Abstract

We describe the first order moduli space of heterotic string theory compactifications which preserve N =1 supersymmetry in four dimensions, that is, the infinitesimal parameter space of the Strominger system. We establish that if we promote a connection on T X to a field, the moduli space corresponds to deformations of a holomorphic structure $$ \overline{D} $$ on a bundle $$ \mathcal{Q} $$ . The bundle $$ \mathcal{Q} $$ is constructed as an extension by the cotangent bundle T ∗ X of the bundle E = End(V )⊕End(TX)⊕TX with an extension class $$ \mathcal{H} $$ which precisely enforces the anomaly cancelation condition. The deformations corresponding to the bundle E are simultaneous deformations of the holomorphic structures on the poly-stable bundles V and T X together with those of the complex structure of X. We discuss the fact that the “moduli” corresponding to End(T X) cannot be physical, but are however needed in our mathematical structure to be able to enforce the anomaly cancelation condition. In the appendix we comment on the choice of connection on T X which has caused some confusion in the community before. It has been shown by Ivanov and others that this connection should also satisfy the instanton equations, and we give another proof of this fact.

Highlights

  • In this paper, we study the heterotic string from the ten-dimensional supergravity point of view

  • We describe the first order moduli space of heterotic string theory compactifications which preserve N = 1 supersymmetry in four dimensions, that is, the infinitesimal parameter space of the Strominger system

  • As the stability of both V and T X is not spoiled by first order deformations of J which preserve the holomorphicity condition of both bundles, the theorem by Li and Yau guarantees that on the deformed heterotic compactification (X, V ) there is a connection on V

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Summary

Heterotic supergravity and the Strominger system

The heterotic compactification we are interested in consists on a pair (X, V ) where X is a six dimensional Riemannian spin manifold, together with a vector bundle V on X. This pair has the geometric properties given by. A six-dimensional compact space X with an SU(3)-structure given by a nowhere vanishing three-form Ψ, and a hermitian form ω satisfying the SU(3)-structure compatibility conditions. A connection ∇I on the tangent bundle with curvature RI which satisfies the instanton condition. As discussed in the appendix, this instanton connection is needed to ensure that supersymmetric solutions which satisfy the anomaly cancelation condition, solve the equations of motion.. We will defer the discussion of higher order α corrections to a future companion paper [41], but we comment briefly on the results of that paper in the appendix

Holomorphic structures and moduli
Constraints on the geometry of X
Constraints on the vector bundle V
Constraints from the anomaly cancelation and equations of motion
Infinitesimal moduli of heterotic compactifications
Variations of the complex structure of X
Deformations of the hermitian structure on X
Variations of the holomorphic structure on V
Variations of the holomorphic structure on T X
Constraints from the anomaly cancellation condition
The moduli space of the Strominger system
Conclusions and future directions
Discussion
Future directions
A First order heterotic supergravity
Instanton condition
The hull connection
Note on the choice of connection and higher order corrections
Full Text
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