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        On Integrable Conditions of Generalized Almost Complex Structures

        2016-10-13 08:43:43YINYANBINANDLIULING

        YIN YAN-BINAND LIU LING

        (1.School of Mathematics and Statistics,Henan University,Kaifeng,Henan,475004)

        (2.School of Applied Science,Beijing Information Science and Technology University, Beijing,100192)

        Communicated by Rong Xiao-chun

        ?

        On Integrable Conditions of Generalized Almost Complex Structures

        YIN YAN-BIN1AND LIU LING2

        (1.School of Mathematics and Statistics,Henan University,Kaifeng,Henan,475004)

        (2.School of Applied Science,Beijing Information Science and Technology University, Beijing,100192)

        Communicated by Rong Xiao-chun

        Generalized complex geometry is a new kind of geometrical structure which contains complex and symplectic geometry as its special cases.This paper gives the equivalence between the integrable conditions of a generalized almost complex structure in big bracket formalism and those in the general framework.

        generalized almost complex geometry,big bracket,supermanifold

        2010 MR subject classification:53D17,17B63

        Document code:A

        Article ID:1674-5647(2016)02-0111-06

        1 Introduction

        Generalized geometry was created by Hitchin[1]originally as a way of characterizing special geometry in low dimensions,and has been further developed by Hitchin’s students.

        In[2],the integrable conditions under which a generalized almost complex structure becomes a generalized complex structure have been given in general way.The same question is discussed by using the big bracket formulism in supermanifold geometry by Kosmann-Schwarzbach and Rubtsov[3].

        In this paper,we firstly recall some basic notions and facts about generalized complex structures,and then we devote to proving the equivalence between the integrable conditions of a generalized almost complex structure in different formalism.

        2 Integrable Conditions of Generalized Almost Complex Structures

        Assume that M is a real manifold with dimension 2n and set TM=TM ⊕T?M.A generalized almost complex is an endomorphism N:TM?→TM such that

        (1)N is symplectic,i.e.,〈Ne1,e2〉+〈e1,Ne2〉=0 for e1,e2∈Γ(TM);

        (2)N is complex,i.e.,N2=?Id,

        where〈·,·〉denotes the natural pairing given by〈X+ξ,Y+η〉=η(X)+ξ(Y)for X+ξ,Y+η∈Γ(TM).

        Any generalized almost complex structure N may be presented by classical tensor fields as follows:

        where π∈Γ(∧2TM),σ∈?2(M),and N is a(1,1)-tensor field over M,π?:T?M?→TM denotes a linear map defined by π?(ξ)=iξπ=π(ξ,·)for ξ∈?1(M).Similarly,σ?is a linear map defined by σ?(X)=iXσ for X∈Γ(TM),N?is the dual map of N.Clearly,N is symplectic if N is of the above form.

        For any e=X+ξ∈Γ(TM),we have

        This structure is described by the big bracket formulism in[3].The big bracket,denoted by{·,·},is an even graded bracket on the space O of functions on the cotangent bundle ΠT?M,which is a supermanifold given by TM,more details are found in[4]–[5].The action of N on e∈Γ(TM)can be expressed as

        that is,Ne={e,N}for any e∈Γ(TM).

        By definition of the generalized almost complex structure,the endomorphism N=N+ π+σ of TM is a generalized almost complex structure if and only if the following equalities hold:

        (a)N2+π?σ?=?Id;

        (b)Nπ?=π?N?;

        (c)σ?N=N?σ?.

        The Dorfman torsion of a generalized almost complex N,denoted by τμN(yùn),is defined by τμN(yùn)(e1,e2)=[Ne1,Ne2]μ?N([Ne1,e2]μ+[e1,Ne2]μ?N[e1,e2]μ),e1,e2∈Γ(TM), where the bracket[·,·]μis the canonical Courant bracket on M defined by [X+ξ,Y+η]μ={{X+ξ,μ},Y+η}=[X,Y]μ+LXη?iYdξ,X+ξ,Y+η∈Γ(TM). More caculations can be found in[3].If we define

        the torsion of N may be expressed as

        Proposition 2.1[3]In terms of big bracket,we have

        and

        Definition 2.1A generalized almost complex structure N is a generalized complex structure if τμN(yùn)=0.

        Theorem 2.1[3]A generalized complex structure is a generalized almost complex structure N satisfying

        Comparing their degrees of two sides of the equality(2.1),we obtain the following theorem.

        Theorem 2.2A generalized almost complex structure N=π+σ+N is a generalized complex structure if and only if

        (I1)[N,N]μ+[π,σ]μ+[σ,π]μ=μ;

        (I2)[N,π]μ+[π,N]μ=0;

        (I3)[N,σ]μ+[σ,N]μ=0;

        (I4)[π,π]μ=0.

        Theorem 2.1 describes the compatible conditions under which a generalized almost complex structure becomes a generalized complex structure.Those compatible conditions are given in big bracket formalism.But it can be rewritten as the following theorem in a general way.

        Theorem 2.3A generalized almost complex structure N=π+σ+N is a generalized complex structure if and only if for X,Y,Z∈Γ(TM),ξ,η∈?1(M),

        (J1)τμN(yùn)(X,Y)=π?(iX∧Ydσ);

        (J2)N?[ξ,η]π=Lπ?(ξ)N?η?Lπ?(η)N?ξ?d(π(N?ξ,η));

        (J3)dσN(X,Y,Z)=dσ(NX,Y,Z)+dσ(X,NY,Z)+dσ(X,NY,Z)+dσ(X,Y,NZ), where σN(X,Y)=σ(NX,Y);

        (J4)π?[ξ,η]μ=[π?(ξ),π?(η)]μ.

        Proof.Since N is complex,we have

        Consider

        It shows that{π,N}is a bivector from its bi-degree(2,0).Thus,πNis a bivector field and

        Proof.Note that

        Moreover,

        and

        Hence

        which shows that

        Furthermore,we can get

        since N is complex.

        Proof of Theorem 2.3We hope to prove that the integrable conditions in Theorem 2.2 are one-to-one equivalent corresponding to the integrable conditions in Theorem 2.3.

        For the first condition,assume that

        Then we have

        Hence,τμN(yùn)={dσ,π},and for X,Y∈Γ(TM),we have

        Thus,

        For the second condition,consider

        Applying the second condition[π,N]μ+[N,π]μ=0 in Theorem 2.2,we have

        and for any ξ,η∈Γ(T?M),

        Hence,

        For the third condition,consider

        Applying the third condition[N,σ]μ+[σ,N]μ=0,we obtain

        Moreover,we have

        Therefore,

        The equivalence between the last compatible conditions in two theorems is obviously.

        Remark 2.1Theorem 2.3 can be directly obtained in a general framework of Lie algebroids(see[2]).

        [1]Hitchin N.Generalized calabi-yau manifolds.Q.J.Math.,2003,54(3):281–308.

        [2]Crainic M.Generalized complex structures and Lie brackets.Bull.Braz.Math.Soc.,2011,42(4): 559–578.

        [3]Kosmann-Schwarzbach Y,Rubtsov V.Compatible structures on Lie algebroids and Monge-Ampere operators.Acta Appl.Math.,2010,109(1):101–135.

        [4]Yin Y B,He L G.Dirac strucures on protobialgebroids.Sci.China Ser.A,2006,49(10):1341–1352.

        [5]Roytenberg D.On the Structure of Graded Symplectic Supermanifolds and Courant Algebroids. in:Quantization,Poisson Brackets and Beyond.Contemp.Math.vol.315.Providence,RI: Amer.Math.Soc.,2002:169–185.

        10.13447/j.1674-5647.2016.02.03

        date:Sept.7,2014.

        The Excellent Talent Program(2012D005007000005)of Beijing.

        E-mail address:yyb@henu.edu.cn(Yin Y B).

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