Abstract
The aim of this paper is to prove continuity of the Riesz potential operator \(R^{s}:E\mapsto{\mathcal {C}}H\) in optimal couple E, \({\mathcal {C}}H\), for the supercritical case on unbounded domain, where E is a rearrangement invariant function space and \({\mathcal {C}}H\) is the generalized Hölder-Zygmund space generated by a function space H. We also construct optimal domain and target quasi-norms for \(R^{s}\) on unbounded domain.
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1 Introduction
Let \(L_{\mathrm{loc}}\) be the space of all locally integrable functions f on \({\mathbf {R}}^{n}\) with lebesgue measure. The Riesz potential operator \(R^{s}\), \(0< s< n\), \(n\geq1\) is defined by
where \(f\in L_{\mathrm{loc}}\).
It is well known that in the supercritical case \(s>n/p\),
where \({\mathcal {C}}^{\gamma}\); \(\gamma>0\) is Hölder-Zygmund space [1], but in the critical case \(s=n/p\) the function \(R^{s}f\) may not be even continuous. We prove the optimal one is obtained if in above \(L^{p}\) is replaced by Marcinkiewicz space \(L^{p,\infty}\). In this paper we prove similar optimal results, when \(L^{p,\infty}\) is replaced by more general rearrangement invariant spaces E. More precisely, we consider quasi-norm rearrangment invariant space E, consisting of functions \(f\in L^{1}+L^{\infty}\), such that the quasi-norm \(\|f\|_{E}=\rho (f^{\ast})<\infty\), where \(\rho_{E}\) a monotone quasi-norm, defined on \(M^{+}\) with values in \([0,\infty]\). Here \(M^{+}\) is the cone of all locally integrable functions \(g\ge0\) on \((0,\infty)\) with Lebesgue measure.
Monotonicity means that \(g_{1}\leq g_{2}\) implies \(\rho_{E}(g_{1})\leq\rho_{E}(g_{2})\). We suppose that \(L^{1}\cap L^{\infty}\hookrightarrow E\hookrightarrow L^{1}+L^{\infty}\), which means continuous embeddings. Here \(f^{\ast}\) is the decreasing rearrangement of f, given by
and \(\mu_{f}\) is the distribution function of f, defined by
\(\vert \cdot \vert _{n}\) denoting the Lebesgue n-measure.
Finally,
Let \(\alpha_{E}\), \(\beta_{E}\) be the Boyd indices of E (see [2–4]). For example, if \(E=L^{p}\), then \(\alpha_{E}=\beta_{E}=1/p\) and the condition \(1>s/n\geq1/p\) means \(p>1\), \(\beta_{E} <1\). For these reasons we suppose that for the general E, \(0<\alpha_{E}=\beta_{E}\leq1\), and the case \(s/n>\alpha_{E}\) is called supercritical, while the case \(s/n=\alpha_{E}\) is called critical. In the supercritical case the function \(R^{s}f\); \(f\in E\) is always continuous [5], while the spaces in the critical case \(\alpha_{E}=s/n\), can be divided into two subclasses: in the first subclass the functions \(R^{s}f\) may not be continuous; then the target space is rearrangement invariant, while these functions in the second subclass are continuous and the target space is the generalized Hölder-Zygmund space \({\mathcal {C}}H\) [6, 7]. The separating space for these two subclasses is given by the Lorentz space \(L^{n/s,1}\). The continuity of fractional maximal operator and Bessel potential operator is discussed in [8] and [9]. Gogatishvili and Ovchinnikov in [10] discussed the optimal Sobolev’s embeddings. The problem of the optimal target rearrangement invariant spaces for potential type operators is considered in [11] by using \(L_{p}\)-capacities. The problem of mapping properties of the Riesz potential in optimal couples of rearrangement invariant spaces is treated in [12–15]. The characterization of the continuous embedding of the generalized Bessel potential spaces into Hölder-Zygmund spaces \(\mathcal{CH}\), when H is a weighted Lebesgue space, is given in [7]. For further literature and reviews, we refer the reader to [16–20].
The main goal of this paper is to prove continuity of the Riesz potential operator \(R^{S}:E\mapsto{\mathcal {C}}H\) in an optimal couple E, \({\mathcal {C}}H\), for the supercritical case on unbounded domain. The same problem was considered in [5] for bounded domain. The critical and subcritical case for the continuity of Riesz potential operator was considered in [12] and [14].
The plane of this paper is as follows. In Section 2 we provide some basic definitions and known results. In Section 3 we characterize the continuity of the Riesz potential operator \(R^{S}:E\mapsto{\mathcal {C}}H\). The optimal quasi-norms are constructed in Section 4.
2 Preliminaries
We use the notations \(a_{1}\lesssim a_{2}\) or \(a_{2}\gtrsim a_{1}\) for nonnegative functions or functionals to mean that the quotient \(a_{1}/a_{2}\) is bounded; also, \(a_{1}\approx a_{2}\) means that \(a_{1}\lesssim a_{2}\) and \(a_{1}\gtrsim a_{2}\). We say that \(a_{1}\) is equivalent to \(a_{2}\) if \(a_{1}\approx a_{2}\).
There is an equivalent quasi-norm \(\rho_{p}\approx\rho_{E}\) that satisfies the triangle inequality \(\rho_{p}^{p}(g_{1}+g_{2})\leq\rho_{p}^{p}(g_{1})+\rho _{p}^{p}(g_{2})\) for some \(p\in(0,1]\) that depends only on the space E (see [21]). We say that the quasi-norm \(\rho_{E}\) satisfies Minkowski’s inequality if for the equivalent quasi-norm \(\rho_{p}\),
Usually we apply this inequality to functions \(g\in M^{+}\) with some kind of monotonicity.
Recall the definition of the lower and upper Boyd indices \(\alpha_{E}\) and \(\beta_{E}\). Let \(g_{u}(t)=g(t/u)\) where \(g\in M^{+}\), and let
be the dilation function generated by \(\rho_{E}\). Suppose that it is finite. Then
The function \(h_{E}\) is sub-multiplicative, increasing, \(h_{E}(1)=1\), \(h_{E}(u) h_{E}(1/u)\geq1\) hence \(0\leq\alpha _{E}\leq\beta_{E}\). We suppose that \(0<\alpha_{E}=\beta_{E}\leq1\) and \(g^{\ast \ast}(\infty)=0\).
If \(\beta_{E}<1\) we have by using Minkowski’s inequality that \(\rho_{E}(f^{\ast})\approx\rho_{E}(f^{\ast\ast})\).
Recall that \(w\in M^{+}\) is slowly varying function, if for every \(\epsilon>0\), the function \(t^{\epsilon}w(t)\) is equivalent to increasing function and \(t^{-\epsilon}w(t)\) is equivalent to a decreasing function.
In order to introduce the Hölder-Zygmund class of spaces, we denote the modulus of continuity of order k by
where \(\Delta^{k}_{h} f\) are the usual iterated differences of f. When \(k=1\) we simply write \(\omega(t,f)\). Let H be a quasi-normed space of locally integrable functions on the interval \((0,1)\) with the Lebesgue measure, continuously embedded in \(L^{\infty}(0,1)\) and \(\|g\|_{H}=\rho_{H}(|g|)\), where \(\rho_{H}\) is a monotone quasi-norm on \(M^{+}\) which satisfies Minkowski’s inequality. The dilation function \(h_{H}\), generated by \(\rho_{H}\), is defined as follows:
where \(( {\tilde{g}}_{u})(t)=g(ut)\) if \(ut<1\), \(( {\tilde{g}}_{u})(t)=g(1)\) if \(ut\geq1\), and
The choice of the space \(M_{a}\) is motivated by the fact that \(\omega ^{n}(t^{1/n},f)\), is equivalent to a function \(g\in M_{a}\).
The function \(h_{H}(u)\) is sub-multiplicative and \(u^{-1} h_{H}(u)\) is decreasing and
Suppose that \(h_{H}\) is finite. Then the Boyd indices of H are well defined,
and they satisfy \(\alpha_{H}\leq\beta_{H}\leq1\). In the following, we suppose that \(0\leq\alpha_{H}=\beta_{H}< 1\).
For example, let \(H=L^{q}_{\ast}(b(t) t^{-\gamma/n})\). Here \(0\leq\gamma< a/n\) and b is a slowly varying function, and \(L^{q}_{\ast}(w)\), or simply \(L^{q}_{\ast}\) if \(w=1\), is the weighted Lebesgue space with a quasi-norm \(\|g\|_{L^{q}_{\ast}(w)}=\rho_{w,q}(|g|)\). It turns out that \(\alpha_{H}=\beta_{H}=\gamma/n\).
Definition 2.1
Let \(j=0,1,\dots \) and let \({C}^{j}\) stand for the space of all functions f, defined on \({\mathbf {R}}^{n} \), that have bounded and uniformly continuous derivatives up to the order j, normed by \(\|f\|_{{C}^{j}}=\sup\sum_{l=0} ^{j} |P^{l} f(x)| \), where \(P^{l} f(x) =\sum_{|\nu|=l} D^{\nu}f(x) \).
-
If \(j/n<\alpha_{H}<(j+1)/n\) for \(j\geq1\) or \(0\leq\alpha_{H}<1/n\) for \(j=0\), then \({\mathcal {C}} H\) is formed by all functions f in \({C}^{j}\) having a finite quasi-norm
$$ \|f\|_{{\mathcal {C}} H}= \|f\|_{{ C}^{j}}+\rho_{H} \bigl(t^{j/n}\omega \bigl(t^{1/n},P^{j} f\bigr)\bigr). $$ -
If \(\alpha_{H}=(j+1)/n\), then \({\mathcal {C}} H\) consists of all functions f in \({C}^{j}\) having a finite quasi-norm
$$ \|f\|_{{\mathcal {C}} H}= \|f\|_{{ C}^{j}}+\rho_{H} \bigl(t^{j/n}\omega ^{2}\bigl(t^{1/n},P^{j} f\bigr)\bigr). $$
In particular, if \(H=L^{\infty}(t^{-\gamma/n})\), \(\gamma>0\), then \({\mathcal {C}} H\) coincides with the usual Hölder-Zygmund space \({\mathcal {C}}^{\gamma}\) (see [1]). Also, if \(H=L^{\infty}\), then \({\mathcal {C}} H= C^{0}\). We need the following result about the equivalent quasi-norm in the generalized Hölder-Zygmund spaces.
Theorem 2.2
(equivalence) ([6])
Let \(\rho_{H}\) be a monotone quasi-norm, satisfying Minkowski’s inequality and let \(0\leq\alpha_{H}=\beta_{H}< m/n\). If \(\rho _{H}(t^{\alpha})<\infty\) for \(\alpha>\alpha_{H}\), then, for all such m,
Let N be the class of all admissible couples, it will be convenient to use the following definitions.
Definition 2.3
(admissible couple)
We say that the couple \((\rho_{E},\rho_{H})\in N\) is admissible for the Riesz potential if
Then the couple E, H is called admissible. Moreover, \(\rho_{E}\) (E) is called domain quasi-norm (domain space), and \(\rho_{H}\) (H) is called the target quasi-norm (target space).
To prove our result we introduce the classes of the domain and target quasi-norms, where the optimality is investigated.
Let \(N_{d}\) consist of all domain quasi-norms \(\rho_{E}\) that are monotone, satisfy Minkowski’s inequality, \(0<\alpha_{E}=\beta_{E}<1\), and the condition
\(\int_{0}^{\infty} g^{\ast}(u)\,du\lesssim\rho_{E}(g^{\ast})\) and \(\rho_{E}(\chi _{(0,1)}t^{-\alpha})<\infty\) if \(\alpha<\alpha_{E}\).
Let \(N_{t}\) consist of all target quasi-norms \(\rho_{H}\) that are monotone, satisfy Minkowski’s inequality, \(0\leq\alpha_{H}=\beta_{H}< 1\), \(\rho _{H}(t^{\alpha})<\infty\) if \(\alpha>\alpha_{H}\) and \(\sup\chi _{(0,1)}g(t)\lesssim\rho_{G}(\chi_{(0,1)}g)\), \(g \in M_{n}\).
Finally
Definition 2.4
(optimal target quasi-norm)
Given the domain quasi-norm \(\rho_{E}\), the optimal target quasi-norm, denoted by \(\rho_{H(E)}\), is the strongest target quasi-norm, such that \((\rho_{E},\rho_{H(E)})\in N\) and
for any target quasi-norm \(\rho_{H}\) such that the couple \((\rho_{E}, \rho _{H})\in N\) is admissible. Since \({\mathcal {C}}H(E)\hookrightarrow {\mathcal {C}}H\), we call \({\mathcal {C}}H(E)\) the optimal Hölder-Zygmund space. For shortness, the space \(H(E)\) is also called an optimal target space.
Definition 2.5
(optimal domain quasi-norm)
Given the target quasi-norm \(\rho_{H}\in N_{t}\), the optimal domain quasi-norm, denoted by \(\rho_{E(H)}\), is the weakest domain quasi-norm, such that \((\rho_{E(H)},\rho_{H})\in N\) and
for any domain quasi-norm \(\rho_{E}\in N_{d}\) such that the couple \((\rho _{E}, \rho_{H})\in N\) is admissible. The space \(E(H)\) is called an optimal domain space.
Definition 2.6
(optimal couple)
The admissible couple \((\rho_{E},\rho_{H})\in N\) is said to be optimal if both \(\rho_{E}\) and \(\rho_{H}\) are optimal. Then the couple E, H is called optimal.
3 Admissible couples
Here we give a characterization of all admissible couples \((\rho_{E}, \rho _{H})\in N\). By using the following Hardy-Littlewood inequality [2], p.44, we get the well-known mapping property:
Now from (2.3) it follows that
We have the following basic estimate.
Theorem 3.1
If \(f\in E\), then
where
Proof
The proof of this result follows from Theorem 3.1 in [5]. □
Now we discuss the mapping property \(R^{s}:E\mapsto C^{0}\).
Theorem 3.2
A necessary and sufficient condition for the mapping
is the following:
Proof
We already know that
To prove that \(R^{s}(E)\subset C^{0}\), it remains to show that \(R^{s} f \) is a uniformly continuous function. It is enough to show that
By using Marchaud’s inequality,
L’Hôpital’s rule, and (3.2), we get
Hence
It remains to prove that if \(R^{s}:E \rightarrow C^{0}\), then (3.4) is true for \(\alpha_{E}\leq s/n\). To this end we choose a test function h as follows. Let \(g\in D_{n-s}\), \(\rho_{E}(g)<\infty\) and
where \(\varphi\geq0\) is a smooth function with compact support in \((-c^{-1/n},c^{-1/n})\) such that if \(\psi=R^{s} \varphi\), then \(\psi(0)>0\). To see that this is possible, we calculate \(\psi(0)\). Since
we have for appropriate \(d>0\),
Note also that, for large \(c>0\),
Indeed
since
We also have
Hence
We may take
hence, for appropriate \(c>0\),
Applying Minkowski’s inequality and using \(\alpha_{E}>0\), we have
Given that
we have in particular
whence
Thus (3.4) is proved. □
In the following theorem, we characterize the admission couple. Note that this result cannot obtained directly from Theorem 3.4 [5], because here we consider an unbounded domain.
Theorem 3.3
The couple \((\rho_{E},\rho_{H})\in N\) is admissible if and only if
Proof
Let (3.9) be true. By using (3.2) and (3.9), we get
Therefore
Thus \(\rho_{E}\), \(\rho_{H}\) is an admissible couple.
For the converse, we have to prove that (2.2) implies (3.9). To this end we choose a test function in the form \(f(x)=R^{s}h(x)\), where h is given by (3.6). We have
To estimate the modulus of continuity of f from below, we split f as follows:
where
First we prove that, for some large \(C>0\),
To this aim consider
Also consider
If \(|h|=Ct^{\frac{1}{n}}\), then for \(u< t\), \(k\geq1\), \(|h|ku^{-\frac{1}{n}} \geq Ck \geq C\), hence by (3.7) and for large \(C>0\),
Therefore,
and, for large \(C>0\),
Hence
or
Further,
Now we estimate the modulus of continuity of the second function from above. To this aim, by using the formula [2], p.336, we get
Hence
Therefore
To simplify (3.11), consider
So (3.11) becomes
whence for \(m>s\), we have
Hence
Now since \((\rho_{E},\rho_{H})\in N\), we get
□
4 Optimal quasi-norms
Here we give a characterization of the optimal domain and optimal target quasi-norms.
4.1 Optimal domain quasi-norms
We can construct an optimal domain quasi-norm \(\rho_{E(H)}\) by Theorem 3.3 as follows.
Definition 4.1
(construction of an optimal domain quasi-norm)
For a given target quasi-norm \(\rho_{H}\in N_{t}\) we set
Note that
Theorem 4.2
The couple \(\rho_{E(H)}\), \(\rho_{H}\) is admissible and the domain quasi-norm \(\rho_{E(H)}\) is optimal. Moreover, the target quasi-norm \(\rho_{H}\) is also optimal and
Proof
The couple \(\rho_{E(H)}\), \(\rho_{H}\) is admissible since
Moreover, \(\rho_{E(H)}\) is optimal, since for any admissible couple \((\rho_{E_{1}},\rho_{H})\in N\) we have
Therefore,
To prove that \(\rho_{H}\) is also optimal, let \((\rho_{E(H)},\rho _{H_{1}})\in N\) be an arbitrary admissible couple. Then
We have to show that
Since \(g\in M_{n}\) is a quasi-concave, it is equivalent to a concave one, hence
Let
Therefore
Thus (4.3) is proved.
To prove the equivalence (4.2), first we prove that
To this aim we consider
Applying Minkowski’s inequality and using \(\alpha_{H}>0\), we have
For the reverse we use
whence
□
Example 4.3
Consider the space \(H=L^{1}_{\ast}(v)\), where v is slowly varying and \(v>1\). Then \(\rho_{H}\in N_{t}\) and by Theorem 4.2, we can construct an optimal domain \(E(H)\), where
and \(w(u)=\int_{u}^{1} v(t)\frac{dt}{t}\). Hence \(E(H)=\Lambda^{1}(t^{s/n}w)\) and this couple is optimal. Also \(\alpha_{E}=\beta_{E}=s/n\).
Example 4.4
Let \(H=L^{\infty}(v)\), where v is slowly varying and \(v>1\). Then \(\rho _{H}\in N_{t}\). Let
Then by Theorem 4.2 this is an optimal domain quasi-norm and the couple \(\rho_{E}\), \(\rho_{H}\) is optimal. In particular, the couple \(\Lambda^{1}(t^{s/n})\), \(C^{0}\) is optimal.
4.2 Optimal target quasi-norms
Definition 4.5
(construction of an optimal target quasi-norm)
For a given domain quasi-norm \(\rho_{E}\in N_{d}\), we set
Note that
Theorem 4.6
The target quasi-norm \(\rho_{H(E)}\in N_{t}\), the couple \(\rho_{E}\), \(\rho_{H(E)}\) is admissible, and the target quasi-norm is optimal.
Proof
The couple \(\rho_{E}\), \(\rho_{H(E)}\) is admissible since
Now to prove that \(\rho_{H(E)}\) is optimal, we take any admissible couple \(\rho_{E}, \rho_{H_{1}}\in N_{t}\). Then
Therefore, if \(g\leq Sh\), h↓, then
whence, taking the infimum, we get
Hence \(\rho_{H(E)}\) is optimal. □
Theorem 4.7
If \(\alpha_{E}< s/n\), then
Moreover, the couple \(\rho_{E}\), \(\rho_{H(E)}\) is optimal.
Proof
Consider
Applying Minkowski’s inequality and using \(\beta_{E}< s/n\), we have
If \(\chi_{(0,1)}g\leq Sh\), \(g\in M_{n}\), then
and, taking the infimum, we get
On the other hand, for \(g\in M_{n}\), let \(h(t)=t^{-s/n}g(t)\chi _{(0,1)}(t)\). Then h↓ and
Therefore
Now we show that the domain quasi-norm \(\rho_{E}\) is also optimal. We have
Therefore
□
Example 4.8
Consider the space \(E=\Lambda^{q}(t^{\alpha}w(t))\), \(0< q\leq\infty\), where w is slowly varying and \(s/n>\alpha>0\). Then \(\beta_{E}=\alpha _{E}=\alpha\) and \(\rho_{E}\in N_{d}\). Hence by Theorem 4.7,
which implies that \(H(E)=L^{q}_{\ast}(t^{-s/n}w)\).
Moreover, the couple \(\rho_{E}\), \(\rho_{H}(E)\) is optimal. In particular, the couple
is optimal.
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This research is supported by Gyeongsang National University. The authors thank the referees for their valuable remarks that improve the paper.
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Kang, S.M., Nazeer, W. & Mehmood, Q. Continuity of Riesz potential operator in the supercritical case on unbounded domain. J Inequal Appl 2015, 398 (2015). https://doi.org/10.1186/s13660-015-0922-y
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DOI: https://doi.org/10.1186/s13660-015-0922-y