Schubert calculus explained

In mathematics, Schubert calculus[1] is a branch of algebraic geometry introduced in the nineteenth century by Hermann Schubert in order to solve various counting problems of projective geometry and, as such, is viewed as part of enumerative geometry. Giving it a more rigorous foundation was the aim of Hilbert's 15th problem. It is related to several more modern concepts, such as characteristic classes, and both its algorithmic aspects and applications remain of current interest. The term Schubert calculus is sometimes used to mean the enumerative geometry of linear subspaces of a vector space, which is roughly equivalent to describing the cohomology ring of Grassmannians. Sometimes it is used to mean the more general enumerative geometry of algebraic varieties that are homogenous spaces of simple Lie groups. Even more generally, Schubert calculus is sometimes understood as encompassing the study of analogous questions in generalized cohomology theories.

The objects introduced by Schubert are the Schubert cells,[2] which are locally closed sets in a Grassmannian defined by conditions of incidence of a linear subspace in projective space with a given flag. For further details see Schubert variety.

The intersection theory[3] of these cells, which can be seen as the product structure in the cohomology ring of the Grassmannian, consisting of associated cohomology classes, allowsin particular the determination of cases in which the intersections of cells results in a finite set of points. A key result is that the Schubert cells (or rather, the classes of their Zariski closures, the Schubert cycles or Schubert varieties) span the whole cohomology ring.

The combinatorial aspects mainly arise in relation to computing intersections of Schubert cycles. Lifted from the Grassmannian, which is a homogeneous space, to the general linear group that acts on it, similar questions are involved in the Bruhat decomposition and classification of parabolic subgroups (as block triangular matrices).

Construction

Schubert calculus can be constructed using the Chow ring[3] of the Grassmannian, where the generating cycles are represented by geometrically defined data.[4] Denote the Grassmannian of

k

-planes in a fixed

n

-dimensional vector space

V

as

Gr(k,V)

, and its Chow ring as

A*(Gr(k,V))

. (Note that the Grassmannian is sometimes denoted

Gr(k,n)

if the vector space isn't explicitly given or as

G(k-1,n-1)

if the ambient space

V

and its

k

-dimensional subspaces are replaced by their projectizations.) Choosing an (arbitrary) complete flag

l{V}=(V1\subset\subsetVn-1\subsetVn=V),\dim{V}i=i,i=1,...,n,

to each weakly decreasing

k

-tuple of integers

a=(a1,\ldots,ak)

, where

n-k\geqa1\geqa2\geq\geqak\geq0,

i.e., to each partition of weight

|a|=

k
\sum
i=1

ai,

whose Young diagram fits into the

k x (n-k)

rectangular one for the partition

(n-k)k

, we associate a Schubert variety[1] [2] (or Schubert cycle)

\Sigmaa(l{V})\subsetGr(k,V)

, defined as

\Sigmaa(l{V})=\{w\inGr(k,V):\dim

(V
n-k+i-ai

\capw)\geqifori=1,...,k\}.

This is the closure, in the Zariski topology, of the Schubert cell[1] [2]

Xa(l{V}):=\{w\inGr(k,V):\dim(Vj\capw)=iforalln-k-ai+i\leqj\leqn-k-ai+1+i,1\lej\len\}\subset\Sigmaa(l{V}),

which is used when considering cellular homology instead of the Chow ring. The latter are disjoint affine spaces, of dimension

|a|

, whose union is

Gr(k,V)

.

An equivalent characterization of the Schubert cell

Xa(l{V})

may be given in terms of the dual complete flag

\tilde{l{V}}=(\tilde{V}1\subset\tilde{V}2\subset\tilde{V}n=V),

where

\tilde{V}i:=Vn\backslashVn-i,i=1,...,n(V0:=\emptyset).

Then

Xa(l{V})\subsetGr(k,V)

consists of those

k

-dimensional subspaces

w\subsetV

that have a basis

(\tilde{W}1,...,\tilde{W}k)

consisting of elements

\tilde{W}i\in

\tilde{V}
k+ai-i+1

,i=1,...,k

of the subspaces

\{\tilde{V}
k+ai-i+1

\}i=1,.

Since the homology class

[\Sigmaa(l{V})]\inA*(Gr(k,V))

, called a Schubert class, does not depend on the choice of complete flag

l{V}

, it can be written as

\sigmaa:=[\Sigmaa]\inA*(Gr(k,V)).

It can be shown that these classes are linearly independent and generate the Chow ring as their linear span. The associated intersection theory is called Schubert calculus. For a given sequence

a=(a1,\ldots,aj,0,\ldots,0)

with

aj>0

the Schubert class
\sigma
(a1,\ldots,aj,0,\ldots,0)
is usually just denoted
\sigma
(a1,\ldots,aj)
. The Schubert classes given by a single integer
\sigma
a1
, (i.e., a horizontal partition), are called special classes. Using the Giambelli formula below, all the Schubert classes can be generated from these special classes.

Other notational conventions

In some sources,[1] [2] the Schubert cells

Xa

and Schubert varieties

\Sigmaa

are labelled differently, as

Sλ

and

\bar{S}λ

, respectively, where

λ

is the complementary partition to

a

with parts

λi:=n-k-ak-i+1

,whose Young diagram is the complement of the one for

a

within the

k x (n-k)

rectangular one (reversed, both horizontally and vertically).

Another labelling convention for

Xa

and

\Sigmaa

is

CL

and

\bar{C}L

, respectively, where

L=(L1,...,Lk)\subset(1,...,n)

is the multi-index defined by

Li:=n-k-ai+ik-i+1+i.

The integers

(L1,...,Lk)

are the pivot locations of the representations of elements of

Xa

in reduced matricial echelon form.

Explanation

In order to explain the definition, consider a generic

k

-plane

w\subsetV

. It will have only a zero intersection with

Vj

for

j\leqn-k

, whereas

\dim(Vj\capw)=i

for

j=n-k+i\geqn-k.

For example, in

Gr(4,9)

, a

4

-plane

w

is the solution space of a system of five independent homogeneous linear equations. These equations will generically span when restricted to a subspace

Vj

with

j=\dimVj\leq5=9-4

, in which case the solution space (the intersection of

Vj

with

w

) will consist only of the zero vector. However, if

\dim(Vj)+\dim(w)>n=9

,

Vj

and

w

will necessarily have nonzero intersection. For example, the expected dimension of intersection of

V6

and

w

is

1

, the intersection of

V7

and

w

has expected dimension

2

, and so on.

The definition of a Schubert variety states that the first value of

j

with

\dim(Vj\capw)\geqi

is generically smaller than the expected value

n-k+i

by the parameter

ai

. The

k

-planes

w\subsetV

given by these constraints then define special subvarieties of

Gr(k,n)

.

Properties

Inclusion

There is a partial ordering on all

k

-tuples where

a\geqb

if

ai\geqbi

for every

i

. This gives the inclusion of Schubert varieties

\Sigmaa\subset\Sigmab\iffa\geqb,

showing an increase of the indices corresponds to an even greater specialization of subvarieties.

Dimension formula

A Schubert variety

\Sigmaa

has dimension equal to the weight

|a|=\sumai

of the partition

a

.Alternatively, in the notational convention

Sλ

indicated above, its codimension in

Gr(k,n)

is the weight

|λ|=

kλ
\sum
i

=k(n-k)-|a|.

of the complementary partition

λ\subset(n-k)k

in the

k x (n-k)

dimensional rectangular Young diagram.

This is stable under inclusions of Grassmannians. That is, the inclusion

i(k,:Gr(k,Cn)\hookrightarrowGr(k,Cn+1),Cn=span\{e1,...,en\}

defined, for

w\inGr(k,Cn)

, by

i(k,:w\subsetCn\mapstow\subsetCnCen+1=Cn+1

has the property
*
i
(k,n)

(\sigmaa)=\sigmaa,

and the inclusion

\tilde{i}(k,n):Gr(k,n)\hookrightarrowGr(k+1,n+1)

defined by adding the extra basis element

en+1

to each

k

-plane, giving a

(k+1)

-plane,

\tilde{i}(k,:w\mapstowCen+1\subsetCnCen+1=Cn+1

does as well

*(\sigma
\tilde{i}
a

)=\sigmaa.

Thus, if

Xa\subsetGrk(n)

and

\Sigmaa\subsetGrk(n)

are a cell and a subvariety in the Grassmannian

Grk(n)

, they may also be viewed as a cell

Xa\subsetGr\tilde{k}(\tilde{n})

and a subvariety

\Sigmaa\subsetGr\tilde{k}(\tilde{n})

within the Grassmannian

Gr\tilde{k}(\tilde{n})

forany pair

(\tilde{k},\tilde{n})

with

\tilde{k}\geqk

and

\tilde{n}-\tilde{k}\geqn-k

.

Intersection product

The intersection product was first established using the Pieri and Giambelli formulas.

Pieri formula

In the special case

b=(b,0,\ldots,0)

, there is an explicit formula of the product of

\sigmab

with an arbitrary Schubert class
\sigma
a1,\ldots,ak
given by

\sigmab\sigma

a1,\ldots,ak

=\sum \begin{matrix|c|=|a|+b\\ ai\leqci\leqai-1\end{matrix}}\sigmac,

where

|a|=a1++ak

,

|c|=c1++ck

are the weights of the partitions. This is called the Pieri formula, and can be used to determine the intersection product of any two Schubert classes when combined with the Giambelli formula. For example,

\sigma1\sigma4,2,1=\sigma5,2,1+\sigma4,3,1+\sigma4,2,1,1.

and

\sigma2\sigma4,3=\sigma4,3,2+\sigma4,4,1+\sigma5,3,1+\sigma5,4+\sigma6,3

Giambelli formula

Schubert classes

\sigmaa

for partitions of any length

\ell(a)\leqk

can be expressed as the determinant of a

(k x k)

matrix having the special classes as entries.
\sigma
(a1,\ldots,ak)

=

\begin{vmatrix} \sigma
a1

&

\sigma
a1+1

&

\sigma
a1+2

&&

\sigma
a1+k-1
\\ \sigma
a2-1

&

\sigma
a2

&

\sigma
a2+1

&&

\sigma
a2+k-2
\\ \sigma
a3-2

&

\sigma
a3-1

&

\sigma
a3

&&

\sigma
a3+k-3

\\ \vdots&\vdots&\vdots&\ddots&\vdots

\\ \sigma
ak-k+1

&

\sigma
ak-k+2

&

\sigma
ak-k+3

&&

\sigma
ak

\end{vmatrix}

sa

as determinants in terms of the complete symmetric functions

\{hj:=s(j)\}

.

For example,

\sigma2,2=\begin{vmatrix} \sigma2&\sigma3\\ \sigma1&\sigma2 \end{vmatrix}=

2
\sigma
2

-\sigma1 ⋅ \sigma3

and

\sigma2,1,1=\begin{vmatrix} \sigma2&\sigma3&\sigma4\\ \sigma0&\sigma1&\sigma2\\ 0&\sigma0&\sigma1 \end{vmatrix}.

General case

The intersection product between any pair of Schubert classes

\sigmaa,\sigmab

is given by

\sigmaa\sigmab=\sumc

c
c
ab

\sigmac,

where

c
\{c
ab

\}

are the Littlewood-Richardson coefficients.[5] The Pieri formula is a special case of this, when

b=(b,0,...,0)

has length

\ell(b)=1

.

Relation with Chern classes

There is an easy description of the cohomology ring, or the Chow ring, of the Grassmannian

Gr(k,V)

using the Chern classes of two natural vector bundles over

Gr(k,V)

. We have the exact sequence of vector bundles over

Gr(k,V)

0\toT\to\underline{V}\toQ\to0

where

T

is the tautological bundle whose fiber, over any element

w\inGr(k,V)

is the subspace

w\subsetV

itself,

\underline{V}:=Gr(k,V) x V

is the trivial vector bundle of rank

n

, with

V

as fiber and

Q

is the quotient vector bundle of rank

n-k

, with

V/w

as fiber. The Chern classes of the bundles

T

and

Q

are

ci(T)=

i\sigma
(-1)
(1)i

,

where

(1)i

is the partition whose Young diagram consists of a single column of length

i

and

ci(Q)=\sigmai.

The tautological sequence then gives the presentation of the Chow ring as

A*(Gr(k,V))=

Z[c1(T),\ldots,ck(T),c1(Q),\ldots,cn-k(Q)]
(c(T)c(Q)-1)

.

Gr(2,4)

One of the classical examples analyzed is the Grassmannian

Gr(2,4)

since it parameterizes lines in

P3

. Using the Chow ring

A*(Gr(2,4))

, Schubert calculus can be used to compute the number of lines on a cubic surface.

Chow ring

The Chow ring has the presentation

A*(Gr(2,4))=

Z[\sigma1,\sigma1,1,\sigma2]
((1-\sigma1+\sigma1,1)(1+\sigma1+\sigma2)-1)

and as a graded Abelian group[6] it is given by

\begin{align} A0(Gr(2,4))&=Z1\\ A2(Gr(2,4))&=Z\sigma1\\ A4(Gr(2,4))&=Z\sigma2Z\sigma1,1\\ A6(Gr(2,4))&=Z\sigma2,1\\ A8(Gr(2,4))&=Z\sigma2,2\\ \end{align}

Lines on a cubic surface

Recall that a line in

P3

gives a dimension

2

subspace of

A4

, hence an element of

G(1,3)\congGr(2,4)

. Also, the equation of a line can be given as a section of

\Gamma(G(1,3),T*)

. Since a cubic surface

X

is given as a generic homogeneous cubic polynomial, this is given as a generic section

s\in\Gamma(G(1,3),Sym3(T*))

. A line

L\subsetP3

is a subvariety of

X

if and only if the section vanishes on

[L]\inG(1,3)

. Therefore, the Euler class of

Sym3(T*)

can be integrated over

G(1,3)

to get the number of points where the generic section vanishes on

G(1,3)

. In order to get the Euler class, the total Chern class of

T*

must be computed, which is given as

c(T*)=1+\sigma1+\sigma1,1

The splitting formula then reads as the formal equation

\begin{align} c(T*)&=(1+\alpha)(1+\beta)\\ &=1+\alpha+\beta+\alpha\beta \end{align},

where

c(l{L})=1+\alpha

and

c(l{M})=1+\beta

for formal line bundles

l{L},l{M}

. The splitting equation gives the relations

\sigma1=\alpha+\beta

and

\sigma1,1=\alpha\beta

.

Since

Sym3(T*)

can be viewed as the direct sum of formal line bundles

Sym3(T*)=l{L}(l{L}l{M}) ⊕ (l{L} ⊗ l{M})l{M}

whose total Chern class is

c(Sym3(T*))=(1+3\alpha)(1+2\alpha+\beta)(1+\alpha+2\beta)(1+3\beta),

it follows that

3(T
\begin{align} c
4(Sym

*))&=3\alpha(2\alpha+\beta)(\alpha+2\beta)3\beta\\ &=9\alpha\beta(2(\alpha+\beta)2+\alpha\beta)\\ &=9\sigma1,1

2
(2\sigma
1

+\sigma1,1)\\ &=27\sigma2,2, \end{align}

using the fact that

\sigma1,1

2
\sigma
1

=\sigma2,1\sigma1=\sigma2,2

and

\sigma1,1\sigma1,1=\sigma2,2.

Since

\sigma2,2

is the top class, the integral is then

\intG(1,3)27\sigma2,2=27.

Therefore, there are

27

lines on a cubic surface.

See also

References

Notes and References

  1. Kleiman . S.L.. Laksov . Dan . Steven Kleiman . Dan Laksov. Schubert Calculus . American Mathematical Society. American Mathematical Monthly . 79. 10 . 1972 . 0377-9017 . 10.1080/00029890.1972.11993188 . 1061-1082 .
  2. Book: Fulton, William . William Fulton (mathematician). Young Tableaux. With Applications to Representation Theory and Geometry, Chapt. 9.4 . 1997 . London Mathematical Society Student Texts . 35 . Cambridge University Press . Cambridge, U.K.. 9780521567244 . 10.1017/CBO9780511626241 .
  3. Book: Fulton . William . William Fulton (mathematician) . Intersection Theory . . Berlin, New York . 978-0-387-98549-7 . 1644323 . 1998 .
  4. Book: 3264 and All That. 132, section 4.1; 200, section 6.2.1.
  5. Book: Fulton, William . William Fulton (mathematician). Young Tableaux. With Applications to Representation Theory and Geometry, Chapt. 5 . 1997 . London Mathematical Society Student Texts . 35 . Cambridge University Press . Cambridge, U.K.. 9780521567244 . 10.1017/CBO9780511626241 .
  6. Book: Katz, Sheldon. Sheldon Katz . Enumerative Geometry and String Theory. 96.