Tops as building blocks for G 2 manifolds

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Introduction
Given the central position of M-Theory in the web of string dualities, a better understanding of M-Theory compactifications is expected to tie together supersymmetric compactifications of all of the weakly coupled string theories. While this makes compactification of M-Theory on manifolds of G 2 holonomy one of the most interesting parts of the landscape of string vacua, the number of concrete examples studied is relatively sparse as compared to compactifications of type II String Theories, heterotic String Theory, or F-Theory on Calabi-Yau manifolds. The main reason for the lack of examples is the comparatively easy construction of Calabi-Yau manifolds, which, using Yau's theorem, benefits from a host of techniques in complex algebraic geometry. The construction of G 2 manifolds as twisted connected sums [7,8] allows such techniques to be applied in the study of G 2 manifolds as well. It is the motivation of the present work to develop further techniques in this direction. Examples of manifolds with metrics of G 2 holonomy fall into three broad classes. The first constructions [1,2] were non-compact examples which are asymptotically conical, see also [3,4] for more examples. These can be thought of as smoothed versions of singular cones, which is very interesting from the point of view of physics: in compactifications of M-Theory on manifolds of G 2 holonomy, non-abelian gauge groups and (chiral) matter arise from singularities of the compactification geometry and interesting singularities can be constructed from such conical manifolds.
The first compact examples of G 2 manifolds are the famous Joyce manifolds [5]. They are constructed from smoothings of toroidal orbifolds T 7 /G. Unfortunately, (the singular versions of) these manifolds do not support interesting singularities on their own and their toroidal origin renders them locally flat. This prevents to simply cut and paste the interesting singular non-compact examples studied in the literature as these are not asymptotically flat.
A third class, which also contains compact G 2 manifolds, will be the subject of the present work. As first discussed by Kovalev [6] and further elaborated on in [7,8], one may construct compact manifolds of G 2 holonomy by forming a twisted connected sum (TCS) of two appropriate 'building blocks' times a circle. These building blocks can be thought of as K3 fibrations over a P 1 base. Besides the two building blocks, the defining data of a TCS G 2 manifold includes the diffeomorphism used to glue two building blocks. On the level of the K3 fibres, this must be a hyper-Kähler rotation.
The simplest construction of building blocks was already contained in [6], where blowups of appropriate curves in Fano threefolds were employed. This has been generalized to so-called semi-Fano threefolds in [7]. Another construction of building blocks is presented in [9]. Here, non-symplectic involutions of K3 surfaces (classified in [10][11][12]) are used to construct building blocks by orbifolding K3 × P 1 and resolving singularities.

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For a pair of building blocks (times a circle) to be glueable into a manifold of G 2 holonomy, one needs to find a diffeomorphism between the two K3 fibres which acts as a particular type of hyper-Kähler rotation, also called a 'Donaldson matching'. Even though the conditions for this to exist can be spelled out purely in terms of lattice data (for lattice polarized families), it is not straightforward to determine in general if (and how many) such maps can be found.
There are hundreds of thousands of semi-Fano threefolds, giving rise to many examples of building blocks. From the glueing techniques used in [8], it has been possible to mass produce G 2 manifolds and at least 50 million examples are known.
The present work starts from the observation that fibrations of toric hypersurface Calabi-Yau threefolds can be very easily detected in Batyrev's reflexive polytopes [13][14][15][16][17][18]. For a toric hypersurface Calabi-Yau threefold to be K3 fibred, the corresponding four-dimensional N-lattice polytope ∆ • must contain a three-dimensional subpolytope ∆ • F which also contains the origin as its unique interior point. The Picard lattice of the generic fibre is determined by ∆ • F . As it is codimension one, ∆ • F furthermore cuts ∆ • into two halves (dubbed 'top' and 'bottom' in [19]) which contain information about degenerate fibres. Most reflexive four-dimensional polytopes give rise to K3 fibred Calabi-Yau threefolds and many of the structures found in the plot of the Hodge numbers based on the Kreuzer-Skarke database [20] can be understood from this point of view [21].
While K3 fibred Calabi-Yau threefolds do not qualify as building blocks for G 2 manifolds, one may think of top and bottom as forming two halves into which a K3 fibred Calabi-Yau threefold can be disassembled. As shown in section 2, which forms the core of this paper, it is possible to define a threefold purely from a top (or bottom). This threefold then has all of the properties of a building block as defined by [6,7]. In particular, the fibre is a lattice polarized K3 surface, described as a toric hypersurface. The construction can be understood in an ad hoc way, but may also be described by using the language of (refinements of) normal fans of polytopes. The latter allows to exploit a wealth of results, such as the powerful methods of [22]. Section 3 contains a detailed discussion of several examples which are meant to showcase the features of building blocks constructed from tops. In particular, we use a top origination from the largest reflexive four-dimensional polytope to construct a building block with contributes 240 two-forms to any G 2 manifold glued from it.
Appendix A contains a collection of background material on lattices, the relation between mirror symmetry for K3 surfaces and Batyrev's reflexive polytopes (which is slightly more subtle than in the case of higher-dimensional Calabi-Yau manifolds). Appendix B demonstrates the familiar usage of the stratification methods of [22] in the case of toric hypersurface Calabi-Yau threefolds. Appendix C discussed the enlightening example of the stable degeneration of K3 surfaces into two dP 9 surfaces, which serves as an inspiration for our construction, in detail. Some technical details regarding the proof of the absence of torsion in H 3 (Z, Z) for building blocks Z constructed from tops is relegated to appendix D.
Some background of construction of G 2 manifolds via twisted connected sums is contained in sections 1.1. As the relevant theorems and constructions from [6][7][8] are also nicely reviewed in the physics literature in [23], the discussion is limited to a minimum. JHEP10(2017)083

Building blocks
The construction of G 2 manifolds as twisted connected sums [6][7][8] starts from K3-fibred threefolds Z which are called building blocks. In this section, we review some of the properties of building blocks. Following [7,8], see also [6], we call an algebraic Kähler threefold Z a building block if the following conditions are met: i) Z has a projection S → Z ↓ π P 1 the generic fibres of which are non-singular K3 surfaces.
ii) The anticanonical class of Z is primitive 1 and equal to the class of the fibre, S: iii) Picking a smooth and irreducible fibre S 0 , we have a natural restriction map and there is no monodromy upon orbiting around S 0 , i.e. the fibration is trivial in the vicinity of S 0 . Denoting the image of ρ by N , we demand that the quotient Λ/N is torsion free, i.e. the embedding N → Λ is primitive.
Under these assumptions, it follows that Z is simply connected and the Hodge numbers H 1,0 (Z) and H 2,0 (Z) vanish. As Z is a K3 fibration over P 1 , the normal bundle of the fibre, and in particular of S 0 , is trivial. The lattice N naturally embeds into the Picard lattice of S 0 and we can think of the fibres as being elements of a family of lattice polarized K3 surfaces with polarizing lattice containing L ⊇ N . By excising a fibre, we may form the open space from a building block Z. V is an asymptotically cylindrical Calabi-Yau threefold. In particular, its Ricci-flat Kähler metric asymptotes to the Ricci-flat metric ds 2 , Kähler form ω and holomorphic three-form Ω 3,0 on the cylinder R + × S 1 × S 0 : Here, ds 2 S 0 , ω S 0 and Ω S 0 are the Ricci-flat metric, Kähler form and holomorphic two-form of S 0 , θ is a coordinate on the S 1 and t is a coordinate on R + . JHEP10(2017)083

Gluing building blocks to G 2 manifolds
Given two building blocks Z + and Z − , we may glue V + × S 1 and V − × S 1 along their asymptotic Calabi-Yau cylinder by swapping 3 the extra S 1 with the S 1 s of the cylinder while glueing the K3 surfaces with a diffeomorphism g : S 0+ → S 0− acting as: This realizes a manifold X as a twisted connected sum which has a metric of G 2 holonomy [6,8]. This metric is not the same as the Calabi-Yau metrics of the asymptotically cylindrical Calabi-Yau manifolds V ± but it is, in a sense, close to these. Note that one may think of X as a (non-holomorphic) K3 fibration over a base B. This base B is a fibration of a torus over an interval for which one of the two circles of the torus collapses at each end. This space is topologically a 3-sphere 4 which is made manifest by using Hopf coordinates on S 3 .
By the Torelli theorem, there is a unique diffeomorphism inducing (1.4) if and only if (1.4) is the effect of a lattice isometry Choosing a marking h : Λ ∼ = H 2 (S, Z) on one of the K3 surfaces, such an isometry defines primitive embeddings of N ± → Λ. Let us denote the orthogonal complement of N ± in Λ by T ± . The cohomology groups of the resulting G 2 manifolds X are then given by [8]: Here, the group K is defined as and K * is its dual.

Tops as building blocks
In this section we introduce the main idea of this paper and show how appropriate, 'projecting', tops can be used to construct building blocks as defined above. The necessary background in toric geometry can be found e.g. in [25][26][27]. JHEP10(2017)083

Tops and fibred Calabi-Yau manifolds
In its most general incarnation [28] a top ♦ • is defined as a bounded lattice polytope (with respect to a lattice N) satisfying relations of the form for a set of lattice points m i and a single m 0 , all sitting in the dual lattice M.
Although not the most general case, thinking of a top as half a reflexive polytope [13], ∆ • in the N-lattice, is sufficient for our purposes. This is also how the concept originally appeared in [19]. A reflexive lattice polytope ∆ • , is a convex polytope such that its dual is also a lattice polytope. Such a pair of lattice polytopes defines a family of Calabi-Yau hypersurfaces as follows. A triangulation of the polytope ∆ • defines a fan Σ by taking all cones over the simplices of the triangulation on the surface of ∆ • . 5 This in turn defines a toric variety P Σ which is projective, i.e. has a non-zero Kähler cone, if the associated star triangulation, for which all simplices contain the origin as a vertex, is regular [26,29]. The dual polytope ∆ is the Newton polytope of a generic section P of −K P Σ and we may find a family of Calabi-Yau hypersurfaces as Here ν i are lattice points on ∆ • , which are associated with rays of the fan Σ and hence with homogeneous coordinates z i of P Σ . The sum runs over lattice points on ∆ and the c m are complex coefficients. If the polytopes ∆ and ∆ • , i.e. the lattices M and N are n−dimensional, the toric variety P Σ is complex n−dimensional and (2.3) gives a complex n−1 dimensional Calabi-Yau manifold X (∆,∆ • ) . For a sufficiently generic choice of c m , there always exists a triangulation such that above always gives a smooth Calabi-Yau manifold if n ≤ 4. Exchanging the roles of ∆ and ∆ • gives a construction of the mirror family of Calabi-Yau manifolds. Starting from ∆, the polytope ∆ • is uniquely determined (via (2.2)) by the vertices of ∆. This gives the first relation of (2.1). From this point of view, the second relation of (2.1) cuts ∆ • through the origin and leaves us with only one of its halves. Cutting polytopes ∆ • in this fashion reveals fibration structures of X (∆,∆ • ) by Calabi-Yau manifolds of one lower dimension [14][15][16][17][18], as we will review in the following.
Before specializing to our case of interest, which will be Calabi-Yau threefolds fibred by K3 surfaces, let us give the general picture of how fibration structures can be found using polytopes. Let us assume that we can find a subspace F of N ⊗ R such that ∆ • F ≡ ∆ • ∩ F is again a reflexive lattice polytope in N f = N ∩ F . In this case there are the dual short exact sequences

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defining lattices N b and M b . The projection to N → N b gives rise to a projection morphism on the level of the ambient space if the induced map on the fan Σ → Σ b is a toric morphism, i.e. maps each cone of Σ into a cone of Σ b (see [26] section 1.3). The fibres of this projection applied to the Calabi-Yau hypersurface X (∆,∆ • ) are again Calabi-Yau hypersurfaces from the algebraic family X (∆ F ,∆ • F ) . The Calabi-Yau hypersurface X ⊂ P Σ hence enjoys a fibration by another Calabi-Yau manifold X F of lower dimension which is determined by the polytope ∆ • F [14][15][16][17][18]. We now specialize to the case where F (and, correspondingly, X F ) is a codimension one submanifold. In this case, we may write F = m ⊥ 0 for a lattice vector m 0 and F separates ∆ • into the two halves which were called top and bottom in [19]. To see the fibration structure explicitely, it is convenient to introduce an equivalence relation on the set of all lattice points of ∆ as follows i.e. we have a hypersurface equation of a Calabi-Yau manifold X F determined by ∆ • F , the coefficients c F m of which are dependent on the remaining coordinates, as expected for a fibration.
For Calabi-Yau manifolds fibred by Calabi-Yau manifolds of one lower dimension, the base of the fibration must be a P 1 . We can write the homogeneous coordinates [z t : z b ] of this P 1 explicitely as z t = JHEP10(2017)083 Points above (below) F hence correspond to fibre components over z t = 0 and z b = 0. In case a top only has a single point above F , the fibre stays irreducible over z t = 0. As we have seen, lattice points on the top and the bottom contain information about degenerate fibres. 6 As such they may not only be used to study fibrations by lowerdimensional Calabi-Yau manifolds, but can also be thought of as characterizing degenerations of the fibre. See [30] for the relation of tops to semi-stable degenerations. This correspondence is particularly nice in the case of three-dimensional tops, corresponding to elliptically fibred K3 surfaces, which show the extended Dynkin diagrams of the corresponding gauge groups in F-theory [19,31,32]. See also [33,34] for an elegant application to models with non-trivial abelian gauge sector in F-theory.

Ad hoc construction, projecting tops and elementary properties
In this work, we use the term top for any lattice polytope ♦ • which can be described as for a reflexive polytope ∆ • and a vector m 0 such that is again reflexive. Furthermore, we are interested in four-dimensional tops, for which ∆ • F = ♦ • ∩ F is a three-dimensional reflexive polytope. In many cases, two such tops which share the same ∆ • F may be combined to define a reflexive polytope ∆ • and hence a K3-fibred Calabi-Yau threefold. It seems intuitively clear that we should be able to cut the base P 1 of such a K3 fibred Calabi-Yau manifold X into two halves, each half corresponding to a single top. In fact, this is a well-known story in the case that X is an elliptic K3 surface: here, tops whose projection to F lies on ∆ • F correspond to families of rational elliptic surfaces (also called dP 9 in the physics literature) and the points on the top correspond to the components of degenerate fibres of the elliptic fibration. Decomposing a K3 surface into two rational elliptic surfaces is accomplished by means of a specific stable degeneration limit, reviewed in appendix C. Note that we can think of dP 9 surfaces as being an analogue of the building blocks defined in section 1.1 in one dimension lower. They are complex surfaces fibred by Calabi-Yau one-fold (elliptic curves), the first Chern class of which is represented by the class of the fibre. Here, we are not interested in the higherdimensional version of this stable degeneration limit, but we want to directly describe the final products, i.e. the components of the central fibre of the degeneration limit.
Before we proceed, we will need to make a further technical assumption, which should become clear in the following. For now, let us merely motivate it by the following observation: as mentioned above, only specific tops are associated with the degeneration of a K3 surface into two dP 9 surfaces. 7 Those tops are such that there projection onto F lies on ∆ • F .

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Following [21], we call tops ♦ • for which the projection onto F is contained in ∆ • F projecting. In the rest of this paper, we shall assume that the tops we are working with all have this property. An interesting property of such tops is that we may form a reflexive polytope from any pair of projecting tops ♦ • and ♦ • for which ∆ • F = ∆ • F . For this reason, they were used in [21] to understand the intricate structures found in the plot of Hodge numbers of toric hypersurface Calabi-Yau threefolds.
Forming a reflexive polytope from two tops sharing a common ∆ • F , the dual polytope ∆ also has a subpolytope given by ∆ F , which is the polar dual of ∆ • F [16]. Hence in this case both a Calabi-Yau threefold and its mirror are K3 fibred by K3 surfaces from algebraic mirror families. Note that this does not mean that mirror symmetry acts fibre-wise on the K3 surfaces.
Note that we may exploit SL(4, Z) to put m 0 in the convenient location (0, 0, 0, 1), which is what we assume in the following. This means that all points on ∆ • F have the form ( v F , 0). As we are only interested in projecting tops, all other points on ♦ • have the form ( v, h) for h > 0 and v ∈ ∆ • F . We are now ready to present our construction. In the same way that a polytope ∆ • defines a toric variety by taking the cones over all faces of ∆ • and then resolving singularities by refining cones according to a triangulation, we may construct a toric variety from ♦ • ∪ν 0 . We denote the generators of the rays of the resulting fan (i.e. lattice points on ♦ • ) by ν i , with ν 0 = (0, 0, 0, −1). In a sense, this means we are turning ♦ • into a reflexive polytope by completing it with the minimal bottom. Let us denote the fan constructed from a fine regular triangulation of ♦ • ∪ ν 0 by Σ and the corresponding toric variety by P Σ . This completes the construction of the ambient space.
The hypersurface equation of our building block is now given by taking the set of all lattice points on a polytope ♦ in the M-lattice, which is defined by: To each such point m we associate the monomial (2.13) We may then sum up all such monomials with generic coefficients c m to find a homogeneous hypersurface equation for a hypersurface Z in P Σ . The points satisfying (2.12) naturally define a top in the M-lattice which is why we denote it by ♦ and call it the dual top. Note that ♦ and ♦ • are not polar dual polytopes and that our definition of dual top is not the same as that adapted in [28]. Rather, ♦ is obtained from the polar dual of ♦ • ∩ ν 0 by excising all points for which ♦, ν 0 < 0. What we have done closely mimics the result of the procedure outlined in appendix C: the new coordinate z 0 corresponds to λ 1 and the condition m, ν 0 ≥ 0 eliminates all monomials which contain non-zero powers of λ 2 .

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As we may combine any two projecting tops ♦ • 1 and ♦ • 2 with the same ∆ • F to form a reflexive polytope, we may in particular use ♦ • along with a copy ♦ • of itself (with the fourth coordinate inverted). The polar dual ∆ of ∆ • = ♦ • ∪ ♦ • is then the same as ∆ = ♦ ∪ ♦ with ♦ given by (2.12). Using the result of [16] cited above it follows that ♦ ∩ F = ∆ F , where ∆ F is the polar dual of ∆ • F in F . A dual top ♦ is also projecting if ♦ • has this property. As ♦ • sits above F and ♦ below F , the product of the fourth components for each point ν ∈ ♦ • and m ∈ ♦ is always non-positive. Hence (2.14) As we have that ♦ • is projecting, ν| F is contained in ∆ • F . The above relation then forces m| F to be contained in ∆ F , so that ♦ must be projecting as well.
Repeating the analysis of the last section, we find that Z is a K3-fibred threefold with base P 1 . The homogeneous coordinates of the P 1 base are 15) and the class of the fibre X F is given by We immediately find by adjunction that i.e. the anticanonical class of Z equals that of the fibre. We can write the defining polynomial of a generic hypersurface as (2.18) We associate the fibre over the point z 0 = 0 with S 0 . It has a particularly simple description: first note that setting z 0 = 0 we cut out a toric variety P Σ F from the ambient space P Σ . As ν 0 never shares a cone with any of the ν i not on ∆ • F , we can effectively set all of the corresponding coordinates to 1. Said more abstractly, Σ F = star(ν 0 ) is a fan over the faces of ∆ • F . On the level of (2.18), setting z 0 = 0 eliminates all terms except the ones for which ν 0 , m = 0. As these are precisely the lattice points of ♦ on F , we find that the fibre over z 0 = 0 is a K3 surface S defined in terms of the pair of reflexive polytopes ∆ • F , ∆ F , described in section A.2.
We can describe a generic fibre by intersecting (2.18) with

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for two complex numbers α and β. Away from α = 0 only lattice points on ∆ • F meet the K3 fibre. Hence all fibres except the (potentially) reducible ones are from the family of lattice polarized K3 surfaces with lattice polarization L = Pic(S). For a non-trivial top, there is a reducible fibre with components ν i z ν i ,m 0 i = 0. There can be additional reducible fibres if ∆ • F contains lattice points interior to its two-dimensional faces, see section 3.2 for an example.
To show that the first two requirements of [8], i.e. i) and ii) from section 1.1, are satisfied, we still need to show that the embedding of S into H 2 (Z, Z) is primitive. If S = [z 0 ] were not primitive, there must be a reducible fibre with several components all giving rise to equal classes in cohomology. Hence ν i z m 0 ,ν i i must be equal to nD for some divisor D. We now argue that this is impossible. First note that in case there are several ν i such that m 0 , ν i > 0, these cannot be all equivalent (or a multiple over Q of some class) as there cannot be a corresponding linear relation. Furthermore, for any projecting top, m 0 , ν i > 1 implies that there is at least a second ν j with m 0 , ν j = 1. Hence [z 0 ] = nD i for n > 1 for any D i inherited from the ambient space. If some of the D i contributing to (2.19) are reducible on Z, each extra components will give rise to an independent class in H 1,1 (Z) in accordance with (2.86), so that [z 0 ] can never be a multiple of a single class in H 2 (Z). Reducible fibres resulting from interior points of two-dimensional faces of ∆ • F can be treated similarly.

Formal construction
In order to continue our analysis and prove all the requirements for Z to be a building block, 1.1, we need to introduce some more machinery. This will also explain why the ad hoc construction presented above gives rise to a threefold with all of the desired properties. Furthermore, it will allow us to give elegant combinatorial formulae for the Hodge numbers of Z and the ranks of the lattices N and K.
For any polytope ∆ the M-lattice, there is an associated normal fan Σ n (∆) giving rise to a toric variety P Σn(∆) along with a divisor D ∆ . This description allows to use the theory of [22], which is a very powerful tool to analyse the geometry of a hypersurface corresponding to D ∆ by means of stratification.
The normal fan of a polytope is defined as follows: to every face Θ [k] of a polytope ∆, we may associate a coneσ where p ∆ is an arbitrary point lying inside ∆ and p Θ is an arbitrary point lying inside

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On the normal fan, there is a convex support function Ψ ∆ , linear on each cone of Σ n . For each cone of maximal dimension (four in our case) Ψ ∆ can be described by using the corresponding vertex m i and setting: for each point p in σ n (m i ). This also determines Ψ ∆ for all cones of lower dimension. The divisor can then be determined from and convexity means that In this construction, points of ∆ are associated with holomorphic sections of O(D ∆ ) and ∆ becomes the Newton polyhedron of a generic hypersurface defined by the zero locus of a section of the line bundle O(D ∆ ). This construction is particularly simple in the case of reflexive pairs of polytopes. Here, the normal fan Σ n (∆) is equal to the fan over the faces Σ f (∆ • ) of its polar dual and D ∆ = −K P Σn(∆) . In particular, for n-dimensional polytopes there is a one-to-one correspondence between k-dimensional faces of ∆ and n − k − 1-dimensional faces of ∆ • . A (regular, fine, star) triangulation of ∆ • then defines a refinement of the normal fan giving rise to a (partial) crepant desingularization of a Calabi-Yau hypersurface.

Normal fans of tops
In the case at hand, we are interested in the normal fan Σ n (♦) for the polytope ♦ defined in (2.12). Consider the face Θ [3] 0 ≡ ♦ ∩ F of ♦. Here, we find thatσ n (Θ [3] 0 ) is the entire lower half-space, bounded by F . Hence the dual cone appearing in the normal fan is This is good news, as the ambient space used in the ad hoc construction presented above not only includes rays over lattice points of ♦ • , but also the extra vertex ν 0 = (0, 0, 0, −1), so that we get a compact toric variety. It is not hard to realize, however, that in general where we use ♦ • ∪ ν 0 to denote the polytope which forms the convex hull over the union of ♦ • and ν 0 . To see this, note that the polytope ♦ • ∩ ν 0 is in fact reflexive for any projecting top ♦ • . Hence its face fan Σ f is equal to the normal fan of its polar dual, which can be described as the convex hull of ♦ ∪ (∆ F , 1) . (2.28)

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As the normal fans of ♦ and ♦ ∪ (∆ F , 1) are, in general, very different, (2.27) follows. As discussed in the following, a weaker statement can be shown, however. Namely, In order to describe the normal fan of a top ♦ and its relation to the dual top ♦ • defined by (2.84), let us try to exploit the known relations between a pair of reflexive polytopes. First of all, ♦ • ∩ F = ∆ • F and ♦ ∩ F = ∆ F form a reflexive pair of three-dimensional polytopes defining the algebraic family of the K3 fibre. We may extend ♦ • to a polytope ∆ • by considering the convex hull of ♦ • ∪ ν 0 .
(2.30) ∆ • is reflexive by the results of [16,21] as it is built from two projecting tops sharing the same ∆ • F . The dual polytope ∆ is described as the convex hull of ♦ together with ∆ F displaced by m 0 : As these polytopes form a reflexive pair, we have the usual relation for a dual pair of faces on ∆ • and ∆ satisfying Trivially, the set of faces of ∆ • is the same as the set of faces of ♦ • ∪ ν 0 . However, the set of faces of ∆ is different from those of ♦. Consequently, not every cone σ f (Θ •[k] ) appears in Σ n (♦). By construction, (2.31), ∆ contains precisely one face Θ [k+1] for every face Θ

[k]
F which extends vertically upwards from ∆ F . This means that such faces Θ [k+1] are orthogonal to the plane F . Depending on ♦, Θ [k+1] may extend also below Θ F is a face of ♦, but not of ∆. Under the polar duality of ( Hence polar duality on (∆, ∆ • ) will identify Θ we can identify Θ [k+1] as this face and conclude that When we collapse ∆ to ♦, it can happen that a face Θ [k+1] entirely disappears along with its cone in the normal fan. In this case there is no cone in Σ n (♦) which is the cone over the face Θ

Vertical and non-vertical faces
To describe in detail in which way Σ n (♦) differs from Σ f (♦ • ), let us introduce the following in its boundary. Such faces are called non-vertically embedded otherwise. As we are only considering projecting tops, it follows that for vertically embedded faces there exists a unique face Θ F ). This face must of course be vertical. Any other face above F (below F ) containing Θ F ) must be non-vertical and will hence be contained in the interior of ♦ • (♦) or the relative interior of one of its faces. For non-vertically embedded faces, however, there can be several non-vertical faces containing them in their boundary.
We now observe that for a dual pair of faces Θ , it will always be the case that one is vertically embedded, whereas the other is non-vertically embedded. First note that by ♦, ♦ • ≥ −1, and Θ it cannot be the case that both are vertically embedded at the same time. It hence remains to be shown that they also cannot both be non-vertically embedded at the same time. To see this, let us assume that both of them are non-vertically embedded. In this case, Θ [2−k] is also a face of the polytope ∆ constructed above (2.31). However, as such it must have a dual face of dimension k + 1 on ∆ • (defined in (2.30)) which is furthermore vertical and contains Θ

•[k]
F , violating our assumption that they are both non-vertically embedded. The only way out is that either Θ is vertically embedded and bounds the vertical face Θ •[k+1] which then becomes the polar dual of Θ under the polar duality of (∆, ∆ • ).
We are now in a position to discuss the structure of the normal fan Σ n (♦). Consider the reflexive pair ∆, ∆ • , (2.30) and (2.31), and the normal fan of ∆. Faces Θ (2.38) When we collapse ∆ to ♦, Θ [3−k] only stays a face if it extends below F , i.e. if the dual face Θ F ) disappears when we collapse ∆ to ♦. If we displace any face Θ when we collapse ∆ to ♦ and correspondingly, σ n (Θ ). These cones are the cones over the faces Θ

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We can hence summarize the discussion as follows: The normal fan of a top ♦ is equal to the face fan of ♦ • except for vertically embedded faces Θ which are connected to them above and below F . For such faces, the normal fan Σ n (♦) contains only a single k + 2-dimensional cone which is the union of σ f (Θ F . As we have described how to obtain the normal fan Σ n (♦) by gluing cones in the face fan As the fan Σ is in turn a refinement of Σ f (♦ • ∪ ν 0 ), we may think of the fan Σ used to define the ambient space for Z in the last section as a refinement of the normal fan of the lattice polytope ♦. Similar to [13], this allows to use the theory of [22] to study the geometry of Z.
Note that (2.12) implies that the support function defined by ♦, (2.24), is precisely such that −[K Z ] = D 0 . Furthermore, any refinement of Σ n (♦) which only introduces rays generated by lattice points on ♦ • is crepant: the proper transform of the hypersurface equation is simply given by (2.13) again and the anticanonical class stays D 0 . Refinements introducing higher-dimensional cones are trivially crepant.

Topological properties of building blocks
Having discussed the detailed structure of the normal fan Σ n (♦), we can now start to discuss the topological properties of the building blocks Z we have constructed. In order to find a matching and then compute the Betti numbers (1.6) of the resulting G 2 manifold, we need to know the Hodge number h 2,1 (Z), as well as the lattices In this section we compute N , the rank of K, as well as the Hodge numbers of a building block Z constructed from a pair of tops ♦, ♦ • . As the building blocks discussed in this paper are constructed from a refinement φ : Σ → Σ n (♦) of the normal fan of the polytope ♦, the theory of [22] can be applied.

The stratification associated with a refinement of the normal fan
Every toric variety P Σ enjoys a stratification into algebraic tori (C * ) d which is determined by its fan Σ [27]. For every k-dimensional cone σ ∈ Σ(k) of the fan of an n-dimensional (complex) toric variety, there exists a corresponding n − k-dimensional stratum S σ ≡ (C * ) n−k and we may write

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which is not unexpected as any toric divisor is again a toric variety (with fan star(σ i )). A ray σ i corresponds to a homogeneous coordinate z i and, for simplicial fans, the closure of the associated stratum S σ i is simply given by setting z i = 0. Similar results hold for toric submanifolds of higher codimension. If we consider an algebraic submanifold Z ⊂ P Σ of such a toric variety, we may intersect each stratum with Z and thereby obtain a stratification of Z: As each cone in the normal fan Σ n (♦) is associated with a face of ♦, the (in general singular) hypersurface Z s in P Σn(♦) has a stratification associated with the face structure of ♦, ). As we have discussed above, the fan Σ giving us the ambient space P Σ of our resolved hypersurface Z is a refinement of Σ n (♦). Here, the resolution φ P : P Σ → P Σn(♦) associated with a refinement φ : Σ → Σ n (♦) induces a resolution φ Z : Z → Z s . This point of view has the advantage that we can describe the stratification of Z as Here E Θ [4−k] is the exceptional set originating from the refinement of the cone σ n (Θ [4−k] ) For every l-dimensional cone of Σ interior to σ n (Θ [4−k] ), there is a stratum (C * ) k−l in E Θ 4−k .

Computing Hodge numbers from stratification
The reason for introducing all of this terminology and studying the normal fan in detail, is that the Hodge numbers of Z can be computed from the Hodge numbers of its strata, which in turn have a combinatorial characterization [22]. The key is using the 'Euler-characteristic' associated with the mixed Hodge structure of cohomology with compact support: The numbers e p,q (X) become equal to the (−1) p+q h p,q (X) for smooth compact varieties and enjoy the properties so that knowledge of the e p,q for all strata Z σ allows the computation of the Hodge numbers of Z.

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Using the methods of [22] it is straightforward to compute the numbers as we discuss now. The Hodge-Deligne numbers of the strata are determined by [22] for p > 0 as well as Here, * counts lattice points contained in the relative interior of a face and the functions ϕ n are defined as where jΘ stands for the polytope which is obtained by scaling all vertices of the face Θ by j and then taking the convex hull. Note that simply Let us introduce the following notation: we denote the number of points on the nskeleton of Θ by n (Θ). We can use this to rewrite e.g. the sum over the number of interior points of all n-dimensional faces as n (Θ) − n−1 (Θ). Using this notation For a face of dimension k ≥ 4 we also have that Finally high Hodge numbers, p + q ≥ n, satisfy As a preparation for later sections, let us derive the Hodge-Deligne numbers e p,q of strata Z Θ [k] for k ≤ 4. As a corollary of (2.54), e 0,0 (Z Θ [1] ) = * (Θ [1] ) + 1, i.e. the stratum Z Θ [1] consists of * (Θ [1] ) + 1 points. Hence

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For Z Θ [2] , we immediately find e 1,1 (Z Θ [2] ) = 1. Furthermore, e 1,0 (Z Θ [2] ) = − * (Θ [2] ), and we can write Similarly, we find for Z Θ [3] that Finally, let us compute some of the Hodge-Deligne numbers of Z Θ [4] . We have that In general, the toric variety P Σn(♦) obtained from the normal fan Σ n (♦), and correspondingly the hypersurface Z is not smooth and we need to resolve it. This can be done torically by refining the fan π : Σ → Σ n (♦). As we will always work with smooth hypersurfaces in practice, we continue to refer to the resolved hypersurface by Z.
The topology of Z σ = Z ∩ S σ solely depends the dimension of σ and on the position of σ within the normal fan Σ n (∆). If σ is an l-dimensional cone contained in the relative interior of the k-dimensional cone of Σ n (♦) associated with a face Θ [n−k] we can write (2.65) In order to compute Hodge numbers we hence also need to know the Hodge-Deligne numbers of (C * ) n , they are simply given by e p,q ((C * ) n ) = δ p,q (−1) n+p n p . (2.66) For a point, i.e. d = 0, we have that all e p,q (pt) vanish except e 0,0 (pt) = 1.

Hodge numbers of building blocks
To compute the Hodge numbers of a building block Z, we start by noting that Z enjoys a stratification points on σn(Θ [3] ) + C * 1-simplices on σn(Θ [3] ) + pt 2-simplices on σn(Θ [3] ) ] JHEP10(2017)083 In the above expression, 'points/n-simplices in σ' for some cone σ is meant to be read as 'points/n-simplices in the relative interior of σ which are lattice points on ♦ • ∪ ν 0 . The contribution of various strata of P Σ crucially depends on the location of the associated points/n-simplices in the normal fan Σ n (♦). As we have worked out the relation between faces of ♦ • and cones in the normal fan Σ n (♦) in section 2.3.1, we can combine (2.67) with the relations of section 2.4.2 to find the Hodge numbers of Z.
To familiarize the reader with this method of computation, let us start with Hodge numbers h i,0 (Z) which are relatively simple to compute. First note that only Z ♦ potentially contributes to e 3,0 and * (♦) = 0, so that we directly find h 3,0 (Z) = 0. Next, we have e 2,0 (Z) = e 2,0 (Z) + and e 1,0 (Z) = e 1,0 (Z) + In the last computation, we have used that each three-dimensional face of ♦ bounds precisely two two-dimensional faces, so that the sum over three-dimensional faces contributes 2( 2 (♦) − 1 (♦)).
One may also easily derive formulae for the Hodge numbers of toric divisors Y i on Z. We have done this for Calabi-Yau hypersurfaces in appendix B and the formulae derived there can be straightforwardly used for toric divisors of building blocks Z constructed from a pair of tops. The crucial input is the location of the point ν i in the normal fan Σ n (♦) and one only needs to replace 'vertex' ('contained in 1D face', 'contained in 2D face') by 'contained in one-dimensional cone' ('contained in two-dimensional cone','contained in three-dimensional cone') of Σ n (♦) to make sense of the formulae.

The lattices N and K
Let us now discuss the lattices N and K. As already remarked in section 2.2 we associate the embedding of the fibre S with the divisor D 0 = {z 0 = 0}. A generic fibre is given by For such a K3 surface, there are two interesting lattices: Pic(X (∆ F ,∆ • F ) ) contains all divisors, whereas Pic tor (X (∆ F ,∆ • F ) ) only contains divisors which originate from divisors of the ambient space. Correspondingly, Pic(X (∆ F ,∆ • F ) ) is contained in the Picard group of every fibre of Z and Pic tor (X (∆ F ,∆ • F ) ) is generated by restricting all divisors corresponding to points on ∆ • F to X (∆ F ,∆ • F ) . As every such point gives rise to a divisor on the threefold Z as well, Pic tor (X (∆ F ,∆ • F ) ) must be contained in N . Note that there is a two-dimensional cone in Σ generated by ν i , ν 0 for every lattice point ν i on ∆ • F . We may think of these two-dimensional cones as the divisors on S in the image of ρ.
Things are slightly more complicated for other generators of Pic(X (∆ F ,∆ • F ) ). Depending on the details of (♦, ♦ • ), these may or may not be contained in N . Whenever there is a JHEP10(2017)083 F on ∆ • F such that, for Θ [1] F the dual face on ∆ F , the product * (Θ is non-zero, there is an extra contribution to Pic which is not contained in Pic tor . Let us consider a point ν i on ∆ • F contained in the interior of a face Θ • [1] for which (2.76) does not vanish. This signals that on S we can write and the D α i will be contained in N if only if the above relation also holds on Z. Whereas the reducibility of toric divisors for X (∆ F ,∆ • F ) corresponding to interior points of twodimensional cones of Σ n (∆ F ), comes from interior points of the dual one-dimensional face Θ of ∆ F , we have to consider the normal fan Σ n (♦) in the case of Z. Here, only those toric divisors which correspond to interior points of three-dimensional cones of Σ n (♦) can become reducible. For every one-dimensional face of ∆ • F , which forms a one-dimensional face Θ

•[1]
F of ♦ • , we must hence discriminate whether they sit in two-or three-dimensional cones of the normal fan Σ n (♦). As we have discussed in section 2.3.2, there is a simple rule: the cone over any face Θ F is contained in a vertical face, then it is contained in a cone of dimension i + 2 of the normal fan. This i + 2-dimensional cone is the cone associated with its dual face Θ [1] F under the polar duality of (∆ F , ∆ • F ). In this situation, the divisors associated with lattice points on Θ F bounds only non-vertical faces, only the contribution to Pic tor associated with Θ

•[1]
F is in the image of ρ.
F bounds a vertical face, the image of ρ contains the lattice besides the contribution to Pic tor .
Note that the lattice N is always primitively embedded into Pic(X (∆ F ,∆ • F ) ). This can be seen as follows: N is given as for all α, β and with i running over all faces Θ contained in a two-dimensional cone of Σ n (♦). By construction, an orthogonal complement is primitively embedded.

•[1]
F,i , the lattice N is hence and its rank is The rank of K can now be found from The divisors contributing to K correspond to singular fibre components, which in turn correspond to lattice points on ♦ above F (see (2.16)) as well as points interior to twodimensional faces of ∆ • F .

Summary
Let us summarize the main points of the construction presented above and finish the proof that it indeed leads to a building block as defined by [8], i.e. show that it satisfies the requirements i) to iv) in 1.1.

Starting from a projecting top ♦
and we may choose coordinates such that m 0 = (0, 0, 0, 1) and ν 0 = (0, 0, 0, −1). As a convex lattice polytope, ♦ defines a toric variety P Σn(♦) via a normal fan Σ n (♦), as well as a line bundle O(D ♦ ) on it. The face fan Σ(♦ ∪ ν 0 ) of ♦ • ∪ ν 0 is a refinement of Σ n (♦). In general, P Σ f (♦∪ν 0 ) will have singularities which meet Z. We may however, further refine the fan Σ according to a appropriate 10 triangulation of the ♦ • to find a maximally crepant desingularisation. In our case of interest, where Z is a threefold and P Σ a fourfold, such a triangulation will only leave point-like singularities 11 in P Σ which do not meet a generic hypersurface. The hypersurface Z is then given by a generic section of O(♦): (2.85) 9 Here, our notation • is meant to indicate 'dual' rather than 'polar dual'. 10 We would like such triangulations to involve all lattice points on ♦ • and give rise to a projective toric variety PΣ. 11 The reason for this is that any fine triangulation of a face of dimension less than three leads to simplices of lattice volume one.

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Its Hodge numbers are and the ranks of the lattices N and K defined in (2.39) are For a projecting top, ∆ • F = ♦ • ∩ F and ∆ F = ♦ ∩ F are a reflexive pair [16]. The hypersurface Z is hence fibred by a K3 surface from the algebraic family defined by the reflexive pair (∆ • F , ∆ F ). We can now start with the proof of requirements i) to iv) in 1.1 needed for a building block.
i) This is true by construction. In particular, setting z 0 = 0, we find a K3 surface S given as a hypersurface in a toric variety constructed from the reflexive pair (∆ F , ∆ • F ). Furthermore, we have that which is equal to the class of the fibre of the fibration implicit in the top. iii) As we have remarked above, the lattice N is primitively embedded in the Picard lattice of the generic fibre, Pic(X (∆ F ,∆ • F ) ). As the Picard lattice is primitively embedded in H 2 (S, Z), it follows that also N is primitively embedded in H 2 (S, Z). iv) As Z is a projective algebraic manifold which is defined as a hypersurface by a Newton polytope ♦ and embedded in a toric variety P Σ , where Σ is a refinement of the normal fan Σ(♦), we may use the results of [38] and compute Tors(H 3 (Z, Z)) combinatorially as Here, N ♦ is generated by all lattice vectors v in N such that the function f v ≡ v, * on ♦ has a minimum along a face of dimension greater than two.
Note that f ν 0 attains a minimum along the face Θ from lattice vectors parallel to F . To show that (2.89) vanishes, we make use of the following three key facts [16,21]: a) For a projecting top ♦ • , its dual ♦, (2.84), is also projecting (see section 2.2). b) Any two projecting tops with the same ∆ F can be assembled into a reflexive polytope.
c) There is a known list of 16 reflexive polyhedra for which (2.89) is non-trivial [38].
For any top ♦ we may use a) and b) to form a reflexive polytope ∆(♦) using ♦ and a copy ♦ with the fourth coordinate inverted. If the quotient (2.89) is nontrivial for such a top ♦, it must also be non-trivial for ∆(♦). However, out of all the four-dimensional reflexive polytopes, there are only sixteen cases for which (2.89) is nontrivial [38] (see also [39]). We have recorded this list in appendix D. It is then possible to directly check if any of the sixteen relevant four-dimensional polytopes admits a sub-polytope cutting it into a pair of projecting tops. We have done this computation using SAGE [40]. Even though all but three of these polytopes do have reflexive subpolytopes, none of these turns out to be projecting. We have hence shown that (2.89) must be trivial for any projecting top.
This completes the proof that our construction for Z leads to a building block as defined in [8] for any projecting top.

Relation to construction via semi-Fano threefolds
In [7], building blocks for G 2 manifolds are constructed by appropriate blowups of so-called semi-Fano threefolds A, which are a subclass of weak Fano threefolds.
A weak Fano threefold is a non-singular projective complex threefold A such that the anticanonical bundle −K A is big and nef. This means that −K A · C > 0 for any curve C in A and (−K X ) 3 = 2g − 2 > 0. The integer g is called the genus of A.
For a weak Fano threefold A, there is an anticanonical morphism ϕ : A → A ac to the anticanonical model A ac of A. If this map only contracts divisors to curves and curves to points (but not divisors to points) it is called semi-small and, following [7], the threefolds for which this is the case are called semi-Fano threefolds. 12 For such threefolds, [7] construct building blocks as follows. First, choose two anticanonical hypersurfaces S and S meeting transversely. Then blow up A along S ∩ S . In practice, we may accomplish this as follows. Let S 0 be defined by an equation P 0 = 0 and S ∞ by P ∞ = 0 in A. The building block Z is then described in A × P 1 where [ξ 0 : ξ ∞ ] are homogeneous coordinates on the P 1 .
In case A is the toric variety associated to a reflexive polytope ∆ • F , such a manifold Z is obtained from our construction by using the trivial top, i.e. the convex hull ♦ • of ∆ • F ∪ (0, 0, 0, 1). A plays the role of the ambient (weak Fano) toric manifold in which JHEP10(2017)083 the fibre S 0 is embedded, i.e. the (resolution of) the toric variety P ∆ F . A toric threefold constructed from a three-dimensional reflexive polytope ∆ • is semi Fano if and only if ∆ • has no interior points to facets [7]. Of the 4319 reflexive polytopes in three dimensions, 899 have this property. For semi-Fano threefolds A, the building blocks obtained as (2.90) have a trivial K if the K3 surfaces S 0 and S ∞ are smooth. Of course, one may choose e.g. a singular S and then construct a crepant resolution of (2.90), as done in [7,9,23]. The strength of our construction is a systematic and convenient characterization of such degenerations, i.e. a framework to systematically enhance K and hence b 2 of the resulting G 2 manifolds. Furthermore, a description in terms of polytopes lends itself to a straightforward description of singular transitions (at least on the level of the building blocks Z).
For the blowup (2.90) to give rise to a building block, it is sufficient to demand that A is a weak Fano threefold. The relevance of the extra condition of being semi-Fano lies in the deformation theory of the anticanonical hypersurfaces of A. For any weak Fano threefold, an anticanonical hypersurface is a member of a family of lattice polarized K3 surfaces with polarizing lattice L A . One may hence wonder whether the moduli space 13 F A of the embedded K3 surface X → A is as large as the moduli space of the lattice polarized family K N A . It turns out that this is indeed the case if A is semi-Fano. In this case the forgetful morphism is generically surjective [7]. If we are given two building blocks and have found primitive lattice embeddings which facilitate a glueing to a G 2 manifold, we furthermore have to be able to choose the holomorphic two-forms and Kähler forms such that they satisfy (1.4). It is not hard to see if this can be satisfied for a pair of families of lattice polarized K3 surfaces, but we need that the K3 fibres of Z + and Z − can be choose appropriately. As these fibre are realized as hypersurfaces (2.91) is the crucial result allowing us to decide whether we can form the twisted connected sum.

Examples
In this section, we discuss a few examples of building blocks obtained from tops in ascending order of complexity.
In compactifications of M-Theory on manifolds of G 2 holonomy, the number of massless U(1) gauge symmetries is determined by the Betti number b 2 . From (1.6), we may distinguish two different sources: The dual cycles of the forms originating from the first part, K ± , are components of degenerate K3 fibres (times the extra S 1 ) and we can think of them as 'localized' on Z. In particular, they do not play any role in the gluing to a G 2 manifold. Collapsing such fibre components (if possible) gives rise to U(1) charged massless matter (as observed in [23]).

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For the second part, N + ∩ N − , the dual 5-cycles can be thought of as two-cycles fibred over the whole base S 3 . Collapsing the fibres of such five-cycles (if possible) would give us singularities of codimension four, which give rise to gauge symmetries in compactifications of M-Theory. We can hence morally think of the U(1)s related to such cycles as the Cartan U(1)s of some non-abelian gauge group [41].

Building blocks with a quartic K3 fibre
Some of the simplest examples of building blocks use a quartic K3 surface embedded in P 3 as the fibre. The trivial top is realized as a polyhedron with the vertices In this case, the dual top has vertices and our construction simply gives a building block realized as a hypersurface of degree (4,1) in P 3 × P 1 . There are 128 degenerate and no reducible fibres. We can use the Lefschetz hyperplane theorem to find h 1,1 = 2 and h 1,0 = h 2,0 = 0. Using adjunction we can also compute characteristic classes of Z, which then give us from the Euler characteristic and the arithmetic genus. The same values can be obtained from (2.86). As we have a quartic K3 surfaces as the fibre, we find rk(N ) = 1 and hence rk(K) = 0, so that this building block does not give rise to any U(1) of the 'localized' type.
A degenerate fibre with four components. We may make this example slightly more interesting by forcing a degenerate fibre given by This example has appeared in [7-9, 23] and we may reconstruct it starting from a pair of dual tops with vertices

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Here, we have implemented the fibre embedding by using the N-lattice polytope corresponding to P 3 as ∆ • F , and engineered four fibre components by placing four points on top of it. We have also indicated a labelling for the vertices of ♦ • .
Evaluating (2.86) one finds that As the rank of N remains 1, we find rk(K) = 3. Hence a G 2 manifold which is constructed from such a building block as a twisted connected sum will receive three classes in H 2 (X) irrespective of the details of the gluing which in turn contribute three U(1) factors to a compactification of M-Theory. The classes in K are contributed from the pointsν i which correspond to the components of the reducible K3 fibre. The four divisors [ẑ i ] are rational surfaces 14 meeting along six rational curves. The dual graph of these intersections is topologically S 2 , so this is a fibre of type III in the classification of [42,43]. Note that the lattice point (0, 0, 0, 1) on ♦ • sits inside a four-dimensional cone of Σ n (♦), so that it does not give rise to a divisor on Z.
Let us repeat some of the analysis of [23] in the language of this paper. The normal fan Σ n (♦) is determined by its cones of maximal dimension, they are as well as the cone ν 1 ,ν 2 ,ν 3 ,ν 4 . Note that the coordinates z i related to the vertices ν i of ♦ • appear as exceptional divisors upon refinement of the normal fan Σ n (♦) to the fan Σ. There are four curves C i which are given by [ẑ i ] · [z 0 ] on Z before resolution (refinement of the normal fan). They correspond to two-dimensional cones of Σ n (♦) spanned byν i and ν 0 . As the dual two-dimensional faces on ♦ are the ones spanned by vertices µ l , µ m and µ n , they have three interior points, so that the genus of the C i is three. Any two such curves meet in four points. In the fan refinement the ν i are introduced inside of the two-dimensional cones spanned byν i and ν 0 . Hence we may think of the [z i ] as being a fibration of P 1 over the curves C i , which have genus 3. Note that we may also think of Z as the blowup of a singular family in P 3 × P 1 . Thinking in this way, the coordinatesẑ i correspond to the exceptional divisors.
The 24 rigid rational curves found in this geometry in [23] can be seen as follows. There is a triangulation of ♦ • such that for any pair of divisors This triangulation corresponds to introducing the rays refining Σ n (♦) to Σ in the order ν 1 , ν 2 , ν 3 , and ν 4 . The corresponding two-dimensional cones of Σ sit inside three-dimensional cones of Σ n (♦), which are in turn dual to one-dimensional faces Θ [1] of ♦ with three interior points each. This means that C ij has four irreducible components, each of which is a P 1 . We hence find 4 · 6 = 24 such curves. Note in particular that these curves do not intersect the fibre S 0 as they are away from ν 0 . This means that we may think of them as being away from the region of Z which is used in the gluing process to a G 2 manifold.

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The intersection numbers of these curves with the divisors [ẑ i ] are Each one of the divisors [ẑ i ] defines a class in H 1,1 (Z, Z) which is in the kernel K of the restriction map to S 0 at z 0 = 0. If we glue the building block (times S 1 ) with an appropriate second building block, each of these divisors hence defines a class in H 2 (X, Z) of the resulting G 2 manifold. For M-Theory compactifications on X, we can hence associate a U(1) generator Q i with each of the [ẑ i ]. There is a linear relation which says that Hence these divisors only define three independent classes in K and correspondingly the Q k only generate three independent U(1)s. States corresponding to wrapped M2 branes on the curves C ij are charged under those U(1)s with charges given by These charges can be read off from the table above. A choice of independent U(1) generators reproducing the charge matrix of [23] is given by (3.11)

Building blocks with a K3 fibre of degree 2
Let us consider another simple type of K3 surface with rk(N ) = 1 as the fibre. We can realize a K3 surface S with P ic(S) = (2) as a double cover over P 2 . Constructing the corresponding polytope ∆ • F as well as the trivial top and its dual is straightforward: As in the first example in section 3.1 above, choosing the trivial top in the N lattice gives a dual top with the maximal number of vertical faces. This example has an extra twist, though. The polytope ∆ • F has an integral point interior to a 2-dimensional face, (1, 0, 0, 0). In the normal fan Σ n (♦), this point sits inside a three-dimensional cone, so that there is a corresponding divisor on Z but not on S 0 . Hence we find K ⊃ Z. The Hodge numbers of this example are h 1,1 (Z) = 3 h 2,1 (Z) = 37 .
We can construct a closely related model Z for which K = 0. Replacing the vertex (0, 0, 0, 1) with (1, 0, 0, 1) creates a vertical face on ♦ • which contains (1, 0, 0, 0) in its boundary. Correspondingly, the 2-dimensional face of ∆ • F containing (1, 0, 0, 0) does not give rise to a cone in the normal fan of ♦ . This means that now (1, 0, 0, 0) sits inside a 4-dimensional cone of Σ n (♦ ), so that there is no corresponding divisor on Z . This is confirmed by computing the Hodge numbers from (2.86): Let us first discuss the geometry of the fibre S and the polytope ∆ • F in some detail. ∆ • F has four vertices and the number of interior points of the dual two-dimensional faces is vertex Divisor * (Θ [2] ) (2, 2, 1, 0) Hence the divisors corresponding to the first two vertices are elliptic curves and the divisors corresponding to the last two vertices have genus 4. Their self-intersection is D 1 · D 1 = D 2 · D 2 = 0 and D 3 ·D 3 = D 4 ·D 4 = 6. The polytope ∆ • F has a further integral point at (1, 1, 0, 0)

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which sits in between ν 1 and ν 2 . The dual of this edge on ∆ F has vertices (−2, 1, 1, 0) and (1, −2, 1, 0). This edge has 2 interior points. Hence the divisor D 5 corresponding to ν 5 = (1, 1, 0, 0) consists of three rational curves D α 5 which each meet D 1 in a single point. A basis of P ic(S) is given by D 1 5 , D 2 5 , D 3 5 , D 1 which have inner form Note that only D 5 = D 1 5 + D 2 5 + D 3 5 and D 1 are realized as toric divisors, so that P ic tor (S) is two-dimensional and has inner form As we have considered the trivial top over ∆ • F above, for which all faces are non-vertical, only Pic tor (S 0 ) is in the image of ρ, so that rk(N ) = 2. Furthermore, rk(K) = 0 as all divisor classes except [S 0 ] restrict non-trivially to S 0 . Geometrically, the K3 fibration Z has a non-trivial monodromy acting on Pic(S) which only leaves D 5 and D 1 invariant. Correspondingly, only those two become divisors on Z.
We can change the top ♦ • to ♦ • by using as a vertex (1, 1, 0, 1) above F instead of (0, 0, 0, 1). This turns the face which contains (1, 1, 0, 0) in its boundary into a vertical face and we hence expect all of the divisors D α 5 to give rise to divisors of Z . Correspondingly, (2.86) now tells us that and we find that N = Pic(S), so that rk(N ) = 4 while keeping K = 0.

A very large top
Finally, let us consider a rather extreme example. There is a unique polytope ∆ • in the Kreuzer-Skarke list which has the maximal possible number of lattice points of any reflexive polytope, 680. The Calabi-Yau manifold X (∆,∆ • ) has the largest Euler characteristic of any toric hypersurface Calabi-Yau threefold, 960, and is the mirror to a generic elliptic fibration over the Hirzebruch surface F 12 . As discussed in [21], we can cut ∆ • in half to find two (isomorphic) projecting tops ♦ • . They are the largest projecting tops over ∆ • F corresponding to an elliptic K3 surface with one II * fibre. The vertices of ♦ • and its dual are so that rk(K) = 240. We may construct an extraordinary G 2 manifold X Z,Z by gluing two building blocks Z ± both isomorphic to the Z just constructed (times S 1 ) such that N + ∩ N − = 0. 15 This means that Λ/(N + + N − ) = U and N ± ∩ T ∓ = U ⊕ (−E 8 ). By (1.6), such a G 2 manifold will have Betti numbers An M-Theory compactification on X Z,Z will hence have gauge group U(1) 480 ! To our knowledge, this would make X Z,Z the G 2 manifold with the largest Betti numbers constructed so far.
Reversing the roles of ♦ • and ♦ yields a building blockẐ with the same K3 fibre (Pic(S) = N = U ⊕ (−E 8 )) but with so that now rk(K) = 0. Orthogonally glueing two copies ofẐ (times S 1 ) to form a G 2 manifold XẐ ,Ẑ or orthogonally gluing one copy of Z with one copy ofẐ to form a G 2 manifold X Z,Ẑ then results in the Betti numbers  We cannot help but wonder if there are singular transitions in M-Theory connecting the compactifications on X Z,Z , XẐ ,Ẑ and X Z,Ẑ . Investigating the associated physics promises to be very interesting.

Discussion and outlook
In this work we have demonstrated that four-dimensional projecting tops can be straightforwardly used to manufacture the building blocks used to construct G 2 manifolds as twisted connected sums (TCS). This is not at all unexpected, as such tops capture the geometry of 'half' a K3-fibred Calabi-Yau threefold. Conveniently, a great deal of information on the geometry of both a generic K3 fibre and its degeneration is captured by the combinatorics of the top. In particular, it is possible to combinatorially determine the 15 Strictly speaking, this requires proving that we can choose the complex structure of the algebraic family such that the matching (1.4) can be satisfied, i.e. Im(Ω±) ⊂ U and Re(Ω±) ⊂ U ⊕ (−E8). In this case we can choose a complex structure and a Kähler form such that there exists a (rather trivial) lattice isometry inducing (1.4). For this example, we unfortunately cannot use the surjectivity of (2.91), as the polytope ∆ • F has interior points in 2-dimensional faces, so that the ambient space of the fibre is not semi Fano.

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relevant topological data: the Hodge numbers of the building block, the group N and the rank of K. While these results are primarily of a mathematical nature, it is hoped that they pave the way for a better understanding of physics associated with compactifications of M-Theory on G 2 manifolds.
Realizing K3 fibres embedded in toric varieties in order to construct building blocks is nothing new and has been already explored in [7]. The description in this paper, however, allows for an elegant characterization of K3 fibrations with degenerate fibres. The usefulness of this is twofold. First of all, it allows a constructive control over the Hodge numbers of building blocks and hence the Betti numbers of resulting G 2 manifolds. Furthermore, all of this is done in a language familiar to string theorists. This should further strengthen the bridge from complex algebraic geometry to G 2 manifolds provided by the TCS construction, in particular in applications to physics. Secondly, as is well-known from the description of Calabi-Yau manifolds, polytopes anticipate possible singular transitions. Presently, this is only clear on the level of the building blocks and more work is needed in order to formulate clear criteria when such a transition is also possible in G 2 moduli space.
The construction of K3 fibred threefolds with c 1 = [f ibre] from tops we have presented is easily generalized to arbitrary dimensions. Here, the result is a Calabi-Yau n-fold fibred algebraic n + 1-fold with c 1 = [f ibre], obtained from a n + 2-dimensional top. As already remarked, this construction yields rational elliptic surfaces for n = 1. As is well-known, there is a semi-stable degeneration of a family of K3 surfaces into a pair of rational elliptic surfaces. When the K3 surface is described as a toric hypersurface and the corresponding polytope can be disassembled into a top and bottom, our construction yields an explicit realization of the two rational elliptic surfaces. It seems likely that similar semi-stable degenerations of Calabi-Yau n-folds are encoded in projecting tops for arbitrary dimensions. From this point of view, building blocks can be thought of as three-dimensional generalizations of rational elliptic surfaces.
From the point of view of physics, the most interesting aspect of G 2 manifolds lies in their possible degenerations. As already remarked, the description of building blocks given here allows for a straightforward construction of singular building blocks. It remains to be seen under which circumstances such singularities can also be reached in the moduli space of the associated G 2 manifolds. Clearly, this necessitates a detailed study of (co)associative submanifolds, which form the calibrated cycles of a G 2 manifold. There exist results on how such submanifolds arise from the point of view of the TCS construction [8], and many interesting ideas for how this can be employed to degenerate the associated G 2 manifolds have been discussed in [23,41].
While questions about existence of the gluing morphism can be cast in the language of lattice embeddings using the Torelli theorem, 16 it remains an open problem to classify all possibilities. As we have seen, both the Picard lattice and the lattice N can be readily determined from the polytope data. It remains to be seen whether this can be used to describe at least a well-defined class of all possible matchings for two given pairs.

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Finally, it should be noted that the TCS construction describes a G 2 manifold as a (nonholomorphic) K3 fibration over S 3 base, which ties in nicely with the M-Theory/heterotic duality and the SYZ fibration. If will be interesting to see if this can be exploited to learn about either side of the duality map.
A Lattices, mirror symmetry for K3 surfaces and reflexive polytopes

A.1 Lattices
In this section a few helpful facts on lattices are reviewed. A good reference for this is given by [44].
A lattice L is a free abelian group of finite rank, so that L ∼ = Z n . It is endowed with an inner form ·, · and the numbers r ± of positive/negative eigenvalues are called its signature. Often it is convenient to think of a lattice as being obtained by forming arbitrary linear combinations, with integer coefficients n i , of a finite set of generators v i in R r + ,r − so that for any l ∈ L l = In this way, a lattice inherits its inner form from R r + ,r − . The dual lattice L * contains all vectors which have an integer inner product with all elements of L.
A lattice is called even if all squares l, l of its elements are even integers. An unimodular lattice L is a lattice such that L * ∼ = L. Even unimodular lattices only exist when r + − r − = 0 mod 8, and they are unique (up to isomorphism) if both r − and r + are non-vanishing. In this case for some integers a and b. Here, ±E 8 is (±) the root lattice of E 8 and U is the hyperbolic lattice with inner form 0 For non-unimodular lattices, there is a nontrivial quotient G L = L * /L which is a finite abelian group. On G L , there is an inner quadratic form q L and a bilinear form b L defined by q L and b L take values in Q/2Z and Q/Z, respectively.

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An embedding N → L of lattices is called primitive if the quotient is torsion-free. This is equivalent to saying that there is no lattice element n in N such that n/m ∈ L but not in N for any integer m > 1. Note that this means that primitive embeddings are transitive, if N → M is primitive and M → L is primitive, then so is N → L.
For a primitive embedding of a lattice N into an even unimodular lattice L, N and its orthogonal complement N ⊥ in L share the same discriminant form (up to a sign) This statement has a converse, i.e. for two lattices N and M there exists a primitive embedding into an even unimodular lattice L such that N = M ⊥ in L (and vice versa) if their discriminant forms satisfy (A.5) and if their ranks and signatures add up in the obvious way.
A family of lattice polarized K3 surfaces with polarizing lattice L is a family for which the holomorphic two-form Ω is perpendicular (under the natural inner form on H 2 ) to L. The period domain of a lattice polarized K3 surface is given by The period map is surjective onto the period domain and the moduli space of a lattice polarized K3 surface is given by where Γ is the group of automorphisms of Λ. One incarnation of mirror symmetry for K3 surfaces associates families of lattice polarized K3 surfaces. This topic goes back a long way in mathematics [49] and exists in several JHEP10(2017)083 versions. In physics [48] the objects we should consider as mirror pairs are pairs of lattice polarized K3 surfaces with lattices N and N such that there is a primitive embedding From the embedding (A.9) we learn that the discriminant forms of N and N must agree as in (A.5). Conversely, for any lattice N which can be primitively embedded into N → U ⊕2 ⊕ (−E 8 ) ⊕2 there is an associated mirror pair of lattice polarized families of K3 surfaces.

A.3 K3 surfaces from reflexive polyhedra
Such a correspondence is indeed realized [51] by using Batyrev's construction of dual reflexive polytopes [13]. Starting from a pair of dual reflexive polytopes ∆ • and ∆, we can define a toric variety P Σ by constructing a fan Σ from a (regular, fine, star) triangulation The inner form on Pic tor (X (∆,∆ • ) ) is determined by combinatorial data and can be computed using the theory of [22]. Every ν i corresponding to a vertex of ∆ • is a curve of genus * (Θ [2] ), where Θ [2] is the dual 2-dimensional face on ∆ and * counts interior lattice points. Hence D i · D i = 2 * (Θ [2] ) − 2 for any vertex ν i . A toric divisor D i corresponding to a point interior to a 1-dimensional face Θ • [1] decomposes into 1 + * (Θ [1] ) P 1 s when restricted to the K3 hypersurface. Only their sum is contained in Pic tor (X (∆,∆ • ) ). These P 1 s are not mutually intersecting, so that D i · D i = −2(1 + * (Θ [1] )) for ν i an interior point of a 1-dimensional face Θ • [1] . Finally, the intersecting between two toric divisors D i and D j is non-zero only if they are neighbours along a common 1-dimensional face Θ • [1] . In this case D i · D j = 1 + * (Θ [1] ), where Θ [1] is the dual 1-dimensional face on ∆. This finishes the description of Pic tor (X (∆,∆ • ) ) which has rank where 1 counts lattice points on the one-skeleton. 18 Although 3-dimensional polytopes do not have a unique triangulation, the strata which have a nontrivial restriction to a Calabi-Yau hypersurface are unique.

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Let us now describe the polarizing lattice of the family of K3 hypersurfaces X in P Σ . As we have already mentioned, toric divisors corresponding to points interior to 1-dimensional faces of ∆ • can become reducible when restricted to X, so that Pic(X (∆,∆ • ) ) is, in general, larger than Pic tor (X (∆,∆ • ) ). Again, using the stratification associated with the ambient toric variety P Σ and the theory of [22] gives a detailed picture of divisors on X (∆,∆ • ) appearing as components of the restriction of toric divisors. Note that this method does not guarantee that we have succesfully determined the whole Picard lattice of a generic member of the algebraic family of K3 surfaces we are considering (although the consideration of mirror pairs of K3 surfaces suggests this is the case), see [50] for a more rigourous treatment. Keeping in mind this cautionairy remark, we continue to denote the lattice obtained by the stratification method by Pic(X (∆,∆ • ) ) throughout this article. Note that we only require the image of the Picard group of the generic fibre under the restriction map for the present work, see sections 1.1 and 2.4, which we can confidently identify.

•[1]
i ): A.4 Mirror symmetry and reflexive three-dimensional polyhedra From the discussion above it follows that gives us the rank of the polarizing lattice (i.e. Picard group of a generic member) of the family X (∆ • ,∆) described above. Applying this formula to a pair of dual reflexive polytopes JHEP10(2017)083 naively leads to contradiction with (A.9) as |Pic(X (∆,∆ • ) )| + |Pic(X (∆ • ,∆) )| = 20 + 17) i.e. the dimension is too large by the value of the correction term in (A.16).
The dimensions do work out if we consider mirror families with lattice polarizations In fact, as has been explicitly verified in [51] (and repeated by the present author), the discriminant forms on Pic(X (∆,∆ • ) ) and Pic tor (X (∆ • ,∆) ) agree for a pair of reflexive polytopes, so that a primitive embedding (A.9) exists and we have found a mirror pair. The reason for this seemingly asymmetric choice is that the correction term [1] ) counts non-toric divisors and non-polynomial deformations of X (∆,∆ • ) at the same time. The two are mutually exclusive, however: if one constructs X (∆,∆ • ) as a hypersurface by summing the monomials (A.10) all divisors which we have described above as Pic(X (∆,∆ • ) ) are sitting in the Picard lattice, including the non-toric ones, (A.14). Furthermore there are |Pic tor (X (∆ • ,∆) )| polynomial deformations which preserve these divisors. 19 As soon as we consider non-polynomial deformations, cycles which are in Pic(X (∆,∆ • ) ) but not in Pic tor (X (∆,∆ • ) ) cease to be purely of Hodge type (1, 1) so that they are no longer in the Picard lattice and the corresponding family is lattice polarized with polarizing lattice Pic tor (X (∆,∆ • ) ) instead of Pic(X (∆,∆ • ) ). Given a pair of reflexive polytopes, we hence have to make a choice as to how to 'distribute' the correction term [1] ) between N and N . The easiest choice is the one described in (A. 18), which is what we adopt in the present work. In general, there are other choices if Θ •[1] * (Θ • [1] ) * (Θ [1] ) > 0. Due to this subtlety, a pair of reflexive 3-dimensional polytopes generally gives rise to several mirror pairs of families of lattice polarized K3 surfaces.

B Toric Calabi-Yau hypersurfaces and toric stratification
As an application in a more familiar setting, we use the technique of stratification employed for building blocks in section 2.4 to compute the Hodge numbers of toric Calabi-Yau manifolds in this appendix. In this case, the M lattice polytope ∆ is reflexive, i.e. there is a lattice polytope ∆ • such that ∆, ∆ • ≥ −1 , (B.1) and the normal fan Σ n (∆) is identical to the fan over the faces of ∆ • , Σ f (∆ • ) [13]. In this correspondence we may identify for a dual pair of faces satisfying

B.1 Hodge numbers of toric Calabi-Yau hypersurfaces
To compute the Hodge numbers of Calabi-Yau threefold hypersurfaces, let us first note that they enjoy a stratification + pt 2-simplices on Θ • [2] ] (B.4) after we have resolved the variety P Σn(∆) using all lattice points on ∆ • . Here we have used that due to (B.2), the location of cones of Σ within the normal fan Σ n (∆) is identical to the location of the corresponding simplex within faces of ∆ • . We may now simply compute h 1,1 (Z) = h 2,2 (Z) = e 2,2 (Z) by summing the numbers e 2,2 of the individual strata. In the expressions below, Θ •[k] of ∆ • is considered to be the dual to the face Θ [4−k−1] being summed over.

B.2 Topology of divisors
In this section we derive combinatorial formulas for the Hodge numbers h 0,i for toric divisors of Calabi-Yau threefolds. The Hodge numbers h 1,1 of toric divisors depend on the triangulation data and are captured by slightly more complicated expression, which can however also easily be obtained from the methods used.

(B.17)
We have h 2,0 (Y i ) = e 2,0 (Y i ) = 0 as no stratum contributes. Already for the highest stratum Z Θ [2] , we have to count interior points to 3-dimensional faces of Θ [2] , of which there are none.
Even though we have started with an elliptic K3 with two singularities of type E 8 , the same construction also works if we start to unfold the two E 8 singularities. E.g. we can deform the E 8 singularity at ξ 1 = 0 by simply adding terms of lower powers in ξ 1 to (C.2). This can be done systematically (i.e. we automatically find which polynomials we have to add) by considering tops which are smaller than the E 8 top. Going through the same steps performed above, this will propagate to (C.5), i.e. we can specify a dP 9 with a specific degenerate fibre using the corresponding top. Note that adding monomials which (partially) deform the E 8 singularity at ξ 2 = 0 do not change at all what happens for the dP 9 at λ 2 = 0 as all such terms come with positive powers of λ 2 . Again, the resulting families of dP 9 surfaces can be directly obtained from the tops by using the construction of section 2.2.

D Polytopes and torsion in H 3
In this section we record a list of reflexive polytopes for which the corresponding Calabi-Yau hypersurface has non-vanishing Tors(H 3 (X, Z)) and give some data on reflexive subpolytopes of codimension one, relevant to the discussion in section 2.5.

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Below, we have listed the 16 N-lattice polytopes ∆ • , taken from [38,39], for which the corresponding reflexive pair (∆, ∆ • ) gives rise to a Calabi-Yau hypersurface X (∆,∆ • ) such that π 1 (X (∆,∆ • ) ) = 0. According to [38], and consistent with mirror symmetry, the mirror Calabi-Yau manifolds X (∆ • ,∆) have non-vanishing torsion, Tors(H 3 (X (∆ • ,∆) , Z)) = 0. Hence Hom( Λ 2 N/(N ∧ N is non-vanishing only for these 16 cases. For a pair of projecting tops ♦ • , ♦ to define a threefold Z with non-vanishing torsion Tors(H 3 (Z, Z)), needs to be non-zero. As we can complete ♦ together with a copy of itself (reflected on F ) to a reflexive polytope for which (D.2) will be the same, it follows that only tops contained in the reflexive polyhedra ∆ • recorded below can lead to Tors(H 3 (Z, Z)). None of these contains any projecting top, so that we can conclude that Tors(H 3 (Z, Z)) = 0 for any Z satisfying the definition of section 2.5.