next up previous
Next: The example Up: Black hole condensation and Previous: Introduction and summary

Classical structure of conifolds

For concreteness, we focus on a particular example in this paper, although our analysis is general. The moduli space of all complex structures on a quintic threefold X can be described in terms of the defining equations of the quintics: the general such equation takes the form of a homogeneous quintic polynomial

 

and involves 126 coefficients. Some 25 of these are redundant due to the action of on the homogeneous coordinates , leaving 101 independent parameters in the moduli space.

For general values of , the equation 1 defines a nonsingular Calabi--Yau manifold in , but at certain special values (along a set of complex codimension 1 in the parameter space), the solution set of 1 becomes singular. These singularities were analyzed many years ago by Lefschetz [15], who showed that:

1) the ``generic'' singular space , has a single node, i.e., a singular point with local equation , (we distinguish between the singular points of the Calabi--Yau---here called nodes---and the points in the moduli space which label such Calabi--Yau's---called conifold points)

2) the singular point determines a ``vanishing cycle'' which shrinks to zero size when the singularity is approached (more precisely, the period integrals over vanish in the limit), and

3) the homology of the Calabi--Yau manifolds undergoes a monodromy transformation

 

upon transport around a loop in encircling the singular locus . (Here, denotes the number of (oriented) intersections of with .) If all of the singular points on are nodes, then is called a ``Calabi--Yau conifold'' (so named [9] because of the conical nature of the singularities).

If we introduce a holomorphic 3-form (depending on the moduli), and use the ``periods'' of to describe the complex structure, we find that some of the periods become multiple-valued near the singular locus. In fact, if we let

 

be the period corresponding to the vanishing cycle, then we find that the singular locus in is locally described by Z=0, and that other periods must take the form

 

near Z=0 in order to have the correct monodromy property.

Let us now consider the set of quintic conifolds in which have k singular points. Since asking for a single node places a single condition on the parameters, one's initial expectation is that asking for a conifold with k singular points will place k conditions on the parameters, leading to a locus of complex codimension k in . When this is true, the generic point of that locus will locally be an intersection of k hypersurfaces, meeting transversally. Near the intersection of all of these, there will be k different monodromy transformations with vanishing cycles , ..., , and the periods must take the form

 

near , where are among the local coordinates near the intersection.

However, in the example which we will study in detail there are k=16 singular points on the conifold which impose only 15 conditions on the parameters. In fact, the vanishing cycles in our example in the next section will satisfy the homology relation

 

which implies a corresponding relation among the periods:

 

The locus of conifolds with (at least) 15 singular points is described by , but since the hypersurface passes through this locus (as a consequence of 7), the point is also present, without imposing any further conditions. This is clearly a special property of the particular collection of 16 points which we are considering.

In this situation, we have 16 monodromy transformations near a locus of codimension 15. The asymptotic form 5 still holds near , but the and are related by 6 and 7. In particular, only a subset of the 's can be included among a list of local coordinates near the intersection locus.



next up previous
Next: The example Up: Black hole condensation and Previous: Introduction and summary



David R. Morrison
Fri Sep 15 17:40:10 EDT 1995