1$ limits and lemma 5.24.3. $\square$

The divisorial convergence follows from inclusions of multiplier ideals at fixed weights. The local Bergman estimate bounds the error in terms of the log discrepancy, and this error tends to zero after division by the weight.

Corollary 18.7.2.5AE1D9158EE3 Let $\epsilon _ j\geq 0$ tend to zero, and let $a_ j\in \mathrm{PSH}(X,\theta +\epsilon _ jh)$ satisfy $u\preceq _{\mathcal I}a_ j$. Suppose that, for every integer $m\geq 1$ and every $\delta >0$,

\[ \mathcal I((1+\delta )m a_ j)\subseteq \mathcal I(mu) \quad \text{for all sufficiently large }j. \]

Then the conclusions of proposition 18.7.1 hold.

Proof. Fix a local divisor $E$ over a coordinate neighborhood $U$, and write $A=A_ U(E)$ for its log discrepancy. By lemma 5.38.9, the assumed inclusion implies

\[ (1+\delta )m\nu _ E(a_ j) \geq \operatorname {ord}_ E\mathcal I((1+\delta )m a_ j) \geq \operatorname {ord}_ E\mathcal I(mu) \geq m\nu _ E(u)-A \]

for all large $j$. Taking the lower limit in $j$ first, and then letting $m\to \infty $ and $\delta \downarrow 0$, we obtain $\liminf _ j\nu _ E(a_ j)\geq \nu _ E(u)$. The opposite inequality $\nu _ E(a_ j)\leq \nu _ E(u)$ holds for every $j$ because $u\preceq _{\mathcal I}a_ j$. Hence proposition 18.7.1 applies. $\square$

The common ideal bound cannot be omitted, even when all divisorial Lelong numbers converge. In the atomic approximation of theorem 18.6.4, every individual atom can tend to zero while the limiting potential is not an ideal model.

Example 18.7.3.504A5958272F On a compact connected curve $Y$ with a positive form $\theta $ of total mass one, there are normalized $a_ j\in \mathrm{PSH}(Y,\theta )$ with analytic singularities and a smooth $u\in \mathrm{PSH}(Y,\theta )$ such that

\[ a_ j\longrightarrow u\text{ in }L^1,\qquad \nu _ E(a_ j)\longrightarrow \nu _ E(u)\text{ for every local divisor }E, \]

but $P_\theta [a_ j]=P_\theta [a_ j]_{\mathcal I}\to u\ne P_\theta [u]=P_\theta [u]_{\mathcal I}$ in $L^1$.

Proof. Choose $u$ smooth, nonconstant and normalized, with $\theta +\mathrm{dd}^{\mathrm{c}}u>0$, and apply the construction in theorem 18.6.4 to the smooth probability measure $\nu =\theta +\mathrm{dd}^{\mathrm{c}}u$. Since $\nu $ has no atoms, the largest mass of a cell tends to zero along partitions of vanishing diameter. Choose the rational approximations of the weights so that their total absolute error tends to zero. The resulting atomic probability measures $\nu _ j$ converge weakly to $\nu $, and their largest atoms tend to zero.

By the same theorem, their normalized Green potentials $a_ j$ have analytic singularities, satisfy $P_\theta [a_ j]=P_\theta [a_ j]_{\mathcal I}=a_ j$, and converge to $u$ in $L^1$. At every point $y\in Y$,

\[ 0\leq \nu (a_ j,y)=\nu _ j(\{ y\} ) \leq \max _{z\in Y}\nu _ j(\{ z\} )\longrightarrow 0=\nu (u,y). \]

Since local modifications of a smooth curve are isomorphisms, this gives all the required divisorial limits. As $u$ is bounded and $\theta >0$, both of its envelopes are zero, and since $u$ is not constant, the envelopes do not converge to them. Each $a_ j$ has a logarithmic pole, so $u\preceq _{\mathcal I}a_ j$ fails. $\square$

18.7.4 Dyadic regularization3A07CE3E627A

Demailly regularization provides the common ideal bound, since its approximants lie above $u$, and the Bergman estimate gives convergence of each divisorial Lelong number. Along dyadic indices, subadditivity of multiplier ideals also orders the ordinary singularity types of the approximants, which makes their envelopes decrease pointwise. This is the mechanism used in Theorem 18.1.2.

Apply theorem 5.36.1 to $u$, with $\gamma =-\theta $, along the indices $m_ j=2^ j$, starting at a sufficiently large index. Denote the resulting potentials by $a_ j$, and choose numbers $\epsilon _ j>0$ decreasing to zero such that

E93CF05C13A8 18.7.5
\begin{equation} a_ j\in \mathrm{PSH}(X,\theta +\epsilon _ jh),\qquad a_ j\geq u,\qquad a_ j\text{ has type }(1/m_ j,\mathcal I(m_ ju)). \end{equation}

These approximants satisfy $a_ j\to u$ in $L^1$. Their values need not decrease, but their ordinary singularity types do: the subadditivity property in (5.37.6) gives

\[ \mathcal I(2m_ ju)\subseteq \mathcal I(m_ ju)^2, \qquad a_{j+1}\preceq a_ j, \]

where the ordinary comparison follows by taking logarithms of local generators, with a constant that may depend on $j$.

Theorem 18.7.6.EA60F3EAF248 For every $u\in \mathrm{PSH}(X,\theta )$ and every choice in (18.7.5), put

\[ q_ j=P_{\theta +\epsilon _ jh}[a_ j]. \]

Then $q_ j$ has analytic singularities, and

\[ q_ j=P_{\theta +\epsilon _ jh}[a_ j]_{\mathcal I} \searrow P_\theta [u]_{\mathcal I} \]

pointwise and in $L^1$. The limit is independent of the choice of the approximants $a_ j$, of the error bounds $\epsilon _ j$ and of the metric $h$.

Proof. By proposition 18.4.8, $q_ j=P_{\theta +\epsilon _ jh}[a_ j]_{\mathcal I}\sim a_ j$. Since the backgrounds decrease and $a_{j+1}\preceq a_ j$, the function $q_{j+1}$ is a competitor for $P_{\theta +\epsilon _ jh}[a_ j]$. Hence $q_{j+1}\leq q_ j$.

The inequality $a_ j\geq u$ gives $u\preceq _{\mathcal I}a_ j$. For every local divisor $E$, lemma 5.38.9 gives

\[ \nu _ E(a_ j)=\frac1{m_ j}\operatorname {ord}_ E\mathcal I(m_ ju) \longrightarrow \nu _ E(u). \]

By proposition 18.7.1, $q_ j\to p:=P_\theta [u]_{\mathcal I}$ in $L^1$, and $p\leq q_ j\leq 0$. The decreasing limit of the $q_ j$ is therefore bounded below by $p$; it is a $\theta $-plurisubharmonic function that agrees with $p$ almost everywhere, hence everywhere. This identifies the limit in terms of $\theta $ and the multiplier-ideal class of $u$ alone, which proves the asserted independence. $\square$

Corollary 18.7.7.E941DFE18F1D For the sequence above, the following are equivalent:

\[ P_\theta [u]=P_\theta [u]_{\mathcal I},\qquad q_ j\longrightarrow P_\theta [u]\text{ in }L^1, \qquad q_ j\searrow P_\theta [u]\text{ pointwise}. \]

They hold for one choice in (18.7.5) if and only if they hold for every such choice. For the fixed volume form $\mathrm{d}V$,

\[ \lim _ j\int _ X(q_ j-P_\theta [u])\, \mathrm{d}V =\int _ X(P_\theta [u]_{\mathcal I}-P_\theta [u])\, \mathrm{d}V\geq 0, \]

and the vanishing of this limit is a further equivalent condition.

Proof. The theorem identifies both limits of the $q_ j$ as $P_\theta [u]_{\mathcal I}$ for every such choice, and its $L^1$ convergence gives the integral formula. By proposition 18.4.4, the limiting difference is nonnegative. Its integral therefore vanishes exactly when the two envelopes agree almost everywhere, hence everywhere by lemma 5.24.3. This proves all the equivalences. $\square$

18.7.8 Absorbing the curvature error13DB6841F63C

When $\theta =\omega $ is Hermitian, we can take $h=\omega $, and dividing the approximants by $1+\epsilon _ j$ absorbs the curvature error. If the error bounds are rational, the analytic coefficients remain rational, so the whole approximation takes place in the fixed class $\mathrm{PSH}(X,\omega )$.

Corollary 18.7.9.A08D826CFAD4 Let $\omega $ be Hermitian and let $u\in \mathrm{PSH}(X,\omega )$. There are $b_ j\in \mathrm{PSH}(X,\omega )$ with analytic singularities and decreasing ordinary singularity types, such that $b_ j\to u$ in $L^1$ and

\[ P_\omega [b_ j]=P_\omega [b_ j]_{\mathcal I}\searrow P_\omega [u]_{\mathcal I}. \]

Consequently the classes of potentials with analytic singularities are dense in the whole metric space of ideal classes of proposition 18.6.1. The equality $P_\omega [u]=P_\omega [u]_{\mathcal I}$ is equivalent to convergence of these ordinary envelopes to $P_\omega [u]$ in $L^1$.

Proof. Use $h=\omega $ in (18.7.5). Enlarge the error bounds to positive rational numbers $\epsilon _ j\downarrow 0$, and set

\[ c_ j=\frac1{1+\epsilon _ j},\qquad b_ j=c_ ja_ j. \]

Then $c_ j\uparrow 1$ is rational and

\[ \omega +\mathrm{dd}^{\mathrm{c}}b_ j =c_ j\bigl ((1+\epsilon _ j)\omega +\mathrm{dd}^{\mathrm{c}}a_ j\bigr )\geq 0. \]

The analytic coefficient of $b_ j$ is $c_ j/m_ j$. Moreover $b_ j\to u$ in $L^1$, since $a_ j\to u$ there and the sequence has bounded $L^1$ norm. Because $a_{j+1}\preceq a_ j$, $c_{j+1}\geq c_ j$, and each $a_ j$ is bounded above, one has $b_{j+1}\preceq b_ j$.

Put $q_ j=P_{(1+\epsilon _ j)\omega }[a_ j]=P_{(1+\epsilon _ j)\omega }[a_ j]_{\mathcal I}$. The preceding theorem gives $q_ j\searrow P_\omega [u]_{\mathcal I}$ pointwise and in $L^1$. Since $b_ j$ has analytic singularities, proposition 18.4.8 and the homogeneity in proposition 18.4.6 give

\[ r_ j:=P_\omega [b_ j]=P_\omega [b_ j]_{\mathcal I}=c_ jq_ j. \]

Here $q_ j\leq 0$ decreases and $c_ j\uparrow 1$, so $r_ j$ also decreases, with pointwise limit $P_\omega [u]_{\mathcal I}$. Moreover

\[ P_\omega [u]_{\mathcal I}\leq q_ j\leq r_ j\leq 0. \]

Since the lower bound is integrable, dominated convergence gives convergence in $L^1$.

The distance in proposition 18.6.1 from $[b_ j]_{\mathcal I}$ to $[u]_{\mathcal I}$ is exactly the $L^1$ distance from $r_ j$ to $P_\omega [u]_{\mathcal I}$, so it tends to zero. The last assertion follows because the limit of the $r_ j$ has been identified. $\square$

Cite this page

Comments

Corrections, questions, and mathematical discussion are welcome. Sign in with GitHub to comment. Comments are public.