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Nonrational polytopes and fans in toric geometry

Fiammetta Battaglia  and  Elisa Prato
The authors were partially supported by the PRIN Project “Real and Complex Manifolds: Topology, Geometry and Holomorphic Dynamics” (MIUR, Italy) and by GNSAGA (INdAM, Italy).

Abstract. First, we examine the notion of nonrational convex polytope and nonrational fan in the context of toric geometry. We then discuss and interrelate some recent developments in the subject.

Keywords. toric variety, nonrational convex polytope, nonrational fan.

Mathematics Subject Classification: 14M25, 52B20, 53D20.

Introduction

Toric varieties are a beautiful class of geometric objects, at the intersection of convex geometry and combinatorics on one side, and of algebraic and symplectic geometry on the other.

The study and interest for toric varieties began in algebraic geometry with Demazure’s foundational paper [24]. Some of the classical references on the subject are the article by Danilov [21] and the books by Fulton [25] and Cox et al. [20]. From the symplectic perspective, the subject started with Delzant’s classification of symplectic toric manifolds [23], which is founded on the convexity theorem by Atiyah [1] and Guillemin–Sternberg [28]. Standard references for this viewpoint are the books by Audin [2], Guillemin [27] and Cannas de Silva [19].

The basic convex geometric objects that provide the starting point in classical toric geometry are rational convex polytopes and fans.

Our aim is to frame the notion of nonrational convex polytope and fan in the context of toric geometry. We give an historical account and then we describe, in the simplest possible way, how this notion has been recently interpreted by a number of authors who have dealt with the subject. The intent is to provide a unitary picture, a sort of dictionary, that makes it easier to move from one context to the other.

In Section 1, we recall the definitions of rational convex polytope and fan and view them in the toric geometric setting. We describe the fundamental starting convex data that are needed to extend toric geometry to the nonrational case. In Section 2, we describe a variant of the starting convex data. In Section 3, we illustrate the notions that were discussed in the previous sections with a number of examples. Finally, we dedicate Section 4 to the aforementioned dictionary.

1. What is a nonrational convex polytope/fan: the fundamental triple

A convex polytope Δ(n)\Delta\subset(\mathbb{R}^{n})^{*} is the convex hull of a finite number of points. Equivalently, it is the bounded intersection of finitely many closed half–spaces

Δ=j=1d{μ(n)|μ,Xjλj},\Delta=\bigcap_{j=1}^{d}\{\;\mu\in(\mathbb{R}^{n})^{*}\;|\;\langle\mu,X_{j}\rangle\geq\lambda_{j}\;\},

where X1,XdnX_{1},\ldots X_{d}\in\mathbb{R}^{n}, λ1,,λd\lambda_{1},\ldots,\lambda_{d}\in\mathbb{R} and dd can be chosen to be exactly the number of codimension 11 faces (facets) of Δ\Delta (see, for example, [54, Theorem 1.1]). We assume, for simplicity, that Δ\Delta has maximal dimension nn. Remark that each vector XjX_{j} is orthogonal to a facet of Δ\Delta and points towards its interior. We will be calling the vectors X1,XdX_{1},\ldots X_{d} normals for Δ\Delta. They are not unique, as each XjX_{j}, together with the corresponding λj\lambda_{j}, can be replaced by any positive scalar multiple.

Convex polytopes are studied in combinatorics, but are also of fundamental importance in symplectic and algebraic geometry. Think of the convexity theorem [1, 28] and of geometric quantization in symplectic geometry. Or think of toric geometry in both algebraic and symplectic geometry. It is a crucial fact that the convex polytopes that appear in these classical geometric settings are all rational. This means that they are always thought of together with a lattice. The precise definition of rational convex polytope goes as follows: a convex polytope Δ(n)\Delta\subset(\mathbb{R}^{n})^{*} is rational if there exists a lattice LnL\subset\mathbb{R}^{n} such that the normals can be taken in LL. Another crucial fact in toric geometry is that, for any rational convex polytope, there is a canonical choice of normals: each XjX_{j} is taken to be the shortest possible vector in LL, also known as primitive vector. Often, the primitive normals generate the lattice. We remark in passing that in symplectic toric geometry it is possible and interesting to consider also nonprimitive normals (see [38]).

In the last few decades, there has been a growing interest in understanding how to make sense of toric varieties when the polytope is no longer rational.

In 1999 [47, 48] the second author approached this question first by replacing the basic framework polytope–lattice–primitive normals, which was clearly no longer suitable, with something more general. Let us explain.

The initial idea consisted in replacing the primitive vectors with any choice of normals, and the lattice with the \mathbb{Z}–span of these normals. The latter is a notion that was already well–known and of fundamental importance in the theory of quasicrystals and in the related theory of aperiodic tilings; it is called a quasilattice [42]. By definition, a quasilattice in n\mathbb{R}^{n} is the \mathbb{Z}–span of a set of \mathbb{R}–spanning vectors; notice that a quasilattice is a lattice if, and only if, these vectors form a basis of n\mathbb{R}^{n}. Take, for example, the regular pentagon (see Figure 1). It can be easily verified that it is not a rational polytope.

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Figure 1. The regular pentagon

Consider the fifth roots of unity

Y0=(1,0)Y1=(cos2π5,sin2π5)Y2=(cos4π5,sin4π5)Y3=(cos6π5,sin6π5)Y4=(cos8π5,sin8π5).\begin{array}[]{l}Y_{0}=(1,0)\\ Y_{1}=(\cos{\frac{2\pi}{5}},\sin{\frac{2\pi}{5}})\\ Y_{2}=(\cos{\frac{4\pi}{5}},\sin{\frac{4\pi}{5}})\\ Y_{3}=(\cos{\frac{6\pi}{5}},\sin{\frac{6\pi}{5}})\\ Y_{4}=(\cos{\frac{8\pi}{5}},\sin{\frac{8\pi}{5}}).\end{array}

Their opposites are normals for the pentagon (see Figure 2).

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Figure 2. The regular pentagon and the fifth roots of unity

The \mathbb{Z}–span of these vectors is a quasilattice, Q5Q_{5}, that is dense in 2\mathbb{R}^{2}. We remark that this particular quasilattice underlies the study of two aperiodic tilings of the plane discovered by Penrose: the rhombus tiling and the kite and dart tiling (see Section 3).

Now, two important remarks. First of all, the quasilattice generated by the chosen set of normals can be replaced by any other quasilattice that contains those normals. Take, for example, the polytope [0,1][0,1]\subset\mathbb{R}^{*}. It is rational with respect to the lattice \mathbb{Z}\subset\mathbb{R}, but also with respect to any lattice aa\mathbb{Z}, aa\in\mathbb{R} (naturally isomorphic to \mathbb{Z}). However, we may also consider any quasilattice Q=+aQ=\mathbb{Z}+a\mathbb{Z}, with aa irrational. Notice that this allows to consider rational convex polytopes in a nonrational setting. This turns out to be a natural choice in certain applications, some of which are described in Subsection 3.2. It also allows to perform symplectic cutting in an arbitrary direction [10].

Secondly, one can consider any other set of normals, provided they are contained in the quasilattice, allowing even more freedom.

This taken into account, it became convenient to define the following notion: given a quasilattice QQ, a convex polytope is said to be quasirational with respect to QQ if the normals can be chosen in QQ. Clearly, a convex polytope is quasirational with respect to a lattice if, and only if, it is rational.

Remark 1.1.

Notice that, unlike rationality, quasirationality is not at all a restrictive requirement. In fact, a convex polytope is always quasirational with respect to the quasilattice that is generated by any set of normals. Think of the regular pentagon: it is not rational, however, it is quasirational with respect to the quasilattice Q5Q_{5}.

We are now ready to recall the notion of fundamental triple; it is the triple given by

(Δ,Q,{X1,,Xd}),(\Delta,Q,\{X_{1},\ldots,X_{d}\}),

where Δ(n)\Delta\subset(\mathbb{R}^{n})^{*} is any convex polytope, QnQ\subset\mathbb{R}^{n} is any quasilattice with respect to which Δ\Delta is quasirational, and {X1,,Xd}\{X_{1},\ldots,X_{d}\} is a choice of normals for Δ\Delta in QQ. We remark that it is not required that {X1,,Xd}\{X_{1},\ldots,X_{d}\} span the quasilattice. The fundamental triple effectively replaces the polytope–lattice–primitive normals triple of the rational case. Once the triple is fixed, one can extend the classical geometric procedures for constructing toric varieties from polytopes. For convex polytopes that are simple, that is, when each vertex is the intersection of exactly nn facets, one gets a significant class of quasifolds.

Quasifolds are highly singular spaces that are locally the quotient of a manifold modulo the action of a countable group. If the countable groups are all finite we get orbifolds, if they are all trivial we get manifolds. As it happens for manifolds, even for quasifolds the local models are required to be mutually compatible and thus form an atlas. Quasifolds are naturally endowed with the usual geometric objects such as vector fields, differental forms and in particular symplectic structures. For the formal definition of quasifold and related notions, in the real and complex setting, we refer the reader to [47, 48, 7, 5].

Going back to nonrational toric geometry, the real and complex tori n/L\mathbb{R}^{n}/L and n/L\mathbb{C}^{n}/L of the rational case are naturally replaced by the quotients n/Q\mathbb{R}^{n}/Q and n/Q\mathbb{C}^{n}/Q, which are abelian groups and quasifolds that are referred to as quasitori [47, 48, 5]. We are now ready to recall the following basic results. Let Δ\Delta be a simple convex polytope. From [48, Theorem 3.3] we have

Theorem 1.2.

For each fundamental triple (Δ,Q,{X1,,Xd})(\Delta,Q,\{X_{1},\ldots,X_{d}\}), there exists a compact, connected 2n2n–dimensional quasifold MM, endowed with a symplectic structure and an effective Hamiltonian action of the quasitorus n/Q\mathbb{R}^{n}/Q such that, if Φ:M(n)\Phi\,\colon M\rightarrow(\mathbb{R}^{n})^{*} is the corresponding moment mapping, then Φ(M)=Δ\Phi(M)=\Delta.

Moreover, from [5, Theorem 2.2]

Theorem 1.3.

For each fundamental triple (Δ,Q,{X1,,Xd})(\Delta,Q,\{X_{1},\ldots,X_{d}\}), there exists a compact, connected, nn–dimensional complex quasifold XX, endowed with a holomorphic action of the complex quasitorus n/Q\mathbb{C}^{n}/Q having a dense open orbit.

Finally, from [5, Theorem 3.2]

Theorem 1.4.

For each fundamental triple (Δ,Q,{X1,,Xd})(\Delta,Q,\{X_{1},\ldots,X_{d}\}), the symplectic quasifold MM of Theorem 1.2 is equivariantly diffeomorphic to the complex quasifold XX of Theorem 1.3. The symplectic and complex structures are compatible and hence define a Kähler structure on MXM\simeq X.

The space MXM\simeq X is known as the toric quasifold associated with the triple (Δ,Q,{X1,,Xd})(\Delta,Q,\{X_{1},\ldots,X_{d}\}). As in the rational case, it is explicitly constructed by means of symplectic and complex quotients. In the proofs of Theorems 1.3 and 1.4 one sees that it is endowed with two beautiful finite atlases that generalize the standard complex affine and symplectic toric atlases of the rational case; their charts are modeled on n2n\mathbb{C}^{n}\simeq\mathbb{R}^{2n} modulo the action of countable subgroups of the standard torus n/n\mathbb{R}^{n}/\mathbb{Z}^{n}.

The case of general convex polytopes was addressed by the first author, who showed that the resulting space MM, which is naturally even more singular, is stratified by toric quasifolds [3, 4].

We remark that, unlike what happens in the rational setting, usually we do not have canonical choices for quasilattices and normals. Sometimes, however, the general geometric setup suggests natural choices. Some instances are described in Section 3. This is also the case when performing symplectic reduction and symplectic cutting in the nonrational toric setting [10, 11].

The notion of rational convex polytope can be naturally expressed in terms of the rationality of its normal fan. The same applies also to quasirationality. Let us first recall the definition of fan, which is the central convex object in the theory of toric varieties in algebraic geometry. A fan Σ\Sigma in n\mathbb{R}^{n} is a collection of cones such that each nonempty face of a cone in Σ\Sigma is itself a cone in Σ\Sigma and such that the intersection of any two cones in Σ\Sigma is a face of each [54]. The one–dimensional cones are said to be the generating rays of the fan. The normal fan ΣΔ\Sigma_{\Delta} of the convex polytope Δ\Delta is the fan whose generating rays are inward pointing and orthogonal to the polytope facets and such that there is an inclusion–reversing bijection between cones in ΣΔ\Sigma_{\Delta} and faces of Δ\Delta. It is a complete fan, namely the union of its cones is n\mathbb{R}^{n}.

Refer to caption
Figure 3. The normal fan of the regular pentagon

Moreover, a fan is said to be simplicial if each of its cones is simplicial, namely spanned by linearly independent vectors. Notice that a convex polytope is simple if, and only if, its normal fan is simplicial. The rationality/quasirationality of the polytope corresponds to the rationality/quasirationality of its normal fan. We recall, in fact, that a fan in n\mathbb{R}^{n} is said to be rational if there exists a lattice LnL\subset\mathbb{R}^{n} which has non–empty intersection with each generating ray. Similarly, we say that a fan in n\mathbb{R}^{n} is quasirational with respect to a quasilattice QnQ\subset\mathbb{R}^{n} if QQ has non–empty intersection with each generating ray.

For any fan Σ\Sigma, we can still introduce the triple

(Σ,Q,{X1,,Xd}),(\Sigma,Q,\{X_{1},\ldots,X_{d}\}),

where QnQ\subset\mathbb{R}^{n} is any quasilattice with respect to which Σ\Sigma is quasirational and where the vectors {X1,,Xd}\{X_{1},\ldots,X_{d}\} are generators of the fan rays in the quasilattice QQ. When the fan is complete and simplicial the complex construction of Theorem 1.3 applies verbatim. When, in addition, the fan is polytopal, namely when Σ\Sigma is the normal fan ΣΔ\Sigma_{\Delta} of a convex polytope Δ\Delta, the choice of such a Δ\Delta endows MM with the symplectic, and hence Kähler, structures of Theorems 1.2 and 1.4. We can draw the following commutative diagram

(Δ,Q,{X1,,Xd})\textstyle{(\Delta,Q,\{X_{1},\ldots,X_{d}\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(ΣΔ,Q,{X1,,Xd})\textstyle{(\Sigma_{\Delta},Q,\{X_{1},\ldots,X_{d}\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}M.\textstyle{M.}

2. The fundamental triple encoded in a triangulated vector configuration: the augmented triple

As we have seen, toric quasifolds are constructed explicitly and share key features with their rational counterparts. However, they are highly singular topological spaces. It is therefore natural to ask if there exists a framework that allows to work with smooth objects. With this motivation in mind, the first author, jointly with Zaffran [13], introduced in 2011 the idea of viewing toric quasifolds as leaf spaces of compact, complex, holomorphically foliated manifolds. This development was built on, and inspired by, two previous articles: the above–mentioned article by the second author on nonrational toric geometry [48], and the article [44] by Meerssemann–Verjovsky. In the latter, simplicial projective toric varieties were already viewed, in the classical rational setting, as leaf spaces of LVM manifolds, a large class of compact, complex, non–Kähler manifolds [41, 43], admitting a holomorphic foliation [40, 43]. The viewpoint developed in [13] naturally brought a new perspective on the convex geometric data as well: the fundamental triple was encoded in a triangulated vector configuration, a well known and studied convex object [22]. Let us recall from [13, Section 2] what a triangulated vector configuration is, how a triple is encoded there and, finally, why this convex datum is instrumental in the construction of LVMB manifolds – a generalization of LVM manifolds [16].

An odd, balanced, triangulated vector configuration is given by a pair (V,𝒯)(V,\mathcal{T}), where V=(X1,,Xp)V=(X_{1},\ldots,X_{p}) is an ordered list of vectors in n\mathbb{R}^{n}, allowing repetitions, that is balanced, namely i=1pXi=0\sum_{i=1}^{p}X_{i}=0, and odd, namely pn=2m+1p-n=2m+1. A subset τ\tau of {1,,p}\{1,\ldots,p\} is a simplex when the vectors indexed by τ\tau are linearly independent. The cone generated by these vectors is called cone(τ)\text{cone}(\tau). A triangulation 𝒯\mathcal{T} of a configuration VV is a collection of simplices satisfying the following conditions:

  1. (1)

    If τ𝒯\tau\in\mathcal{T} and ττ\tau^{\prime}\subset\tau then τ𝒯\tau^{\prime}\in\mathcal{T}

  2. (2)

    For all τ,τ𝒯\tau,\tau^{\prime}\in\mathcal{T}, cone(τ)cone(τ)=cone(ττ)\text{cone}(\tau)\cap\text{cone}(\tau^{\prime})=\text{cone}(\tau\cap\tau^{\prime})

  3. (3)

    τ𝒯cone(τ)cone(V)\cup_{\tau\in\mathcal{T}}\ \text{cone}(\tau)\supset\text{cone}(V).

Remark that (V,𝒯)(V,\mathcal{T}) encodes

  • a simplicial fan, not necessarily polytopal: the union of the cones indexed by 𝒯\mathcal{T}

  • ray generators (the vectors indexed by 𝒯\mathcal{T})

  • a quasilattice Q=Span(X1,,Xp)Q=\text{Span}_{\mathbb{Z}}(X_{1},\dots,X_{p})

  • a number of ghost vectors (those which are not indexed by 𝒯\mathcal{T}).

Viceversa, let Σ\Sigma be a simplicial fan. We can construct a triangulated vector configuration (V,𝒯)(V,\mathcal{T}) that encodes a given triple (Σ,Q,{X1,,Xd})(\Sigma,Q,\{X_{1},\ldots,X_{d}\}) as follows: if Span{X1,,Xd}=Q\text{Span}_{\mathbb{Z}}\{X_{1},\ldots,X_{d}\}=Q and the vector configuration (X1,,Xd)(X_{1},\ldots,X_{d}) is odd and balanced, we keep it as it is, otherwise we can add ghost vectors, so as to have a set of generators of the quasilattice QQ and a balanced, odd configuration. Notice that there are infinitely many choices of ghost vectors that comply with these conditions. We remark that, in the rational case, this procedure of adding vectors so as to have a set of generators of the lattice and a balanced, odd configuration, is already used in [44], where additional vectors correspond to indispensable points. The fan is complete if, and only if, the vectors in VV span n\mathbb{R}^{n}. In conclusion, the vector configuration VV takes care of the quasilattice and the vectors in the triple, while 𝒯\mathcal{T} is determined by the fan combinatorics.

In short, we consider the augmented triple

(V,𝒯)=triple+ghost vectors,(V,\mathcal{T})=\text{triple}+\text{ghost vectors},

where we have chosen a set of generators for the quasilattice QQ that includes a set of ray generators. The technical conditions, for the vector configuration to be balanced and odd are not at all restrictive. They allow to obtain, from a pair (V,𝒯)(V,\mathcal{T}), the exact convex datum that produces an LVMB manifold. More precisely, Gale duality applied to VV gives a configuration Λ=(Λ1,,Λp)\Lambda=(\Lambda_{1},\ldots,\Lambda_{p}) of points in affine space m\mathbb{C}^{m} (viceversa, Gale duality applied to Λ\Lambda determines VV up to automorphisms [14, Section 1.2]). On the other hand, the combinatorial datum 𝒯\mathcal{T} yields a combinatorial datum 𝒯\mathcal{T}^{*}, which is a virtual chamber of Λ\Lambda. In turn, each pair (Λ,𝒯)(\Lambda,\mathcal{T}^{*}) determines a compact, complex, holomorphically foliated manifold (N,)(N,\mathcal{F}), of complex dimension n+mn+m, where mm is the dimension of the leaves [13, Section 2.2.4]. We can draw the following diagram:

(1) (V,𝒯)\textstyle{(V,\mathcal{T})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(Λ,𝒯)\textstyle{(\Lambda,\mathcal{T}^{*})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(N,)\textstyle{(N,\mathcal{F})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(Σ,Q,{X1,,Xd})\textstyle{(\Sigma,Q,\{X_{1},\ldots,X_{d}\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}M\textstyle{M}

Two arrows are dashed as they are not maps, in the sense that the target object is not uniquely determined. This implies that, to a given fundamental triple there corresponds a whole family of LVMB manifolds of different dimensions. When the fan is polytopal, NN is an LVM manifold and the leaf space of each member of this family is exactly the corresponding complex toric quasifold MM (see [13, Section 2.3.1] and [14, Theorem 2.1]). Polytopality of the fan Σ\Sigma can be expressed in terms of the above–mentioned convex objects (for more details see [13] and references therein). In terms of the corresponding LVM manifold, polytopality implies that the foliation is transversely Kähler [40, 43]. The converse is also true; the proof, by Ishida [32], is based on a convexity theorem in this context. In the polytopal case, diagram (1) can be constructed in the symplectic setting: NN turns out to be a presymplectic manifold, while the symplectic quasifold MM is given by NN modulo the action of a connected abelian group [14]. Taking the augmented triple ensures that the presymplectic manifold NN is even dimensional and that the group is connected.

Subsequently, other important convexity theorems were proved, for transversely symplectic foliations [51, 39] and for étale symplectic stacks [30].

3. Examples

As far as examples go, two situations arise naturally. In the first, we have examples of convex polytopes/fans that are nonrational. In the second, we have rational convex polytopes/fans inside of a geometric context where it is interesting, and sometimes downright necessary, to replace the lattice by a suitable quasilattice.

3.1. Purely nonrational

The first example that comes to mind of a purely nonrational convex polytope is the regular pentagon that we discussed in Section 1. An even simpler example is given by the Penrose kite, which, together with the dart, has been used by Penrose to construct aperiodic tilings of the plane [45]. The kite is the quadrilateral pictured in Figure 4. Three of its angles equal 2π5\frac{2\pi}{5}, while the other equals 4π5\frac{4\pi}{5}. Moreover, its long edge is ϕ\phi times its short edge, where ϕ=1+52\phi=\frac{1+\sqrt{5}}{2} is the golden ratio.

Refer to caption
Figure 4. The Penrose kite

The regular pentagon and the Penrose kite are actually closely related; in fact, the kite can be obtained from the regular pentagon via a standard construction (see, for example, [7]). Moreover, the kite is quasirational with respect to the same quasilattice Q5Q_{5} that we introduced for the pentagon.

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Figure 5. Quasirationality of the Penrose kite

In fact, a natural choice of normals for the kite is given by Y1-Y_{1}, Y2Y_{2}, Y3-Y_{3}, Y4Y_{4} (see Figure 5). These vectors generate the four rays of the corresponding normal fan. A vector configuration here is given by V=(Y1,Y2,Y3,Y4,Y0)V=(-Y_{1},Y_{2},-Y_{3},Y_{4},Y_{0}); it is odd and balanced, with triangulation, in term of maximal simplices, given by 𝒯={{1,4},{4,3},{3,2},{2,1}}\mathcal{T}=\{\{1,4\},\{4,3\},\{3,2\},\{2,1\}\}.

More details on the Penrose kite from the symplectic toric viewpoint can be found in [7].

Other interesting and elementary examples of nonrational convex polytopes are given by the regular dodecahedron and the regular icosahedron, only the first of which is simple. We refer the reader to [49, 9] for a suitable choice of quasilattice and normals and for a description of the corresponding toric spaces.

All of the above are closely related to the physics of quasicrystals, see for example [8, 52].

We conclude by remarking that any simple nonrational convex polytope can be perturbed into a combinatorially equivalent rational one. This is not necessarily the case for nonsimple convex polytopes. See [26, 55] for the first counterexample, due to Perles.

3.2. Rational convex polytope in a nonrational setting

We have already seen in Section 1 how the unit interval [0,1][0,1], obviously rational, can be viewed as quasirational. The corresponding toric quasifold is a quasisphere [47, 48, 50].

We illustrate two other examples where this is natural.

Let us consider first the Penrose rhombus tiling [45]. It is another fundamental aperiodic tiling, whose tiles are given by two types of rhombuses, known as thick and thin. The thick rhombus has angles equal to 2π5\frac{2\pi}{5} and 3π5\frac{3\pi}{5}, and the long diagonal is given by ϕ\phi times the edge; the thin rhombus has angles equal to π5\frac{\pi}{5} and 4π5\frac{4\pi}{5}, and the edge is given by ϕ\phi times the short diagonal (see Figure 6).

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Figure 6. The thick and thin Penrose rhombuses

Each of them viewed individually is actually a rational convex polytope, but it is natural to want to consider a geometric setup that takes into account the entire tiling. In order to do so, they need to be viewed as quasirational with respect to the same quasilattice Q5Q_{5} that we have considered for the pentagon and the kite. In Figure 7 we see normals ±Y0\pm Y_{0}, ±Y4\pm Y_{4} for the thick rhombus and ±Y1\pm Y_{1}, ±Y4\pm Y_{4} for the thin one.

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Figure 7. Quasirationality of the Penrose rhombuses

To obtain vector configurations here we need to consider more vectors than we did in the case of the kite. For example, for the thick rhombus, we can take V=(Y0,Y4,Y0,Y4,Y1,Y2,Y3+Y4+Y0)V=(Y_{0},Y_{4},-Y_{0},-Y_{4},Y_{1},Y_{2},Y_{3}+Y_{4}+Y_{0}); it is odd and balanced, with same triangulation as the kite. We refer the reader to [6] for further details on rhombus tilings from the symplectic viewpoint.

Other interesting examples arise when generalizing Hirzebruch surfaces to the nonrational setting. Namely, consider, for any positive real number aa, the trapezoid TaT_{a} of vertices (0,0)(0,0), (1,0)(1,0), (0,1)(0,1) and (a+1,1)(a+1,1) (see Figure 8).

Refer to caption
Figure 8. The trapezoid TaT_{a}

When aa equals a positive integer nn, we get the trapezoid TnT_{n} that corresponds, in standard toric geometry, to the Hirzebruch surface n\mathbb{H}^{n}. We recall that this toric variety is constructed relatively to the standard lattice 2\mathbb{Z}^{2} and to the primitive normals (1,0)(1,0), ±(0,1)\pm(0,1), (1,n)(-1,n). For aa irrational, the trapezoid TaT_{a}, though rational with respect to the lattice that is generated by (1,0)(1,0) and (0,a)(0,a), is not rational with respect to the standard lattice 2\mathbb{Z}^{2}. If we want to consider a setup that yields, as a special case, the standard one for Hirzebruch surfaces, it is necessary to consider normals (1,0)(1,0), ±(0,1)\pm(0,1), (1,a)(-1,a) (see Figure 9),

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Figure 9. Quasirationality of the trapezoid TaT_{a}

which span the quasilattice Qa=×(+a)2Q_{a}=\mathbb{Z}\times(\mathbb{Z}+a\mathbb{Z})\supseteq\mathbb{Z}^{2}. Notice that, for aa rational, QaQ_{a} is a lattice and that, for a=na=n, this lattice equals 2\mathbb{Z}^{2}, as required.

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Figure 10. The normal fan of the trapezoid TaT_{a}

The normal fan here is the complete fan in 2\mathbb{R}^{2} whose generating rays are spanned by the four normals (1,0)(1,0), ±(0,1)\pm(0,1) and (1,a)(-1,a) (see Figure 10). A corresponding triangulated vector configuration is given by (Va,𝒯)(V_{a},\mathcal{T}), with

Va=((1,0),(0,1),(0,1),(1,a),(0,a)),V_{a}=((1,0),(0,1),(0,-1),(-1,a),(0,-a)),
𝒯={{1,2},{2,4},{3,4},{1,3},{1},{2},{3},{4},}.\mathcal{T}=\{\{1,2\},\{2,4\},\{3,4\},\{1,3\},\{1\},\{2\},\{3\},\{4\},\varnothing\}.

We refer the reader to [12] for more details, including a description of the one–parameter family of generalized Hirzebruch surfaces corresponding to the fundamental triple

(Ta,Qa,{(1,0),±(0,1),(1,a)}).(T_{a},Q_{a},\{(1,0),\pm(0,1),(-1,a)\}).

4. A dictionary

In recent years, there have been a number of articles on nonrational toric geometry from different viewpoints and new results have been obtained. A common factor of all of these works is of course the presentation of starting convex geometric data. A shared feature of these different approaches is the datum of the fundamental triple. Sometimes, further data are added that are instrumental for the constructions; we have already seen an instance of this in Section 2, where the additional data are the ghost vectors. Some viewpoints also consider a variant of the notion of quasitorus.

Toric quasifolds can be thought of as stacks, and some authors study nonrational toric geometry within this framework. The first are Hoffman–Sjaamar in the symplectic category [30, Examples 7.4.3, 9.2.5 and Remark 7.4.4]. In their work, a quasilattice is a crossed Lie module :QV\partial\colon Q\rightarrow V, where QQ is a finitely generated abelian group and VV is a real vector space spanned by (Q)\partial(Q). Therefore, the quasilattice QQ is no longer a subgroup of VV, but is surjectively mapped onto one, namely (Q)\partial(Q). In this way, there are infinitely many :QV\partial\colon Q\rightarrow V that project onto the same pair ((Q),V)(\partial(Q),V). Notice that the quasilattice QQ contains more information than (Q)\partial(Q); this is, in this setting, the extra datum that we were referring to earlier. Remark also that the pair ((Q),V)(\partial(Q),V) gives rise to the quasitorus V/(Q)V/\partial(Q). Here the group that generalizes the torus is called stacky torus. The definition is quite involved; for our purposes it is sufficient to recall that the datum of a stacky torus GG is equivalent to their notion of quasilattice. In [29, Section 5] Hoffman introduces the starting triple (Δ,G,ΛfFmax)(\Delta,G,\Lambda_{f\in F^{max}}), where Δ\Delta is a simple convex polytope, GG is a stacky torus, FmaxF^{max} is the set of facets of Δ\Delta and Λf{\Lambda_{f}} is a free subgroup of rank 11, given by the intersection of (Q)\partial(Q) with the straight line normal to the facet ff. Notice that there is a unique inward pointing vector that generates Λf{\Lambda_{f}}. This corresponds to the vector, in the fundamental triple, that is associated with the facet ff. We can draw the following diagram

(Δ,Q,{X1,,Xd})\textstyle{(\Delta,Q,\{X_{1},\ldots,X_{d}\})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}(Δ,G,ΛfFmax),\textstyle{(\Delta,G,\Lambda_{f\in F^{max}}),\ignorespaces\ignorespaces\ignorespaces\ignorespaces}

where Λf{\Lambda_{f}} is generated by the normal XiX_{i} in the corresponding ray and GG is any :Q~V\partial\colon\widetilde{Q}\rightarrow V with (Q~)=Q\partial(\widetilde{Q})=Q. The arrows have the same meaning as in diagram (1): given a fundamental triple, there are infinitely many triples of the kind (Δ,G,ΛfFmax)(\Delta,G,\Lambda_{f\in F^{max}}) that project onto it. Viceversa, any triple (Δ,G,ΛfFmax)(\Delta,G,\Lambda_{f\in F^{max}}) uniquely determines a fundamental triple. Now, let us recall the following observation in [29]: assigning the triple (Δ,G,ΛfFmax)(\Delta,G,\Lambda_{f\in F^{max}}) is equivalent to assigning the triple (Δ,G,ΛfF)(\Delta,G,\Lambda_{f\in F}), where FF is the set of all faces of Δ\Delta and the groups Λf\Lambda_{f} are subgroups of (Q~)\partial(\widetilde{Q}) satisfying certain conditions. The triple (Δ,G,ΛfF)(\Delta,G,\Lambda_{f\in F}) is said to be a decorated stacky moment polytope, for which a natural notion of isomorphism is given. The author defines per se symplectic toric stacks and then proves that the moment mapping defines a bijective correspondence between the set of isomorphism classes of decorated stacky moment polytopes and the set of equivalence classes of symplectic toric stacks [29, Theorem 6.1]. In our understanding, each equivalence class of symplectic toric stacks corresponds to the symplectic toric quasifold constructed from the associated fundamental triple.

Another article that addresses the problem of generalized toric manifolds is that by Ishida–Krutowsky–Panov [34]. Their focus is on cohomology. In [34, Definition 5.5] they introduce the quadruple (V~,Γ~,Σ~,λ~)(\widetilde{V},\widetilde{\Gamma},\widetilde{\Sigma},\widetilde{\lambda}), which they call marked fan, where V~\widetilde{V} is a finite–dimensional real vector space, Γ~\widetilde{\Gamma} is a quasilattice in V~\widetilde{V}, Σ~\widetilde{\Sigma} is a fan that is quasirational with respect to Γ~\widetilde{\Gamma} and is additionally assumed to be complete and simplicial. Finally, λ~\widetilde{\lambda} is a function on the set of one–dimensional cones of Σ~\widetilde{\Sigma}, with values in the quasilattice Γ~\widetilde{\Gamma}, such that λ~(ρ)\widetilde{\lambda}(\rho) is a generator of ρ\rho. Therefore, λ~\widetilde{\lambda} corresponds exactly to a set of ray generators in the fundamental triple. The authors then consider compact, connected, complex manifolds with maximal torus actions. These were defined by Ishida in [33] and later endowed with a canonical foliation in [32]. In this class of manifolds, the authors define an equivalence relation called principal equivalence. Then they prove, building on [33], that the set of equivalence classes is in bijective correspondence with isomorphism classes of marked fans [34, Theorem 5.7]. Using this and moment angle manifolds, they are able to drop the hypothesis of shellability in the result by Battaglia–Zaffran [13] on the basic cohomology ring of complete simplicial shellable fans. Further results on the cohomology of complete simplicial fans can be found in the recent paper by Krutowsky–Panov [37]. For the connection between moment angle manifolds and complex manifolds with maximal torus action see also [53]. As recalled in Section 2, by the construction in [13], we are able to associate with a given fundamental triple a family of LVMB manifolds. Each of these is endowed with a maximal torus action and, therefore, belongs to the equivalence class, defined in [34], corresponding to the given fundamental triple. We know that the leaf space of each of these LVMB manifolds is isomorphic to the complex toric quasifold corresponding to the fundamental triple. We expect that the leaf space of each complex manifold with maximal torus action in the equivalence class is isomorphic to that complex toric quasifold.

The problem of generalized toric manifolds is again addressed in the framework of stacks in a recent article by Lupercio–Meersseman–Verjovsky–Katzarkov [36]. As starting convex data, they consider quantum fans and calibrated quantum fans [36, Section 4], which correspond to fundamental triples and augmented triples, respectively. More specifically, a quantum fan in a quasilattice Γn\Gamma\subset\mathbb{R}^{n} (which they have renamed quantum lattice) is a pair (Δ,v)(\Delta,v), where Δ\Delta is a fan quasirational with respect to Γ\Gamma and vv is a set of rays generators contained in Γ\Gamma, one for each 11–dimensional cone of Δ\Delta. On the other hand, a calibrated quantum fan is a quantum fan plus the additional datum of a calibration. Denote by {e1,,ep}\{e_{1},\ldots,e_{p}\} the standard basis of p\mathbb{Z}^{p}. Then a calibration is an epimorphism h:pΓh\colon\mathbb{Z}^{p}\longrightarrow\Gamma together with a subset JJ of {1,,p}\{1,\ldots,p\}, with the following property: the vectors h(ei)h(e_{i}), with iJi\notin J, generate n\mathbb{R}^{n} and give the set vv of dd rays generators, while the vectors h(ei)h(e_{i}), with iJi\in J, are the ghost vectors described in Section 2. The complex quasitorus n/Γ\mathbb{C}^{n}/\Gamma is viewed as a quotient stack and called quantum torus. In correspondence to a complete (calibrated) simplicial quantum fan and to the relative quasilattice Γ\Gamma, the authors construct a (calibrated) quantum toric variety. The (calibrated) quantum toric variety is built by suitably gluing the (calibrated) quantum affine toric stacks associated with the maximal cones. From the viewpoint of complex toric quasifolds, this is the affine atlas introduced in [5, Theorem 2.2]. They define a notion of morphism for (calibrated) quantum fans and (calibrated) quantum toric varieties. The map between these two categories given by the construction turns out to be functorial, it is naturally surjective, and is proved to be an equivalence of categories [36, Theorems 5.18, 6.24].

Finally, Boivin extends the above equivalence of categories to calibrated nonsimplicial fans and the corresponding calibrated quantum toric varieties [15, Theorem 4.2.2.2]. He makes use of the same starting convex data, that he calls (calibrated) quantum fans and quantum lattices as well. But he needs to introduce an auxiliary datum, a further calibration, in order to deal with nonsimpliciality.

The following diagram gives a synthetic and unified picture of the various constructions:

triple + additional data Ψ\scriptstyle{\quad\overset{\approx}{\Psi}}
geometric space
fundamental triple Ψ\scriptstyle{\quad\Psi}Ψ~\scriptstyle{\quad\quad\widetilde{\Psi}} toric quasifold

The box on the left represent a whole family of data projecting down to the same fundamental triple, the box on the right represent the corresponding family of geometric spaces. The lower level is the mapping that associates the fundamental triple with the toric quasifold. Notice that we can always construct, from a given fundamental triple, an object that lies in the family above. The articles [13, 29] and, in the calibrated case, [36, 15] can be viewed as instances of the mapping Ψ\overset{\approx}{\Psi}, [34] can be viewed as an instance of the mapping Ψ~\widetilde{\Psi}, and finally [47, 48, 5], and [36, 15] can be viewed as instances of the mapping Ψ\Psi. In our understanding, in each of the above–mentioned constructions relative to the mappings Ψ\overset{\approx}{\Psi} and Ψ~\widetilde{\Psi}, there is a mapping that projects any space of the family to the toric quasifold. An instance is given in [14, Theorem 2.1].

We conclude by briefly mentioning a number of other related works. Ratiu–Zung [51] and Lin–Sjamaar [39] study nonrational convex polytopes in the context of presymplectic manifolds. The first authors specialize to the toric case, but a triple is not explicitly provided. Pir–Sottile [46] introduce the notion of irrational toric variety for arbitrary fans and show that, when the fan is the normal fan of a polytope, the irrational toric variety is homeomorphic to that polytope. Quasifolds have been studied in the framework of diffeology in [31]. We expect that this approach will have implications in nonrational toric geometry. Finally, we remark that Bressler–Lunts [17, 18] and Karu [35] devised a powerful approach to the combinatorics of nonrational polytopes that extends cohomological properties of toric varieties to general fans, without constructing a corresponding toric space.

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Dipartimento di Matematica e Informatica ”U. Dini”, Università di Firenze
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fiammetta.battaglia@unifi.it, elisa.prato@unifi.it