999精品在线视频,手机成人午夜在线视频,久久不卡国产精品无码,中日无码在线观看,成人av手机在线观看,日韩精品亚洲一区中文字幕,亚洲av无码人妻,四虎国产在线观看 ?

R2n 中P 循環對稱緊星型超曲面上P 循環對稱閉特征的多重性

2022-07-01 23:37:02李洋洋劉會
數學理論與應用 2022年2期

李洋洋 劉會

(1.四川大學附屬中學,成都,610044?2.武漢大學數學與統計學院,武漢,430072)

1 Introduction

The study on closed characteristics in the global sense started in 1978,when the existence of at least one closed characteristic was first established on any Σ∈Hst(2n)by Rabinowitz in[32]and on any Σ∈Hcon(2n)by Weinstein in[38]independently. Since then the existence of multiple closed characteristics on Σ∈Hcon(2n) has been deeply studied by many mathematicians, for example, studies in [10, 11,18,20,29,30,31,35,37,39]for convex hypersurfaces. For star shaped hypersurfaces, in[4]and[16],#T(Σ)≥nfor Σ∈Hst(2n) was proved under some pinching conditions. In [36], Viterbo proved a generic existence result for infinitely many closed characteristics on star shaped hypersurfaces. In [17],Hu and Long proved that#T(Σ)≥2 for Σ∈Hst(2n)on which all the closed characteristics and their iterates are non degenerate. In [19], Hofer, Wysocki, and Zehnder proved any non degenerate compact star shaped hypersurface has either two or infinitely closed characteristics, provided that all stable and unstable manifolds of the hyperbolic closed characteristics intersect transversally. In 2016,#T(Σ)≥2 was first proved for every Σ∈Hst(4)by Cristofaro Gardiner and Hutchings in[5]without any pinching or non degeneracy conditions. Different proofs of this result can also be found in[12],[15]and[22]. For the recent progresses on closed characteristics on compact star shaped hypersurfaces,one can also refer to[8,9,13,14,23,24]and the references therein.

It is very interesting to consider closed characteristics on hypersurfaces with special symmetries.Note that there are many studies about closed characteristics on compact convexPcyclic symmetric hypersurfaces,one can refer to[6,7,21,26,27,40]. In this paper,we study the multiplicity ofPcyclic symmetric closed characteristics on compact star shapedPcyclic symmetric hypersurfaces under a pinching condition. Letk ≥2 be a positive integer andP=, where

Theorem 1.1There holds#TP(Σ)≥1 for any Σ∈(2n).

Letn(y)be the unit outward normal vector of Σ atyandd(y):=n(y)·y,i.e.,the distance between the origin of R2nand the tangent hyperplane to Σ aty. Thend(y)> 0 for ally ∈Σ since Σ is strictly star shaped. Letd=min{d(y):y ∈Σ},R=max{|y|:y ∈Σ}andr=min{|y|:y ∈Σ}.

Theorem 1.2AssumeR2< (k+ 1)rdfor some Σ∈(2n). Then there exist at leastngeometrically distinctPcyclic symmetric closed characteristics on Σ.

Remark 1.1LetP=?I2nandk= 2,then Theorems 1.1–1.2 are the main results of[16]. Thus our results are slightly extensions of those of[16]. We should emphasize that we follow the ideas of[16].Compared with[11]and[26],the pinching condition of Theorem 1.2 is slightly broader,and it’s used to guarantee the closed characteristics we obtained are prime and geometrically distinct. The topic aboutPcyclic symmetric closed characteristics on compact star shapedPcyclic symmetric hypersurfaces are interesting, one can also refer to [1], [25]and [28]for the recent studies on convexPcyclic symmetric hypersurfaces. Note that our Theorem 1.2 extends Theorem 1.21 of [1] to the star shaped case. Our Theorem 1.2 also has potential applications to celestial mechanics,for example in[34],the H′enon Heiles Hamiltonian energy level presents Z3symmetry and the Hamiltonian energy level presents Z4symmetry in Hill’s lunar problem.

2 Proof of Theorem 1.2

We shall prove Theorem 1.2. Theorem 1.1 will be an easy consequence.

LetH(x)=j2(x),?x ∈R2n,wherej:R2n →R is the gauge function of Σ,that is,j(λx)=λforx ∈Σ andλ ≥0. Then Σ=H?1(1)andH(Px)=H(x)since Σ∈(2n). In the following,we will find distinct solutions of the Hamiltonian system

lying on Σ satisfying thatz(t+τ)=Pz(t)for someτ>0.

SetE=(R/(kπ)Z,R2n). Foranysmoothu∈E,we consider theactionintegralf(u) =uJu˙.Here we notethatJisminusof thatin[16].Then wehavef ∈C1(E,R).Define the bounded self adjoint linear operatorL:E →Eby:=f′(u)v,?u,v ∈E,where<·,·>is the scalar product inE. By direct calculation,we have

Noticing that

and

we obtain

Lemma 2.1Ifu ∈Sis a critical point off|S,withf(u)>0,then there exists aλ>0,such that

Obviously,there exists aλ,such that ˙u=λJH(u). The positivity ofλeasily follows(see(2.5)). In the following we shall show that=H′(u)w, ?w ∈E.

Note thatH(Pu) =H(u). Differentiatinguon the two sides,we haveH(Pu) =PH(u). ThenH′(un(t+π))=H′(Pun(t))=PH′(un(t)),sinceun ∈E1. ThenH′(un)∈E1,which implies

From(2.2)and(2.3),=H′(u)w,?w ∈E. The Lemma is proved.

Ifusatisfies(2.1),thenu?(t)≡u()is a solution ofu˙ =JH′(u)of periodkπλ,andu?(t+λπ) =P?u(t). Ifuhas minimal periodkπ,then ?u(t)has minimal periodkπλ.

It is easy to know that the existence ofngeometrically distinctPcyclic symmetric closed characteristics on Σ is equivalent to the existence ofncritical points off|S, say,u1,u2,··· ,un,such thatf(ui)>0,ui(t)?=uj(t+θ)fori ?=j,θ ∈R/(kπZ)anduihas minimal periodkπ.

LetZ={u ∈S|f′|S(u)= 0,f(u)> 0}. If we consider the functionfand the manifoldSin the spaceE,then we have:

Lemma 2.2Ifu ∈Z,thenf(u)≥.

Recall thatH(αz)=α2H(z),by differentiatingαon the two sides,then we have

Ifu ∈Z,we can know there exists aλ>0,such that ˙u=λJH′(u)from lemma 2.1. Then

Hence,from(2.5),we have

The Lemma is proved.

If we consider the functionfand the manifoldSin the spaceE1,then we have a stronger result:

Lemma 2.3Ifu ∈Z,thenf(u)≥.

The Lemma is proved.

The following lemma is a consequence of Lemma 2.3.

Lemma 2.4Ifu ∈Zandf(u)<πdr, thenucan not be any multiple iteration of someu1∈Z,which implies thatuhas minimal periodkπ.

If 2≤m ≤k, we can multiply the left and right sides of (2.6) byPk?m. Then we getu1(t) =Pk?m+1u1(t)by usingPk=I2n. Thus,there exists anl ∈N such thatk ?m+1 =lk. However,if 2≤m ≤k,we have 1≤lk ≤k ?1,which is impossible.

Ifm ≥k+1,we have

It is impossible, becausef(u1)>by Lemma 2.3. Souhas minimal periodkπ. The Lemma is proved.

Now, we define a pseudo index (see [2], [3]) and make use of the invariance offandSthrough theS1actionS1×E1→E1: (θ,u(t))→u(t+θ),u ∈E1,θ ∈S1, whereS1= R/(kπ)Z. Letφm= ek2mtJam+ek2(?m+2?k)tJa?m+2?k, whereal ∈R2nforl=m,?m+2?k,σm=f(φm),m ∈N,m ≡1(modk). Let

Obviously,E1=is the orthogonal decomposition ofE1with regard to the functionalf(see[33]). LetGbe aC1manifold ofE1,radially diffeomorphic to the unit sphere ofE1,invariant under theS1action. LetU:E1→E1be a self adjoint linear equivariant isomorphism such thatU()?.Denote by∪the set of these isomorphisms. Leth:G →Gbe an equivariant homeomorphism satisfying that there exist a continuous mapg:G →R+and aU ∈∪such thath ?gU|Gis compact. Denote by ΓGthe family of all suchh,which is a group. LetVbe the family of closed,S1invariant subsets ofE1.ForA ?G,A ∈V,the pseudo index is defined as

whereiis theS1index introduced by Benci[3]. Recall the following results:

Proposition 2.1AssumeG1andG2areC1manifolds radially diffeomorphic to a sphere ofE1and invariant under theS1action. Letp:G1→G2be the radical projection fromG1toG2. Then

Proposition 2.2LetHh ?E1be a 2hdimensional invariant subspace andHh ⊕W=E1. Then forA ?G,A ∈V,

Supposef|Gsatisfies the Palais Smale condition. LetZc={u ∈G|f′|G(u) = 0,f(u) =c}. We define

Thenckis a critical value off|G. Moreover ifc=ck+1=···=ck+p,theni(Zc)≥p. It is the famous Minimax principle. And it is known thatf|Ssatisfies the Palais Smale condition,see[4]and[16].

Let us considerSR={u ∈E1||u|2=R2},which is aC1manifold radially deffeomorphic to a sphere ofE1, invariant under theS1action.f|SRverifies the Palais Smale condition. So we can apply the Minimax Principle toSR. Let us denote bya1,a2,··· ,anthe firstncritical values off|SRof minimax type. We have the following lemma.

Lemma 2.5Forf|SRwe havea1=···=an=.

By Proposition 2.6,we havei?(An)=n. We can immediately know that

The Lemma is proved.

Now,we can prove Theorem 1.2.

Let

We know thatc1,c2,··· ,cnare critical values off|S,andcj ≥. For everyu ∈SR,there exists a uniqueλsuch thatλu ∈Sandλ ≤1. ForA ∈S ∩V,we have

wherepis the radical projection fromStoSR. By(2.7),we see that

So

By the assumption thatR2<(k+1)dr,we have

From Lemma 2.4,ifcj=f(uj),then we can easily knowujis a critical point off|Sandujhas minimal periodkπ.

Theorem 1.2 is proved.

主站蜘蛛池模板: 福利小视频在线播放| 国产精品美女免费视频大全 | 自偷自拍三级全三级视频| 亚洲精品国产自在现线最新| 欧美爱爱网| 午夜性刺激在线观看免费| 国产一级妓女av网站| 久久久精品国产SM调教网站| 日韩欧美国产中文| 日韩乱码免费一区二区三区| 国产日韩精品一区在线不卡| 亚洲高清免费在线观看| 在线永久免费观看的毛片| 综合亚洲色图| 日韩精品成人在线| 亚洲成人动漫在线| 国产噜噜噜| 在线观看亚洲人成网站| 日韩在线网址| 国产一级二级三级毛片| 日韩色图在线观看| 一级毛片中文字幕| 亚洲综合精品香蕉久久网| 国产精品自在线拍国产电影| 看看一级毛片| 国产成人综合日韩精品无码不卡| 在线精品亚洲一区二区古装| 免费AV在线播放观看18禁强制| 色有码无码视频| 亚洲午夜福利在线| 青青青视频91在线 | 中文字幕免费在线视频| 亚洲国产高清精品线久久| 欧美亚洲日韩不卡在线在线观看| 国产性生大片免费观看性欧美| 亚洲中文字幕久久无码精品A| 国产精品人成在线播放| 亚洲欧美激情小说另类| 老司机午夜精品网站在线观看| 人妻无码中文字幕一区二区三区| 午夜欧美理论2019理论| 精品撒尿视频一区二区三区| 国产黄在线免费观看| 欧美激情视频一区二区三区免费| 欧美亚洲网| 亚洲视频免费在线| 欧美久久网| 美女视频黄频a免费高清不卡| 国产成人无码综合亚洲日韩不卡| 久久久久人妻精品一区三寸蜜桃| 99re热精品视频国产免费| 狠狠色狠狠色综合久久第一次| 91成人免费观看| 国内毛片视频| 欧美日韩精品一区二区在线线 | 午夜啪啪福利| 国内精自线i品一区202| 波多野结衣无码中文字幕在线观看一区二区 | 福利片91| 久久这里只有精品8| 天天爽免费视频| 亚洲成人免费看| 免费欧美一级| 99久久成人国产精品免费| 午夜成人在线视频| 国产尤物在线播放| 久久精品国产电影| 国产精品视频观看裸模| 欧美在线一二区| 亚洲一级毛片免费观看| www.日韩三级| 9999在线视频| 国国产a国产片免费麻豆| 97国产精品视频自在拍| 2020精品极品国产色在线观看| 精品91在线| 美女扒开下面流白浆在线试听| 亚洲最大综合网| 秘书高跟黑色丝袜国产91在线| 国产视频一区二区在线观看| 欧美高清国产| 国产一级小视频|