ebook img

Generalized Almost Product Structures and Generalized CRF-structures PDF

0.29 MB·
Save to my drive
Quick download
Download
Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.

Preview Generalized Almost Product Structures and Generalized CRF-structures

GENERALIZED ALMOST PRODUCT STRUCTURES AND GENERALIZED CRF-STRUCTURES MARCO ALDI AND DANIELE GRANDINI 7 1 Abstract. We give severalequivalent characterizationsof orthogonalsubbundles of 0 the generalized tangent bundle defined, up to B-field transform, by almost product 2 and local product structures. We also introduce a pure spinor formalism for gen- n eralized CRF-structure and investigate the resulting decomposition of the de Rham a J operator. As applicationswegiveacharacterizationofgeneralizedcomplexmanifolds that are locally the product of generalized complex factors and discuss infinitesimal 0 1 deformations of generalized CRF-structures. ] G D . h 1. Introduction t a m Generalized CRF-structures were introduced in [16] as Courant involutive, (not nec- [ essarilymaximal) isotropicsubbundles Lofthecomplexified generalized tangentbundle with no non-trivial totally real section. In this paper we continue the work initiated 1 v in [2] and focus on generalized CRF-structures L such that L L = E C, where E ⊕ ⊗ 2 is a split structure i.e. a subbundle of the generalized tangent bundle with the prop- 2 erty that the restriction of the tautological inner product to E is non-degenerate of 6 2 signature (k,k). If this is the case we say that L is a generalized CRF-structure on 0 the split structure E. Since generalized complex structures [6] and strongly integrable . 1 generalized contact structures [12] are all examples of generalized CRF-structures on 0 split structures, their study is important in order to develop a unified understanding of 7 1 geometric structures on the generalized tangent bundle. : v The goal of this paper is to investigate the geometry of generalized CRF-structures i X on a particular class of split structures called generalized almost product structures. By r definition a generalized almost product structure is a split structure E whose projection a π(E) onto the tangent bundle is “minimal” in the sense that its rank is half the rank of E. As we show, this notion is equivalent to requiring that (π(E),π(E )) is a classical ⊥ almost product structure (as defined in [7]) or, alternatively, to the condition that the cotangent bundle is a direct sum of its intersections with E and E . This last ⊥ characterization implies that each generalized almost product structure gives rise to a canonical bigrading on the exterior algebra of differential forms which is a refinement of its standard Z-grading. In particular we obtain a decomposition of the de Rham operator d = d + d , with d of bidegree (1,0)+ ( 1,2). Interestingly, restricting E E E ⊥ − thestandardDorfmanbrackettoE andcomposingwiththeorthogonalprojectionofthe generalized tangent bundle onto E gives rise to a binary operationJ, K which coincides E with the derived bracket for d . We show that J, K (together with the restrictions of E E the tautological inner product and anchor map to E) defines a structure of Courant 1 2 MARCO ALDIANDDANIELEGRANDINI algebroid on an almost product E if and only if π(E) is a foliation. Moreover, π(E) and π(E ) are complementary foliations if and only if d2 = 0. ⊥ E An appealing feature of generalized CRF-structures on generalized almost product structures is that they admit an alternate description in terms of pure spinors, which generalizes the spinorial approach to generalized complex structures and generalized contact structures discussed in [6], [9], [4] and[1]. In particular we show that each generalized CRF-structure gives rise to a canonical (up to shift) Z-grading on complex differential forms. With respect to this grading, d is of degree 0 while d decom- E E ⊥ poses into a components of degree 1 and 1 which in the case of generalized complex − structures respectively to the ∂ and and ∂ operators defined in [6]. Wealsodiscuss aweaker integrability conditioninwhich d isstillrequired todecom- E pose into components of degree 1, but no assumption is made on the degree of d . E ± ⊥ These more general structures, which we refer to as weak generalized CRF-structures, contain interesting examples (e.g. classical contact structures) that dare not generalized CRF-structures. In the particular case of generalized CRF-structures on an almost product structure E such that π(E ) is a foliation, d restricts to a differential on basic forms for this ⊥ E foliation. The grading induced by the generalized CRF-structure and the resulting de- composition of d can be restricted to basic forms. In particular, the spinorial approach E to transverse generalized complex structures of [18] and the basic dd -lemma discussed J in [13] fit naturally into the framework of the present paper. Moreover if π(E) is also a foliation, we show that the results of [4] on the ∂∂-lemma and the canonical spectral sequence apply to all forms, not just those that are basic with respect to π(E ). ⊥ In addition to illustrating with examples that our framework effectively unifies previ- ous spinorial approaches to generalized geometry, we offer two applications. The first is a characterization of generalized complex manifolds (M,J) that are locally the product of two generalized complex manifolds in terms of certain integrability conditions satis- fied by the restriction of J to an almost product structure. Our second application is a characterization of infinitesimal deformations of (weak) generalized CRF-structures along the lines of the Kodaira-Spencer formalism developed for generalized complex structures in [6], [10] and [15]. We prove that that deformations of weak generalized CRF-structures are governed by a single equation which specializes to the well-known Kodaira-Spencer/Maurer-Cartanequationinthecaseofgeneralizedcomplexstructures. On the other hand a second equation, stating that the operator that represents the de- formation commutes with d is required to characterized deformations of generalized E ⊥ CRF-structures. The paper is organized as follows. In Section 2 we collect some basic facts about R-linear operators acting on differential forms, the preferred language of this paper. In particular, we view sections of the generalized tangent bundle as operators acting on forms in such a way that (up to scaling by a factor of 2), the tautological inner product coincides with the obvious graded commutators of operators. We also intro- duce generalized Lie derivatives as well as derived brackets for operators that are not necessarily the de Rham operator, as this level of generality is useful in the bulk of the paper. In Section 3 we introduce generalized almost product structures. After GENERALIZED ALMOST PRODUCT STRUCTURES AND GENERALIZED CRF-STRUCTURES 3 proving several equivalent characterizations of generalized almost product structures among all split structures, we describe the decomposition of the de Rham operator that they induce and the corresponding derived brackets. We then proceed to investigate the additional structure that emerges if one additionally assumes that π(E) and/or π(E ) is a foliation. In this context, we also introduce our slight generalization (ac- ⊥ counting for a possible B-field transform) of the standard notions of basic differential forms and basic complex attached to a foliation. In Section 4 is devoted to Vaisman’s generalized F-structures, which we view as operators acting on forms. In the particular case in which the kernel of the generalized F-structure is an almost product struc- ture (or, more generally, is equipped with a decomposition into isotropic subbundles), we construct a canonical Z-grading on complex differential forms. After illustrating these notions with several examples, we show that with respect to this grading d E ⊥ decomposes into components of degree 0 or 2. In Section 5 we investigate the integra- ± bility conditions which define (weak) generalized CRF-structures among all generalized F-structures. Our characterizations of integrability are intended to be reminiscent of those established for generalized complex structures in [6], [4] and [15]. In the last part of this section we specialize to the case in which both π(E) and π(E ) are foliations. In ⊥ particular, we discuss the role of the ∂∂-lemma in this framework and prove the char- acterization of local products of generalized complex manifolds mentioned above. The paper ends with Section 6, which is devoted to the study of infinitesimal deformations of (weak) generalized CRF-structures. While (in the spirit of [10] and [15]), our results are stated in the language of operators acting on forms, we also remark that in the case in which the image of the generalized F-structure is a foliation our finding are in agreement with the standard theory of deformations of Lie bialgebroids developed in [11]. Acknowledgments: Parts of this paper were written while visiting Swarthmore Col- lege, the Simons Center for Geometry and Physics and IMPA. We would like to thank theseinstitutions forhospitality andexcellent working conditions. Wealso wouldlike to thank Reimundo Heluani, Ralph Gomez, Janet Talvacchia and Alessandro Tomasiello for inspiring conversations. 2. Operators on forms Definition 1. Unless otherwise specified, we let M be a connected, finite dimensional smooth manifold. We denote by Ω = Γ( T M) be the graded commutative algebra M • ∗ of R-valued differential forms on M. We d∧enote by Ωk , k = 0,...,dimM, the graded M component with respect to the standard Z-grading and by Ωk¯ , k¯ = ¯0,¯1 the components M of the standard Z/2-grading by parity. We denote by the graded algebra of R-linear M E endomorphisms of Ω and by the graded Lie algebra of graded derivations of . M M M D E We define the adjoint map ad HomR( M, M) such that ∈ E D (1) ad (ψ) = [ϕ,ψ] = ϕ ψ ( 1)klψ ϕ ϕ ◦ − − ◦ for all ϕ k and ψ l . ∈ EM ∈ EM 4 MARCO ALDIANDDANIELEGRANDINI Remark 2. Left multiplication defines a canonical embedding of Ω into . On the M M E other hand, if ϕ is such that Ω1 ker(ad ), then ϕ = ϕ(1) Ω . Therefore, ∈ EM M ⊆ ϕ ∈ M ϕ Ω if and only if Ω1 ker(ad ). Similarly, ϕ is Ω0 -linear if and only if ∈ M M ⊆ ϕ ∈ EM M Ω0 ker(ad ). M ⊆ ϕ Remark 3. The canonical embedding of Ω1 in 1 can be extended to a canonical embedding of sections of the generalized taMngentEbMundle TM = TM T M of M ∗ ⊕ into 1 1 by identifying each X Γ(TM) with the interior product ι , i.e. the EM ⊕ EM− ∈ X unique Ω0 -linear operator such that [X,α] = α(X) for all α Ω1 . By Remark 2, Γ(TM) Mker(ad ) if and only if ϕ is a form on M such that Γ(T∈M)M ker(ad ), i.e. if ϕ ϕ ⊆ ⊆ and only if ϕ Ω0 . ∈ M Remark 4. Let d 1 be the de Rham operator on M. Since T M is maximal isotropic in TM (wit∈h rEeMspect to the Ω0 -valued pairing , defined as t∗wice the graded M h i commutator) and Ω1 is generated over Ω0 by d(Ω0 ), we conclude that M M M (2) Ω1 = x Γ(TM) d(Ω0 ) ker(ad ) . M { ∈ | M ⊆ x } Definition 5. We define the generalized Lie derivative associated with δ to be M ∈ E Lδ = ad◦adδ ∈ HomR(EM,DM) which assigns to each ϕ ∈ EM the operator Lδϕ = ad[ϕ,δ]. The derived bracket associated with δ is J, Kδ : M R M M defined by Jϕ1,ϕ2Kδ = E ⊗ E → E Lδ (ϕ ). In the important case of the de Rham operator, we use the shorthand notation ϕ1 2 L = Ld and J, K = J, K . d Remark 6. Let deg 0 be the diagonal operator on Ω with k-eigenspace equal ∈ EM M to Ωk for each k. Then ad is diagonal on with l-eigenspace equal to l for M deg EM EM each l. Therefore, each derivation δ of degree l = 0 can be recovered from the M ∈ E 6 corresponding generalized Lie derivative as δ = 1Lδ . In particular, d = L . l deg deg Remark 7. Using the Jacobi identity for ( ,[, ]), conveniently written as M E (3) [ad ,ad ] = ad ϕ ψ [ϕ,ψ] for all all ϕ,ψ , it is straightforward to check that the identities M ∈ E (4) ad = [Lδ ,ad ] Jϕ,ψKδ ϕ ψ (5) ( 1)kj[[ϕ,ψ],δ] = Jϕ,ψK ( 1)k(i+j)+ijJψ,ϕK δ δ − − − hold for all ϕ i , ψ j and δ k . ∈ EM ∈ EM ∈ EM Remark 8. If α Ωk , then L (f) = ( 1)k[f,dα] = 0 = ad (f) for all f Ω0 . ∈ M α − α ∈ M Conversely, if (6) Ω0 ker(ad ) ker(L ) M ⊆ ϕ ∩ ϕ then by Remark 2, ϕ is Ω0 -linear and, by (3), M (7) ad (df) = ad (ad (f)) = 0 ϕ ϕ d for all f Ω0 . Using Remark 2 again we conclude that ϕ Ω if and only if (7) ∈ M ∈ M holds. GENERALIZED ALMOST PRODUCT STRUCTURES AND GENERALIZED CRF-STRUCTURES 5 Remark 9. If X Γ(TM), then L acts on Ω as the usual Lie derivative. In X M particular, Ω0 is clo∈sed under the action of L for each ϕ Γ(TM) Ω . Conversely, suppose thatMϕ is Ω0 -linear and L (Ω0ϕ) Ω0 . Th∈en L is a⊕deMrivation of Ω0 and therefore th∈erEeMexistsMX Γ(TM) suϕchMtha⊆t Ω0M ker(L ϕ ). By Remark 8 wMe ∈ M ⊆ ϕ−X conclude that ϕ X Ω and thus ϕ Γ(TM) Ω . M M − ∈ ∈ ⊕ Definition 10. If ϕ is nilpotent, the adjoint automorphism associated with ϕ is M ∈ E Adϕ AutR( M) such that Adϕ(ψ) = eϕ ψ e−ϕ for all ψ M. ∈ E ◦ ◦ ∈ E Remark 11. Since M is finite dimensional, every ϕ of positive or negative degree M ∈ E is automatically nilpotent. Remark 12. Let ϕ ¯0 be nilpotent. Then ad is also nilpotent and Ad = eadϕ. ∈ EM ϕ ϕ Furthermore, since (8) Ad ad Ad = ad ϕ ◦ ψ ◦ −ϕ Adϕ(ψ) for all ψ , we obtain M ∈ E (9) Ad (Jψ ,ψ K ) = JAd (ψ ),Ad (ψ )K ϕ 1 2 δ ϕ 1 ϕ 2 Adϕ(δ) for all ψ ,ψ ,δ . 1 2 M ∈ E Definition 13. The Leibnizator of δ is the function : defined M δ M M M by (ϕ,ψ) = [Lδ ,Lδ ] Lδ for ea∈chEϕ,ψ . L E ×E → E Lδ ϕ ψ − Jϕ,ψKδ ∈ EM Lemma 14. If δ ¯1 , then 2 (ϕ,ψ) = ( 1)kad for all ϕ and ψ k . ∈ EM Lδ − − Jϕ,ψKδ2 ∈ EM ∈ EM Proof: Using (3) repeatedly, we obtain (10) 2 (ϕ,ψ) = 2ad = ( 2)kad = ( 1)kad . Lδ [[ϕ,δ],[ψ,δ]]−[[[ϕ,δ],ψ],δ] − − [[[ϕ,δ],δ],ψ] − − Jϕ,ψKδ2 Example 15. In particular, d2 = 0 implies that the Leibnizator of the de Rham operator vanishes identically. Unraveling the definition we obtain (11) Jϕ ,Jϕ ,ϕ KK = JJϕ ,ϕ K,ϕ K+( 1)k1+k2+k1k2Jϕ ,Jϕ ,ϕ KK 1 2 3 1 2 3 2 1 3 − for all ϕ ki, i = 1,2,3. In particular, if φ ,φ ,φ Γ(TM) we recover the familiar i ∈ EM 1 2 3 ∈ Jacobi identity for the Dorfman bracket. 3. Generalized Almost Product Structures Definition 16. A split structure of rank 2k on M is a subbundle E TM on which ⊆ the restriction , of the tautological bilinear form , to E is non-degenerate and E of signature (k,hk)i. We denote by pr the orthogonal phroijection of TM onto E. E Remark 17. If B Ω2 , then Ad restricts to an automorphism of TM, which by (8) is orthogonal with∈respMect to , .B In particular, E TM is a split structure if and h i ⊆ only if Ad (E) is. B Remark 18. E is a split structure of rank 2k on M if and only if E is a split structure ⊥ of rank 2(dim(M) k). − 6 MARCO ALDIANDDANIELEGRANDINI Remark 19. If E is a non-zero split structure on M, non-degeneracy implies that π(E) has nowhere vanishing fibers. Using partitions of unity and the local existence theorem for ODEs, it follows that every function in Ω0 can be written locally as L (f) for M π(x) some x Γ(E) and for some f Ω0 . On the other hand, (4) implies ∈ ∈ M (ad L )(f) = ad ([x,df]) = ad ([x,pr (df)]) ϕ π(x) ϕ ϕ E ◦ (12) = ( 1)k(Jx,pr (df)K +Jpr (df),xK ) − − E ϕ E ϕ for x Γ(E), f Ω0 and for any ϕ k . Setting ϕ = d, we conclude that E is closed under∈the Dorfm∈anMbracket if and on∈lyEiMf T M E if and only if E = TM. ∗ ⊆ Lemma 20. Let ϕ and assume there exists a split structure E on M such that M ∈ E Jx,yK ker(ad) for all x,y Γ(E). Then ϕ is Ω0 -linear. ϕ ∈ ∈ M Proof: By assumption, Jx,yK commutes with Γ(E) and with d and thus must be a ϕ constant multiple of the identity of all x,y Γ(E). By (3), we conclude that ad is a ϕ ∈ derivation of Ω0 whose image consists of constant functions. This concludes the proof M since the only such derivation is the zero derivation. Lemma 21. Let δ ¯1 be such that δ(1) = 0 and [δ2,d] = 0. Then following are ∈ EM equivalent 1) δ2 = 0; 2) = 0; δ L 3) there exists a non-zero split structure E on M such (x,y) = 0 for all x,y Γ(E). δ L ∈ Proof: By Lemma 14, 1) implies 2). Since TM is a split structure, 2) implies 3). If 3) holds, then it follows from Lemma 14 and Lemma 20 that δ2 is Ω0 -linear. Combining M Remark 8 with the assumption [δ2,d] = 0, we conclude that δ2 = δ2(1) = 0 which concludes the proof. Definition 22. Let E be a split structure of rank 2k on M. The type of E at m M ∈ is the rank, denoted by p (m), of π at m. E E Remark 23. Let E be a split structure of rank 2k on M. Since ker(π ) = T M E E ∗ ∩ is isotropic, then p (m) k for all m M. E ≥ ∈ Definition 24. A generalized almost product structure is a split structure E of rank 2k on M such that p = k. E Example 25. Recall that an almost product structure [7] is a pair (F,G) of subbundles of TM such that TM = F G. Each almost product structure (F,G) defines two ⊕ canonical generalized almost product structures: E = F Ann(G) and E = G ⊥ ⊕ ⊕ Ann(F). Proposition 26. Let E be a split structure on M. The following are equivalent 1) E is a generalized almost product structure; 2) T M = (T M E) (T M E ); ∗ ∗ ∗ ⊥ ∩ ⊕ ∩ 3) (π(E),π(E )) is an almost product structure; ⊥ GENERALIZED ALMOST PRODUCT STRUCTURES AND GENERALIZED CRF-STRUCTURES 7 4) There exists B Ω2 such that E ∈ M Ad (E) = π(E) Ann(π(E )) and Ad (E ) = π(E ) Ann(π(E)); BE ⊕ ⊥ BE ⊥ ⊥ ⊕ 5) [pr (df),pr (dg)] = 0 each f,g Ω0 . E E ∈ M Proof: Since E is a generalized almost product structure on M, then T M E E ∗ ∩ ⊆ is maximal isotropic. On the other hand, Ann(π(E)) = T M E and is a subbundle ∗ ⊥ ∩ of rank n k. Consequently, 1) implies 2). If 2) holds, then T M E E and ∗ − ∩ ⊆ T M E E are maximal isotropic. Therefore E and E are generalized almost ∗ ⊥ ⊥ ⊥ ∩ ⊆ product structures. Since TM = π(E E ) = π(E) + π(E ), we conclude that 2) ⊥ ⊥ ⊕ implies 1) and 3). Since (13) 0 = [x,y] = ad (π(x))+ad (π(y)). y x for any x Γ(E) and y Γ(E ), if 3) holds there exists a well defined B Ω2 ∈ ∈ ⊥ E ∈ M such that (ad ad )(B ) = ad (π(x)) if x Γ(E) and y Γ(E ) while (ad π(x) π(y) E y ⊥ π(x) ◦ ∈ ∈ ◦ ad )(B ) = 0 if x,y Γ(E) or x,y Γ(E ). If x Γ(E), then π(Ad (x)) = π(x) π(y) E ∈ ∈ ⊥ ∈ BE and ad (Ad (x) π(x)) = ad (x π(x) ad (B )) π(y) BE − y − − π(x) E (14) = ad (π(x)) (ad ad )(B ) y π(y) π(x) E − − ◦ (15) = 0 for all y Γ(E ). Therefore, Ad (E) π(E) Ann(π(E )). On the other hand ∈ ⊥ BE ⊆ ⊕ ⊥ (16) (ad Ad )(π(x)) = ad (π(x))+(ad ad )(B ) = 0 y ◦ −BE y π(y) ◦ π(x) E for all x Γ(E) and y Γ(E ). Together with ⊥ ∈ ∈ (17) Ad (Ann(π(E )) = Ann(π(E )) E −BE ⊥ ⊥ ⊆ this implies π(E) Ann(π(E )) Ad (E). A similar calculation for E shows that ⊕ ⊥ ⊆ BE ⊥ 3) implies 4). If 4) holds, then (Ad (E)) = Ad (E ) implies BE ⊥ BE ⊥ (18) T M = (T M Ad (E)) (T M Ad (E )) = (T M E) (T M E ) ∗ ∗ ∩ BE ⊕ ∗ ∩ BE ⊥ ∗ ∩ ⊕ ∗ ∩ ⊥ and thus 1). Finally for each fixed f Ω0 , [pr (df),dg] = [pr (df),pr (dg)] = 0 for ∈ M E E E all g Ω0 if and only if pr (df) Γ(T M E). Therefore, 5) is equivalent to 2). ∈ M E ∈ ∗ ∩ Corollary 27. A split structure E on M is a generalized almost product structure if and only if E is. ⊥ Definition 28. Let E be an almost product structure on M. The E-bigrading is the canonical (Z Z)-grading of Ω induced by the decomposition T M = (T M E) M ∗ ∗ × ∩ ⊕ (T M E ) so that the bigraded components are Ωk,l = Γ( k(T M E) l(T M ∗ ∩ ⊥ E ∧ ∗ ∩ ⊗∧ ∗ ∩ k,l E )). We denote by the components of the induced decomposition of . The E⊥-biparity is the (Z/2EEZ/2)-reduction of the E-bigrading. The E-parity isEtMhe Z/2- × grading corresponding to the decomposition ΩM = Ω0E,• ⊕ΩE1,•. Remark 29. The E-biparity is a simultaneous (Z/2 Z/2)-refinement of both the × standard parity and the E-parity. 8 MARCO ALDIANDDANIELEGRANDINI Corollary 30. Generalized almost product structures on M are in canonical bijection with pairs (Ω , ,B), where Ω , denotes a (Z Z)-refinement of the standard grading •• •• × on Ω and B Ω1,1. M ∈ Remark 31. Let E be a generalized almost product structure on M. If B = 0, E 6 then sections of E (and of E ) do not in general have definite E-bigrading. However, ⊥ Proposition 26 implies that Γ(E) ⊆ EE1,0 ⊕EE−1,0 ⊕EE0,1. Remark 32. Let E be a generalized almost product structure on M. By construction, the E-bigrading coincides with the canonical bigrading of the almost product structure (π(E),π(E⊥)), as defined in [7]. In particular, d ∈ EE1,0 ⊕EE−1,2 ⊕EE0,1 ⊕EE2,−1. Definition 33. Given a generalized almost product structure E on M, we define d to E WbeetuhseectohmepsohnoernthtaonfdodndotEat-ipoanrsitLyEof=thLedEdeanRdhaJm, Kop=eraJt,oKr, s.o that dE ∈ EE1,0⊕EE−1,2. E dE Example 34. Let M = S3, let X ,X ,X be a frame of TM with dual frame 1 2 3 { } α ,α ,α such that dα = α α , dα = α α and dα = α α . Given f,g Ω0 , { 1 2 3} 1 2 3 2 3 1 3 1 2 ∈ M consider the split structure E = span α ,α ,x ,x where x = X fα and x = 2 3 2 3 2 2 1 3 { } − X gα . It follows that E = span α ,x , where x = X +fα +gα . Then E is a 3 1 ⊥ 1 1 1 1 2 3 − { } generalized almost product structure for all f,g Ω0 . A direct calculation shows that ∈ M d (hα ) = d (h)α for i = 1,2,3. E i E i Remark 35. If E is a generalized almost product structure on M, then d f = pr (df) E E for every f Ω0 . Moreover, d = d for every B Ω2 . ∈ M E AdB(E) ∈ M Remark 36. Let E be a generalized almost product structure on M. Separating the termsofdifferentE-biparityintheidentityd2 = 0yields[d ,d ] = 0andd2+d2 = 0. In particular, d2 = 0 if and only if d2 = 0 if and onlyEif [dE,⊥d ] = 0. OEn thEe⊥other E E E ⊥ hand (19) [d ,[d ,d ]] = [d ,[d ,d ]] = 2[d ,[d ,d ]] = 0 E E E E E E E E E − ⊥ ⊥ − ⊥ ⊥ for any generalized almost product structure E. Remark37. LetE beageneralizedalmostproductstructureonM andletx,y Γ(E). Then ad = [[ad ,ad ],ad ] is an operator of E-biparity (¯1,¯0) on .∈ Simi- Jx,yKE x dE y EM larly, ad has E-biparity (¯0,¯1). Matching E-biparities yields Jx,yK = pr (Jx,yK) Jx,yK E E E⊥ and Jx,yK = pr (Jx,yK). Similarly if x Γ(E) and y Γ(E ), then Jx,yK = E E ⊥ E ⊥ ⊥ ∈ ∈ pr (Jx,yK). E ⊥ Remark38. LetE beageneralizedalmostproductstructureonM andletx,y Γ(E). ∈ Since by Lemma 14 the components of different E-biparity in (x,y) must vanish d L independently, itfollowsthatinparticular (x,y) = (x,y)foreveryx,y Γ(E). E E L −L ⊥ ∈ Remark 39. Let E be a generalized almost product structure on M. By projecting onto E the axioms of Courant algebroid (written in terms of the Dorfman bracket as in [6]), we conclude that (E,J, K , , ,π ) is a Courant algebroid if and only if J, K E h iE E E satisfies the Jacobi identity i.e. Γ(E) ker( (x,y)) for all x,y, Γ(E). E ⊆ L ∈ GENERALIZED ALMOST PRODUCT STRUCTURES AND GENERALIZED CRF-STRUCTURES 9 Remark 40. Let E be a generalized almost product structure on M. By a result of [14], π(E) is a foliation if and only if d 0,1. If this is the case, we see that in E⊥ ∈ EE particular d2 = d2 0,2. E − E⊥ ∈ EE Proposition 41. Let E be an almost product structure on M. The following are equiv- alent 1) π(E) is a foliation; 2) Ω0 ker( (x,y)) for all x,y Γ(E); M ⊆ LE ∈ 3) Jx,yK Ω1 for all x,y Γ(E); E⊥ ∈ M ∈ 4) (E,J, K , , ,π ) is a Courant algebroid. E E E h i Proof: By Remark 37, 3) is equivalent to (20) 0 = [Jx,yK ,df] = [Jx,yK ,d f] E E E ⊥ ⊥ ⊥ for all x,y Γ(E) and for all f Ω0 . Since Jx,fK = [x,d f] = 0 for all x Γ(E) and f Ω0∈, using Remark 38 w∈e obMtain E⊥ E⊥ ∈ ∈ M (21) ( (x,y))(f) = ( (x,y))(f) = LE⊥ (f) = [Jx,yK ,d f]. LE − LE⊥ Jx,yKE⊥ E⊥ E⊥ Therefore, 2) is equivalent to 3). On the other hand, Lemma 14 implies (22) 2( E(x,y))(f) = [Jx,yKd2 ,f] = Jx,yKd2f L E E for all x,y Γ(E) and for all f Ω0 . By Lemma 14, 4) is equivalent to ∈ ∈ M (23) 0 = [Jx,yKd2,z] = Jy,zK[x,d2] E E for all x,y,z Γ(E). Lemma 20 then implies that [x,d2] is Ω0 -linear and (since x ∈ E M and y are also Ω0M-linear) we obtain that Jx,yKd2Ef = 0 for all x,y ∈ Γ(E) and for all f Ω0 . Therefore, 4) implies 2). Since 4) clearly implies that π(E) is a foliation, it ∈ M remains to prove that 1) implies 4). Let x,y,z be arbitrary sections of E. On the one hand, ( (x,y))(z) has only components of bidegree ( ,q) with q 1 by Remark 31. E L • ≤ Ontheother handby byRemark38andRemark40, ( (x,y))(z) hasonlycomponents E L of E-bigradee ( ,q) with q 2. Therefore, it must vanish and the proof is completed. • ≥ Definition 42. Let E be a generalized almost product structure on M such that π(E ) is a foliation. A differential form is basic with respect to E if it is an element of ⊥ BE = Ω•E,0 ∩ ker(dE⊥). Accordingly, an operator ϕ ∈ EM is basic with respect to E if ϕ( ) . E E B ⊆ B Example 43. Let E be a generalized almost product structure on M such that π(E ) ⊥ is a foliation, then d is basic with respect to E. Moreover d2( ) = d2 ( ) = 0 and E E BE E⊥ BE thus ( ,d ) is a complex known as the basic complex of E. E E B Definition 44. A split structure E is a generalized local product structure on M if (π(E),π(E )) is a local product structure in the sense of [14] i.e. TM = π(E) π(E ) ⊥ ⊥ ⊕ is a decomposition into constant-rank foliations. Proposition 45. A split structure E on M is a generalized local product structure if and only if it is a generalized almost product structure and d2 = 0. E 10 MARCO ALDIANDDANIELEGRANDINI Proof: By Proposition 26, every generalized local product structure is also a generalized almost product structure. By Remark 40, if (π(E),π(E )) is a local product structure, ⊥ then d2 0,2 0,2 = 0,2 2,0 = 0 . Conversely, if d2 = 0 then by (23), π(E) is a E ∈ EE ∩EE⊥ EE ∩EE { } E foliation. By Remark 40, π(E ) is also a foliation and the Proposition is proved. ⊥ Corollary 46. The collection of all split structures on M such that d2 = 0 is in canon- E ical bijection with the collection of pairs (Ω , ,B) consisting of a (Z Z)-refinement •• × of the standard grading on Ω such that d(Ωi,j) Ωi+1,j Ωi,j+1 for all i,j 0 and M ⊆ ⊕ ≥ B Ω1,1. ∈ 4. Generalized F-structures Definition 47. Let E be a split structure on M. A generalized F-structure on E is an element Φ such that M ∈ E i) Ω0 Γ(E ) ker(ad ); ii) adM(⊕Γ(TM⊥)) ⊆Γ(TM)Φ; Φ ⊆ iii) Γ(E) ker(ad2 +Id). ⊆ Φ We denote by J the restriction of ad to Γ(TM) and by L the √ 1-eigenbundle of Φ Φ Φ − J . Φ Remark 48. IfΦisageneralizedF-structureonasplitstructureE,J isanorthogonal Φ bundle endomorphism of TM such that J3 + J = 0 i.e. a generalized F-structure in Φ Φ the sense of [16]. Conversely, given any bundle endomorphism J o(TM), there is an element Φ such that J(x) = ad (x) for all x TM. For i∈nstance, let ω be the M Φ ∈ E ∈ unique 2-form on M such that ω(X,Y) = [X,J(Y)] for all X,Y Γ(TM) and consider ∈ Φ such that Φ(f) = fω for any f Ω0 and ∈ EM ∈ M p (24) Φ(α α ) = α α ω + α J(α ) α 1··· p 1··· k X 1··· i ··· k i=1 for any α ,...,α Ω1 . Then Φ is Ω0 -linear and the restriction of ad to TM 1 p ∈ M M Φ coincideswithJ. Furthermore, supposethatΦ isanotherΩ0 -linearelement such ′ ∈ EM M thatJ(x) = ad (x),thenRemark3impliesΦ Φ Ω0 . Therefore, moduloadditionof Φ′ − ′ ∈ M functions, generalized F-structures on split structures are in canonical correspondence with the split generalized F-structures defined in [2]. Example 49. Every generalized almost complex structure is of the form J for some Φ generalized F-structures Φ on M. Example 50. In the language of [1], every generalized almost contact triple is of the form (J ,e ,e ) for some generalized F-structure Φ on a split structure E such that Φ 1 2 E is globally trivialized by isotropic sections e ,e Γ(E ). If one further imposes ⊥ 1 2 ⊥ ∈ the condition e Γ(TM),e Γ(T M) one obtains the generalized almost contact 1 2 ∗ ∈ ∈ triples of [12]. Remark 51. Since J3 + J = 0, then L is empty if and only if Φ is Ω0 -linear. Φ Φ Φ M Moreover, L E C is maximal isotropic with respect to the tautological inner Φ product and E⊆ C =⊗L L . Φ Φ ⊗ ⊕

See more

The list of books you might like

Most books are stored in the elastic cloud where traffic is expensive. For this reason, we have a limit on daily download.