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8.6 Proper equations and admissible approximationA493740DE457

A493740DE457

For a smooth potential write $H_ m(w)=(\omega +\mathrm{dd}^{\mathrm{c}}w)^ m\wedge \omega ^{n-m}$. The positive exponential coefficient controls additive constants by the maximum principle. The resulting smooth equations will also construct admissible approximations of bounded potentials, before any continuous Hessian product is defined.

Lemma 8.6.1.8B310CC2C1A1 For every $a>0$ and smooth real $H$ on $X$, there is a unique smooth strictly admissible solution of

\[ H_ m(w)=e^{aw+H}\omega ^ n. \]

It satisfies

\[ -\frac{\max _ X H}{a}\leq w\leq -\frac{\min _ X H}{a}. \]

Proof. At a maximum of $w$, the admissible form $\omega +\mathrm{dd}^{\mathrm{c}}w$ is at most $\omega $, hence $e^{aw+H}\leq 1$ there. At a minimum it is at least $\omega $, and the reverse inequality holds. These give the bounds. For two solutions, a positive maximum of their difference would imply $H_ m(w_1)\leq H_ m(w_2)$ there, contradicting the exponential factor. This proves uniqueness.

First take $a=1$ and use the path $H_ m(w_ t)=e^{w_ t+tH}\omega ^ n$, starting with $w_0=0$. The trace estimate of 8.4.6 applies with prescribed potential $v=0$, fixed smooth comparison $0$, and $h(x,v)=tH(x)$; its constants are uniform for $t\in [0,1]$. 8.3.3 then gives a uniform gradient and complex-Hessian bound. 8.5.1 gives uniform $W^{2,p}$ and hence $C^{1,\alpha }$ bounds, for any fixed $\alpha <1$. Consequently $r_ t=e^{(w_ t+tH)/m}$ has a uniform Hölder bound.

The extension of 8.5.3 is uniformly elliptic and concave on all real Hessians, with coefficient oscillation bounded by $C|x-y|(1+\| R\| )$. The analytic estimate recalled in section 8.5 therefore gives uniform $C^{2,\beta }$ bounds on a finite cover. The original smooth Hessian operator is uniformly elliptic near the attained compact cone set. Differentiating and applying Schauder estimates gives bounds for every higher derivative.

The linearization of $\log (H_ m(w)/\omega ^ n)-w-tH$ is $L_ w-1$, where

\[ L_ w\xi =\frac{m\mathrm{dd}^{\mathrm{c}}\xi \wedge (\omega +\mathrm{dd}^{\mathrm{c}}w)^{m-1} \wedge \omega ^{n-m}}{H_ m(w)}. \]

Its principal coefficients are positive definite. The maximum principle gives zero kernel; smooth elliptic Fredholm theory gives surjectivity and Schauder inversion. The implicit-function theorem proves openness. The uniform estimates prove closedness, so the path reaches $t=1$. For general $a$, use the metric $a\omega $ and potential $\widehat w=aw$. Both sides of its coefficient-one equation acquire the same factor $a^ n$, so it is exactly the stated equation after division by that factor. $\square$

An ordinary smooth approximation need not be admissible. To obtain an admissible one, choose a smooth obstacle above the continuous potential and penalize the solution's distance from that obstacle.

Lemma 8.6.2.B8367971A40D Every continuous admissible $\varphi $ on $X$ is the uniform limit of smooth strictly admissible functions.

Proof. Fix a smooth $h\geq \varphi $ and a constant

\[ b>\max \left\{ 1,\left\| H_ m(h)/\omega ^ n\right\| _\infty \right\} . \]

For each positive integer $N$ solve, by the preceding lemma,

\[ H_ m(w_ N)=b e^{N(w_ N-h)}\omega ^ n. \]

At a positive maximum of $w_ N-h$, the form $\omega +\mathrm{dd}^{\mathrm{c}}h$ lies above the strictly admissible form $\omega +\mathrm{dd}^{\mathrm{c}}w_ N$, hence is admissible there. Monotonicity would give $b e^{N(w_ N-h)}\leq H_ m(h)/\omega ^ n<b$, a contradiction. Thus $w_ N\leq h$. The preceding zero-order estimate also gives

\[ \| w_ N\| _\infty \leq M_ N:=\| h\| _\infty +\frac{\log b}{N}. \]

Let $x_ N$ maximize $\varphi -(1+N^{-1})w_ N$. The smooth positive form $T_ N=(\omega +\mathrm{dd}^{\mathrm{c}}w_ N)^{m-1}\wedge \omega ^{n-m}$ defines a strictly elliptic linear operator. Admissibility gives $(\omega +\mathrm{dd}^{\mathrm{c}}\varphi )\wedge T_ N\geq 0$ in distributions. Its linear maximum principle, applied to the upper test $(1+N^{-1})w_ N$ plus the maximum value, gives at $x_ N$

\[ 0\leq \bigl (\omega +(1+N^{-1})\mathrm{dd}^{\mathrm{c}}w_ N\bigr )\wedge T_ N. \]

This application is to a continuous distributional subsolution of a smooth strictly elliptic operator. It does not assume a second derivative of $\varphi $. Writing $d_ N=H_ m(w_ N)/\omega ^ n$, polarized Gårding positivity yields

\[ (N+1)d_ N\geq \omega \wedge T_ N/\omega ^ n \geq d_ N^{(m-1)/m}. \]

Therefore, at this maximum point,

\[ w_ N-h\geq -E_ N,\qquad E_ N=\frac{m\log (N+1)+\log b}{N}. \]

Since $\varphi \leq h$, the maximum of $\varphi -(1+N^{-1})w_ N$ is at most $E_ N+M_ N/N$. It follows on all of $X$ that

\[ \varphi -E_ N-2M_ N/N\leq w_ N\leq h. \]

Given $\delta >0$, choose an ordinary smooth majorant $\varphi \leq h\leq \varphi +\delta $, and then $N$ so large that $E_ N+2M_ N/N\leq \delta $. The resulting $w_ N$ is strictly admissible and within $\delta $ of $\varphi $. Let $\delta \downarrow 0$. No monotonicity of the chosen approximants is needed. $\square$

8.6.3 Decreasing approximation of bounded potentialsABD764A7564F

Upper semicontinuity supplies smooth obstacles decreasing to a bounded potential. The same penalty equation gives admissible functions between the potential and each obstacle, up to an error tending to zero. Choosing successive obstacles below the preceding smooth approximation makes the admissible approximations decrease as well.

Lemma 8.6.4.EBF9BA687F39 Every bounded upper semicontinuous real function $u$ on $X$ is the pointwise decreasing limit of smooth functions $h_ j>u$.

Proof. Fix a Riemannian distance $d$ on $X$ and put

\[ c_ j(x)=\sup _{y\in X}\{ u(y)-j d(x,y)\} . \]

Each $c_ j$ is Lipschitz, $c_ j\geq u$, and $c_{j+1}\leq c_ j$. The supremum is attained. If $y_ j$ attains it at a fixed $x$, then $j d(x,y_ j)\leq \sup _ X u-u(x)$, so $y_ j\to x$. Upper semicontinuity gives $\limsup _ j c_ j(x)\leq u(x)$, and hence $c_ j\downarrow u$ pointwise.

Set $\delta _ j=4^{-j}$. Smooth approximation of continuous functions on a compact manifold gives $s_ j\in C^\infty (X)$ with $\| s_ j-c_ j\| _\infty \leq \delta _ j/4$. Take $h_ j=s_ j+\delta _ j$. Then

\[ u+\tfrac 34\delta _ j\leq h_ j\leq c_ j+\tfrac 54\delta _ j, \qquad h_{j+1}\leq c_ j+\tfrac 5{16}\delta _ j < c_ j+\tfrac 34\delta _ j\leq h_ j. \]

The bounds also imply $h_ j(x)\to u(x)$ at every point. $\square$

Lemma 8.6.5.DFE78235C5E9 Let $u$ be bounded admissible and $h\geq u$ smooth. Choose

\[ b>\max \{ 1,\| H_ m(h)/\omega ^ n\| _\infty \} . \]

For each positive integer $N$, let $w_ N$ be the smooth strictly admissible solution of

\[ H_ m(w_ N)=b e^{N(w_ N-h)}\omega ^ n. \]

With

\[ M_ N=\| h\| _\infty +\frac{\log b}{N},\qquad E_ N=\frac{m\log (N+1)+\log b}{N}, \]

one has $\| w_ N\| _\infty \leq M_ N$ and

\[ u-E_ N-2M_ N/N\leq w_ N\leq h. \]

Proof. Existence follows from 8.6.1. The maximum comparison with $h$ in the proof of 8.6.2 gives $w_ N\leq h$; it involves only the smooth obstacle and solution. The zero-order bound from 8.6.1 gives $\| w_ N\| _\infty \leq M_ N$.

The upper semicontinuous function $u-(1+N^{-1})w_ N$ attains its maximum at some $x_ N$. The smooth function $(1+N^{-1})w_ N$ plus this maximum is an upper test for $u$ there. Put

\[ T_ N=(\omega +\mathrm{dd}^{\mathrm{c}}w_ N)^{m-1}\wedge \omega ^{n-m}, \qquad d_ N=H_ m(w_ N)/\omega ^ n>0. \]

Condition (8.2.2) and polarized positivity yield, at $x_ N$,

\[ (N+1)d_ N\geq \omega \wedge T_ N/\omega ^ n \geq d_ N^{(m-1)/m}. \]

Consequently $d_ N\geq (N+1)^{-m}$ and $w_ N-h\geq -E_ N$ there. Using $u\leq h$, the maximum is at most $E_ N+M_ N/N$. On all of $X$ this gives

\[ u\leq (1+N^{-1})w_ N+E_ N+M_ N/N \leq w_ N+E_ N+2M_ N/N. \]
$\square$

Theorem 8.6.6.68BE4F589DCE Every bounded admissible potential $u$ on $X$ is the pointwise decreasing limit of smooth strictly admissible potentials. The sequence may be chosen uniformly bounded.

Proof. Choose smooth $h_ k\downarrow u$ by 8.6.4 and put $\varepsilon _ j=8^{-j}$. We construct smooth strictly admissible $u_ j$ with $u_ j\geq u+\varepsilon _ j$. For $j=1$, take $k_1=1$. At a subsequent step choose $k_ j\geq \max \{ j,k_{j-1}+1\} $ so large that

\[ h_{k_ j}<u_{j-1}-\tfrac 12\varepsilon _{j-1}\quad \hbox{on }X. \]

Such an index exists: the open sets $\{ h_ k<u_{j-1}-\varepsilon _{j-1}/2\} $ increase with $k$ and cover $X$, since $h_ k\downarrow u\leq u_{j-1}-\varepsilon _{j-1}$. Compactness gives a single index for all of $X$.

For this fixed obstacle $h_{k_ j}$ choose $b_ j$ as in 8.6.5, and then choose $N_ j$ so large that its error $E_{N_ j}+2M_{N_ j}/N_ j$ is at most $\varepsilon _ j$. The resulting smooth solution $w_ j$ satisfies

\[ u-\varepsilon _ j\leq w_ j\leq h_{k_ j}. \]

Put $u_ j=w_ j+2\varepsilon _ j$. Adding a constant preserves strict admissibility, and $u_ j\geq u+\varepsilon _ j$. For $j\geq 2$,

\[ u_ j\leq h_{k_ j}+2\varepsilon _ j <u_{j-1}-\tfrac 12\varepsilon _{j-1}+2\varepsilon _ j =u_{j-1}-\tfrac 14\varepsilon _{j-1}. \]

Finally, $u\leq u_ j\leq h_{k_ j}+2\varepsilon _ j$ and $k_ j\geq j$ give pointwise convergence to $u$. The bounds $\inf _ X u\leq u_ j\leq \sup _ X u_1$ give a common uniform bound. $\square$

For continuous $u$, Dini's theorem makes these decreasing approximations converge uniformly on $X$. This is the convergence used for the continuous mixed products in the next section.

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