propertiesofthePoincar´emapforsystem(1.1)areestablishedinSection3.Bothnecessaryandsu cientconditionsforbifurcationofperiodicsolutionsto(1.1)areobtainedinSection4.Finally,intheappendixofSection5wegiveaproofofatechnicalresultneededinSection3.
2Lyapunov-Schmidtreduction
F(ξ,ε)=P(ξ) ξ+εQ(ξ,ε),LetEbeaBanachspaceandconsiderthefunctionF:E×[0,1]→Egivenby
whereP:E→EandQ:E×[0,1]→E.Assumethat
(A1)thereexisth0∈Rk,r0>0andafunctionS∈C1(BRk(h0,r0),E)suchthat
P(ξ)=ξforanyξ∈Z={S(h):h∈BRk(h0,r0)}.
HereandinwhatfollowsBX(c,r)denotestheballinthenormedspaceXcenteredatcwithradiusr>0.Itiswellknownthat,undertheassumption(A1)withP∈C1(E,E)andQ∈C1(E×[0,1],E),theLyapunov-Schmidtreduction([4],Ch.2,§4)allowstosolvetheequation
F(ξ,ε)=0,(2.1)
forε>0su cientlysmall.NexttheoremextendsthisresulttothecasewhenQsatis esthefollowingLipschitzcondition:
(L)ForanyR>0thereexistsL(R)>0suchthat
Q(ξ1,ε) Q(ξ2,ε) ≤L(R) ξ1 ξ2
wheneverξ1,ξ2∈BE(0,R)andε∈[0,1].
Theorem2.1LetP∈C1(E,E),Q∈C0(E×[0,1],E),whereEisaBanachspace.AssumethatQsatis es(L).Moreover,assume(A1)and
(A2)dimS′(h0)Rk=k.
LetE1,h=S′(h)Rk.LetE2,hbeanysubspaceofEsuchthatE=E1,h
assumethat E2,hand(A3)thereexistsr0>0suchthatboththeprojectorsπ1,hofEontoE1,halong
E2,handπ2,hofEontoE2,halongE1,harecontinuousinh∈BRk(h0,r0),(A4)forξ0=S(h0)wehave
π2,h0(P′(ξ0) I)π2,h0isinvertibleonE2,h0.
3(2.2)
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