Differential Operators and Invariant Theory Will Traves Colorado State University

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Differential Operators and Invariant Theory
Will Traves
Department of Mathematics
United States Naval Academy
SIAM Conference on Applied Algebraic Geometry
Colorado State University
04 August 2013
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Outline
Background on invariant theory and Grassmannians
Differential operators on Grassmannians
Conjecture inspired by a Hilbert series calculation
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Invariant Theory
Given a k × n matrix M filled with variables,


x11 x12 . . . x1n

..
..  ,
M =  ...
.
. 
xk1 xk2 . . . xkn
we let SLk act on the left by matrix multiplication.
C[Mk,n ] = C[x11 , . . . , xkn ]
C[Mk,n ]SLk = polys invariant on SLk orbits of full rank matrices
= C[G(k, n)]
G(k , n): affine cone over variety param k-planes in n-space
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Some obvious invariants
SLk acts by multiplication on the left so it acts on each column of


x11 . . . x1k . . . x1n

..
..  ,
M =  ...
.
. 
xk1 . . . xkk
. . . xkn
simultaneously.
The k × k subdeterminants are invariant because
det(σN) = det(σ) det(N) = 1 det(N).
Denote the k × k minor involving columns I1 , . . . , Ik by
[I] = [I1 . . . Ik ].
This is a polynomial of degree k in the variables xij .
det(N) = [12 . . . k]
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First Fundamental Theorem of Invariant Theory
The First Fundamental Theorem of Invariant Theory
The k × k minors [I] generate the ring of invariants C[Mk,n ]SLk .
The coordinate ring of the Grassmannian C[G(k, n)] = C[Mk,n ]SLk
is called the bracket algebra.
The variables (the minors [I]) are the Plücker coordinates.
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Second Fundamental Theorem of Invariant Theory
The 2nd Fundamental Theorem of Invariant Theory
The generators of C[Mk,n ]SLk satisfy the Plücker relations – quadratic
relations involving the brackets.
Example
When k = 2 and n = 4 all the Plücker relations are multiples of
[12][34] − [13][24] + [14][23] = 0.
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SLk invariants of V n and its dual
Shift from C[Mk,n ] = C[V n ] to C[V n ⊕ (V ∗ )n ]
Coordinates on (V ∗ ) are ξ1` , . . . , ξk` with hξi` , xj`0 i = δij δ``0 .
SLk acts on the ξij by the contragredient representation
If σ ∈ SLk acts on C[V ] by A then σ acts on C[V ∗ ] by (A−1 )T
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Some invariants




x11 . . . x1n
ξ11 . . . ξ1n




..
..
M=
 M∗ = 

.
.
xk1 . . . xkn
ξk1 . . . ξkn
Define: |J| = |J1 . . . Jk | = k × k minor of columns J1 . . . Jk of M ∗
Inner product of a vector in V and a vector in V ∗ is SLk -invariant
New invariants: hiji = inner product of i th column of M with j th
column of M ∗ .
In coordinates: hiji =
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Pk
`=1 x`i ξ`j
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First Fundamental Theorem of Invariant Theory
First Fundamental Theorem of Invariant Theory
The invariants [I], |J| and hiji generate the ring C[V n ⊕ (V ∗ )n ]SLk .
The theory of invariants came into
existence about the middle of the
nineteenth century somewhat like
Minerva: a grown-up virgin, mailed in
the shining armor of algebra, she
sprang forth from Cayley’s Jovian
head. (Weyl, 1939)
H. Weyl
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Second Fundamental Theorem of Invariant Theory
Second Fundamental Theorem of Invariant Theory
The relations among the [I], |J| and hiji are:
1.
2.
3.
4.
5.
Plücker relations on V : [I] [I 0 ]
Plücker relations
on V ∗ : |J| |J 0 |
P
hiji w/ [I] : Pi [Ii ]hiji
hiji w/ |J|: j hiji|Jj |
dethIJi = [I]|J|.
Example
If [I] = [134], |J| = |235| then


h12i h13i h15i
det h32i h33i h35i = [134] |235|
h42i h43i h45i
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The Weyl algebra
The ring of differential operators on Ck is the Weyl algebra
D(Ck ) = D(C[x1 , . . . , xk ]) = Chx1 , . . . , xk , ∂1 , . . . , ∂k i
Product Rule:
∂i = ∂/∂xi ⇒ ∂i xj = xj ∂i + δij
Filtration by order: x1 ∂1 ∂2 + ∂1 − 3x2 has order 2
Symbol map: D(Ck ) −→ GrD(Ck ) = C[x1 , . . . , xk , ξ1 , . . . , ξk ]
θ 7−→ θ mod lower order terms
∂i
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7−→ ξi
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The group action on D(C[Mk ,n ])
We are interested in the operators on Mk,n = V n .
Write R = C[Mk,n ] = C[V n ]
SLk acts on each variable ∂ij in the same way it acts on ξij (A−1 )T
Gr [D(R)SLk ] = [GrD(R)]SLk = C[V n ⊕ (V ∗ )n ]SLk
Write D = D(R). Lifts of generators for Gr [D SLk ] generate D SLk .
1st Fundamental Theorem for D SLk [T-]
The generators of D SLk have the form [I], |J| and hiji, where ξij is
replaced by ∂ij .
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2nd Fundamental Theorem for D SLk
2nd Fundamental Theorem for D SLk [T-]
The relations among the [I], |J| and hiji are:
1.
2.
3.
4.
5.
Plücker relations on V : [I] [I 0 ]
Plücker relations
on V ∗ : |J| |J 0 |
P
hiji w/ [I] : Pi hiji[Ii ]
hiji w/ |J|: j hiji|Jj |
dethIJi = [I]|J|.
Example (Capelli’s Relation)
The fifth relation needs to be interpreted as Capelli’s relation:
replace hkki with hkki+ (index of k in [I] - 1)


h12i h13i
h15i
det  h32i h33i+1 h35i  = [134]|235|.
h42i h43i
h45i
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Differential Operators on Grassmannians
Rings of differential operators on singular varieties are often hard to
describe.
SLk
Restriction map π∗ : D SLk = D(Mk,n )SLk −→ D(Mk,n
) = D(G(k , n))
Theorem (T-, based on work of Schwarz)
The map π∗ is surjective. So D(G(k , n)) is generated by the restriction
of the operators [I], |J|, and hiji.
Theorem (Schwarz)
The kernel of π∗ is (Dslk )SLk , a two-sided ideal in D SLk .
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Example: D(G(2, 4))
The kernel of π∗ is just (D(C[M2,4 ])slk )SLk
sl2 = Trace zero matrices (generated by E12 , E21 , E11 − E22 ).
Each acts as a derivation on C[M2,4 ]: g12 , g21 , g11 − g22 .
These derivations are eigenvectors of the torus action for the
maximal torus sitting in SL2 . Their images form a regular
sequence in GrD(G(2, 4)).
Reduction to torus action (technical) gives
H(GrD(G(2, 4)), t) =
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1 + 18t 2 + 65t 4 + 65t 6 + 18t 8 + t 10
.
(1 − t 2 )10
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Gorenstein?
Theorem (T-)
GrD(G(2, 4)) is Gorenstein. Moreover, GrD(G(2, n)) is Gorenstein for
n ≤ 16.
Stanley: Enough to check that GrD(G(2, 4)) is Cohen-Macaulay.
Hochster-Roberts Theorem: GrD SL2 is CM.
GrD(G(2, 4)) is CM since it is a quotient of GrD SL2 by a regular
sequence.
Conjecture
The graded rings GrD(G(k, n)) are always Gorenstein.
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