Gluing construction of compact Spin(7)-manifolds

preprint2015arXivOpen access

Abstract

We give a differential-geometric construction of compact manifolds with holonomy Spin(7)\mathrm{Spin}(7) which is based on Joyce's second construction of compact Spin(7)\mathrm{Spin}(7)-manifolds in \cite{Joyce00} and Kovalev's gluing construction of G2G_2-manifolds in \cite{Kovalev03}. We also give some examples of compact Spin(7)\mathrm{Spin}(7)-manifolds, at least one of which is \emph{new}. Ingredients in our construction are \emph{orbifold admissible pairs with} a compatible antiholomorphic involution. Here in this paper we need orbifold admissible pairs (X‾,D)(\overline{X}, D) consisting of a four-dimensional compact Kähler orbifold X‾\overline{X} with isolated singular points modelled on C4/Z4\mathbb{C}^4/\mathbb{Z}_4, and a smooth anticanonical divisor DD on X‾\overline{X}. Also, we need a compatible antiholomorphic involution σσ on X‾\overline{X} which fixes the singular points in X‾\overline{X} and acts freely on the anticanoncial divisor DD. If two orbifold admissible pairs (X‾1,D1)(\overline{X}_1, D_1), (X‾2,D2)(\overline{X}_2, D_2) with dim⁡CX‾i=4\dim_{\mathbb{C}} \overline{X}_i = 4 and compatible antiholomorphic involutions σiσ_i on X‾i\overline{X}_i satisfy the \emph{gluing condition}, we can glue (X‾1∖D1)/⟨σ1⟩(\overline{X}_1 \setminus D_1)/\braket{σ_1} and (X‾2∖D2)/⟨σ2⟩(\overline{X}_2 \setminus D_2)/\braket{σ_2} together to obtain a compact Riemannian 88-manifold (M,g)(M, g) whose holonomy group Hol(g)\mathrm{Hol}(g) is contained in Spin(7)\mathrm{Spin}(7). Furthermore, if the A^\widehat{A}-genus of MM equals 11, then MM is a Spin(7)\mathrm{Spin}(7)-manifold, i.e., a compact Riemannian manifold with holonomy Spin(7)\mathrm{Spin}(7). We shall investigate our gluing construction using (X‾i,Di)(\overline{X}_i,D_i) with i=1,2i=1,2 when D1=D2=DD_1=D_2=D and DD is a complete intersection in a weighted projective space, as well as when (X‾1,D1)=(X‾2,D2)(\overline{X}_1,D_1)=(\overline{X}_2,D_2) and σ1=σ2σ_1=σ_2 (the \emph{doubling} case).

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