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FAKE 13-PROJECTIVE SPACES WITH COHOMOGENEITY ONE ACTIONS 6 1 CHENXUHEANDPRIYANKARAJAN 0 2 n a J Abstract. We show that someembedded standard 13-spheres inShimada’s 4 exotic15-sphereshaveZ2quotientspaces,P13s,thatarefakereal13-dimensional 1 projectivespaces,i.e.,theyarehomotopyequivalent,butnotdiffeomorphicto thestandardRP13. AsobservedbyF.Wilhelmandthesecondnamedauthor ] in[RW],theDavisSO(2)×G2actionsonShimada’sexotic15-spheresdescend G to the cohomogeneity one actions on the P13s. We prove that the P13s are D diffeomorphic to well-known Z2 quotients of certain Brieskorn varieties, and thattheDavisSO(2)×G2 actionsontheP13sareequivariantlydiffeomorphic h. to well-known actions on these Brieskornquotients. The P13s areoctonionic t analogues of the Hirsch-Milnorfake5-dimensional projective spaces, P5s. K. a GroveandW.ZillershowedthattheP5sadmitmetricsofnon-negativecurva- m turethatareinvariantwithrespecttotheDavisSO(2)×SO(3)-cohomogeneity [ one actions. In contrast, we show that the P13s do not support SO(2)×G2- invariantmetricswithnon-negativesectional curvature. 1 v 3 Contents 2 7 1. Introduction 2 3 2. Preliminaries 5 0 2.1. Shimada’s exotic 15-spheres Σ15s, the embedded 13- and 14-spheres k . 1 and the Davis action 5 0 2.2. Brieskorn varieties, Kervaire spheres and homotopy projective spaces 8 6 3. The cohomogeneity one actions of G=SO(2) G on S13 and P13 11 1 4. The G-invariant metrics on M13 × 2 k k 17 : k v 5. Rigidities of non-negatively curved metrics 23 i 6. Proof of Theorem 1.8 26 X Appendix A. The computations of Riemann curvature tensors 33 r a A.1. The Riemann curvature tensors in Proposition 5.3 34 A.2. The curvature formula in Lemma 6.2 35 A.3. The Riemann curvature tensors R ,...,R in Lemma 6.5 36 1 10 References 37 2000 Mathematics Subject Classification. 53C20,53C30. 1 2 CHENXUHEANDPRIYANKARAJAN 1. Introduction A fake real projective space is a manifold homotopy equivalent, but not diffeo- morphic, to the standard real projective space. Equivalently, it is the orbit space ofa free exotic involutionon a sphere. A free involutionis calledexotic, if it is not conjugate by a diffeomorphism to the standard antipodal map on the sphere. The firstexamples ofsuch exotic involutions were constructed by Hirsch andMilnor on S5 and S6, see [HM]. They are restrictions of certain free involutions on the im- ages of embedded standard 5- and 6-spheres in Milnor’s exotic spheres [Mi]. Thus the quotient spaces of such embedded S5 and S6 are homotopy equivalent, but not diffeomorphic, to the standard real projective spaces. Theanalogousexotic15-spheresΣ15swereconstructedbyN.Shimadain[Sh]as certain7-spherebundlesoverthe8-sphere. Theantipodalmaponthe7-spherefiber defines a natural involution T on the Σ15s. In [RW], F. Wilhelm and the second named author observed that the images of certain embedded standard 13- and 14- spheresinΣ15sareinvariantundertheinvolution,andthusthequotientspacesare homotopy equivalent to the standard 13- and 14-real projective spaces. Our first main result is the diffeomorphism classification of the quotients. In particular we show the following Theorem 1.1. The quotient spaces of the embedded 13-spheres in certain Shi- mada’s spheres Σ15s are fake real projective spaces, i.e., they are homotopy equiv- alent, but not diffeomorphic to the standard 13-projective space. Remark 1.2. (a) In [RW], they showed that the quotients of the embedded 14- spheres in some Σ15s are not diffeomorphic to the standard RP14 following the Hirsch-Milnor argument. (b) They also observed that the Hirsch-Milnor’s argument breaks down in the case of the embedded 13-spheres as there is an exotic 14-sphere in contrast to the 6-sphere. Our proof of diffeomorphism classification is through the study of the so called Davis action of G = SO(2) G on Shimada’s exotic 15-spheres, where G is the 2 2 simple exceptional Lie group×as the automorphism group of the octonions O. For each odd integer k, denote Σ15 the total space of the 7-sphere bundle over the k 8-sphere, with the Euler class [S8] and the second Pontrjagin class 6k[S8] where [S8] is the standard generator of the cohomology group H8(S8). Shimada showed thateachΣ15 is homeomorphicto the standard15-sphere,but notdiffeomorphic if k k2 1 mod 127, see [Sh]. In [Da](or see Section 2.1), using the octonion algebra, M.6≡DavisintroducedtheactionsofGonΣ15ssuchthatG actsdiagonallyonthe7- k 2 sphere fiber andthe 8-sphere base,whereas SO(2) acts via Mo¨bius transformation. It is observed in [RW], that the Davis action on Σ15 leaves the image S13 of the k k embedded 13-sphere invariant and commutes with the involution T. Thus the restricted action on S13 descends to the quotient space P13 = S13/T. They also k k k observed that the G-actions on S13 and P13 are cohomogeneity one, i.e., the orbit k k spaces are one dimensional. On the other hand, for the cohomogeneityone actions on the homotopy spheres, aside from linear actions on the standard spheres, there are families of non-linear actions [St]. They are examples given by the 2n 1 − dimensional Brieskornvarieties Md2n−1, which are defined by the equations zd+z2+...+z2 =0 and z 2+ z 2+...+ z 2 =1. 0 1 n | 0| | 1| | n| FAKE RP13 WITH COHOMOGENEITY ONE ACTIONS 3 The Brieskorn varieties carry cohomogeneity one actions by SO(2) SO(n) via × (eiθ,A)(z0,z1,...,zn)= e2iθz0,e−idθA(z1,...,zn)t withA SO(n). Anaturalinvolution,de(cid:0)notedbyI,isdefinedbyI((cid:1)z0,z1,...,zn)= ∈ (z , z ,..., z ). It is clear that the involution has no fixed point and commutes 0 1 n awditmh−ittsheaScOoh(−o2m)×ogSenOe(inty)-aocnteioanc;tiaonndbtyhuSsOt(h2e)quSotOie(nnt).spNacoeteNtdh2na−t1w=henMdn2n−=1/7I, the actions on M13 and N13 restricted to the×group G = SO(2) G are also d d × 2 cohomogeneity one. We have the following Theorem 1.3. For each odd integer k, the G-manifolds: the 13-sphere S13 and the k Brieskorn variety M13, with G = SO(2) G are equivariantly diffeomorphic, and so are the quotient spkaces P13 =S13/T a×nd 2N13 =M13/I. k k k k Remark 1.4. Theorem1.1followsfromTheorem1.3aboveandthe diffeomorphism classification of Nd2n−1 in [AB] and [Gi] (or see Section 2.2). Remark 1.5. The space P13, i.e., k = 1, is diffeomorphic to the standard RP13 1 from the construction in [Sh] and [RW]. From Theorem 1.3 above, the known diffeomorphism classification of N13 implies that there are 64 different oriented k diffeomorphism types of P13s. k Remark 1.6. (a) The Davis actions of SO(2) G on Shimada’s exotic spheres 2 Σ15s can be viewed as the octonionic analogs×of the SO(2) SO(3) actions on Mkilnor’s exotic spheres Σ7s found in the same paper [Da]. No×te that SO(3) is the automorphism group of the quaternions, and a special case of the SO(2) SO(3) × actions on a certain Σ7 was found in [GM]. (b) The DavisactionsofSO(2) SO(3)onMilnor’sexotic spheresalsoleavethe × images of the embedded 5-sphere invariant, and hence induce cohomogeneity one actions on the Hirsch-Milnor’s fake 5-projectivespaces as observedin [RW]. These actions are equivariantly diffeomorphic to those on the Brieskorn varieties N5’s, d which was first discovered by E. Calabi(unpublished, cf. [HH, p. 368]) Remark 1.7. In [ADPR], U. Abresch,C.Dura´n, T. Pu¨ttmannandA. Rigasgavea geometricconstructionof free exotic involutions on the Euclideansphere S13 using the wiedersehen metric on the Euclidean sphere S14. Thus the quotient spaces are fake 13-projective spaces. Moreover, in [DP], Dura´n and Pu¨ttmann provided an explicitnonlinearactionofO(2) G ontheEuclideansphereS13,andshowedthat 2 × it is equivariantly diffeomorphic to the Brieskornvariety M13. 3 The second part of this paper is the study of the curvature properties of the invariantmetrics on S13 and P13 with G=SO(2) G . Since any invariant metric on the quotient spacekP13 cankbe lifted to an inv×aria2nt metric on S13, we restrict k k ourselves to the spheres S13s, or equivalently M13s. Note that M13 and M13 are k k k k equivariantly diffeomorphic, and so we assume that k 1. − ≥ On a Riemannian manifold with cohomogeneity one action, the principal or- bits are hypersurfaces, and there are precisely two non-principal orbits that have codimensions strictly bigger than one if the manifold is simply-connected. They are called singular orbits. In [GZ1], K. Grove and W. Ziller constructed invariant metrics with non-negative sectional curvature on cohomogeneity one manifolds for which both singular orbits have codimension two. Particularly, their construction yields non-negativelycurvedmetrics on10 of 14 (unoriented) Milnor’s spheres and 4 CHENXUHEANDPRIYANKARAJAN allHirsch-Milnor’sfake5-projectivespaces. However,noteverycohomogeneityone manifold admits an invariant metric with non-negative curvature. The first exam- ples were found by K. Grove, L. Verdiani, B. Wilking and W. Ziller in [GVWZ], and then generalized to a larger class in [He] by the first named author. The most interesting class in [GVWZ] is the Brieskorn varieties Md2n−1. The Brieskornvari- ety Md2n−1 is homeomorphic to the sphere, if and only if, both n and d are odd. SInO([G2)VWSZO],(nit)iisnvsahroiwanetdmtheatrticfowrinth≥no4n-annedgadti≥ve3c,urMvad2tnu−r1e.dIonespnarotticsuulpapr,orthtearne isnon×on-negativelycurvedSO(2) SO(7)invariantmetriconM13,ifd 3. Since Gis apropersubgroupinSO(2) ×SO(7), there aremoreinvariandtmetric≥s onM13. × k One may suspect that there might be a chance to find an invariant metric with non-negative curvature. Nevertheless we show that the obstruction does appear even though the metric has a smaller symmetry group. Theorem 1.8. For any odd integer k 3, the Brieskorn variety M13 does not support an SO(2) G invariant metric≥with non-negative curvature. k 2 × Remark 1.9. The techniques used to prove Theorem 1.8 are similar to those in [GVWZ]and[He]. Howeverthe specialfeature ofthe LiegroupG andthe strictly 2 larger class of invariant metrics make the argument more involved. Remark 1.10. For the Brieskorn variety M13 with d 4 an even integer, the d ≥ principal isotropy subgroup has a simpler form than the one in the odd case, see Remark2.11. This leadstoa muchmorecomplicatedformofthe invariantmetrics inthe evencase,seeRemark 4.4,whichis notcoveredby ourproof. So foraneven integer d 4, the question whether M13 admits an SO(2) G -invariant metric ≥ d × 2 with non-negative curvature remains open. From Theorems 1.3 and 1.8, we have the following Corollary 1.11. For any odd integer k 3, the fake 13-projective space P13 does not support an SO(2) G invariant met≥ric with non-negative curvature. k 2 × Remark 1.12. In contrastto the P13s, it is observedby O. Dearricottthat, follow- k ing Grove-Ziller’s construction, all fake Hirsch-Milnor’s 5-projective spaces admit SO(2) SO(3) invariant metrics with non-negative curvature, see [GZ1, p. 334]. × Remark 1.13. As observed in [ST], all P13s and S13s support even SO(2) SO(7) k k × invariantmetricsthatsimultaneouslyhavepositiveRiccicurvatureandalmostnon- negativesectionalcurvature. FortheinvariantmetricswithpositiveRiccicurvature alone, it also follows from the result in [GZ2]. A Riemannian manifold admits an almost non-negative sectional curvature if it collapses to a point with a uniform lower curvature bound. From the classification of cohomogeneity one actions on homotopy spheres in [St] by E. Straume, M13s with G = SO(2) G are the only nonlinear actions where the symmetry grokupdoes not have the×form2 SO(2) SO(n). Combining the × classification in [St], the obstructions in [GVWZ] and Theorem 1.8, we have the following Corollary 1.14. For n 2, let Σn be a homotopy sphere. Suppose that Σnadmits ≥ a non-negatively curved metric that is invariant under a cohomogeneity one action. Then either FAKE RP13 WITH COHOMOGENEITY ONE ACTIONS 5 (1) Σn is equivariantly diffeomorphic to the standard sphere and the action is linear, or (2) n = 5, Σ5 is the standard 5-sphere and the non-linear action is given by SO(2) SO(3) on the Brieskorn variety M5, with k 3 odd. × k ≥ We refer to the Table of Contents for the organization of the paper. Theorem 1.3 is proved in Section 3, and Section 6 is the proof of Theorem 1.8. Acknowledgement. It is a great pleasure to thank Frederick Wilhelm who has brought this problem to our attention, and we had numerous discussions with him on this paper. We also thank Wolfgang Ziller for useful communications, and Karsten Grove for his interest. 2. Preliminaries Inthis section,werecallthe Davisactiononthe exotic 15-spheresΣ15s,andthe k Brieskorn varieties with cohomogeneity one action. We refer to [Ba] and [Mu] for the basics of the algebra of the Cayley numbers (i.e., the octonions) and the Lie group G . 2 2.1. Shimada’s exotic 15-spheres Σ15s, the embedded 13- and 14-spheres k and the Davis action. Consider the Cayley numbers O and let u u¯ be the standardconjugation. ArealinnerproductonOisdefinedbyu v =1/7→2(uv¯+vu¯). Let e ,e ,...,e beanorthonormalbasisofOoverRwithe =· 1. Wefollowthe 0 1 7 0 mult{iplications of}elements in O given by [Mu], for example, e e = e , e e = e 1 2 3 1 4 5 and e e =e . Any v O has the following form 1 7 6 ∈ v =v e +v e + +v e . 0 0 1 1 7 7 ··· Denote v = v the real part and v = v e +...+v e the imaginary part. We 0 1 1 7 7 ℜ ℑ have v¯=v e v e ... v e 0 0 1 1 7 7 − − − and v 2 =v2+v2+ +v2 =vv¯. | | 0 1 ··· 7 The unit 7-sphere consists of all unit octonions: S7 = v O: v =1 . { ∈ | | } We write S8 = O O as the union of two copies of O which are glued together φ along O 0 via⊔the following map −{ } (2.1) φ:O 0 O 0 −{ } → −{ } u u φ(u)= . 7→ u2 | | For any two integers m and n, let E be the manifold formed by gluing the two m,n copies of O S7 via the following diffeomorphism on (O 0 ) S7: × −{ } × u um un (2.2) Φ :(u,v) (u,v )= , v . m,n 7→ ′ ′ u2 um un! | | | | | | The natural projection p : E S8 sends (u,v) to u and (u,v ) to u. It m,n m,n ′ ′ ′ gives E the structure of an S7-bu→ndle over S8 with the transition map Φ . m,n m,n The total space E is homeomorphic to S15, if and only if, m+n= 1; see [Sh, m,n ± Section 2]. 6 CHENXUHEANDPRIYANKARAJAN Using the fact that G is the automorphismgroup of O, in [Da], Davis observed 2 that G acts on E as follows: 2 m,n g(u,v)=(g(u),g(v)) and g(u,v )=(g(u),g(v )). ′ ′ ′ ′ From[Da,Remark1.13],theG2-manifoldsEm,nandEm′,n′ areequivariantlydiffeo- morphic, whenever (m,n) = (m,n) or (n,m). Furthermore, the bundles E m,n admit another SO(2) symmet±ry via Mo¨b±ius transformations that commutes with the G -action. Write an element γ SO(2) as 2 ∈ a b (2.3) γ =γ(a,b)= and a2+b2 =1. b a (cid:18)− (cid:19) In terms of the coordinate charts, the action on the sphere bundle E is defined m,n by (2.4) γ⋆u = (au+b)( bu+a)−1 − γ⋆u = ( b+au)(a+bu) 1 ′ ′ ′ − − and ( bu+a)mv( bu+a)n (2.5) γ⋆v = − − bu+am+n |− | (a+bu¯)mv (a+bu¯)n ′ ′ ′ γ⋆v = . ′ a+bu¯ m+n | ′| The formulas above are compatible with the transition map Φ . Davis showed m,n the following Lemma 2.1 (Davis). The formulas (2.4) and (2.5) give a well-defined action of SO(2) on E . Furthermore the action is G -equivariant, and for any v O(not m,n 2 ∈ necessarily unit) we have γ⋆v = v and γ⋆v = v . ′ ′ | | | | | | | | Suppose now that m+n=1 and k =m n. So k is an odd number and − k+1 k+1 (2.6) m= and n= − . 2 2 We set Σ15 = E , and note that it is homeomorphic to the 15-sphere. A Morse k m,n function on Σ15 in [Sh] is given by k v (u(v ) 1) ′ ′ − (2.7) f (x)= ℜ = ℜ . 1 1+ u2 1+ u(v ) 1 2 | | | ′ ′ − | q q Note that f has only two critical points as (u,v)=(0, 1). Set 1 ± (2.8) S1k4 =f1−1(0)= x∈Σ1k5 :ℜv =ℜ(u′(v′)−1)=0 anditisdiffeomorphictothestan(cid:8)dardS14 forallk. Considerthef(cid:9)ollowingfunction on S14: k (uv) v ′ (2.9) f (x)= ℜ = ℜ . 2 1+ u2 1+ u 2 | | | ′| q q FAKE RP13 WITH COHOMOGENEITY ONE ACTIONS 7 It is straightforward to verify that on S14, the function f has precisely two non- k 2 degenerate critical points as (u,v )=(0, 1). It follows that ′ ′ ± S1k3 = f2−1(0)∩S1k4 (2.10) = x Σ : (uv)= v = v = (u(v ) 1)=0 Σ15 ∈ k ℜ ℜ ℜ ′ ℜ ′ ′ − ⊂ k is diffeomorphic to(cid:8)the standard 13-sphere for all k. Let (cid:9) (2.11) T : E E m,n m,n → (u,v) (u, v) and (u,v ) (u, v ) ′ ′ ′ ′ 7→ − 7→ − be the antipodal map on the fiber S7. The two spheres S14 and S13 are invariant k k under this involution T. Denote P14 =S14/T and P13 =S13/T k k k k the quotient spaces. Remark 2.2. Note thatMilnor’sexotic 7-spheresΣ7sarediffeomorphic to 3-sphere bundles overthe 4-sphere. The involutionT on Σ15s is the analogueof the natural involution on Σ7s given by the antipodal map of the 3-sphere fiber, see [Mi] and [HM]. In [RW], Wilhelm and the second named author observedthat the Davis action of G = SO(2) G on Σ15 leaves both S14 and S13 invariant and commutes with × 2 k k k the involution T. Lemma 2.3. The SO(2) G action on Σ15 restricts to an action on the spheres S14, S13 and descends to t×he q2uotient spaceskP14, P13. k k k k Proof. It is easy to see that the action commutes with the involution T. So it is sufficient to show that the defining conditions of S13 and S14 in Σ15 are preserved k k k bytheSO(2) G action. InthefollowingwegiveaproofforS13,andtheargument for S14 is sim×ilar2. k k Since G is the automorphism group of O, it is easy to see that the defining 2 conditions are preserved. Next we consider the action by SO(2). Let γ =γ(a,b) in equation (2.3). Note that (xy)= (yx) for any x,y O. We have ℜ ℜ ∈ 1 (γ⋆v) = (a bu)mv(a bu)n ℜ a bu ℜ{ − − } | − | 1 = (a bu)m+nv a bu ℜ − | − | 1 (cid:8) (cid:9) = (a v b (uv)) a bu ℜ − ℜ | − | = 0, and 1 ((γ⋆u)(γ⋆v)) = (au+b)(a bu)−1(a bu)mv(a bu)n ℜ a bu ℜ − − − | − | 1 (cid:8) (cid:9) = (au+b)v a bu ℜ | − | = 0. 8 CHENXUHEANDPRIYANKARAJAN For the coordinates (u,v ), since u(v ) 1 = uv¯/ v 2 and u(v ) 1 = 0; it ′ ′ ′ ′ − ′ ′ ′ ′ ′ − | | ℜ follows that (u¯v )=0. Similar to the case of (u,v), we have ′ ′ ℜ (cid:0) (cid:1) 1 (γ⋆v ) = (a+bu¯)mv (a+bu¯)n ′ ′ ′ ′ ℜ a+bu¯ ℜ{ } | ′| 1 = (a+bu¯)v ′ ′ a+bu¯ ℜ{ } | ′| = 0 and (γ⋆u)(γ⋆v ) 1 = a+bu¯ ( b+au)(a+bu) 1(a+bu¯) n(v ) 1(a+bu¯) m ′ ′ − ′ ′ ′ − ′ − ′ − ′ − ℜ | |ℜ − (cid:0) (cid:1) = a+bu¯′ (cid:8)( b+au′)(a+bu′)−1(a+bu¯′)−1(v′)−1 (cid:9) | |ℜ − = a+bu¯ a(cid:8)2+b2 u 2+ab(u +u¯) ( b+au)((cid:9)v ) 1 ′ ′ ′ ′ ′ ′ − | | | | ℜ − = 0. (cid:16) (cid:17) (cid:8) (cid:9) This shows that S13 is invariant under the SO(2) action, which finishes the proof. k (cid:3) Remark 2.4. In [RW], following the Hirsch-Milnor argument in [HM], they also showedthatP14 andP13 arehomotopyequivalenttothe standardRP14 andRP13 k k for all k; and P14 is not diffeomorphic to RP14, when k 3,5 mod 8. k ≡ 2.2. Brieskornvarieties,Kervairespheresandhomotopyprojectivespaces. F(2onr an1y)-idnitmegeenrssionna≥l su3bmanadnidfol≥d o1f,Cthn+e1B,rdieefisknoerdnbvyartiheetyeqMuad2tni−on1sis the smooth − zd+z2+ +z2 = 0 0 1 ··· n z 2+ z 2+ + z 2 = 1. (cid:26) | 0| | 1| ··· | n| When d = 1, M12n−1 is diffeomorphic to the standard sphere S2n−1; and when d=2, M22n−1 is diffeomorphic to the unit tangent bundle of Sn. Thohmeeoormemorp2hi.c5t(oBtrhieesksotarnnd).arSdusppphoesreenS2≥n 31,ainfdandd≥on2l.y iTf,hebomthannifaonldd Md da2nre−1odids − numbers. Assume that n and d are odd numbers, it is the Kervaire sphere, if and only if, d 3 mod 8. ≡± Remark 2.6. The Kervaire sphere is known to be exotic if n 1 mod 4. ≡ Denote I the following involution on Md2n−1: (z ,z ,...,z ) (z , z ,..., z ). 0 1 n 0 1 n 7→ − − Clearly it is fixed-point free. Atiyah and Bott showed the following result, see also [Gi, Corollary 4.2]. Theorem 2.7 ([AB, Theorem 9.8]). If the involution I on the topological spheres Md4m−3 and Mk4m−3 are isomorphic, then d k mod 22m. ≡± In particular the involution I acting on M34m−3 = S4m−3 is not isomorphic to the standard antipodal map whenever m 2. ≥ Corollary 2.8. There are 64 smoothly distinct real projective spaces M13/I with k k =1,3,...,127. FAKE RP13 WITH COHOMOGENEITY ONE ACTIONS 9 The group G˜ =SO(2)×SO(n) acts on Md2n−1 by eiθ,A (z ,Z)= e2iθz ,e idθAZ , for (z ,Z) C Cn. 0 0 − 0 ∈ ⊕ Note that o(cid:0)ur con(cid:1)vention is (cid:0)different from th(cid:1)e one in [GVWZ], as we have e idθ − for the action of eiθ on Z = (z ,...,z )t. The norm z is invariant under this 1 n 0 | | action, and two points belong to the same orbit if and only if they have the same valueof z . Lett bethe uniquepositivesolutionoftd+t2 =1,andthenwehave | 0| 0 0 0 0 z t . It follows that the orbitspace is [0,t ]. The orbit types and isotropy 0 0 0 ≤| |≤ subgroups of this action have been well-studied, see for example, [HH], [BH] and [GVWZ]. In our case, we assume that d is odd. When n =7, the embedding G SO(7) 2 induces the action of G=SO(2) G on M13. To describe the isotropy su⊂bgroups of the G-action we introduce the×follo2wing sdubgroups in G : 2 Denote O(6), the subgroup in SO(7) that maps e to e , SO(6) the sub- 1 1 • group that fixes e , and SU(3)=SO(6) G . ± 1 2 The other subgroup in G that fixes e∩ is denoted by SU(3) , and the 2 3 3 • complex structure on C3 = spanR e1,e2,e4,e7,e6,e5 is given by the left { } multiplication of e . Note that 3 (SO(2) SO(5)) G =U(2) SU(3) 2 3 × ∩ ⊂ whereSO(2) SO(5) SO(7)hastheblock-diagonalform,andtheembed- ding U(2) ×SU(3) is⊂given by h diag (deth) 1,h . To see this, take 3 − A=diag ⊂A ,A (SO(2) SO(7→5)) G with 1 2 2 { }∈ × ∩ (cid:8) (cid:9) cost sint A = 1 sint cost (cid:18)− (cid:19) for some t. Since e =e e , we have 3 1 2 A(e ) = A(e )A(e ) 3 1 2 = (e cost+e sint)( e sint+e cost) 1 2 1 2 − = e 3 and thus A SU(3) . Using the complex structure of SU(3) , A acts on 3 3 1 C=spanR e∈1,e2 byeit,andA2actsinvariantlyonC2 =spanR e4,e7,e6,e5 . So the elem{ent A}embeds diagonally in SU(3) with (1,1)-entry{eit. } 3 The common subgroup SU(2) = SU(3) SU(3) and it is also given by 3 • SU(2) = SO(4) G where SO(4) SO(∩7) as A diag I ,A and I is 2 3 3 ∩ ⊂ 7→ { } the identity matrix. Since G acts transitively on S6 = v O: v =0 and v =1 with SU(3) and 2 SU(3) as isotropy subgroups at e a{nd∈e resℜpectively, th|es|e two}groups are con- 3 1 3 jugate by an element in G . 2 We follow the notions in [GVWZ] to determine the isotropy subgroups. Denote B the singular orbit with z = 0, and choose p = (0,1,i,0,...,0) B with 0 iso−tropy subgroup K . We|als|o denote B the sin−gular orbit with z ∈= t−, and − + 0 0 | | choose p =(t ,i td,0,...,0) with isotropy subgroupK+. Note that B and B + 0 0 + − have codimensions 2 and n 1 = 6 respectively. Let c(t) be a normal minimal p − geodesic connecting p = c(0) and p = c(L). The isotropy subgroup at c(t)(0 < + t<L) stays unchange−d that is the principal isotropy subgroup H. We have 10 CHENXUHEANDPRIYANKARAJAN Theorem 2.9. The cohomogeneity one action of G = SO(2) G on M13 with d × 2 d odd has the following isotropy subgroups: (1) The principal isotropy subgroup is H=Z SU(2)=(ε,diag ε,ε,1,A ) 2 · { } where ε= 1 and A is a 4 4-matrix. ± × (2) At p , the isotropy subgroup is − cosdθ sindθ K =SO(2)SU(2)= eiθ,diag ,1,A − sindθ cosdθ (cid:18) (cid:26)(cid:18)− (cid:19) (cid:27)(cid:19) where A is a 4 4-matrix. × (3) At p , the isotropy subgroup is + K+ =O(6) G =(detB,diag detB,B ) 2 ∩ { } where B O(6) G . 2 ∈ ∩ Remark 2.10. Denote j, the complex structure given by the left multiplication of e . For the group H, we have diag ε,ε,1,A (SO(2) SO(5)) G and A 3 2 U(2) SU(3) with detA=ε. For th{e group K} ∈, we have× ∩ ∈ 3 − ⊂ cosdθ sindθ diag ,1,A (SO(2) SO(5)) G sindθ cosdθ ∈ × ∩ 2 (cid:26)(cid:18)− (cid:19) (cid:27) and A U(2) SU(3) with detA=e jdθ. 3 − ∈ ⊂ Remark 2.11. If d is an even integer, then the isotropy subgroup K is the same − as in the case d odd. The other two isotropy subgroups are H=Z SU(2)=(ε,diag I ,A ) 2 3 × { } K+ =Z SU(3)=(ε,diag 1,B ) 2 × { } where ε= 1, A SO(4) G =SU(2) and B SO(6) G =SU(3). 2 2 ± ∈ ∩ ∈ ∩ ClearlytheG-actioncommuteswiththeinvolutionI andhenceinducesanaction on N13 = M13/I. Write [z ,z ,...,z ] N13, the equivalent class under the d d 0 1 7 ∈ d involution I. Corollary 2.12. The cohomogeneity one action of G = SO(2) G on N13 = × 2 d M13/I with d odd, has the following isotropy subgroups. d (1) The principal isotropy subgroup is H¯ =Z (Z SU(2))=(ε ,diag ε ,ε ,1,A ) 2 2 1 2 2 × · { } where ε = 1 and A is a 4 4-matrix. 1,2 ± × (2) The singular isotropy subgroup at [0,1,i,0,...,0] is cosdθ sindθ K¯ =Z SO(2)SU(2)= eiθ,diag ε ,1,A − 2· sindθ cosdθ (cid:18) (cid:26) (cid:18)− (cid:19) (cid:27)(cid:19) where ε= 1 and A is a 4 4-matrix. ± × (3) The singular isotropy subgroup at [t ,i td,0,...,0] is 0 0 K¯+ =Z (O(6) G )=(εp,diag detB,B ) 2 2 × ∩ { } where ε= 1 and B O(6) G . 2 ± ∈ ∩

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