Abstract

We construct novel classes of compact G2 spaces from lifting type IIA flux backgrounds with O6 planes. There exists an extension of IIA Calabi-Yau orientifolds for which some of the D6 branes (required to solve the RR tadpole) are dissolved in F2 fluxes. The backreaction of these fluxes deforms the Calabi-Yau manifold into a specific class of SU(3)-structure manifolds. The lift to M-theory again defines compact G2 manifolds, which in case of toroidal orbifolds are a twisted generalisation of the Joyce construction. This observation also allows a clear identification of the moduli space of a warped compactification with fluxes. We provide a few explicit examples, of which some can be constructed from T-dualising known IIB orientifolds with fluxes. Finally we discuss supersymmetry breaking in this context and suggest that the purely geometric picture in M-theory could provide a simpler setting to address some of the consistency issues of moduli stabilisation and de Sitter uplifting.

Highlights

  • For that we first use the observation of Kachru and McGreevy [11] that compact G2 spaces obtained from desingularising certain orbifolds of T7 have a simple IIA dual description in terms of IIA Calabi-Yau (CY) orientifolds

  • In this paper we have argued that a class of supersymmetric IIA flux compactifications to 4d N = 1 Minkowski vacua are in one-to-one correspondence with compactifications of 11-dimensional supergravity on new G2 spaces

  • The IIA flux compactifications for which this works are constrained by demanding that the only sources are O6 planes and D6 branes and the only fluxes are RR F2 fluxes

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Summary

General discussion

Since the IIA flux vacua of concern feature O6/D6 sources, a non-constant dilaton, and F2 flux they lift to pure geometry in 11d. In the case of vanishing two-form flux, each O6-plane comes with two D6-branes that cancel its charge The uplift of this setup to the sevendimensional manifold in M-theory naturally corresponds to a (R3 × S1)/Z2 singularity, whose appearance suggests non-Abelian gauge theories. For this construction to be consistent, we have to ensure that gluing in such a double cover of Atiyah-Hitchin space is consistent with the non-trivial SU(3) structure obeying (2.7) Note that this construction of G2 spaces is closely related to the construction obtained by lifting Calabi-Yau orientifolds in which the 7-dimensional manifold has a covering space that corresponds to a direct product of a circle with the Calabi-Yau 3-fold. It turns out that with a non-trivial twist of the circle a G2 space can still be defined on the condition that the SU(3) holonomy gets relaxed into a more general SU(3) structure

An example from its type IIB mirror
Comments on RR tadpoles
Moduli spaces
Closed string sector
Open string sector
Examples
A simple example without flux
With fluxes
A class of examples
Comments on supersymmetry breaking
A non-homogenous extension of the Scherk-Schwarz mechanism
Non-perturbative quantum effects and uplifting?
Discussion
A Conventions
B Localised O6 solution
Full Text
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