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11.43.9 A family with nonanalytic isolated poles592E13B7D2ED

The hypothesis of a common simplex allows ordinary singularity types that contain no potential with analytic singularities. Let $o=[1:0:\cdots :0]$ be the origin of the affine chart $Z_0\ne 0$, with affine coordinates $z_ i=Z_ i/Z_0$. For $0<a\leq 1$, define

\[ P_ a=\{ p\in \Sigma :\textstyle \sum _ i\sqrt{p_ i}\geq \sqrt a\} , \qquad \kappa _ n=\frac{2^ n n!}{(2n)!}=\frac1{(2n-1)!!}. \]

Proposition 11.43.10.70BE47F32080 The function $\Phi _{P_ a}$ is locally bounded outside the single point $o$, where it has a pole, and it does not have the ordinary singularity type of any function with analytic singularities. Its generic Lelong number along every prime divisor of $\mathbb P^ n$ is zero, and

47DDB1E89607 11.43.11
\begin{equation} \int _{\mathbb P^ n}\mathrm{MA}_{\omega _{\mathrm{FS}}}(\Phi _{P_ a}) =1-\kappa _ n a^ n>0. \end{equation}

The same assertions about the pole, nonanalyticity and generic Lelong numbers hold for $\pi ^*\Phi _{P_ a}$ on the blowup $\operatorname {Bl}_ q\mathbb P^ n$ at a fixed point $q\ne o$.

Proof. The function $p\mapsto \sum _ i\sqrt{p_ i}$ is concave, so $P_ a$ is convex. Set

\[ b=\frac{n+1}{2n},\qquad p_{*,i}=\frac bn, \qquad \delta =\frac{n-1}{4n}. \]

Then $b+\delta <1$ and $\sum _ i\sqrt{p_{*,i}}=\sqrt{(n+1)/2}>1$. Adding a point of $\delta \Sigma $ preserves the last inequality and keeps the sum of the coordinates below one, so $p_*+\delta \Sigma $ lies in every $P_ a$.

All the standard basis vectors $e_ i$ belong to $P_ a$, and therefore

\[ \psi _{P_ a}\geq \log \frac{\max _{1\leq i\leq n}|Z_ i|^2}{\sum _{i=0}^ n|Z_ i|^2}. \]

Hence the reference is locally bounded away from $o$. The Cauchy–Schwarz inequality gives $\sum _ ip_ i\geq a/n$ on $P_ a$. When all $x_ i<0$, this yields $h_{P_ a}(x)\leq (a/n)\max _ i x_ i$, which tends to $-\infty $ as $z\to o$, and lemma 11.43.2 gives the pole at $o$. Local boundedness outside one point implies that all generic Lelong numbers along prime divisors vanish, and pulling back to the blowup at a different point introduces no pole.

To test analyticity, fix positive $\lambda _1,\ldots ,\lambda _ n$ and approach $o$ along $|z_ i|^2=\mathrm{e}^{-R\lambda _ i}$, $R\to \infty $. Writing $y_ i=\sqrt{p_ i}$, the Cauchy–Schwarz inequality gives

6654DDDC658F 11.43.12
\begin{equation} \min _{p\in P_ a}\sum _ i\lambda _ i p_ i =\frac a{\sum _ i\lambda _ i^{-1}}=:d_ a(\lambda ),\qquad y_ i=\frac{\sqrt a}{\lambda _ i\sum _ k\lambda _ k^{-1}}, \end{equation}

where the minimizer satisfies $\sum _ ip_ i\leq a\leq 1$, so that it lies in $P_ a$. Since $L(-R\lambda )\to 0$ and $\Phi _{P_ a}-\psi _{P_ a}$ is bounded, $-\Phi _{P_ a}/R\to d_ a(\lambda )$ along these curves.

Suppose that the type were that of $c\log \sum _ k|f_ k|^2$ near $o$, with $c>0$ and holomorphic germs $f_ k=\sum _\alpha c_{k,\alpha }z^\alpha $. Exponentiating the two inequalities expressing this equivalence and averaging over the arguments of the $z_ i$ gives the positive series

\[ \sum _{k,\alpha }|c_{k,\alpha }|^2\mathrm{e}^{-R\alpha \cdot \lambda }, \]

whose exponential decay rate in $R$ must be $d_ a(\lambda )/c$. That rate is the minimum of $\alpha \cdot \lambda $ over the monomials with nonzero coefficients: a minimizing term gives one bound, and convergence at a fixed $R_0$ bounds the series above by a constant times $\mathrm{e}^{-(R-R_0)\min \alpha \cdot \lambda }$. Near any $\lambda $ with positive coordinates, only finitely many monomials can attain the minimum, because these coordinates have a common positive lower bound and any one nonzero coefficient bounds the degree of the minimizing monomials. The rate is therefore locally piecewise linear in $\lambda $. But

\[ d_ a(s,1,\ldots ,1)=\frac{as}{1+(n-1)s},\qquad \frac{\mathrm{d}^2}{\mathrm{d}s^2}d_ a(s,1,\ldots ,1) =-\frac{2a(n-1)}{(1+(n-1)s)^3}<0. \]

This contradiction proves nonanalyticity. The assertion persists on a blowup at a point different from $o$, which does not change a neighborhood of the pole.

The removed corner $C_ a=\{ p\in \mathbb R^ n:p_ i\geq 0,\ \sum _ i\sqrt{p_ i}<\sqrt a\} =aC_1$ lies in $\Sigma $. The substitution $p_ i=y_ i^2$ gives

\[ \operatorname {Vol}_ n(C_1) =2^ n\int _{y_ i\geq 0,\, \sum y_ i<1}\prod _ i y_ i\, \mathrm{d}y =\frac{2^ n}{(2n)!}. \]

The last equality follows by iterated integration of monomials over a simplex. Removing the corner from $\Sigma $, whose volume is $1/n!$, and applying (11.43.4) gives (11.43.11). Since $n\geq 2$, one has $\kappa _ n<1$. $\square$

Corollary 11.43.13.F57433433789 Put $a_ j=1-1/(j+2)$ and $r_ j=1+1/(j+2)$ for $j\geq 1$. On $\mathbb P^ n$, or on its blowup at a fixed point $q\ne o$, the references $r_ j\pi ^*\Phi _{P_{a_ j}}$ satisfy the hypotheses of theorem 11.43.6, with limit $\pi ^*\Phi _{P_1}$. Their ordinary types and masses vary with $j$, and

\[ \sup _ G|B_ j(G)-B(G)| \leq n|\log r_ j|+\frac{n\kappa _ n}{1-\kappa _ n}|1-a_ j|\longrightarrow 0. \]

The equation is solvable in the limiting ordinary type, whose mass is $1-\kappa _ n$; for $n=2$ this mass is $2/3$.

Proof. If $p\in P_{a_ j}\setminus P_1$, then $u=(\sum _ i\sqrt{p_ i})^2\in [a_ j,1)$ and $p/u\in P_1$. Since $|p|\leq \sum _ ip_ i\leq u$, one has $|p/u-p|\leq 1-u\leq 1-a_ j$. Thus $d_ H(P_{a_ j},P_1)\leq 1-a_ j$, and the hypotheses of the theorem hold with the simplex found in the proof of proposition 11.43.10. The mass formula (11.43.11) and the derivative bound $|\mathrm{d}\log (1-\kappa _ n a^ n)/\mathrm{d}a|\leq n\kappa _ n/(1-\kappa _ n)$ give the estimate for the functionals. By (11.43.12), the directional coefficients of the $j$th reference are multiplied by $r_ ja_ j=1-(j+2)^{-2}$, which strictly increases with $j$, so the ordinary types are distinct, while the masses $r_ j^ n(1-\kappa _ n a_ j^ n)$ strictly decrease to $1-\kappa _ n>0$. $\square$

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