Adapted complex tubes on the symplectization of pseudo-Hermitian manifolds

preprint2010arXivOpen access

Abstract

Let (M,ω)(M,ω) be a pseudo-Hermitian space of real dimension 2n+12n+1, that is $\RManBase$ is a $\CR-$manifold of dimension 2n+12n+1 and ωω is a contact form on MM giving the Levi distribution HT(M)⊂TMHT(M)\subset TM. Let Mω⊂T∗MM^ω\subset T^*M be the canonical symplectization of (M,ω)(M,ω) and MM be identified with the zero section of MωM^ω. Then MωM^ω is a manifold of real dimension 2(n+1)2(n+1) which admit a canonical foliation by surfaces parametrized by C∋t+iσ↦ϕp(t+iσ)=σωgt(p)\mathbb{C}\ni t+iσ\mapsto ϕ_p(t+iσ)=σω_{g_t(p)}, where $p\inM$ is arbitrary and gtg_t is the flow generated by the Reeb vector field associated to the contact form ωω. Let JJ be an (integrable) complex structure defined in a neighbourhood UU of MM in MωM^ω. We say that the pair (U,J)(U,J) is an {adapted complex tube} on MωM^ω if all the parametrizations ϕp(t+iσ)ϕ_p(t+iσ) defined above are holomorphic on ϕp−1(U)ϕ_p^{-1}(U). In this paper we prove that if (U,J)(U,J) is an adapted complex tube on MωM^ω, then the real function EE on Mω⊂T∗MM^ω\subset T^*M defined by the condition α=E(α)ωπ(α)α=E(α)ω_{π(α)}, for each α∈Mωα\in M^ω, is a canonical equation for MM which satisfies the homogeneous Monge-Ampère equation (ddcE)n+1=0(dd^c E)^{n+1}=0. We also prove that if MM and ωω are real analytic then the symplectization MωM^ω admits an unique maximal adapted complex tube.

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