On the topology of determinantal links
Abstract.
We study the cohomology of the generic determinantal varieties , their polar multiplicities, their sections by generic hyperplanes of various codimension , and the real and complex links of the spaces . Such complex links were shown to provide the basic building blocks in a bouquet decomposition for the (determinantal) smoothings of smoothable isolated determinantal singularities. The detailed vanishing topology of such singularities was still not fully understood beyond isolated complete intersections and a few further special cases. Our results now allow to compute all distinct Betti numbers of any determinantal smoothing.
1. Introduction and results
The motivation for this paper is to understand the vanishing (co-)homology of isolated determinantal singularities (abbreviated as IDS in the following) which admit a determinantal smoothing . Despite their seemingly odd definition (see below), they are quite frequently encountered; for instance any normal surface singularity in and any so-called “space curve” is determinantal by virtue of the Hilbert-Burch theorem, see e.g. [Wah16] and [Sch77]. It was shown in [Zac20] that sections of the generic determinantal varieties by hyperplanes , which are of codimension and in general position off the origin, provide the fundamental building blocks in a bouquet decomposition of the determinantal smoothing .
In this paper we aim to study these building blocks
which we shall refer to as complex links of codimension , and discuss the implications for the vanishing topology of various singularities. Our main result in this regard is that whenever is sufficiently big so that the hyperplane misses the singular locus of and is smooth, then the cohomology in degrees below the middle degree is
that is, it is isomorphic to the cohomology of a Grassmannian, see (37).
In the general case, i.e. for arbitrary codimension , we provide a formula (11) for the Euler characteristic of based on the polar methods developed by Lê and Teissier. We proceed to study the polar multiplicities of the generic determinantal varieties in Section 2.4 and obtain a formula (21) for these numbers as an integral of Segre classes. It should be noted that this formula does not depend on the choice of any generic hyperplane section and it can be implemented effectively in a computer algebra system. However, we were unable to prove a closed formula for the numbers as a function of , and ; even though the calculated Tables 1, and 3 – 7 yield several patterns.
Coming back to the case of smooth links, this allows then to also compute the middle Betti number of (but unfortunately not the full cohomology group with integer coefficients in general, i.e. there could also be torsion).
We would like to point out that many methods developed in this article apply much more generally to compute the cohomology of the links of higher codimension for spaces which decompose into orbits of a Lie group action . The generic determinantal varieties treated here are just one particular, accessible example.
We continue with the discussion of the implications of these results for arbitrary smoothable IDS. Let
be a holomorphic map germ to the space of -matrices. We say that is determinantal for and of type if we have and such that . In this case we also write to emphasize the chosen determinantal structure for .
By definition, a determinantal deformation is induced by an unfolding of on parameters such that is equal to the original map and is transverse to in a stratified sense for . Then is a smoothing of , provided that is strictly smaller than the codimension of the singular locus of . In this case we shall speak of the determinantal smoothing111Note that in the case of an isolated determinantal hypersurface singularity given by a smoothing of the singularity always exists, but it can be realized by a determinantal deformation only when . of and it can be shown that, up to diffeomorphism, this smoothing depends only on the choice of the determinantal structure for , but not on the particular unfolding of the matrix. We will therefore also write for the determinantal smoothing of .
Note that every complete intersection singularity of codimension is determinantal of type for the matrix whose entries are given by a regular sequence generating the ideal of . In this case the determinantal deformations coincide with the usual deformations of the singularity. We refer to [FKZ21] for the details on determinantal singularities and their deformations and further references for the above statements.
The aforementioned bouquet decomposition of the determinantal smoothing of an IDS from [Zac20] reads
(1) |
where we denote by the unit sphere of real dimension . Combining this with our results we find
Theorem 1.1.
Let be the determinantal smoothing of a -dimensional smoothable isolated determinantal singularity of type with . Then the truncated cohomology
embeds into the cohomology of with a quotient concentrated in cohomological degree . Moreover, the left hand side is generated as an algebra by the Segre classes of the vector bundle on whose fiber at a point is presented by the perturbed matrix
which defines the smoothing .
0 | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 | |
1 | 1 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 |
2 | 3 | 4 | 3 | 0 | 0 | 0 | 0 | 0 | 0 | 0 |
3 | 6 | 16 | 27 | 24 | 10 | 0 | 0 | 0 | 0 | 0 |
4 | 10 | 40 | 105 | 176 | 190 | 120 | 35 | 0 | 0 | 0 |
5 | 15 | 80 | 285 | 696 | 1200 | 1440 | 1155 | 560 | 126 | 0 |
6 | 21 | 140 | 630 | 2016 | 4760 | 8352 | 10815 | 10080 | 6426 | 2520 |
7 | 28 | 224 | 1218 | 4816 | 14420 | 33216 | 59143 | 80976 | 83916 | 63840 |
8 | 36 | 336 | 2142 | 10080 | 36540 | 104112 | 235557 | 424384 | 606564 | 680400 |
9 | 45 | 480 | 3510 | 19152 | 81480 | 276480 | 758205 | 1691920 | 3077838 | 4551840 |
10 | 55 | 660 | 5445 | 33792 | 165000 | 649440 | 2091705 | 5563360 | 12278970 | 22518200 |
10 | 11 | 12 | 13 | 14 | 15 | 16 | 17 | 18 | 19 | |
6 | 462 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 | 0 |
7 | 33726 | 11088 | 1716 | 0 | 0 | 0 | 0 | 0 | 0 | 0 |
8 | 587202 | 376992 | 169884 | 48048 | 6435 | 0 | 0 | 0 | 0 | 0 |
9 | 5430810 | 5155920 | 3809520 | 2114112 | 830115 | 205920 | 24310 | 0 | 0 | 0 |
10 | 34240800 | 42926400 | 43929600 | 36132096 | 23326875 | 11394240 | 3962530 | 875160 | 92378 | 0 |
In the case of smoothable isolated Cohen-Macaulay codimension singularities we obtain some more specific results which might be of particular interest. As remarked earlier, these singularities admit a canonical determinantal structure by virtue of the Hilbert-Burch theorem (see [Hil90], [Bur68], or [Eis95] for a textbook): Let be a minimal set of generators for the ideal defining . Then the minimal free resolution of over the ring takes the form
for some matrix and then is determinantal of type for the matrix . Moreover, any deformation of is also automatically determinantal (see [Sch77]), i.e. it arises from a perturbation of . Isolated Cohen-Macaulay codimension singularities exist up to dimension and they are smoothable if and only if this inequality is strict.
The generic determinantal varieties appearing in the context of the Hilbert-Burch theorem are naturally limited to and we list their polar multiplicities for values in Table 1. From these numbers we can then also compute the Euler characteristic of the smooth complex links of their generic hyperplane sections, listed in Table 2.
1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 | 10 | |
0 | 1 | 3 | 6 | 10 | 15 | 21 | 28 | 36 | 45 | 55 |
1 | 0 | -1 | -10 | -30 | -65 | -119 | -196 | -300 | -435 | -605 |
2 | 0 | 2 | 17 | 75 | 220 | 511 | 1022 | 1842 | 3075 | 4840 |
3 | 0 | 2 | -7 | -101 | -476 | -1505 | -3794 | -9138 | -16077 | -28952 |
As a consequence of Theorem 1.1 we obtain:
Corollary 1.2.
Let be a Cohen-Macaulay germ of codimension with an isolated singularity at the origin and its smoothing. Then is free of rank one and generated by the Chern class of the canonical bundle on .
This has been conjectured by the author in [Zac18] where a special case of Corollary 1.2 was obtained for those singularities defined by -matrices. Our results on the Euler characteristic of the complex links also give lower bounds for the third Betti number
(2) |
which can be read off directly from Table 2 depending on the size of the matrix . Unfortunately, we were unable to prove a closed algebraic formula for this number as a function of .
While in the case of threefolds the cohomology of the complex link prominently sticks out in the sense that it entirely covers the nontrivial contributions outside the middle degree, the situation is a little more hidden in dimensions since then all the non-trivial (reduced) cohomology of the smoothing is concentrated in the middle degree. Nevertheless, using Theorem 1.1, a lower bound for the middle Betti number can be read off from Table 2 as
(3) |
for smoothings of isolated Cohen-Macaulay codimension surfaces and
(4) |
in the case of space curves in . The proofs of Theorem 1.1 and Corollary 1.2 will be given in the last section.
Remark 1.3.
Wahl has shown in [Wah16] that for a normal surface singularity which is not Gorenstein, the second Betti number of the smoothing and the Tjurina number of obey an inequality
with equality whenever is quasi-homogeneous. In particular, this applies to all generic hyperplane sections for and of dimension . It follows from the above that and the first few values can be read off from Table 2. Comparing Wahl’s results with the bouquet decomposition (1) we see that for non-linear quasi-homogeneous singularities, the difference of the numbers and is determined by the offset
depending only on the size of the matrix . This is different compared to the case of isolated complete intersections (the case ) where we have equalities ; see [Wah85].
2. Real and complex links of higher codimension
2.1. Definitions
Let be the closed embedding of an equidimensional reduced complex analytic variety of dimension in some open set of and suppose is a complex analytic Whitney stratification for . Such stratifications always exist; a construction of a unique minimal stratification has been described in [TT81] and if not specified further, we will in the following always assume to be endowed with its minimal Whitney stratification. Moreover, we may suppose that every stratum is connected for if this was not the case, we could replace it by its distinct irreducible components.
Recall the notions of the real and complex links of along its strata. These can be defined as follows: Let be a stratum of and an arbitrary point. For simplicity, we may assume to be the origin. Choose a normal slice to through , i.e. a submanifold of complementary dimension which meets transversally in . Let be the closed ball of radius centered at . Then the real link of along the stratum is
(5) |
for sufficiently small. Similarly, the complex link is
(6) |
for a sufficiently general linear form and . For a rigorous definition of these objects see for example [GM88, Part I, Chapter 1.4] and [GM88, Part II, Chapter 2.2]. There, one can also find a proof of the fact that the real and complex links are independent of the choices involved in their definition: They are invariants of the particular stratification of and unique up to non-unique homeomorphism.
In this note we shall also be concerned with the real and complex links of higher codimension for a germ at the point .
Definition 2.1.
The real and complex links of codimension of at the origin are the classical real and complex links of a section of with a sufficiently general plane of codimension .
Note that in this definition, the classical complex link is the complex link of codimension , even though it has complex codimension as an analytic subspace of . This choice was made in order to be compatible with the notation for the real links. The reader may think of the word “link” as an indicator to increment the codimension by one to arrive at the actual codimension of the space.
By “sufficiently general” we mean that has to belong to a Zariski open subset in the Grassmannian. This set consists of planes for which variation of results in a Whitney equisingular family in and we shall briefly discuss the existence of such a set. From this it will follow immediately that the real and complex links of higher codimension are invariants of the germ itself and unique up to non-unique homeomorphism.
Consider the Grassmann modification of :
where by we denote the Grassmannian of codimension planes in the ambient space through the point . It comes naturally with two projections
(7) |
where by construction for any plane . The Grassmannian itself has a natural embedding into as the zero section of and we may think of as parametrizing the intersections of with planes of codimension . For the intersection of any plane with will be of positive dimension at and therefore is necessarily contained in the closure of its complement.
Note that for an arbitrary point the fiber over in consists of all planes containing both and the origin. It follows that the restriction
is not an isomorphism, but nevertheless a holomorphic fiber bundle with smooth fibers. In particular, any given Whitney stratification on determines a unique Whitney stratification of by pullback of the strata.
Given such a stratification on the complement of , there exists some maximal Zariski open subset such that all the strata of satisfy Whitney’s conditions (a) and (b) along . We may extend the stratification on the open subset to a Whitney stratification of , containing as a stratum. Since the Grassmannian is irreducible and complex analytic subsets have real codimension , this stratum is necessarily dense and connected.
A plane of codimension is sufficiently general in the sense of Definition 2.1 if it belongs to . The projection provides us with a canonical choice of normal slices along and by construction, we may therefore identify the real and complex links of along with the real and complex links of the germ for any . Given that the classical real and complex links are invariants of the strata in a Whitney stratification, it follows immediately that the real and complex links of higher codimension for a germ are well defined invariants of the germ itself and unique up to non-unique homeomorphism.
2.2. Synopsis with polar varieties
While it was already established in the previous discussion that the real and complex links of higher codimension are invariants of the germ itself, a more specific setup will be required in the following. Let be a sequence of linear forms defining a flag of subspaces
in via .
Definition 2.2.
Let be an equidimensional reduced complex analytic germ of dimension and a Whitney stratification of . A sequence of linear forms is called admissible for if for every the restriction of to does not annihilate any limiting tangent space of at the origin.
This particular definition is chosen with a view towards the fibration theorems and inductive arguments used in Section 4.1. However, we shall also need the results on polar varieties by Lê and Teissier from [TT81]. To this end, we recall the necessary definitions and explain how Definition 2.2 fits into the context of their paper.
The geometric setup for the treatment of limiting tangent spaces is the Nash modification. Let be a suitable representative of in some open neighborhood of the origin. The Gauss map is defined on the regular locus via
Then the Nash blowup of is defined as the closure of the graph of the Gauss map. It comes with two morphisms
where is the projection to and the natural prolongation of the Gauss map. We denote by the pullback of the tautological bundle on along and by the dual of . By construction, the fiber over a point consists of pairs where is a limiting tangent space to at . In particular, such a limiting tangent space is unique at regular points and is an isomorphism identifying the restriction of with the tangent bundle of .
A flag as above determines a set of degeneraci loci in the Grassmannian as follows. Every linear form can be pulled back to a global section in the dual of the tautological bundle of : On a fiber of the tautological bundle the section is defined to be merely the restriction of to regarded as a linear subspace of . This generalizes in the obvious way for the linear maps
for every . Adapting the notation from [TT81] we now have
Note that by construction is the whole Grassmannian. We set to be the corresponding degeneraci locus on the Nash modification and
its image in . By construction, a point belongs to if and only if there exists a limiting tangent space to at such that the restriction of to does not have full rank.
The -th polar multiplicity of is then defined for to be
(8) |
the multiplicity of the -th polar variety. We shall see below that for the variety is empty for a generic flag so that a definition of does not make sense. In the other extreme case where , the polar multiplicity is simply the multiplicity of itself.
Lemma 2.3.
Let be a sufficiently small representative of . A sequence of linear forms is admissible for if and only if for every one has
(9) |
for the associated flag . Here and denotes the strict transform of in the Nash modification.
Proof.
The proof will proceed by induction on . For we have and the statement is about the choice of . Consider the projectivized analytic set of degenerate covectors
along the central fiber of the Nash modification. Since this fiber has strictly smaller dimension than , the set of degenerate covectors has dimension and therefore the discriminant, i.e. the image of its projection to , is a closed analytic set of positive codimension. Now (9) is satisfied if and only if belongs to the complement of the affine cone of the discriminant.
Such a choice for determines . Note that by construction this intersection is transversal and therefore inherits a Whitney stratification from the one on . Moreover, at a regular point the tangent space
is naturally contained in the tangent space of to that point. Let be the strict transform of in the Nash modification. Taking limits of appropriate (sub-)sequences of regular points, it is easy to see that every limiting tangent space of at is contained in a limiting tangent space of along . Consequently, a second linear form annihilates the limiting tangent space of if and only if is degenerate on . But this means nothing else than
which establishes the claim for . The remainder of the induction is a repetition of the previous steps and left to the reader. ∎
The previous lemma provides the link of Definition 2.2 with the “Théorème de Bertini idéaliste” by Lê and Teissier [TT81, Théorème 4.1.3]. They establish the existence of Zariski open subsets with certain good properties concerning the variety for . A posteriori, they discuss in [TT81, Proposition 4.1.5] that if the whole flag has been chosen such that for all , then also (9) is in fact satisfied for all . Thus we obtain the following
Corollary 2.4.
For every equidimensional reduced analytic germ there exists a Zariski open and dense subset of admissible sequences of linear forms . Moreover, this sequence can be chosen such that for the associated flag the space is sufficiently general in the sense of Definition 2.1 so that the real and complex links of codimension are given by
and
for , respectively.
Proof.
Consider the sets with from Lê’s and Teissier’s “Théorème de Bertini idéaliste” and the set of Whitney equisingular sections from the discussion of Definition 2.1. Since the intersection of Zariski open sets is again Zariski open, we may choose to be any sequence of linear forms such that
for all . ∎
We will henceforth assume that the sequence of linear forms has been chosen such that the associated flag has where is the Zariski open subset of Lê’s and Teissiers’ “Théorème de Bertini idéaliste” and the Zariski open subset of Whitney equisingular sections of codimension from the discussion of Definition 2.1.
2.3. The Euler characteristic of complex links
Lê and Teissier have described a method to compute the Euler characteristic of complex links from the polar multiplicities in [TT81, Proposition 6.1.8]. We briefly sketch how to use their results inductively in our setup from Definition 2.2.
As before, let be a reduced, equidimensional complex analytic germ of dimension , endowed with a Whitney stratification . We will assume that is a stratum and write for the closure of any other stratum of . Throughout this section, we will assume that an admissible sequence of linear forms and the associated flag have been chosen as in Corollary 2.4 for all germs at once. This flag being fixed, we will in the following suppress it from our notation and simply write for the polar varieties of the germ with being understood.
Denote by the classical complex links of along the stratum and by the complex link of codimension of at the origin. Then by [TT81, Théorème 6.1.9]
(10) |
For our specific setup we may interpret this formula in the context of stratified Morse theory. To this end, note that the restriction of to the complex link
is a stratified Morse function with critical points on the interior of the strata of precisely at the intersection points
cf. [TT81, Corollaire 4.1.6] and [TT81, Corollaire 4.1.9]. The complex link of codimension can be identified with the general fiber
for some regular value off the discriminant and we can use the function as a Morse function in order to reconstruct from . It can be shown that for suitable choices of the represenatives involved, the critical points of on the boundary of are “outward pointing” and hence do not contribute to changes in topology; see for instance [Zac17] or [PnZ18] for a discussion. For an interior critical point we have the product of the tangential and the normal Morse data
where is the disc of real dimension and the cone over the complex link of along . It is a straighforward calculation that the Euler characteristic changes precisely by for the attachement of this cell at any of the critical points . Summation over all these points on all relevant strata therefore gives us back the Formula (10) by Lê and Teissier.
It is evident that the above procedure can be applied inductively, cf. [TT81, Remarque 6.1.10]. This allows to reconstruct the codimension complex link of from its hyperplane sections
starting with which is just a set of points whose number is equal to the multiplicity of at the origin. We leave it to the reader to verify the formula
(11) |
The coefficients appearing in this formula are nothing but the local Euler obstruction of at the origin:
(12) |
cf. [TT81, Corollaire 5.1.2].
2.4. Polar multiplicities of generic determinantal varieties
We now turn towards the study of the generic determinantal varieties . These are equipped with the rank stratification, i.e. the decomposition
Due to its local analytic triviality, this stratification is easily seen to satisfy both Whitney’s conditions (a) and (b).
The reduced Euler characteristics of the classical complex links have been computed by Ebeling and Gusein-Zade in [EGZ09, Proposition 3]:
(13) |
where, without loss of generality, it is assumed that . The generic determinantal varieties admit a recursive pattern in the following sense. For , a normal slice to the stratum through the point is given by the set of matrices of the form
It follows immediately that and hence
(14) |
In order to determine the topological Euler characteristic of the complex links of higher codimension of the generic determinantal varieties by means of the previous section, we need to know all the relevant polar multiplicities
(15) |
There are several methods to achieve this. For instance, one could simply choose random linear forms and compute the resulting multiplicity with the aid of a computer algebra system using e.g. Serre’s intersection formula. However, this approach provides very little insight and the results a priori depend on the choice of the linear forms. Recently, X. Zhang has computed the polar multiplicities in [Zha17] using Chern class calculus which is an exact computation not depending on any particular choices. His formulas, however, are very complicated since they appear as byproducts of the study of the Chern-Mather classes of determinantal varieties. In this section we will follow a more direct approach to the computation of the polar multiplicities using Chern classes.
In [TT81, Théorème 5.1.1], Lê and Teissier give the following formula for the polar multiplicities of a germ :
(16) |
Here the integral is taken over the exceptional divisor of the blowup of the Nash modification along the pullback of the maximal ideal at the origin for and denotes the dual of the tautological bundle for that blowup. By construction, these spaces can be arranged in a commutative diagram
(17) |
where denotes the usual blowup of at the origin. We will now describe this diagram for the particular case where is a generic determinantal variety and deduce our particular formula (21) from that.
The Nash blowup of has been studied by Ebeling and Gusein-Zade in [EGZ09] and we briefly review their discussion. Let be the rank of the matrices in the open stratum . The tangent space to at a point is known to be
(18) |
This fact can be exploited to replace the Grassmannian for the Nash blowup of by a product: Let be the Grassmannian of -planes in and the Grassmannian of -planes in , the dual of . Then the Gauss map factors through
where by we mean the linear forms in vanishing on . We denote this double Grassmannian by . On we have the two tautological exact sequences and coming from the two factors with corresponding to the images and to the kernels of the matrices under the modified Gauss map . With this notation, the space of matrices
pulls back to the trivial bundle from which we may project to the product
Then the condition on in (18) becomes and consequently the Nash bundle on is given by
(19) |
The Nash transform itself can easily be seen to be isomorphic to the total space of the vector bundle
(20) |
on . In particular, is smooth and the maximal ideal of the origin in pulls back to the ideal sheaf of the zero section in . Thus the exceptional divisor in (17), i.e. the domain of integration in (16), is nothing but the projectivized bundle
Proposition 2.5.
The -th polar multiplicity of is given by
(21) |
where , and are the tautological sub- and quotient bundles coming from either one of the two factors, and denotes the -th Segre class.
Proof.
Starting from the Lê-Teissier formula (16) we substitute the different terms according to the above identifications for the generic determinantal varieties. From (19) we see that for every
is the -th Segre class of the complement of in . The integral in question becomes
and we may perform this integration in two steps with the first one being integration along the fibers of the projection . Since denotes the dual of the tautological bundle for the projectivization of the underlying vector bundle , the result now follows from the projection formula, cf. [Ful98, Chapter 3.1]. ∎
Formula (21) can be implemented
in computer algebra systems such as Singular [Dec+19]. For instance,
using the library schubert.lib
, the computations can easily be
carried out for on a desktop computer. Series such as,
for example, are also still feasible, but take up to 9
minutes to finish.
We have computed several polar multiplicities of the generic determinantal varieties using this formula. The results are listed in Tables 3 – 7.
Remark 2.6.
The reader will also note a symmetry that first appears in Table 4: For the polar multiplicities satisfy
(22) |
This phenomenon is based on a duality of the (projectivized) conormal modifications of the generic determinantal varieties, as has been explained to the author by Terence Gaffney in an oral communication. Formula (22) then follows from [Ura81, Theorem 3.3]. Interestingly, we have not succeeded to derive this symmetry from the formula in (21), but we nevertheless use it in the following tables in order to not duplicate the statements.
Remark 2.7.
The computation of Chern- and Segre classes of tensor products of
vector bundles is a surprisingly expensive task from a computational
point of view. Different formulas and algorithms have, for instance, been implemented
in the Singular libraries chern.lib
; see also [Szi19] for a
further discussion.
The -th Segre class of the tensor product of the two tautological subbundles on is the restriction of a universal polynomial
in the Chern classes of the tautological bundles on the product of infinite Grassmannians . However, these polynomials are not sparse and their degree in the Chern roots is bounded only by . Given that we have variables, the number of coefficients of the polynomials can roughly be estimated by . Already for values for we can therefore expect to have flooded the full RAM of any modern desktop computer.
Compared to that,
the explicit model for the cohomology of introduced above leads
to an algebra of dimension for the cohomology of
. This number is in general strictly smaller than the number of
coefficients of .
Since we shall only need the results for fixed values of and , it
seems likely that a manual implementation of a modular approach,
using the ideals introduced above,
could produce some further results for the polar multiplicities
which can not be reached using the methods provided by schubert.lib
and
chern.lib
.
Other than that, it would, of course, be even more appealing to find a closed formula for the polar multiplicities as a function of , and .
2 | 2 | 2 | |
3 | 4 | 3 | |
4 | 6 | 4 | |
5 | 8 | 5 | |
6 | 10 | 6 | |
7 | 12 | 7 |
6 | 12 | 12 | 6 | 3 | 3 | 6 | 12 | 12 | 3 | |
10 | 24 | 27 | 16 | 6 | 6 | 16 | 27 | 24 | 10 | |
15 | 40 | 48 | 30 | 10 | 10 | 30 | 48 | 40 | 15 | |
21 | 60 | 75 | 48 | 15 | 15 | 48 | 75 | 60 | 21 | |
28 | 84 | 108 | 70 | 21 | 21 | 70 | 108 | 84 | 28 | |
36 | 112 | 147 | 96 | 28 | 28 | 96 | 147 | 112 | 36 | |
45 | 144 | 192 | 126 | 36 | 36 | 126 | 192 | 144 | 45 | |
55 | 180 | 243 | 160 | 45 | 45 | 160 | 243 | 180 | 55 | |
66 | 220 | 300 | 198 | 55 | 55 | 198 | 300 | 220 | 66 | |
78 | 264 | 363 | 240 | 66 | 66 | 240 | 363 | 264 | 78 | |
91 | 312 | 432 | 286 | 78 | 78 | 286 | 432 | 312 | 91 | |
105 | 364 | 507 | 336 | 91 | 91 | 336 | 507 | 364 | 105 | |
120 | 420 | 588 | 390 | 105 | 105 | 390 | 588 | 420 | 120 | |
136 | 480 | 675 | 448 | 120 | 120 | 448 | 675 | 480 | 136 | |
153 | 544 | 768 | 510 | 136 | 136 | 510 | 768 | 554 | 153 | |
171 | 612 | 867 | 576 | 153 | 153 | 576 | 876 | 612 | 171 | |
190 | 684 | 972 | 646 | 171 | 171 | 646 | 972 | 684 | 190 | |
210 | 760 | 1083 | 720 | 190 | 190 | 720 | 1038 | 760 | 210 |
with running from the left to the right | with running from the left to the right | |||||||||||||||
0 | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 0 | 1 | 2 | 3 | 4 | 5 | 6 | |
20 | 80 | 176 | 256 | 286 | 256 | 176 | 80 | 20 | 20 | 60 | 84 | 68 | 36 | 12 | 4 | |
50 | 240 | 595 | 960 | 1116 | 960 | 595 | 240 | 50 | 35 | 120 | 190 | 176 | 105 | 40 | 10 | |
105 | 560 | 1488 | 2520 | 2980 | 2520 | 1488 | 560 | 105 | 56 | 210 | 360 | 360 | 228 | 90 | 20 | |
196 | 1120 | 3115 | 5432 | 6488 | 5432 | 3115 | 1120 | 196 | 84 | 336 | 609 | 640 | 420 | 168 | 35 | |
336 | 2016 | 5792 | 10304 | 12390 | 10304 | 5792 | 2016 | 336 | 120 | 504 | 952 | 1036 | 696 | 280 | 56 | |
540 | 3360 | 9891 | 17856 | 21576 | 17856 | 9891 | 3360 | 540 | 165 | 720 | 1404 | 1568 | 1071 | 432 | 84 | |
825 | 5280 | 15840 | 28920 | 35076 | 28920 | 15840 | 5280 | 825 | 220 | 990 | 1980 | 2256 | 1560 | 630 | 120 | |
1210 | 7920 | 24123 | 44440 | 54060 | 44440 | 24123 | 7920 | 1210 | 286 | 1320 | 2695 | 3120 | 2178 | 880 | 165 | |
1716 | 11440 | 35280 | 65472 | 79838 | 65472 | 35280 | 11440 | 1716 | 364 | 1716 | 3564 | 4180 | 2940 | 1188 | 220 | |
- | - | - | - | - | - | - | - | - | 455 | 2184 | 4602 | 5456 | 3861 | 1560 | 286 | |
- | - | - | - | - | - | - | - | - | 560 | 2730 | 5824 | 6968 | 4956 | 2002 | 364 | |
- | - | - | - | - | - | - | - | - | 680 | 3360 | 7245 | 8736 | 6240 | 2520 | 455 | |
- | - | - | - | - | - | - | - | - | 816 | 4080 | 8880 | 10780 | 7728 | 3120 | 560 | |
- | - | - | - | - | - | - | - | - | 969 | 4896 | 10744 | 13120 | 9435 | 3808 | 680 | |
- | - | - | - | - | - | - | - | - | 1140 | 5814 | 12852 | 15776 | 11376 | 4590 | 816 | |
- | - | - | - | - | - | - | - | - | 1330 | 6840 | 15219 | 18768 | 13566 | 5472 | 969 | |
- | - | - | - | - | - | - | - | - | 1540 | 7980 | 17860 | 22116 | 16020 | 6460 | 1140 | |
- | - | - | - | - | - | - | - | - | 1771 | 9240 | 20790 | 25840 | 18753 | 7560 | 1330 | |
- | - | - | - | - | - | - | - | - | 2024 | 10626 | 24024 | 29960 | 21780 | 8778 | 1540 | |
- | - | - | - | - | - | - | - | - | 2300 | 12144 | 27577 | 34496 | 25116 | 10120 | 1771 | |
- | - | - | - | - | - | - | - | - | 2600 | 13800 | 31464 | 39468 | 28776 | 11592 | 2024 | |
6 | 5 | 4 | 3 | 2 | 1 | 0 | ||||||||||
with running from the right to the left |
with running from the left to the right | |||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
0 | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | 9 | 10 | 11 | 12 | |
175 | 1050 | 3180 | 6320 | 9180 | 10320 | 9360 | 7080 | 4545 | 2430 | 1020 | 300 | 50 | |
490 | 3360 | 11445 | 25396 | 40890 | 50520 | 49495 | 39120 | 24981 | 12640 | 4830 | 1260 | 175 | |
1176 | 8820 | 32480 | 77280 | 132300 | 172074 | 175080 | 141120 | 89880 | 44310 | 16128 | 3920 | 490 | |
2520 | 20160 | 78498 | 196080 | 349860 | 470400 | 489930 | 399504 | 253980 | 123200 | 43470 | 10080 | 1176 | |
4950 | 41580 | 168840 | 437220 | 803916 | 1106640 | 1171360 | 962640 | 611100 | 293076 | 101160 | 22680 | 2520 | |
9075 | 79200 | 332310 | 884840 | 1664685 | 2332440 | 2498535 | 2064960 | 1309290 | 622560 | 211365 | 46200 | 4950 | |
15730 | 141570 | 609840 | 1660296 | 3180705 | 4518690 | 4885440 | 4055040 | 2568456 | 1213080 | 406560 | 87120 | 9075 | |
26026 | 240240 | 1057485 | 2931760 | 5699760 | 8188224 | 8918470 | 7427640 | 4700460 | 2207920 | 732303 | 154440 | 15730 | |
12 | 11 | 10 | 9 | 8 | 7 | 6 | 5 | 4 | 3 | 2 | 1 | 0 | |
with running from the right to the left |
with running from the left to the right | |||||||||
---|---|---|---|---|---|---|---|---|---|
0 | 1 | 2 | 3 | 4 | 5 | 6 | 7 | 8 | |
70 | 280 | 520 | 580 | 430 | 220 | 80 | 20 | 5 | |
126 | 560 | 1155 | 1440 | 1200 | 696 | 285 | 80 | 15 | |
210 | 1008 | 2240 | 3010 | 2700 | 1680 | 728 | 210 | 35 | |
330 | 1680 | 3948 | 5600 | 5285 | 3440 | 1540 | 448 | 70 | |
495 | 2640 | 6480 | 9576 | 9380 | 6300 | 2880 | 840 | 126 | |
715 | 3960 | 10065 | 15360 | 15480 | 10640 | 4935 | 1440 | 210 | |
1001 | 5720 | 14960 | 23430 | 24150 | 16896 | 7920 | 2310 | 330 | |
1365 | 8008 | 21450 | 34320 | 36025 | 25560 | 12078 | 3520 | 495 | |
1820 | 10920 | 29848 | 48620 | 51810 | 37180 | 17680 | 5148 | 715 | |
2380 | 14560 | 40495 | 66976 | 72280 | 52360 | 25025 | 7280 | 1001 | |
3060 | 19040 | 53760 | 90090 | 98280 | 71760 | 34440 | 10010 | 1365 | |
3876 | 24480 | 70040 | 118720 | 130725 | 96096 | 46280 | 13440 | 1820 | |
4845 | 31008 | 89760 | 153680 | 170600 | 126140 | 60928 | 17680 | 2380 | |
5985 | 38760 | 113373 | 195840 | 218960 | 162720 | 78795 | 22848 | 3060 | |
7315 | 47880 | 141360 | 246126 | 276930 | 206720 | 100320 | 29070 | 3876 | |
8855 | 58520 | 174230 | 305520 | 345705 | 259080 | 125970 | 36480 | 4845 | |
8 | 7 | 6 | 5 | 4 | 3 | 2 | 1 | 0 | |
with running from the right to the left |
Example 2.8.
We may use the above tables together with formula (11) to compute the Euler characteristics of complex links of higher codimension for the generic determinantal varieties. For instance
Note that since is smooth of complex dimension , the summation over degenerates and only the smooth stratum is relevant. Moreover, the complex link of along this stratum is empty, so that the factor simply reduces to .
This computation confirms the results in an earlier paper [FKZ15] where it was shown that the Betti numbers of are
In [FKZ15], this was a very particular example. We will discuss in Section 4 how the distinct Betti numbers can be computed for all smooth complex links of generic determinantal varieties.
To also give an example for a singular complex link, consider : This space is of complex dimension and has isolated singularities which are themselves determinantal of the form . If is a plane of codimension in in general position off the origin such that , then these singular points are precisely the intersection points of with and their number is equal to the multiplicity .
If we let be a further, sufficiently general linear form on , then the generic fiber of its restriction to is the previous space whose topology we already know. According to Table (4), has classical Morse critical points on and further stratified Morse critical points on .
For the first set of points, more cells of real dimension are added which changes the Euler characteristic by in Formula (10) (resp. (11)).
The second set of critical points on the lower dimensional stratum have a nontrivial complex link appearing in the normal Morse datum. This complex link is nothing but the Milnor fiber of the -singularity in [FKZ15]: Despite being a space of complex dimension , it is homotopy equivalent to a -sphere and its Betti numbers are in accordance with the Formula by Ebeling and Gusein-Zade (13). This means that we attach real -cells rather than -cells and the Euler characteristic changes by rather than , as one might have expected. The overall outcome therefore is
It is interesting to see the cancellation of the two contributions to the Euler characteristic given that the equality of the two relevant multiplicities is not a coincidence, but due to the duality noted by Gaffney.
We shall see later on that the first four Betti numbers of the open stratum of are
It can be shown that the attachements of the -cells at the points of glue their boundaries all to the very same generator of the second homology group. From the long exact sequence of the pair and the previous computation of the Euler characteristic one can then deduce that the Betti numbers of must be
In particular we see that the cells attached at the classical critical points of on the smooth stratum kill off all the cycles in the top homology group of . Those coming from the stratified Morse critical points on the lower dimensional stratum survive and lead to new cycles. Details for the computation of the Betti numbers in this example will appear in a forthcoming note.
3. Determinantal strata as homogeneous spaces
Let be a Lie group and a smooth action on a manifold . Then for every point the orbit is a locally closed submanifold which is diffeomorphic to the quotient of by the stabilizer of . The next lemma shows that up to homotopy we can always find a compact model for this orbit by choosing an appropriate maximal compact subgroup of .
Lemma 3.1.
Let be a Lie group, a closed subgroup, and a maximal compact subgroup such that is again a maximal compact subgroup of . Then the inclusion is a weak homotopy equivalence.
Proof.
The projection is a fiber bundle with fiber and the same holds for with fiber . Hence, there is a commutative diagram of long exact sequences of homotopy groups
and it is well known that for any Lie group the inclusion of its maximal compact subgroup is a homotopy equivalence. The assertion therefore follows from the five-lemma. ∎
3.1. The Lie group action on
We now turn to the discussion of the strata in the rank stratification as homogeneous spaces. Fix integers . The space of complex -matrices has a natural left action by the complex Lie group
via multiplication:
For two matrices and we will denote by the block matrix
Let be the zero matrix. For any number we will write for the -matrix with a unit matrix of rank in the upper left corner and zeroes in all other entries. Then clearly
where is the stabilizer of in . A direct computation yields that consists of pairs of block matrices of the form
with , and invertible, and and arbitrary of appropriate sizes.
As a compact subgroup we may choose the unitary matrices . It is easily verified that its intersection with the subgroup consists of pairs of matrices
with , , and , and that this is in fact a maximal compact subgroup of . Note that due to the fact that in contrast to the off-diagonal blocks in the subgroup are all zero, we find that
(23) |
is again isomorphic to a product of unitary groups.
Let us, for the moment, consider only the first factor of which we may consider as a subgroup via the inclusion . The stabilizer of of the restriction of the action to is simply the subgroup . The -orbit can easily be identified with the Stiefel manifold of orthonormal -frames in :
(24) |
so that an -frame in is given by the first columns of the matrix for some . The group operates naturally on the Stiefel manifold via the left action
The quotient of this action is the Grassmannian of -planes since either two -frames span the same subspace if and only if they lay in the same orbit under this -action.
It is easy to see with the above identifications (24) that two matrices and in represent the same element in if and only if :
for some . In other words, the above action is compatible with the natural inclusion of subgroups
and accordingly
(25) |
We can repeat these considerations for the second factor embedded into as . Then
with any -frame given by the first rows of the matrix for some . Accordingly, we will write the left action by on as
in this case.
Note that, on the one hand, the subgroup intersects the subgroups and in and , respectively, and the action of the latter subgroups affects only either one of the two factors. The -action, on the other hand, is “diagonal” and we may exploit these facts by observing that the quotient
(26) |
is a product of Stiefel manifolds, equipped with a free, diagonal -action. The quotient is then naturally isomorphic to and, via the particular choice of the matrix , this manifold can be identified with the orbit . We will in the following denote this orbit by and refer to it as the compact orbit model for the stratum .
Lemma 3.2.
The two natural projections
equip the space with two structures as a fiber bundle over the respective Grassmannian with Stiefel manifolds as fibers.
Proof.
It suffices to establish this claim for the first projection to . Consider the commutative diagram
where takes a pair of -frames to , is the quotient map from (25) and the one from the discussion of (26). We need to describe the fiber of an arbitrary point . To this end, consider its preimages
with some -frame in with . The fiber of over is simply the Stiefel manifold . Now if is any other -frame spanning , then there exists a unique matrix such that . The free diagonal action on gives a natural identification of the fibers of over and via
and this furnishes an obvious notion of parallel sections of over the orbit . These parallel sections can then be identified with either one of the Stiefel manifolds over a point in the orbit. ∎
Remark 3.3.
The structures of the manifolds as fiber bundle is in general not trivial. For instance
is the Hopf fibration which is known not to be a product.
3.2. The Cartan model
The cohomology of homogeneous spaces can be computed via the Cartan model as outlined by Borel in [Bor53, Théorème 25.2]. Let be a compact, connected Lie group and a closed subgroup thereof. Then [Bor53, Théorème 25.2] allows for the description of the cohomology of the quotient as the cohomology of an explicit complex
(27) |
under certain favourable assumptions on and . The objects on the right hand side are the following.
-
•
The ring is the cohomology ring of a classifying space for the group , see for instance [Hus94, Part I, Chapter 4.11]. Such a classifying space for a compact Lie group is given by the quotient of any weakly contractible space with a free -action. Then the projection turns into a universal bundle in the sense that every principal -bundle over a paracompact Haussdorff space can be written as for some continuous map .
In particular, this property can be used to show that the cohomology ring is in fact unique up to unique isomorphism and independent of the choice of the space , see e.g. [Bor53, Section 18]222The approach by Borel might seem unnecessarily technical given the Milnor construction of universal bundles in [Mil56] three years later.. In most practical cases (cf. [Bor53, Théorème 19.1]) the cohomology rings of classifying spaces are weighted homogeneous polynomial rings in variables of even degree and therefore in particular commutative.
Furthermore, we note that the total space of a universal bundle is naturally equipped with a free action, as well. It can therefore also be used to construct a classifying space as the intermediate quotient
The pullback in cohomology of the projection is called the characteristic homomorphism for the inclusion of the subgroup , cf. [Bor53, Théorème 22.2].
-
•
The module is a free, graded -module
in generators of odd degree. Hopf has shown in [Hop41, Satz 1] that the rational homology of a compact Lie group is graded isomorphic to the homology of a product of odd-dimensional spheres. This result has been strengthened to also include cohomology with integer coefficients in the absence of torsion in , see e.g. [Bor53, Proposition 7.3]. Then the generators can be thought of as the volume forms of the spheres and the cup product turns the cohomology of the group into an exterior algebra on these generators
which appears as in (27).
-
•
The differential on is given by linear extension of the map
for all , where is a transgression element of in a universal -bundle and the characteristic homomorphism from before. A transgression can be defined in a universal -bundle as above: The element is called universally transgressive if there exists a cochain on which restricts to the cohomology class in every fiber and for which there exists another cochain on with . Then is taken to be the cohomology class of and it is said to “correspond to under transgression”. For a more detailed account see [Bor53]. We will discuss the particular form of this transgression below in the cases of interest for this article.
Note that (27) is an isomorphism of graded -modules with grading given by the degree of the cohomology classes on either side. But we can also think of the algebra as a Koszul algebra in the generators over the ring :
This gives another grading on the right hand side of (27) by the degrees of the distinct exterior powers. In the following we will refer to the two gradings as the cohomological degree and the Koszul degree respectively.
3.3. Maximal tori and the Weyl group
As explained in [Bor53, Section 29], the characteristic homomorphism associated to an inclusion of a subgroup is best understood in terms of inclusions of maximal tori and . This will be an essential ingredient for the computation of the cohomology of the orbits in the determinantal strata.
For the group a classifying space is given by the infinite projective space
which can be understood as a direct limit with included in as the hyperplane section at infinity. A universal -bundle is then given by , the tautological bundle with its zero section removed or, equivalently, by the direct limit of unit spheres which are projected to via the Hopf fibration. Then the cohomology ring of is a free polynomial ring in , the first Chern class of , and the generator of corresponds to under transgression.
Now it is easy to see that for a torus the classifying spaces and universal bundles can be chosen to be merely products of the one just described for . It follows that is a polynomial ring
with all of degree .
If is a maximal torus in a compact connected Lie group , then is contained in as the invariant ring under the action of the Weyl group. Moreover, if is a subgroup and the tori and have been chosen such that , then the characteristic homomorphism for the inclusion is completely determined by the one for the inclusion so that one has a commutative diagram
(28) |
where the vertical arrows denote the inclusions of invariant subgroups. We note that in general one needs real coefficients in cohomology as in [Bor53, Proposition 29.2]. For the particular cases that we shall need below, however, the calculations have been carried out for integer coefficients as well.
3.4. Cohomology of Stiefel manifolds and Grassmannians
As discussed earlier the Stiefel manifolds and Grassmannians can be considered as homogeneous spaces of modulo various subgroups of block matrices with unitary blocks. Also the orbit varieties can be decomposed into these building blocks. Therefore we briefly review the theory for the Lie group as it can be found in [Bor53] or [Hus94] and illustrate the formula (27) for the classical cases, thereby fixing notation for the description of the cohomology of the orbit models that we are really aiming for.
The cohomology of the unitary group is known to be
(29) |
with generators of degree , see for example [Bor53, Proposition 9.1] or [Hus94, Part I, Chapter 7]. We will write
for the free graded module whose direct summands are shifted by for so that with this notation . A maximal torus in is given by the diagonal matrices
and the Weyl group is the symmetric group of permutations of elements in this case. Writing for the generators of the cohomology of as above we find that
is the inclusion of the invariant subring . According to the fundamental theorem of symmetric functions, is itself a polynomial ring in the elementary symmetric functions
Moreover, the generators correspond to these under transgression in a universal bundle , see for example [Bor53, Section 19].
The cohomology of Stiefel manifolds turns out to be a truncated version of the cohomology of :
(30) |
In order to make the connection with Formula (27) recall that . As maximal tori in the subgroup we may choose
so that with as before. Writing for the cohomology of the classifying space we find that the diagram (28) becomes
where the map is given by
It follows that is merely a substitution of the variables in the symmetric functions given by so that
With these considerations at hand we can now investigate the homology of the complex , with its transgression differential from (27). To this end we shall apply the following well known reduction lemma.
Lemma 3.4.
Let be a ring, an -module and be elements. When is a non-zerodivisor on , then there is a canonical isomorphism
for the entire cohomology of the Koszul complexes.
Proof.
See [BH93, Corollary 1.6.13 (b)]. ∎
The ring is freely generated in the elementary symmetric functions in the . Now the transgression differential takes the form
Since the form a regular sequence on the module with quotient , it follows inductively from Lemma 3.4 that
as anticipated.
Let be integers. The case of a Grassmannian
is similar, only that the maximal tori for and its subgroup can be chosen to be the same so that . The difference comes from the Weyl groups. For we again have the full symmetric group , but for the subgroup we find
whose action on respects the partion of the variables into subsets and . We write
for the elementary symmetric polynomials in the respective set of variables. Then is a free polynomial subring in these variables
containing as the invariant subring under arbitrary permutations, i.e. forgetting about the particular partition. It is an elementary exercise in the theory of symmetric functions to verify that in this situation
(31) |
Now the complex in (27) looks as follows, cf. [Bor53, Proposition 31.1]: The differential takes each one of the generators to . These are weighted homogeneous relations in a free graded polynomial ring with variables . From the fact that the cohomology of the associated Koszul complex is finite dimensional, we see that the elements (31) must form a regular sequence on so that the complex is exact except at Koszul degree zero where we find
(32) |
with the weighted homogeneoeus ideal generated by the elements (31).
Remark 3.5.
This model for the cohomology is linked to the geometry of the Grassmannians as follows. Let
be the tautological sequence on . Then modulo we find that is the -th Chern class of the tautological bundle and the -th Chern class of the tautological quotient bundle. The latter are nothing but the -th Segre classes of which gives us precisely the relations (31) by expansion of the product of total Chern classes
in all degrees.
This cohomological model can be simplified further. Let be the Chern classes of the tautological subbundle and those of the tautological quotient bundle. The relations given by the images , i.e. the generators of the ideal are
The first equations can be used to eliminate all of the -variables and express them in terms of . Substituting these into the last equations we obtain polynomials in which we denote by
If we let be the ideal generated by these elements then
(33) |
Moreover, the polynomials satisfy a recurrence relation that can easily be derived from their explicit construction. Writing them in a vector we have
and
(34) |
Comparing this with the construction of the infinite Grassmannian we see the following: Since the cohomology ring of is generated by the Chern classes of the tautological bundle for every and the tautological bundle on restricts to the one on , the pullback in cohomology for the inclusion is given by
where the containment of ideals is confirmed by the recurrence relation (34) above.
3.5. Cohomology of the matrix orbits
This section will entirely consist of the proof of the following:
Proposition 3.6.
Let be integers. The cohomology of the orbit variety is graded isomorphic to the Koszul algebra
over the ring with each a free generator of degree .
We use the Cartan model (27) for . The group in question is with the subgroup
As a maximal torus of this subgroup we choose pairs of diagonal block matrices
with all nontrivial entries . This is contained in the maximal torus of in the obvious way.
We will write for the ring . If we let be the set of Chern roots associated to the subgroup , the ones for and those for , then similar to the case of flag varieties, the ring is the invariant subring of by the action of the group
acting by the permutation of the distinct sets of variables. We set
so that is a free polynomial ring containing as another free polynomial subring.
Since the group is a product, also the exterior algebra in (27) takes the form of a product:
We let be the generators of and those of . With the notation above it is easy to see from the inclusion of maximal tori that the differential of (27) takes these generators to the elements
in and, as already discussed in Remark 3.5, these are precisely the relations between the Chern classes of the tautological sub- and quotient bundles.
We now consider Koszul complexes on associated to various subsets of the generators and . As discussed earlier in Remark 3.5 the elements
form a regular sequence on that can be used to eliminate the variables and . Using the reduction lemma for the homology of Koszul complexes, Lemma 3.4, this reduces the problem to a Koszul complex on the ring
In this quotient, the next relations reduce to
and they form another regular sequence with successive quotient as in Remark 3.5. Consequently, the last relations
all reduce to zero in due to (34) since by assumption . In terms of the identification of the homology of Koszul complexes from Lemma 3.4 this means
where the differentials of the complex in the second last line are all zero so that we may drop the homology functor . To finish the proof of Proposition 3.6 we now set to be equal to for in the last line.
Remark 3.7.
We review the fiber bundle structure
described in Lemma 3.2. Given the explicit descriptions of the cohomology of both the Stiefel manifold and the Grassmannian, we may infer from the proof of Proposition 3.6 that, similar to the case the Hopf’s theorem, the cohomology of is isomorphic to that of a product
despite the fact that the structure of as a fiber bundle is in general non-trivial. By construction, the cohomology classes restrict to the generators of the cohomology of in every fiber. Yet it seems difficult to write down an explicit lift of these elements to the original complex .
Remark 3.8.
It would be nice to have a more geometric understanding of the elements that might, for example, be derived from the tautological sequence
(35) |
on where the denote the tautological quotient bundles on respective Grassmannians for the projections and as in Lemma 3.2 and denotes the tautological section
on , identifying the subbundles with .
4. Betti numbers of smooth links
A hyperplane of codimension in general position will intersect in a non-trivial way whenever . This intersection will have isolated singularity as long as meets the singular locus of only at the origin, i.e. . The real and complex links of codimension of will therefore be smooth within the range
In this section we will be concerned with the cohomology of and for in this range. More precisely, we will show for that for in the above range
(36) | |||||
(37) | |||||
(38) |
where . The left hand sides all agree with the cohomology of in this range for and the above maps are given by the pullback in cohomology for the natural inclusions of the real and complex links into that stratum.
For the complex links the middle Betti number can then be computed from the polar multiplicities using Formula (11). In case this gives a complete description of the classical real and complex links of , see Remark 4.5.
However, besides the case and , we are unable to determine whether or not has torsion. Also, the two middle cohomology groups of can not be computed by our methods for .
4.1. The variation sequence on stratified spaces
Throughout this section, let be an equidimensional reduced complex analytic germ of complex dimension , endowed with a complex analytic Whitney stratification . We will denote by the germ of a holomorphic function with an isolated singularity on in the stratified sense. For a Milnor ball of sufficiently small radius and representatives and of the space and the function we let
be the real link of and
the Milnor fiber of for some . Denote the regular part of by . Then clearly by construction of and
are the regular loci of and , respectively.
Lemma 4.1.
The natural maps in cohomology
are injective for and an isomorphism for .
Proof.
It is well known that we may “inflate” the Milnor-Lê fibration for and identify its total space with an open subset of itself:
See for example [GM88, Part II, Chapter 2.A, Proposition 2.A.3], or [GM88, Part II, Chapter 2.4] for the particular case where is linear.
Since has isolated singularity on it is a stratified submersion on near the boundary of the central fiber. We may therefore identify
and extend the fibration by over to the whole complement of .
The assertion is now a consequence of the variation sequence for the regular loci. It is evident from Thom’s first isotopy lemma that
respects the stratification of induced from . Therefore, the common chain of isomorphisms for the variation sequence
restricts to the regular loci for every . Here, we deliberately identified with the boundary part of the regular locus of . In the last step we used the Künneth formula for pairs of spaces, see e.g. [Hat02, Theorem 3.21]. For a more thorough treatment see also [GM88, Part II, Chapter 2.5].
With these identifications, the long exact sequence of the pair reads
The assertion now follows from the fact that for all which is due to complex stratified Morse theory for non-proper Morse functions, see [GM88, Introduction, Chapter 2.2]. ∎
Remark 4.2.
The cited theorem [GM88, Introduction, Chapter 2.2] is a statement on the relative homology for the smooth locus of a projective algebraic variety and its intersection with a generic hyperplane. The statement can be generalized to germs of complex analytic sets and their intersections with a suitable ball, cf. [GM88, Introduction, Chapter 2.4]. Then one can use complex stratified Morse theory for non-proper Morse functions to study the connectivity of the pair via a Morsification of the squared distance function to the origin. The key observation is that for the regular locus the local Morse datum at a critical point is always -connected. The last statement can easily be derived by induction on dimension from [GM88, Part II, Chapter 3.3, Corollary 1].
Now suppose we are given as above and an admissible sequence of linear forms in the sense of Definition 2.2 and Corollary 2.4. Then we can apply Lemma 4.1 inductively to on :
Proposition 4.3.
Let be an equidimensional reduced complex analytic germ of dimension , and an admissible sequence of linear forms as in Corollary 2.4. Let and be the regular loci of the real and complex links of codimension of . Then for arbitrary the natural maps
are isomorphisms for every and injective for .
Proof.
We proceed by induction on the codimension of the complex links. For this follows directly from Lemma 4.1.
Now suppose the statement holds up to codimension . As already discussed in the proof of Lemma 4.1, the real link can be identified with the boundary of . But the pair is cohomologically -connected due to the LHT and the long exact sequence yields
for and
for the middle part. Since by our induction hypothesis the cohomology groups are all isomorphic for , the first part of the assertion on follows.
For the second part on consider
By construction the Milnor fiber of this function is while is the real link of . All the relevant cohomology groups of have already been determined by our previous considerations so that the remaining statements follow readily from Lemma 4.1 applied to .
∎
4.2. Proof of Formulas (36) – (38)
As remarked earlier, the relevant range for the codimension for the real and complex links and of the generic determinantal variety is
We may assume . Then for these values of the dimension of the complex links does not exceed
Recall that due to the homogeneity of the singularity, the cohomology of the regular part of the classical real link of is given by
according to Proposition 3.6. Now note that the bound on assures that each and every generator is taken to a vanishing cohomology group of a smooth complex link . The formulas (36), (37), and (38) now follow directly from Proposition 4.3.
4.3. The middle cohomology groups
The results of the previous section allow to determine the cohomology below the middle degrees of the real and complex links and of codimension for a purely -dimensional germ , provided so that has isolated singularity and the links are smooth. We shall now discuss how to obtain information on the remaining part of the cohomology and to which extend this is possible.
When the complex link is Stein and the higher cohomology groups vanish due to the LHT. We can use Lefschetz duality (see e.g. [Hat02, Theorem 3.43]) to identify homology with cohomology:
Note that the middle homology group is known to always be free; this is the case even for arbitrary smooth Stein manifolds. The real link is an oriented smooth compact manifold of real dimension and we have Poincaré duality (cf. [Hat02, Theorem 3.30]):
for all . All these cohomology groups sit in the classical variation sequence with its middle part being of particular interest:
We return to the particular case of the generic determinantal singularity . For the smooth complex links we can use the knowledge of the Euler characteristic from the polar multiplicities in Section 2.3, Formula (11) to also determine the rank of the middle cohomology group:
(39) |
Switching from integer to rational coefficients, this allows us to fully compute the rational cohomology, but unfortunately this method does not allow to detect torsion in the middle cohomology group with integer coefficients. However, so far no example of a smooth complex link of a generic determinantal variety is known for which the middle cohomology group does have torsion.
Being an oriented smooth compact manifold of odd real dimension, is always zero and therefore computation of the Euler characteristic does not help in this case; not even the full rational cohomology of can be computed by our methods. It should be noted, however, that there are examples for which torsion appears:
Example 4.4.
Consider the singularity for a generic plane of codimension . This is an isolated normal surface singularity, the simplest one of the “rational triple points” discussed by Tjurina [Tju68]. It was shown in [Zac20] that the so-called Tjurina modification of is smooth and hence a resolution of singularities for . The space is isomorphic to the total space of the bundle
and hence the complex link can be identified with the sphere bundle of . Then a part of the Euler sequence for this bundle reads
But with the canonical generators for , the cup product with the Euler class is simply multiplication by and we find that
(40) |
The complex link , i.e. the “Milnor fiber” in the variation sequence, is known to have middle cohomology ; see e.g. [Zac20]. Since is also free and the map necessarily has rank , it follows that
To conclude this section, we mention one last case that might be of particular interest:
Remark 4.5.
For the generic determinantal varieties all have isolated singularity and therefore the classical real and complex links and are already smooth. In this case we know all the cohomology groups of
which is free Abelian in all degrees. Using the variation sequence we infer that the middle cohomology of can not have torsion: By Poincaré duality also the relative cohomology group to the left is isomorphic to the middle homology group of . Now the latter is known to always be free Abelian for Stein manifolds. Therefore we have
(41) |
We would like to mention one particular consequence of the previous remark. It is well known that on a locally complete intersection the constant sheaf is perverse for the middle perversity; see e.g. [Dim04, Theorem 5.1.20]. Most of the generic determinantal varieties are not complete intersections and we can now show that this algebraic property is also reflected in their topology:
Corollary 4.6.
For , i.e. for non-square matrices, the constant sheaf on the generic determinantal variety, shifted by its dimension, is never a perverse sheaf for the middle perversity.
Proof.
For these values of , and the rank stratification is the minimal Whitney stratification of . Now the constant sheaf can only be perverse (for the middle perversity) if the variety has a certain rectified homological depth, meaning that along every stratum the real link along satisfies
See [HL91, Section 1.1.3], [HL91, Theorem 1.4] for a discussion on rectified homological depth and e.g. the proof of [Dim04, Theorem 5.1.20] for its relation to perversity. For the codimension on the right hand side is
for all values . But according to Remark 4.5 we have
so that the criterion for the perversity given above is violated. ∎
5. Implications for the vanishing topology of smoothable IDS
5.1. Proof of Theorem 1.1
We consider a -miniversal unfolding
of the defining matrix for on parameters . See, for instance, [FKZ21] for the underlying notion of -equivalence and the existence and construction of such miniversal unfoldings. The induced deformation
given by the projection of to the parameter space is versal in the sense that it covers all possible determinantal deformations of coming from this particular choice of a determinantal structure.
Let the discriminant be the set of parameters with singular fibers . For a suitable representative of the unfolding we may choose a Milnor ball around the origin and a polydisc in the parameter space such that
is a smooth fiber bundle of manifolds with boundary with fiber , the smoothing of .
Since for the map
is transverse to the rank stratification implies that does not degenerate on the fiber in the sense that it has constant rank at all points . Therefore the cokernel
presented by is a well defined vector bundle of rank on the fiber over .
Variation of in does not change the fiber up to diffeomorphism. In the same sense, it varies the vector bundle in a way on these fibers, but does not change its isomorphism class as a smooth complex vector bundle.
Due to the versality of , the various deformations of and its smoothing in the proof of the bouquet decomposition (1) in [Zac20] can be realized using piecewise smooth paths in the parameter space . In particular, this leads to a representative of which has an embedding of the complex link . Now it follows from the results in Section 4 that the truncated cohomology of the Grassmannian is generated by the algebra of Segre classes of the tautological quotient bundle. Since by construction the pullback of this bundle to both and is the vector bundle in question, the result follows.
5.2. Proof of Corollary 1.2
Let be a smoothing of the isolated Cohen-Macaulay threefold on some open set on which a perturbation
of the matrix is defined. By definition the canonical sheaf on is given by which can be computed from a free resolution of as an -module. Such a free resolution is provided by the deformation of the resolution of from the Hilbert-Burch theorem. Now it is easy to see from the proof of Theorem 1.1 that the line bundle is presented by the restriction of to , i.e. it is the vector bundle in Theorem 1.1 and the claim follows.
Acknowlegdements
The author wishes to thank Duco van Straten for introducing him to the work of Borel on the cohomology of homogeneous spaces and Sam Hagh Shenas Noshari for further helpful conversations on the topic, Terence Gaffney for discussions on polar varieties and –multiplicities, Xiping Zhang for an exchange on their computation, and James Damon for conversations on the “characteristic cohomology” of determinantal singularities.
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