Schubert polynomial explained

In mathematics, Schubert polynomials are generalizations of Schur polynomials that represent cohomology classes of Schubert cycles in flag varieties. They were introduced by and are named after Hermann Schubert.

Background

described the history of Schubert polynomials.

The Schubert polynomials

ak{S}w

are polynomials in the variables

x1,x2,\ldots

depending on an element

w

of the infinite symmetric group

Sinfty

of all permutations of

\N

fixing all but a finite number of elements. They form a basis for the polynomial ring

\Z[x1,x2,\ldots]

in infinitely many variables.

The cohomology of the flag manifold

Fl(m)

is

\Z[x1,x2,\ldots,xm]/I,

where

I

is the ideal generated by homogeneous symmetric functions of positive degree. The Schubert polynomial

ak{S}w

is the unique homogeneous polynomial of degree

\ell(w)

representing the Schubert cycle of

w

in the cohomology of the flag manifold

Fl(m)

for all sufficiently large

m.

Properties

w0

is the permutation of longest length in

Sn

then
ak{S}
w0

=

n-1
x
1
n-2
x
2

1
x
n-1

\partialiak{S}w=

ak{S}
wsi
if

w(i)>w(i+1)

, where

si

is the transposition

(i,i+1)

and where

\partiali

is the divided difference operator taking

P

to

(P-siP)/(xi-xi+1)

.

Schubert polynomials can be calculated recursively from these two properties. In particular, this implies that

ak{S}w=

\partial
w-1w0
n-1
x
1
n-2
x
2

1
x
n-1
.

Other properties are

ak{S}id=1

si

is the transposition

(i,i+1)

, then
ak{S}
si

=x1++xi

.

w(i)<w(i+1)

for all

ir

, then

ak{S}w

is the Schur polynomial

sλ(x1,\ldots,xr)

where

λ

is the partition

(w(r)-r,\ldots,w(2)-2,w(1)-1)

. In particular all Schur polynomials (of a finite number of variables) are Schubert polynomials.

As an example

ak{S}24531(x)=x1

2
x
3

x4

2
x
1

x3x4

2
x
1
2
x
3

x4x2.

Multiplicative structure constants

Since the Schubert polynomials form a

Z

-basis, there are unique coefficients
\alpha
c
\beta\gamma
such that

ak{S}\betaak{S}\gamma=\sum\alpha

\alpha
c
\beta\gamma

ak{S}\alpha.

These can be seen as a generalization of the Littlewood−Richardson coefficients described by the Littlewood–Richardson rule.For algebro-geometric reasons (Kleiman's transversality theorem of 1974), these coefficients are non-negative integers and it is an outstanding problem in representation theory and combinatorics to give a combinatorial rule for these numbers.

Double Schubert polynomials

Double Schubert polynomials

ak{S}w(x1,x2,\ldots,y1,y2,\ldots)

are polynomials in two infinite sets of variables, parameterized by an element w of the infinite symmetric group, that becomes the usual Schubert polynomials when all the variables

yi

are

0

.

The double Schubert polynomial

ak{S}w(x1,x2,\ldots,y1,y2,\ldots)

are characterized by the properties

ak{S}w(x1,x2,\ldots,y1,y2,\ldots)=\prod\limitsi(xi-yj)

when

w

is the permutation on

1,\ldots,n

of longest length.

\partialiak{S}w=

ak{S}
wsi
if

w(i)>w(i+1).

The double Schubert polynomials can also be defined as

ak{S}w(x,y)

=\sum
w=v-1uand\ell(w)=\ell(u)+\ell(v)

ak{S}u(x)ak{S}v(-y).

Quantum Schubert polynomials

introduced quantum Schubert polynomials, that have the same relation to the (small) quantum cohomology of flag manifolds that ordinary Schubert polynomials have to the ordinary cohomology.

Universal Schubert polynomials

introduced universal Schubert polynomials, that generalize classical and quantum Schubert polynomials. He also described universal double Schubert polynomials generalizing double Schubert polynomials.

See also