Some Properties of Thinness and Fine Topology with Relative Capacity
Cihan Unal, Ismail Aydin

TL;DR
This paper explores the concept of thinness in relation to a specific relative capacity within weighted variable exponent Sobolev spaces, examining its properties, connections with fine topology, and implications for potential theory.
Contribution
It introduces a new notion of thinness based on relative capacity, analyzes its properties, and compares the fine topology with the Euclidean topology in the context of potential theory.
Findings
Thinness relates to the structure of weighted variable exponent Sobolev spaces.
Fine topology differs from Euclidean topology and is significant in potential theory.
Properties of finely open and closed sets are characterized in this framework.
Abstract
In this paper, we introduce a thinness in sense to a type of relative capacity for weighted variable exponent Sobolev space. Moreover, we reveal some properties of this thinness and consider the relationship with finely open and finely closed sets. We discuss fine topology and compare this topology with Euclidean one. Finally, we give some information about importance of the fine topology in the potential theory.
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Taxonomy
TopicsAdvanced Numerical Methods in Computational Mathematics · Mathematical Approximation and Integration
Some Properties of
Thinness and Fine Topology with Relative Capacity
Cihan UNAL
Sinop University
Faculty of Arts and Sciences
Department of Mathematics
and
Ismail AYDIN
Sinop University
Faculty of Arts and Sciences
Department of Mathematics
Abstract.
In this paper, we introduce a thinness in sense to a type of relative capacity for weighted variable exponent Sobolev space. Moreover, we reveal some properties of this thinness and consider the relationship with finely open and finely closed sets. We discuss fine topology and compare this topology with Euclidean one. Finally, we give some information about importance of the fine topology in the potential theory.
Key words and phrases:
Fine topology, Thinness, Relative capacity, Weighted variable exponent Sobolev spaces
2000 Mathematics Subject Classification:
Primary 31C40, 46E35; Secondary 32U20, 43A15
1. Introduction
The history of potential theory begins in 17th century. Its development can be traced to such greats as Newton, Euler, Laplace, Lagrange, Fourier, Green, Gauss, Poisson, Dirichlet, Riemann, Weierstrass, Poincaré. We refer to the book by Kellogg [21] for references to some of the old works.
The Sobolev spaces are usually defined for open sets This makes sometimes difficulties to classical method for nonopen sets. The authors in [22] and [25] present different approach is to investigate Sobolev spaces on finely open sets. This is just a part of fine potential theory in .
Kováčik and Rákosník [24] introduced the variable exponent Lebesgue space and the Sobolev space . They present some basic properties of the variable exponent Lebesgue space and the Sobolev space such as reflexivity and Hölder inequalities were obtained. For a historical journey, we refer [9], [12], [24], [27] and [28].
The variational capacity has been used extensively in nonlinear potential theory on . Let is open and is compact. Then the relative variational -capacity is defined by
[TABLE]
where the infimum is taken over smooth and zero boundary valued functions in such that in The set of admissible functions can be replaced by the continuous first order Sobolev functions with in The -capacity is a Choquet capacity relative to For more details and historical background, see [19]. Also, Harjulehto et al. [16] defined a relative capacity with variable exponent. They studied properties of the capacity and compare it with the Sobolev capacity. In [29], the authors expanded this relative capacity to weighted variable exponent. Moreover, they investigate properties of this capacity and give some relationship between defined capacity in [16] and Sobolev capacity. Besides to these studies, the Riesz capacity which is an another representative for capacity theory has been considered by [30].
In [1] and [8], the authors have explored some properties of the -Dirichlet energy integral
[TABLE]
over a bounded domain They have discussed the existence and regularity of energy integral minimizers. As an alternative method the minimizers in one dimensional case have been studied by the authors in [15]. Moreover, Harjulehto et al. [17] considered the Dirichlet energy integral, with boundary values given in the Sobolev sense, has a minimizer provided the variable exponent satisfies a certain jump condition.
The fine topology was introduced by Cartan [6] in 1946. Classical fine topology has found many applications such as its connections to the theory of analytic functions and probability. For classical treatment we can refer [4], [7], [11], [13] and [20]. Also, Meyers [26] first generalized the fine topology to nonlinear theories. For the historical background and an excellent scientific survey we refer [19] and references therein.
In this study, we present -thin sets in sense to -relative capacity and consider the basic and advanced properties. We discuss some results about -relative capacity in -thin sets. Moreover, we generalize several properties of fine topology and find new results by Wiener type integral.
2. Notation and Preliminaries
In this paper, we will work on with Lebesgue measure . The measure is doubling if there is a fixed constant called the doubling constant of such that
[TABLE]
for every ball in Also, the elements of the space are the infinitely differentiable functions with compact support. We denote the family of all measurable functions (called the variable exponent on ) by the symbol . In this paper, the function always denotes a variable exponent. For put
[TABLE]
A measurable and locally integrable function is called a weight function. The weighted modular is defined by
[TABLE]
The weighted variable exponent Lebesgue spaces consist of all measurable functions on endowed with the Luxemburg norm
[TABLE]
When the space is the variable exponent Lebesgue space. The space is a Banach space with respect to Also, some basic properties of this space were investigated in [2], [3], [23].
We set the weighted variable exponent Sobolev spaces by
[TABLE]
with the norm
[TABLE]
where is a multiindex, and It is already known that is a reflexive Banach space.
Now, let , and Thus, the embedding holds and then the weighted variable exponent Sobolev spaces is well-defined by [[3], Proposition 2.1].
In particular, the space is defined by
[TABLE]
The function is shown as Also, the norm makes the space a Banach space. The local weighted variable exponent Sobolev space is defined in the classical way. More information on the classic theory of variable exponent spaces can be found in [10],[24].
Let is bounded and is a weight function. It is known that a function satisfy Poincaré inequality in if and only if the inequality
[TABLE]
holds [19].
Unal and Aydın [29] defined an alternative capacity -called relative -capacity-for Sobolev capacity in sense to [16]. For this, they recall that
[TABLE]
where supp is the support of . Suppose that is a compact subset of Also, they denote
[TABLE]
and define
[TABLE]
In addition, if is open, then
[TABLE]
and also for an arbitrary set we define
[TABLE]
They call the variational -capacity of relative to , briefly the relative -capacity. Also, the relative -capacity has the following properties.
- P1
. 2. P2
. If then 3. P3
. If is a subset of then
[TABLE] 4. P4
. If and are compact subsets of then
[TABLE] 5. P5
. Let is a decreasing sequence of compact subsets of for Then
[TABLE] 6. P6
. If is an increasing sequence of subsets of for then
[TABLE] 7. P7
. If for then
[TABLE]
Theorem 1**.**
[29*]*If and is a doubling measure, then there exist positive constants such that
[TABLE]
where the constants depend on , constants of doubling measure and Poincaré inequality.
Theorem 2**.**
[29*]*If and then the inequality
[TABLE]
holds where the constants depend on , constants of doubling measure and Poincaré inequality.
The proofs can be found in [29].
We say that a property holds -quasieverywhere if it satisfies except in a set of capacity zero. Recall also a function is -quasicontinuous in if for each there exists a set with the capacity of is less than such that restricted to is continuous. If the capacity is an outer capacity, we can suppose that is open. More detail can be found in [3].
Let be an open set. The space is denoted as the set of all measurable functions if there exists a -q.c. function such that a.e. in and -q.e. in . In other words, if there exist a -q.c. function such that the trace of vanishes. More detail about the space can be seen by [14], [19], [31].
Moreover, means that is a compact subset of Throughout this paper, we assume that and Also, we will denote
[TABLE]
3. The -Thinness
and Fine Topology
Now, we present -thinness and consider some properties of this thinness before considering the fine topology.
Definition 1**.**
A set is -thin at if
[TABLE]
Also, we say that is -thick at if is not -thin at
In the definition of -thinness we make a convention that the integral is 1 if . Also, the integral in (3.1) is usually called the Wiener type integral, briefly Wiener integral, as
[TABLE]
In addition, we denote the Wiener sum as
[TABLE]
Now we give a relationship between these two notions. The proof can be found in [29].
Theorem 3**.**
Assume that the hypotheses of Theorem 1 and Theorem 2 are hold. Then there exist positive constants such that
[TABLE]
for every and In particular, is finite if and only if is finite.
The previous theorem tell us that the notions and are equivalent under some conditions. In some cases, the Wiener sum is more practical than the Wiener integral .
Definition 2**.**
A set is called -finely open if is -thin at Equivalently, a set is -finely closed if it includes all points where it is not -thin. Moreover, the fine interior of briefly fine-int, is the largest -finely open set contained in In a similar way, the fine closure of briefly fine-clo is the smallest -finely closed set containing
Theorem 4**.**
The -fine topology on is generated by -finely open sets.
Proof.
Firstly, we denote
[TABLE]
It is obvious that Since we have
[TABLE]
This follows that Now, we assert that finite intersections of -finely open sets are -finely open. Assume that where are -finely open. Thus, if we consider the subadditivity of relative -capacity and the cases of the exponent as and then we get
[TABLE]
where depends on Therefore is -finely open. Finally, we need to show that arbitrary unions of -finely open sets are -finely open. Let where are -finely open sets, and is an index set. Thus, for every we have
[TABLE]
Moreover, it is clear that or equivalently for If we consider the properties of relative -capacity and (3.2), then we get
[TABLE]
Therefore, is -thin at and as was arbitrary, is -finely open.
Corollary 1**.**
Every open set is -finely open.
Proof.
Assume that is an open set in For every by the definition of openness, there exists a such that It is easy to see that for small enough . This follows that
[TABLE]
,that is, is -finely open.
Remark 1**.**
By the similar method in Corollary 1, it can be shown that every closed set is -finely closed and that finite union of -finely closed sets is -finely closed again.
Corollary 2**.**
The -fine topology generated by the -finely open sets is finer than Euclidean topology.
The opposite claim of Corollary 1 is not true in general. To see this, we give the Lebesgue spine
[TABLE]
as a counter example, see [5, Example 13.4].
Now, we consider the more general case in sense to Corollary 1.
Theorem 5**.**
Assume that is an open or -finely open set. Moreover, let, the relative -capacity of is zero. Then is -finely open.
Proof.
By the Corollary 1, we can consider that is an open set. Thus, for all
[TABLE]
Moreover, if we consider the properties of relative -capacity, for all and , we have
[TABLE]
Using the (3.3) and (3.4), we get
[TABLE]
This completes the proof.
Now, we give that -thinness is a local property.
Theorem 6**.**
* is -thin at if and only if for any the set is -thin at *
Proof.
Let and Assume that is -thin at This follows that
[TABLE]
By the monotonicity of relative -capacity, we have
[TABLE]
for any . This completes the necessary condition part of the proof. Now, we assume that for any the set is -thin at Thus (3.5) is satisfied for all in particular, for Let is -thick at Then we have
[TABLE]
This is a contradiction. That is the desired result.
Theorem 7**.**
Let the hypotheses of Theorem 3 hold. Moreover, assume that there is a point such that is -thin at Then there exist a point and such that
[TABLE]
Proof.
Since is -thin at , by the Theorem 3, we have
[TABLE]
This follows that
[TABLE]
By the definition of limit, we get the desired result.
Remark 2**.**
The proof of the previous theorem can be considered by using Wiener integral with similar method. Here, there is not necessary the condition that the hypotheses of Theorem 3 are hold.
Definition 3**.**
Let be a -finely open set. A function is -finely continuous at if is -thin at for each
Remark 3**.**
Assume that is a -finely open set and is -finely continuous at Then is continuous function with respect to the -fine topology on Indeed, if we consider the definition of finely continuous, then the set is -finely open. This follows that is continuous at in sense to the -fine topology on . The converse argument is still an open problem, see [14]. Moreover, this argument for the constant exponent was considered by [25, Teorem 2.136].
It is note that a set is a -fine neighbourhood of a point if and only if and is -thin at see [19].
Theorem 8**.**
Let and Assume that is -thin at . Then there exists an open neighbourhood of such that is -thin at and
Proof.
Using the same methods in the Theorem 2 and Theorem 1, it can be found for that
[TABLE]
and
[TABLE]
where the constants in depend on , , , constants of doubling measure and Poincaré inequality, see [29]. If we consider the Theorem 2 and the monotonicity of relative -capacity, then we have
[TABLE]
By the definition of relative -capacity, it can be taken open sets such that
[TABLE]
Denote
[TABLE]
where It is easy to see that is open, holds and Since holds for it is clear that . By (3.8), we have
[TABLE]
Moreover, if we consider (3.6), then we get
[TABLE]
By (3.7), the inequality
[TABLE]
holds. If we combine (3.9) and (3.10), then we have
[TABLE]
Since is -thin at by considering the definition of Wiener sum we conclude
[TABLE]
This follows that
[TABLE]
Hence is -thin at Thus the claim is follows from definition of open neighbourhood.
Now, we consider the usage area of -fine topology in potential theory. We define -Laplace equation as
[TABLE]
for every
Definition 4**.**
([31]) Let for be an open set. A function called a (weak) weighted solution (briefly -solution) of (3.11) in , if
[TABLE]
whenever Moreover, a function is a (weak) weighted supersolution (briefly -supersolution) of (3.11) in , if
[TABLE]
whenever is nonnegative. A function is a weighted subsolution in if is a -supersolution in , and a weighted solution in .
Definition 5**.**
([14], [19]) A function is -superharmonic in if
- (i)
f is lower semicontinuous, 2. (ii)
f is finite almost everywhere, 3. (iii)
Assume that is an open set. If is a -solution in which is continuous in and satisfies on then in
Note that every -supersolution in , which satisfies
[TABLE]
for all is -superharmonic in On the other hand every locally bounded -superharmonic function is a -supersolution. The proof can be easily seen by using the similar method in [18], [19].
Let be the class of all -superharmonic functions in . Since -superharmonic functions are lower semicontinuous and since is closed under truncations, -fine topology is the coarsest topology on making all locally bounded -superharmonic functions continuous, see [19].
4. Acknowledgment
We express our thanks to Professor Jana Björn for kind comments and helpful suggestions.
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