Liyuan MA() School of Mathematical Sciences,Dalian University of Technology,Dalian 116024,China E-mail:liyuan ma@126.com Liang LIANG() School of Mathematics,Liaoning Normal University,Dalian 116029,China E-mail:liang liang@aliyun.com Fengchun LEI()† School of Mathematical Sciences,Dalian University of Technology,Dalian 116024,China E-mail:fclei@dlut.edu.cn Abstract In this paper,we will give a sufficient condition for the self-amalgamation of a handlebody to be strongly irreducible. Key words Heegaard splitting;self-amalgamation;strongly irreducble Dedicated to Professor Banghe LI on the occasion of his 80th birthday LetMbe a compact connected orientable 3-manifold.If there is a separating surfaceFproperly embedded inMsuch thatFcutsMinto two pieces,M1andM2,withF1⊂∂M1andF2⊂∂M2as the two cutting sections ofF,thenMis called a surface sum ofM1andM2alongF1andF2.In particular,ifMis a surface sum of two compression bodiesVandWsuch that∂+V=∂+W=S,thenV∪SWis called a Heegaard splitting ofM.Here,Sis called the Heegaard surface and the genus ofSis called the Heegaard genus.A Heegaard splittingV∪SWforMis said to be stabilized if there are essential disksDinVandEinWsuch that|D∩E|=1. Suppose that a compact orientable 3-manifoldMis a surface sum ofM1andM2alongF1andF2,andofMi,i=1,2.Schultens [13]found a natural Heegaard splitting forMinduced bythis is called an amalgamation ofIn general,an amalgamation of Heegaard splittings is weakly reducible,so it is natural to ask:when is the amalgamation of two Heegaard splittings unstabilized? In the case whereSis a 2-sphere,Bachman [1]and Qiu-Scharlemann [11]independently proved that the connected sum of unstabilized Heegaard splittings is unstabilized.However,many counterexamples show that an amalgamation of two unstabilized Heegaard splittings might be stabilized wheng(F)≥1(we refer to [2],[6],or [14]).On the other hand,if the factor manifolds have high distance Heegaard splittings,see [5,16],or the gluing map of the surface sum is complicated enough,see [7–9,15],then the amalgamation of Heegaard splittings is unstabilized. Suppose thatFis a non-separating surface properly embedded inM.LetM1=andF1,F2⊂∂M1be two cutting sections ofF.ThenMis called the self surface sum ofM1alongF1andF2.By a similar construction,each Heegaard splitting ofM1will induce a natural Heegaard splitting ofMwhich is called the self-amalgamation ofM1.It has been proven that if the Heegaard splitting is complicated enough,then the self-amalgamation is unstabilized;see [3,17]. In the present paper,we will consider the self-amalgamation of a handlebody.It is a fact that the Heegaard splittings of a handlebody are unique(see [12]),i.e.,each Heegaard splittingV∪FWof a handlebodyHnis isotopic to one which is a finite number of elementary stabilizations of the trivial splittingwhereF0is a surface inHnparallel to∂Hn.The main result of the paper is that we give a sufficient condition for such a self-amalgamation to be strongly irreducible. The rest of this article is organized as follows:in Section 2,we review some necessary preliminaries.The statement and proof of the main result are given in Section 3. Suppose thatMis a compact orientable 3-manifold.A Heegaard splittingV∪SWforMis said to be reducible if there are essential disksDinVandEinWsuch that∂D=∂E;otherwise,it is called irreducible.If there are essential disksDinVandEinWsatisfying∂D∩∂E=∅,thenV∪SWis said to be weakly reducible;otherwise,it is strongly irreducible. SupposeFis a compact orientable surface.A simple closed curve inFis said to be essential if it is neither contractible nor∂-parallel inF.A subsurfaceF′ofFis said to be essential inFif each component of∂F′is essential inF. The curve complex ofF,first introduced by Harvey [4],is defined as follows:each vertex inC(F)is the isotopy class of an essential simple closed curve inFand(k+1)vertices determine ak-simplex if they can be realized by pairwise disjoint curves.Masur and Minsky [10]extended the definition to the case in whichFis a torus or once-punctured torus. For simplicity,we do not distinguish an essential simple closed curve or its isotopy class.For any two verticesαandβinC(F),dC(F)(α,β)is the minimal number of 1-simplices among all possible simplicial paths jointingαtoβ.For any two sets of simple closed curvesAandBinC(F),the distance betweenAandB,denoted bydC(F)(A,B),isdefined to be min {dC(F)(α,β)|∀α∈A,∀β∈B}. Suppose thatHis a handlebody withg(H)≥1.LetF1andF2be two disjoint homeomorphic subsurfaces in∂Hwhere each component of∂F1and∂F2is essential in∂H.LetMbe the 3-manifold obtained fromHby gluingF1andF2together along a homeomorphismf.Denote thatdi=dC(∂H)(D,Ci),where D is the set of boundaries of essential disks inHand Ciis the set of simple closed curves inFithat are essential in∂Hfori=1,2.Then we have the following proposition. Proposition 2.1LetMbe the self surface sum ofHalongF1andF2.Ifdi≥2,then∂Mis incompressible inM. ProofOtherwise,suppose that∂Mis compressible inMand thatDis a compressing disk.Denote the surfaceF1=F2byFinM.IsotopeDsuch that|D∩F|is minimal. First weconsider the caseg(H)>1.IfD∩F=∅,thenDisan essential disk inHsatisfyingD∩Fi=∅fori=1,2.Thus,for any essential simple closed curveCi∈Ci,Ci∩∂D=∅wherei=1,2,sodC(∂H)(D,Ci)≤dC(∂H)(∂D,Ci)≤1,which is a contradiction. ThusD∩F∅ up to isotopy.The surfaceFis incompressible inM.Otherwise,suppose that there is a compressing diskDFforFand∂DF∩∂H⊂F1.ThenDFis a compressing disk forF1inH.This means that there is an essential simple closed curveCinF1such thatC=∂D.ThusdC(∂H)(D,C1)≤dC(∂H)(∂D,C)=0,which is a contradiction.ThereforeFis incompressible inM. An innermost closed curveargument impliesthat there is no simple closed curvecomponent inD∩F,soD∩Fconsists of arcs.Choose an arcαinD∩Fsuch thatαis outermost inD.Thenαcuts a diskDαfromDsuch thatDα∩F=α.Dαis essential inH.Otherwise,we can isotopeDto reduce|D∩F|,which is a contradiction.Suppose thatDα∩F1=α.Ifαis inessential inF,then we isotopeDαsuch thatDα∩F1=∅.A similar argument as to that above implies thatdC(∂H)(D,C1)≤1,which is a contradiction.Thusαis essential inFandF1.IfF1ia an annulus,then there is a core curveCinF1satisfyingC∈C1and|C∩α|=1.It is clear thatC∩D=C∩α.Then|C∩D|=1 and∂N(C∪D)bounds an essential disk inHwhich is disjoint fromC,whereN(C∪D)is the regular neighborhood ofC∪DinH.This implies thatdC(∂H)(D,C1)≤1,which is a contradiction.IfF1is not an annulus,then there always exists a curveCinF1satisfyingC∩α=∅andC∈C1.SinceDα∩F1=α,C∩D=∅.SodC(∂H)(D,C1)≤1,which is a contradiction.Thus the proposition holds in this case. For the caseg(H)=1,a similar argument implies that the conclusion holds. This completes the proof of the proposition. □ There is a Heegaard splitting forMcalled the self-amalgamation constructed as follows: LetH=∂H×I,whereV1is homeomorphic toHand∂H=∂H×{0}.Choose a pointp1inF1and a pointp2inF2such thatf(p1)=p2.Letαi=pi×Ibe a spanning arc in∂H×I.Denote the surfaceF1=F2byFand the pointp1=p2bypinM.Letα=andN(α)=N(α1)∪N(α2)be the regular neighborhood ofαinMwhereN(αi)=αi×Dis the regular neighborhood ofαiin∂H×Ifori=1,2.LetDi=pi×{1}×DandD=p×D.ThenN(α)∩S1=D1∪D2andN(α)∩F=D.LetV=V1∪N(α)andW=.ThenV∪SWis a Heegaard splitting ofMcalled the self-amalgamation ofH. Assume that the Heegaard splittingV∪SWis weakly reducible.Choose an essential diskBinVandEinWsuch thatB∩E=∅and|E∩F|is minimal among all such pairs of disks.Furthermore,we can isotopeBsuch that|B∩D|is minimal andB∩E=∅. Assume thatγis an outermost arc inE∩F0and thatγcutsEγfromEjust the same as above.Thenγis essential inF0andEγis isotopic toγ×I.Choose a component of∂D−γ,which we denote byδ.ThenEγ∪δ×Iis a spanning annulus in∂H×I.It is clear thatγ∪δis an essential simple closed curve inF1.LetC=(Eγ∪δ×I)∩S1.ThenCis essential inS1andC=f1(γ∪δ)∈f1(C1).We have the following claim: Claim 4There is an essential disk inV1which is disjoint fromC. IfB∩D=∅,thenBis an essential disk inV1,and it is clear thatB∩C=∅.The claim holds in this case. IfB∩D∅,then an innermost closed curve argument implies thatB∩Dconsists of arcs.Choose an arcξinB∩Dsuchξis outermost inB.Thenξcuts a diskB0fromBsuch thatB0∩D=ξ.Since|B∩D|is minimal,B0is an essential disk inV1.IfB0∩F1=∅,thenB0∩C=∅,and the claim holds. Now assume thatB0∩F1∅.If∂ ξlie inδorthen after isotopyB0∩C=∅,and the claim holds.If one component of∂ ξlies inδand the other one lies inthen after isotopy,|B0∩C|=1.In this case,∂N(B0∪C)bounds an essential disk which is disjoint fromC,so the claim holds. For the caseg(H)=1,a similar argument as to that above implies that the conclusion holds. This completes the proof of the theorem. □ Remark 3.3In fact,d1andd2can be viewed as a description of the complexity for a selfamalgamation.LetF1andF2be disjoint essential homeomorphic subsurfaces in∂H.If there is an essential diskDinHsuch thatD∩Fi=∅,thendi≤1,wherei=1,2.By the construction ofV∪SW,we can choose an essential arcγ1⊂F1andγ2⊂F2satisfyingf(γ1)=γ2.LetE=It is clear thatEis an essential disk inWthat andDis an essential disk inVsatisfying that∂D∩∂E=∅.Therefore in this case the self-amalgamationV∪SWis weakly reducible. Moreover,suppose thatg(H)=2.There exist two disjoint two essential simple closed curvesC1andC2in∂Hsatisfying the following conditions: (1)∂H−C2is incompressible; (2)there exists an essential diskDinHsuch that|C1∩D|=1 and|C2∩D|=2;see Figure 2. Figure 1 Self-amalgamation of a handlebody Figure 2 Those two examples show that the self-amalgamation of a handlebody might be stabilized ifdi≤1 fori=1 or 2.Hence the conditions in Theorem 3.2 are optimal in sense of the complexity of the self-amalgamation. IfFiis an annulus,then there is only one essential simple closed curve inFiup to isotopy.Thus we have the following corollary. Corollary 3.4LetHbe a handlebody withg(H)≥1 and letF1andF2be two disjoint homeomorphic essential annuli in∂H.If∂H−Fiis incompressible fori=1,2,then the self-amalgamationV∪SWis strongly irreducible. By the definition of curve complex,we have the following corollary. Corollary 3.5LetHbe a handlebody withg(H)≥1 andF1,F2two disjoint homeomorphic essential subsurfacesin∂H.IfdC(∂H)(D,∂Fi)≥3 fori=1,2,then the self-amalgamationV∪SWis strongly irreducible. With a similar argument,we can extend the results to compression bodies. Corollary 3.6Suppose thatCis a compression body withg(∂+C)≥1 and thatF1andF2aretwo disjoint homeomorphic essential subsurfacesin∂+C.Let DCbetheset of boundaries of essential disks inC.IfdC(∂+C)(DC,Ci)≥2 fori=1,2,then the self-amalgamation ofCalongF1andF2is strongly irreducible. |