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DOI: 10.22034/kjm.2016.41345

ANISOTROPIC HERZ-MORREY SPACES WITH VARIABLE EXPONENTS

HONGBIN WANG1∗ AND YIHONG WU2 Communicated by Z. Hu

Abstract. In this paper, the authors introduce the anisotropic Herz-Morrey spaces with two variable exponents and obtain some properties of these spaces.

Subsequently as an application, the authors give some boundedness on the anisotropic Herz-Morrey spaces with two variable exponents for a class of sub- linear operators, which extend some known results.

1. Introduction

In recent years, the theory of function spaces with variable exponents has developed since the paper [10] of Kov´aˇcik and R´akosn´ık appeared in 1991.

Lebesgue and Sobolev spaces with integrability exponent have been extensively investigated, see [6] and the references therein. In 2009, Izuki [8] defined the Herz-Morrey spaces with variable exponent. In 2012, Almeida and Drihem [1]

introduced the Herz spaces with two variable exponents and proved the bound- edness of some operators on these spaces. Meanwhile, extending classic function spaces arising in harmonic analysis of Euclidean spaces to other domains and non-isotropic settings is an important topic. In 2003, Bownik [2] introduced the anisotropic Hardy spaces associated with very general discrete groups of dilations.

The above spaces include the classical isotropic Hardy space theory of Fefferman and Stein [7] and parabolic Hardy space theory of Calder´on and Torchinsky [3,4].

In 2015, Wang [12] defined the anisotropic Herz spaces with variable exponents and gave some applications.

Date: Received: 15 August 2016; Revised: 29 November 2016; Accepted: 29 December 2016.

Corresponding author.

2010 Mathematics Subject Classification. Primary 46E30; Secondary 42B35, 42B20.

Key words and phrases. Anisotropic Herz-Morrey space, variable exponent, boundedness, sublinear operator.

177

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Inspired by the above results, we introduce the anisotropic Herz-Morrey spaces with two variable exponents which is a generalization of the anisotropic Herz- Morrey spaces and the Herz-Morrey spaces with variable exponent, and we obtain the boundedness of some sublinear operators on the anisotropic Herz-Morrey spaces with two variable exponents.

To be precise, we first briefly recall some standard notations in the remainder of this section. In Section 2, we will define the anisotropic Herz-Morrey spaces with two variable exponents M ˙Kq(·),pα(·),λ(A; Rn) and M Kq(·),pα(·),λ(A; Rn), and give some properties. In Section 3, we will give the boundedness of some sublinear operators on M ˙Kq(·),pα(·),λ(A; Rn) and M Kq(·),pα(·),λ(A; Rn).

Now, we first recall some notations in variable function spaces. Given an open set Ω ⊂ Rn, and a measurable function p(·) : Ω −→ [1, ∞), Lp(·)(Ω) denotes the set of measurable functions f on Ω such that for some λ > 0,

Z

 |f (x)|

λ

p(x)

dx < ∞.

This set becomes a Banach function space when equipped with the Luxemburg- Nakano norm

kf kLp(·)(Ω) = inf (

λ > 0 : Z

 |f (x)|

λ

p(x)

dx ≤ 1 )

.

These spaces are referred to as variable Lebesgue spaces or, more simply, as variable Lp spaces, since they generalized the standard Lp spaces: if p(x) = p is constant, then Lp(·)(Ω) is isometrically isomorphic to Lp(Ω). The Lp spaces with variable exponent are a special case of Musielak-Orlicz spaces.

The space Lp(·)loc(Ω) is defined by

Lp(·)loc(Ω) := {f : f ∈ Lp(·)(E) for all compact subsets E ⊂ Ω}.

Define P(Ω) to be set of p(·) : Ω −→ [1, ∞) such that

p = ess inf{p(x) : x ∈ Ω} > 1, p+ = ess sup{p(x) : x ∈ Ω} < ∞.

Denote p0(x) = p(x)/(p(x) − 1). Let B(Ω) be the set of p(·) ∈ P(Ω) such that the Hardy-Littlewood maximal operator M is bounded on Lp(·)(Ω).

In variable Lp spaces there are some important lemmas as follows.

Lemma 1.1 ([10]). Let p(·) ∈ P(Rn). If f ∈ Lp(·)(Rn) and g ∈ Lp0(·)(Rn), then f g is integrable on Rn and

Z

Rn

|f (x)g(x)|dx ≤ rpkf kLp(·)kgkLp0(·), where

rp = 1 + 1/p− 1/p+.

This inequality is named by generalized H¨older inequality with respect to the variable Lp spaces.

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Lemma 1.2 ([5]). Let p(·), q(·), r(·) ∈ P(Rn) such that 1/p(x) = 1/q(x)+1/r(x).

If f ∈ Lq(·)(Rn) and g ∈ Lr(·)(Rn), then f g ∈ Lp(·)(Rn) and kf gkLp(·) ≤ Ckf kLq(·)kgkLr(·), where C is a constant independent of the functions f and g.

Lemma 1.3 ([9]). Suppose q(·) ∈ B(Rn). Then there exists a constant C > 0 such that for all balls B in Rn,

1

|B|kχBkLq(·)(Rn)BkLq0(·)(Rn) ≤ C.

Lemma 1.4 ([9]). Let q(·) ∈ B(Rn). Then for all balls B in Rnand all measurable subsets S ⊂ B,

BkLq(·)(Rn)

SkLq(·)(Rn)

. |B|

|S|, kχSkLq(·)(Rn)

BkLq(·)(Rn)

. |S|

|B|

δ1

,kχSkLq0(·)(Rn)

BkLq0(·)(Rn)

. |S|

|B|

δ2

, where 0 < δ1, δ2 < 1 are constants.

Throughout this paper δ2 is the same as in Lemma1.4, and the notation f . g means that there exists a constant C > 0 such that f ≤ Cg. If f . g and g . f , then f ≈ g.

We recall the following two definitions in [1].

Definition 1.5 ([1]). Let a function g(·) : Rn → R.

(1) g(·) is locally log-H¨older continuous, if there exists a constant C > 0 such that

|g(x) − g(y)| ≤ C

log(e + 1/|x − y|) for all x, y ∈ Rn and |x − y| < 1/2.

(2) g(·) is locally log-H¨older continuous at the origin (or has a log decay at the origin), if there exists a constant C > 0 such that

|g(x) − g(0)| ≤ C log(e + 1/|x|) for all x ∈ Rn.

(3) g(·) is locally log-H¨older continuous at infinity (or has a log decay at infinity), if there exist some g∈ R and C > 0 such that

|g(x) − g| ≤ C log(e + |x|) for all x ∈ Rn.

By P0(Rn) and P(Rn) we denote the class of all exponents p ∈ P(Rn) which are locally log-H¨older continuous at the origin and at infinity, respectively.

Next we will introduce some basic definitions and properties of non-isotropic spaces associated with general expansive dilations. A n × n real matrix A is called an expansive matrix, sometimes called a dilation, if all eigenvalues λ of A

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satisfy |λ| > 1. We suppose λ1, ..., λn are eigenvalues of A (taken according to the multiplicity) so that 1 < |λ1| ≤ ... ≤ |λn|. A set ∆ ⊂ Rn is said to be an ellipsoid if ∆ = {x ∈ Rn : |P x| < 1}, for some nondegenerate n × n matrix P , where | · | denotes the Euclidean norm in Rn. For a dilation A, there exists an ellipsoid ∆ and r > 1 such that ∆ ⊂ r∆ ⊂ A∆, where |∆|, the Lebesgue measure of ∆, equals 1. Let Bk = Ak∆ for k ∈ Z, then we have Bk ⊂ rBk ⊂ Bk+1, and |Bk| = bk, where b = |detA| > 1. Let w be the smallest integer so that 2B0 ⊂ AwB0 = Bw. A quasi-norm associated with an expansive matrix A is a measurable mapping ρA: Rn→ [0, ∞) satisfying

ρA(x) > 0 for x 6= 0, ρA(Ax) = |detA|ρ(x) for x ∈ Rn, ρA(x + y) ≤ C(ρA(x) + ρA(y)) for x, y ∈ Rn,

where C ≥ 1 is a constant. One can show that all quasi-norms associated to a fixed dilation A are equivalent, see [2, Lemma 2.4]. Define the step homogeneous quasi-norm ρ on Rn induced by dilation A as

ρ(x) = bj if x ∈ Bj+1\ Bj, 0, if x = 0.

For any x, y ∈ Rn, we have

ρ(x + y) ≤ bw(ρ(x) + ρ(y)). (1.1) 2. Some properties for the anisotropic Herz-Morrey spaces with

two variable exponents

In this section, we first introduce the definition of anisotropic Herz-Morrey spaces with two variable exponents. Let Ck = Bk\ Bk−1 for k ∈ Z. Denote Z+

and N as the sets of all positive and non-negative integers, χk = χCk for k ∈ Z,

˜

χk= χk if k ∈ Z+ and ˜χ0 = χB0, where χCk is the characteristic function of Ck. Definition 2.1. Let α(·) : Rn → R with α(·) ∈ L(Rn), 0 < p < ∞, q(·) ∈ P(Rn) and 0 ≤ λ < ∞. The homogeneous anisotropic Herz-Morrey space M ˙Kq(·),pα(·),λ(A; Rn) associated with the dilation A is defined by

M ˙Kq(·),pα(·),λ(A; Rn) = {f ∈ Lq(·)loc(Rn\ {0}) : kf kM ˙Kα(·),λ q(·),p

< ∞}, where

kf kM ˙Kα(·),λ q(·),p

= sup

L∈Z

b−Lλ ( L

X

k=−∞

kbkα(·)f χkkpLq(·)

(Rn)

)1/p .

The non-homogeneous anisotropic Herz-Morrey space M Kq(·),pα(·),λ(A; Rn) associated with the dilation A is defined by

M Kq(·),pα(·),λ(A; Rn) = {f ∈ Lq(·)loc(Rn) : kf kM Kα(·),λ q(·),p

< ∞},

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where

kf kM Kα(·),λ

q(·),p

= sup

L∈Z

b−Lλ ( L

X

k=0

kbkα(·)f ˜χkkpLq(·)(Rn)

)1/p . Remark 2.2. If λ = 0, then

M ˙Kq(·),pα(·),0(A; Rn) = ˙Kq(·)α(·),p(A; Rn) and

M Kq(·),pα(·),0(A; Rn) = Kq(·)α(·),p(A; Rn),

where ˙Kq(·)α(·),p(A; Rn) and Kq(·)α(·),p(A; Rn) are the anisotropic Herz spaces associated with the dilation A.

Next we will consider some properties of M ˙Kq(·),pα(·),λ(A; Rn). There are similar properties for M Kq(·),pα(·),λ(A; Rn).

Theorem 2.3. Suppose α(·), α1(·), α2(·) ∈ L(Rn)∩P0(Rn)∩P(Rn), q(·), q1(·), q2(·) ∈ P(Rn), 1 < p, p1, p2 < ∞, and 0 ≤ λ, λ1, λ2 < ∞ such that α(·) = α1(·) + α2(·), 1/q(·) = 1/q1(·) + 1/q2(·), 1/p = 1/p1 + p2 and λ = λ1 + λ2. If f ∈ M ˙Kqα1(·),λ1

1(·),p1 (A; Rn) and g ∈ M ˙Kqα2(·),λ2

2(·),p2 (A; Rn), then f g ∈ M ˙Kq(·),pα(·),λ(A; Rn) and

kf gkM ˙Kα(·),λ q(·),p

≤ kf kM ˙Kα1(·),λ1

q1(·),p1

kgkM ˙Kα2(·),λ2

q2(·),p2

. Proof. By Lemma 1.2 and the H¨older inequality we have

kf gkM ˙Kα(·),λ q(·),p

= sup

L∈Z

b−Lλ ( L

X

k=−∞

kbkα(·)f gχkkpLq(·)

(Rn)

)1/p

≤ sup

L∈Z

b−Lλ1b−Lλ2 ( L

X

k=−∞

kb1(·)f χkkp

Lq1(·)(Rn)kb2(·)kkp

Lq2(·)(Rn)

)1/p

≤ sup

L∈Z

b−Lλ1 ( L

X

k=−∞

kb1(·)f χkkp1

Lq1(·)(Rn)

)1/p1

×b−Lλ2 ( L

X

k=−∞

kb2(·)kkpL2q2(·)

(Rn)

)1/p2

= kf kM ˙Kα1(·),λ1 q1(·),p1

kgkM ˙Kα2(·),λ2 q2(·),p2

.

So we complete the proof of Theorem2.3. 

From Theorem 2.3 we can get the following Corollary.

Corollary 2.4. Suppose α(·), αi(·) ∈ L(Rn) ∩ P0(Rn) ∩ P(Rn), q(·), qi(·) ∈ P(Rn), 1 < p, pi < ∞, and 0 ≤ λ, λi < ∞(1 ≤ i ≤ m) such that α(·) =

m

X

i=1

αi(·),

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1/q(·) =

m

X

i=1

1/qi(·), 1/p =

m

X

i=1

1/pi and λ =

m

X

i=1

λi. If fi ∈ M ˙Kqαi(·),λi

i(·),pi (A; Rn), then

m

Y

i=1

fi ∈ M ˙Kq(·),pα(·),λ(A; Rn) and

k

m

Y

i=1

fikM ˙Kα(·),λ q(·),p

m

Y

i=1

kfik

M ˙Kαi(·),λi

qi(·),pi

.

Theorem 2.5. Suppose α(·) ∈ L(Rn) ∩ P0(Rn) ∩ P(Rn), q(·) ∈ P(Rn), 1 <

p < ∞, and 0 ≤ λ < ∞. If f, g ∈ M ˙Kq(·),pα(·),λ(A; Rn), then f + g ∈ M ˙Kq(·),pα(·),λ(A; Rn) and

kf + gkM ˙Kα(·),λ

q(·),p

≤ kf kM ˙Kα(·),λ

q(·),p

+ kgkM ˙Kα(·),λ

q(·),p

. Proof. By the Minkowski inequality we have

kf + gkM ˙Kα(·),λ q(·),p

= sup

L∈Z

b−Lλ ( L

X

k=−∞

kbkα(·)(f + g)χkkpLq(·)

(Rn)

)1/p

≤ sup

L∈Z

b−Lλ ( L

X

k=−∞

kbkα(·)f χkkpLq(·)(Rn)+ kbkα(·)kkpLq(·)(Rn)

)1/p

≤ sup

L∈Z

b−Lλ

L

X

k=−∞

kbkα(·)f χkkpLq(·)(Rn)

!1/p +

L

X

k=−∞

kbkα(·)kkpLq(·)(Rn)

!1/p

≤ kf kM ˙Kα(·),λ q(·),p

+ kgkM ˙Kα(·),λ q(·),p

.

So we obtain Theorem 2.5. 

From Theorem 2.5 we can get the following Corollary.

Corollary 2.6. Suppose α(·) ∈ L(Rn) ∩ P0(Rn) ∩ P(Rn), q(·) ∈ P(Rn), 1 < p < ∞, and 0 ≤ λ < ∞. If fi ∈ M ˙Kq(·),pα(·),λ(A; Rn), 1 ≤ i ≤ m, then

m

X

i=1

fi ∈ M ˙Kq(·),pα(·),λ(A; Rn) and

k

m

X

i=1

fik

M ˙Kα(·),λq(·),p

m

X

i=1

kfik

M ˙Kq(·),pα(·),λ.

3. Boundedness of some sublinear operators

In this section, we will investigate the boundedness on the anisotropic Herz- Morrey spaces with two variable exponents for some sublinear operators.

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Theorem 3.1. Let 0 < p < ∞, q(·) ∈ B(Rn), α(·) ∈ L(Rn) ∩ P0(Rn) ∩ P(Rn), 0 < 2λ < α(0), α< δ2. If a sublinear operator T satisfies

|T f (x)| . Z

Rn

|f (y)|

ρ(x − y)dy, x /∈ suppf, (3.1) for any f ∈ Lq(·)(Rn) with a compact support and T is bounded on Lq(·)(Rn), then T is bounded on M ˙Kq(·),pα(·),λ(A; Rn) and M Kq(·),pα(·),λ(A; Rn), respectively.

Proof. It suffices to prove that T is bounded on M ˙Kq(·),pα(·),λ(A; Rn). The non- homogeneous case can be proved in the similar way. Suppose f ∈ M ˙Kq(·),pα(·),λ(A; Rn).

Similar to the method of Proposition 2.5 in [11] we get kT f kM ˙Kα(·),λ

q(·),p

≈ max

 sup

L≤0,L∈Z

b−Lλ

 L

X

k=−∞

bkα(0)pk(T f )χkkpLq(·)(Rn)

1/p

,

sup

L>0,L∈Z

 b−Lλ

 −1 X

k=−∞

bkα(0)pk(T f )χkkpLq(·)

(Rn)

1/p

+b−Lλ

 L X

k=0

bpk(T f )χkkp

Lq(·)(Rn)

1/p

= max{I, II}.

It suffices to prove that I is bounded on M ˙Kq(·),pα(·),λ(A; Rn), while the estimate of II is essentially similar to that of I. Denote fj = f χj for each j ∈ Z, then we have f (x) =

X

j=−∞

fj(x). It is easy to see that

Ip . sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p

k−w−1

X

j=−∞

k(T fjkkLq(·)(Rn)

!p

+ sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p

L−1

X

j=k−w

k(T fjkkLq(·)(Rn)

!p

+ sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p

X

j=L

k(T fjkkLq(·)(Rn)

!p

= I1 + I2+ I3.

Let us first estimate I1. If j ≤ k − w − 1, x ∈ Ck and y ∈ Bj, by (1.1) we have ρ(x − y) ≥ b−wρ(x) − ρ(y) ≥ b−wρ(x) − b−w−1ρ(x) = b−w(1 − 1/b)ρ(x).

Therefore by (3.1) and the generalized H¨older inequality, we get

|T fj(x)| ≤ Cρ(x)−1 Z

Bj

|fj(y)|dy

≤ Cb−kkfjkLq(·)(Rn)BjkLq0(·)(Rn).

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So by Lemma1.3 and Lemma1.4, we have

k(T fjkkLq(·)(Rn) . b−kkfjkLq(·)(Rn)BjkLq0(·)(Rn)BkkLq(·)(Rn)

. b−kkfjkLq(·)(Rn) |Bk|kχBkk−1

Lq0(·)(Rn)kχBjkLq0(·)(Rn)

. kfjkLq(·)(Rn)

BjkLq0(·)(Rn)

BkkLq0(·)(Rn)

. bδ2(j−k)kfjkLq(·)(Rn). (3.2)

Therefore, when 0 < p ≤ 1, by 0 < α(0) < δ2, we get

I1 . sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p

k−w−1

X

j=−∞

bδ2(j−k)pkfjkpLq(·)

(Rn)

. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

k−w−1

X

j=−∞

bjα(0)pb(j−k)(δ2−α(0))pkfjkpLq(·)

(Rn)

. sup

L≤0,L∈Z

b−Lλp

L−w−1

X

j=−∞

bjα(0)p

L

X

k=j+w+1

b(j−k)(δ2−α(0))pkfjkpLq(·)

(Rn)

. sup

L≤0,L∈Z

b−Lλp

L−w−1

X

j=−∞

bjα(0)pkfjkp

Lq(·)(Rn). kf kpM ˙Kα(·),λ q(·),p

. (3.3)

When 1 < p < ∞, take 1/p + 1/p0 = 1. Since 0 < α(0) < δ2, by (3.2) and the H¨older inequality, we have

I1 . sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p

k−w−1

X

j=−∞

bδ2(j−k)kfjkLq(·)(Rn)

!p

. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

k−w−1 X

j=−∞

bjα(0)pb(j−k)[δ2−α(0)]p/2kfjkpLq(·)(Rn)



×

k−w−1 X

j=−∞

b(j−k)[δ2−α(0)]p0/2

p/p0

. sup

L≤0,L∈Z

b−Lλp

L−w−1

X

j=−∞

bjα(0)p

L

X

k=j+w+1

b(j−k)(δ2−α(0))p/2kfjkpLq(·)(Rn)

. sup

L≤0,L∈Z

b−Lλp

L−w−1

X

j=−∞

bjα(0)pkfjkpLq(·)

(Rn). kf kpM ˙Kα(·),λ q(·),p

. (3.4)

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Let us now estimate I2. Similarly, we consider two cases for p. When 0 < p ≤ 1, by 0 < α(0) and Lq(·)(Rn) boundedness of T , we have

I2 = sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p

L−1

X

j=k−w

k(T fjkkLq(·)(Rn)

!p

. sup

L≤0,L∈Z

b−Lλp

L−1

X

j=−∞

bjα(0)pkfjkpLq(·)

(Rn) j+w

X

k=−∞

b(k−j)α(0)p . kf kpM ˙Kα(·),λ

q(·),p

. (3.5)

When 1 < p < ∞, take 1/p + 1/p0 = 1. By 0 < α(0), Lq(·)(Rn) boundedness of T and the H¨older inequality, we have

I2 . sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p

L−1

X

j=k−w

kfjkLq(·)(Rn)

!p

. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

L−1

X

j=k−w

bjα(0)pkfjkp

Lq(·)(Rn)b(k−j)α(0)p/2

!

×

L−1

X

j=k−w

b(k−j)α(0)p0/2

!p/p0

. sup

L≤0,L∈Z

b−Lλp

L−1

X

j=−∞

bjα(0)pkfjkpLq(·)

(Rn) j+w

X

k=−∞

b(k−j)α(0)p/2

. kf kpM ˙Kα(·),λ q(·),p

. (3.6)

For I3, when 0 < p ≤ 1, by 0 < 2λ < α(0) and Lq(·)(Rn) boundedness of T , we get

I3 = sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p

X

j=L

k(T fjkkLq(·)(Rn)

!p

. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

X

j=L

b(k−j)α(0)pbjα(0)pkfjkpLq(·)(Rn)

. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

X

j=L

b(k−j)α(0)pbjλpb−jλp

j

X

m=−∞

bmα(0)pkfmkpLq(·)(Rn)

!

(3.7)

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. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

X

j=L

b(k−j)α(0)pbjλpkf kp

M ˙Kq(·),pα(·),λ

. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p

! X

j=L

b(λ−α(0))jp

! kf kp

M ˙Kq(·),pα(·),λ

. sup

L≤0,L∈Z

b−LλpbLα(0)pb(λ−α(0))Lpkf kp

M ˙Kq(·),pα(·),λ

. kf kpM ˙Kα(·),λ q(·),p

. (3.8)

When 1 < p < ∞, take 1/p + 1/p0 = 1. Since 0 < 2λ < α(0), by Lq(·)(Rn) boundedness of T and the H¨older inequality, we have

I3 . sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p

X

j=L

kfjkLq(·)(Rn)

!p

. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

X

j=L

bjα(0)pkfjkpLq(·)

(Rn)b(k−j)α(0)p/2

! X

j=L

b(k−j)α(0)p0/2

!p/p0

. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

X

j=L

b(k−j)α(0)p/2bjα(0)pkfjkpLq(·)

(Rn)

. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

X

j=L

b(k−j)α(0)p/2bjλpkf kp

M ˙Kq(·),pα(·),λ

. sup

L≤0,L∈Z

b−Lλp

L

X

k=−∞

bkα(0)p/2

! X

j=L

b(λ−α(0)/2)jp

! kf kp

M ˙Kq(·),pα(·),λ

. sup

L≤0,L∈Z

b−LλpbLα(0)p/2b(λ−α(0)/2)Lpkf kp

M ˙Kα(·),λq(·),p

. kf kpM ˙Kα(·),λ q(·),p

. (3.9)

Combining (3.3)-(3.9), we have

I . kf kM ˙Kα(·),λ

q(·),p

.

Thus, the proof of Theorem3.1 is completed. 

Remark 3.2. From the proof of Theorem 3.1, it is easy to see that the size con- dition (3.1) can be replaced by

|T f (x)| ≤ Ckf kL1

ρ(x) , if inf

y∈suppfρ(x − y) ≥ b−w(1 − 1/b)ρ(x), (3.10) for all f ∈ Lq(·)(Rn) with compact support.

(11)

Acknowledgement. The authors are very grateful to the referees for their valuable comments. This work was supported by China Postdoctoral Science Foundation (Grant No. 2016M601105).

References

1. A. Almeida and D. Drihem, Maximal, potential and singular type operators on Herz spaces with variable exponents, J. Math. Anal. Appl., 394 (2012), 781–795.

2. M. Bownik, Anisotropic Hardy spaces and wavelets, Mem. Amer. Math. Soc., 164 (2003), 122pp.

3. A.P. Calder´on and A. Torchinsky, Parabolic maximal functions associated with a distribu- tion, Adv. Math., 16 (1975), 1–64.

4. A.P. Calder´on and A. Torchinsky, Parabolic maximal functions associated with a distribution II, Adv. Math., 24 (1977), 101–171.

5. D.V. Cruz-Uribe and A. Fiorenza, Variable Lebesgue Spaces: Foundations and Harmonic Analysis, Applied and Numerical Harmonic Analysis, Springer, Heidelberg, 2013.

6. L. Diening, P. Harjulehto, P. H¨ast¨o and M. R˚ziˇcka, Lebesgue and Sobolev spaces with variable exponents, Lecture Notes in Math., vol. 2017, Springer-Verlag, Berlin, 2011.

7. C. Fefferman and E.M. Stein, Hp spaces of several variables, Acta Math., 129 (1972), 137–193.

8. M. Izuki, Boundedness of vector-valued sublinear operators on Herz-Morrey spaces with variable exponent, Math. Sci. Res. J., 13 (2009), 243–253.

9. M. Izuki, Boundedness of sublinear operators on Herz spaces with variable exponent and application to wavelet characterization, Anal. Math., 36 (2010), 33–50.

10. O. Kov´cik and J. R´akosn´ık, On spaces Lp(x) and Wk,p(x), Czechoslovak Math. J., 41 (1991), 592–618.

11. Y. Lu and Y. Zhu, Boundedness of multilinear Calder´on-Zygmund singular operators on Morrey-Herz spaces with variable exponents, Acta Math. Sin.(Engl. Ser.), 30 (2014), 1180–

1194.

12. H. Wang, Anisotropic Herz spaces with variable exponents, Commun. Math. Anal., 18 (2015), 1–14.

1 School of Mathematical Sciences,, University of Chinese Academy of Sci- ences,, Beijing 100049, China;

School of Science, Shandong University of Technology, Zibo 255049, China.

E-mail address: [email protected]

2 Department of Recruitment and Employment, Zibo Normal College, Zibo 255130, China.

E-mail address: [email protected]

References

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