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A survey on strong KT structures - SSMR

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104 Anna Fino and Adriano TomassiniC<<strong>strong</strong>>on</<strong>strong</strong>>sider the inner product g defined byg =6∑e j ⊗ e j . (2)j=1Thus g is J-Hermitian. Denote by F the fundamental 2-form associated with theHermitian structure (J,g). By a direct computati<<strong>strong</strong>>on</<strong>strong</strong>> we haveJdF = −e 1 ∧ e 2 ∧ e 3 ,with e 1 ∧ e 2 ∧ e 3 a closed and n<<strong>strong</strong>>on</<strong>strong</strong>>-exact 3-form.Therefore g admits a str<<strong>strong</strong>>on</<strong>strong</strong>>g <strong>KT</strong> structure defined by (J,g). The Bismut c<<strong>strong</strong>>on</<strong>strong</strong>>necti<<strong>strong</strong>>on</<strong>strong</strong>>∇ B in this case is flat. Indeed, the torsi<<strong>strong</strong>>on</<strong>strong</strong>> of ∇ B is the 3-formJdF = −e 1 ∧ e 2 ∧ e 3 .Hence, the torsi<<strong>strong</strong>>on</<strong>strong</strong>> forms τ i ,i = 1,...,6 of ∇ B are given byτ 1 = e 2 ∧ e 3 , τ 2 = −e 2 ∧ e 3 , τ 3 = e 1 ∧ e 2 , τ 4 = 0, τ 5 = 0, τ 6 = 0.Denoting by ω i j the c<<strong>strong</strong>>on</<strong>strong</strong>>necti<<strong>strong</strong>>on</<strong>strong</strong>>s 1-forms of ∇B , by the Cartan structure equati<<strong>strong</strong>>on</<strong>strong</strong>>s6∑de i + ωj i ∧ e j = τ i , ωj i + ω j ij=1= 0, i,j = 1,...,6, (3)we immediately getω 5 6 = e 4 ,the other ω i j being zero. Hence ∇B is flat and c<<strong>strong</strong>>on</<strong>strong</strong>>sequently its hol<<strong>strong</strong>>on</<strong>strong</strong>>omy algebrais trivial. Moreover, the Lee form, given by e 4 is closed and then the Hermitianmetric is locally c<<strong>strong</strong>>on</<strong>strong</strong>>formally balanced. The simply c<<strong>strong</strong>>on</<strong>strong</strong>>nected Lie group H withLie algebra h is a semi-direct product of the form IR⋉IR 2 and by c<<strong>strong</strong>>on</<strong>strong</strong>>sidering thelattice Γ in H generated by 1 2 and Z2 , <<strong>strong</strong>>on</<strong>strong</strong>>e has that b 1 (Γ\H) = 1. Therefore, theabove Hermitian structure (J,g) <<strong>strong</strong>>on</<strong>strong</strong>> g induces a left-invariant Hermitian structure(J,g) <<strong>strong</strong>>on</<strong>strong</strong>> the compact manifold M = Γ\H ×S 3 /K, which can be viewed as a n<<strong>strong</strong>>on</<strong>strong</strong>>trivialT 2 -bundle over the Hopf surface. Note that∂ ( η 1 ∧ η 2 ∧ η 3) = 1 2 (1 − i) η1 ∧ η 1 ∧ η 2 ∧ η 3 ,and thus there are no left-invariant holomorphic (3,0)-forms <<strong>strong</strong>>on</<strong>strong</strong>> M. Since thehol<<strong>strong</strong>>on</<strong>strong</strong>>omy of the Bismut c<<strong>strong</strong>>on</<strong>strong</strong>>necti<<strong>strong</strong>>on</<strong>strong</strong>> is c<<strong>strong</strong>>on</<strong>strong</strong>>tained in SU(3), then by [16, Theorem4.1] (M,J) cannot admit any n<<strong>strong</strong>>on</<strong>strong</strong>>-vanishing holomorphic (3,0)-form. Indeed, if(M,J) admits such a form, then (J,g) has to be c<<strong>strong</strong>>on</<strong>strong</strong>>formally balanced, but thisis not possible since (J,g) is str<<strong>strong</strong>>on</<strong>strong</strong>>g <strong>KT</strong>.

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