Theorem 15.32.1.D988D47D5E0E Suppose $f_ j,f$ are nonzero nonnegative $L^1$ densities and $f_ j\to f$ in $L^1(\mathrm{d}V)$. Then
Moreover,
ACC15559958B
15.32.2
and the suprema are finite for sufficiently small $\delta $.
06284CD8A9D406284CD8A9D4
We now study how the threshold $b_ h(f)$ depends on $f$. By (15.29.3), $b_ h^{1/n}$ is an infimum of functions that are continuous on $L^1$, and is therefore upper semicontinuous. It is not continuous in general: when $v_-(h)=0$, every density with positive threshold is an $L^1$ limit of densities with zero threshold. For density roots, (15.29.2) expresses $\rho _ h$ as a supremum of positive linear functionals. Hence $\rho _ h$ is a norm on the space where it is finite, this space is complete for a suitable norm, and the threshold depends continuously on the root in that norm.
Theorem 15.32.1.D988D47D5E0E Suppose $f_ j,f$ are nonzero nonnegative $L^1$ densities and $f_ j\to f$ in $L^1(\mathrm{d}V)$. Then
Moreover,
ACC15559958B
15.32.2
and the suprema are finite for sufficiently small $\delta $.
Proof. For a Gauduchon form $\gamma $ on $X$, write $A_\gamma (f)=\int _ X(f\, \mathrm{d}V/\gamma ^ n)^{1/n}\gamma ^ n$. Since $|s^{1/n}-t^{1/n}|\leq |s-t|^{1/n}$ for $s,t\geq 0$, Hölder's inequality shows that $A_\gamma $ is continuous on $L^1$; it is positive at every nonzero nonnegative density. By theorem 15.29.1, $b_ h^{1/n}$ is the infimum over $\gamma $ of the continuous positive functions $f\mapsto \int _ Xh\wedge \gamma ^{n-1}/A_\gamma (f)$. It is therefore upper semicontinuous, and testing a single $\gamma $ bounds it above on an $L^1$ neighborhood of $f$.
For the second assertion, recall that $b_ h(q)=c_ h(q)$ for bounded $q$ (proposition 15.28.7). By the first assertion, $\limsup _ jc_ h(q_ j)\leq b_ h(f)$ for every sequence of nonzero nonnegative bounded densities $q_ j\to f$ in $L^1$. Hence the limit in (15.32.2) is at most $b_ h(f)$, and the local upper bound makes the suprema finite for small $\delta $. Conversely, the truncations $f_ k$ converge to $f$ in $L^1$ and satisfy $c_ h(f_ k)\geq b_ h(f)$, so every supremum in (15.32.2) is at least $b_ h(f)$. $\square$
Since $b_ h\geq 0$, upper semicontinuity makes $b_ h$ continuous at every density where it vanishes. If $v_-(h)=0$, these are its only points of continuity. Indeed, let $b_ h(f)>0$ and $g=f/\int _ Xf\, \mathrm{d}V$. By corollary 15.27.6 and theorem 15.28.4, the densities $(1-t)g+tf_0$, where $f_0$ is the density of theorem 15.27.3, have zero threshold and converge to $g$ in $L^1$ as $t\downarrow 0$; multiplying them by $\int _ Xf\, \mathrm{d}V$ gives densities with zero threshold converging to $f$. These statements concern only the scalar $b_ h$; they say nothing about capacity convergence of the corresponding potentials or about the limits of their Monge–Ampère measures.
3DD22F1D6AC3Since (15.29.2) expresses $\rho _ h(p)$ as a supremum of positive linear functionals evaluated at $|p|$, the root functional is homogeneous, monotone and subadditive. Subadditivity shows that the sum of two densities with positive threshold again has positive threshold. In the statements below, $f$ and $g$ are nonzero nonnegative $L^1$ densities, and $p$ and $q$ are real or complex functions in $L^ n$.
Proposition 15.32.4.D697A55DE07C The functional $\rho _ h$ satisfies $\rho _ h(tp)=|t|\rho _ h(p)$ for scalars $t\ne 0$, $\rho _ h(p)\leq \rho _ h(q)$ whenever $|p|\leq |q|$, and
In particular, if $b_ h(f),b_ h(g)>0$, then
Proof. By (15.29.2), $\rho _ h(p)=\sup _\gamma L_{h,\gamma }(|p|)$ is a supremum of positive linear functionals evaluated at $|p|$. This gives homogeneity and monotonicity, and, together with $|p+q|\leq |p|+|q|$, the triangle inequality. Finally, $(f+g)^{1/n}\leq f^{1/n}+g^{1/n}$ gives
which is equivalent to the asserted lower bound for $b_ h(f+g)$. $\square$
Proposition 15.32.5.4C06D1B94BD1 The real or complex vector space
is complete for the norm $\| p\| _{\mathcal D_ h}=\| p\| _{L^ n}+\rho _ h(p)$. It is an order ideal in $L^ n$: if $q\in \mathcal D_ h$ and $|p|\leq |q|$, then $p\in \mathcal D_ h$. It contains $L^\infty $ and is therefore dense in $L^ n$ for the $L^ n$ norm.
Moreover, $\mathcal D_ h=L^ n$ if and only if $v_-(h)>0$, and in that case the norm $\| \cdot \| _{\mathcal D_ h}$ is equivalent to the $L^ n$ norm. If $h$ is Kähler, then
Proof. By proposition 15.32.4, $\mathcal D_ h$ is a vector space and an order ideal, and $\| \cdot \| _{\mathcal D_ h}$ is a norm on it. Bounded functions belong to $\mathcal D_ h$, because $b_ h(|p|^ n)=c_ h(|p|^ n)>0$ for bounded nonzero $p$.
We next show that $\rho _ h$ is lower semicontinuous on $L^ n$. If $p_ j\to p$ in $L^ n$, then $|p_ j|^ n\to |p|^ n$ in $L^1$, and the upper semicontinuity of $b_ h$ in theorem 15.32.1 gives
This includes the case $b_ h(|p|^ n)=0$, in which the right side must be infinite; for $p=0$ the inequality is trivial. Now let $(p_ j)$ be a Cauchy sequence in $\mathcal D_ h$. It converges in $L^ n$ to some $p$, and lower semicontinuity gives $\rho _ h(p)\leq \liminf _ j\rho _ h(p_ j)<+\infty $, so $p\in \mathcal D_ h$. Applied to $p_ j-p_ k$ as $k\to \infty $, lower semicontinuity also gives
which tends to zero as $j\to \infty $. Together with $L^ n$ convergence, this proves completeness.
If $v_-(h)>0$, proposition 15.28.7 gives $\rho _ h(p)\leq v_-(h)^{-1/n}\| p\| _{L^ n}$, so $\mathcal D_ h=L^ n$ with an equivalent norm. If $v_-(h)=0$, the density $f$ of theorem 15.27.3 has $b_ h(f)=0$ by theorem 15.28.4; thus $f^{1/n}$ belongs to $L^ n$ but not to $\mathcal D_ h$. The Kähler formula follows from the same proposition. $\square$
Thus, when the lower mass vanishes, $\mathcal D_ h$ is a proper dense subspace of $L^ n$, complete for the stronger norm $\| \cdot \| _{\mathcal D_ h}$; its nonnegative elements are the $n$th roots of the densities admitting a positive scaled subsolution. A finite sum of such densities again admits a positive scaled subsolution, but a convergent infinite sum need not: the smooth summands in theorem 15.27.3 give an example. By proposition 15.29.5, the space $\mathcal D_ h$ does not depend on the Hermitian form $h$, and the norms $\| \cdot \| _{\mathcal D_ h}$ for different Hermitian forms are equivalent. The closure of the bounded functions for this norm is studied in 15.32.7.
The restriction of $\rho _ h$ to $\mathcal D_ h$ is itself a norm: if $p\ne 0$, then $\rho _ h(p)\geq L_{h,\gamma }(|p|)>0$ for any Gauduchon form $\gamma $. Whether this weaker norm is complete depends on the upper mass.
Proposition 15.32.6.C926F63790E3 The norm $\rho _ h$ is complete on $\mathcal D_ h$ if and only if $v_+(h)<+\infty $. When the upper mass is finite,
so $\rho _ h$ and $\| \cdot \| _{\mathcal D_ h}$ are equivalent norms.
Proof. Suppose $v_+(h)<+\infty $. A continuous solution for a bounded density $q$ has mass $c_ h(q)\int _ Xq\, \mathrm{d}V\leq v_+(h)$. Applying this to the truncations of $|p|^ n$ and letting the truncation level increase gives $b_ h(|p|^ n)\| p\| _{L^ n}^ n\leq v_+(h)$, which is the asserted inequality. Hence $\rho _ h$ and $\| \cdot \| _{\mathcal D_ h}$ are equivalent, and completeness follows from proposition 15.32.5.
Suppose instead that $v_+(h)=+\infty $. By theorem 12.15.4, theorem 12.2.3, the normalization scalars of smooth strictly positive probability densities are unbounded above. For each $j$, choose such a density $f_ j$ with
Then $\| p_ j\| _{L^ n}=j$ and $\rho _ h(p_ j)=jc_ h(f_ j)^{-1/n}\leq 2^{-j}$, so the partial sums $P_ N=\sum _{j\leq N}p_ j$ form a Cauchy sequence for $\rho _ h$.
Fix a Gauduchon form $\gamma $. Its coefficient $a_\gamma $ is bounded below by a positive constant, so (15.29.2) gives $\rho _ h(p)\geq c\| p\| _{L^1}$ with a constant $c>0$. Hence $\sum _ jp_ j$ converges in $L^1$ to a nonnegative function $P$. If $P_ N$ converged for $\rho _ h$ to an element of $\mathcal D_ h$, that element would also be the $L^1$ limit, hence equal to $P$ almost everywhere. But $P\geq p_ j$ gives $\| P\| _{L^ n}\geq j$ for every $j$, so $P\notin L^ n$. Therefore $\rho _ h$ is not complete. $\square$
The two mass properties play separate roles: positive lower mass makes every $L^ n$ function admissible, whereas finite upper mass makes the root norm control the $L^ n$ norm. The norm $\| \cdot \| _{\mathcal D_ h}$ is complete without either assumption.
All four combinations occur. On a compact Kähler manifold both mass properties hold. The Hopf threefold has positive lower mass and infinite upper mass (corollary 23.1.40). The elliptic threefold of theorem 12.19.1 has zero lower mass, and finite upper mass for its balanced metric (proposition 12.19.18). The product manifolds of corollary 12.19.16 have zero lower mass and infinite upper mass. Since neither $\mathcal D_ h$ nor the completeness of $\rho _ h$ depends on the choice of $h$ (proposition 15.29.5, proposition 13.14.15), we obtain the following table.
Manifold | Domain $\mathcal D_ h$ | Is $\rho _ h$ complete? |
Kähler manifold | $L^ n$ | Yes |
Hopf threefold | $L^ n$ | No |
Elliptic threefold | $\mathcal D_ h\subsetneq L^ n$ | Yes |
Product example | $\mathcal D_ h\subsetneq L^ n$ | No |
1BD556522380Bounded functions are dense in $\mathcal D_ h$ for the $L^ n$ norm, but not obviously for the norm $\| \cdot \| _{\mathcal D_ h}$. Let $\mathcal D_ h^0$ denote the closure of $L^\infty $ in $\mathcal D_ h$ for this norm. We show that a function belongs to $\mathcal D_ h^0$ exactly when its tails are small uniformly over all Gauduchon tests. The basic tool is a subcritical estimate. For every $r>n$,
CA92BD48A42D
15.32.8
where the constant $C_ r$ depends on $h$, the reference volume and $r$, but not on $p$. Indeed, for nonzero $p\in L^ r$ the density $|p|^ n$ belongs to $L^{r/n}$, so $b_ h(|p|^ n)=c_ h(|p|^ n)$ by proposition 15.28.7, and the lower-density estimate of theorem 14.19.19, with exponent $r/n$, gives $c_ h(|p|^ n)\| |p|^ n\| _{L^{r/n}}\geq c_{r/n}>0$.
Proposition 15.32.9.2210D4123A64 For $p\in \mathcal D_ h$, the following conditions are equivalent:
$p\in \mathcal D_ h^0$;
$\rho _ h(|p|\mathbf1_{\{ |p|>K\} })\to 0$ as $K\to \infty $;
whenever $|q_ j|\leq |p|$ and $q_ j\to 0$ in measure, one has $\| q_ j\| _{\mathcal D_ h}\to 0$.
By (15.29.2), the second condition can be written as
The space $\mathcal D_ h^0$ is a closed order ideal in $\mathcal D_ h$. It contains $L^ r$ for every $r>n$, and smooth functions are dense in it. If $v_-(h)>0$, then $\mathcal D_ h^0=\mathcal D_ h=L^ n$.
Proof. For $K>0$, set $p_ K=p\min (1,K/|p|)$ where $p\ne 0$, and $p_ K=0$ where $p=0$. Then $|p-p_ K|=(|p|-K)_+$ and
Since the $L^ n$ norms of the tails tend to zero, these inequalities and the monotonicity of $\rho _ h$ show that the second condition is equivalent to $p_ K\to p$ in $\mathcal D_ h$; in particular, it implies the first. Conversely, if $a$ is bounded and $K\geq \| a\| _{L^\infty }$, then $(|p|-K)_+\leq |p-a|$, so $\| p-p_ K\| _{\mathcal D_ h}\leq \| p-a\| _{\mathcal D_ h}$. Approximating $p$ by bounded functions $a$ shows that the first condition implies $p_ K\to p$, hence the second.
Assume the second condition, and let $q_ j$ be as in the third. Fix $K$. On $\{ |p|\leq K\} $, the functions $q_ j$ are bounded by $K$ and tend to zero in measure, hence in $L^{2n}$; by (15.32.8) with $r=2n$, the root functional of $q_ j\mathbf1_{\{ |p|\leq K\} }$ tends to zero. On the complementary set, $\rho _ h(q_ j\mathbf1_{\{ |p|>K\} })\leq \rho _ h(|p|\mathbf1_{\{ |p|>K\} })$. Letting first $j$ and then $K$ tend to infinity gives $\rho _ h(q_ j)\to 0$, and dominated convergence gives $\| q_ j\| _{L^ n}\to 0$. Conversely, the third condition applied to $q_ j=|p|\mathbf1_{\{ |p|>j\} }$ gives the second.
Since the second condition passes from $p$ to every function dominated by $|p|$, the space $\mathcal D_ h^0$ is an order ideal; it is closed by definition. For $p\in L^ r$ with $r>n$, the truncations $p_ K$ converge to $p$ in $L^ r$, hence in $\mathcal D_ h$ by (15.32.8). Bounded functions can be approximated in $L^{2n}$ by smooth functions, which then converge in $\mathcal D_ h$ by the same estimate; hence smooth functions are dense in $\mathcal D_ h^0$. Under positive lower mass, proposition 15.32.5 shows that $\mathcal D_ h=L^ n$ with an equivalent norm, and bounded functions are dense in $L^ n$; hence $\mathcal D_ h^0=\mathcal D_ h=L^ n$. $\square$
By proposition 15.29.5, the space $\mathcal D_ h^0$ does not depend on the choice of the Hermitian form $h$. Convergence in $\mathcal D_ h$ controls the threshold: if $p_ j\to p\ne 0$ in $\mathcal D_ h$, then
For $p\in \mathcal D_ h^0$, the uniform tail condition also gives a uniform modulus for exponential damping and error bounds for the scalars of the exponential equations; see proposition 15.35.5. It does not by itself give capacity convergence of the solutions. We do not know whether $\mathcal D_ h^0=\mathcal D_ h$ when $v_-(h)=0$.
6436CD7911BDThe product formula of theorem 15.30.6 identifies a complete subspace of density roots with uniformly vanishing tails even when the ambient lower mass is zero. Use the product data $X_0,Y,N,H,c_0,\mu ,R$ of 15.30.5. The spaces $\mathcal D_ H$ and $\mathcal D_ H^0$ are now taken on the $N$-dimensional product with reference volume $\mathrm dV$.
Proposition 15.32.11.7A2CC1A3258E For real or complex $\xi \in L^ N(Y,\kappa ^ k)$, put $J\xi =R^{1/N}\pi _ Y^*\xi $. Then
The image of $J$ is a closed linear subspace of $\mathcal D_ H^0$. If $g=|\xi |^ N$ and $A=\max _ XR$, then
For $\mathrm dV=\mu $, so that $R=1$, the exact tail formula is
Proof. Since $|J\xi |^ N=R|\xi |^ N$, integration against $\mathrm dV$ gives the first norm identity. For nonzero $\xi $, theorem 15.30.6 applied to $g=|\xi |^ N$ gives the root-functional identity; for $\xi =0$ it holds by definition. Applying the two identities to differences yields
Bounded approximations of $\xi $ in $L^ N$ have bounded images because $R$ is bounded, so $J\xi \in \mathcal D_ H^0$. Completeness of $L^ N(Y,\kappa ^ k)$ and the displayed identity make the image closed.
On $\{ |J\xi |>K\} $ one has $g>K^ N/A$, and hence
Monotonicity of the root functional and its identity for factor roots give the estimate, with the value zero when the tail vanishes. Integrability of $g$ makes the bound tend to zero; the $L^ N$ tails also vanish. When $R=1$, the amplitude cutoff itself is pulled back from $Y$, so the same norm identity gives equality. $\square$
For $Y=\mathbb P^ k$ and $\mathrm dV=\mu $, take $p_\alpha =\pi _ Y^*(q_\alpha ^{1/N})$ with $q_\alpha $ from lemma 15.30.1. Then $p_\alpha \in \mathcal D_ H^0$ but $p_\alpha \notin L^ r(\mathrm dV)$ for every $r>N$. Moreover,
Indeed, the radial estimate of that lemma gives $q_\alpha \asymp r^{-k}(1-\log r)^{-1-k(1-\alpha )}$. With $L=1-\log r$, the density level set $\{ q_\alpha >K^ N\} $ lies between two sets $\{ L>c\log K\} $ for fixed positive constants $c$, once $K$ is large. Integrating the radial density $L^{-1-k(1-\alpha )}\, \mathrm dL$ and taking its $N$th root gives the claimed tail. The integrability exclusion follows from $q_\alpha \notin L^ s$ for $s>1$.
These roots enlarge the examples in $\mathcal D_ H^0$ beyond the subcritical $L^ r$ classes. They give neither $\mathcal D_ H^0=\mathcal D_ H$ nor a general criterion for an exact equation at zero lower mass.
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