M-theory moduli spaces and torsion-free structures

Motivated by the description of N=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \mathcal{N}=1 $$\end{document} M-theory compactifications to four-dimensions given by Exceptional Generalized Geometry, we propose a way to geometrize the M-theory fluxes by appropriately relating the compactification space to a higher-dimensional manifold equipped with a torsion-free structure. As a non-trivial example of this proposal, we construct a bijection from the set of Spin(7)-structures on an eight-dimensional S1-bundle to the set of G2-structures on the base space, fully characterizing the G2-torsion clases when the total space is equipped with a torsion-free Spin(7)-structure. Finally, we elaborate on how the higher-dimensional manifold and its moduli space of torsion-free structures can be used to obtain information about the moduli space of M-theory compactifications.


Introduction
In the context of String/M-theory compactifications, supersymmetry implies the existence of a topological G-structure satisfying a particular set of differential conditions on the appropriate principal bundle over the internal manifold. In particular, this set of differential conditions can be written as first-order partial differential equations on the tensors that define the G-structure. The moduli space of a given supersymmetric compactification is an important space from the physics point of view; it is expected to be a finite-dimensional manifold equipped with a Riemannian metric closely related to the non-linear sigma-model appearing in the effective supergravity action of the compactification. In the simplest cases, namely in the absence of fluxes, the topological reduction is on the frame bundle of the internal space and the differential conditions implied by supersymmetry are equivalent to imposing the G-structure to be torsion-free [1,2], meaning that the reduction is not only topological but also geometric. Usually the moduli space of this torsion-free structures is well under control when the internal space is an oriented, compact manifold [3,4]. In particular, the Riemannian metric is known and thus it can be used to explicitly write the effective action of the compactification [5,6].
From the phenomenological point of view, realistic scenarios require the moduli spaces to be just isolated points, and for that the presence of non-vanishing fluxes is crucial. 1 This implies that the topological G-structure induced by supersymmetry will have nonvanishing torsion [9,10], always subject to the corresponding differential equations. It is JHEP05(2015)085 thus desirable to have a better understanding of the moduli space in the presence of fluxes, in order to find as explicitly as possible the four-dimensionl models coming from String/Mtheory compactifications, that can ultimately be used to make contact with particle physics or cosmology.
A huge effort has been devoted so far in understanding the supersymmetric compactifications, see [11] and references therein. One approach, namely generalized geometry either in its complex [12,13] or exceptional flavour [14,15], has proven to be particularly interesting and fruitful, giving a unified geometrical description of the different flux backgrounds as well as their moduli spaces [15][16][17][18][19][20].
In this note we are going to argue that through the exceptional generalized geometric description of the moduli space of N = 1 supersymmetric M-theory compactifications to four-dimensions, we can associate to every internal seven-dimensional manifold M 7 an eight-dimensional manifold M 8 equipped with a particular set of tensors S (given in Definition 2.6) that contain all the information about the topological reduction implied by supersymmetry. This eight-dimensional manifold (M 8 , S) was dubbed intermediate manifold in [21], where the study of its topological properties was initiated. The geometry of an intermediate manifold (M 8 , S) is completely specified once the tensors S are required to satisfy the differential conditions obtained from supersymmetry. In order to translate the supersymmetry conditions to the intermediate structure S, it is necessary first to write them in the exceptional generalized geometry language, which has not been done yet. Once they are known we will be able to fully uncover the role of intermediate manifolds in relation to M-theory compactifications and their moduli spaces. However, it is clear that the moduli space of intermediate structures on M 8 is closely related to the moduli space of the corresponding compactification, and therefore we can resort to this guiding principle in order to construct particular examples of M 8 .
More precisely, here we will propose that it is natural to construct M 8 from M 7 in such a way that M 8 is equipped with a torsion-free Spin(7)-structure induced by a oneto-one map from the G 2 -structure in seven dimensions, obtaining therefore a candidate for a map between G 2 -structures with non-zero torsion in seven dimensions and torsion-free structures in eight-dimensions. This is interesting because the moduli space of the latter is much more under control than the moduli space of the former, and thus it is reasonable to expect that using the map some new information can be obtained about the moduli space of G 2 -structures with non-vanishing torsion.
Once we realize that one can embed structures with torsion in a given dimension into torsion-free structures in a higher dimension, there is no need to stop at eight-dimensions. In fact, for a general enough G 2 -structure in seven-dimensions we should not expect to obtain a torsion-free Spin(7)-structure in eight dimensions, but that could be possible if we consider instead a manifold of dimension large enough. This construction can be as well motivated from the Exceptional Generalized Geometry formulation of the compactification.
The outline of this note is as follows. In section 2 we review N = 1 M-theory compactifications to four dimensions, motivate the definition of intermediate manifolds and show how they can be constructed from the physical manifold M 7 . In section 3 we present a few examples of this construction. In particular, and also as a non-trivial example JHEP05(2015)085 of intermediate manifold, we obtain a bijection from the set of Spin(7)-structures on an eight-dimensional S 1 -bundle and the set of G 2 -structures on the base space, fully characterizing the G 2 -torsion clases when the total space is equipped with an invariant torsion-free Spin(7)-structure. In section 4 we define the moduli space of supersymmetric M-theory compactifications and explain how the map between G 2 -structures in seven-dimensions and torsion-free structures in eight-dimensions can be used to obtain information about the former.
2 Intermediate manifolds from exceptional generalized geometry Let us consider the bosonic sector (g, G) of eleven-dimensional Supergravity on a space-time manifold M that can be written as a topologically trivial direct product where M 1,3 is a four-dimensional Lorentzian oriented, spin manifold and M 7 is a sevendimensional, Riemannian, oriented, spin manifold. Although we will speak about compactifications, we are not going to assume that M 7 is compact since it might be consistent to compactify in non-compact space-times with finite volume and appropriate behavior of the laplacian operator [22]. According to the product structure (2.1) of the space-time manifold M, we choose the Lorentzian metric g on M to be given by is the warp factor and g 1,3 is a Lorentzian metric on M 1,3 . In addition, and in accordance again with the product structure of M and the choice of metric (2.2), we will assume that the four-form G is given by 3) we guarantee that, given a particular Lorentzian four-dimensional manifold (M 1,3 , g 1,3 ), the equations of motion that the bosonic fields of the theory (the full metric g and four-form G) need to satisfy, can written as a set of differential equation exclusively on M 7 . This will be important in section 4 in order to properly define the moduli space of this kind of solutions. Although the set-up presented above is more general, we will be usually interested in compactifications on maximally symmetric spaces (M 1,3 , g 1,3 ), which thus will be taken to be the AdS or Minkowski space. The dS-metric is discarded since it cannot be obtained supersymmetrically.

Seven-dimensional supersymmetric G 2 structures
Supersymmetric solutions of eleven-dimensional Supergravity have to satisfy the Killing spinor equation of the theory, given by

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where S → M the 32-dimensional real, symplectic spinor bundle over M, ǫ ∈ Γ (S) is a Majorana spinor, v ♭ is the one-form associated to v through the metric and the terms in parenthesis act on the spinor via the Clifford multiplication. Given the decomposition (2.1) and the choice of metric (2.2) we have to decompose the Spin(1, 10) spinor ǫ in terms of Spin(1, 3) × Spin (7) representations. Let us denote by ∆ R the 32-dimensional symplectic real representation of Spin(1, 10), by ∆ + 1,3 and ∆ − 1,3 the positive and negative chirality complex Weyl representation of Spin(1, 3) ≃ Sl(2, C), of complex dimension two, and by ∆ R 7 the real Majorana representation of Spin (7). The branching rule Spin(1, 10) → Spin(1, 3) × Spin (7) is given by 2 and therefore where S ± 1,3 is the positive (negative) chirality spin bundle over M 1,3 and S R 7 is the real spin bundle over M 7 .
For each linearly independent eleven-dimensional spinor of the form (2.6) satisfying the Killing spinor equation (2.4), there is one out of 32 supersymmetries preserved. Therefore ν = 1 32 supersymmetry requires the existence of a single Majorana Spin(7) spinor in the internal space M 7 . 3 The existence of a global spinor implies that the structure group of the spin bundle S R 7 is reduced from Spin(7) to G 2 . This structure can alternatively be defined by a positve 3form ϕ, 4 which additionally induces a Riemannian metric g 7 that can explicitly be written as follows where V 7 is the Riemannian volume form of M 7 . The supersymmetry conditions coming from the Killing spinor equation (2.4) can be translated into a set of differential conditions on ϕ. In the absence of fluxes, and for a Minkowski four-dimensional vacuum these amount to dϕ = 0, d * ϕ = 0, which implies that the structure is torsion-free, or equivalenetly that the manifold has G 2 holonomy. In the presence of fluxes the structure is not torsion-free anymore. It is useful to decompose the torsion classes into G 2 representations, namely

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where τ 0,1,2,3 are a 0,1,2 and 3-form, respectively in the 1, 7, 14 and 27 representations of G 2 . Supersymmetry relates these torsion classes to the different representations of the 4form flux G. For a Minkowski vacuum, and particular decomposition of the supersymmetry spinor, these relations can be found in [23].
In this paper we are interested in the set of all supersymmetric solutions of the form given in (2.2) and (2.3) as a space by itself; namely, we are interested in the moduli space of supersymmetric compactifications to four-dimensional AdS or Minkowski space. Due to the presence of a non-trivial warp factor e 2A , a supersymmetric solution cannot be fully characterized by a set of first-order differential equations. Indeed, to obtain a supersymmetric solution to the full set of equations of motion of eleven-dimensional Supergravity one has to impose, on top of the supersymmetry conditions, the equation of motion for the flux. This is a second-order differential equation for e 2A . Hence, the moduli space of supersymmetric solutions to eleven-dimensional Supergravity cannot be characterized in terms of first-order differential equations. Therefore, we will consider instead the moduli space of supersymmetric configurations, which depends exclusively on the Killing spinor equation (2.4), which is a first-order partial differential equation. We define then the concept of supersymmetric G 2 -structure, which will be used in section 4, in the following way Definition 2.1. Let (M 1,3 , g 1,3 ) be a particular Lorentzian, four-dimensional, oriented and spin manifold and let M 7 be a fixed seven-dimensional, oriented, spin manifold. A supersymmetric is a function and µ ∈ R, such that combined with the four-dimensional data in the form given by Remark 2.2. Notice that depending on the choice of four-dimensional manifold (M 1,3 , g 1,3 ) the set of corresponding supersymmetric G 2 -structures may be empty, for example if (M 1,3 , g 1,3 ) is dS-space, which is known to be non-supersymmetric. When talking about the set of supersymmetric G 2 -structures we will always omit the space they are relative to, assuming that it is one such that the set is non-empty.

Eight-dimensional intermediate manifolds
Using the tools of generalized geometry, compactifications of M-theory down to fourdimensions with N = 1 supersymmetry were geometrically characterised in [15] in terms of the space of sections of a real, 912-rank, vector bundle over M 7 with structure group E 7(7) × R + , where E 7(7) stands for the maximally non-compact real form of E 7 acting in the 912 representation 6 and R + represents conformal rescalings. 5 The Killing spinor equation (2.4) is written in terms of the spinor η instead of the 3-form ϕ, but from it one can obtain equations for ϕ in terms of the components of G and the warp factor (see (3.25) in reference [23]). 6 Here 912 denotes the real representation induced on E 7(7) by the 912 of the exceptional complex Lie group E7 = E 7(7) ⊗ C. The 912 representation of E7 can be characterized as a particular subspace of V56 ⊗ e7, see appendix B in reference [15].

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Let us denote by N 912 the vector space corresponding to the 912 representation of E 7(7) × R + . In terms of Sl(8, R) representations, it decomposes according to 7 where V is an eight-dimensional real vector space where Sl(8, R) acts in the vector representation, S stands for symmetric and the subscript 0 denotes traceless. We can apply the decomposition (2.10) to the bundle E (2.9), since at every point p ∈ M 7 , E p is the 912 irreducible representation of E 7 (7) . Hence we can write (2.10) for E where now V would denote a rank-eight real vector bundle over M 7 with structure group Sl(8, R) × R + acting in the 8 of Sl(8, R). Therefore, every section φ ∈ Γ (E) can be decomposed as in (2.10). Given a spinor η ∈ ∆ R 7 , there exists a canonical element ψ η ∈ N 912 which is stabilized by SU(7) ⊂ E 7(7) [15,20] and can be written as follows in terms of SU (8) representations (see footnote 7) ψ η = (η η, 0, 0, 0) .
Corollary 2.5. Let E → M be a rank-912 vector bundle with structure group E 7(7) × R + . If E is equipped with a E-admissible section ψ ∈ Γ (E), then it admits a topological reduction of the frame bundle from E 7(7) × R + to SU(7).
Off-shell N = 1 supersymmetry implies the existence of an E-admissible section ψ ∈ Γ (E), and thus a topological reduction on E from E 7(7) × R + to SU(7) and vice-versa, such a topological reduction implies the existence of a globally defined spinor on M 7 . It is then necessary to take a closer look at the space of E-admissible sections, since it corresponds to the space of topological reductions on E implied by supersymmetry. Notice that the space of E-admisible elements N E 912 ⊂ N 912 is transitive under the action of E 7(7) × R + , and since every E-admissible element is stabilized by SU (7) we obtain (2.14)

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Hence, the space of E-admissible elements N E 912 is an 85-dimensional real homogeneous manifold times R + , and it was conjectured to be a Kähler-Hodge manifold 8 in reference [15] in order to make contact with the geometry of the non-linear sigma-model of N = 1 Supergravity. Let us define then the fibre bundle The setX of all E-admissible structures on E can be thus written as the space of sections of E Ẽ (2.16) In order to properly define the moduli space of supersymmetric compactifications as a subset ofX there are two missing pieces. These are the differential conditions implied on ψ ∈ Γ (E E ) by supersymmetry, which come from the Killing spinor equation (2.4), and the quotient by the appropriate equivalence relation. If we had them we could readily characterize the moduli space of N = 1 compactifications to four dimensions as follows whered is an appropriate coboundary operator and D are generalized diffeomorphisms, combining diffeomorphisms and gauge transformations. However, given on one hand that we do not know the differential conditions, and on the other that there are not yet available any mathematical results on deformations on these structures, we will pursue here a different path, more straightforward in some sense, though restricted to particular set of supersymmetric backgrounds. We have seen that off-shell N = 1 supersymmetry is equivalent to the existence of an E-admissible section, which at every point p ∈ M 7 can be written as as follows in terms of SL(8, R) representations (cf. eq. (2.10)) [20] where g 8 is a Riemannian metric on V → M 7 and φ,φ are appropriate elements in the second and fourth components of (2.10). Therefore (g 8 , φ,φ) carry all the information of the E-admissible section of E. However, E is an extrinsic bundle over M 7 , while it would be desirable to have a description given in terms of intrinsic bundles, namely tensor bundles of a given manifold, since they are easier to handle. Given that the exceptional bundle E can be written as the Whitney sum of rank-eight real vector bundles over the seven dimensional base M 7 , we propose an eight-dimensional manifold M 8 such that it contains in its tensor bundles all the information that is present in the set of E-admissible sections of E. This way, the role of the rank-eight vector bundle V → M 7 is played by the tangent bundle T M 8 of M 8 , which then must be equipped with the corresponding sections to contain a decomposition of the 912 representation of E 7(7) × R + in terms of tensors over M 8 . This motivates the following definition. 8 To the best of our knowledge this has not been proven yet JHEP05(2015)085 Definition 2.6. Let M 8 be an eight-dimensional, oriented, spin differentiable manifold. We say that M 8 is an intermediate manifold if it is equipped with the following data We will say then that S = g, φ,φ is an intermediate structure on M 8 . Therefore, we relate to every compactification manifold M 7 an eight-dimensional manifold M 8 whose physical role remains to be found.
Since an intermediate manifold (M 8 , S) is equipped with the same tensors than those implied by an E-admissible section on E, we expect a very close relation between the spaceX of E-admissible sections and the space of intermediate structures on M 8 , which we will denote byH. Now, the difference between the description in terms ofX and the description in terms ofH is that on one hand in the latter we expect the differential conditions that are implied by supersymmetry to have a simpler form and on the other it is a more manageable space, since it consists of sections of tensor bundles, instead of sections of an extrinsic exceptional bundle. However, appropriately lifting the set of forms, together with their differential conditions, to the eight-dimensional manifold (M 8 , S) is a tricky step, since there is not an obvious or unique way of doing it. As explained in [21], in the simplest case where the intermediate manifold ( where φ 3 ∈ Ω 3 (M 8 ) and v ∈ X (M 8 ). In reference [21] we showed that it is natural to consider M 8 either as a rank-one vector bundle over M 7 or as having a codimensionone foliation in terms of leaves such that at least one of them is diffeomorphic to M 7 . Furthermore, if φ 3 is the unique lift of a positive positive three-form on M 7 , the following four-form [21] is admissible 9 , or in other words it defines a Spin (7)-structure on M 8 . We now turn to the differential conditions on the intermediate manifold imposed by supersymmetry.

Spin(7) holonomy on M 8
We will not attempt to uplift the differential conditions in their full generality, but we note that remarkably enough, one can impose a very natural and useful condition on M 8 that basically fixes the way in which M 8 is constructed from M 7 , and provides M 8 with a nice geometrical structure with more well-known mathematical properties. This condition is the JHEP05(2015)085 requirement that (M 8 , S) has at least Spin(7)-holonomy. Restricting to a given class of G 2 structures, M 8 can be built from M 7 in such a way that for every restricted G 2 -structure on M 7 there is a unique torsion-free Spin(7)-structure on M 8 . As we will see in section 3, one can describe this way a particular set of torsion-full G 2 structures, namely those with constant τ 0 and harmonic τ 2 torsion classes (see eq. (2.8)).
There are basically two reasons to impose Spin(7)-holonomy on (M 8 , S), namely • Due to the presence of fluxes, M 7 is equipped with a G 2 -structure which is not torsion free. The moduli space of such G 2 -structures is very poorly understood, and thus if we relate M 7 to an eight-dimensional manifold M 8 in such a way that the supersymmetric G 2 -structure induces a torsion-free Spin (7)-structure, we are geometrizing the fluxes and at the same time precisely relating M 7 with a manifold M 8 whose moduli space 10 is much more under control. Notice that this is an interesting problem by itself, aside from the study of intermediate manifolds. A word of caution is needed here though: constructing a compact Spin (7)-holonomy manifold M 8 from M 7 is an extremely difficult task, one of the reasons being that a compact Spin (7)-holonomy manifold has no isometries. On the other hand, constructing a non-compact M 8 is doable, but then in that case the moduli space of non-compact Spin (7)-manifolds is not as well understood as in the compact counterpart, although some results are known for cases with controlled asymptotics. 11 • The eight-dimensional manifold M 8 is constructed from the physical sevendimensional one M 7 and thus it is natural to study if it has some physical significance beyond being an auxiliary tool. Since we are considering compactifications to fourdimensions and M 8 is eight-dimensional, it is natural to study the possibility of M 8 being an admissible compactification background for F-theory. Therefore it is reasonable to impose at least Spin (7) For instance, in reference [24] it was shown that a configuration of D6-branes wrapping a special Lagrangian cycle of a non-compact Calabi-Yau manifold such that the internal string frame metric is Kähler, is dual to a purely geometrical background in eleven dimensions with an internal metric of G 2 -holonomy. Other examples of torsion-free structures dual to configuration with fluxes, in other words, non-zero torsion, can be found in references [25][26][27][28], this time from six-dimensions to a G 2 -holonomy.
For further examples and results in the Spin(7) and G 2 cases see reference [29,30]. 10 Meaning the moduli space of torsion-free Spin(7) structures on M8. 11 We thank Dominic Joyce for a clarification about this point.

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3 Examples (7) holonomy starting from supersymmetric G 2 structures in seven dimensions. (7)-manifolds from trivial products of G 2 -structure manifolds and R Let M 7 be a seven-dimensional oriented manifold equipped with a positive three-form ϕ.

Spin
Let M 8 = R + × M 7 be the topologically trivial product of R + and M 7 , which we take to be oriented with volume form V 8 = dt ∧ V 7 . We define the following four-form Ω on M 8 where t is the natural coordinate on R + and f 1 , f 2 ∈ C ∞ (M 8 ) are positive functions on M 8 . The four-form Ω defines therefore a unique topological reduction on F (M 8 ) from Gl + (8, R) to Spin (7), which however is redundant since it can be further reduced to G 2 . Notice however that the holonomy of M 8 is not G 2 , unless, as we will see in a moment, f 1 = f 2 = 1, but in that case M 8 is a reducible Riemannian manifold and thus not covered by Berger's list of possible holonomy groups. Furthermore, the admissible four-form Ω induces a Riemannian metric g 8 on M 8 . 12 Taking f 1 = f 2 = 1 the following result can be proven.
andφ given by the dual of φ by the corresponding musical isomorphisms. However, this construction does not illustrate the geometrization of fluxes since the G 2 structure (ϕ, g 7 ) is already torsion-free. This situation can be modified by considering non-constant functions f 1 and f 2 . Let us first consider the cone-like construction [32]. 3) and f 1 = 1 , f 2 = λt. 12 Since the expression for g8 in terms of Ω is not particularly illuminating and will not be needed, we do not write it here. It can be found in [31], theorem 4.3.5.

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The proof is straightforward: since f 1 can always be eliminated by a change of coordinates on t given by dt dt = f 1 (t), we will assume that f 1 = 1 without relabelling t. The condition dΩ = 0 then translates into and thus d * 7 ϕ = 0 , dϕ = ∂ t f 2 * 7 ϕ (3.5) which implies where τ i are the torsion classes defined in (2.8).
Again (M 8 , Ω), as in the preposition above can be easily embedded in an intermediate structure G as in (3.2). However in this case, since ϕ defines a nearly G 2 -structure on M 7 , we obtain a torsion-free Spin(7)-structure from a G 2 -structure which is not torsionfree. This is therefore the simplest non-trivial example of intermediate manifold, which is constructed as a cone over a seven-dimensional compact nearly G 2 -manifold (namely τ 0 is the only non-vanishing torsion-class), in such a way that we obtain an a torsion free Spin(7)-structure on the eight-dimensional manifold M 8 . The relation between nearly G 2 -structures on M 7 and torsion-free structures on M 8 is in fact one-to-one.
Unfortunately, this is the only torsion class that can be geometrized using (3.1). Indeed, if we take f 1 and f 2 as generic real positive functions on M 8 the following result holds. Proof. The condition dΩ = 0 splits in two independent requirements, namely where the subscript 7 denotes objects on M 7 . The second equation can be used to rescale ϕ so that we eliminate the dependence of f 2 in M 7 , so we will assume that f 2 ∈ C ∞ (R) and thus d 7 * 7 ϕ = 0 .

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Therefore, the previous proposition proves that if we impose Spin(7)-holonomy on an eight-dimensional manifold M 8 of the form M 8 = R × M 7 then the only possibility is a cone over a nearly-G 2 manifold.
Nearly G 2 -structures appear in Freund-Rubin-type of N = 1 compactifications to AdS 4 -space [33][34][35], where the radius of AdS is given by the four-form flux µ, which is proportional to τ 0 . In particular, the space-time is assumed to be of the form equipped with the product metric and four-form flux G given by the volume form of the AdS-space Under this provisos, it can be shown that M 7 must be a nearly-G 2 manifold and thus the cone construction geometrizes the flux present in this class of compactification backgrounds. We want to consider now more general intermediate manifolds, or, from another point of view, more general embeddings of supersymmetric G 2 -structures into torsion-free Spin(7)-structures. In the following section we are going to consider the natural next step, which is the case of M 8 being an S 1 principal bundle.

Spin(7)-manifolds as S 1 -bundles
Let M 8 π − → M 8 /S 1 be an S 1 -bundle over M 7 , equipped with an S 1 -invariant Spin(7)structure Ω, which is a non-trivial instance of intermediate manifold. Then, as proven in reference [21], there is an induced G 2 -structure on the base M 8 /S 1 and conversely, a G 2 -structure ϕ on M 8 /S 1 induces a Spin(7)-structure on M 8 . Now we are going to show that this correspondence is one-to-one, providing thus a non-trivial example of the map I Top to be introduced in section 4. First we need the following proposition. Proposition 3.5 (Proposition 3.12 [21]). Let V denote an eight-dimensional oriented vector space equipped with a fixed metric g. Fix v ∈ V of unit norm. Let i * g denote the restricted metric on the seven-dimensional subspace H ≡ v ⊥ endowed with the orientation induced by that on V and by v. Then there is a bijection from the space of all admissible four-forms Λ 4 a (V ) on V inducing the metric g to the space of all positive three-forms Λ 3 + (H) on H inducing i * g. The inverse map is given by (3.15) where ϕ = φ| H .

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As a direct application of proposition 3.5 we have the following corollary.
Corollary 3.6. Let V denote an eight-dimensional oriented vector space equipped with an admissible four-form Ω ∈ Λ 4 a (V ). Then, for every unit norm vector v ∈ V , Ω can be written as The following theorem extends proposition 3.5 to the case of an eight-dimensional S 1 -bundle equipped with an invariant Spin(7)-structure Ω.
The inverse map is given by Proof. Let us denote by v the norm of the vector v. It can easily be seen that L v v = 0 and thus v descends to a well defined function on M 8 , so we are in the conditions of theorems 5.27 and 5.29 in [21], from which we see that the map T and its inverse T −1 are well-defined. Let us see now that it is a bijection. Let us use the kernel of the connection θ = v ♭ to define a co-dimension one distribution H ⊂ T M 8 , which thus implies the splitting Therefore, at every point p ∈ M 8 we are in the conditions of proposition 3.5, and thus at every point there is a bijection T ′ p between the set of admissible four-forms in T p M 8 inducing g 8 | p and the set of three-forms on H p inducing g 8 | H . Now, dπ : H → T M 8 /S 1 is an isometry and then point-wise composing with T ′ we obtain T and we conclude.
As a consequence of theorem 3.7, we obtain the following proposition.

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Proof. Let us pick a S 1 -invariant metric g 8 on M 8 and let θ = v ⊥ be a connection with horizontal distribution H ⊂ T M 8 . Then we have (3.20) where V → M 8 is a one-dimensional vector bundle. Since v ∈ Γ (V ) is a global section V is oriented and spin, and thus H → M 8 is also an oriented spin vector bundle, namely w 1 (H) = w 2 (H) = 0. Now, π : M 8 → M 8 /S 1 is a continuous map and since the first and second Stiefel-Whitney classes are natural [36], we obtain 21) where π * T M 8 /S 1 denotes de pull-back vector bundle of T M 8 /S 1 by π. But π * T M 8 /S 1 ≃ H and thus which implies w 1 T M 8 /S 1 = 0 and w 2 T M 8 /S 1 = 0, namely M 8 /S 1 is a spin manifold, and hence it is equipped with a G 2 -structure ϕ. Applying theorem 3.7 we obtain that J −1 (ϕ) is an S 1 -invariant admissible four-form in M 8 . Once we now that M 8 /S 1 is spin, lifting the corresponding G 2 -structure using in [Theorem 5.27 [21]] a codimension-one distribution H perpendicular to v but non-invariant results in a non-invariant Spin (7)structure on M 8 . Remark 3.9. Theorem 3.7 implies that if there are no admissible four-forms on M 8 compatible with g 8 , then the base space M 8 /S 1 cannot be equipped with a G 2 -structure and therefore cannot be a spin manifold, which in turn implies than M 8 is not a spin manifold, in agreement with proposition 3.8.
Theorem 3.7 gives us the first explicit example of a map J relating Spin(7)-structures into G 2 -structures and vice-versa. Following the discussion of section 4 we have to study now the differential conditions on the induced G 2 -structure on M 8 /S 1 implied by requiring a torsion-free S 1 -invariant Spin(7)-structure on M 8 . This way we will see if it is possible to have a one-to-one map from G 2 -structures on M 8 /S 1 with some non-zero torsion, to torsion-free Spin(7)-structures on M 8 . We will prove a proposition that completely characterizes the situation.

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Proof. Using theorem 3.7, the induced G 2 -structure on M 8 /S 1 is given by π * (ϕ) = ι w Ω = φ (where ω = v ||v|| ) and we can write Ω as follows The torsion-free condition dΩ = 0 translates into where for notational simplicity we omitted the pull-back of all seven-dimensional objects, τ i are the torsion classes defined in (2.8) and we have used * φ = w b ∧ π * ( * 7 ϕ) , (3.26) which is straightforward to show. Contracting (3.25) with w and using that the metric On the other hand, τ 0 = τ 1 = τ 3 = 0 imply that L w Ω = 0. However, by assumption L v Ω = 0 and thus we obtain and we conclude.
Note that proposition 3.10 implies that ϕ satisfies and thus τ 2 is a closed two-form. In fact, since τ 2 ∈ Ω 2 14 M 8 /S 1 it has to satisfy the constraint τ 2 ∧ ϕ + * 7 τ 2 = 0 , (3.31) and hence applying the exterior derivative we obtain that d * τ 2 = 0, so τ 2 is closed and coclosed and thus that is, τ 2 is a harmonic two-form on M 8 /S 1 . Furthermore, using that τ 2 is closed and coclosed in equation (3.23) we arrive at namely dv ♭ is a harmonic two-form on M 8 . We see then that the requirement of a Spin(7) torsion-free S 1 -invariant structure imposes strong constrains on the induced G 2 -structure, namely the only possible non-zero torsion class is τ 2 and it has to be an harmonic function. Indeed, in theorem 3.7 the set-up, although naturally compatible with the S 1 -action on M 8 ,

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is quite constrained: we start with a S 1 -invariant admissible four-form Ω, which induces a Riemannian metric g 8 , and we rewrite Ω as We then require the G 2 structure ϕ to be given by π * ϕ = ι w Ω. This way, we guarantee that π : M 8 → M 8 /S 1 is a Riemannian submersion with respect to the corresponding induced metric. A less restricted scenario would be to relax the S 1 -invariance, namely still consider an eight-dimensional S 1 -bundle M 8 π − → M 8 /S 1 equipped with an admissible four-form, but the latter is not necessarily S 1 -invariant. Start from an arbitrary G 2 structureφ on M 8 /S 1 , and we will construct an admissible four-form on M 8 as follows • Pick a codimension-one distribution H ⊂ T M 8 transverse toṽ, whereṽ is a vector field C ∞ (M 8 )-proportional to v.
• Equip M 8 with the following admissible four-form Then, by means of theorem 5.27 of reference [21] we have thatΩ inducesg 8 and in general it will not be S 1 -invariant.
Notice that are now in exactly the same set-up as in proposition 3.10 but dropping the requirement of Ω being S 1 -invariant. We obtain the following proposition. Proof. The torsion-free condition dΩ = 0 translates into where again the pull-back of seven-dimensional objects should be understood. Contracting equation (3.37) withṽ we obtain
From the supersymmetry conditions relating fluxes to torsion classes obtained in [23], it seems that a supersymmetric compactification to Minskowski with torsion given only by τ 2 is possible. We leave more explicit constructions with more general G 2 -torsion classes, and thus involving higher-dimensional manifolds, for future work.

Relating moduli spaces
In this section we give an idea of how to extract information about the moduli space of supersymmetric G 2 -structures on a seven-dimensional manifold from the moduli space of torsion-free Spin(7)-structures on an eight-dimensional one. It is intended to be only descriptive.
Recall that (see definition 2.1), given a seven-dimensional oriented and spin manifold M 7 , a supersymmetric G 2 -structure is defined to be a quadruplet ϕ, G, e 2A , µ satisfying a set of differential conditions coming from the Killing spinor equation (2.4). We will denote by B the set of all supersymmetric G 2 -structures ϕ, G, e 2A , µ on a given manifold M 7 . if they are related by a diffeomorphism or by a gauge transformation of G. We will denote the elements of X 7 , namely the corresponding equivalence classes, by ϕ, G, e 2A , µ .
The moduli space X 7 of supersymmetric G 2 -structures remains as a largely unexplored space, and, to the best of our knowledge it has not even been proven if it is a finitedimensional manifold. We are going to argue that such space can be related, at least in some special instances, to the moduli space of torsion-free structures on a higher-dimensional manifold, which is a space much more under control. Indeed, this procedure can be justified to work from the exceptional generalized geometry formulation of the moduli space; we will JHEP05(2015)085 come back again to this point at the end of the section. For now, we will illustrate the procedure in the simplest case where the higher-dimensional manifold is eight-dimensional and thus it can be identified with an intermediate manifold, keeping in mind that for higher-dimensional manifolds the construction proceeds along similar lines. In fact, the construction presented in section 2 already suggests to consider instead of the space of supersymmetric G 2 -structures an eight-dimensional manifold M 8 constructed from M 7 in such a way that a supersymmetric G 2 -structure on M 7 induces a torsion-free Spin(7)structure on M 8 . Let us just very briefly recall some basic facts about the moduli space of torsion-free Spin(7)-structures on M 8 .
Given an eight-dimensional, compact, oriented manifold M 8 , the moduli space of torsion-free Spin(7)-structures on M 8 is given by [4] where We want to use X 8 to infer properties about X 7 . For that, we have shown that one can construct the eight-dimensional manifold M 8 from a seven-dimensional one M 7 such that from every supersymmetric G 2 -structure on M 7 one can construct a topological Spin(7)structure Ω on M 8 . We have thus a map  where B Hol = I −1 Top (N 8 ) ⊂ B is the restricted set of supersymmetric G 2 -structures that induce through I Top a torsion-free Spin(7)-structure on M 8 . We presented explicit examples of I Hol of this in sections 3.1 and 3.2. For example, in the Spin(7)-cone construction, for every nearly G 2 structure on M 7 one obtains a torsion-free Spin(7) structure on M 8 , although in this case the M 8 turns out to be non-compact.
The last step consists in evaluating if the map (4.5) descends to a well defined map on the corresponding equivalence classes. Assuming that it is the case, then we obtain a new map I : B Hol /D → X 8 , of this map, one may be able to extract information about B Hol /D taking into account what is known about X 8 . The first property to be checked is the continuity and injectivity of the map. Remarkably enough, if one can proove that I is a local homeomorphism between topological spaces, then B Hol /D would be a topological manifold of the same dimension as N 8 , namely b 4 1 +b 4 7 +b 4 35 . That is, we would have obtained the dimension of the moduli space of restricted supersymmetric G 2 -structures on M 7 in terms of the topological data of M 8 .
For supersymmetry reasons, the moduli space X 8 must be identified with the Kähler-Hodge manifold appearing in the non-linear sigma model of four-dimensional N = 1 Supergravity. A Kähler-Hodge manifold is a Kähler manifold such that the Kähler form represents an integer cohomology class, and therefore is the curvature form of the associated U(1)-bundle. There are several obstructions on a manifold to be Kähler-Hodge, the most obvious one being that its dimension must be even. Therefore, if the map I exists then the dimension of X 8 must be even, and we conclude that there are as well topological obstructions to the existence of I.
The example of the Spin(7)-conifold is again useful. In that case, there is a one-to-one correspondence between nearly G 2 -structures on M 7 and torsion-free Spin(7)-structures on M 8 . However, the resulting M 8 is non-compact so there are not as many available results about its moduli space as there are in the compact case. In fact, we have been talking about an eight-dimensional manifold M 8 constructed from M 7 . Ideally we would like this M 8 to be compact, since in that case the moduli space of torsion-free Spin(7)-structures is under control. However, as we already explained, this is a too optimistic scenario, since constructing a compact Spin(7)-manifold M 8 from M 7 is an extremely difficult task, for instance there are no isometries that may allow for an adapted system of coordinates to write the metric. Still, constructing a non-compact M 8 is interesting, because depending on its asymptotics, some results are also known about the moduli space, in particular if it is a smooth manifold of a finite dimensionality, which would be the first thing to check for the moduli space of supersymmetric G 2 -structures on M 7 .
The procedure explained here refers to seven-dimensional manifolds equipped with a supersymmetric G 2 -structure which induces a torsion-free Spin(7)-structure in an eightdimensional manifold M 8 . It is to be expected that if the supersymmetric G 2 -structure is general enough, i.e. if it has many nonzero torsion classes, then there is no way it induces a torsion-free Spin(7) structure on any eight-dimensional manifold, namely the inclusion B Hol ⊂ B is strict. It is natural to ask under which conditions one should expect B Hol = B, namely, when we can geometrize the full space of supersymemtric G 2 -structures. We expect that considering a n > 8 -dimensional manifold of special holonomy and doing the same procedure, this time imposing that the supersymmetric G 2 -structure in seven dimensions induces a torsion-free structure in n-dimensions, which can be for example a SU( n 2 ) or Sp( n 4 ) torsion-free structure, one might be able to completely geometrize the most general supersymmetric G 2 -structure. This is an open question that can be formulated as follows • Is there a n-dimensional principal fibre bundle M with fibre G and seven-dimensional base M/G such that every G 2 -structure on M 7 induces a torsion-free structure on M?

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In the eight-dimensional case M 8 corresponds to an intermediate manifold. The question is now, if we choose to embed the supersymmetric G 2 -torsion in a higher dimensional manifold, is there again a connection to exceptional generalized geometry as there is in the eight-dimensional case? The answer is afirmative. Recall that the definition 2.6 of an intermediate manifold was based on the decomposition of the 912 of E 7(7) × R + in terms of Sl(8, R) representations, which, acting on an eight-dimensional vector space required an eight-dimensional manifold. However, we can consider other subgroups G ⊂ E 7(7) × R + and follow the same steps defining now a n-dimensional manifold, where n is equal to the dimension of the representation of G, equipped with the tensors S n appearing in the corresponding branching rule. This way, we can translate again all the information of the moduli space to a n-dimensional manifold M n equipped with the appropriate tensors, and impose a torsion-free condition on them. Imposing the torsion-free condition will again restrict the moduli space to the appropriate subspace, but since the manifold is of a higher dimension, the restriction will be less severe than on the eight-dimensional case. Therefore, in some sense, we have a dictionary to go from the description of the moduli space given in exceptional generalized geometry, to the particular geometry of a n-dimensional manifold M n whose dimension and geometric characteristics are determined by a subgroup G of G ⊂ E 7(7) × R + . In this note however we have focused for simplicity only on the eight-dimensional case.

Summary
It is convenient to give a brief summary of the main results of the paper.
• Using Exceptional Generalized Geometry, the moduli space of M-theory N = 1 compactifications to four dimensions can be described through the space of sections of a particular E 7(7) × R + -bundle over the internal space M 7 . We propose that, using a subgroup G ⊂ E 7(7) × R + , all the information of this bundle can be translated to an n-dimensional manifold M n , using appropriate sections S of its tensor bundles, determined by the branching rule E 7(7) × R + → G. Here n is the dimension of the representation of G.
• Since the moduli space of S-tensors on M n corresponds to the moduli space of M-theory compactifications, we propose the existence of a map I that relates both spaces and which can be used to study the geometry of the latter from the geometry of the former.
• In order to fully specify the geometry of the moduli space of S-tensors, we need to know the supersymmetry conditions in the exceptional generalized language, something that is not currently available in the literature. Therefore, we consider the case where S induces a classical torsion-free structure on M n , when n is eight. The moduli space of classical torsion-free structures is well under control, so it is reasonable that given the map I one can extract from it information about the moduli space of N = 1 M-theory compactifications.
• We give explicit examples of the previous abstract constructions for the case where n is eight and M 8 is either a product manifold or an S 1 -bundle over the internal space M 7 , fully characterizing the torsion classes on the base when the total space is equipped with a torsion-free Spin(7)-structure.
• We have proven that every eight-dimensional, oriented, spin S 1 -bundle admits a topological Spin (7)-structure.
We have found that by imposing Spin (7) holonomy on an eight-dimensional manifold built either as a product manifold or as a spin S 1 -bundle, one can describe situations in which the G 2 torsion classes are respectively τ 0 and τ 2 . We summarize our results in table 1.
To embedd other torsion classes (or in other words to geometrize fluxes in other representations) via a torsion-free structure, one has to either build the eight-dimensional manifold in a different way (like for example as a codimension-one foliation), or consider torsion-free structures in higer-dimensions than eight, which would correspond to decompositions of E 7(7) × R + respect to subgroups G with representations of dimension higher than eight.