Home Mathematics Lp estimates for maximal functions along surfaces of revolution on product spaces
Article Open Access

Lp estimates for maximal functions along surfaces of revolution on product spaces

  • Mohammed Ali EMAIL logo and Musa Reyyashi
Published/Copyright: November 19, 2019

Abstract

This paper is concerned with establishing Lp estimates for a class of maximal operators associated to surfaces of revolution with kernels in Lq(Sn−1 × Sm−1), q > 1. These estimates are used in extrapolation to obtain the Lp boundedness of the maximal operators and the related singular integral operators when their kernels are in the L(logL)κ(Sn−1 × Sm−1) or in the block space Bq0,κ1 (Sn−1 × Sm−1). Our results substantially improve and extend some known results.

1 Introduction and main results

Let n, m ≥ 2, and let RN (N = n or m) be the N-dimensional Euclidean space. Let SN−1 be the unit sphere in RN equipped with the normalized Lebesgue surface measure = (⋅). Also, let x = x|x| for xRn ∖ {0}, y = y/|y| for yRm ∖ {0}.

Let KΩ,h(x, y) = Ω(x, y) |x|n|y|m h(|x|, |y|), where h is a measurable function on R+ × R+ and Ω is an integrable function on Sn−1 × Sm−1 that satisfies

Sn1Ω(x,.)dσ(x)=Sm1Ω(.,y)dσ(y)=0and (1.1)
Ω(rx,ty)=Ω(x,y)forallr,t>0. (1.2)

For suitable mappings ϕ, ψ : R+R, consider the singular integral operator TΩ,h,ϕ,ψP1,P2 defined, initially for C0 functions on Rn+1 × Rm+1, by

TΩ,h,ϕ,ψP1,P2(f)(x¯,y¯)=p.vRn×RmeiP1(u)+iP2(v)×f(xu,xn+1ϕ(u),yv,ym+1ψ(v))KΩ,h(u,v)dudv,

where (x, y) = (x, xn+1, y, ym+1) ∈ Rn+1 × Rm+1 and P1 : RnR, P2 : RmR are two real-valued polynomials.

When P1(u) = 0 and P2(v) = 0, we denote TΩ,h,ϕ,ψP1,P2 by TΩ,h,ϕ,ψ. Also, when ϕ(t) = ψ(t) = t, then TΩ,h,ϕ,ψ (denoted by TΩ,h) is just the classical singular integral operator introduced by Fefferman in [1] in which he obtained the Lp boundedness of TΩ,h for all 1 < p < ∞ whenever Ω satisfies some regularity conditions and h ≡ 1. As a matter of fact, the systematic study of such operator began by Fefferman in [1], and then it was elaborated very much by Fefferman and Stein in [2]. Subsequently, the investigation of the Lp boundedness of TΩ,h under very various conditions on Ω and h has attracted the attention of many authors. For example, it was proved in [3] that TΩ,h is bounded on Lp(Rn × Rm) for 1 < p < ∞ when ΩL(log L)2(Sn−1 × Sm−1) and h satisfies certain integrability-size condition. Furthermore, the authors of [3] established the optimality of the condition in the sense that the space L(log L)2(Sn−1 × Sm−1) cannot be replaced by L(log L)2–ε(Sn−1 × Sm−1) for any 0 < ε < 2. For more information about the importance and the recent advances on the study of such operators, the readers are refereed (for instance to [1, 2, 3, 4, 5], and the references therein).

On the other side, the study of the singular integrals on product spaces along surfaces of revolution has been started. For example, if ϕ and ψ are in C2([0, ∞)), convex and increasing functions with ϕ(0) = ψ(0) = 0, then Al-Salman in [4] showed that TΩ,1,ϕ,ψ is bounded on Lp(Rn+1 × Rm+1) (1 < p < ∞) provided that ΩL(log L)2(Sn−1 × Sm−1). Recently, Al-Salman improved this result in [6]. In fact, when ϕ, ψ are given as in [4], he verified the Lp boundedness of TΩ,h,ϕ,ψ for all p ∈ (1, ∞) under the conditions ΩL(log L)(Sn−1 × Sm−1) and hL2(R+×R+,drdtrt) with hL2(R+×R+,drdtrt)1.

The maximal operator that related to our singular integral operator is MΩ,ϕ,ψP1,P2 that given by

MΩ,ϕ,ψP1,P2(f)(x¯,y¯)=suphUTΩ,h,ϕ,ψP1,P2(f)(x¯,y¯),

where U=hL2(R+×R+,drdtrt);hL2(R+×R+,drdtrt)1.

Again, when P1(u) = 0 and P2(v) = 0, we denote MΩ,ϕ,ψP1,P2 by 𝓜Ω,ϕ,ψ. Also, when ϕ(t) = ψ(t) = t, then 𝓜Ω,ϕ,ψ reduces to the classical maximal operator denoted by 𝓜Ω. Historically, The operator 𝓜Ω was introduced by Ding in [7] in which he proved the L2 boundedness of 𝓜Ω whenever ΩL(log L)2(Sn−1 × Sm−1). This result was improved independently by Al-Qassem and Pan in [8] and by Al-Salman in [9]. Precisly, they showed that 𝓜Ω is of type (p, p) for all p ≥ 2 provided that ΩL(log L)(Sn−1 × Sm−1). Moreover, they pointed out that the condition ΩL(log L)(Sn−1 × Sm−1) is optimal in the sense that the exponent 1 in L(log L)(Sn−1 × Sm−1) cannot be replaced by any smaller positive number τ < 1 so that 𝓜Ω is bounded on L2(Rn+1 × Rm+1). Also, an improvement of the result in [7] was obtained by Al-Qassem in [10]. Indeed, Al-Qassem established the Lp(2 ≤ p < ∞) estimates for the class 𝓜Ω whenever Ω belongs to the block space Bq(0,0) (𝓢n−1 × 𝓢m−1) for some q > 1. Furthermore, he proved that the condition Ω Bq(0,0) (𝓢n−1 × 𝓢m−1) is nearly optimal in the sense that the operator 𝓜Ω may lose the L2 boundedness if Ω is assumed to be in the space Bq(0,ε) (𝓢n−1 × 𝓢m−1) for some –1 < ε < 0. Recently, it was found in [6] that the maximal operator 𝓜Ω,ϕ,ψ is bounded on Lp(Rn+1 × Rm+1) for any p ≥ 2 if ΩL(log L)(Sn−1 × Sm−1), and ϕ, ψ are in C2([0, ∞)), convex and increasing functions with ϕ(0) = ψ(0) = 0. Very recently, when ϕ(t) = ψ(t) = t, Al-Dolat and et al. found in [11] that the Lp (p ≥ 2) boundedness of MΩ,ϕ,ψP1,P2 is obtained under the condition ΩL(log L)(𝓢n−1 × Sm−1) ∪ Bq(0,0) (𝓢n−1 × Sm−1) with q > 1. Subsequently, the investigation of the Lp boundedness of MΩ,ϕ,ψP1,P2 under weak conditions has received much attentions from many mathematicians. For the significance of considering the integral operators MΩ,ϕ,ψP1,P2 , we refear the readers to consult [8] and [11, 12, 13], among others.

The main result of this work is formulated as follows:

Theorem 1.1

Let ΩLq(Sn−1 × Sm−1), q > 1 and satisfy the conditions (1.1)-(1.2) withΩL1(Sn−1×Sm−1) ≤ 1, and let μ = μq(Ω) = log(e + ∥ΩLq(Sn−1×Sm−1)). Assume that ϕ, ψ are in C2([0, ∞)), convex and increasing functions with ϕ(0) = ψ(0) = 0. Let P1 : RnR and P2 : RmR be two real-valued polynomials of degrees d1, d2, respectively. Then there exists a constant Cp,q > 0 such that

MΩ,ϕ,ψP1,P2(f)Lp(Rn+1×Rm+1)Cp,q1+μfLp(Rn+1×Rm+1) (1.3)

for all p ≥ 2, where Cp,q=21/q21/q12Cp and Cp is a positive constant that may depend on the degrees of the polynomials P1, P2 but it is independent on Ω, ϕ, ψ, q, and the coefficients of the polynomials P1, P2.

We remark that by the result in Theorem 1.1 and using an extrapolation argument, we get that MΩ,ϕ,ψP1,P2 is bounded on Lp(Rn+1 × Rm+1) for 2 ≤ p < ∞ if ΩL(log L)(𝓢n−1 × Sm−1) ∪ Bq(0,0) (𝓢n−1 × Sm−1) for some q > 1.

Here and henceforth, the letter C denotes a bounded positive constant that may vary at each occurrence but independent of the essential variables.

2 Preliminary lemmas

In this section, we present and prove some lemmas used in the sequel. The first lemma can be derived by applying the same technique that Al-Qassam and Pan used in [14, pp. 64-65].

Lemma 2.1

Let ΩLq(SN−1), q > 1 be a homogeneous function of degree zero on RN withΩL1(SN−1) ≤ 1, and let ϕ : R+R be a C2([0, ∞)), convex and increasing function with ϕ(0) = 0. Consider the maximal function 𝓝Ω,ϕ given by

NΩ,ϕf(z¯)=supjZ2jy2j+1f(zy,zN+1ϕ(y))Ω(y)yNdy.

Then for p > 1 and fLp(𝓢N+1) there exists a positive number Cp such that

NΩ,ϕ(f)pCpfp.

Lemma 2.2

Assume that ϕ, ψ are C2([0, ∞)), convex and increasing functions with ϕ(0) = ψ(0) = 0. Let ΩLq(Sn−1 × Sm−1), q > 1 and satisfy the conditions (1.1)-(1.2) withΩL1(Sn−1×Sm−1) ≤ 1. Then for all fLp(𝓢n+1 × Rm+1) and p > 1, the maximal function

NΩ,ϕ,ψf(x¯,y¯)=supi,jZΛi,jf(xu,xn+1ϕ(u),yv,ym+1ψ(v))Ω(u,v)unvmdudv

satisfies

NΩ,ϕ,ψ(f)pCpfp,

where Λi,j = {(u, v) ∈ Rn × Rm : 2i ≤ ∥u∥ ≤ 2i+1, 2j ≤ ∥v∥ ≤ 2j+1} and the positive constant Cp is independent of the functions ϕ, ψ and Ω.

It is easy to prove the above lemma by using Lemma 2.1 and the inequality 𝓝Ω,ϕ,ψ f(x, y) ≤ 𝓝Ω,ψ ∘ 𝓝Ω,ϕ f(x, y), where 𝓝Ω,ϕ f(x, y) = 𝓝Ω,ϕ f(⋅, y)(x), 𝓝Ω, ψ f(x, y) = 𝓝Ω,ψ f(x, ⋅)(y), and ∘ denotes the composition of operators.

A significant step toward proving Theorem 1.1 is to estimate the following Fourier transform:

Lemma 2.3

Let ΩLq(Sn−1 × Sm−1), q > 1 and satisfy the conditions (1.1)-(1.2) withΩL1(Sn−1×Sm−1) ≤ 1, and let μ = μq(Ω) = log(e + ∥ΩLq(Sn−1×Sm−1)). Assume that ϕ, ψ are arbitrary functions on R+, and assume also that P1 = ∑α∥≤d1 aα xα is a polynomial of degree d1 ≥ 1 such thatxd1 is not one of its terms andα∥=d1aα∥ = 1; and P2 = ∑β∥≤d2 bβyβ is a polynomial of degree d2 ≥ 1 such thatyd2 is not one of its terms andβ∥=d2bβ∥ = 1. For i, jZ, define 𝓙i,j,Ω,ϕ,ψ : Rn+1 × Rm+1R by

Ji,j,Ω,ϕ,ψ(ξ¯,η¯)=122μ122μSn1×Sm1Ω(u,v)Ai,Ω,ϕ(r,u,ξ.u,ξn+1)Bj,Ω,ψ(t,v,η.v,ηm+1)dσ(u)dσ(v)2drdtrt,

where

Ai,Ω,ϕ(r,u,ξ.u,ξn+1)=eiP1(2(i+1)μru)+(2(i+1)μ)ruξ+ϕ(2(i+1)μr)ξn+1

and

Bj,Ω,ψ(t,v,η.v,ηm+1)=eiP2(2(j+1)μtv)+(2(j+1)μ)tvη+ψ(2(j+1)μt)ηm+1.

Then, a positive constant C exists such that

sup(ξ¯,η¯)Rn+1×Rm+1Ji,j,Ω,ϕ,ψ(ξ¯,η¯)Cμ22(i+j+2)/4q.

Proof

On one hand, it is trivial to get that

Ji,j,Ω,ϕ,ψ(ξ¯,η¯)C122μ122μSn1×Sm1Ω(u,v)dσ(u)dσ(v)2drdtrtCμ2Ω12Cμ2. (2.1)

Also, it is easy to see that

P1(γru)P1(γrz)+γruξγrzξ=(γr)d1α=d1aαuαα=d1aαzα+γr(uz)ξ+H(u,z,r,ξ),

with dd1drd1H(u,z,r,ξ)=0 and γ = 2–(i+1)μ. Without lossing of generality, we may assume that d1 > 1. Hence, by Van der-Corput Lemma, we obtain

122μAi,Ω,ϕ(r,u,ξ.u,ξn+1)Ai,Ω,ϕ(r,z,ξ.z,ξn+1)¯drrCγd1α=d1aαuαzα1/d1.

Combine the last inequality with the trivial estimates

122μAi,Ω,ϕ(r,u,ξ.u,ξn+1)Ai,Ω,ϕ(r,z,ξ.z,ξn+1)¯drrCμ,

we deduce

122μAi,Ω,ϕ(r,u,ξ.u,ξn+1)Ai,Ω,ϕ(r,z,ξ.z,ξn+1)¯drrCμ1θγd1α=d1aαuαzαθ/d1

for any 0 < θ < 1. In the same manner, we derive

122μBj,Ω,ψ(t,v,η.v,ηm+1)Bj,Ω,ψ(t,w,η.w,ηm+1)¯dttCμ1θ2(j+1)μd2β=d2bβvβwβθ/d2.

Thus, using Hölder’s inequality leads to

Ji,j,Ω,ϕ,ψ(ξ¯,η¯)qΩq2qSn1×Sm12122μ122μAi,Ω,ϕ(r,u,ξ.u,ξn+1)Ai,Ω,ϕ(r,z,ξ.z,ξn+1)¯drr×Bj,Ω,ψ(t,v,η.v,ηm+1)Bj,Ω,ψ(t,w,η.w,ηm+1)¯dttqσ(u)dσ(z)σ(v)dσ(w). (2.2)

Since α=d1aα=β=d2bβ=1, then by taking θ = 1/4μq′, we have

Ji,j,Ω,ϕ,ψ(ξ¯,η¯)Ωq22(i+1)/4q2(j+1)/4qμ21/2μqCμ22(i+j+2)/4q. (2.3)

We shall need the following Lemma which can be acquired by using the arguments employed in the proof of [6, Theorem 4.1] as well as [15, Theorem 1.6].

Lemma 2.4

Let ΩLq(Sn−1 × Sm−1), q > 1 and satisfy the conditions (1.1)-(1.2) withΩL1(Sn−1×Sm−1) ≤ 1. Assume that ϕ, ψ and μ are given as in Theorem 1.1. Then there exists a constant Cp,q > 0 such that

MΩ,ϕ,ψ(f)Lp(Rn+1×Sm1)Cp,q1+μfLp(Rn+1×Rm+1) (2.4)

for 2 ≤ p < ∞.

Proof

Choose collections of functions {Φi}iZ and {Ψj}jZ defined on Rn and Rm, respectively with the following properties:

(i)Φ^iissupportedinξRn:ξIi,μ=2(i+1)μ,2(i1)μ;(ii)Ψ^jissupportedinηRm:ηIj,μ;(iii)0Φ^i,Ψ^j1;(iv)iZΦ^i2(ξ)=jZΨ^j2(η)=1.

Define the multiplier operators Sj,i in Rn+1 × Rm+1 via the Fourier transform given by

Sj,i^(ξ¯,η¯)=Φ^i(ξ))Ψ^j(η)).

Hence, for any f C0 (Rn+1 × Rm+1), we have

MΩ,ϕ,ψ(f)(x¯,y¯)j,iZTΩ,ϕ,ψ,j,i(f)(x¯,y¯), (2.5)

where

TΩ,ϕ,ψ,j,i(f)(x¯,y¯)=R+×R+WΩ,ϕ,ψ,j,i(f)(x¯,y¯)2drdtrt1/2,
WΩ,ϕ,ψ,j,i(f)(x¯,y¯)=s,lZSn1×Sm1Sj+l,i+s(f)(xru,xn+1ϕ(r),ytv,ym+1ψ(t))χIs,μ×Il,μΩ(u,v)dσ(u)σ(v).

Therefore, by using [6, Theorem 4.1], we get

TΩ,ϕ,ψ,j,i(f)pCp,qμ2ε1|j|2ε2|i|fp (2.6)

for some constants 0 < ε1, ε2 < 1 and for all 2 ≤ p < ∞. Consequently, the inequality (2.4) follows by using (2.5) and (2.6).□

3 Proof of Theorem 1.1

The proof of Theorem 1.1 mainly depends on the approaches employed in the proof of [11, Theorem 1.1], which have their roots in [16]. Precisly, we argue the mathematical induction on the degrees of the polynomials P1 and P2.

If d1 = d2 = 0, then by Lemma 2.4, we directly attain

MΩ,ϕ,ψP1,P2(f)pCp,q1+μfp (3.1)

for all p ≥ 2. Also, if d1 = 0 or d2 = 0, then by [17, Theorem 1.1], it is easy to satisfy the inequality (1.3) for all p ≥ 2.

Now, assume that (1.3) is true for any polynomial P1 of degree less than or equal to d1 and for any polynomial P2 of degree d2. We need to show that (1.3) is still true if degree(P1) = d1 + 1, and degree(P2) = d2. Without loss of generality, we may assume P1(x) = |α|d1+1 aα xα is a polynomial of degree d1 + 1 such that α=d1+1 aα∥ = 1 and does not contain ∥xd1+1 as one of its terms. Also, we may assume P2(y) = |β|d2 bβyβ is a given polynomial of degree d2 such that β=d2 bβ∥ = 1 and does not contain ∥yd2 as one of its terms. By duality and a simple change of variables, we have

MΩ,ϕ,ψP1,P2(f)(x¯,y¯)=R+×R+GP1,P2,ϕ,ψ,Ω(f)(x¯,y¯,r,t)2drdtrt1/2,

where

GP1,P2,ϕ,ψ,Ω(f)(x¯,y¯,r,t)=Sn1×Sm1eiP1(ru)+iP2(tv)f(xru,xn+1ϕ(r),ytv,ym+1ψ(t))Ω(u,v)dσ(u)dσ(v).

Choose two collections of 𝓒 functions {Υi}iZ and {Γj}jZ on (0, ∞), that satisfying the following conditions:

supp YiJi,μ=2(i+1)μ,2(i1)μ;supp ΓjJj,μ;0Yi,Γj1;andiZYiu=jZΓjv=1.

Define the multiplier operators Sj,i in Rn+1 × Rm+1 by

(Sj,if)^(ξ¯,η¯)=Yi(ξ)Γj(η)f^(ξ,η)for(ξ¯,η¯)=(ξ,ξn+1,η,ηm+1)Rn+1×Rm+1.

Set

A(u)=i=0Yi(u),A0(u)=i=1Yi(u),B(v)=j=0Γj(v),andB0(v)=j=1Γj(v).

Thanks to Minkowski’s inequality, we have

MΩ,ϕ,ψP1,P2(f)(x¯,y¯)MΩ,ϕ,ψ,,P1,P2(f)(x¯,y¯)+MΩ,ϕ,ψ,,0P1,P2(f)(x¯,y¯)+MΩ,ϕ,ψ,0,P1,P2(f)(x¯,y¯)+MΩ,ϕ,ψ,0,0P1,P2(f)(x¯,y¯), (3.2)

where

MΩ,ϕ,ψ,,P1,P2(f)(x¯,y¯)=2μ2μA(r)B(t)GP1,P2,ϕ,ψ,Ω(f)(x¯,y¯,r,t)2drdtrt1/2,MΩ,ϕ,ψ,,0P1,P2(f)(x¯,y¯)=2μ01A(r)B0(t)GP1,P2,ϕ,ψ,Ω(f)(x¯,y¯,r,t)2drdtrt1/2,MΩ,ϕ,ψ,0,P1,P2(f)(x¯,y¯)=012μA0(r)B(t)GP1,P2,ϕ,ψ,Ω(f)(x¯,y¯,r,t)2drdtrt1/2,

and

MΩ,ϕ,ψ,0,0P1,P2(f)(x¯,y¯)=0101A0(r)B0(t)GP1,P2,ϕ,ψ,Ω(f)(x¯,y¯,r,t)2drdtrt1/2.

Let us first estimate the Lp-norm of MΩ,ϕ,ψ,,P1,P2 (f). Define

MΩ,ϕ,ψ,,,i,jP1,P2(f)(x¯,y¯)=2(i1)μ2(i+1)μ2(j1)μ2(j+1)μGP1,P2,ϕ,ψ,Ω(f)(x¯,y¯,r,t)2drdtrt1/2.

Hence, by generalized Minkowski’s inequality, it is easy to reach

MΩ,ϕ,ψ,,P1,P2(f)(x¯,y¯)i,j=0MΩ,ϕ,ψ,,,i,jP1,P2(f)(x¯,y¯). (3.3)

If p = 2, then by a simple change of variables, Plancherel’s theorem, Fubini’s theorem, and Lemma 2.3, we get that

MΩ,ϕ,ψ,,,i,jP1,P2(f)2=Rn+1×Rm+1f^(ξ¯,η¯)2Ji,j,Ω,ϕ,ψ(ξ¯,η¯)dξ¯dη¯1/2C2(i+j+2)8q1+μf2. (3.4)

However, if p > 2, then by the duality, there exists bL(p/2)(Rn+1 × Rn+1) with ∥bL(p/2)(Rn+1×Rm+1) = 1 such that

MΩ,ϕ,ψ,,,i,jP1,P2(f)p2=Rn+1×Rm+1122μ122μSn1×Sm1Ω(u,v)Ai,Ω,ϕ(r,u,0,0)Bj,Ω,ψ(t,v,0,0)×f(x2(i+1)μru,xn+1ϕ(2(i+1)μr),y2(j+1)μtu,ym+1ψ(2(j+1)μt))dσ(u)dσ(v)2×drdtrtb(x¯,y¯)dx¯dy¯.

So, by Hölder’s inequality and Lemma 2.2, we conclude that

MΩ,ϕ,ψ,,,i,jP1,P2(f)p2CRn+1×Rm+1f(z¯,w¯)2122μ122μSn1×Sm1Ω(u,v)×b(z+2(i+1)μru,zn+1+ϕ(2(i+1)μr),w+2(j+1)μtu,wm+1+ψ(2(j+1)μt))dσ(u)dσ(v)drdtrtdz¯dw¯C1+μ2f2(p/2)NΩ,ϕ,ψ(b~)(p/2)Cp1+μ2fp2b~(p/2)Ω1,

where (z, w) = b(–z, –w). Thus,

MΩ,ϕ,ψ,,,i,jP1,P2(f)pCp1+μfp,

which when Combined with (3.4) gives that there is ϵ ∈ (0, 1) so that

MΩ,ϕ,ψ,,,i,jP1,P2(f)pCp2ϵ(i+j+2)8q1+μfp (3.5)

for all p ≥ 2. Therefore, by (3.3) and (3.5), we obtain

MΩ,ϕ,ψ,,P1,P2(f)pCp,q1+μfp (3.6)

for all p ≥ 2. Now, let us estimate the Lp-norm of MΩ,ϕ,ψ,0,0P1,P2 (f). Take Q1(x) = |α|d1 aα xα, and define MΩ,ϕ,ψ,0,0Q1,P2 (f) and MΩ,ϕ,ψ,0,0P1,P2,Q (f) by

MΩ,ϕ,ψ,0,0Q1,P2(f)(x¯,y¯)=0101GQ1,P2,ϕ,ψ,Ω(f)(x¯,y¯,r,t)2drdtrt1/2,

and

MΩ,ϕ,ψ,0,0P1,P2,Q(f)(x¯,y¯)=0101HP1,P2,ϕ,ψ,ΩQ(f)(x¯,y¯,r,t)2drdtrt1/2,

where

HP1,P2,ϕ,ψ,ΩQ(f)(x¯,y¯,r,t)=Sn1×Sm1eiP1(ru)+iP2(tv)eiQ1(ru)+iP2(tv)×f(xru,xn+1ϕ(r),ytv,ym+1ψ(t))Ω(u,v)dσ(u)dσ(v).

Thus, by Minkowski’s inequality, we deduce

MΩ,ϕ,ψ,0,0P1,P2(f)(x¯,y¯)MΩ,ϕ,ψ,0,0Q1,P2(f)(x¯,y¯)+MΩ,ϕ,ψ,0,0P1,P2,Q(f)(x¯,y¯). (3.7)

On one hand, since deg(Q1) ≤ d1, then by induction step we have

MΩ,ϕ,ψ,0,0Q1,P2(f)pCp,q1+μfp (3.8)

for all p ≥ 2. On the other hand, it is easy to check that

eiP1(ru)eiQ1(ru)r(d1+1)α=d1+1aαuαrd1+1.

So, by following a similar argument as in [18] and by Cauchy-Schwartz inequality, we have that

MΩ,ϕ,ψ,0,0P1,P2,Q(f)(x¯,y¯)C0101Sn1×Sm1eiP2(tv)f(xru,xn+1ϕ(r),ytv,ym+1ψ(t))×Ω(u,v)dσ(u)dσ(v)2eiP1(ru)eiQ1(ru)2drdtrt1/2C01rd1Sn101Sm1eiP2(tv)f(xru,xn+1ϕ(r),ytv,ym+1ψ(t))×Ω(u,v)dσ(v)2dttdσ(u)dr1/2CSn1j=12jd12j2j+101Sm1eiP2(tv)f(xru,xn+1ϕ(r),ytv,ym+1ψ(t))×Ω(u,v)dσ(v)2dttdrdσ(u)1/2Cj=12jd12j2j+1Sn1MP1,Ωn,ϕ(2)(fr(x¯,y¯))2dσ(u)dr1/2CNΩ,ψMP1,Ωn,ϕ(2)(fr(x¯,y¯)))21/2,

where ∘ denotes the composition of operators, 𝓝Ω,ψ f(x, y) = 𝓝Ω,ψ f(⋅, y)(x) is the maximal function defined as in Lemma 2.1; and MP1,Ωn,ϕ(2)(fr(x¯,y¯)=MP1,Ωn,ϕ(2)(fr(x¯,)(y¯) is the maximal operator in the one parameter setting defined as in [17, Eq. (1.2)]. Hence, by following a similar argument as in [18, p. 607] together with [17] and Lemma 2.1, we get

MΩ,ϕ,ψ,0,0P1,P2,Q(f)pCp,q1+μfp (3.9)

for all p ≥ 2. Therefore, by (3.7)-(3.9), we obtain that for all p ≥ 2,

MΩ,ϕ,ψ,0,0P1,P2(f)pCp,q1+μfp. (3.10)

In the same manner, we can derive that

MΩ,ϕ,ψ,,0P1,P2(f)pCp,q1+μfp (3.11)

and

MΩ,ϕ,ψ,0,P1,P2(f)pCp,q1+μfp (3.12)

for all p ≥ 2. Consequently, by (3.2), (3.6) and (3.10)-(3.12), we satisfy the inequality (1.3) for any polynomial P1 of degree d1 + 1 and for any polynomial P2 of degree d2. Similarly, we can show that the inequality (1.3) holds for any polynomial P2 of degree d2 + 1 and for any polynomial P1 of degree d1. This completes the proof of Theorem 1.1.

4 Further results

For γ > 1, define Δγ (R+ × R+) to be the set of all measurable functions h on R+ × R+ satisfying the condition

supR1,R2>01R1R20R10R2h(t,r)γdtdr1/γ<

and define Δ (R+ × R+) = L(R+ × R+). Also, for 1 ≤ γ < ∞, define 𝔏γ(R+ × R+) to be the set of all measurable functions h : R+ × R+R that satisfy the condition hLγ(R+×R+,drdtrt)=00h(r,t)γdrdtrt1/γ1 and define L(R+×R+)=L(R+×R+,drdtrt).

It is obvious that 𝔏γ(R+ × R+) ⊂ Δγ (R+ × R+) for 1 < γ < ∞, Δγ1(R+ × R+) ⊂ Δγ2 (R+ × R+) for γ1 > γ2 and Δ (R+ × R+) = 𝔏(R+ × R+).

The purpose of this section is to study the Lp boundedness of the singular inegral operator TΩ,h,ϕ,ψP1,P2 (f)(x, y) and the maximal operator MΩ,ϕ,ψP1,P2,(γ) under weaker conditions, where MΩ,ϕ,ψP1,P2,(γ) is defined, initially for f C0 (Rn+1 × Rm+1), by

MΩ,ϕ,ψP1,P2,(γ)(f)(x¯,y¯)=suphLγ(R+×R+)TΩ,h,ϕ,ψP1,P2(f)(x¯,y¯).

The first result of this section is the following:

Theorem 4.1

Suppose that ΩLq(Sn−1 × Sm−1), q > 1 and satisfy the conditions (1.1)-(1.2) withΩ1 ≤ 1. Assume that ϕ, ψ, μ, P1, and P2 are given as in Theorem 1.1. Then there exists a constant Cp,q > 0 such that

MΩ,ϕ,ψP1,P2,(γ)(f)pCp,q1+μ2/γfp (4.1)

for all γ′ ≤ p < ∞ with 1 < γ ≤ 2; and

MΩ,ϕ,ψP1,P2,(1)(f)Cf.

Proof

It is clear that if γ = 2, then we have MΩ,ϕ,ψP1,P2,(γ)=MΩ,ϕ,ψP1,P2. So, by Theorem 1.1, the inequality (4.1) holds for all p ≥ 2. However, if γ = 1; we assume that hL1(R+×R+,drdtrt) and fL(Rn+1 × Rm+1). Then for all (x, y) ∈ Rn+1 × Rm+1, we have

R+×R+h(r,t)GP1,P2,ϕ,ψ,Ω(f)(x¯,y¯,r,t)drdtrtCfh1.

Hence, by taking the supremum on both sides over all h with ∥h1 ≤ 1, we reach

MΩ,ϕ,ψP1,P2,(1)(f)(x¯,y¯)Cf

for almost every where (x, y) ∈ Rn+1 × Rm+1, which leads to

MΩ,ϕ,ψP1,P2,(1)(f)Cf. (4.3)

Finally, if 1 < γ ≤ 2. We follow a similar approach as in [15]. By duality, we get

MΩ,ϕ,ψP1,P2,(γ)(f)(x¯,y¯)=R+×R+GP1,P2,ϕ,ψ,Ω(f)(x¯,y¯,r,t))γdrdtrt1/γ,

which gives

MΩ,ϕ,ψP1,P2,(γ)(f)p=GP1,P2,ϕ,ψ,Ω(f)Lp(Lγ(R+×R+,drdtrt),Rn+1×Rm+1). (4.4)

Therefore, by applying the interpolation theorem for the Lebesgue mixed normed spaces to the inequalities (1.3) and (4.3), we directly obtain

MΩ,ϕ,ψP1,P2,(γ)(f)pCp,q(1+μ)2/γfp (4.5)

for γ′ ≤ p < ∞ with 1 < γ ≤ 2; and MΩ,ϕ,ψP1,P2,(1)(f)Cf. This completes the proof.□

It is worth mentioning that when ϕ(t) = ψ(t) = t and P1(u) = P2(v) = 0, Al-Qassem and Pan in [8] extended the results of Theorem 4.1. In fact, they established the Lp boundedness of MΩ,ϕ,ψP1,P2,(γ) provided that ΩL(log L)2/γ(Sn−1 × Sm−1) for γ′ ≤ p < ∞ with 1 < γ ≤ 2.

By the conclusion in Theorem 4.1 and applying an extrapolation argument (see [16, 19, 20]), we shall improve and extend the corresponding results in [4, 6, 8, 11, 13]. Precisely, we obtain the following:

Theorem 4.2

Suppose that P1, P2, ϕ, and ψ are given as in Theorem 1.1. Assume that ΩL(log L)2/γ(𝓢n−1 × Sm−1) ∪ Bq(0,2/γ1) (𝓢n−1 × Sm−1) with q > 1. Then MΩ,ϕ,ψP1,P2,(γ) (f) is bounded on Lp(Rn+1 × Rm+1) for γ′ ≤ p < ∞ with 1 < γ ≤ 2; and it is bounded on L(Rn+1 × Rm+1) for γ = 1.

Proof

The idea of proving Theorem 4.2 is taken form [17], which has its roots in [16] as well as in [19]. When ΩL(log L)2/γ(𝓢n−1 × Sm−1) with 1 < γ ≤ 2 and Ω satisfies the conditions (1.1)-(1.2), then Ω can be decomposed as a sum of functions in L2(𝓢n−1 × Sm−1) (see [21]). In fact, we have

Ω=k=0Ωk, (4.6)

where

Sn1Ωk(x,.)dσ(x)=Sm1Ωk(.,y)dσ(y)=0,Ω0L2(Sn1×Sm1),ΩkC24k,Ωk1C,

and

i=1k2/γΩk1CΩL(logL)2/γ(Sn1×Sm1)fork=0,1,2,.

Hence, it is easy to see that

MΩ,ϕ,ψP1,P2,(γ)(f)(x¯,y¯)MΩ0,ϕ,ψP1,P2,(γ)(f)(x¯,y¯)+k=1Ωk1MΩk,ϕ,ψP1,P2,(γ)(f)(x¯,y¯) (4.7)

and

1+log2/γ(e+Ωk)1+log2/γ(e+C24k)Ck2/γ. (4.8)

As Ω0L2(𝓢n−1 × 𝓢m−1), then by Thorem 4.1 we get

MΩ0,ϕ,ψP1,P2,(γ)pCp1+log2/γ(e+Ω02)fp (4.9)

for γ′ ≤ p < ∞. Therefore, by Minkoswski’s inequality and (4.7)-(4.9), we obtain that

MΩ,ϕ,ψP1,P2,(γ)(f)pMΩ0,ϕ,ψP1,P2,(γ)(f)p+k=1Ωk1MΩk,ϕ,ψP1,P2,(γ)(f)pCp1+k=1Ωk1k2/γfpCpΩL(logL)2/γ(Sn1×Sm1)fpCpfp.

However, when Ω Bq(0,2/γ1) 𝓢(𝓢n−1 × 𝓢m−1) with q > 1, 1 < γ ≤ 2 and Ω satisfies the conditions (1.1)-(1.2), then Ω can be written as

Ω=μ=1cμbμ, (4.10)

where each cμ is a complex number, each bμ is a q-block supported in an interval Iμ on (𝓢n−1 × 𝓢m−1) and

Mq(0,2/γ1)({cμ})=μ=1cμ1+log2/γ(Iμ1)<.

For each μ, define the blocklike function μ by

bμ~(x,y)=bμ(x,y)Sn1bμ(u,y)dσ(u)Sm1bμ(x,v)dσ(v)+Sn1×Sm1bμ(u,v)dσ(u)dσ(v). (4.11)

It is clear that each μ(x, y) satisfies the following:

Sn1bμ~u,dσu=Sm1bμ~,vdσv=0, (4.12)
bμ~qCI1/q,andbμ~1C. (4.13)

Without loss of generality, we may assume that ∥Iμ∥ < 1. Therefore, by Minkoswski’s inequality, Theorem 4.1 and (4.10)-(4.13), we obtain that

MΩ,ϕ,ψP1,P2,(γ)(f)pμ=1cμMbμ~,ϕ,ψP1,P2,(γ)(f)pCp,qμ=1cμ1+log2/γ(e+Iμ1)fpCp,qfp

for all pγ′.□

We point out that under the assumptions Ω belongs to the block space Bq(0,1) (𝓢n−1 × Sm−1), hΔγ (R+ × R+) for some q, γ > 1, and when ϕ, ψ are C2([0, ∞)), convex increasing functions with ϕ(0) = ψ(0) = 0, the author of [22] proved that for every p satisfying |1/p – 1/2| < min {1/2, 1/γ}, there exists a constant Cp such that

TΩ,h,ϕ,ψfpCpfp

for every fLp(Rn+1 × Rm+1). By this result, it is clear that the range of p is the full range (1, ∞) whenever h ∈ 𝔏γ(R+ × R+) with γ ≥ 2. But what is about the Lp boundedness of TΩ,h,ϕ,ψ when h ∈ 𝔏γ(R+ × R+) for 1 < γ < 2. We shall obtain an answer to this question in the affirmative as described in the following theorem.

Theorem 4.3

Assume that ΩL(log L)2/γ(𝓢n−1 × Sm−1) ∪ Bq(0,2/γ1) (𝓢n−1 × Sm−1), q > 1, and satisfying the conditions (1.1)-(1.2). Let h ∈ 𝔏γ(R+ × R+) for some 1 < γ ≤ 2, and let ϕ, ψ be given as in Theorem 1.1. Then the singular integral operator TΩ,h,ϕ,ψP1,P2 (f)(x, y) is bounded on Lp(Rn+1 × Rm+1) for all 1 < p < ∞.

Proof

As a direct consequence of Theorem 4.2 and the statement that

TΩ,h,ϕ,ψP1,P2(f)(x¯,y¯)hLγ(R+×R+,drdtrt)MΩ,ϕ,ψP1,P2,(γ)(f)(x¯,y¯), (4.14)

we acheive that TΩ,h,ϕ,ψP1,P2 is bounded on Lp(Rn+1 × Rm+1) for γ′ ≤ p < ∞ with 1 < γ ≤ 2. Moreover, by a standard duality argument, we can show that TΩ,h,ϕ,ψP1,P2 is bounded on Lp for 1 < pγ with 1 < γ ≤ 2. So, if γ = 2, then we are done. However, if 1 < γ < 2, then we apply the real interpolation theorem to acquire the Lp boundedness of TΩ,h,ϕ,ψP1,P2 for (γ < p < γ′). This completes the proof. □

Acknowledgement

The authors would like to thank the referees for their valuable comments and suggestions.

References

[1] Fefferman R., Singular integrals on product domains, Bull. Amer. Math. Soc., 1981, 4, 195–201.10.1090/S0273-0979-1981-14883-7Search in Google Scholar

[2] Fefferman R., Stein M., Singular integrals on product spaces, Adv. Math., 1982, 45, 117–143.10.1016/S0001-8708(82)80001-7Search in Google Scholar

[3] Al-Salman A., Al-Qassem H., Pan Y., Singular integrals on product domains, Indiana Univ. Math. J., 2006, 55(1), 369–387.10.2298/FIL0418001ASearch in Google Scholar

[4] Al-Salman A., Flat singular integrals on product domains, Filomat (Nis), 2004, 18, 1–13.10.2298/FIL0418001ASearch in Google Scholar

[5] Duoandikoetxea J., Multiple singular integrals and maximal functions along hypersurfaces, Ann. Inst. Fourier (Grenoble), 1986, 36, 185–206.10.5802/aif.1073Search in Google Scholar

[6] Al-Salman A., Maximal functions associated to surfaces of revolution on product domains, J. Math. Anal. Appl., 2009, 351, 43–56.10.1016/j.jmaa.2008.09.050Search in Google Scholar

[7] Ding Y., A note on a class of rough maximal operators on product domains, J. Math. Anal. Appl., 1999, 232, 222–228.10.1006/jmaa.1998.6232Search in Google Scholar

[8] Al-Qassem H., Pan Y., A class of maximal operators related to rough singular integrals on product spaces, J. Int. Eq. Appl., 2005, 17(4), 331–356.10.1216/jiea/1181075347Search in Google Scholar

[9] Al-Salman A., Maximal operators with rough kernels on product domains, J. Math. Anal. Appl., 2005, 311, 338–351.10.1016/j.jmaa.2005.02.048Search in Google Scholar

[10] Al-Qassem H., Lp estimates for a rough maximal operator on product spaces, J. Korean Math. Soc., 2005, 42(3), 405–434.10.4134/JKMS.2005.42.3.405Search in Google Scholar

[11] Al-Dolat M., Ali M., Jaradat I., Al-Zoubi K., On the boundedness of a certain class of maximal functions on product spaces and extrapolation, Anal. Math. Phys., 2018, 10.1007/s13324-018-0208-x.Search in Google Scholar

[12] Al-Qassem H., Cheng L., Pan Y., On the boundedness of a class of rough maximal operators on product spaces, Hokkaido Math. J., 2011, 40(1), 1–32.10.14492/hokmj/1300108396Search in Google Scholar

[13] Al-Salman A., Maximal functions along surfaces on product domains, Anal. Math., 2008, 34, 163–175.10.1007/s10476-008-0301-8Search in Google Scholar

[14] Al-Qassem H., Pan Y., Singular integrals along surfaces of revolution with rough kernels, CSUT. J. Math., 2003, 39(1), 55–70.10.55937/sut/1059541339Search in Google Scholar

[15] Al-Qassem H., On the boundedness of maximal operators and singular operators with kernels in L(logL)α (Sn−1), J. Ineq. Appl., 2006, Article ID 96732.10.1155/JIA/2006/96732Search in Google Scholar

[16] Al-Salman A., A unifying approach for certain class of maximal functions, J. Ineq. Appl., 2006, Article ID 56272, https://doi.org/10.1186/s13660-018-1900-y.10.1155/JIA/2006/56272Search in Google Scholar

[17] Ali M., Al-Mohammed O., Boundedness of a class of rough maximal functions, J. Ineq. Appl., 2018, Article number: 305.10.1186/s13660-018-1900-ySearch in Google Scholar PubMed PubMed Central

[18] Al-Qassem H., Pan Y., Lp boundedness for singular integrals with rough kernels on product domains, Hokkaido Math. J., 2002, 31(1), 555–613.10.14492/hokmj/1350911903Search in Google Scholar

[19] Al-Qassem H., Pan Y., On certain estimates for Marcinkiewicz integrals and extrapolation, Collec. Math., 2009, 60(2), 123–145.10.1007/BF03191206Search in Google Scholar

[20] Sato S., Estimates for singular integrals and extrapolation, arXiv:0704.1537v1.10.4064/sm192-3-2Search in Google Scholar

[21] Al-Salman A., Pan Y., Singular integrals with rough kernels in L log+ L (Sn−1), J. London Math. Soc., 2002, 66(2), 153–174.10.1112/S0024610702003241Search in Google Scholar

[22] Al-Qassem H., Singular integrals along surfaces on product domains, Anal. Theory and Appl., 2004, 20(2), 99–112.10.1007/BF02901436Search in Google Scholar

Received: 2018-06-10
Accepted: 2019-10-18
Published Online: 2019-11-19

© 2019 Mohammed Ali and Musa Reyyashi, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 Public License.

Articles in the same Issue

  1. Regular Articles
  2. On the Gevrey ultradifferentiability of weak solutions of an abstract evolution equation with a scalar type spectral operator of orders less than one
  3. Centralizers of automorphisms permuting free generators
  4. Extreme points and support points of conformal mappings
  5. Arithmetical properties of double Möbius-Bernoulli numbers
  6. The product of quasi-ideal refined generalised quasi-adequate transversals
  7. Characterizations of the Solution Sets of Generalized Convex Fuzzy Optimization Problem
  8. Augmented, free and tensor generalized digroups
  9. Time-dependent attractor of wave equations with nonlinear damping and linear memory
  10. A new smoothing method for solving nonlinear complementarity problems
  11. Almost periodic solution of a discrete competitive system with delays and feedback controls
  12. On a problem of Hasse and Ramachandra
  13. Hopf bifurcation and stability in a Beddington-DeAngelis predator-prey model with stage structure for predator and time delay incorporating prey refuge
  14. A note on the formulas for the Drazin inverse of the sum of two matrices
  15. Completeness theorem for probability models with finitely many valued measure
  16. Periodic solution for ϕ-Laplacian neutral differential equation
  17. Asymptotic orbital shadowing property for diffeomorphisms
  18. Modular equations of a continued fraction of order six
  19. Solutions with concentration and cavitation to the Riemann problem for the isentropic relativistic Euler system for the extended Chaplygin gas
  20. Stability Problems and Analytical Integration for the Clebsch’s System
  21. Topological Indices of Para-line Graphs of V-Phenylenic Nanostructures
  22. On split Lie color triple systems
  23. Triangular Surface Patch Based on Bivariate Meyer-König-Zeller Operator
  24. Generators for maximal subgroups of Conway group Co1
  25. Positivity preserving operator splitting nonstandard finite difference methods for SEIR reaction diffusion model
  26. Characterizations of Convex spaces and Anti-matroids via Derived Operators
  27. On Partitions and Arf Semigroups
  28. Arithmetic properties for Andrews’ (48,6)- and (48,18)-singular overpartitions
  29. A concise proof to the spectral and nuclear norm bounds through tensor partitions
  30. A categorical approach to abstract convex spaces and interval spaces
  31. Dynamics of two-species delayed competitive stage-structured model described by differential-difference equations
  32. Parity results for broken 11-diamond partitions
  33. A new fourth power mean of two-term exponential sums
  34. The new operations on complete ideals
  35. Soft covering based rough graphs and corresponding decision making
  36. Complete convergence for arrays of ratios of order statistics
  37. Sufficient and necessary conditions of convergence for ρ͠ mixing random variables
  38. Attractors of dynamical systems in locally compact spaces
  39. Random attractors for stochastic retarded strongly damped wave equations with additive noise on bounded domains
  40. Statistical approximation properties of λ-Bernstein operators based on q-integers
  41. An investigation of fractional Bagley-Torvik equation
  42. Pentavalent arc-transitive Cayley graphs on Frobenius groups with soluble vertex stabilizer
  43. On the hybrid power mean of two kind different trigonometric sums
  44. Embedding of Supplementary Results in Strong EMT Valuations and Strength
  45. On Diophantine approximation by unlike powers of primes
  46. A General Version of the Nullstellensatz for Arbitrary Fields
  47. A new representation of α-openness, α-continuity, α-irresoluteness, and α-compactness in L-fuzzy pretopological spaces
  48. Random Polygons and Estimations of π
  49. The optimal pebbling of spindle graphs
  50. MBJ-neutrosophic ideals of BCK/BCI-algebras
  51. A note on the structure of a finite group G having a subgroup H maximal in 〈H, Hg
  52. A fuzzy multi-objective linear programming with interval-typed triangular fuzzy numbers
  53. Variational-like inequalities for n-dimensional fuzzy-vector-valued functions and fuzzy optimization
  54. Stability property of the prey free equilibrium point
  55. Rayleigh-Ritz Majorization Error Bounds for the Linear Response Eigenvalue Problem
  56. Hyper-Wiener indices of polyphenyl chains and polyphenyl spiders
  57. Razumikhin-type theorem on time-changed stochastic functional differential equations with Markovian switching
  58. Fixed Points of Meromorphic Functions and Their Higher Order Differences and Shifts
  59. Properties and Inference for a New Class of Generalized Rayleigh Distributions with an Application
  60. Nonfragile observer-based guaranteed cost finite-time control of discrete-time positive impulsive switched systems
  61. Empirical likelihood confidence regions of the parameters in a partially single-index varying-coefficient model
  62. Algebraic loop structures on algebra comultiplications
  63. Two weight estimates for a class of (p, q) type sublinear operators and their commutators
  64. Dynamic of a nonautonomous two-species impulsive competitive system with infinite delays
  65. 2-closures of primitive permutation groups of holomorph type
  66. Monotonicity properties and inequalities related to generalized Grötzsch ring functions
  67. Variation inequalities related to Schrödinger operators on weighted Morrey spaces
  68. Research on cooperation strategy between government and green supply chain based on differential game
  69. Extinction of a two species competitive stage-structured system with the effect of toxic substance and harvesting
  70. *-Ricci soliton on (κ, μ)′-almost Kenmotsu manifolds
  71. Some improved bounds on two energy-like invariants of some derived graphs
  72. Pricing under dynamic risk measures
  73. Finite groups with star-free noncyclic graphs
  74. A degree approach to relationship among fuzzy convex structures, fuzzy closure systems and fuzzy Alexandrov topologies
  75. S-shaped connected component of radial positive solutions for a prescribed mean curvature problem in an annular domain
  76. On Diophantine equations involving Lucas sequences
  77. A new way to represent functions as series
  78. Stability and Hopf bifurcation periodic orbits in delay coupled Lotka-Volterra ring system
  79. Some remarks on a pair of seemingly unrelated regression models
  80. Lyapunov stable homoclinic classes for smooth vector fields
  81. Stabilizers in EQ-algebras
  82. The properties of solutions for several types of Painlevé equations concerning fixed-points, zeros and poles
  83. Spectrum perturbations of compact operators in a Banach space
  84. The non-commuting graph of a non-central hypergroup
  85. Lie symmetry analysis and conservation law for the equation arising from higher order Broer-Kaup equation
  86. Positive solutions of the discrete Dirichlet problem involving the mean curvature operator
  87. Dislocated quasi cone b-metric space over Banach algebra and contraction principles with application to functional equations
  88. On the Gevrey ultradifferentiability of weak solutions of an abstract evolution equation with a scalar type spectral operator on the open semi-axis
  89. Differential polynomials of L-functions with truncated shared values
  90. Exclusion sets in the S-type eigenvalue localization sets for tensors
  91. Continuous linear operators on Orlicz-Bochner spaces
  92. Non-trivial solutions for Schrödinger-Poisson systems involving critical nonlocal term and potential vanishing at infinity
  93. Characterizations of Benson proper efficiency of set-valued optimization in real linear spaces
  94. A quantitative obstruction to collapsing surfaces
  95. Dynamic behaviors of a Lotka-Volterra type predator-prey system with Allee effect on the predator species and density dependent birth rate on the prey species
  96. Coexistence for a kind of stochastic three-species competitive models
  97. Algebraic and qualitative remarks about the family yy′ = (αxm+k–1 + βxmk–1)y + γx2m–2k–1
  98. On the two-term exponential sums and character sums of polynomials
  99. F-biharmonic maps into general Riemannian manifolds
  100. Embeddings of harmonic mixed norm spaces on smoothly bounded domains in ℝn
  101. Asymptotic behavior for non-autonomous stochastic plate equation on unbounded domains
  102. Power graphs and exchange property for resolving sets
  103. On nearly Hurewicz spaces
  104. Least eigenvalue of the connected graphs whose complements are cacti
  105. Determinants of two kinds of matrices whose elements involve sine functions
  106. A characterization of translational hulls of a strongly right type B semigroup
  107. Common fixed point results for two families of multivalued A–dominated contractive mappings on closed ball with applications
  108. Lp estimates for maximal functions along surfaces of revolution on product spaces
  109. Path-induced closure operators on graphs for defining digital Jordan surfaces
  110. Irreducible modules with highest weight vectors over modular Witt and special Lie superalgebras
  111. Existence of periodic solutions with prescribed minimal period of a 2nth-order discrete system
  112. Injective hulls of many-sorted ordered algebras
  113. Random uniform exponential attractor for stochastic non-autonomous reaction-diffusion equation with multiplicative noise in ℝ3
  114. Global properties of virus dynamics with B-cell impairment
  115. The monotonicity of ratios involving arc tangent function with applications
  116. A family of Cantorvals
  117. An asymptotic property of branching-type overloaded polling networks
  118. Almost periodic solutions of a commensalism system with Michaelis-Menten type harvesting on time scales
  119. Explicit order 3/2 Runge-Kutta method for numerical solutions of stochastic differential equations by using Itô-Taylor expansion
  120. L-fuzzy ideals and L-fuzzy subalgebras of Novikov algebras
  121. L-topological-convex spaces generated by L-convex bases
  122. An optimal fourth-order family of modified Cauchy methods for finding solutions of nonlinear equations and their dynamical behavior
  123. New error bounds for linear complementarity problems of Σ-SDD matrices and SB-matrices
  124. Hankel determinant of order three for familiar subsets of analytic functions related with sine function
  125. On some automorphic properties of Galois traces of class invariants from generalized Weber functions of level 5
  126. Results on existence for generalized nD Navier-Stokes equations
  127. Regular Banach space net and abstract-valued Orlicz space of range-varying type
  128. Some properties of pre-quasi operator ideal of type generalized Cesáro sequence space defined by weighted means
  129. On a new convergence in topological spaces
  130. On a fixed point theorem with application to functional equations
  131. Coupled system of a fractional order differential equations with weighted initial conditions
  132. Rough quotient in topological rough sets
  133. Split Hausdorff internal topologies on posets
  134. A preconditioned AOR iterative scheme for systems of linear equations with L-matrics
  135. New handy and accurate approximation for the Gaussian integrals with applications to science and engineering
  136. Special Issue on Graph Theory (GWGT 2019)
  137. The general position problem and strong resolving graphs
  138. Connected domination game played on Cartesian products
  139. On minimum algebraic connectivity of graphs whose complements are bicyclic
  140. A novel method to construct NSSD molecular graphs
Downloaded on 24.12.2025 from https://www.degruyterbrill.com/document/doi/10.1515/math-2019-0118/html
Scroll to top button