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On metrics on 2-orbifolds all of whose geodesics are closed

  • Christian Lange ORCID logo EMAIL logo

Abstract

We show that the periods and the topology of the space of closed geodesics on a Riemannian 2-orbifold all of whose geodesics are closed depend, up to scaling, only on the orbifold topology and compute it. In the manifold case we recover the fact proved by Gromoll, Grove and Pries that all prime geodesics have the same length, without referring to the existence of simple geodesics. We partly strengthen our result in terms of conjugacy of contact forms and explain how to deduce rigidity on the projective plane based on a systolic inequality due to Pu.

Funding statement: The author is partially supported by the DFG funded project SFB/TRR 191 “Symplectic Structures in Geometry, Algebra and Dynamics”.

A Appendix

A.1 Rigidity on the real projective plane

For a Riemannian metric g on 𝒪=2 we denote its corresponding area measure by νg, its total area by Ag and the length of a shortest non-contractible loop by ag. The following inequality is due to Pu [25]:

Ag2πag2.

We recall its proof and show how it implies rigidity for Besse metrics on 2. This argument was explained to us by A. Abbondandolo.

Table 1

Orbifolds of geodesics and (labeled) geodesic periods of Besse 2-orbifolds. For definitions and notations see Sections 2.1 and 2.7. Expressions that only hold in the good orbifold case, i.e. when p=q, are stated in parentheses. For the good orbifolds 𝒪=S2/G, G<O(3), appearing in the table the second column specifies G in terms of the Schönflies notation, see for example [19]). Recall that G+=GSO(3), G×={gG:det(g)g} and G*=G,-1. A detailed discussion of the finite subgroups of O(3) and their relations can for instance be found in [19].

(G<O(3))𝒪(S2/G)𝒪g(S2/G×)𝒪g/i(S2/G*)geod. periods
(G<SO(3), G=G+)(S2/G)(S2/G*)
(Cp)S2(p,q)
012(p+q), 2pqS2/Cp+q2S2/Cp+q2h(1,p+q2¯)
2(p+q), 2pqS2/Cp+q2S2/Sp+q(p+q2¯)
01’2(p+q), 2pqS2/Cp+qS2/Cp+qh(1,p+q¯)
02D2nS2(2,2,2n)S2/D2nS2/D2nh(1,2,2,2n)
03D2n+1S2(2,2,2n+1)S2/D2n+1S2/D2n+1d(1,2¯,2n+1)
04TS2(2,3,3)S2/TS2/Th(1,2,3¯)
05OS2(2,3,4)S2/OS2/Oh(1,2,3,4)
06IS2(2,3,5)S2/IS2/Ih(1,2,3,5)
(-1GSO(3), GG×)(S2/G×)(S2/G*)
(Cpv)D2(;p,q)
072(p+q), 2pqS2/Dp+q2S2/Dp+q2h(1,p+q2)
2(p+q), 2pqS2/Dp+q2S2/Dp+q2d(1,p+q2)
07’2(p+q), 2pqS2/Dp+qS2/Dp+qh(1,2,p+q)
08S4n2(2n)S2/C4nS2/C4nh(1,4n¯)
09C2n+1hD2(2n+1;)S2/C4n+2S2/C4n+2h(1,2n+1¯)
10D2ndD2(2;2n)S2/D4nS2/D4nh(1,2,4n)
11D2n+1hD2(;2,2,2n+1)S2/D4n+2S2/D4n+2h(1,2,2n+1)
12TdD2(;2,3,3)S2/OS2/Oh(1,3,4)
(-1G=G*G+×2)(S2/G+)(S2/G)
13S4n+22(2n+1)S2/C2n+1S2/S4n+2(2n+1¯)
14C2nhD2(2n;)S2/C2nS2/C2nh(1,n¯)
15D2n+1dD2(2;2n+1)S2/D2n+1S2/D2n+1d(1,2n+1)
16D2nhD2(;2,2,2n)S2/D2nS2/D2nh(1,n)
17ThD2(3;2)S2/TS2/Th(1,3¯)
18OhD2(;2,3,4)S2/OS2/Oh(1,2,3)
19IhD2(;2,3,5)S2/IS2/Ih(1,3,5)

Suppose that g is some Riemannian metric on 2 and let g0 be the standard Riemannian metric on 2 of constant curvature 1. The group G=SO(3) acts on 2 in its standard way. By the uniformization theorem there is some positive smooth function φ on 2 such that g=φg0. We endow G with its Haar measure μ and define

φ¯=(G(g*φ)12𝑑μ)2

and g¯=φ¯g0. By construction g¯ is a G-invariant Riemannian metric on M=2 and hence has constant curvature. We claim that AgAg¯ and ag¯ag . Indeed, we have

Ag¯=Mφ¯𝑑νg0=M(G(h*φ)12𝑑μ)2𝑑νg0M(Gh*φ𝑑μ)𝑑νg0=G(Mh*φ𝑑νg0)𝑑μ=GAg𝑑μ=Ag,

where we have applied the Cauchy–Schwarz inequality. Moreover, with a shortest non-contractible loop (and hence geodesic) γ on 2 with respect to g¯ we have

ag¯=01φ¯(γ(s))12γ˙(s)g0𝑑s=01(G((h*φ)(γ(s)))12γ˙(s)g0𝑑μ)𝑑s=G(01((h*φ)(γ(s)))12γ˙(s)g0𝑑s)𝑑μGag𝑑μ=ag.

In particular, this proves Pu’s inequality, since we have Ag¯=2πag¯2 for the metric of constant curvature g¯ (see [25]). Now suppose that g is Besse. Theorem 4.1 implies that the same equality also holds for the Besse metric g. In fact, after normalizing g such that ag=π, Theorem 4.1 implies vol(T12,α0dα0)=vol(T12,αdα) which in turn implies Ag=2π by fiberwise integration with respect to T122. (Alternatively, this follows from a theorem of Weinstein: The two-fold covering (S2,g^) of (2,g) has area 2Ag and the minimal geodesic period is 2ag due to the fact that 𝒪gS2. Now the theorem by Weinstein says that for a Besse metric g^ on S2 we have area(S2,g^)=l2π, where l is the minimal geodesic period [33], cf. [3, Proposition 2.24].) It follows that Ag¯=Ag, i.e. we have equality in the Cauchy–Schwarz inequality implying that φ is constant. Hence, g is proportional to g0 and has constant curvature.

Acknowledgements

The author would like to thank Alexander Lytchak for drawing his attention to the subject. He is grateful to Alberto Abbondandolo for explaining to him how this paper’s result combined with work by Pu implies rigidity on the real projective plane (see Section A.1). He thanks the referee for critical comments and suggestions that helped to improve the exposition. The research in this paper is part of a project in the SFB/TRR 191 “Symplectic Structures in Geometry, Algebra and Dynamics”. A partial support is gratefully acknowledged.

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Received: 2016-05-26
Revised: 2017-09-22
Published Online: 2018-01-13
Published in Print: 2020-01-01

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