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Polynomials with exponents in compact convex sets and associated weighted extremal functions -
Approximations and regularity

Bergur Snorrason
Abstract

We study various regularization operators on plurisubharmonic functions that preserve Lelong classes with growth given by certain compact convex sets. The purpose is to study when the weighted Siciak-Zakharyuta functions associated with these Lelong classes are lower semicontinuous. These operators are given by integral, infimal, and supremal convolutions. Continuity properties of the logarithmic supporting function are studied and a precise description is given of when it is uniformly continuous. This gives a contradiction to published results about the Hölder continuity of these Siciak-Zakharyuta functions.

Subject Classification (2020): 32U35. Secondary 32U15.

1 Introduction

A useful tool in pluripotential theory is regularization by convolution. If u𝒫𝒮(Ω)u\in\mathcal{PSH}(\Omega), for some open Ωn\Omega\subset\mathbb{C}^{n}, then uχδ𝒫𝒮𝒞(Ωδ)u*\chi_{\delta}\in\mathcal{PSH}\cap\mathcal{C}^{\infty}(\Omega_{\delta}), for δ>0\delta>0, where we define

uχδ(z)=nu(zw)χδ(w)𝑑λ(w),zΩδ.u*\chi_{\delta}(z)=\int_{\mathbb{C}^{n}}u(z-w)\chi_{\delta}(w)\,d\lambda(w),\quad z\in\Omega_{\delta}.

Here, Ωδ={zΩ;B(z,δ)Ω}\Omega_{\delta}=\{z\in\Omega\,;\,B(z,\delta)\subset\Omega\}, where B(z,δ)B(z,\delta) is the open euclidean ball with center zz and radius δ\delta, χδ\chi_{\delta} is a standard smoothing kernel in n\mathbb{C}^{n} with support in the closed ball B¯(0,δ)\overline{B}(0,\delta), and 𝒞(Ωδ)\mathcal{C}^{\infty}(\Omega_{\delta}) is the family of smooth function on Ωδ\Omega_{\delta}. We also have that uχδuu*\chi_{\delta}\searrow u, as δ0\delta\searrow 0. In the specific setting of Ω=n\Omega=\mathbb{C}^{n}, we have Ωδ=n\Omega_{\delta}=\mathbb{C}^{n}. So, every function in 𝒫𝒮(n)\mathcal{PSH}(\mathbb{C}^{n}) can approximated by a decreasing sequence in 𝒫𝒮𝒞(n)\mathcal{PSH}\cap\mathcal{C}^{\infty}(\mathbb{C}^{n}). For details on smoothing by convolution, see Klimek [9, Thm. 2.9.2].

In some cases, it is necessary to choose a method for regularizing plurisubharmonic functions that preserves a certain subclass of 𝒫𝒮(n)\mathcal{PSH}(\mathbb{C}^{n}). One such case is the Lelong class (n)\mathcal{L}(\mathbb{C}^{n}). We say that u𝒫𝒮(n)u\in\mathcal{PSH}(\mathbb{C}^{n}) belongs to the Lelong class, denoted by (n)\mathcal{L}(\mathbb{C}^{n}), if u(z)log+z+cuu(z)\leq\log^{+}\|z\|_{\infty}+c_{u} for some constant cuc_{u}, where \|\cdot\|_{\infty} is the supremum norm in n\mathbb{C}^{n} and log+x=max{0,logx}\log^{+}x=\max\{0,\log x\}. A powerful tool in the study of pluripotential theory is the Siciak-Zakharyuta function of EnE\subset\mathbb{C}^{n}, defined by

VE(z)=sup{u(z);u(n),u|E0},zn.V_{E}(z)=\sup\{u(z)\,;\,u\in\mathcal{L}(\mathbb{C}^{n}),u|_{E}\leq 0\},\quad z\in\mathbb{C}^{n}.

One can show that smoothing with a standard smoothing kernel preserves the Lelong class. Namely, if u(n)u\in\mathcal{L}(\mathbb{C}^{n}) then uχδ(n)u*\chi_{\delta}\in\mathcal{L}(\mathbb{C}^{n}). This is used to show that VKV_{K} is lower semicontinuous, for compact KnK\subset\mathbb{C}^{n}. See Klimek [9, Section 5.1].

In the recent study of pluripotential theory related to convex sets, the Lelong classes are generalized by describing the growth more freely. We fix a compact convex set 0S+n0\in S\subset\mathbb{R}^{n}_{+} and recall that the supporting function of SS, given by φS(ξ)=supxSx,ξ\varphi_{S}(\xi)=\sup_{x\in S}\langle x,\xi\rangle, is positively homogeneous and convex, which is equivalent to φS(tξ)=tφS(ξ)\varphi_{S}(t\xi)=t\varphi_{S}(\xi) and φS(ξ+η)φS(ξ)+φS(η)\varphi_{S}(\xi+\eta)\leq\varphi_{S}(\xi)+\varphi_{S}(\eta), for t+t\in\mathbb{R}_{+} and ξ,ηn\xi,\eta\in\mathbb{R}^{n}. We define the logarithmic supporting function of SS by

HS(z)={φS(log|z1|,,log|zn|),zn,lim¯nwzHS(w),znn,H_{S}(z)=\left\{\begin{array}[]{l l}\varphi_{S}(\log|z_{1}|,\dots,\log|z_{n}|),&z\in\mathbb{C}^{*n},\\ \varlimsup\limits_{\mathbb{C}^{*n}\ni w\rightarrow z}H_{S}(w),&z\in\mathbb{C}^{n}\setminus\mathbb{C}^{*n},\end{array}\right.

where n=()n\mathbb{C}^{*n}=(\mathbb{C}^{*})^{n} and ={0}\mathbb{C}^{*}=\mathbb{C}\setminus\{0\}. This function is continuous and plurisubharmonic on n\mathbb{C}^{n} and its behavior on the coordinate hyperplanes nn\mathbb{C}^{n}\setminus\mathbb{C}^{*n} can be described using logarithmic supporting functions of sets of lower dimensions. See [12, Props. 3.3 and 3.4]. We define the Lelong class given by SS as the set of all u𝒫𝒮(n)u\in\mathcal{PSH}(\mathbb{C}^{n}) satisfying uHS+cuu\leq H_{S}+c_{u}, for some constant cuc_{u}, and denote it by S(n)\mathcal{L}^{S}(\mathbb{C}^{n}). Similarly, we define +S(n)\mathcal{L}^{S}_{+}(\mathbb{C}^{n}) as the set of all functions uS(n)u\in\mathcal{L}^{S}(\mathbb{C}^{n}) satisfying HS+cuuH_{S}+c_{u}\leq u, for some constant cuc_{u}. This leads to our definition of the Siciak-Zakharyuta function of EnE\subset\mathbb{C}^{n} and SS with weight q:E{+}q\colon E\rightarrow\mathbb{R}\cup\{+\infty\},

VE,qS(z)=sup{u(z);uS(n),u|Eq},zn.V^{S}_{E,q}(z)=\sup\{u(z)\,;\,u\in\mathcal{L}^{S}(\mathbb{C}^{n}),u|_{E}\leq q\},\quad z\in\mathbb{C}^{n}.

We write VKS=VK,0SV^{S}_{K}=V^{S}_{K,0}, VK,q=VK,qΣV_{K,q}=V^{\Sigma}_{K,q}, and VK=VK,0ΣV_{K}=V^{\Sigma}_{K,0}, where Σ\Sigma is the standard simplex in n\mathbb{R}^{n} given by Σ=ch{0,e1,,en}\Sigma=\operatorname{ch}\{0,e_{1},\dots,e_{n}\}, where chA\operatorname{ch}A denotes the closed convex hull of the set AA.

A weight q:E{+}q\colon E\rightarrow\mathbb{R}\cup\{+\infty\} is called admissible if qq is lower semicontinuous, the set {zE;q(z)<+}\{z\in E\,;\,q(z)<+\infty\} is non-pluripolar, and limEz,|z|(HS(z)q(z))=\lim_{E\ni z,|z|\rightarrow\infty}(H_{S}(z)-q(z))=-\infty, if EE is unbounded.

Fundamental results of the Siciak-Zakharyuta function are developed in [12]. There, it is proven that VK,qSV^{S}_{K,q} is lower semicontinuous on n\mathbb{C}^{*n}, but it is not proven that it is lower semicontinuous on all of n\mathbb{C}^{n}. The obstruction to proving lower semicontinuity on n\mathbb{C}^{n} is a suitable method of approximating functions in S(n)\mathcal{L}^{S}(\mathbb{C}^{n}) by functions in S𝒞(n)\mathcal{L}^{S}\cap\mathcal{C}(\mathbb{C}^{n}), where 𝒞(n)\mathcal{C}(\mathbb{C}^{n}) denotes all continuous functions on n\mathbb{C}^{n}, since smoothing by convolution with a standard smoothing kernel does not always preserve S(n)\mathcal{L}^{S}(\mathbb{C}^{n}). In fact, S(n)\mathcal{L}^{S}(\mathbb{C}^{n}) is preserved by the standard convolution operator if and only if SS is a lower set, that is when SS is such that for all xSx\in S we have that [0,x1]××[0,xn]S[0,x_{1}]\times\dots\times[0,x_{n}]\subset S. See [12, Thm. 5.8].

In Section 2, we demonstrate the connection between the lower semicontinuity of VK,qSV^{S}_{K,q} and regularization in S(n)\mathcal{L}^{S}(\mathbb{C}^{n}). We also show that if SS contains a neighborhood of 0 in +n\mathbb{R}^{n}_{+} then the standard convolution operator, along with gluing, suffices to show that VK,qSV^{S}_{K,q} is lower semicontinuous. Namely, we prove the following.

Theorem 1.1.

Let S+nS\subset\mathbb{R}^{n}_{+} be a convex compact neighborhood of 0 in +n\mathbb{R}^{n}_{+}, KnK\subset\mathbb{C}^{n} be compact, and q:K{+}q\colon K\rightarrow\mathbb{R}\cup\{+\infty\} admissible. Then VK,qSV^{S}_{K,q} is lower semicontinuous.

This is significantly stronger than the case when SS is a lower set. For example, if S1,S2,S_{1},S_{2},\dots are lower sets, then so is S=j=1SjS=\cap_{j=1}^{\infty}S_{j}. However, for an arbitrary convex compact S+nS\subset\mathbb{R}^{n}_{+}, with 0S0\in S, we can define Sj=ch((1/j)ΣS)S_{j}=\operatorname{ch}\big{(}(1/j)\Sigma\cup S\big{)}. Then S=j=1SjS=\cap_{j=1}^{\infty}S_{j}. This idea, along with [12, Prop. 4.8(i)], can sometimes be used to strengthen results. This is done in [19, the proof of Thm. 1.1].

An important consequence of Theorem 1.1 is sharpening the Siciak-Zakharyuta theorem proved in [11, Thm. 1.1].

In Sections 3-5 we study regularization operators other than standard convolution. In Section 3 we consider a generalization of an operator of Siciak [16, Prop. 1.3].

Theorem 1.2.

Let S+nS\subset\mathbb{R}_{+}^{n} be a lower set, uS(n)u\in\mathcal{L}^{S}(\mathbb{C}^{n}) be bounded below, μ\mu be a distance function on n\mathbb{C}^{n}, uHS+cuu\leq H_{S}+c_{u} for some constant cuc_{u}, and δ]0,σS1ecurμ[\delta\in]0,\sigma_{S}^{-1}e^{c_{u}}r_{\mu}[, where σS=φS(1,,1)\sigma_{S}=\varphi_{S}(1,\dots,1) and rμ=inf|z|=1μ(z)>0r_{\mu}=\inf_{|z|=1}\mu(z)>0. Then

(1.1) Rμ,δau(z)=loginfwn{eu(w)+δ1μ(zw)},zn,R^{a}_{\mu,\delta}u(z)=-\log\inf_{w\in\mathbb{C}^{n}}\{e^{-u(w)}+\delta^{-1}\mu(z-w)\},\quad z\in\mathbb{C}^{n},

is in S(n)𝒞(n)\mathcal{L}^{S}(\mathbb{C}^{n})\cap\mathcal{C}(\mathbb{C}^{n}) and Rμ,δauuR^{a}_{\mu,\delta}u\searrow u, as δ0\delta\searrow 0.

With μ=||\mu=|\cdot|, Siciak proved that Rμ,δau(n)𝒞(n)R^{a}_{\mu,\delta}u\in\mathcal{L}(\mathbb{C}^{n})\cap\mathcal{C}(\mathbb{C}^{n}) and that Rμ,δauuR^{a}_{\mu,\delta}u\searrow u, as δ0\delta\searrow 0. In [1] this process is referred to as Ferrier approximation, since Siciak developed it using a result from Ferrier [2, Lemma 2, p. 48]. Here it is attributed to Siciak, since Ferrier was not concerned with approximations. It is claimed in [1, Prop. 3.1] that if μ=||\mu=|\cdot|, uS(n)u\in\mathcal{L}^{S}(\mathbb{C}^{n}), and SS is such that it contains a neighborhood of 0 in +n\mathbb{R}^{n}_{+}, then Rμ,δauS(n)𝒞(n)R^{a}_{\mu,\delta}u\in\mathcal{L}^{S}(\mathbb{C}^{n})\cap\mathcal{C}(\mathbb{C}^{n}). The following example shows that this claim is false.

Example 1.3.

Let S=ch{(0,0),(a,0),(0,a),(b,a)}S=\operatorname{ch}\{(0,0),(a,0),(0,a),(b,a)\}, a>0a>0, b>a(a+1)b>a(a+1), and μ=||\mu=|\cdot|. Note that, S=ch(aΣ{(b,a)})S=\operatorname{ch}(a\Sigma\cup\{(b,a)\}), so SS contains a neighborhood of 0 in +2\mathbb{R}^{2}_{+}. We have

HS(z1,z2)=max{blog|z1|+alog|z2|,alog+z},z1,z2.H_{S}(z_{1},z_{2})=\max\{b\log|z_{1}|+a\log|z_{2}|,a\log^{+}\|z\|_{\infty}\},\quad z_{1},z_{2}\in\mathbb{C}^{*}.

Hence, with r=b/(a+1)>ar=b/(a+1)>a, we have that

HS(ζ,|ζ|r)log|ζ|bra,ζ.H_{S}(\zeta,|\zeta|^{-r})\geq\log|\zeta|^{b-ra},\quad\zeta\in\mathbb{C}^{*}.

Setting w=(ζ,|ζ|r)w=(\zeta,|\zeta|^{-r}) in (1.1), with ζ\zeta\in\mathbb{C}^{*}, yields

Rμ,δaHS(ζ,0)\displaystyle R^{a}_{\mu,\delta}H_{S}(\zeta,0) log(eHS(ζ,|ζ|r)+δ1|ζ|r)\displaystyle\geq-\log(e^{-H_{S}(\zeta,|\zeta|^{-r})}+\delta^{-1}|\zeta|^{-r})
log(|ζ|arb+δ1|ζ|r)\displaystyle\geq-\log(|\zeta|^{ar-b}+\delta^{-1}|\zeta|^{-r})
=log(|ζ|r(a+1)b+δ1)+rlog|ζ|\displaystyle=-\log(|\zeta|^{r(a+1)-b}+\delta^{-1})+r\log|\zeta|
=log(1+δ1)+rlog|ζ|.\displaystyle=-\log(1+\delta^{-1})+r\log|\zeta|.

So, Rμ,δaHS(ζ,0)HS(ζ,0)(ra)log|ζ|log(1+δ1)R^{a}_{\mu,\delta}H_{S}(\zeta,0)-H_{S}(\zeta,0)\geq(r-a)\log|\zeta|-\log(1+\delta^{-1}) is not bounded above, since ra>0r-a>0. Hence, Rμ,δaHSR^{a}_{\mu,\delta}H_{S} is not in S(n)\mathcal{L}^{S}(\mathbb{C}^{n}).

The infimum in the definition of the operator Rμ,δaR^{a}_{\mu,\delta} is an infimal convolution of the functions eue^{-u} and δ1||\delta^{-1}|\cdot|. Details on infimal convolutions and its application in convexity theory can be found in Rockafellar [15]. Applications in complex analysis can be found in Kiselman [8] and Halvarsson [3, 4, 5].

In Section 4 we consider the following supremal convolution.

Theorem 1.4.

Let 0S+n0\in S\subset\mathbb{R}^{n}_{+} be compact convex, 1n=(1,,1)n1_{n}=(1,\dots,1)\in\mathbb{N}^{n}, σS=φS(1n)\sigma_{S}=\varphi_{S}(1_{n}), δ]0,σS1[\delta\in]0,\sigma_{S}^{-1}[, uS(n)u\in\mathcal{L}^{S}(\mathbb{C}^{n}) be locally bounded, and set

Rδbu(z)=supwn{u(Zw)δ1log(w1n+1)},zn,R^{b}_{\delta}u(z)=\sup_{w\in\mathbb{C}^{n}}\{u(Zw)-\delta^{-1}\log(\|w-1_{n}\|_{\infty}+1)\},\quad z\in\mathbb{C}^{n},

where Zw=(z1w1,,znwn)Zw=(z_{1}w_{1},\dots,z_{n}w_{n}). Then RδbuS(n)R^{b}_{\delta}u\in\mathcal{L}^{S}(\mathbb{C}^{n}), RδbuR^{b}_{\delta}u is continuous on n\mathbb{C}^{*n}, and RδbuuR^{b}_{\delta}u\searrow u, as δ0\delta\searrow 0.

The meaning of ZwZw is justified in Section 4. We note that σS\sigma_{S} may be 0. This only happens when S={0}S=\{0\}, which is a case of no interest, since then S(n)\mathcal{L}^{S}(\mathbb{C}^{n}) would only contain the constant functions.

In Section 5 we consider two related operators. The first one was developed in [12, Section 5].

Theorem 1.5.

Let 0S+n0\in S\subset\mathbb{R}^{n}_{+} be compact convex, δ]0,1[\delta\in]0,1[, uS(n)u\in\mathcal{L}^{S}(\mathbb{C}^{n}), and set

Rδcu(z)=nu(Zw)ψδ(w)𝑑λ(w),zn,R^{c}_{\delta}u(z)=\int_{\mathbb{C}^{n}}u(Zw)\psi_{\delta}(w)\ d\lambda(w),\quad z\in\mathbb{C}^{n},

where ψδ(w)=δ2nψ((w1n)/δ)\psi_{\delta}(w)=\delta^{-2n}\psi((w-1_{n})/\delta) and ψ\psi is a smoothing kernel that is rotationally invariant in each variable. Then RδcuS(n)R^{c}_{\delta}u\in\mathcal{L}^{S}(\mathbb{C}^{n}), RδcuR^{c}_{\delta}u is smooth on n\mathbb{C}^{*n}, and RδcuuR^{c}_{\delta}u\searrow u, as δ0\delta\searrow 0. If uu is locally bounded below and limzauz=ua\lim_{z\rightarrow a}u_{z}=u_{a}, in Lloc1(n)L^{1}_{\text{loc}}(\mathbb{C}^{n}), for all ana\in\mathbb{C}^{n}, where uzu_{z} is given by uz(w)=u(Zw)u_{z}(w)=u(Zw), for wnw\in\mathbb{C}^{n}, then Rδcu𝒞(n)R^{c}_{\delta}u\in\mathcal{C}(\mathbb{C}^{n}).

The assumption that uu is locally bounded below ensure that Rδcu>R^{c}_{\delta}u>-\infty. Taking u(z)=log|z1|u(z)=\log|z_{1}|, we have Rδcu(z)=R^{c}_{\delta}u(z)=-\infty, for z{0}×n1z\in\{0\}\times\mathbb{C}^{n-1}. So, RδcuR^{c}_{\delta}u fails to be continuous.

A possible approach to showing continuity on all of n\mathbb{C}^{n} is to regularize eue^{u} instead of uu. The second operator in Section 5 is given by logRδceu\log R^{c}_{\delta}e^{u}. It must be shown that this function is plurisubharmonic.

Theorem 1.6.

Let 0S+n0\in S\subset\mathbb{R}^{n}_{+} be compact convex, δ]0,1[\delta\in]0,1[, uS(n)u\in\mathcal{L}^{S}(\mathbb{C}^{n}), and set

Rδdu(z)=logneu(Zw)ψδ(w)𝑑λ(w),zn.R^{d}_{\delta}u(z)=\log\int_{\mathbb{C}^{n}}e^{u(Zw)}\psi_{\delta}(w)\ d\lambda(w),\quad z\in\mathbb{C}^{n}.

Then RδduS(n)R^{d}_{\delta}u\in\mathcal{L}^{S}(\mathbb{C}^{n}), RδduR^{d}_{\delta}u is smooth on n\mathbb{C}^{*n}, and RδduuR^{d}_{\delta}u\searrow u, as δ0\delta\searrow 0.

In a recent paper of Perera [13], a classical result on the regularity of VKV_{K} is considered, and attempts are made to generalize it to the setting of VK,qSV^{S}_{K,q}. Perera [13] claims to give sufficient condition for VK,qSV^{S}_{K,q} to be Hölder continuous on n\mathbb{C}^{n}, with the only assumption that SS is a convex body. In Section, 6 we show that this can not hold without additional restrictions on SS. The main result, Corollary 6.2, states that if SS is not a lower set then +S(n)\mathcal{L}^{S}_{+}(\mathbb{C}^{n}) contains no uniformly continuous functions. Since VK,qS+S(n)V^{S*}_{K,q}\in\mathcal{L}^{S}_{+}(\mathbb{C}^{n}), by [12, Prop. 4.5], we have that VK,qSV^{S}_{K,q} can not be Hölder continuous if SS is not a lower set.

Acknowledgment

The results of this paper are a part of a research project, Holomorphic Approximations and Pluripotential Theory, with project grant no. 207236-051 supported by the Icelandic Research Fund. I would like to thank the Fund for its support and the Mathematics Division, Science Institute, University of Iceland, for hosting the project. I thank my supervisors Benedikt Steinar Magnússon and Ragnar Sigurðsson for their guidance and careful reading of the paper.

2 Regularity of the Siciak-Zakharyuta function

The main motivation for studying the regularization operators in Sections 3-5 is proving that VK,qSV^{S}_{K,q} is lower semicontinuous on n\mathbb{C}^{n}, not just n\mathbb{C}^{*n}, for compact KnK\subset\mathbb{C}^{n} and admissible qq. To prove lower semicontinuity using regularizations, we use the following variant of Dini’s theorem.

Theorem 2.1 (Dini’s theorem).

Let (fj)j(f_{j})_{j\in\mathbb{N}} be a decreasing sequence of upper semicontinuous functions on a compact space XX, with pointwise limit ff, and gg be a lower semicontinuous function on XX such that f<gf<g. Then there exists j0j_{0} such that fj<gf_{j}<g, for all j>j0j>j_{0}.

Proof.

For every xXx\in X, we can take jxj_{x}\in\mathbb{N} such that fjx(x)g(x)<0f_{j_{x}}(x)-g(x)<0. Since fjxf_{j_{x}} is upper semicontinuous and gg is lower semicontinuous, we can take an open neighborhood UxU_{x} of xx such that fjx(y)g(y)<0f_{j_{x}}(y)-g(y)<0, for yUxy\in U_{x}. Since XX is compact, we can take x1,,xXx_{1},\dots,x_{\ell}\in X such that Ux1,,UxU_{x_{1}},\dots,U_{x_{\ell}} is a cover of XX. Let j0=max{jx1,,jx}j_{0}=\max\{j_{x_{1}},\dots,j_{x_{\ell}}\}. Then, since (fj)j(f_{j})_{j\in\mathbb{N}} is decreasing, we have fj<gf_{j}<g, for j>j0j>j_{0}. ∎

To see how regularization is used to show that VK,qSV^{S}_{K,q} is lower semicontinuous, we fix an open set Ωn\Omega\subset\mathbb{C}^{n} and assume that for all uS(n)u\in\mathcal{L}^{S}(\mathbb{C}^{n}) there exists a decreasing sequence (uj)j(u_{j})_{j\in\mathbb{N}} in S(n)\mathcal{L}^{S}(\mathbb{C}^{n}) such that uj|Ωu_{j}|_{\Omega} is continuous and ujuu_{j}\searrow u. If we take ε>0\varepsilon>0 and assume that uqu\leq q on KK then, by Dini’s theorem, we can find jj\in\mathbb{N}, such that ujεqu_{j}-\varepsilon\leq q on KK. Hence, VK,qSV^{S}_{K,q} is given as the supremum over a family of functions continuous on Ω\Omega, and is therefore lower semicontinuous on Ω\Omega.

The regularizations considered in this paper work for Ω=n\Omega=\mathbb{C}^{*n}. Whether these, or any other, regularizations work on all of n\mathbb{C}^{n} remains an open question.

We now turn to the main result in this section, Theorem 1.1. To prove it we will regularize using standard convolution, as discussed at the start on Section 1. This regularization will generally not have that right growth, but we will fix this using gluing.

Proof of Theorem 1.1.

Since qq is admissible, it is bounded below. So, we may assume that q>0q>0, and therefore, that VK,qS>0V^{S}_{K,q}>0, since VK,q+cS=VK,qS+cV^{S}_{K,q+c}=V^{S}_{K,q}+c, for every constant cc. There also exists a constant a>0a>0, such that aΣSa\Sigma\subset S, since SS contains a neighborhood of 0 in +n\mathbb{R}^{n}_{+}. This implies that HSHaΣalog+H_{S}\geq H_{a\Sigma}\geq a\log^{+}\|\cdot\|_{\infty}.

Fix wnw\in\mathbb{C}^{n} and ε>0\varepsilon>0, take uS(n)u\in\mathcal{L}^{S}(\mathbb{C}^{n}) such that u|Kqu|_{K}\leq q, and let cuc_{u} such that uHS+cuu\leq H_{S}+c_{u}. Let t]0,1[t\in]0,1[ such that tu(w)+ε/2u(w)tu(w)+\varepsilon/2\geq u(w). By [12, Prop. 4.5], there exists a constant C>0C>0 such that HSCVK,qSH_{S}-C\leq V^{S}_{K,q}. But,

HSCtu\displaystyle H_{S}-C-tu HStHSCtcu\displaystyle\geq H_{S}-tH_{S}-C-tc_{u}
(1t)alog+Ctcu,\displaystyle\geq(1-t)a\log^{+}\|\cdot\|_{\infty}-C-tc_{u},

so tu<HSCtu<H_{S}-C on (r𝔻n)\partial(r\mathbb{D}^{n}), for r>R0=max{1,e(C+tcu)/((1t)a)}r>R_{0}=\max\{1,e^{(C+tc_{u})/((1-t)a)}\}. We fix R>R0R>R_{0} such that wR𝔻nw\in R\mathbb{D}^{n}. By Theorem 2.1, we can choose δ>0\delta>0 such that

(i) (tu)χδ(w)+ε>u(w)(tu)*\chi_{\delta}(w)+\varepsilon>u(w),
(ii) (tu)χδ<HSC(tu)*\chi_{\delta}<H_{S}-C on (R𝔻n)\partial(R\mathbb{D}^{n}), and
(iii) (tu)χδ<q(tu)*\chi_{\delta}<q on KK,

since q>0q>0, and therefore tu<qtu<q. The function

uε,w(z)={max{HS(z)C,(tu)χδ(z)},zR𝔻n,HS(z)C,znR𝔻n,u_{\varepsilon,w}(z)=\bigg{\{}\begin{array}[]{ll}\max\{H_{S}(z)-C,(tu)*\chi_{\delta}(z)\},&z\in R\mathbb{D}^{n},\\ H_{S}(z)-C,&z\in\mathbb{C}^{n}\setminus R\mathbb{D}^{n},\end{array}

is plurisubharmonic, by Klimek [9, Cor. 2.9.15]. So uε,wS(n)u_{\varepsilon,w}\in\mathcal{L}^{S}(\mathbb{C}^{n}). We also have that HSCVK,qSqH_{S}-C\leq V^{S}_{K,q}\leq q on KK, so uε,wqu_{\varepsilon,w}\leq q on KK. Since wR𝔻nw\in R\mathbb{D}^{n}, we have

uε,w(w)(tu)χδ(w)>u(w)ε.u_{\varepsilon,w}(w)\geq(tu)*\chi_{\delta}(w)>u(w)-\varepsilon.

We also have that uε,wu_{\varepsilon,w} is continuous on n\mathbb{C}^{n}, since HSCH_{S}-C and (tu)χδ(tu)*\chi_{\delta} both are.

For every wnw\in\mathbb{C}^{n} and ε>0\varepsilon>0, we can take uS(n)u\in\mathcal{L}^{S}(\mathbb{C}^{n}), such that u|Kqu|_{K}\leq q and u(w)>VK,qS(w)εu(w)>V^{S}_{K,q}(w)-\varepsilon. Since uε,w(w)>u(w)εu_{\varepsilon,w}(w)>u(w)-\varepsilon, we have that

VK,qS(z)=sup{uε,w(z);uS(n),ε>0,wn},zn.V^{S}_{K,q}(z)=\sup\{u_{\varepsilon,w}(z)\,;\,u\in\mathcal{L}^{S}(\mathbb{C}^{n}),\ \varepsilon>0,\ w\in\mathbb{C}^{n}\},\quad z\in\mathbb{C}^{n}.

Since uε,wu_{\varepsilon,w} are continuous, we have that VK,qSV^{S}_{K,q} is lower semicontinuous on n\mathbb{C}^{n}. ∎

3 Infimal convolutions

Recall that Siciak’s infimal convolution was given by

Rμ,δau(z)=loginfwn{eu(w)+δ1μ(zw)},zn,R^{a}_{\mu,\delta}u(z)=-\log\inf_{w\in\mathbb{C}^{n}}\{e^{-u(w)}+\delta^{-1}\mu(z-w)\},\quad z\in\mathbb{C}^{n},

with μ=||\mu=|\cdot|. In Ferrier [2], it is proven that Rμ,δauR^{a}_{\mu,\delta}u is plurisubharmonic and continuous when uu is plurisubharmonic, δ=1\delta=1, and μ=||\mu=|\cdot|. Generalizing for δ>0\delta>0 is not significant. In Siciak [16], it is shown that if

log(|z|+1)cuu(z)log(|z|+1)+cu,zn,\log(|z|+1)-c_{u}\leq u(z)\leq\log(|z|+1)+c_{u},\quad z\in\mathbb{C}^{n},

for some constant cuc_{u}, then Rμ,δau(z)log(|z|+1)+cuR^{a}_{\mu,\delta}u(z)\leq\log(|z|+1)+c_{u}, for δ<ecu\delta<e^{c_{u}}, and consequently that Rμ,δau(n)R^{a}_{\mu,\delta}u\in\mathcal{L}(\mathbb{C}^{n}). He also shows that Rμ,δauuR^{a}_{\mu,\delta}u\searrow u, as δ0\delta\searrow 0. The fact that Rμ,δauR^{a}_{\mu,\delta}u is plurisubharmonic is not obvious, but follows from geometric arguments. We will recall some useful results on pseudoconvex domains before going through the proof.

Let u𝒫𝒮(n)u\in\mathcal{PSH}(\mathbb{C}^{n}). Recall that Ω={zn;u(z)<c}\Omega=\{z\in\mathbb{C}^{n}\,;\,u(z)<c\} is pseudoconvex. To see this, assume uu is continuous and take compact KΩK\subset\Omega. Note that, ucδu\leq c-\delta on KK, for some δ>0\delta>0, so ucδu\leq c-\delta on K^𝒫𝒮(n)\widehat{K}_{\mathcal{PSH}(\mathbb{C}^{n})}, which is compact. So, we have that K^𝒫𝒮(Ω)K^𝒫𝒮(n)Ω\widehat{K}_{\mathcal{PSH}(\Omega)}\subset\widehat{K}_{\mathcal{PSH}(\mathbb{C}^{n})}\subset\Omega, which implies that K^𝒫𝒮(Ω)\widehat{K}_{\mathcal{PSH}(\Omega)} is relatively compact in Ω\Omega. Hence, Ω\Omega is pseudoconvex. In the case that uu is not continuous, we consider the pseudoconvex sets Ωδ={zn;uχδ(z)<c}\Omega_{\delta}=\{z\in\mathbb{C}^{n}\,;\,u*\chi_{\delta}(z)<c\}, for δ>0\delta>0. Since ΩδΩ\Omega_{\delta}\nearrow\Omega, as δ0\delta\searrow 0, we have, by the Behnke-Stein theorem, that Ω\Omega is pseudoconvex.

We call a continuous function μ:n+\mu\colon\mathbb{C}^{n}\rightarrow\mathbb{R}_{+} a distance function if (i) μ(z)=0\mu(z)=0 if and only if z=0z=0 and (ii) μ(tz)=|t|μ(z)\mu(tz)=|t|\mu(z) for znz\in\mathbb{C}^{n} and tt\in\mathbb{C}. Note that, by (ii), we have constants rμ=inf|z|=1μ(z)r_{\mu}=\inf_{|z|=1}\mu(z) and sμ=sup|z|=1μ(z)s_{\mu}=\sup_{|z|=1}\mu(z) such that rμ|z|μ(z)sμ|z|r_{\mu}|z|\leq\mu(z)\leq s_{\mu}|z|, for znz\in\mathbb{C}^{n}, and by (i) we have that rμ>0r_{\mu}>0. For an open Ωn\Omega\subset\mathbb{C}^{n}, we define the μ\mu-distance to the boundary by

μΩ(z)=infwΩμ(zw),zΩ,\mu_{\Omega}(z)=\inf_{w\not\in\Omega}\mu(z-w),\quad z\in\Omega,

and note that it is a continuous function. Pseudoconvex domains are classically characterized by distances, namely an open Ωn\Omega\subset\mathbb{C}^{n} is pseudoconvex if and only if logμΩ-\log\mu_{\Omega} is plurisubharmonic for every (or some) distance function μ\mu. See Klimek [9, Thm. 2.10.4].

Proof of Theorem 1.2.

To start off we show that Rμ,δauR^{a}_{\mu,\delta}u is continuous and plurisubharmonic. We let

Ω={(z,a)n×;|a|<eu(z)}\Omega=\{(z,a)\in\mathbb{C}^{n}\times\mathbb{C}\,;\,|a|<e^{-u(z)}\}

and note that Ω\Omega is a sublevel set of (z,a)u(z)+log|a|(z,a)\mapsto u(z)+\log|a|, so it is pseudoconvex. We define a distance function μ^\widehat{\mu} on n+1\mathbb{C}^{n+1} by μ^(z,a)=|a|+δ1μ(z)\widehat{\mu}(z,a)=|a|+\delta^{-1}\mu(z), and see that, for (z,a)n×(z,a)\in\mathbb{C}^{n}\times\mathbb{C},

μ^Ω(z,a)=inf{|ab|+δ1μ(zw);(w,b)n×,|b|eu(w)}.\widehat{\mu}_{\Omega}(z,a)=\inf\{|a-b|+\delta^{-1}\mu(z-w)\,;\,(w,b)\in\mathbb{C}^{n}\times\mathbb{C},|b|\geq e^{-u(w)}\}.

By [9, Thm. 2.10.4], we have that logμ^Ω-\log\widehat{\mu}_{\Omega} is continuous and plurisubharmonic on Ωn×{0}\Omega\supset\mathbb{C}^{n}\times\{0\}, so nzlogμ^Ω(z,0)\mathbb{C}^{n}\ni z\mapsto-\log\widehat{\mu}_{\Omega}(z,0) is continuous and plurisubharmonic and

μ^Ω(z,0)\displaystyle\widehat{\mu}_{\Omega}(z,0) =inf{|b|+δ1μ(zw);(w,b)n×,|b|eu(w)}\displaystyle=\inf\{|b|+\delta^{-1}\mu(z-w)\,;\,(w,b)\in\mathbb{C}^{n}\times\mathbb{C},|b|\geq e^{-u(w)}\}
=infwn{eu(w)+δ1μ(zw)}=eRμ,δau(z),zn.\displaystyle=\inf_{w\in\mathbb{C}^{n}}\{e^{-u(w)}+\delta^{-1}\mu(z-w)\}=e^{-R^{a}_{\mu,\delta}u(z)},\qquad z\in\mathbb{C}^{n}.

So, Rμ,δauR^{a}_{\mu,\delta}u is plurisubharmonic and continuous.

Since SS is a lower set, we have, by [12, Thm. 5.8], that HS(zw)HS(z)+σS|w|H_{S}(z-w)\leq H_{S}(z)+\sigma_{S}|w|. So, since eHS1e^{-H_{S}}\leq 1,

Rμ,δau(z)\displaystyle R^{a}_{\mu,\delta}u(z) loginfwn{eHS(zw)+δ1ecurμ|w|}+cu\displaystyle\leq-\log\inf_{w\in\mathbb{C}^{n}}\{e^{-H_{S}(z-w)}+\delta^{-1}e^{c_{u}}r_{\mu}|w|\}+c_{u}
loginfwn{eHS(z)σS|w|+eHS(z)δ1ecurμ|w|}+cu\displaystyle\leq-\log\inf_{w\in\mathbb{C}^{n}}\{e^{-H_{S}(z)-\sigma_{S}|w|}+e^{-H_{S}(z)}\delta^{-1}e^{c_{u}}r_{\mu}|w|\}+c_{u}
HS(z)loginfwn{eσS|w|+δ1ecurμ|w|}+cu,zn.\displaystyle\leq H_{S}(z)-\log\inf_{w\in\mathbb{C}^{n}}\{e^{-\sigma_{S}|w|}+\delta^{-1}e^{c_{u}}r_{\mu}|w|\}+c_{u},\quad z\in\mathbb{C}^{n}.

Note that, if f:+f\colon\mathbb{R}_{+}\rightarrow\mathbb{R}, f(x)=eax+bxf(x)=e^{-ax}+bx for a,b>0a,b>0, then f(x)=baeax>baf^{\prime}(x)=b-ae^{-ax}>b-a. So, ff is increasing if a<ba<b. We have that δ<σS1ecurμ\delta<\sigma_{S}^{-1}e^{c_{u}}r_{\mu}, implying that σS<δ1ecurμ\sigma_{S}<\delta^{-1}e^{c_{u}}r_{\mu}.. Hence, the last infimum is obtained at w=0w=0. Therefore, Rμ,δau(z)HS(z)+cuR^{a}_{\mu,\delta}u(z)\leq H_{S}(z)+c_{u} and Rμ,δauS(n)R^{a}_{\mu,\delta}u\in\mathcal{L}^{S}(\mathbb{C}^{n}).

We let δj0\delta_{j}\searrow 0, and set uδ,w(z)=log(eu(zw)+δ1μ(w))u_{\delta,w}(z)=-\log(e^{-u(z-w)}+\delta^{-1}\mu(w)) and

Kj={wn;uδj,w(z)u(z)}.K_{j}=\{w\in\mathbb{C}^{n}\,;\,u_{\delta_{j},w}(z)\geq u(z)\}.

Since uu is bounded below, we have lim¯|z|uδj,w(z)=\varliminf_{|z|\rightarrow\infty}u_{\delta_{j},w}(z)=-\infty, and therefore KjK_{j} is bounded. We also have that uu is upper semicontinuous, so KjK_{j} is closed, and consequently compact. We also have that uδj,w(z)u_{\delta_{j},w}(z) is upper semicontinuous as a function of ww, so there exists wjKjw_{j}\in K_{j} such that Rμ,δjau(z)=uδj,wj(z)R^{a}_{\mu,\delta_{j}}u(z)=u_{\delta_{j},w_{j}}(z). Note that, uδ,w(z)u_{\delta,w}(z)\searrow-\infty, as δ0\delta\searrow 0, for all znz\in\mathbb{C}^{n} and wnw\in\mathbb{C}^{n*}. So, jKj={0}\cap_{j}K_{j}=\{0\}, wj0w_{j}\rightarrow 0 as jj\rightarrow\infty, and

u(z)limjRμ,δjau(z)=limjuδj,wj(z)lim¯ju(zwj)u(z),zn.u(z)\leq\lim_{j\rightarrow\infty}R^{a}_{\mu,\delta_{j}}u(z)=\lim_{j\rightarrow\infty}u_{\delta_{j},w_{j}}(z)\leq\varlimsup_{j\rightarrow\infty}u(z-w_{j})\leq u(z),\quad z\in\mathbb{C}^{n}.

Hence, Rμ,δauuR^{a}_{\mu,\delta}u\searrow u, as δ0\delta\searrow 0. ∎

4 Supremal convolutions

Let us recall some topological properties of 𝒫𝒮(Ω)\mathcal{PSH}(\Omega), with the goal of determining when sup\sup\mathcal{F} is upper semicontinuous, for some family 𝒫𝒮(Ω)\mathcal{F}\subset\mathcal{PSH}(\Omega) that is locally upper bounded. For more details, see Hörmander [6, Thms. 4.1.8-9] and [7, Thm. 3.2.11-13]. Recall that 𝒫𝒮(Ω)\mathcal{PSH}(\Omega) is the family of plurisubharmonic functions on Ω\Omega that are not identically -\infty on any connected component of Ω\Omega. So,

𝒫𝒮(Ω)Lloc1(Ω)𝒟(Ω).\mathcal{PSH}(\Omega)\subset L^{1}_{\text{loc}}(\Omega)\subset\mathcal{D}^{\prime}(\Omega).

The topology 𝒫𝒮(Ω)\mathcal{PSH}(\Omega) inherits from the weak topology on 𝒟(Ω)\mathcal{D}^{\prime}(\Omega) coincides with topology it inherits from Lloc1(Ω)L_{\text{loc}}^{1}(\Omega), as a Fréchet space topology with semi-norms fK|f|𝑑λf\mapsto\int_{K}|f|\ d\lambda, for compact KK. With this topology, 𝒫𝒮(Ω)\mathcal{PSH}(\Omega) is a closed subspace of Lloc1(Ω)L_{\text{loc}}^{1}(\Omega), so it is a complete metrizable space.

Furthermore, 𝒫𝒮(Ω)\mathcal{PSH}(\Omega) has a Montel property, which says that every sequence (uj)j(u_{j})_{j\in\mathbb{N}} in 𝒫𝒮(Ω)\mathcal{PSH}(\Omega), that is locally bounded above and does not converge to -\infty uniformly on every compact subset of Ω\Omega, has a subsequence that converges in 𝒫𝒮(Ω)\mathcal{PSH}(\Omega).

Sometimes, sup=sup0\sup\mathcal{F}=\sup\mathcal{F}_{0} for some 0\mathcal{F}_{0}\subset\mathcal{F} containing a minimal element. The Montel property then states that 0\mathcal{F}_{0} is relatively compact. If, in addition, 0\mathcal{F}_{0} is closed then sup\sup\mathcal{F} is upper semicontinuous. This follows from Sigurdsson [18, Prop. 2.1], which we include for the convenience of the reader.

Lemma 4.1.

Let Ωn\Omega\subset\mathbb{C}^{n} be open and \mathcal{F} be a compact family in 𝒫𝒮(Ω)\mathcal{PSH}(\Omega). Then sup\sup\mathcal{F} is upper semicontinuous and, consequently, plurisubharmonic.

Proof.

To start off the proof, we recall some essential properties of integral averages. For fLloc1(Ω)f\in L_{\text{loc}}^{1}(\Omega), we let Mrf(z)M_{r}f(z) denote the integral average of ff over a euclidean ball with center zz and radius r>0r>0, where we assume that the euclidean distance from zΩz\in\Omega to the boundary of Ω\Omega is strictly less than rr. We have that Lloc1(Ω)×n×+L_{\text{loc}}^{1}(\Omega)\times\mathbb{C}^{n}\times\mathbb{R}_{+}^{*}\rightarrow\mathbb{R}, (f,z,r)Mrf(z)(f,z,r)\mapsto M_{r}f(z) is continuous.

Let u=supu=\sup\mathcal{F}, z0Ωz_{0}\in\Omega, and aa\in\mathbb{R} such that u(z0)<au(z_{0})<a. If we can show that there exists a neighborhood VV of z0z_{0} such that u|V<au|_{V}<a then uu is upper semicontinuous. Let ε>0\varepsilon>0 such that u(z0)<aεu(z_{0})<a-\varepsilon and v0v_{0}\in\mathcal{F}, and take r0>0r_{0}>0 such that

v0(z0)Mr0v0(z0)aε.v_{0}(z_{0})\leq M_{r_{0}}v_{0}(z_{0})\leq a-\varepsilon.

By the continuity of (f,z)Mr0f(z)(f,z)\mapsto M_{r_{0}}f(z), there exists an open neighborhood U0U_{0} of v0v_{0} in 𝒫𝒮(Ω)\mathcal{PSH}(\Omega) and an open neighborhood V0V_{0} of z0z_{0} such that

Mr0v(z)<aε,vU0,zV0.M_{r_{0}}v(z)<a-\varepsilon,\quad v\in U_{0},\ z\in V_{0}.

The submean value property implies that v(z)<aεv(z)<a-\varepsilon for vU0v\in U_{0} and zV0z\in V_{0}. Since v0v_{0} was arbitrary and \mathcal{F} is compact, there exists a finite covering U1,,UU_{1},\dots,U_{\ell} of \mathcal{F} and open neighborhoods V1,,VV_{1},\dots,V_{\ell} of z0z_{0} such that v(z)<aεv(z)<a-\varepsilon, for vUjv\in U_{j} and zVjz\in V_{j}. If we set V=jVjV=\cap_{j}V_{j} then v(z)<aεv(z)<a-\varepsilon, for all vv\in\mathcal{F} and zVz\in V. So, u|V<au|_{V}<a and uu is therefore upper semicontinuous. ∎

As usual, we let 0S+n0\in S\subset\mathbb{R}^{n}_{+} be compact and convex, 1n=(1,,1)n1_{n}=(1,\dots,1)\in\mathbb{N}^{n}, and σS=φS(1n)\sigma_{S}=\varphi_{S}(1_{n}). We will allow us a slight abuse of notation by identifying a vector in n\mathbb{C}^{n}, denoted by a lower case letter, with a diagonal matrix, denoted by the corresponding upper case letter. Thus, we identify ana\in\mathbb{C}^{n} with the diagonal matrix AA with diagonal aa. In this notation, the subadditivity of the supporting function of SS implies that

(4.1) HS(Zw)\displaystyle H_{S}(Zw) =HS(Wz)=HS(z1w1,,znwn)\displaystyle=H_{S}(Wz)=H_{S}(z_{1}w_{1},\dots,z_{n}w_{n})
HS(z)+HS(w),z,wn.\displaystyle\leq H_{S}(z)+H_{S}(w),\qquad z,w\in\mathbb{C}^{n}.
Proof of Theorem 1.4.

Recall that we are studying the operator defined by

Rδbu(z)\displaystyle R^{b}_{\delta}u(z) =supwn{u(Zw)δ1log(w1n+1)}\displaystyle=\sup_{w\in\mathbb{C}^{n}}\{u(Zw)-\delta^{-1}\log(\|w-1_{n}\|_{\infty}+1)\}
=logsupwneu(Zw)(w1n+1)1/δ,zn.\displaystyle=\log\sup_{w\in\mathbb{C}^{n}}\frac{e^{u(Zw)}}{(\|w-1_{n}\|_{\infty}+1)^{1/\delta}},\qquad z\in\mathbb{C}^{n}.

With uδ,w(z)=u(Zw)δ1log(w1n+1)u_{\delta,w}(z)=u(Zw)-\delta^{-1}\log(\|w-1_{n}\|_{\infty}+1), which is plurisubharmonic, we have that Rδbu=supwnuδ,wR^{b}_{\delta}u=\sup_{w\in\mathbb{C}^{n}}u_{\delta,w}. The assumption that uu is locally bounded ensures that uδ,w𝒫𝒮(n)u_{\delta,w}\in\mathcal{PSH}(\mathbb{C}^{n}). For every δ>0\delta>0, we have that uδ,1n=uu_{\delta,1_{n}}=u, so RδbuuR^{b}_{\delta}u\geq u. Additionally,

HS(w)σSlog+wσSlog(w1n+1),wn.H_{S}(w)\leq\sigma_{S}\log^{+}\|w\|_{\infty}\leq\sigma_{S}\log(\|w-1_{n}\|_{\infty}+1),\quad w\in\mathbb{C}^{n}.

This, along with (4.1), implies that if uHS+cuu\leq H_{S}+c_{u} then

RδbuHS+supwn{(σSδ1)log(w1n+1)}+cu.R^{b}_{\delta}u\leq H_{S}+\sup_{w\in\mathbb{C}^{n}}\{(\sigma_{S}-\delta^{-1})\log(\|w-1_{n}\|_{\infty}+1)\}+c_{u}.

Since δ<σS1\delta<\sigma_{S}^{-1}, we have RδbuHS+cuR^{b}_{\delta}u\leq H_{S}+c_{u}. We also have, for all γ>0\gamma>0 and znz\in\mathbb{C}^{n},

Rδbu(z)max{supw1n+γ𝔻¯nu(Zw),HS(z)+cu+(σSδ1)log(γ+1)}.R^{b}_{\delta}u(z)\leq\max\bigg{\{}\sup_{w\in 1_{n}+\gamma\overline{\mathbb{D}}^{n}}u(Zw),H_{S}(z)+c_{u}+(\sigma_{S}-\delta^{-1})\log(\gamma+1)\bigg{\}}.

With znz\in\mathbb{C}^{n} fixed and ε>0\varepsilon>0, we may take γ\gamma small enough that u(Zw)u(z)+εu(Zw)\leq u(z)+\varepsilon for all w1n+γ𝔻¯nw\in 1_{n}+\gamma\overline{\mathbb{D}}^{n}, since uu is upper semicontinuous. Consequently,

Rδbumax{u+ε,HS+cu+(σSδ1)log(γ+1)}.R^{b}_{\delta}u\leq\max\{u+\varepsilon,H_{S}+c_{u}+(\sigma_{S}-\delta^{-1})\log(\gamma+1)\}.

The second term converges to -\infty, as δ0\delta\searrow 0. Hence, since RδbuuR^{b}_{\delta}u\geq u, we have that RδbuuR^{b}_{\delta}u\searrow u, as δ0\delta\searrow 0.

We now observe that Rδbu=supu,δR^{b}_{\delta}u=\sup\mathcal{F}_{u,\delta}, for u,δ={max{u,uδ,w};wn}\mathcal{F}_{u,\delta}=\{\max\{u,u_{\delta,w}\}\,;\,w\in\mathbb{C}^{n}\}, and u,δ𝒫𝒮(n)\mathcal{F}_{u,\delta}\subset\mathcal{PSH}(\mathbb{C}^{n}). All functions in u,δ\mathcal{F}_{u,\delta} are bounded above by HS+cuH_{S}+c_{u} and uu is a minimal element of u,δ\mathcal{F}_{u,\delta}, so u,δ\mathcal{F}_{u,\delta} is relatively compact by the Montel property. To show that u,δ\mathcal{F}_{u,\delta} is closed in 𝒫𝒮(n)\mathcal{PSH}(\mathbb{C}^{n}), and thus that RδbuR^{b}_{\delta}u is plurisubharmonic, we note that

uδ,wHS+cu+(σSδ1)log+w,wn,u_{\delta,w}\leq H_{S}+c_{u}+(\sigma_{S}-\delta^{-1})\log^{+}\|w\|_{\infty},\quad w\in\mathbb{C}^{n},

and recall as well that uu is assumed to be locally bounded below. So, fixing ana\in\mathbb{C}^{n} and U=B(z,1)U=B(z,1) as the euclidean ball with center zz and radius 11, and setting M2<M1M_{2}<M_{1} as constants such that M2u(z)cuM_{2}\leq u(z)-c_{u} and HS(z)M1H_{S}(z)\leq M_{1}, for zUz\in U, where cu>0c_{u}>0 is such that uHS+cuu\leq H_{S}+c_{u}, we have

uδ,w(z)u(z)M1M2+(σSδ1)log+w,zU,wn.u_{\delta,w}(z)-u(z)\leq M_{1}-M_{2}+(\sigma_{S}-\delta^{-1})\log^{+}\|w\|_{\infty},\quad z\in U,\ w\in\mathbb{C}^{n}.

So, if wnw\in\mathbb{C}^{n} is such that log+w(M1M2)/(δ1σS)>0\log^{+}\|w\|_{\infty}\geq(M_{1}-M_{2})/(\delta^{-1}-\sigma_{S})>0, then uδ,w(z)u(z)u_{\delta,w}(z)\leq u(z), for zUz\in U. Hence, since uRδbuu\leq R^{b}_{\delta}u, we have

Rδbu(z)=supwB¯(z,r)uδ,w(z),zU,R^{b}_{\delta}u(z)=\sup_{w\in\bar{B}(z,r)}u_{\delta,w}(z),\quad z\in U,

where r=max{1,e(M1M2)/(δ1σS)}r=\max\{1,e^{(M_{1}-M_{2})/(\delta^{-1}-\sigma_{S})}\}. If we take a sequence (wj)j(w_{j})_{j\in\mathbb{N}} in n\mathbb{C}^{n} such that vδ,wjvv_{\delta,w_{j}}\rightarrow v in 𝒫𝒮(n)\mathcal{PSH}(\mathbb{C}^{n}), where vδ,w=max{u,uδ,w}v_{\delta,w}=\max\{u,u_{\delta,w}\}, we need to show that vu,δv\in\mathcal{F}_{u,\delta}. If (wj)j(w_{j})_{j\in\mathbb{N}} is unbounded then we can pick a subsequence (wjk)knB¯(z,r)(w_{j_{k}})_{k\in\mathbb{N}}\subset\mathbb{C}^{n}\setminus\overline{B}(z,r). Since vδ,wjk=uv_{\delta,w_{j_{k}}}=u, we have that v=uu,δv=u\in\mathcal{F}_{u,\delta}. If (wj)j(w_{j})_{j\in\mathbb{N}} is bounded we can pick a convergent subsequence (wjk)k(w_{j_{k}})_{k\in\mathbb{N}} with limit ww. By the upper semicontinuity of (z,w)vδ,w(z,w)\mapsto v_{\delta,w}, we have that lim¯kvδ,wjk=vδ,w\varlimsup_{k\rightarrow\infty}v_{\delta,w_{j_{k}}}=v_{\delta,w}, and, by Hörmander [6, Thm. 4.1.9], we have that lim¯kvδ,wjk=v\varlimsup_{k\rightarrow\infty}v_{\delta,w_{j_{k}}}=v almost everywhere. So, v=vδ,wv=v_{\delta,w} almost everywhere and, since they are plurisubharmonic, we have v=vδ,wu,δv=v_{\delta,w}\in\mathcal{F}_{u,\delta}. Consequently, u,δ\mathcal{F}_{u,\delta} is compact and, by Lemma 4.1, RδbuR^{b}_{\delta}u is plurisubharmonic.

All that remains to be proven is that RδbuR^{b}_{\delta}u is lower semicontinuous. By a change of variables, we have

Rδbu(z)\displaystyle R^{b}_{\delta}u(z) =supwn{u(Zw)δ1log(w1n+1)}\displaystyle=\sup_{w\in\mathbb{C}^{n}}\{u(Zw)-\delta^{-1}\log(\|w-1_{n}\|_{\infty}+1)\}
=supwn{u(w)δ1log(Z1w1n+1)},zn.\displaystyle=\sup_{w\in\mathbb{C}^{n}}\{u(w)-\delta^{-1}\log(\|Z^{-1}w-1_{n}\|_{\infty}+1)\},\quad z\in\mathbb{C}^{n}.

So, we set vδ,w(z)=u(w)δ1log(Z1w1n+1)v_{\delta,w}(z)=u(w)-\delta^{-1}\log(\|Z^{-1}w-1_{n}\|_{\infty}+1), and note that vδ,wv_{\delta,w} is continuous on n\mathbb{C}^{*n} and Rδbu(z)=supwnvδ,w(z)R^{b}_{\delta}u(z)=\sup_{w\in\mathbb{C}^{n}}v_{\delta,w}(z), for znz\in\mathbb{C}^{*n}. So, RδbuR^{b}_{\delta}u is given as the supremum of continuous functions on the open set n\mathbb{C}^{*n}, and is consequently lower semicontinuous on n\mathbb{C}^{*n}. See Klimek [9, Lemma 2.3.2]. ∎

5 Integral convolutions over diagonal matrices

Let us recall that the regularization from Theorem 1.5 was define by

Rδcu(z)\displaystyle R^{c}_{\delta}u(z) =nu(Az)ψδ(A)𝑑λ(A)=nu((I+δB)z)ψ(B)𝑑λ(B)\displaystyle=\int_{\mathbb{C}^{n}}u(Az)\psi_{\delta}(A)\ d\lambda(A)=\int_{\mathbb{C}^{n}}u((I+\delta B)z)\psi(B)\ d\lambda(B)
=nu((1+δw1)z1,,(1+δwn)zn)ψ(w)𝑑λ(w),zn,\displaystyle=\int_{\mathbb{C}^{n}}u((1+\delta w_{1})z_{1},\dots,(1+\delta w_{n})z_{n})\psi(w)\ d\lambda(w),\quad z\in\mathbb{C}^{n},

where ψ𝒞0(n)\psi\in\mathcal{C}_{0}^{\infty}(\mathbb{C}^{n}) is rotationally symmetric in each variable and nψ𝑑λ=1\int_{\mathbb{C}^{n}}\psi\ d\lambda=1, and ψδ(z)=δ2nψ((z1n)/δ)\psi_{\delta}(z)=\delta^{-2n}\psi((z-1_{n})/\delta).

Proof of Theorem 1.5.

By the Fubini-Tonelli theorem, Rδc:Lloc1(n)Lloc1(n)R^{c}_{\delta}\colon L_{\text{loc}}^{1}(\mathbb{C}^{n})\rightarrow L_{\text{loc}}^{1}(\mathbb{C}^{n}) and RδcuuR^{c}_{\delta}u\rightarrow u, in the Lloc1L_{\text{loc}}^{1} topology, as δ0\delta\searrow 0. Also, Rδc:𝒫𝒮(n)𝒫𝒮(n)R^{c}_{\delta}\colon\mathcal{PSH}(\mathbb{C}^{n})\rightarrow\mathcal{PSH}(\mathbb{C}^{n}). By [12, Prop. 3.2], we have HS(1n+δw)δσSH_{S}(1_{n}+\delta w)\leq\delta\sigma_{S}, for all w𝔻¯nw\in\overline{\mathbb{D}}^{n}, so Rδc:S(n)S(n)R^{c}_{\delta}\colon\mathcal{L}^{S}(\mathbb{C}^{n})\rightarrow\mathcal{L}^{S}(\mathbb{C}^{n}), for all compact convex S+nS\subset\mathbb{R}_{+}^{n} containing 0. In fact, if uS(n)u\in\mathcal{L}^{S}(\mathbb{C}^{n}) and cuc_{u} is a constant such that uHS+cuu\leq H_{S}+c_{u} then, by (4.1),

Rδcu(z)\displaystyle R^{c}_{\delta}u(z) n(HS(z)+HS(1n+δw)+cu)ψ(w)𝑑λ(w)\displaystyle\leq\int_{\mathbb{C}^{n}}(H_{S}(z)+H_{S}(1_{n}+\delta w)+c_{u})\psi(w)\ d\lambda(w)
=HS(z)+CσSδ+cu,zn,\displaystyle=H_{S}(z)+C\sigma_{S}\delta+c_{u},\qquad z\in\mathbb{C}^{n},

for C=supwsuppψwC=\sup\limits_{w\in\operatorname{supp}\psi}\|w\|_{\infty}. Since the map AAzA\mapsto Az has the Jacobi determinant |z1zn|2|z_{1}\cdots z_{n}|^{2},

Rδcu(z)=nu(w)ψδ(Z1w)|z1zn|2𝑑λ(w),zn.R^{c}_{\delta}u(z)=\int_{\mathbb{C}^{n}}u(w)\psi_{\delta}(Z^{-1}w)|z_{1}\cdots z_{n}|^{-2}\ d\lambda(w),\quad z\in\mathbb{C}^{*n}.

By applying Lebesgue’s theorem on dominated convergence, we may differentiate by zjz_{j} under the integral sign arbitrarily often. So, if uLloc1(n)u\in L_{\text{loc}}^{1}(\mathbb{C}^{n}) then Rδcu𝒞(n)R^{c}_{\delta}u\in\mathcal{C}^{\infty}(\mathbb{C}^{*n}).

Note that, Rδcu(z)=Uz(ψδ)R^{c}_{\delta}u(z)=U_{z}(\psi_{\delta}), where UzU_{z} is the distribution associated to uzu_{z}, which is locally integrable since uu is locally bounded. Let us fix ana\in\mathbb{C}^{n}. Since uzuau_{z}\rightarrow u_{a}, in 𝒫𝒮(n)\mathcal{PSH}(\mathbb{C}^{n}), as zaz\rightarrow a, we have that

limzaRδcu(z)=limzaUz(ψδ)=Ua(ψδ)=Rδcu(a).\lim_{z\rightarrow a}R^{c}_{\delta}u(z)=\lim_{z\rightarrow a}U_{z}(\psi_{\delta})=U_{a}(\psi_{\delta})=R^{c}_{\delta}u(a).\qed

Recall that the operator in Theorem 1.6 is given by

Rδdu(z)=logRδceu(z)=logneu(Za)ψδ(a)𝑑λ(a),zn.R^{d}_{\delta}u(z)=\log R^{c}_{\delta}e^{u}(z)=\log\int_{\mathbb{C}^{n}}e^{u(Za)}\psi_{\delta}(a)\ d\lambda(a),\quad z\in\mathbb{C}^{n}.

We have already shown that eRδdueue^{R^{d}_{\delta}u}\searrow e^{u}, as δ0\delta\searrow 0. We also have

RδduHS+cu+logneHS(a)ψδ(A)𝑑λ(A),R^{d}_{\delta}u\leq H_{S}+c_{u}+\log\int_{\mathbb{C}^{n}}e^{H_{S}(a)}\psi_{\delta}(A)\ d\lambda(A),

if cuc_{u} is a constant such that uHS+cuu\leq H_{S}+c_{u}. To show that RδduR^{d}_{\delta}u is plurisubharmonic, we recall that following result.

Lemma 5.1.

Let Ω\Omega\subset\mathbb{C} and u:Ω[0,[u\colon\Omega\rightarrow[0,\infty[. Then logu𝒮(Ω)\log u\in\mathcal{SH}(\Omega) if and only if zu(z)e2Re(τz)𝒮(Ω)z\mapsto u(z)e^{2\operatorname{Re}(\tau z)}\in\mathcal{SH}(\Omega) for all τ\tau\in\mathbb{C}.

Proof.

To simplify notation, we denote by Re(τ)\operatorname{Re}(\tau\cdot) the function zRe(τz)z\mapsto\operatorname{Re}(\tau z). If logu\log u is subharmonic then elogu+2Re(τ)e^{\log u+2\operatorname{Re}(\tau\cdot)} is as well, since 2Re(τ)2\operatorname{Re}(\tau\cdot) is subharmonic, for all τ\tau\in\mathbb{C}.

Now assume ue2Re(τ)ue^{2\operatorname{Re}(\tau\cdot)} is subharmonic, for all τ\tau\in\mathbb{C}. We further more assume uu is smooth and u>0u>0. We have

Δlogu=4z(1uuz¯)=Δuu4u2uzuz¯=uΔu|u|2u2.\Delta\log u=4\frac{\partial}{\partial z}\left(\frac{1}{u}\frac{\partial u}{\partial\bar{z}}\right)=\frac{\Delta u}{u}-\frac{4}{u^{2}}\frac{\partial u}{\partial z}\frac{\partial u}{\partial\bar{z}}=\frac{u\Delta u-|\nabla u|^{2}}{u^{2}}.

For all τ\tau\in\mathbb{C}, we also have

0Δ(ue2Re(τ))\displaystyle 0\leq\Delta(ue^{2\operatorname{Re}(\tau\cdot)}) =4zz¯(ue2Re(τ))=4e2Re(τ)z(uz¯+τ¯u)\displaystyle=4\frac{\partial}{\partial z}\frac{\partial}{\partial\bar{z}}(ue^{2\operatorname{Re}(\tau\cdot)})=4e^{2\operatorname{Re}(\tau\cdot)}\frac{\partial}{\partial z}\left(\frac{\partial u}{\partial\bar{z}}+\bar{\tau}u\right)
=4ue2Re(τ)(Δu4u+τuuz¯+τ¯uuz+|τ|2)\displaystyle=4ue^{2\operatorname{Re}(\tau\cdot)}\left(\frac{\Delta u}{4u}+\frac{\tau}{u}\frac{\partial u}{\partial\bar{z}}+\frac{\bar{\tau}}{u}\frac{\partial u}{\partial z}+|\tau|^{2}\right)
=4ue2Re(τ)(Δu4u+|τ+1uuz|21u2uzuz¯).\displaystyle=4ue^{2\operatorname{Re}(\tau\cdot)}\left(\frac{\Delta u}{4u}+\left|\tau+\frac{1}{u}\frac{\partial u}{\partial z}\right|^{2}-\frac{1}{u^{2}}\frac{\partial u}{\partial z}\frac{\partial u}{\partial\bar{z}}\right).

As this holds for all τ\tau\in\mathbb{C} and u>0u>0, we have

0Δu4u1u2uzuz¯=Δlogu,0\leq\frac{\Delta u}{4u}-\frac{1}{u^{2}}\frac{\partial u}{\partial z}\frac{\partial u}{\partial\bar{z}}=\Delta\log u,

so logu\log u is subharmonic. For a general u0u\geq 0, we set vδ=(u+δ)χδ>0v_{\delta}=(u+\delta)*\chi_{\delta}>0, where χδ\chi_{\delta} is a standard smoothing kernel. Then, for zz\in\mathbb{C},

B(z,r)vδ(w)e2Re(τw)𝑑λ(w)B(z,r)(uχδ)(w)e2Re(τw)𝑑λ(w)+δe2Re(τz)\int_{B(z,r)}v_{\delta}(w)e^{2\operatorname{Re}(\tau w)}\ d\lambda(w)\geq\int_{B(z,r)}(u*\chi_{\delta})(w)e^{2\operatorname{Re}(\tau w)}\ d\lambda(w)+\delta e^{2\operatorname{Re}(\tau z)}

and, by the Fubini-Tonelli theorem,

B(z,r)(uχδ)(w)e2Re(τw)𝑑λ(w)=χδ(a)B(z,r)e2Re(τw)u(wa)𝑑λ(w)𝑑λ(a)\int_{B(z,r)}(u*\chi_{\delta})(w)e^{2\operatorname{Re}(\tau w)}\ d\lambda(w)=\int_{\mathbb{C}}\chi_{\delta}(a)\int_{B(z,r)}e^{2\operatorname{Re}(\tau w)}u(w-a)\ d\lambda(w)d\lambda(a)
e2Re(τz)u(za)χδ(a)𝑑λ(a)=uχδ(z)e2Re(τz).\geq e^{2\operatorname{Re}(\tau z)}\int_{\mathbb{C}}u(z-a)\chi_{\delta}(a)\ d\lambda(a)=u*\chi_{\delta}(z)e^{2\operatorname{Re}(\tau z)}.

So, vδe2Re(τ)v_{\delta}e^{2\operatorname{Re}(\tau\cdot)} satisfies the submean inequality, and is therefore subharmonic. We have already shown that this implies that logvδ\log v_{\delta} is subharmonic, and since logvδlogu\log v_{\delta}\searrow\log u, as δ0\delta\searrow 0, logu\log u must also be subharmonic. See Ransford [14, Thm. 2.4.6]. ∎

Proof of Theorem 1.6.

What remains is to show that RδduR^{d}_{\delta}u is plurisubharmonic. We fix a,bna,b\in\mathbb{C}^{n}, τ\tau\in\mathbb{C}, and set, for ζ\zeta\in\mathbb{C},

v(ζ)=Rδceu(a+ζb)e2Re(τζ)=neu(W(a+ζb))+2Re(τζ)ψδ(W)𝑑λ(W).v(\zeta)=R^{c}_{\delta}e^{u}(a+\zeta b)e^{2\operatorname{Re}(\tau\zeta)}=\int_{\mathbb{C}^{n}}e^{u(W(a+\zeta b))+2\operatorname{Re}(\tau\zeta)}\psi_{\delta}(W)\ d\lambda(W).

By [14, Thm. 2.4.8], we have that v𝒮()v\in\mathcal{SH}(\mathbb{C}). So, by Lemma 5.1, ζRδdu(a+ζb)\zeta\mapsto R^{d}_{\delta}u(a+\zeta b) is subharmonic and, consequently, RδduR^{d}_{\delta}u is plurisubharmonic. ∎

6 Uniform continuity in Lelong classes

Classically, sufficient conditions on KK such that VKV_{K} is Hölder continuous on n\mathbb{C}^{n} have been studied. See, for example, Siciak [17]. In Perera [13], this study is continued for VK,qSV^{S}_{K,q}. Her main result, stated in the abstract, claims that if SS is a convex body, and KK and qq are sufficiently regular then VK,qSV^{S}_{K,q} is α\alpha-Hölder continuous on n\mathbb{C}^{n}. The main aim of this section is to show that this result can not be true if SS is not a lower set, no matter what regularity we impose on KK and qq. We will do this by showing that if SS is not a lower set then VK,qSV^{S}_{K,q} is not uniformly continuous. Let us begin by recalling the definition of some classes of regularity.

Let UnU\subset\mathbb{C}^{n} be an open set and ff be a function on UU. We say that ff is uniformly continuous if for ε>0\varepsilon>0 there exists δ>0\delta>0 such that |f(x+y)f(x)|<ε|f(x+y)-f(x)|<\varepsilon, for all x,yUx,y\in U, such that x+yUx+y\in U and |y|<δ|y|<\delta. We say ff is α\alpha-Hölder continuous, for 0<α10<\alpha\leq 1, if

|f(x)f(y)|C|xy|α,x,yU,|f(x)-f(y)|\leq C|x-y|^{\alpha},\quad x,y\in U,

for some constant CC. We say that ff is Hölder continuous if it is α\alpha-Hölder continuous for some 0<α10<\alpha\leq 1. If ff is α\alpha-Hölder continuous for α=1\alpha=1 we say that ff is Lipschitz continuous and call CC its Lipschitz constant. Note that, Hölder continuous functions are uniformly continuous. We can describe HSH_{S} in these terms, depending on whether SS is a lower set or not.

Theorem 6.1.

Let 0S+n0\in S\subset\mathbb{R}^{n}_{+} be compact and convex. If SS is a lower set then HSH_{S} is Lipschitz continuous with Lipschitz constant σS=φS(1n)\sigma_{S}=\varphi_{S}(1_{n}). If SS is not a lower set then, for δ>0\delta>0, there exists wδ𝔻¯nw\in\delta\overline{\mathbb{D}}^{n} such that the function

(6.1) zHS(z+w)HS(z)z\mapsto H_{S}(z+w)-H_{S}(z)

is not bounded above. Hence, HSH_{S} is not uniformly continuous.

Proof.

First, we assume SS is a lower set. Then, by [12, Thm. 5.8],

HS(z)=φS(log+|z1|,,log+|zn|),zn,H_{S}(z)=\varphi_{S}(\log^{+}|z_{1}|,\dots,\log^{+}|z_{n}|),\quad z\in\mathbb{C}^{n},

where log+x=logx\log^{+}x=\log x if x>1x>1, and log+x=0\log^{+}x=0 if x1x\leq 1. Note that, log+x\log^{+}x is Lipschitz continuous with Lipschitz constant 11 and φS\varphi_{S} is Lipschitz continuous with Lipschitz constant σS\sigma_{S}. To see this, note that

φS(ξ)=φS(ξη+η)φS(ξη)+φS(η),ξ,ηn,\varphi_{S}(\xi)=\varphi_{S}(\xi-\eta+\eta)\leq\varphi_{S}(\xi-\eta)+\varphi_{S}(\eta),\quad\xi,\eta\in\mathbb{R}^{n},

so φS(ξ)φS(η)φS(ξη)\varphi_{S}(\xi)-\varphi_{S}(\eta)\leq\varphi_{S}(\xi-\eta) and consequently

φS(ξ)φS(η)φS(ξη)σSξησS|ξη|,ξ,ηn.\varphi_{S}(\xi)-\varphi_{S}(\eta)\leq\varphi_{S}(\xi-\eta)\leq\sigma_{S}\|\xi-\eta\|_{\infty}\leq\sigma_{S}|\xi-\eta|,\quad\xi,\eta\in\mathbb{R}^{n}.

With Log+z=(log+|z1|,,log+|zn|)\operatorname{Log}^{+}z=(\log^{+}|z_{1}|,\dots,\log^{+}|z_{n}|), we have

|HS(z)HS(w)|\displaystyle|H_{S}(z)-H_{S}(w)| =|φS(Log+z)φS(Log+w)|\displaystyle=|\varphi_{S}(\operatorname{Log}^{+}z)-\varphi_{S}(\operatorname{Log}^{+}w)|
σS|Log+zLog+w|σS|zw|,z,wn.\displaystyle\leq\sigma_{S}|\operatorname{Log}^{+}z-\operatorname{Log}^{+}w|\leq\sigma_{S}|z-w|,\quad z,w\in\mathbb{C}^{n}.

Before continuing, recall that φSφT\varphi_{S}\leq\varphi_{T} if and only if STS\subset T, for convex S,TnS,T\subset\mathbb{R}^{n}. So, HSHTH_{S}\leq H_{T} if and only if STS\subset T. It will prove useful to us that if SS is not a subset of TT then HSHTH_{S}-H_{T} is not bounded above.

Now assume SS is not a lower set. Then, after possibly rearranging the variables, there exists s=(s1,,sn)=(s,s′′)+×+ns=(s_{1},\dots,s_{n})=(s^{\prime},s^{\prime\prime})\in\mathbb{R}^{\ell}_{+}\times\mathbb{R}^{n-\ell}_{+} such that sSs\in S and (s,0)S(s^{\prime},0)\not\in S. By [12, Prop. 3.3], we have that HS(z,0)=HT(z)H_{S}(z^{\prime},0)=H_{T}(z^{\prime}), for zz^{\prime}\in\mathbb{C}^{\ell}, where 0T+0\in T\subset\mathbb{R}^{\ell}_{+} is compact convex and sTs^{\prime}\not\in T. So, with L=ch{0,s}+L=\operatorname{ch}\{0,s^{\prime}\}\subset\mathbb{R}^{\ell}_{+}, we have that HLHTH_{L}-H_{T} is not bounded above. Note that, for z𝔻z^{\prime}\in\mathbb{C}^{*\ell}\setminus\mathbb{D}^{\ell},

HS(z,δ,,δ)\displaystyle H_{S}(z^{\prime},\delta,\dots,\delta) =supxS(x1log|z1|++xlog|z|+(x+1++xn)logδ)\displaystyle=\sup_{x\in S}\big{(}x_{1}\log|z^{\prime}_{1}|+\dots+x_{\ell}\log|z^{\prime}_{\ell}|+(x_{\ell+1}+\dots+x_{n})\log\delta\big{)}
s1log|z1|++slog|z|+(s+1++sn)logδ\displaystyle\geq s_{1}\log|z^{\prime}_{1}|+\dots+s_{\ell}\log|z^{\prime}_{\ell}|+(s_{\ell+1}+\dots+s_{n})\log\delta
=HL(z)+(s+1++sn)logδ.\displaystyle=H_{L}(z^{\prime})+(s_{\ell+1}+\dots+s_{n})\log\delta.

So,

HS(z,δ,,δ)HS(z,0,,0)HL(z)HT(z)+Cδ,z𝔻,H_{S}(z^{\prime},\delta,\dots,\delta)-H_{S}(z^{\prime},0,\dots,0)\geq H_{L}(z^{\prime})-H_{T}(z^{\prime})+C_{\delta},\quad z^{\prime}\in\mathbb{C}^{\ell}\setminus\mathbb{D}^{\ell},

where Cδ=(s+1++sn)logδC_{\delta}=(s_{\ell+1}+\dots+s_{n})\log\delta. Consequently, (6.1) is not bounded above for w=(0,,0,δ,,δ)δ𝔻¯nw=(0,\dots,0,\delta,\dots,\delta)\in\delta\overline{\mathbb{D}}^{n}. To be clear, the first \ell elements of ww are 0. ∎

We have, by [12, Prop. 4.3], that V𝕋nS=V𝔻¯nS=HSV^{S}_{\mathbb{T}^{n}}=V^{S}_{\overline{\mathbb{D}}^{n}}=H_{S}, where 𝕋={z;|z|=1}\mathbb{T}=\{z\in\mathbb{C}\,;\,|z|=1\}. However, the previous proposition does not provide a counterexample to the main result in [13], since 𝔻n\mathbb{D}^{n} does not satisfy the boundary condition required by the Proposition and 𝕋n\mathbb{T}^{n} is not the closure of an open set. A consequence of the previous result will, however, suffice.

Corollary 6.2.

Let 0S+n0\in S\subset\mathbb{R}^{n}_{+} be compact and convex. If SS is not a lower set then +S(n)\mathcal{L}^{S}_{+}(\mathbb{C}^{n}) contains no uniformly continuous functions.

Proof.

Let δ>0\delta>0, u+S(n)u\in\mathcal{L}^{S}_{+}(\mathbb{C}^{n}), and cuc_{u} be a constant such that

HS(z)cuu(z)HS(z)+cu,zn.H_{S}(z)-c_{u}\leq u(z)\leq H_{S}(z)+c_{u},\quad z\in\mathbb{C}^{n}.

By Theorem 6.1, there exists wδ𝔻¯nw\in\delta\overline{\mathbb{D}}^{n} such that the function given by (6.1) is not bounded above. Since

u(z+w)u(z)HS(z+w)HS(z)2cu,z,wn,u(z+w)-u(z)\geq H_{S}(z+w)-H_{S}(z)-2c_{u},\quad z,w\in\mathbb{C}^{n},

the function zu(z+w)u(z)z\mapsto u(z+w)-u(z) is also not bounded above. Hence, uu is not uniformly continuous. ∎

By [12, Prop. 4.5], we have that VK,qS+S(n)V^{S*}_{K,q}\in\mathcal{L}^{S}_{+}(\mathbb{C}^{n}), for all compact convex S+nS\subset\mathbb{R}^{n}_{+} containing 0, compact KnK\subset\mathbb{C}^{n}, and admissible qq on KK. So, if SS is not a lower set then VK,qSV^{S}_{K,q} can not be uniformly continuous, and thus it can not be Hölder continuous.

There is an error in the proof of Lemma 2.4 in [13]. A major step in the proof involves finding a constant CwC_{w}, depending on ww, such that Vn,qS(z+w)HS(z)+CwV^{S}_{\mathbb{C}^{n},q}(z+w)\leq H_{S}(z)+C_{w}, for znz\in\mathbb{C}^{n}, where qq has been extended to n\mathbb{C}^{n} by standard methods of extending Hölder continuous functions. This is in contradiction to [12, Thm. 5.8], where it is shown that S(n)\mathcal{L}^{S}(\mathbb{C}^{n}) is translation invariant if and only if SS is a lower set.

The precise location of the error is the third step of the large inequality of Case 1, where it is incorrectly stated that

HS(z1,z2)=supxSx2log|z2|,z1𝔻,z2𝔻.H_{S}(z_{1},z_{2})=\sup_{x\in S}x_{2}\log|z_{2}|,\quad z_{1}\in\mathbb{D},\ z_{2}\in\mathbb{C}\setminus\mathbb{D}.

By [12, Thm. 5.8], this can only hold when SS is a lower set. We can also show that it fails by a direct counterexample.

Example 6.3.

Let S=ch{(0,0),(1,1),(1,0)}S=\operatorname{ch}\{(0,0),(1,1),(1,0)\}. Then supxSx2log|z2|=log|z2|\sup_{x\in S}x_{2}\log|z_{2}|=\log|z_{2}|. However, if |z2|>1|z_{2}|>1, then

HS(z21,z2)=supxS(x2x1)log|z2|=0,H_{S}(z_{2}^{-1},z_{2})=\sup_{x\in S}(x_{2}-x_{1})\log|z_{2}|=0,

since x2x10x_{2}-x_{1}\leq 0 for all xSx\in S.

It is worth noting that other results in [13] need correcting, as they depend on wrong results from other papers. Corollary 1.31.3 depends on [1, Prop. 3.1], which is shown to be incorrect in Example 1.3 herein. Proposition 2.32.3 also depends on [1, Prop. 3.1], as well as depending on Levenberg and Perera [10, Prop. 2.2]. Proposition 2.2 in [10] relies on constructing a strictly plurisubharmonic function in +S(n)\mathcal{L}^{S}_{+}(\mathbb{C}^{n}). This construction is the content of Section 33 in the paper. First, it is done under the assumption that SS is a convex polytope, that is S=ch{v1,,v}+nS=\operatorname{ch}\{v_{1},\dots,v_{\ell}\}\subset\mathbb{R}^{n}_{+}, where v1=0v_{1}=0. The specific function chosen is

hS(z)=log(j=1|z|vj),zn.h_{S}(z)=\log\Big{(}\sum_{j=1}^{\ell}|z|^{v_{j}}\Big{)},\quad z\in\mathbb{C}^{n}.

In the case where SS is not a convex polytope but still contains a neighborhood of 0, Levenberg and Perera [10] take a decreasing sequence of convex polytopes SjS_{j} such that jSj=S\cap_{j}S_{j}=S. They then claim that hSjh_{S_{j}} is a decreasing sequence and use its limit as a candidate function. But the sequence is not decreasing. This can be seen by considering the point 1n=(1,,1)1_{n}=(1,\dots,1). In fact, hSj(1n)=log(#extSj)h_{S_{j}}(1_{n})=\log(\#\operatorname{ext}S_{j}), where #A\#A denotes the number of elements in the set AA and extB\operatorname{ext}B denotes the set of extremal points of the convex set BB. So, if SS is not a convex polytope, then hSj(1n)+h_{S_{j}}(1_{n})\rightarrow+\infty, as j+j\rightarrow+\infty. An alternative to [10, Prop. 2.2] can be found in [19, Lemma 2.1 and Prop. 2.2], which apply when SS contains a neighborhood of 0.

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Science Institute, University of Iceland, IS-107 Reykjavík, ICELAND.

bergur@hi.is.