亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        THE EXISTENCE OF A NONTRIVIAL WEAK SOLUTION TO A DOUBLE CRITICAL PROBLEM INVOLVING A FRACTOL LOL

        2021-01-07 06:44:22GongbaoLI李工寶TaoYANG楊濤
        關(guān)鍵詞:楊濤

        Gongbao LI(李工寶)? Tao YANG (楊濤)

        Hubei Key Laboratory of Mathematical Sciences and School of Mathematics and Statistics, Central China Normal University, Wuhan 430079, China E-mail : ligb@mail.ccnu.edu.cn; yangt@mails.ccnu.edu.cn

        1 Introduction

        In this paper,we consider the existence of nontrivial weak solutions to a double critical problem involving a fractional Laplacian with a Hardy term:

        The rest of the paper is organized as follows:in Section 2,we give some preliminaries.In Section 3,we introduce the weighted Morrey space and establish improved Sobolev inequalities,i.e.,we prove Proposition 1.3 and Corollary 1.4.In Section 4,we solve the minimization problems(1.12)–(1.13).In Section 5,we prove Theorem 1.1.

        NotationWe use→and?to denote the strong and weak convergence in the corresponding spaces respectively.Write“Palais-Smale”as(PS)for short.N={1,2,···}is the set of natural numbers.R and C denote the sets of real and complex numbers respectively.By saying that a function is“measurable”,we always mean that the function is“Lebesgue”measurable.“∧”denotes the Fourier transform and“∨”denotes the inverse Fourier transform.Generic fixed and numerical constants will be denoted byC(with subscript in some case),and they will be allowed to vary within a single line or formula.

        2 Preliminaries

        In this section,we give some preliminary results.

        Lemma 2.1(fractional Hardy inequality:Formula(2.1)in[26])Lets∈(0,1)andn>2s.Then we have

        3 Proof of Proposition 1.3 and Corollary 1.4

        In this section,we give some basic properties of a weighted Morrey space and then prove Proposition 1.3 and Corollary 1.4.

        The Morrey spaces were introduced by Morrey in 1938[30]to investigate the local behavior of solutions to some partial differential equations.Nowadays the Morrey spaces are extended to more general cases(see[1,31,32]).Lettingp∈[1,+∞)andγ∈(0,n),the usual homogeneous Morrey space

        4 Solving the Minimization Problems(1.12)–(1.13)

        Thus we have that?v 6≡0.The rest is the sameas the proof of Proposition 4.1-(1),so Proposition 4.1-(2)holds.

        (3)The proof is similar to Proposition 4.1-(1).Although Proposition 4.1-(3)has been proved in[2],the strategy we adopted in Proposition 4.1-(1)is more direct and effective.

        (4) Imitate the proof of Proposition 4.1-(2). ?

        Remark4.3To prove Proposition 4.1-(2),firstly we choose aminimizing sequence{uk}of Sμ(n,s,γ,0),then we prove that vk=|uk|?is also aminimizing sequence of Sμ(n,s,γ,0),since 0≤γ<γH.Since vkis radial symmetric and decreasing,we can easily eliminate vanishing.If α>0 and 0≤γ<γH,the same strategy can be applied to the proof of Proposition 4.1-(1).W hen it comes to α>0 and γ<0,we fail to prove that vk=|uk|?is a minimizing sequence of Sμ(n,s,γ,α),but(1.9)and(1.10)are very effective in this situation.

        5 Proof of Theorem 1.1

        We shall now use the minimizers of Sμ(n,s,γ,α)and Λ(n,s,γ,β)obtained in Proposition 4.1 to prove the existence of a nontrivial weak solution for equation(1.1).Recall that the energy functional associated to(1.1)is

        Note that a nontrivial critical point of I is a nontrivial weak solution to equation(1.1).

        Lemma5.1(Mountain Pass Lemma,[37])Let(E,||·||)be a Banach space and let I∈C1(E,R)such that the following conditions are satisfied:

        (1)I(0)=0;

        (2)There exist ρ,r>0 such that I(u)≥ρ for all u∈E with||u||=r;

        Hencevis a nontrivial weak solution of(1.1).

        (II)If is the case thats∈(0,1),0≤α,β<2s

        Case(i)α=0<β<2sorβ=0<α<2s.

        In this case,the embeddings(1.9)and inequality(1.10)are still effective.Sinceα>0 orβ>0,we get a nontrivial weak solution to(1.1),as above,by using(1.9),(1.10)and Proposition 5.3.

        Case(ii)α=0 andβ=0.

        In this case,(1.9)and(1.10)are useless.Since the limit equation for(1.1)is

        by using the Nehari manifold method in[5],we can also get a non-trivial weak solution to(1.1),if 0≤γ<γH.

        Remark 5.4The method we adopt to prove Theorem 1.1 can be applied to prove a similar existence result for thep-Laplace type problem involving double critical exponents.To go further,we consider

        We say thatu∈D1,p(Rn)is a weak solution to(5.12)if

        for anyφ∈D1,p(Rn).The following main result holds:

        Theorem 5.5The problem(5.12)possesses at least a nontrivial weak solution provided that either

        (I)n≥2,p∈(1,n),0<α1,α2

        (II)n≥2,p∈(1,n),0≤α1,α2

        猜你喜歡
        楊濤
        目擊
        傳承好紅巖精神 走好新時(shí)代長(zhǎng)征路
        九龍坡:一江繞半島 藝術(shù)煥新生
        Distribution of charged lunar dust in the south polar region of the moon
        Quantum reflection of a Bose–Einstein condensate with a dark soliton from a step potential?
        Effect of Sb composition on the band alignment of InAs/GaAsSb quantum dots*
        The Role of Teacher , Learner and Material in Foreign Language Teaching and Learning
        Changes in fi sh diversity and community structure in the central and southern Yellow Sea from 2003 to 2015*
        訣別詩(shī)
        幸福夢(mèng)
        国产av在线观看91| 亚洲av日韩av无码av| 日韩精品久久久一区| 水蜜桃在线视频在线观看| 国产av剧情久久精品久久| 黑人巨茎大战俄罗斯美女| 亚洲av成人一区二区三区在线观看| 亚洲欧洲日产国码久在线| 国产成人综合久久大片| 97人伦影院a级毛片| 内射精品无码中文字幕| 青春草在线视频精品| 日本大片一区二区三区| 国产做无码视频在线观看| 亚洲av日韩av不卡在线观看| 草莓视频在线观看无码免费| av在线入口一区二区| 色先锋av影音先锋在线| 亚洲日本va中文字幕久久| 国产一级黄色av影片| 蜜桃tv在线免费观看| 性欧美videofree高清精品| 午夜亚洲国产理论片亚洲2020| 国产高清自产拍av在线| 国产精品久久国产精麻豆99网站 | 国产亚洲自拍日本亚洲| 亚洲人成网站18禁止久久影院| 97福利视频| 一本色道久久88加勒比—综合| 亚洲av无码国产精品色午夜字幕| 国产又黄又大又粗视频| 成年女人18毛片毛片免费| 草逼动态图视频免费观看网站| 无码av无码天堂资源网| 在线视频中文字幕乱人伦| 久久精品亚洲热综合一本色婷婷| 婷婷丁香五月激情综合| 93精91精品国产综合久久香蕉| 久久国产精品av在线观看| 蜜桃视频插满18在线观看| 亚洲av片不卡无码久久|