American Journal of Mathematics and Statistics

p-ISSN: 2162-948X    e-ISSN: 2162-8475

2013;  3(6): 445-453

doi:10.5923/j.ajms.20130306.20

Some Embedding Theorems and Properties of Riesz Potentials

Rahim M. Rzaev1, Fuad N. Aliyev2

1Institute of Mathematics and Mechanics of National Academy of Sciences of Azerbaijan; Baku; AZ1141, Azerbaijan

2Azerbaijan State Pedagogical University; Baku; AZ1000, Azerbaijan

Correspondence to: Rahim M. Rzaev, Institute of Mathematics and Mechanics of National Academy of Sciences of Azerbaijan; Baku; AZ1141, Azerbaijan.

Email:

Copyright © 2012 Scientific & Academic Publishing. All Rights Reserved.

Abstract

It is well known that potential type integrals play an important role in research of the partial differential equations. The present paper studies properties of Riesz potential in terms of local oscillation of functions.

Keywords: local oscillation, bounded mean oscillation, Morrey spaces, Riesz potential

Cite this paper: Rahim M. Rzaev, Fuad N. Aliyev, Some Embedding Theorems and Properties of Riesz Potentials, American Journal of Mathematics and Statistics, Vol. 3 No. 6, 2013, pp. 445-453. doi: 10.5923/j.ajms.20130306.20.

1. Introduction

Let be -dimensional Euclidean space of the points , and be a closed ball in of radius with the center at point . Denote by , , a class of all local -power summable functions defined on and by the class of all local bounded functions defined on . By we mean the usual Lebesgue space on , and we denote by the corresponding norm, that is
if , and .
Denote by the totality of all polynomials on whose degrees are equal to or less than .
Let, , , ( is the set of all positive integers). Define the following
functions
Let , , be non-negative integers, . Apply the orthogonalization process by the scalar product
to the system of the power functions , , arranged by partially lexicographic order1 [1], where is the Lebesque measure of the set . Denote by the obtained orthogonal normed system.
Let . Suppose that ([2],[3]):
.
It is obvious that is a polynomial degree of which is equal or less than .
Denote
for . Let us call local oscillation of -th order of the function on the ball in the metric of .
Note that if then
,and therefore
.
It is known that (cf.[4]) for each polynomial and each ball the inequality
is true, where the positive constant does not depend on and . Hence it follows that
.
It should be mentioned that the theory of spaces defined by local oscillation has been developed by several authors, for instance F.John and L.Nirenberg[5], S.Campanato[6], N.G.Meyers[7], S.Spanne[8], J. Peetre[9], D.Sarason[10] etc. (see also[11],[12]).
Let , . We introduce the following denotations
, , , .
Let be a class of all positive monotonically increasing on functions. Let , . By we denote the set of all the functions , for which
, .
We introduce the norm in the space by the equality
.
If and , , , then , where is the Morrey space, i.e.
.
Let is a positive number. We denote by a set of all such that almost decreases on .
If , , then we denote by the set of all functions such that , where
.
If we consider the class as a subset in the quotient space , then is the norm on . In the introduced norm the space is a Banach space.
If , , then we will denote by the class of all the functions for which the following relation
is valid.
We define the norm on by the equality
.
In particular, if then , where is the space of all local summable functions of bounded mean oscillation. The class for the first time was introduced in[5].
It is easy to see that if , , , then and their norms are equivalent.
Consider also a class which was introduced in[10]: is the class of all for which the relation
is valid. For we define .
Let . By we mean the weak Lebesgue space on , and we denote
.
Potential type integrals play an important role in the mathematical analysis. For the properties of Riesz potentials in terms of mean oscillations we refer the readers to[9],[4],[16] and the related papers for further information.
In this paper we study the properties of Riesz potential of a function in terms of local oscillation of functions when belongs to , or general Morrey type spaces.
The structure of the paper is as follows. In section 2 some inequalities and embedding theorems is proved. The mean results of the paper are given in Theorems 5, 6 and 7, which was proved in section 3.

2. Some Inequalities and Embedding Theorems

Proposition 1. Let , . Then the inequality
is true, where the constant depends only on , and .
Proof. Let . Applying the Hölder’s Inequality we obtain
.
Therefore
, .
The case is obvious.
Corollary 1. If , , , then the inequality
, , is true.
Proposition 2. Let . Then there exists a function such that
(1)
where the constant is independent of and .
Proof. Let and , . Then we have
,
, and similarly
, , where is the unit sphere, is a surface area of . From here we obtain the inequality (1).
Proposition 3. Let , . Then and there exists a constant independent of , such that
(2)
for all and .
Proof. It follows from well known equality (see[17], Chapter 1, Lemma 4.1) that (for any positive constant )
.
Now choosing we obtain
From here we obtain the inequality (1) with .
Remark 1. In the case the inequality (2), in general, is not true. For instance, the function belong to , but .
Proposition 4. Let , , . Then and there exists a constant , depends only on , , , such that
(3)
for all .
Proof. We have
.
Therefore
.
This means that and .
Further we obtain
, ,
where is the unit sphere, is a surface area of . From here
, .
The previous proposition shows that it is impossible to improve the estimation (2).
Proposition 5. Let , . Then the inequality
(4)
is true, where a constant is independent of , .
Proof. At first we consider the case . Then we have
,
where . Further, applying the Minkowski’s Inequality we have
,
where is the volume of the unit ball .
In the case the proof of inequality (4) is obvious.
The following proposition shows that it is impossible to improve the estimation (4) in the case .
Proposition 6. Let . Then there exists the function such that for the inequality
(5)
is true, where a constant is independent of and .
Proof. Let
.
If , , , then we obtain
.
If , , then . Besides, for all ,
.
Thus the function is integrable on the with respect to argument . Further we obtain that if , then
.
It is obvious that
Therefore we obtain that
, .
In the case the arguments are similar.
With help of Proposition 3, Proposition 5 and Corollary 1 we obtain correspondingly, the following theorems.
Theorem 1. Let . Then and
, where , .
Theorem 2. Let , . Then and
Theorem 3. Let , and . Then and
: , where , .

3. Properties of Riesz Potentials

Consider the following potential type integral operator
where
are non-negative integers,
,
,
is the characteristic function of the set .
Operator is a certain modification of the Riesz potential
.
It should be noted that if and , then the integral differs from integral by a polynomial power of which is equal or less than . If , then the potential is defined not for all functions .
Moreover, if and , for example, then for integral absolutely converges almost everywhere.
Note that modified Riesz potential similar to the was considered, for example, in T.Kurokawa[13], T.Shimomura and Y. Mizuta[14] etc. (see also[15]).
The following assertion holds true.
Theorem 4[16]. Let , , , and
.
Then the inequality
(6)
is valid, where , and constant does not depend on , and .
Corollary 2. Let , , , and
.
Then inequality
(7)
is valid, where , and constant does not depend on and .
Theorem 5. Let , . If , then and
where , .
Proof. With help of Proposition 3 and Theorem 4 we have
where . From here the theorem statement easily turns out.
Corollary 3. Let , , , , . Then
Corollary 4. Let , , . Then and
Corollary 5. If , ,
, then , where , and
.
Theorem 6. Let , , , , . Then and
where , . In the case , in addition , , where .
Proof. Taking into account the inequalities (4) and (7), it is easy to obtain the inequality
(8)
where a constant is independent of , . From here we obtain that
If , , then . Therefore if , and , then from estimation (7), in addition, we have .
Corollary 6. Let , , , . Then and
,
where , . In the case , in addition, we have .
Corollary 7. Let . Then and
.
Corollary 8. Let , , If , then and
,
where . If , then in addition, .
Theorem 7. Let , , , and
.
If , then and
, where , .
Let , . Then and . From Theorem 7 we obtain that if , , , , then , i.e. the operator boundedly acts from into .
Corollary 9. If , then .
Corollary 10. If , then .
Corollary 11. If , , , then , where .

Notes

1. It means that precedes if either , or but the first nonzero difference is negative.

References

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