99 research outputs found

    Martin boundary of a fine domain and a Fatou-Naim-Doob theorem for finely superharmonic functions

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    We construct the Martin compactification Uˉ{\bar U} of a fine domain UU in RnR^n, n≥2n\ge 2, and the Riesz-Martin kernel KK on U×UˉU \times{\bar U}. We obtain the integral representation of finely superharmonic fonctions ≥0\ge 0 on UU in terms of KK and establish the Fatou-Naim-Doob theorem in this setting.Comment: Manuscript as accepted by publisher. To appear in Potential Analysi

    Sweeping at the Martin boundary of a fine domain

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    We study sweeping on a subset of the Riesz-Martin space of a fine domain in \RR^n (n≥2n\ge2), both with respect to the natural topology and the minimal-fine topology, and show that the two notions of sweeping are identical.Comment: Minor correctio

    Domains of existence for finely holomorphic functions

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    We show that fine domains in C\mathbf{C} with the property that they are Euclidean FσF_\sigma and GδG_\delta, are in fact fine domains of existence for finely holomorphic functions. Moreover \emph{regular} fine domains are also fine domains of existence. Next we show that fine domains such as C∖Q\mathbf{C}\setminus \mathbf{Q} or C∖(Q×iQ)\mathbf{C}\setminus (\mathbf{Q}\times i\mathbf{Q}), more specifically fine domains VV with the properties that their complement contains a non-empty polar set EE that is of the first Baire category in its Euclidean closure KK and that (K∖E)⊂V(K\setminus E)\subset V, are NOT fine domains of existence.Comment: 13 pages 1 figure. This new version has Bent Fuglede as coauthor. We extended the main result to include that regular fine domains are fine domains of existence and corrected many typo's and inaccuracies. In the third version a mistake at the end of the proof of Proposition 2.6 has been correcte

    Plurisubharmonic and holomorphic functions relative to the plurifine topology

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    A weak and a strong concept of plurifinely plurisubharmonic and plurifinely holomorphic functions are introduced. Strong will imply weak. The weak concept is studied further. A function f is weakly plurifinely plurisubharmonic if and only if f o h is finely subharmonic for all complex affine-linear maps h. As a consequence, the regularization in the plurifine topology of a pointwise supremum of such functions is weakly plurifinely plurisubharmonic, and it differs from the pointwise supremum at most on a pluripolar set. Weak plurifine plurisubharmonicity and weak plurifine holomorphy are preserved under composition with weakly plurifinely holomorphic maps.Comment: 28 page

    Constrained minimum Riesz and Green energy problems for vector measures associated with a generalized condenser

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    For a finite collection A=(Ai)i∈I\mathbf A=(A_i)_{i\in I} of locally closed sets in Rn\mathbb R^n, n⩾3n\geqslant3, with the sign ±1\pm1 prescribed such that the oppositely charged plates are mutually disjoint, we consider the minimum energy problem relative to the α\alpha-Riesz kernel ∣x−y∣α−n|x-y|^{\alpha-n}, α∈(0,2]\alpha\in(0,2], over positive vector Radon measures μ=(μi)i∈I\boldsymbol\mu=(\mu^i)_{i\in I} such that each μi\mu^i, i∈Ii\in I, is carried by AiA_i and normalized by μi(Ai)=ai∈(0,∞)\mu^i(A_i)=a_i\in(0,\infty). We show that, though the closures of oppositely charged plates may intersect each other even in a set of nonzero capacity, this problem has a solution λAξ=(λAi)i∈I\boldsymbol\lambda^{\boldsymbol\xi}_{\mathbf A}=(\lambda^i_{\mathbf A})_{i\in I} (also in the presence of an external field) if we restrict ourselves to μ\boldsymbol\mu with μi⩽ξi\mu^i\leqslant\xi^i, i∈Ii\in I, where the constraint ξ=(ξi)i∈I\boldsymbol\xi=(\xi^i)_{i\in I} is properly chosen. We establish the sharpness of the sufficient conditions on the solvability thus obtained, provide descriptions of the weighted vector α\alpha-Riesz potentials of the solutions, single out their characteristic properties, and analyze the supports of the λAi\lambda^i_{\mathbf A}, i∈Ii\in I. Our approach is based on the simultaneous use of the vague topology and an appropriate semimetric structure defined in terms of the α\alpha-Riesz energy on a set of vector measures associated with A\mathbf A, as well as on the establishment of an intimate relationship between the constrained minimum α\alpha-Riesz energy problem and a constrained minimum α\alpha-Green energy problem, suitably formulated. The results are illustrated by examples.Comment: 35 pages. arXiv admin note: substantial text overlap with arXiv:1711.0548

    An alternative concept of Riesz energy of measures with application to generalized condensers

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    In view of a recent example of a positive Radon measure μ\mu on a domain D⊂RnD\subset\mathbb R^n, n⩾3n\geqslant3, such that μ\mu is of finite energy Eg(μ)E_g(\mu) relative to the α\alpha-Green kernel gg on DD, though the energy of μ−μDc\mu-\mu^{D^c} relative to the α\alpha-Riesz kernel ∣x−y∣α−n|x-y|^{\alpha-n}, 0<α⩽20<\alpha\leqslant2, is not well defined (here μDc\mu^{D^c} is the α\alpha-Riesz swept measure of μ\mu onto Dc=Rn∖DD^c=\mathbb R^n\setminus D), we propose a weaker concept of α\alpha-Riesz energy for which this defect has been removed. This concept is applied to the study of a minimum weak α\alpha-Riesz energy problem over (signed) Radon measures on Rn\mathbb R^n associated with a (generalized) condenser A=(A1,Dc){\mathbf A}=(A_1,D^c), where A1A_1 is a relatively closed subset of DD. A solution to this problem exists if and only if the gg-capacity of A1A_1 is finite, which in turn holds if and only if there exists a so-called measure of the condenser A\mathbf A, whose existence was analyzed earlier in different settings by Beurling, Deny, Kishi, Bliedtner, and Berg. Our analysis is based particularly on our recent result on the completeness of the cone of all positive Radon measures μ\mu on DD with finite Eg(μ)E_g(\mu) in the metric determined by the norm ∥μ∥g:=Eg(μ)\|\mu\|_g:=\sqrt{E_g(\mu)}. We also show that the pre-Hilbert space of Radon measures on Rn\mathbb R^n with finite weak α\alpha-Riesz energy is isometrically imbedded into its completion, the Hilbert space of real-valued tempered distributions with finite energy, defined with the aid of Fourier transformation. This gives an answer in the negative to a question raised by Deny in 1950.Comment: 23 pages. arXiv admin note: text overlap with arXiv:1802.07171, arXiv:1711.0548
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