ScalingStacks

1. Proof of Theorem A [0280]

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1. Proof of Theorem A

The following proposition will allow us to reduce the proof of Theorem A to the case M=ℂnM={\mathbb{C}}^{n}. We include its short proof for the convenience of the reader.

Proposition 1.1.

Let VV be a complex submanifold of ℂN{\mathbb{C}}^{N} and uu be a continuous psh exhaustion function on VV. Then there exists a continuous psh exhaustion function u~\widetilde{u} on ℂN{\mathbb{C}}^{N} so that u~|V=u\widetilde{u}\,|_{{}_{V}}=u.

Proof.

The argument is very similar to the one of Sadullaev ([Sa],[BL, Theorem 3.2]). By [Si], there exists an open neighborhood WW of VV in ℂN{\mathbb{C}}^{N} and a holomorphic retraction r:W→Vr:W\to V. We can find an open neighborhood UU of VV so that U⊂WU\subset W and ‖r⁡(z)−z‖<2\|r(z)-z\|<2 for every z∈Uz\in U. Indeed, if B⁡(p,r)B(p,r) denotes the open ball in ℂN{\mathbb{C}}^{N} centered at pp and of radius rr, then Up=r−1​(B⁡(p,1))∩B⁡(p,1)U_{p}=r^{-1}(B(p,1))\cap B(p,1) is an open neighborhood of p∈Vp\in V, and we let U=⋃p∈VUpU=\bigcup_{p\in V}U_{p}. Since uu is a continuous psh exhaustion function on VV, it follows that the function u⁡(r⁡(z))u(r(z)) is continuous psh on UU and limz∈U,‖z‖→+∞u⁡(r⁡(z))=+∞\lim_{z\in U,\|z\|\to+\infty}u(r(z))=+\infty.

It is well known that there exist entire functions f0,…,fNf_{0},\dots,f_{N}, so that V={z∈ℂN:fk(z)=0, 0≤k≤N}V=\{z\in{\mathbb{C}}^{N}:\,f_{k}(z)=0,\;0\leq k\leq N\} (see [Ch, p.63]). The function ρ=log⁡(∑|fk|2)\rho=\log(\sum|f_{k}|^{2}) is psh on ℂN{\mathbb{C}}^{N} and V={ρ=−∞}V=\{\rho=-\infty\}.

Let DD be an open set so that V⊂D⊂D¯⊂UV\subset D\subset\overline{D}\subset U. Since ρ\rho is continuous on ℂN∖V{\mathbb{C}}^{N}\setminus V, we can find a convex increasing function χ\chi on [0,+∞)[0,+\infty) which verifies for every R≥0R\geq 0 the following two properties:

(i)(i) χ⁡(R)>R−ρ⁡(z)\chi(R)>R-\rho(z) for all z∈ℂN∖Dz\in{\mathbb{C}}^{N}\setminus D with ‖z‖=R\|z\|=R.

(i​i)(ii) χ⁡(R)>u⁡(r⁡(z))−ρ⁡(z)\chi(R)>u(r(z))-\rho(z) for all z∈∂Dz\in\partial D with ‖z‖=R\|z\|=R.
Then

u~​(z)={max⁡{u⁡(r⁡(z)),χ⁡(‖z‖)+ρ⁡(z)},if​z∈D,χ⁡(‖z‖)+ρ⁡(z),if​z∈ℂN∖D,\widetilde{u}(z)=\left\{\begin{array}[]{ll}\max\{u(r(z)),\chi(\|z\|)+\rho(z)\},\;{\rm if}\;z\in D,\\ \chi(\|z\|)+\rho(z),\;{\rm if}\;z\in{\mathbb{C}}^{N}\setminus D,\end{array}\right.

is a continuous psh exhaustion function on ℂN{\mathbb{C}}^{N} and u~=u\widetilde{u}=u on VV. ∎

Employing the methods of Coltoiu [Co] we now construct psh extensions with growth control over bounded sets in ℂn{\mathbb{C}}^{n}.

Proposition 1.2.

Let χ\chi be a psh function on a subvariety X⊂ℂnX\subset{\mathbb{C}}^{n} and let vv be a continuous psh function on ℂn{\mathbb{C}}^{n} with χ<v\chi<v on XX. If R>0R>0, there exists a psh function χ~=χ~R\widetilde{\chi}=\widetilde{\chi}_{R} on ℂn{\mathbb{C}}^{n} so that χ~|X=χ\widetilde{\chi}\,|_{{}_{X}}=\chi and χ~​(z)<v​(z)\widetilde{\chi}(z)<v(z) for all z∈ℂnz\in{\mathbb{C}}^{n} with ‖z‖≤R\|z\|\leq R.

Proof.

We use a similar argument to the one in the proof of Proposition 2 in [Co]. Consider the subvariety A=(X×ℂ)∪(ℂn×{0})⊂ℂn+1A=(X\times{\mathbb{C}})\cup({\mathbb{C}}^{n}\times\{0\})\subset{\mathbb{C}}^{n+1}, and let

D={(z,w)∈X×ℂ:log⁡|w|+χ⁡(z)<0}∪(ℂn×{0})⊂A.D=\{(z,w)\in X\times{\mathbb{C}}:\,\log|w|+\chi(z)<0\}\cup({\mathbb{C}}^{n}\times\{0\})\subset A.

Since D∩(X×ℂ)D\cap(X\times{\mathbb{C}}) is Runge in X×ℂX\times{\mathbb{C}}, it follows that DD is Runge in AA. Let

K={(z,w)∈ℂn+1:ρ⁡(z,w)=max⁡{log+⁡(‖z‖/R),log⁡|w|+v⁡(z)}≤0}.K=\{(z,w)\in{\mathbb{C}}^{n+1}:\,\rho(z,w)=\max\{\log^{+}(\|z\|/R),\log|w|+v(z)\}\leq 0\}.

Since vv is continuous, ρ\rho is a continuous psh exhaustion function on ℂn+1{\mathbb{C}}^{n+1}, so KK is a polynomially convex compact set. As χ<v\chi<v on XX, we have K∩A⊂DK\cap A\subset D. By [Co, Theorem 3] there exists a Runge domain D~⊂ℂn+1\widetilde{D}\subset{\mathbb{C}}^{n+1}, with D~∩A=D\widetilde{D}\cap A=D and K⊂D~K\subset\widetilde{D}. Let δ⁡(z,w)\delta(z,w) denote the distance from (z,w)∈D~(z,w)\in\widetilde{D} to ∂D~\partial\widetilde{D} in the ww-direction. Since D~\widetilde{D} is pseudoconvex, −log⁡δ-\log\delta is psh on D~\widetilde{D} (see e.g. [FS, Proposition 9.2]). Hence χ~​(z)=−log⁡δ⁡(z,0)\widetilde{\chi}(z)=-\log\delta(z,0) is psh on ℂn{\mathbb{C}}^{n}, as ℂn×{0}⊂D~{\mathbb{C}}^{n}\times\{0\}\subset\widetilde{D}. Since D~∩A=D\widetilde{D}\cap A=D, it follows that χ~|X=χ\widetilde{\chi}\,|_{{}_{X}}=\chi. Moreover, K⊂D~K\subset\widetilde{D} implies that χ~​(z)<v​(z)\widetilde{\chi}(z)<v(z) for all z∈ℂnz\in{\mathbb{C}}^{n} with ‖z‖≤R\|z\|\leq R. ∎

The proof of Theorem A proceeds like this. Given a partition

ℂn=⋃{mj−1<u≤mj},{\mathbb{C}}^{n}=\bigcup\{m_{j-1}<u\leq m_{j}\},

where mj↗+∞m_{j}\nearrow+\infty, we apply Proposition 1.2 inductively to construct an extension dominated in each “annulus” {mj−1<u≤mj}\{m_{j-1}<u\leq m_{j}\} by γj​u\gamma_{j}u, where γj>1\gamma_{j}>1 is an increasing sequence defined in terms of the mjm_{j}’s. Theorem A will follow by showing that it is possible to choose {mj}\{m_{j}\} rapidly increasing so that limγj\lim\gamma_{j} is arbitrarily close to 1.

We fix next an increasing sequence {mj}j≥−1\{m_{j}\}_{j\geq-1} so that

m−1=m0=0<m1<m2<…,{u<m1}≠∅,mj↗+∞.m_{-1}=m_{0}=0<m_{1}<m_{2}<\dots,\>\{u<m_{1}\}\neq\emptyset,\;m_{j}\nearrow+\infty.

Define inductively a sequence {γj}j≥0\{\gamma_{j}\}_{j\geq 0}, as follows:

(1) γ0=1,γj​(mj−mj−1)=γj−1​(mj−mj−2)+1​for​j≥1.\gamma_{0}=1,\;\;\gamma_{j}(m_{j}-m_{j-1})=\gamma_{j-1}(m_{j}-m_{j-2})+1\;{\rm for}\;j\geq 1.

Clearly, γj>γj−1>1\gamma_{j}>\gamma_{j-1}>1 for all j>1j>1.

Proposition 1.3.

Let X,φ,uX,\,\varphi,\,u be as in Theorem A with M=ℂnM={\mathbb{C}}^{n}, and let {mj}\{m_{j}\}, {γj}\{\gamma_{j}\} be as above. There exists a psh function ψ\psi on ℂn{\mathbb{C}}^{n} so that ψ|X=φ\psi\,|_{{}_{X}}=\varphi and for all z∈ℂnz\in{\mathbb{C}}^{n} we have

ψ⁡(z)<{γj​u​(z),if​mj−1<u⁡(z)≤mj,j≥2,γ1​max⁡{u⁡(z),0},if​u​(z)≤m1.\psi(z)<\left\{\begin{array}[]{ll}\gamma_{j}u(z),\;{\rm if}\;m_{j-1}<u(z)\leq m_{j},\;j\geq 2,\\ \gamma_{1}\max\{u(z),0\},\;{\rm if}\;u(z)\leq m_{1}.\end{array}\right.
Proof.

We introduce the sets

Dj={z∈ℂn:u⁡(z)<mj},Kj={z∈ℂn:u⁡(z)≤mj}.D_{j}=\{z\in{\mathbb{C}}^{n}:\,u(z)<m_{j}\}\;,\;\;K_{j}=\{z\in{\mathbb{C}}^{n}:\,u(z)\leq m_{j}\}.

Since uu is a continuous psh exhaustion function, KjK_{j} is a compact set. Let

ρj=γj​max⁡{u−mj−1,0}−j,j≥0.\rho_{j}=\gamma_{j}\max\{u-m_{j-1},0\}-j,\;j\geq 0.

Then ρj\rho_{j} is psh on ℂn{\mathbb{C}}^{n} and (1) implies that

(2) ρj​(z)=ρj−1​(z)​if​u​(z)=mj,j≥1.\rho_{j}(z)=\rho_{j-1}(z)\;{\rm if}\;u(z)=m_{j},\;j\geq 1.

We claim that

(3) ρj​(z)≥u⁡(z)​if​z∈ℂn∖Dj,j≥0.\rho_{j}(z)\geq u(z)\;{\rm if}\;z\in{\mathbb{C}}^{n}\setminus D_{j},\;j\geq 0.

Indeed, since γj≥1\gamma_{j}\geq 1 and using (1) we obtain

ρj​(z)−u​(z)\displaystyle\rho_{j}(z)-u(z) =\displaystyle= (γj−1)​u​(z)−γj​mj−1−j≥(γj−1)​mj−γj​mj−1−j\displaystyle(\gamma_{j}-1)u(z)-\gamma_{j}m_{j-1}-j\geq(\gamma_{j}-1)m_{j}-\gamma_{j}m_{j-1}-j
=\displaystyle= (γj−1−1)​mj−γj−1​mj−2−j+1\displaystyle(\gamma_{j-1}-1)m_{j}-\gamma_{j-1}m_{j-2}-j+1
≥\displaystyle\geq (γj−1−1)​mj−1−γj−1​mj−2−(j−1).\displaystyle(\gamma_{j-1}-1)m_{j-1}-\gamma_{j-1}m_{j-2}-(j-1).

So xj:=(γj−1)​mj−γj​mj−1−j≥x0=0x_{j}:=(\gamma_{j}-1)m_{j}-\gamma_{j}m_{j-1}-j\geq x_{0}=0, and (3) is proved.

Let φj=max⁡{φ,−j}\varphi_{j}=\max\{\varphi,-j\}. We construct by induction on j≥1j\geq 1 a sequence of continuous psh functions ψj\psi_{j} on ℂn{\mathbb{C}}^{n} with the following properties:

(4) ψj​(z)>φj​(z)​for​z∈X,∫X∩Kj−1(ψj−φj)<2−j.\displaystyle\psi_{j}(z)>\varphi_{j}(z)\;{\rm for}\;z\in X\;,\;\;\int_{X\cap K_{j-1}}(\psi_{j}-\varphi_{j})<2^{-j}.
(5) ψj​(z)≥ρj​(z)​for​z∈Dj,ψj​(z)=ρj​(z)​for​z∈ℂn∖Dj.\displaystyle\psi_{j}(z)\geq\rho_{j}(z)\;{\rm for}\;z\in D_{j}\;,\;\;\psi_{j}(z)=\rho_{j}(z)\;{\rm for}\;z\in{\mathbb{C}}^{n}\setminus D_{j}.
(6) ψj​(z)<ψj−1​(z)​for​z∈Kj−1,where​ψ0=ρ0=max⁡{u,0}.\displaystyle\psi_{j}(z)<\psi_{j-1}(z)\;{\rm for}\;z\in K_{j-1},\;{\rm where}\;\psi_{0}=\rho_{0}=\max\{u,0\}.

Here the integral in (4) is with respect to the area measure on each irreducible component, i.e.

∫X∩Kf:=∑∫Y∩Kf​βdimY,\int_{X\cap K}f:=\sum\int_{Y\cap K}f\,\beta^{\dim Y},

where the sum is over all irreducible components YY of XX which intersect KK and β\beta is the standard Kähler form on ℂn{\mathbb{C}}^{n}. (Note that this is a finite sum.)

Assume that the function ψj−1\psi_{j-1} is constructed with the desired properties. We construct ψj\psi_{j} by applying Proposition 1.2 with χ=φj\chi=\varphi_{j} and v=ψj−1v=\psi_{j-1}. (If j=1j=1, ψ1\psi_{1} is constructed in the same way by applying Proposition 1.2 with χ=φ1\chi=\varphi_{1} and v=ψ0v=\psi_{0}.) By (4), φj≤φj−1<ψj−1\varphi_{j}\leq\varphi_{j-1}<\psi_{j-1} on XX (and for j=1j=1, clearly φ1<ψ0\varphi_{1}<\psi_{0} on XX). Therefore Proposition 1.2 yields a psh function φ~j\widetilde{\varphi}_{j} on ℂn{\mathbb{C}}^{n} so that φ~j|X=φj\widetilde{\varphi}_{j}\,|_{{}_{X}}=\varphi_{j} and φ~j<ψj−1\widetilde{\varphi}_{j}<\psi_{j-1} on KjK_{j}. Using the standard regularization of φ~j\widetilde{\varphi}_{j} and the dominated convergence theorem (as φj≥−j\varphi_{j}\geq-j) we obtain a continuous psh function ψ~j\widetilde{\psi}_{j} on ℂn{\mathbb{C}}^{n} which verifies

ψ~j​(z)>φj​(z)​for​z∈X,∫X∩Kj(ψ~j−φj)<2−j.\widetilde{\psi}_{j}(z)>\varphi_{j}(z)\;{\rm for}\;z\in X\;,\;\;\int_{X\cap K_{j}}(\widetilde{\psi}_{j}-\varphi_{j})<2^{-j}.

Moreover, since ψj−1\psi_{j-1} is continuous, we can ensure by the Hartogs lemma that we also have ψ~j​(z)<ψj−1​(z)\widetilde{\psi}_{j}(z)<\psi_{j-1}(z) for z∈Kjz\in K_{j}.

We now define

ψj​(z)={max⁡{ψ~j​(z),ρj​(z)},if​z∈Dj,ρj​(z),if​z∈ℂn∖Dj.\psi_{j}(z)=\left\{\begin{array}[]{ll}\max\{\widetilde{\psi}_{j}(z),\rho_{j}(z)\},\;{\rm if}\;z\in D_{j},\\ \rho_{j}(z),\;{\rm if}\;z\in{\mathbb{C}}^{n}\setminus D_{j}.\end{array}\right.

By (5) and (2) we have ψ~j<ψj−1=ρj−1=ρj\widetilde{\psi}_{j}<\psi_{j-1}=\rho_{j-1}=\rho_{j} on ∂Dj\partial D_{j} (for j=1j=1, recall that ψ0=ρ0\psi_{0}=\rho_{0} by definition). So ψj\psi_{j} is a continuous psh function on ℂn{\mathbb{C}}^{n} which verifies (5). On X∖DjX\setminus D_{j} we have by (3) that ψj=ρj≥u>φj\psi_{j}=\rho_{j}\geq u>\varphi_{j}, while on X∩DjX\cap D_{j}, ψj≥ψ~j>φj\psi_{j}\geq\widetilde{\psi}_{j}>\varphi_{j}. Since ρj=−j≤φj<ψ~j\rho_{j}=-j\leq\varphi_{j}<\widetilde{\psi}_{j} on X∩Kj−1X\cap K_{j-1}, we see that ψj=ψ~j\psi_{j}=\widetilde{\psi}_{j} on X∩Kj−1X\cap K_{j-1} so

∫X∩Kj−1(ψj−φj)≤∫X∩Kj(ψ~j−φj)<2−j.\int_{X\cap K_{j-1}}(\psi_{j}-\varphi_{j})\leq\int_{X\cap K_{j}}(\widetilde{\psi}_{j}-\varphi_{j})<2^{-j}.

Hence ψj\psi_{j} verifies (4). Finally, we have by (5), ρj=−j<ρj−1≤ψj−1\rho_{j}=-j<\rho_{j-1}\leq\psi_{j-1} on Kj−1K_{j-1} (and for j=1j=1, ρ1=−1<ψ0=0\rho_{1}=-1<\psi_{0}=0 on K0K_{0}). Since ψ~j<ψj−1\widetilde{\psi}_{j}<\psi_{j-1} on KjK_{j} we conclude that ψj<ψj−1\psi_{j}<\psi_{j-1} on Kj−1K_{j-1}, so (6) is verified.

So we have constructed a sequence of continuous psh functions ψj\psi_{j} on ℂn{\mathbb{C}}^{n} verifying properties (4)-(6). Since ⋃j≥1Dj=ℂn\bigcup_{j\geq 1}D_{j}={\mathbb{C}}^{n}, we have by (6) that the function

ψ⁡(z)=limj→∞ψj​(z)\psi(z)=\lim_{j\to\infty}\psi_{j}(z)

is well defined and psh on ℂn{\mathbb{C}}^{n}. As …<ψj+2<ψj+1<ψj\ldots<\psi_{j+2}<\psi_{j+1}<\psi_{j} on KjK_{j}, it follows that ψ<ψj\psi<\psi_{j} on KjK_{j}.

Suppose now that z∈Kj∖Dj−1z\in K_{j}\setminus D_{j-1}, for some j≥2j\geq 2, so mj−1≤u⁡(z)≤mjm_{j-1}\leq u(z)\leq m_{j}. By the above construction and property (5), we have

ψ~j​(z)<ψj−1​(z)=ρj−1​(z)⟹ψ⁡(z)<ψj​(z)≤max⁡{ρj−1​(z),ρj​(z)}≤γj​u​(z).\widetilde{\psi}_{j}(z)<\psi_{j-1}(z)=\rho_{j-1}(z)\Longrightarrow\psi(z)<\psi_{j}(z)\leq\max\{\rho_{j-1}(z),\rho_{j}(z)\}\leq\gamma_{j}u(z).

Similarly, for z∈K1z\in K_{1} we have

ψ⁡(z)<ψ1​(z)≤max⁡{ρ0​(z),ρ1​(z)}≤γ1​max​{u⁡(z),0}.\psi(z)<\psi_{1}(z)\leq\max\{\rho_{0}(z),\rho_{1}(z)\}\leq\gamma_{1}\max\{u(z),0\}.

Hence ψ\psi satisfies the desired global upper estimates on ℂn{\mathbb{C}}^{n}.

Property (4) implies that ψ⁡(z)≥φ⁡(z)\psi(z)\geq\varphi(z) for every z∈Xz\in X. Let KK be a compact in ℂn{\mathbb{C}}^{n} and YY be an irreducible component of XX so that φ|Y≢−∞\varphi\,|_{{}_{Y}}\not\equiv-\infty. By (4) we have that for all jj sufficiently large

0≤∫Y∩K(ψj−φ)=∫Y∩K(ψj−φj)+∫Y∩K(φj−φ)≤2−j+∫Y∩K(φj−φ).0\leq\int_{Y\cap K}(\psi_{j}-\varphi)=\int_{Y\cap K}(\psi_{j}-\varphi_{j})+\int_{Y\cap K}(\varphi_{j}-\varphi)\leq 2^{-j}+\int_{Y\cap K}(\varphi_{j}-\varphi).

Hence by dominated convergence, ∫Y∩K(ψ−φ)=0\int_{Y\cap K}(\psi-\varphi)=0, which shows that ψ=φ\psi=\varphi on YY.

Assume now that YY is an irreducible component of XX so that φ|Y≡−∞\varphi\,|_{{}_{Y}}\equiv-\infty. Then using (4) and the monotone convergence theorem we conclude that

∫Y∩Kψ=limj→∞∫Y∩Kψj=limj→∞(∫Y∩K(ψj−φj)+∫Y∩Kφj)=−∞,\int_{Y\cap K}\psi=\lim_{j\to\infty}\int_{Y\cap K}\psi_{j}=\lim_{j\to\infty}\left(\int_{Y\cap K}(\psi_{j}-\varphi_{j})+\int_{Y\cap K}\varphi_{j}\right)=-\infty,

so ψ|Y≡−∞\psi\,|_{{}_{Y}}\equiv-\infty. Therefore ψ=φ\psi=\varphi on XX, and the proof is finished. ∎

Proof of Theorem A. We consider first the case M=ℂnM={\mathbb{C}}^{n}. Fix c>1c>1. We define inductively a sequence {mj}\{m_{j}\} with the following properties: m−1=m0=0<m1m_{-1}=m_{0}=0<m_{1}, {u<m1}≠∅\{u<m_{1}\}\neq\emptyset, and for j≥1j\geq 1, mj>mj−1m_{j}>m_{j-1} is chosen large enough so that

aj=mj−1−mj−2+1mj−mj−1≤log⁡c2j.a_{j}=\frac{m_{j-1}-m_{j-2}+1}{m_{j}-m_{j-1}}\leq\frac{\log c}{2^{j}}\;.

Since γj≥γ0=1\gamma_{j}\geq\gamma_{0}=1 we have by (1),

γj​(mj−mj−1)≤γj−1​(mj−mj−2+1)⟹γj≤γj−1​(1+aj).\gamma_{j}(m_{j}-m_{j-1})\leq\gamma_{j-1}(m_{j}-m_{j-2}+1)\Longrightarrow\gamma_{j}\leq\gamma_{j-1}(1+a_{j}).

Thus

γj<γ=∏j=1∞(1+aj),log⁡γ≤∑j=1∞aj≤log⁡c.\gamma_{j}<\gamma=\prod_{j=1}^{\infty}(1+a_{j})\;,\;\;\log\gamma\leq\sum_{j=1}^{\infty}a_{j}\leq\log c.

Let ψ=ψc\psi=\psi_{c} be the psh extension of φ\varphi provided by Proposition 1.3 for this sequence {mj}\{m_{j}\}. Then for every z∈ℂnz\in{\mathbb{C}}^{n} we have

ψ⁡(z)<γ​max​{u⁡(z),0}≤c​max​{u⁡(z),0}.\psi(z)<\gamma\max\{u(z),0\}\leq c\max\{u(z),0\}.

Assume now that MM is a Stein manifold of dimension nn. Then MM can be properly embedded in ℂ2​n+1{\mathbb{C}}^{2n+1}, hence we may assume that MM is a complex submanifold of ℂ2​n+1{\mathbb{C}}^{2n+1} (see e.g. [Ho, Theorem 5.3.9]). Proposition 1.1 implies the existence of a continuous psh exhaustion function u~\widetilde{u} on ℂ2​n+1{\mathbb{C}}^{2n+1} so that u~=u\widetilde{u}=u on MM. By what we already proved, given c>1c>1 there exists a psh function ψ~\widetilde{\psi} on ℂ2​n+1{\mathbb{C}}^{2n+1} which extends φ\varphi and such that ψ~<c​max⁡{u~,0}\widetilde{\psi}<c\max\{\widetilde{u},0\} on ℂ2​n+1{\mathbb{C}}^{2n+1}. We let ψ=ψ~|M\psi=\widetilde{\psi}\,|_{{}_{M}}. □\Box

We end this section by noting that some hypothesis on the growth of uu is necessary in Theorem A. Indeed, suppose that XX is a submanifold of ℂn{\mathbb{C}}^{n} for which there exists a non-constant negative psh function φ\varphi on XX. Then any psh extension of φ\varphi to ℂn{\mathbb{C}}^{n} cannot be bounded above. However, by Theorem A, given any ε>0\varepsilon>0 there exists a psh function ψ=ψε\psi=\psi_{\varepsilon} so that ψ|X=φ\psi\,|_{{}_{X}}=\varphi and ψ⁡(z)<ε​log+​‖z‖\psi(z)<\varepsilon\log^{+}\|z\| on ℂn{\mathbb{C}}^{n}.

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