Computational Algebraic Geometry in String and Gauge TheoryView this Special Issue
Review Article | Open Access
Rhys Davies, "The Expanding Zoo of Calabi-Yau Threefolds", Advances in High Energy Physics, vol. 2011, Article ID 901898, 18 pages, 2011. https://doi.org/10.1155/2011/901898
The Expanding Zoo of Calabi-Yau Threefolds
This is a short review of recent constructions of new Calabi-Yau threefolds with small Hodge numbers and/or nontrivial fundamental group, which are of particular interest for model building in the context of heterotic string theory. The two main tools are topological transitions and taking quotients by actions of discrete groups. Both of these techniques can produce new manifolds from existing ones, and they have been used to bring many new specimens to the previously sparse corner of the Calabi-Yau zoo, where both Hodge numbers are small. Two new manifolds are also obtained here from hyperconifold transitions, including the first example with fundamental group , the smallest non-Abelian group.
This paper is a short review of recent work on constructing smooth Calabi-Yau threefolds with interesting topological properties, such as small cohomology groups and nontrivial fundamental group. In practice, these two properties often go hand-in-hand, as emphasised in [1, 2].
The majority of known three-dimensional Calabi-Yau manifolds are constructed as complete intersections in higher-dimensional toric varieties [3–8]. Most of the new examples found in recent years are in fact obtained from these via one of two techniques. The first is to take the quotient by a holomorphic action of some finite group. As explained in Section 2, when the group action is fixed-point-free, this is guaranteed to yield another Calabi-Yau manifold, and many Calabi-Yau threefolds with nontrivial fundamental group have been constructed in this way. Several early examples can be found in [9–14], but recent efforts have brought to light many more [2, 15–26], some of which will be discussed later. In the case that the group action has fixed points, it is often possible to resolve the resulting orbifold singularities in such a way as to again obtain a Calabi-Yau manifold. Examples can be found in [27–29]. The second technique is to vary either the complex structure or Kähler moduli of a known space until it becomes singular and then desingularise it by varying the other type of moduli. Topologically, such a process is a surgery and yields a Calabi-Yau manifold topologically distinct from the original. Two classes of such topological transitions, the conifold and hyperconifold transitions, are discussed in Section 3, and explicit examples of each are given. Conifold transitions have been known for some time to connect many Calabi-Yau threefolds [30–33] and have been used to construct new manifolds in [2, 24, 34, 35]. Hyperconifold transitions were described in , and the first examples of new manifolds discovered this way were given in . The examples of Section 3.2 yield two more new manifolds, one of which is the first known with fundamental group , the smallest non-Abelian group.
The fruit of these labours is that there are now many more known Calabi-Yau threefolds with small Hodge numbers (defined arbitrarily in this paper by ) than were known to the authors of . The number with nontrivial fundamental group has also increased dramatically, thanks largely to Braun's classification of free group actions on complete intersections in products of projective spaces . (The Hodge numbers of many of these quotients are yet to be calculated, but some are likely to be “small” as defined above.)
The physical motivation for studying such manifolds comes predominantly from heterotic string theory. In this context, a nontrivial fundamental group is necessary to be able to turn on discrete Wilson lines and thus obtain a realistic four-dimensional gauge group. The requirement of small Hodge numbers is not so clear-cut, but it seems advantageous if one wants to appeal to the methods of [38, 39] to stabilise the moduli, and this is currently the only known way to stabilise all (geometric) moduli in heterotic Calabi-Yau backgrounds. Although heterotic model building is not the theme of this review, other recent developments will be mentioned sporadically.
Throughout the paper, an arbitrary Calabi-Yau and its universal cover will be denoted by and , respectively, while a particular Calabi-Yau threefold with Hodge numbers will be denoted by . will denote a singular member of the family , and a resolution of such a singular variety.
2. Quotients by Group Actions
2.1. The Calabi-Yau Condition
It is an elementary fact of topology that every manifold has a simply connected universal covering space , from which it can be obtained as a quotient by the free action of a group . We will write this relationship as . Although our interest is in (complex) threefolds, we will allow the dimension of to be arbitrary through much of this section.
If is a Calabi-Yau manifold, it is easy to see that its universal cover is too, by pulling back the complex structure, Kähler form , and holomorphic -form under the covering map (for this reason, we will often abuse notation by using the same symbols for these objects on and ). Only a little more difficult is the converse: under what conditions is a Calabi-Yau manifold, given that is? There are several points to consider (we assume always that is a finite group). (i) will be a manifold as long as the action of is fixed-point free. Otherwise, it will have orbifold singularities. (ii)It will furthermore be a complex manifold if and only if acts by biholomorphic maps. In this case, simply inherits the complex structure of . (iii)To see that is Kähler, pick any Kähler form on . Now, note that for any element , is also a Kähler form, since , and for any -dimensional complex submanifold , We can use this to construct a Kähler form which is invariant under and, therefore, descends to a Kähler form on . (iv)Finally, we must check whether supports a nowhere-vanishing holomorphic -form. This can only descend from the one on , so we need to check whether is -invariant. Note that is the unique (up to scale) element of , so since acts freely, the Atiyah-Bott fixed point formula [40, 41] for any reduces to where denotes the induced action of on the cohomology . The group is generated by , which is invariant, so we conclude that , and therefore, In odd dimensions, therefore, is automatically invariant under free group actions. In even dimensions, on the other hand, this simple calculation shows that there are no multiply-connected Calabi-Yau manifolds.
In summary, if is a smooth Calabi-Yau threefold, then is a Calabi-Yau manifold if and only if acts freely and holomorphically.
Above, we have simply assumed that the covering space is smooth. In practice, usually belongs to a family of spaces of which only a subfamily admits a free action. It may be the case that although a generic member of is smooth, members of the symmetric sub-family are all singular, so we never get a smooth quotient. Although this seems to be rare, it does occur for -symmetric complete intersections of four quadrics in [11, 18], -symmetric complete intersections of five bilinears in , and a number of other examples, including some found in . The extra condition, that a generic symmetric member is smooth, must, therefore, be checked on a case-by-case basis.
Let us start with the special case of complete intersection Calabi-Yau manifolds in smooth ambient spaces. This includes what have traditionally been called the “CICY” manifolds, where the ambient space is a product of projective spaces [3–5] and certain of the toric hypersurfaces [7, 8]. The complete intersection condition means that if the ambient space has dimension , then the Calabi-Yau is given by the intersection of hypersurfaces, each given by a single polynomial equation . In other words, the number of equations needed to specify is equal to its codimension. When the ambient space is smooth, it can be covered in affine patches each isomorphic to , and the condition for to be smooth is that is nonzero at every point on . This is a very intuitive condition—if it holds, then at any point of we can choose local coordinates such that . Locally, then, projects biholomorphically onto the linear subspace , and is, therefore, smooth. On any affine coordinate patch, the components of the differential form are just the minors of the Jacobian matrix , so the condition is that this matrix has rank everywhere on . It is, therefore, necessary to check that there is no simultaneous solution to the equations along with the vanishing of all minors of , which is equivalent to the algebraic statement that the ideal generated by the polynomials and the minors is the entire ring . This is checked by calculating a Gröbner basis for the ideal, algorithms for which are implemented in a variety of computer algebra packages [42–44]; a Gröbner basis for the entire ring is just a constant (usually given as 1 or −1 by software).
The more general case of singular ambient spaces or noncomplete intersections is not much harder than the above. Suppose is not a complete intersection so that it is given by equations in an -dimensional ambient space, where now we allow . (A typical example is the Veronese embedding of in . If we take homogeneous coordinates for , and for , where , then the embedding is given by . The equations needed to specify the image of this map are , which amount to six independent equations, whereas the codimension of the embedded surface is only three.) Then, the condition for to be smooth is still that the rank of the Jacobian be equal to (the codimension) everywhere on . The reasoning is the same as before—if this is true, of the polynomials will provide good local coordinates on the ambient space, allowing us to define a smooth coordinate patch on .
If some affine patch on the ambient space is singular, it can still be embedded in for some , by polynomial equations . The Calabi-Yau is then given by , and the condition for smoothness is once again that the Jacobian has rank equal to the codimension, , at all points.
For examples of interest, Gröbner basis calculations are often very computationally intensive, since at intermediate stages the number of polynomials, as well as their coefficients, can become extremely large. It is, therefore, convenient to choose integer coefficients for all polynomials and perform the calculation over a finite field . As explained in , if a collection of polynomial equations are inconsistent over , then they are also inconsistent over , so the corresponding variety is smooth.
Note that there does exist a slight variation on the above procedure which still leads to smooth quotient manifolds. It may be the case that although the symmetric manifolds admit a free group action, they are all singular. If, however, these singularities can be resolved in a group-invariant way, the resolved space still admits a free group action, with a smooth quotient. Examples can be found in [15, 18, 21].
The final possibility is that the symmetric manifolds are smooth, but the group action always has fixed points, in which case the quotient space has orbifold singularities. It is frequently possible to resolve these in such a way as to again obtain a Calabi-Yau manifold, but this will not be discussed in detail here.
2.2. Notable Examples
2.2.1. New Three-Generation Manifolds
Calabi-Yau threefolds with Euler number were of particular interest in the early days of string phenomenology, since these give physical models with three generations of fermions via the “standard embedding” compactification of the heterotic string . This typically gives an grand unified theory, and although the gauge symmetry can be partially broken by Wilson lines, it is impossible to obtain exactly the standard model gauge group in this way . Nevertheless, it was argued by Witten that deformations of the standard embedding, combined with Wilson lines, can give realistic models , and this was put on firmer mathematical foundations by Li and Yau .
The archetypal example of a three-generation manifold is Yau's manifold, with fundamental group , but recently two new promising three-generation manifolds were constructed in . These are quotients of a manifold by groups of order twelve, which are the cyclic group and the non-Abelian group (this is generated by two elements, one of order three and one of order four, satisfying ), and each has Hodge numbers . Unfortunately, it was shown in  that the physical model on the non-Abelian quotient does not admit a deformation which yields exactly the field content of the minimal supersymmetric standard model (MSSM) in four dimensions. However, the quotient allows many more distinct deformations, and the analysis of the corresponding physical models has not been completed.
The covering space is an anticanonical hypersurface in , where is the del Pezzo surface of degree six, which is blown up in three generic points. This surface is rigid and toric, and its fan is shown in Figure 1.
As well as the action of the torus , also admits an action by the dihedral group , as suggested by its fan. This can be realised as a group of lattice morphisms preserving the fan, generated by an order-six rotation and a reflection , with matrix representations The product therefore has symmetry group , where the extra factor swaps the two copies of the surface. The quotient groups and are both order-twelve subgroups of this which act transitively on the vertices of the fan. Many more details can be found in .
2.2.2. Quotients of the (19, 19) Manifold
The Euler number of a three-dimensional Calabi-Yau manifold is given by the simple formula . If a group acts freely, then , so this gives a simple necessary condition for the existence of such an action: the order of the group must divide . This usually gives a fairly strong restriction on the groups which can act freely on any given manifold. The only time it gives no restriction is when . In this section, we will look at a particular manifold, , which admits free actions by a number of disparate groups, including groups of order five, eight, and nine. For a Calabi-Yau threefold with , this would imply .
The manifold can be represented in a number of different ways. Abstractly, it is the fibre product of two rational surfaces, each elliptically fibred over [16, 19]. Such a surface is given by blowing up at the nine points given by the intersection of two cubic curves; if we take homogeneous coordinates on and on , the corresponding equation is where and are homogeneous cubic polynomials. We can easily see that this corresponds to blown up at the nine points given by . Indeed, for any point of , where or , we get a unique solution for , whereas for , the equation is satisfied identically, giving a whole copy of . To see that it is also an elliptic fibration over , note that for any fixed value of , we get a cubic equation in , which defines an elliptic curve.
To get the fibre product of two such surfaces, we introduce another , with homogeneous coordinates , and another equation of the form (2.6) over the same . The resulting threefold is Calabi-Yau, and has a projection to , with typical fibre which is a product of two elliptic curves. In , Bouchard and Donagi studied group actions which preserve the elliptic fibration, and found free actions by the groups , , and (as well as all subgroups of these, of course).
Certain of these quotient manifolds have, in fact, played crucial roles in the heterotic string literature. A model with the spectrum of the -extended supersymmetric standard model was constructed on a quotient by and studied in [50, 51] (a similar model on the quotient of the “bicubic”, which is related to this manifold by a conifold transition, was found in ), while a model with the exact MSSM spectrum exists on a quotient and was described in [53, 54]. In [55, 56], the quotient by a different action was used as a test case for calculating instanton corrections on manifolds with torsion curves.
There are, in fact, further (relatively large) groups which act freely on , which can be easily described using its representation(s) as a CICY. First, we note that the fibre product construction above is equivalent to the rather more prosaic statement that the manifold is a complete intersection of two hypersurfaces in , of multi-degrees and . In the notation of [3, 4], can, therefore, be specified by the “configuration matrix” By utilising various splittings and contractions (see, e.g., [2, 4, 30, 31]), and checking that the Euler number remains constant, it is easy to show that can also be specified by the configuration matrices It was shown in  that in the first form, admits a free action of the order-eight quaternion group (denoted in  by , but more conventionally by ), with elements , induced by a linear action of this group on the ambient space.
In the second form, admits free actions by two groups of order twelve. One is the cyclic group , and the other is the dicyclic group (introduced in Section 2.2.1) . These were in fact discovered via conifold transitions from the corresponding quotients of , an idea reviewed in Section 3.
In summary, is rather exceptional in that it admits free actions by the groups , and . The Hodge numbers for the quotients by all these groups and their subgroups are collected in Table 1.
2.2.3. Manifolds with Hodge Numbers (1,1)
For a long time, the smallest known Hodge numbers of a Calabi-Yau threefold satisfied . This record has now been overtaken by Braun's examples of manifolds with  (as well as Freitag and Salvati Manni's manifold with ).
The covering space of Braun's manifolds is a self-mirror manifold . This is realised as an anticanonical hypersurface in the toric fourfold determined by the face fan over the 24-cell, which is a self-dual regular four-dimensional polytope.
There are three different groups of order 24 which act freely on particular smooth one-parameter subfamilies of ; these are , and . The first two are self-explanatory, while the third is the group of two-by-two matrices of determinant one over the field with three elements. All the groups act via linear transformations on the lattice in which the polytope lives, and act transitively on its vertices. Full details can be found in .
2.2.4. Complete Intersections of Four Quadrics in
A particularly fertile starting point for finding new Calabi-Yau manifolds has been the complete intersection of four quadrics in . A smooth member of this family is a Calabi-Yau manifold with Hodge numbers . Hua classified free group actions on smooth subfamilies in , finding groups of order 2, 4, 8, 16, and 32. The quotients all have , and 33, 17, 9, 5, and 3, respectively.
Certain nodal families allow free actions of groups of order 64 and, furthermore, have equivariant small resolutions [15, 18]. The resolutions have Hodge numbers and inherit the free group actions. Remarkably, in this case, all the quotients have the same Hodge numbers as the covering space. The quotient by was investigated as a background for heterotic string theory in , but unfortunately, no realistic models were found.
Freitag and Salvati Manni have also constructed a large number of new manifolds by starting with a particular complete intersection of four quadrics which has 96 nodes and a very large symmetry group [28, 29]. They show that the quotients by many subgroups admit crepant projective resolutions, thereby giving rise to a large number of new Calabi-Yau manifolds. Some of the subgroups of order 2, 4, 8, and 16 act freely on a small resolution of , and the corresponding quotient manifolds are connected to some of Hua's examples by conifold transitions. The manifolds from  with small Hodge numbers are listed in the appendix 4, including one with , which is, therefore, equal with Braun's manifolds for smallest known Hodge numbers. Note that the theoretical minimum is .
3. New Manifolds From Topological Transitions
One fascinating feature of Calabi-Yau threefolds is the interconnectedness of moduli spaces of topologically distinct manifolds. Generally speaking, there are two ways to pass from one smooth Calabi-Yau to another. We may deform the complex structure until a singularity develops and then “resolve” this singularity using the techniques of algebraic geometry, which involves replacing the singular set with new embedded holomorphic curves or surfaces. Alternatively, we may allow certain embedded curves or surfaces to collapse to zero size and then “smooth” the resulting singular space by varying its complex structure. Obviously these two processes are inverses of each other.
Our main interest here is in constructing new smooth Calabi-Yau threefolds via such topological transitions, but first we will indulge in a few comments about the connectedness of the space of all Calabi-Yau threefolds.
The suggestion that all Calabi-Yau threefolds might be connected by topological transitions goes back to . Early work showed that this was true for nearly all examples known at the time [30, 31]. These papers considered conifold transitions, in which the intermediate variety has only nodal singularities; the smoothing process replaces these singular points by three-spheres, while the “small” resolution replaces them by two-spheres (holomorphically embedded). Such singularities were shown to be at finite distance in moduli space [32, 33], and conifold transitions were later shown to be smooth processes in type II string theory [59, 60].
If we wish to connect all Calabi-Yau threefolds, conifold transitions are not sufficient, because they cannot change the fundamental group. To see this, we note that topologically, a conifold transition consists of removing neighbourhoods of some number of copies of , each with boundary , and replacing them with similar neighbourhoods of . Since all these spaces are simply connected, a simple application of van Kampen's theorem (see, e.g., ) shows that the fundamental group does not change.
There do exist relatively mild topological transitions which can change the fundamental group; these are known as hyperconifold transitions and were described by the author in [36, 37]. Here, the singularities of the intermediate variety are finite quotients of a node, and their resolutions are no longer “small”. It is an interesting question whether all Calabi-Yau threefolds can be connected by conifold and hyperconifold transitions.
In the following sections, we will consider these two types of transition separately, mostly through examples. The examples in Section 3.2 actually yield previously unknown manifolds, with Hodge numbers and and fundamental groups and , respectively.
3.1. Conifold Transitions
In [2, 24], free group actions were followed through conifold transitions, leading to webs of conifold transitions between smooth quotients with the same fundamental group (conifold transitions were also used in [34, 35] to construct new simply connected manifolds). Here, we will just consider a simple example (taken from ) which exemplifies the idea.
Consider the well-known family of quintic hypersurfaces in , with Hodge numbers and hence Euler number . If we take homogeneous coordinates on , then an action of can be defined by the generator Then, there is a smooth family of invariant quintics, given by For generic coefficients, acts freely, so we get a family of smooth quotients with Hodge numbers .
Now, let us consider a nongeneric choice for the coefficients in (3.2) such that is the determinant of some matrix which is linear in the homogeneous coordinates. If we take the entries of to be then the induced action is , so the determinant does indeed correspond to an invariant quintic. The action of is still generically fixed-point-free on the family given by det , but the hypersurfaces are no longer smooth. Indeed, using a computer algebra package, it can be checked that the rank of drops to three at exactly fifty points on a typical such hypersurface, and that these points are nodes. Furthermore, they fall into ten orbits of five nodes under the action.
We now ask whether these nodes can be resolved in a group-invariant way; if so, the group will still act freely on the resolved manifolds, and we will have constructed a conifold transition between the quotient manifolds. In fact this is easy to do. Introduce a second , with homogeneous coordinates , and consider the equations These are five bilinears in , and it can be checked that they generically define a smooth Calabi-Yau threefold . Since we cannot have , there are only simultaneous solutions to these equations when det , so this gives a projection from to nodal members of . At most points, this is one-to-one, but at the fifty points where the rank of drops to three, we get a whole copy of projecting to a (nodal) point of . In this way we see that we have constructed a conifold transition .
To see that the free action is preserved by the conifold transition above, it suffices to note that if we extend the action by defining , then this induces , implying that the manifolds defined by (3.4) are -invariant. The absence of fixed points follows from the absence of fixed points on the nodal members of although this can also be checked directly.
Since the conifold transition from to can be made -equivariant, it descends to a conifold transition between their quotients, , where the intermediate variety has ten nodes.
3.2. Hyperconifold Transitions
The conifold transition in the last section illustrates two completely general features of such transitions: the fundamental group does not change, for reasons explained previously, and the intermediate singular variety has multiple nodes . We now turn our attention to a class of transitions for which neither of these statements hold—the so-called hyperconifold transitions introduced in . Here, the intermediate space typically has only one singular point, which is a quotient of a node by some finite cyclic group . (Quotients by non-Abelian groups can also occur, but these do not admit a toric description, and their resolutions have not been studied.) These arise naturally when a generically free group action is allowed to develop a fixed point. A -hyperconifold transition changes the Hodge numbers according to
The resolution of a hyperconifold singularity replaces the singular point with a simply connected space, and in this way, we see that the transitions can change the fundamental group. It is worth pausing here to consider this in more detail than has been done in previous papers.
Suppose that we have a smooth quotient and deform the complex structure until some order- element , which generates a subgroup , develops a fixed point . Then, as described in , this point will be singular, and generically a node. In some cases, the group structure implies that other elements will simultaneously develop fixed points, which we can see by taking a group element and performing an elementary calculation So, the point is fixed by . We see that every subgroup conjugate to also develops a fixed point. All such points are identified by , so the singular quotient has only one -hyperconifold singularity.
What is the fundamental group of the resolution ? To calculate this, excise a small ball around each fixed point of to obtain a smooth space on which the whole group acts freely. We can then quotient by to obtain , with fundamental group . Finally, we glue in a neighbourhood of the exceptional set of the resolution of the hyperconifold. is simply connected. We now have , and can use van Kampen's theorem to calculate . Note that the intersection of the two subspaces and is homotopy equivalent to , since the stabiliser of each point on the covering space was isomorphic to . So, we have the data which by van Kampen's theorem immediately implies that , where is the smallest normal subgroup of which contains , usually called the normal closure.
Trivial examples arise when or , and the generator of develops a fixed point. In this case, the corresponding hyperconifold transition changes the fundamental group from to .
3.2.1. Example 1:
We will first consider an example related to that in Section 3.1. If we demand that the matrix appearing in (3.4) is symmetric, , then the resulting family of threefolds are invariant under a further order-two symmetry, generated by . As shown in , this family is still generically smooth, and the entire group acts freely, so we get a smooth quotient family .
Suppose now that we ask for to develop a fixed point. In the ambient space, it fixes an entire copy of , given by . Choose a single point on this locus (as long as it is not also a fixed point of ), say . The evaluation of the defining polynomials at this point is , so it lies on the hypersurface if . One can check that for arbitrary choices of the other coefficients; this point is a node on the covering space, and there are no other singularities. This, therefore, corresponds to a sub-family of with an isolated -hyperconifold singularity. Such a singularity has a crepant projective resolution, as described in , obtained by a simple blowup of the singular point. This introduces an irreducible exceptional divisor, thus increasing by one, and since we imposed a single constraint on the complex structure of , (naïvely, it seems that we have imposed five constraints, . However, we had the freedom to choose a generic point on the fixed , corresponding to a four-parameter choice of possible conditions, so the number of complex structure parameters is actually only reduced by one.) the resolved space has Hodge numbers , and its fundamental group is . (Note that this is, in fact, a new “three-generation” manifold, with . Unfortunately, -valued Wilson lines cannot perform the symmetry breaking required for a realistic model.)
So we have constructed a -hyperconifold transition , where the fundamental group of the first space is and that of the second space is .
3.2.2. Example 2:
For a second example, which will also yield an interesting new manifold, consider the quotient of , described in Section 2.2.1. As shown in , there is a codimension-one locus in moduli space, where the unique order-two element of the group develops a fixed point. It is easy to check that on the covering space, this is the only singular point, and is a node. As such, the quotient space develops a -hyperconifold singularity. Blowing up this point yields a new Calabi-Yau manifold, with Hodge numbers , as per the general formula (3.5).
The subgroup of is actually the centre, so it is trivially normal, and the fundamental group of the new manifold is , which is isomorphic to , the symmetric group on three letters. To see this, recall that is generated by two elements, and , of orders three and four, respectively, subject to the relation . So, the subgroup is generated by , meaning that in , . To reflect this, we rename to and obtain which is the standard presentation of .
So, in summary, we have constructed a -hyperconifold transition , where the fundamental group of the first space is and that of the second space is . This is the first known Calabi-Yau threefold with fundamental group .
The New-Look Zoo
The techniques reviewed in Sections 2 and 3, along with a few exceptional constructions, have led in recent years to the construction of a relatively large number of new Calabi-Yau threefolds with small Hodge numbers and/or nontrivial fundamental group. A table appeared in  of all manifolds known at the time with . Instead of repeating that list here, only new manifolds discovered since the appearance of  are listed in Table 2 and Table 3. Since they are of most relevance for string theory, those with nontrivial fundamental group are listed separately in Table 2, while Table 3 contains new simply connected manifolds and those with fundamental group yet to be calculated. Figure 2 displays the tip of the distribution of manifolds catalogued by their Hodge numbers, showing which values of satisfying are realised by known examples (and their mirrors, which are assumed to exist).
|This table complements the one in , and briefly describes the manifolds which have and nontrivial fundamental group discovered since that paper appeared in 2008. There should still be a number of other manifolds in this region, including quotients from  whose Hodge numbers have not yet been calculated, and manifolds obtained from known quotients by hyperconifold transitions , of which only a few have so far been written down explicitly. In the “Manifold” column, denotes the Calabi-Yau toric hypersurface associated to the 24-cell, discussed in  and Section 2.2.3, while refers to the manifold discussed in Section 2.2.2, and to that in Section 2.2.1. is the del Pezzo surface of degree . Multiple quotient groups indicate different quotients with the same Hodge numbers. denotes a singular member of a generically smooth family, while denotes a resolution of a singular variety . The column labelled by gives the fundamental group. For each manifold listed here there should also be a mirror, which is not listed.|
|This table is the same as that above, except all the manifolds listed either have trivial fundamental group, or a fundamental group which has not been calculated (which is the case for several examples from ). The notation is the same as above, and the manifolds with no description are all desingularisations of quotients by various groups of a singular complete intersection of four quadrics in .|
The author would like to thank Eberhard Freitag for useful correspondence, and Philip Candelas for helpful comments on a draft of this paper. This work was supported by the Engineering and Physical Sciences Research Council (Grant no. EP/H02672X/1).
- P. Candelas, X. de la Ossa, Y.-H. He, and B. Szendroi, “Triadophilia: a special corner in the landscape,” Advances in Theoretical and Mathematical Physics, vol. 12, no. 2, pp. 429–473, 2008.
- P. Candelas and R. Davies, “New Calabi-Yau manifolds with small hodge numbers,” Fortschritte der Physik, vol. 58, no. 4-5, pp. 383–466, 2010.
- P. Green and T. Hubsch, “Calabi-Yau manifolds as complete intersections in products of complex projective spaces,” Communications in Mathematical Physics, vol. 109, no. 1, pp. 99–108, 1987.
- P. Candelas, A. M. Dale, C. A. Lutken, and R. Schimmrigk, “Complete intersection Calabi-Yau manifolds,” Nuclear Physics B, vol. 298, no. 3, pp. 493–525, 1988.
- P. S. Green, T. Hubsch, and C. A. Lutken, “All the Hodge numbers for all Calabi-Yau complete intersections Calabi-Yau manifolds,” Classical and Quantum Gravity, vol. 6, no. 2, pp. 105–124, 1989.
- V. Batyrev and L. A. Borisov, “On Calabi-Yau complete intersections in toric varieties,” http://arxiv.org/abs/alg-geom/9412017.
- M. Kreuzer and H. Skarke, “On the classification of reflexive polyhedra,” Communications in Mathematical Physics, vol. 185, no. 2, pp. 495–508, 1997.
- M. Kreuzer and H. Skarke, “Complete classification of reflexive polyhedra in four-dimensions,” Advances in Theoretical and Mathematical Physics, vol. 4, no. 6, pp. 1209–1230, 2000.
- P. Candelas, G. T. Horowitz, A. Strominger, and E. Witten, “Vacuum configurations for superstrings,” Nuclear Physics B, vol. 258, no. 1, pp. 46–74, 1985.
- S.-T. Yau, “Compact three-dimensional Kähler manifolds with zero Ricci curvature,” in Proceedings of the Argonne-Chicago Symposium on Anomalies, Geometry and Topology, A. White, Ed., pp. 395–406, World Scientific, 1985.
- A. Strominger and E. Witten, “New manifolds for superstring compactification,” Communications in Mathematical Physics, vol. 101, no. 3, pp. 341–361, 1985.
- P. Candelas, C. A. Lutken, and R. Schimmrigk, “Complete intersection Calabi-Yau manifolds II: three generation manifolds,” Nuclear Physics B, vol. 306, no. 1, pp. 113–136, 1988.
- R. Schimmrigk, “A new construction of a three-generation Calabi-Yau manifold,” Physics Letters B, vol. 193, no. 2-3, pp. 175–180, 1987.
- A. Beauville, “A Calabi-Yau threefold with non-abelian fundamental group,” in New Trends in Algebraic Geometry, vol. 264 of London Mathematical Society Lecture Note Series, pp. 13–17, Cambridge University Press, Cambridge, UK, 1999.
- M. Gross and S. Popescu, “Calabi-Yau threefolds and moduli of abelian surfaces I,” Compositio Mathematica, vol. 127, no. 2, pp. 169–228, 2001.
- V. Braun, B. A. Ovrut, T. Pantev, and R. Reinbacher, “Elliptic Calabi-Yau threefolds with Wilson lines,” Journal of High Energy Physics, vol. 2004, no. 12, article 062, 2004.
- V. Batyrev and M. Kreuzer, “Integral cohomology and mirror symmetry for Calabi-Yau 3-folds,” in Proceedings of "Mirror Symmetry IV", AMS/IP Studies in Advanced Mathematics, N. Yui, S.-T. Yau, S.-T. Yau, and J. D. Lewis, Eds., 2006, http://arxiv.org/abs/math/0505432.
- Z. Hua, “Classification of free actions on complete intersections of four quadrics,” http://arxiv.org/abs/0707.4339.
- V. Bouchard and R. Donagi, “On a class of non-simply connected Calabi-Yau threefolds,” Communications in Number Theory and Physics, vol. 2, no. 1, pp. 1–61, 2008.
- L. Borisov and Z. Hua, “On Calabi-Yau threefolds with large nonabelian fundamental groups,” Proceedings of the American Mathematical Society, vol. 136, no. 5, pp. 1549–1551, 2008.
- M. Gross and S. Popescu, “Calabi-yau three-folds and moduli of abelian surfaces II,” Transactions of the American Mathematical Society, vol. 363, no. 7, pp. 3573–3599, 2011.
- V. Braun, P. Candelas, and R. Davies, “A three-generation Calabi-Yau manifold with small Hodge numbers,” Fortschritte der Physik, vol. 58, no. 4-5, pp. 467–502, 2010.
- V. Braun, “On free quotients of complete intersection Calabi-Yau manifolds,” JHEP 1104 (2011) 005, http://arxiv.org/abs/1003.3235.
- P. Candelas and A. Constantin, “Completing the web of —quotients of complete intersection Calabi-Yau manifolds,” http://arxiv.org/abs/1010.1878.
- V. Braun, “The 24-cell and Calabi-Yau threefolds with hodge numbers (1,1),” http://arxiv.org/abs/1102.4880.
- G. Bini and F. F. Favale, “Groups acting freely on Calabi-Yau threefolds embedded in a product of del Pezzo surfaces,” http://arxiv.org/abs/1104.0247.
- A. Stapledon, “New mirror pairs of Calabi-Yau orbifolds,” http://arxiv.org/abs/1011.5006.
- E. Freitag and R. Salvati Manni, “Some siegel threefolds with a Calabi-Yau model II,” http://arxiv.org/abs/1001.0324.
- E. Freitag and R. Salvati Manni, “On siegel threefolds with a projective Calabi-Yau model,” http://arxiv.org/abs/1103.2040.
- P. S. Green and T. Hubsch, “Connecting moduli spaces of Calabi-Yau threefolds,” Communications in Mathematical Physics, vol. 119, no. 3, pp. 431–441, 1988.
- P. S. Green and T. Hubsch, “Possible phase transitions among Calabi-Yau compactifications,” Physical Review Letters, vol. 61, no. 10, pp. 1163–1166, 1988.
- P. Candelas, P. S. Green, and T. Hubsch, “Finite distance between distinct Calabi-Yau manifolds,” Physical Review Letters, vol. 62, no. 17, pp. 1956–1959, 1989.
- P. Candelas, P. S. Green, and T. Hubsch, “Rolling among Calabi-Yau vacua,” Nuclear Physics B, vol. 330, no. 1, pp. 49–102, 1990.
- V. Batyrev and M. Kreuzer, “Constructing new Calabi-Yau 3-folds and their mirrors via conifold transitions,” Advances in Theoretical and Mathematical Physics, no. 14, pp. 879–898, 2010, http://arxiv.org/abs/0802.3376.
- S. Filippini and V. Garbagnati, “A rigid Calabi—Yau 3-fold,” http://arxiv.org/abs/1102.1854.
- R. Davies, “Quotients of the conifold in compact Calabi-Yau threefolds, and new topological transitions,” Advances in Theoretical and Mathematical Physics, no. 14, pp. 965–990, 2010, http://arxiv.org/abs/0911.0708.
- R. Davies, “Hyperconifold transitions, mirror symmetry, and string theory,” Nuclear Physics B, vol. 850, pp. 214–233, 2011, http://arxiv.org/abs/1102.1428.
- L. B. Anderson, J. Gray, A. Lukas, and B. Ovrut, “Stabilizing the complex structure in heterotic Calabi-Yau vacua,” Journal of High Energy Physics, vol. 2011, no. 2, article 88, 2011.
- L. B. Anderson, J. Gray, A. Lukas, and B. Ovrut, “Stabilizing all geometric moduli in heterotic Calabi-Yau vacua,” Physical Review D, vol. 83, Article ID 106011, 14 pages, 2011.
- M. F. Atiyah and R. Bott, “A Lefschetz fixed point formula for elliptic differential operators,” Bulletin of the American Mathematical Society, vol. 72, pp. 245–250, 1966.
- M. F. Atiyah and R. Bott, “A Lefschetz fixed point formula for elliptic complexes: II applications,” Annals of Mathematics, vol. 88, pp. 451–491, 1968.
- W. Decker, G.-M. Greuel, G. Pfister, and H. Schönemann, “Singular 3-1-2—a computer algebra system for polynomial computations,” http://www.singular.uni-kl.de.
- Wolfram Research, Mathematica, Version 8.0, Wolfram Research, 2010.
- J. Gray, Y.-H He, A. Ilderton, and A. Lukas, “Stringvacua: a mathematica package for studying vacuum configurations in string phenomenology,” Computer Physics Communications, vol. 180, no. 1, pp. 107–119, 2009.
- R. Hartshorne, Algebraic Geometry, Graduate Texts in Mathematics, Springer, New York, NY, USA, 1977.
- B. McInnes, “Group-theoretic aspects of the Hosotani mechanism,” Journal of Physics A, vol. 22, no. 13, pp. 2309–2328, 1989.
- E. Witten, “New issues in manifolds of SU(3) holonomy,” Nuclear Physics B, vol. 268, no. 1, pp. 79–112, 1986.
- J. Li and S.-T. Yau, “The existence of supersymmetric string theory with torsion,” Journal of Differential Geometry, vol. 70, no. 1, pp. 143–181, 2005.
- R. Davies, Calabi-Yau threefolds and heterotic string compactification, DPhil thesis, Oxford University, Oxford, UK, 2010, http://ora.ouls.ox.ac.uk/objects/uuid:be92aac5-6874-431e-95a0-ac61a88ee63d.
- V. Braun, Y.-H. He, B. A. Ovrut, and T. Pantev, “The exact MSSM spectrum from string theory,” Journal of High Energy Physics, vol. 2006, no. 5, article 043, 2006.
- V. Braun, Y.-H. He, and B. A. Ovrut, “Yukawa couplings in heterotic standard models,” Journal of High Energy Physics, vol. 2006, no. 4, article 019, 2006.
- L. B. Anderson, J. Gray, Y.-H. He, and A. Lukas, “Exploring positive monad bundles and a new heterotic standard model,” Journal of High Energy Physics, vol. 2010, no. 2, article 054, 2010.
- V. Bouchard and R. Donagi, “An SU(5) heterotic standard model,” Physics Letters B, vol. 633, no. 6, pp. 783–791, 2006.
- V. Bouchard, M. Cvetic, and R. Donagi, “Tri-linear couplings in an heterotic minimal supersymmetric standard model,” Nuclear Physics B, vol. 745, no. 1-2, pp. 62–83, 2006.
- V. Braun, B. A. Ovrut, M. Kreuzer, and E. Scheidegger, “Worldsheet instantons and torsion curves, part A: direct computation,” Journal of High Energy Physics, vol. 2007, no. 10, article 022, 2007.
- V. Braun, B. A. Ovrut, M. Kreuzer, and E. Scheidegger, “Worldsheet instantons and torsion curves part B: mirror symmetry,” Journal of High Energy Physics, vol. 2007, no. 10, article 023, 2007.
- A. Bak, V. Bouchard, and R. Donagi, “Exploring a new peak in the heterotic landscape,” Journal of High Energy Physics, vol. 2010, no. 6, article 108, 2010.
- M. Reid, “The moduli space of 3-folds with may nevertheless be irreducible,” Mathematische Annalen, vol. 278, no. 1–4, pp. 329–334, 1987.
- A. Strominger, “Massless black holes and conifolds in string theory,” Nuclear Physics B, vol. 451, no. 1-2, pp. 96–108, 1995.
- B. R. Greene, D. R. Morrison, and A. Strominger, “Black hole condensation and the unification of string vacua,” Nuclear Physics B, vol. 451, no. 1-2, pp. 109–120, 1995.
- A. Hatcher, Algebraic Topology, Cambridge University Press, Cambridge, UK, 2002.
- P. Candelas and X. C. de la Ossa, “Comments on conifolds,” Nuclear Physics B, vol. 342, no. 1, pp. 246–268, 1990.
Copyright © 2011 Rhys Davies. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.