Boundary Value Problems
Volume 2009 (2009), Article ID 835865, 18 pages
doi:10.1155/2009/835865
Research Article

A Note on Generalized Fractional Integral Operators on Generalized Morrey Spaces

1Department of Mathematics, Kyoto University, Kitasir-akawa, Sakyoku, Kyoto 606-8502, Japan
2Kobe City College of Technology, 8-3 Gakuen-higashimachi, Nishi-ku, Kobe 651-2194, Japan
3Graduate School of Mathematical Sciences, The University of Tokyo, 3-8-1 Komaba, Meguro-ku, Tokyo 153-8914, Japan

Received 21 July 2009; Revised 31 August 2009; Accepted 13 December 2009

Academic Editor: Peter Bates

Copyright © 2009 Yoshihiro Sawano et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

We show some inequalities for generalized fractional integral operators on generalized Morrey spaces. We also show the boundedness property of the generalized fractional integral operators on the predual of the generalized Morrey spaces.

1. Introduction

The present paper is an offspring of [1]. We obtain some inequalities for generalized fractional integral operators on generalized Morrey spaces. We also show the boundedness property of the generalized fractional integral operators on the predual of the generalized Morrey spaces. They generalize what was shown in [1]. We will go through the same argument as [1].

For 0 < 𝛼 < 1 the classical fractional integral operator 𝐼 𝛼 and the classical fractional maximal operator 𝑀 𝛼 are given by 𝐼 𝛼 𝑓 ( 𝑥 ) = 𝑛 𝑓 ( 𝑦 ) | | | | 𝑥 𝑦 𝑛 ( 1 𝛼 ) 𝑀 𝑑 𝑦 , 𝛼 𝑓 ( 𝑥 ) = s u p 𝑥 𝑄 𝒬 1 | | 𝑄 | | 1 𝛼 𝑄 | | | | 𝑓 ( 𝑦 ) 𝑑 𝑦 . ( 1 . 1 )

In the present paper, we generalize the parameter 𝛼 . Let 𝜌 [ 0 , ) [ 0 , ) be a suitable function. We define the generalized fractional integral operator 𝑇 𝜌 and the generalized fractional maximal operator 𝑀 𝜌 by 𝑇 𝜌 𝑓 ( 𝑥 ) = 𝑛 𝜌 | | | | 𝑓 ( 𝑦 ) 𝑥 𝑦 | | | | 𝑥 𝑦 𝑛 𝑀 𝑑 𝑦 , 𝜌 𝑓 ( 𝑥 ) = s u p 𝑥 𝑄 𝒬 𝜌 ( ( 𝑄 ) ) | | 𝑄 | | 𝑄 | | | | 𝑓 ( 𝑦 ) 𝑑 𝑦 . ( 1 . 2 )

Here, we use the notation 𝒬 to denote the family of all cubes in 𝑛 with sides parallel to the coordinate axes, ( 𝑄 ) , to denote the sidelength of 𝑄 and | 𝑄 | to denote the volume of 𝑄 . If 𝜌 ( 𝑡 ) 𝑡 𝑛 𝛼 , 0 < 𝛼 < 1 , then we have 𝑇 𝜌 = 𝐼 𝛼 and 𝑀 𝜌 = 𝑀 𝛼 .

A well-known fact in partial differential equations is that 𝐼 𝛼 is an inverse of ( Δ ) 𝑛 𝛼 / 2 . The operator ( 1 Δ ) 1 admits an expression of the form 𝑇 𝜌 for some 𝜌 . For more details of this operator we refer to [2]. As we will see, these operators will fall under the scope of our main results.

Among other function spaces, it seems that the Morrey spaces reflect the boundedness properties of the fractional integral operators. To describe the Morrey spaces we recall some definitions and notation. All cubes are assumed to have their sides parallel to the coordinate axes. For 𝑄 𝒬 we use 𝑐 𝑄 to denote the cube with the same center as 𝑄 , but with sidelength of 𝑐 ( 𝑄 ) . | 𝐸 | denotes the Lebesgue measure of 𝐸 𝑛 .

Let 0 < 𝑝 < and 𝜙 [ 0 , ) [ 0 , ) be a suitable function. For a function 𝑓 locally in 𝐿 𝑝 ( 𝑛 ) we set 𝑓 𝑝 , 𝜙 = s u p 𝑄 𝒬 1 𝜙 ( ( 𝑄 ) ) | | 𝑄 | | 𝑄 | | | | 𝑓 ( 𝑥 ) 𝑝 𝑑 𝑥 1 / 𝑝 . ( 1 . 3 ) We will call the Morrey space 𝑝 , 𝜙 ( 𝑛 ) = 𝑝 , 𝜙 the subset of all functions 𝑓 locally in 𝐿 𝑝 ( 𝑛 ) for which 𝑓 𝑝 , 𝜙 = 𝑓 𝑝 , 𝜙 is finite. Applying Hölder's inequality to (1.3), we see that 𝑓 𝑝 1 , 𝜙 𝑓 𝑝 2 , 𝜙 provided that 𝑝 1 𝑝 2 > 0 . This tells us that 𝑝 1 , 𝜙 𝑝 2 , 𝜙 when 𝑝 1 𝑝 2 > 0 . We remark that without the loss of generality we may assume 𝜙 ( 𝑡 ) i s n o n d e c r e a s i n g b u t 𝜙 ( 𝑡 ) 𝑝 𝑡 𝑛 i s n o n i n c r e a s i n g . ( 1 . 4 ) (See [1].) Hereafter, we always postulate (1.4) on 𝜙 .

If 𝜙 ( 𝑡 ) 𝑡 𝑛 / 𝑝 0 , 𝑝 0 𝑝 , 𝑝 , 𝜙 coincides with the usual Morrey space and we write this for 𝑝 , 𝑝 0 and the norm for 0 𝑝 , 𝑝 . Then we have the inclusion 𝐿 𝑝 0 = 𝑝 0 , 𝑝 0 𝑝 1 , 𝑝 0 𝑝 2 , 𝑝 0 ( 1 . 5 ) when 𝑝 0 𝑝 1 𝑝 2 > 0 .

In the present paper, we take up some relations between the generalized fractional integral operator 𝑇 𝜌 and the generalized fractional maximal operator 𝑀 𝜌 in the framework of the Morrey spaces 𝑝 , 𝜙 (Theorem 1.2). In the last section, we prove a dual version of Olsen's inequality on predual of Morrey spaces (Theorem 3.1). As a corollary (Corollary 3.2), we have the boundedness properties of the operator 𝑇 𝜌 on predual of Morrey spaces.

Let 𝜃 [ 0 , ) [ 0 , ) be a function. By the Dini condition we mean that 𝜃 fulfills 1 0 𝜃 ( 𝑠 ) 𝑠 𝑑 𝑠 < , ( 1 . 6 ) while the doubling condition on 𝜃 (with a doubling constant 𝐶 1 > 0 ) is that 𝜃 satisfies 1 𝐶 1 𝜃 ( 𝑠 ) 𝜃 ( 𝑡 ) 𝐶 1 1 , i f 2 𝑠 𝑡 2 . ( 1 . 7 ) We notice that (1.4) is stronger than the doubling condition. More quantitatively, if we assume (1.4), then 𝜙 satisfies the doubling condition with the doubling constant 2 𝑛 / 𝑝 . A simple consequence that can be deduced from the doubling condition of 𝜃 is that l o g 2 𝐶 1 𝜃 ( 𝑡 ) 𝑡 𝑡 / 2 𝜃 ( 𝑠 ) 𝑠 𝑑 𝑠 l o g 2 𝐶 1 𝜃 ( 𝑡 ) 𝑡 > 0 . ( 1 . 8 ) The key observation made in [1] is that it is frequently convenient to replace 𝜃 satisfying (1.6) and (1.7) by ̃ 𝜃 : ̃ 𝜃 ( 𝑡 ) = 𝑡 0 𝜃 ( 𝑠 ) 𝑠 𝑑 𝑠 . ( 1 . 9 )

Before we formulate our main results, we recall a typical result obtained in [1].

Proposition 1.1 (see [1, Theorem  1.3]). Let 1 𝑝 < , 𝑝 𝑞 i f 𝑝 = 1 , 𝑝 < 𝑞 i f 𝑝 > 1 , ( 1 . 1 0 ) 0 𝑏 1 and 𝑏 < 𝑎 . Suppose that ̃ 𝜌 ( 𝑡 ) m a x ( 𝑎 𝑝 , 𝑏 𝑞 ) 𝑡 𝑛 is nonincreasing. Then 𝑔 𝑇 𝜌 𝑓 𝑝 , ̃ 𝜌 𝑎 𝐶 𝑔 𝑞 , ̃ 𝜌 𝑏 𝑀 ̃ 𝜌 1 𝑏 𝑓 𝑝 , ̃ 𝜌 𝑎 , ( 1 . 1 1 ) where the constant 𝐶 is independent of 𝑓 and 𝑔 .

The aim of the present paper is to generalize the function spaces to which 𝑓 and 𝑔 belong. With theorem 1.2, which we will present just below, we can replace ̃ 𝜌 𝑎 with 𝜙 and ̃ 𝜌 𝑏 with 𝜂 . We now formulate our main theorems. In the sequel we always assume that 𝜌 satisfies (1.6) and (1.7), and 𝐶 is used to denote various positive constants.

Theorem 1.2. Let 1 𝑝 < , 𝑝 𝑞 i f 𝑝 = 1 , 𝑝 < 𝑞 i f 𝑝 > 1 . ( 1 . 1 2 ) Suppose that 𝜙 ( 𝑡 ) and 𝜂 ( 𝑡 ) are nondecreasing but that 𝜙 ( 𝑡 ) 𝑝 𝑡 𝑛 and 𝜂 ( 𝑡 ) 𝑞 𝑡 𝑛 are nonincreasing. Assume also that 𝑡 𝜌 ( 𝑠 ) 𝜂 ( 𝑠 ) 𝑠 ̃ 𝜌 ( 𝑠 ) 𝜙 ( 𝑠 ) 𝑑 𝑠 𝐶 𝜂 ( 𝑡 ) 𝜙 ( 𝑡 ) 𝑡 > 0 , ( 1 . 1 3 ) then 𝑔 𝑇 𝜌 𝑓 𝑝 , 𝜙 𝐶 𝑔 𝑞 , 𝜂 𝑀 ̃ 𝜌 / 𝜂 𝑓 𝑝 , 𝜙 , ( 1 . 1 4 ) where the constant 𝐶 is independent of 𝑓 and 𝑔 .

Remark 1.3. Let 0 𝑏 1 and 𝑏 < 𝑎 . Then 𝜙 = ̃ 𝜌 𝑎 and 𝜂 = ̃ 𝜌 𝑏 satisfy the assumption (1.13). Indeed, 𝑡 𝜌 ( 𝑠 ) ̃ 𝜌 ( 𝑠 ) 𝑏 𝑠 ̃ 𝜌 ( 𝑠 ) ̃ 𝜌 ( 𝑠 ) 𝑎 𝑑 𝑠 = 𝑡 ̃ 𝜌 ( 𝑠 ) 𝑏 𝑎 1 𝜌 ( 𝑠 ) 𝑠 = 𝑑 𝑠 𝑡 𝑑 1 𝑑 𝑠 𝑏 𝑎 ̃ 𝜌 ( 𝑠 ) 𝑏 𝑎 1 𝑑 𝑠 𝑎 𝑏 ̃ 𝜌 ( 𝑡 ) 𝑏 𝑎 . ( 1 . 1 5 ) Hence, Theorem 1.2 generalizes Proposition 1.1.

Letting 𝜂 ( 𝑡 ) 1 and 𝑔 ( 𝑥 ) 1 in Theorem 1.2, we obtain the result of how 𝑀 ̃ 𝜌 controls 𝑇 𝜌 .

Corollary 1.4. Let 1 𝑝 < . Suppose that 𝑡 𝜌 ( 𝑠 ) 𝐶 𝑠 ̃ 𝜌 ( 𝑠 ) 𝜙 ( 𝑠 ) 𝑑 𝑠 𝜙 ( 𝑡 ) 𝑡 > 0 , ( 1 . 1 6 ) then 𝑇 𝜌 𝑓 𝑝 , 𝜙 𝑀 𝑓 𝐶 ̃ 𝜌 𝑝 , 𝜙 . ( 1 . 1 7 )

Corollary 1.4 generalizes [3, Theorem  4.2]. Letting 𝜂 = ̃ 𝜌 in Theorem 1.2, we also obtain the condition on 𝑔 and 𝜌 under which the mapping 𝑓 𝑝 , 𝜙 𝑔 𝑇 𝜌 𝑓 𝑝 , 𝜙 ( 1 . 1 8 ) is bounded.

Corollary 1.5. Let 1 𝑝 < , 𝑝 𝑞 i f 𝑝 = 1 , 𝑝 < 𝑞 i f 𝑝 > 1 . ( 1 . 1 9 ) Suppose that 𝑡 𝜌 ( 𝑠 ) 𝑠 𝜙 ( 𝑠 ) 𝑑 𝑠 𝐶 ̃ 𝜌 ( 𝑡 ) 𝜙 ( 𝑡 ) 𝑡 > 0 , ( 1 . 2 0 ) then 𝑔 𝑇 𝜌 𝑓 𝑝 , 𝜙 𝐶 𝑔 𝑞 , ̃ 𝜌 𝑀 𝑓 𝑝 , 𝜙 . ( 1 . 2 1 ) In particular, if 1 < 𝑝 < 𝑞 < , then 𝑔 𝑇 𝜌 𝑓 𝑝 , 𝜙 𝐶 𝑔 𝑞 , ̃ 𝜌 𝑓 𝑝 , 𝜙 . ( 1 . 2 2 )

Here, 𝑀 denotes the Hardy-Littlewood maximal operator defined by 𝑀 𝑓 ( 𝑥 ) = s u p 𝑥 𝑄 𝒬 1 | | 𝑄 | | 𝑄 | | | | 𝑓 ( 𝑦 ) 𝑑 𝑦 . ( 1 . 2 3 )

We will establish that 𝑀 is bounded on 𝑝 , 𝜙 when 𝑝 > 1 (Lemma 2.2). Therefore, the second assertion is immediate from the first one.

Theorem 1.6. Let 1 < 𝑝 𝑟 < 𝑞 < . Suppose that 𝜙 ( 𝑡 ) and 𝜂 ( 𝑡 ) are nondecreasing but that 𝜙 ( 𝑡 ) 𝑝 𝑡 𝑛 and 𝜂 ( 𝑡 ) 𝑞 𝑡 𝑛 are nonincreasing. Suppose also that ̃ 𝜌 ( 𝑡 ) + 𝜙 ( 𝑡 ) 𝑡 𝜌 ( 𝑠 ) 𝑠 𝜙 ( 𝑠 ) 𝑑 𝑠 𝐶 𝜂 ( 𝑡 ) 𝜙 ( 𝑡 ) 𝑝 / 𝑟 𝑡 > 0 , ( 1 . 2 4 ) then 𝑔 𝑇 𝜌 𝑓 𝑟 , 𝜙 𝑝 / 𝑟 𝐶 𝑔 𝑞 , 𝜂 𝑓 𝑝 , 𝜙 , ( 1 . 2 5 ) where the constant 𝐶 is independent of 𝑓 and 𝑔 .

Theorem 1.6 extends [4, Theorem  2], [1, Theorem  1.1], and [5, Theorem  1]. As the special case 𝜂 ( 𝑡 ) 1 and 𝑔 ( 𝑥 ) 1 in Theorem 1.6 shows, this theorem covers [1, Remark  2.8].

Corollary 1.7 (see [1, Remark  2.8], see also [68]). Let 1 < 𝑝 𝑟 < . Suppose that ̃ 𝜌 ( 𝑡 ) + 𝜙 ( 𝑡 ) 𝑡 𝜌 ( 𝑠 ) 𝐶 𝑠 𝜙 ( 𝑠 ) 𝑑 𝑠 𝜙 ( 𝑡 ) 𝑝 / 𝑟 𝑡 > 0 , ( 1 . 2 6 ) then 𝑇 𝜌 𝑓 𝑟 , 𝜙 𝑝 / 𝑟 𝐶 𝑓 𝑝 , 𝜙 . ( 1 . 2 7 )

Nakai generalized Corollary 1.7 to the Orlicz-Morrey spaces ([9, Theorem  2.2] and [10, Theorem  7.1]).

We dare restate Theorem 1.6 in the special case when 𝑇 𝜌 is the fractional integral operator 𝐼 𝛼 . The result holds by letting 𝜌 ( 𝑡 ) 𝑡 𝑛 𝛼 , 𝜙 ( 𝑡 ) 𝑡 𝑛 / 𝑝 0 , and 𝜂 ( 𝑡 ) 𝑡 𝑛 / 𝑞 0 .

Proposition 1.8 (see [1, Proposition  1.7]). Let 0 < 𝛼 < 1 , 1 < 𝑝 𝑝 0 < , 1 < 𝑞 𝑞 0 < , and 1 < 𝑟 𝑟 0 < . Suppose that 𝑞 > 𝑟 , 1 / 𝑝 0 > 𝛼 , 1 / 𝑞 0 𝛼 , 1 / 𝑟 0 = 1 / 𝑞 0 + 1 / 𝑝 0 𝛼 , and 𝑟 / 𝑟 0 = 𝑝 / 𝑝 0 then 𝑔 𝐼 𝛼 𝑓 0 𝑟 , 𝑟 𝐶 𝑔 0 𝑞 , 𝑞 𝑓 0 𝑝 , 𝑝 , ( 1 . 2 8 ) where the constant 𝐶 is independent of 𝑓 and 𝑔 .

Proposition 1.8 extends [4, Theorem  2] (see [1, Remark  1.9]).

Remark 1.9. The special case 𝑞 0 = and 𝑔 ( 𝑥 ) 1 in Proposition 1.8 corresponds to the classical theorem due to Adams (see [11]).
The fractional integral operator 𝐼 𝛼 , 0 < 𝛼 < 1 , is bounded from 𝑝 , 𝑝 0 to 𝑟 , 𝑟 0 if and only if the parameters 1 < 𝑝 𝑝 0 < and 1 < 𝑟 𝑟 0 < satisfy 1 / 𝑟 0 = 1 / 𝑝 0 𝛼 and 𝑟 / 𝑟 0 = 𝑝 / 𝑝 0 .
Using naively the Adams theorem and Hölder's inequality, one can prove a minor part of 𝑞 in Proposition 1.8. That is, the proof of Proposition 1.8 is fundamental provided ( 𝑝 / 𝑝 0 ) 𝑞 0 𝑞 𝑞 0 . Indeed, by virtue of the Adams theorem we have, for any cube 𝑄 𝒬 , | | 𝑄 | | 1 / 𝑠 0 1 | | 𝑄 | | 𝑄 | | 𝐼 𝛼 | | 𝑓 ( 𝑥 ) 𝑠 𝑑 𝑥 1 / 𝑠 𝐶 𝑓 0 𝑝 , 𝑝 , 1 𝑠 = 𝑝 0 𝑝 1 𝑠 0 , 1 𝑠 0 = 1 𝑝 0 𝛼 . ( 1 . 2 9 ) The condition 𝑟 / 𝑟 0 = 𝑝 / 𝑝 0 , 1 / 𝑟 0 = 1 / 𝑞 0 + 1 / 𝑝 0 𝛼 reads 1 𝑟 = 𝑝 0 𝑝 1 𝑞 0 + 1 𝑝 0 = 𝑝 𝛼 0 𝑝 1 𝑞 0 + 1 𝑠 . ( 1 . 3 0 ) These yield | | 𝑄 | | 1 / 𝑞 0 + 1 / 𝑠 0 1 | | 𝑄 | | 𝑄 | | 𝑔 ( 𝑥 ) 𝐼 𝛼 | | 𝑓 ( 𝑥 ) 𝑟 𝑑 𝑥 1 / 𝑟 𝐶 𝑔 0 𝑞 , 𝑞 𝑓 0 𝑝 , 𝑝 ( 1 . 3 1 ) if 𝑟 / 𝑟 0 = 𝑝 / 𝑝 0 = 𝑞 / 𝑞 0 . In view of inclusion (1.5), the same can be said when ( 𝑝 / 𝑝 0 ) 𝑞 0 𝑞 𝑞 0 . Also observe that 1 / 𝑟 0 = 1 / 𝑞 0 + 1 / 𝑝 0 𝛼 > 1 / 𝑞 0 . Hence we have 𝑞 0 > 𝑟 0 . Thus, since the condition 𝑞 > 𝑟 , Proposition 1.8 is significant only when ( 𝑝 / 𝑝 0 ) 𝑟 0 < 𝑞 < ( 𝑝 / 𝑝 0 ) 𝑞 0 . The case 𝑝 / 𝑝 0 = 𝑟 / 𝑟 0 = 1 (the case of the Lebesgue spaces) corresponds (so-called) to the Fefferan-Phong inequality (see [12]). An inequality of the form 𝑛 | | | | 𝑢 ( 𝑥 ) 2 𝑣 ( 𝑥 ) 𝑑 𝑥 𝐶 𝑣 𝑛 | | | | 𝑢 ( 𝑥 ) 2 𝑑 𝑥 , 0 𝑢 𝐶 0 ( 𝑛 ) , 𝑣 0 ( 1 . 3 2 ) is called the trace inequality and is useful in the analysis of the Schrödinger operators. For example, Kerman and Sawyer utilized an inequality of type (1.32) to obtain an eigenvalue estimates of the operators (see [13]). By letting 𝛼 = 1 / 𝑛 , we obtain a sharp estimate on the constant 𝐶 𝑣 in (1.32).

In [14], we characterized the range of 𝐼 𝛼 , which motivates us to consider Proposition 1.8.

Proposition 1.10 (see [14]). Let 1 < 𝑝 𝑝 0 < , 1 < 𝑠 𝑠 0 < , and 0 < 𝛼 < 1 . Assume that 𝑝 𝑝 0 = 𝑠 𝑠 0 , 1 𝑠 0 = 1 𝑝 0 𝛼 . ( 1 . 3 3 ) (1) 𝐼 𝛼 𝑝 , 𝑝 0 𝑠 , 𝑠 0 is continuous but not surjective. (2)Let 𝜑 𝒮 be an auxiliary function chosen so that 𝜑 ( 𝑥 ) = 1 , 2 | 𝑥 | 4 and that 𝜑 ( 𝑥 ) = 0 , | 𝑥 | 1 , | 𝑥 | 8 . Then the norm equivalence 𝑓 0 𝑝 , 𝑝 𝑗 = 2 2 𝑗 ( 𝑛 𝛼 ) | | 𝜑 ( 2 𝑗 ) 𝐼 𝛼 𝑓 | | 2 1 / 2 0 𝑝 , 𝑝 ( 1 . 3 4 ) holds for 𝑓 𝑝 , 𝑝 0 , where denotes the Fourier transform.

In view of this proposition 𝑠 , 𝑠 0 is not a good space to describe the boundedness of 𝐼 𝛼 , although we have (1.29). As we have seen by using Hölder's inequality in Remark 1.9, if we use the space 𝑠 , 𝑠 0 , then we will obtain a result weaker than Proposition 1.8.

Finally it would be interesting to compare Theorem 1.2 with the following Theorem 1.11.

Theorem 1.11. Let 0 < 𝑝 < . Suppose that 𝜌 , 𝜂 , and 𝜙 are nondecreasing and that 𝜂 ( 𝑡 ) 𝑝 𝑡 𝑛 and 𝜙 ( 𝑡 ) 𝑝 𝑡 𝑛 are nonincreasing. Then 𝑔 𝑀 𝜌 𝑓 𝑝 , 𝜙 𝐶 𝑔 𝑝 , 𝜂 𝑀 𝜌 / 𝜂 𝑓 𝑝 , 𝜙 , ( 1 . 3 5 ) where the constant 𝐶 is independent of 𝑓 and 𝑔 .

Theorem 1.11 generalizes [1, Theorem  1.7] and the proof remains unchanged except some minor modifications caused by our generalization of the function spaces to which 𝑓 and 𝑔 belong. So, we omit the proof in the present paper.

2. Proof of Theorems

For any 1 < 𝑝 < we will write 𝑝 for the conjugate number defined by 1 / 𝑝 + 1 / 𝑝 = 1 . Hereafter, for the sake of simplicity, for any 𝑄 𝒬 and 0 < 𝑝 < we will write 𝑚 𝑄 ( 1 𝑓 ) = | | 𝑄 | | 𝑄 𝑓 ( 𝑥 ) 𝑑 𝑥 , 𝑚 𝑄 ( 𝑝 ) ( 𝑓 ) = 𝑚 𝑄 | | 𝑓 | | 𝑝 1 / 𝑝 . ( 2 . 1 )

2.1. Proof of Theorem 1.2

First, we will prove Theorem 1.2. Except for some sufficient modifications, the proof of the theorem follows the argument in [15]. We denote by 𝒟 the family of all dyadic cubes in 𝑛 . We assume that 𝑓 and 𝑔 are nonnegative, which may be done without any loss of generality thanks to the positivity of the integral kernel. We will denote by 𝐵 ( 𝑥 , 𝑟 ) the ball centered at 𝑥 and of radius 𝑟 . We begin by discretizing the operator 𝑇 𝜌 𝑓 following the idea of Pérez (see [16]): 𝑇 𝜌 𝑓 ( 𝑥 ) = 𝜈 2 𝜈 1 < | 𝑥 𝑦 | 2 𝜈 𝜌 | | | | 𝑓 ( 𝑦 ) 𝑥 𝑦 | | | | 𝑥 𝑦 𝑛 𝑑 𝑦 𝐶 𝜈 𝜌 2 𝜈 2 𝑛 𝜈 𝐵 ( 𝑥 , 2 𝜈 ) 𝑓 ( 𝑦 ) 𝑑 𝑦 𝐶 𝜈 𝑄 𝒟 𝑄 𝑥 , ( 𝑄 ) = 2 𝜈 𝜌 ( ( 𝑄 ) ) | | 𝑄 | | 3 𝑄 𝑓 ( 𝑦 ) 𝑑 𝑦 = 𝐶 𝑄 𝒟 𝜌 ( ( 𝑄 ) ) | | 𝑄 | | 3 𝑄 𝑓 ( 𝑦 ) 𝑑 𝑦 𝜒 𝑄 ( 𝑥 ) = 𝐶 𝑄 𝒟 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝜒 𝑄 ( 𝑥 ) , ( 2 . 2 ) where we have used the doubling condition of 𝜌 for the first inequality. To prove Theorem 1.2, thanks to the doubling condition of 𝜙 , which holds by use of the facts that 𝜙 ( 𝑡 ) is nondecreasing and that 𝜙 ( 𝑡 ) 𝑝 𝑡 𝑛 is nonincreasing, it suffices to show 𝑄 0 𝑔 ( 𝑥 ) 𝑇 𝜌 𝑓 ( 𝑥 ) 𝑝 𝑑 𝑥 1 / 𝑝 𝐶 𝑔 𝑞 , 𝜂 𝑀 ̃ 𝜌 / 𝜂 𝑓 𝑝 , 𝜙 | | 𝑄 0 | | 1 / 𝑝 𝜙 𝑄 0 1 , ( 2 . 3 ) for all dyadic cubes 𝑄 0 . Hereafter, we let 𝒟 1 𝑄 0 = 𝑄 𝒟 𝑄 𝑄 0 , 𝒟 2 𝑄 0 = 𝑄 𝒟 𝑄 𝑄 0 . ( 2 . 4 )

Let us define for 𝑖 = 1 , 2 𝐹 𝑖 ( 𝑥 ) = 𝑄 𝒟 𝑖 𝑄 0 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝜒 𝑄 ( 𝑥 ) ( 2 . 5 ) and we will estimate 𝑄 0 𝑔 ( 𝑥 ) 𝐹 𝑖 ( 𝑥 ) 𝑝 𝑑 𝑥 1 / 𝑝 . ( 2 . 6 ) The case 𝑖 = 1 and 𝑝 = 1 We need the following crucial lemma, the proof of which is straightforward and is omitted (see [15, 16]).

Lemma 2.1. For a nonnegative function in 𝐿 ( 𝑄 0 ) one lets 𝛾 0 = 𝑚 𝑄 0 ( ) and 𝑐 = 2 𝑛 + 1 . For 𝑘 = 1 , 2 , let 𝐷 𝑘 = 𝑄 𝒟 1 ( 𝑄 0 ) 𝑚 𝑄 ( ) > 𝛾 0 𝑐 𝑘 𝑄 . ( 2 . 7 ) Considering the maximal cubes with respect to inclusion, one can write 𝐷 𝑘 = 𝑗 𝑄 𝑘 , 𝑗 , ( 2 . 8 ) where the cubes { 𝑄 𝑘 , 𝑗 } 𝒟 1 ( 𝑄 0 ) are nonoverlapping. By virtue of the maximality of 𝑄 𝑘 , 𝑗 one has that 𝛾 0 𝑐 𝑘 < 𝑚 𝑄 𝑘 , 𝑗 ( ) 2 𝑛 𝛾 0 𝑐 𝑘 . ( 2 . 9 ) Let 𝐸 0 = 𝑄 0 𝐷 1 , 𝐸 𝑘 , 𝑗 = 𝑄 𝑘 , 𝑗 𝐷 𝑘 + 1 . ( 2 . 1 0 ) Then { 𝐸 0 } { 𝐸 𝑘 , 𝑗 } is a disjoint family of sets which decomposes 𝑄 0 and satisfies | | 𝑄 0 | | | | 𝐸 2 0 | | , | | 𝑄 𝑘 , 𝑗 | | | | 𝐸 2 𝑘 , 𝑗 | | . ( 2 . 1 1 ) Also, one sets 𝒟 0 = 𝑄 𝒟 1 𝑄 0 𝑚 𝑄 ( ) 𝛾 0 𝑐 , 𝒟 𝑘 , 𝑗 = 𝑄 𝒟 1 𝑄 0 𝑄 𝑄 𝑘 , 𝑗 , 𝛾 0 𝑐 𝑘 < 𝑚 𝑄 ( ) 𝛾 0 𝑐 𝑘 + 1 . ( 2 . 1 2 ) Then 𝒟 1 𝑄 0 = 𝒟 0 𝑘 , 𝑗 𝒟 𝑘 , 𝑗 . ( 2 . 1 3 )

With Lemma 2.1 in mind, let us return to the proof of Theorem 1.2. We need only to verify that 𝑄 0 𝑔 ( 𝑥 ) 𝐹 1 ( 𝑥 ) 𝑑 𝑥 𝐶 𝑔 𝑞 , 𝜂 𝑄 0 𝑀 ̃ 𝜌 / 𝜂 𝑓 ( 𝑥 ) 𝑑 𝑥 . ( 2 . 1 4 ) Inserting the definition of 𝐹 1 , we have 𝑄 0 𝑔 ( 𝑥 ) 𝐹 1 ( 𝑥 ) 𝑑 𝑥 = 𝑄 𝒟 1 𝑄 0 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝑄 𝑔 ( 𝑥 ) 𝑑 𝑥 . ( 2 . 1 5 )

Letting = 𝑔 , we will apply Lemma 2.1 to estimate this quantity. Retaining the same notation as Lemma 2.1 and noticing (2.13), we have 𝑄 0 𝑔 ( 𝑥 ) 𝐹 1 ( 𝑥 ) 𝑑 𝑥 = 𝑄 𝒟 0 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝑄 𝑔 ( 𝑥 ) 𝑑 𝑥 + 𝑘 , 𝑗 𝑄 𝒟 𝑘 , 𝑗 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝑄 𝑔 ( 𝑥 ) 𝑑 𝑥 . ( 2 . 1 6 )

We first evaluate 𝑄 𝒟 𝑘 , 𝑗 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝑄 𝑔 ( 𝑥 ) 𝑑 𝑥 . ( 2 . 1 7 ) It follows from the definition of 𝒟 𝑘 , 𝑗 that (2.17) is bounded by 𝐶 𝛾 0 𝑐 𝑘 + 1 𝑄 𝒟 𝑘 , 𝑗 𝜌 ( ( 𝑄 ) ) 3 𝑄 𝑓 ( 𝑦 ) 𝑑 𝑦 . ( 2 . 1 8 )

By virtue of the support condition and (1.8) we have 𝑄 𝒟 𝑘 , 𝑗 𝜌 ( ( 𝑄 ) ) 3 𝑄 𝑓 ( 𝑦 ) 𝑑 𝑦 = l o g 2 ( 𝑄 𝑘 , 𝑗 ) 𝜈 = 𝜌 2 𝜈 𝑄 𝒟 𝑘 , 𝑗 ( 𝑄 ) = 2 𝜈 3 𝑄 𝑓 ( 𝑦 ) 𝑑 𝑦 𝐶 3 𝑄 𝑘 , 𝑗 𝑓 ( 𝑦 ) 𝑑 𝑦 l o g 2 ( 𝑄 𝑘 , 𝑗 ) 𝜈 = 𝜌 2 𝜈 𝐶 3 𝑄 𝑘 , 𝑗 𝑓 ( 𝑦 ) 𝑑 𝑦 ( 𝑄 𝑘 , 𝑗 ) 0 𝜌 ( 𝑠 ) 𝑠 𝑄 𝑑 𝑠 = 𝐶 ̃ 𝜌 𝑘 , 𝑗 3 𝑄 𝑘 , 𝑗 𝑓 ( 𝑦 ) 𝑑 𝑦 . ( 2 . 1 9 )

If we invoke relations | 𝑄 𝑘 , 𝑗 | 2 | 𝐸 𝑘 , 𝑗 | and 𝛾 0 𝑐 𝑘 < 𝑚 𝑄 𝑘 , 𝑗 ( 𝑔 ) , then (2.17) is bounded by 𝑄 𝐶 ̃ 𝜌 𝑘 , 𝑗 𝑚 3 𝑄 𝑘 , 𝑗 ( 𝑓 ) 𝑚 𝑄 𝑘 , 𝑗 | | 𝐸 ( 𝑔 ) 𝑘 , 𝑗 | | . ( 2 . 2 0 )

Now that we have from the definition of the Morrey norm 𝑚 𝑄 𝑘 , 𝑗 ( 𝑔 ) 𝑚 𝑄 ( 𝑞 ) 𝑘 , 𝑗 ( 𝑔 ) 𝑔 𝑞 , 𝜂 𝜂 𝑄 𝑘 , 𝑗 1 , ( 2 . 2 1 )

we conclude that ( 2 . 1 7 ) 𝐶 𝑔 𝑞 , 𝜂 𝑄 ̃ 𝜌 𝑘 , 𝑗 𝜂 𝑄 𝑘 , 𝑗 𝑚 3 𝑄 𝑘 , 𝑗 | | 𝐸 ( 𝑓 ) 𝑘 , 𝑗 | | 𝐶 𝑔 𝑞 , 𝜂 𝐸 𝑘 , 𝑗 𝑀 ̃ 𝜌 / 𝜂 𝑓 ( 𝑥 ) 𝑑 𝑥 . ( 2 . 2 2 )

Here, we have used the fact that ̃ 𝜌 is nondecreasing, that 𝜂 satisfies the doubling condition and that ̃ 𝜌 3 𝑄 𝑘 , 𝑗 𝜂 3 𝑄 𝑘 , 𝑗 𝑚 3 𝑄 𝑘 , 𝑗 ( 𝑓 ) i n f 𝑦 𝑄 𝑘 , 𝑗 𝑀 ̃ 𝜌 / 𝜂 𝑓 ( 𝑦 ) . ( 2 . 2 3 )

Similarly, we have 𝑄 𝒟 0 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝑄 𝑔 ( 𝑥 ) 𝑑 𝑥 𝐶 𝑔 𝑞 , 𝜂 𝐸 0 𝑀 ̃ 𝜌 / 𝜂 𝑓 ( 𝑥 ) 𝑑 𝑥 . ( 2 . 2 4 )

Summing up all factors, we obtain (2.14), by noticing that { 𝐸 0 } { 𝐸 𝑘 , 𝑗 } is a disjoint family of sets which decomposes 𝑄 0 .

The case 𝑖 = 1 and 𝑝 > 1 In this case we establish 𝑄 0 𝑔 ( 𝑥 ) 𝐹 1 ( 𝑥 ) 𝑝 𝑑 𝑥 1 / 𝑝 𝐶 𝑔 𝑞 , 𝜂 𝑄 0 𝑀 ̃ 𝜌 / 𝜂 𝑓 ( 𝑥 ) 𝑝 𝑑 𝑥 1 / 𝑝 , ( 2 . 2 5 ) by the duality argument. Take a nonnegative function 𝑤 𝐿 𝑝 ( 𝑄 0 ) , 1 / 𝑝 + 1 / 𝑝 = 1 , satisfying that 𝑤 𝐿 𝑝 ( 𝑄 0 ) = 1 and that 𝑄 0 𝑔 ( 𝑥 ) 𝐹 1 ( 𝑥 ) 𝑝 𝑑 𝑥 1 / 𝑝 = 𝑄 0 𝑔 ( 𝑥 ) 𝐹 1 ( 𝑥 ) 𝑤 ( 𝑥 ) 𝑑 𝑥 . ( 2 . 2 6 ) Letting = 𝑔 𝑤 , we will apply Lemma 2.1 to estimation of this quantity. First, we will insert the definition of 𝐹 1 , 𝑄 0 𝑔 ( 𝑥 ) 𝐹 1 ( 𝑥 ) 𝑤 ( 𝑥 ) 𝑑 𝑥 = 𝑄 𝒟 1 𝑄 0 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝑄 = 𝑔 ( 𝑥 ) 𝑤 ( 𝑥 ) 𝑑 𝑥 𝑄 𝒟 0 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝑄 + 𝑔 ( 𝑥 ) 𝑤 ( 𝑥 ) 𝑑 𝑥 𝑄 𝒟 𝑗 , 𝑘 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝑄 𝑔 ( 𝑥 ) 𝑤 ( 𝑥 ) 𝑑 𝑥 . ( 2 . 2 7 ) First, we evaluate 𝑄 𝒟 𝑘 , 𝑗 𝜌 ( ( 𝑄 ) ) 𝑚 3 𝑄 ( 𝑓 ) 𝑄 𝑔 ( 𝑥 ) 𝑤 ( 𝑥 ) 𝑑 𝑥 . ( 2 . 2 8 ) Going through the same argument as the above, we see that (2.28) is bounded by 𝑄 𝐶 ̃ 𝜌 𝑘 , 𝑗 𝑚 3 𝑄 𝑘 , 𝑗 ( 𝑓 ) 𝑚 𝑄 𝑘 , 𝑗 | | 𝐸