About polynomiality of the Poisson semicentre for parabolic subalgebras

Similar documents
A relative version of Kostant s theorem

Defining equations for some nilpotent varieties

(Finite) W-algebras associated to truncated current Lie algebras

On the singular elements of a semisimple Lie algebra and the generalized Amitsur-Levitski Theorem

arxiv: v1 [math.rt] 14 Nov 2007

Lecture Notes Introduction to Cluster Algebra

BLOCKS IN THE CATEGORY OF FINITE-DIMENSIONAL REPRESENTATIONS OF gl(m n)

On the Irreducibility of the Commuting Variety of the Symmetric Pair so p+2, so p so 2

GEOMETRIC STRUCTURES OF SEMISIMPLE LIE ALGEBRAS

Symplectic varieties and Poisson deformations

PART I: GEOMETRY OF SEMISIMPLE LIE ALGEBRAS

Representations of semisimple Lie algebras

19-23 JULY Abstracts

L(C G (x) 0 ) c g (x). Proof. Recall C G (x) = {g G xgx 1 = g} and c g (x) = {X g Ad xx = X}. In general, it is obvious that

On the Harish-Chandra Embedding

Lie Algebras of Finite and Affine Type

Classification of semisimple Lie algebras

The Cartan Decomposition of a Complex Semisimple Lie Algebra

16.2. Definition. Let N be the set of all nilpotent elements in g. Define N

Birational geometry and deformations of nilpotent orbits

Lecture 4: LS Cells, Twisted Induction, and Duality

Eigenvalue problem for Hermitian matrices and its generalization to arbitrary reductive groups

Max-Planck-Institut für Mathematik Bonn

k=0 /D : S + S /D = K 1 2 (3.5) consistently with the relation (1.75) and the Riemann-Roch-Hirzebruch-Atiyah-Singer index formula

Dirac Cohomology, Orbit Method and Unipotent Representations

Primitive Ideals and Unitarity

Math 249B. Geometric Bruhat decomposition

Background on Chevalley Groups Constructed from a Root System

INTRODUCTION TO LIE ALGEBRAS. LECTURE 10.

Lectures on the Orbit Method

1.4 Solvable Lie algebras

Workshop on B-stable ideals and nilpotent orbits

Lecture 11 The Radical and Semisimple Lie Algebras

Spherical varieties and arc spaces

A Study on Kac-Moody Superalgebras

SEMISIMPLE LIE GROUPS

The Morozov-Jacobson Theorem on 3-dimensional Simple Lie Subalgebras

Homogeneous para-kähler Einstein manifolds. Dmitri V. Alekseevsky

Representation Theory and Orbital Varieties. Thomas Pietraho Bowdoin College

SYMMETRIC SUBGROUP ACTIONS ON ISOTROPIC GRASSMANNIANS

Highest-weight Theory: Verma Modules

INTRODUCTION TO LIE ALGEBRAS. LECTURE 7.

LECTURE 20: KAC-MOODY ALGEBRA ACTIONS ON CATEGORIES, II

5 Quiver Representations

Reducibility of generic unipotent standard modules

Lie Algebras. Shlomo Sternberg

Subsystems, Nilpotent Orbits, and Weyl Group Representations

Sheets of Symmetric Lie Algebras and Slodowy Slices

Quaternionic Complexes

Comparison for infinitesimal automorphisms. of parabolic geometries

SPHERICAL UNITARY REPRESENTATIONS FOR REDUCTIVE GROUPS

Root systems. S. Viswanath

ON THE MAXIMAL PRIMITIVE IDEAL CORRESPONDING TO THE MODEL NILPOTENT ORBIT

Notes on nilpotent orbits Computational Theory of Real Reductive Groups Workshop. Eric Sommers

Subcomplexes in Curved BGG Sequences

On the unitary dual of classical and exceptional real split groups. Alessandra Pantano, University of California, Irvine MIT, March, 2010

LIE ALGEBRAS: LECTURE 7 11 May 2010

Weyl s Character Formula for Representations of Semisimple Lie Algebras

Longest element of a finite Coxeter group

THE SEMISIMPLE SUBALGEBRAS OF EXCEPTIONAL LIE ALGEBRAS

Category O and its basic properties

Representations Are Everywhere

Toshiaki Shoji (Nagoya University) Character sheaves on a symmetric space and Kostka polynomials July 27, 2012, Osaka 1 / 1

Intersection of stable and unstable manifolds for invariant Morse functions

Classification of discretely decomposable A q (λ) with respect to reductive symmetric pairs UNIVERSITY OF TOKYO

2.4 Root space decomposition

Notes on D 4 May 7, 2009

On some conjectures on VOAs

Vanishing Ranges for the Cohomology of Finite Groups of Lie Type

Lecture 5: Admissible Representations in the Atlas Framework

LECTURE 4: REPRESENTATION THEORY OF SL 2 (F) AND sl 2 (F)

A CHARACTERIZATION OF DYNKIN ELEMENTS

Differential Geometry, Lie Groups, and Symmetric Spaces

LECTURE 25-26: CARTAN S THEOREM OF MAXIMAL TORI. 1. Maximal Tori

Polar orbitopes. Leonardo Biliotti, Alessandro Ghigi and Peter Heinzner. Università di Parma - Università di Milano Bicocca - Ruhr Universität Bochum

Talk at Workshop Quantum Spacetime 16 Zakopane, Poland,

Representations of algebraic groups and their Lie algebras Jens Carsten Jantzen Lecture III

Rigid Schubert classes in compact Hermitian symmetric spaces

LECTURE 11: SOERGEL BIMODULES

The local geometry of compact homogeneous Lorentz spaces

EKT of Some Wonderful Compactifications

arxiv: v1 [math.rt] 28 Jan 2009

NEW REALIZATIONS OF THE MAXIMAL SATAKE COMPACTIFICATIONS OF RIEMANNIAN SYMMETRIC SPACES OF NON-COMPACT TYPE. 1. Introduction and the main results

LECTURE 3: TENSORING WITH FINITE DIMENSIONAL MODULES IN CATEGORY O

arxiv: v4 [math.rt] 9 Jun 2017

Pacific Journal of Mathematics

THE p-smooth LOCUS OF SCHUBERT VARIETIES. Let k be a ring and X be an n-dimensional variety over C equipped with the classical topology.

LIE ALGEBRAS: LECTURE 3 6 April 2010

On some combinatorial aspects of Representation Theory

Lemma 1.3. The element [X, X] is nonzero.

The Poisson Embedding Problem

Weyl orbits of π-systems in Kac-Moody algebras

Topics in Representation Theory: Roots and Weights

The Geometry of Conjugacy Classes of Nilpotent Matrices

Weyl Group Representations and Unitarity of Spherical Representations.

TITS SYSTEMS, PARABOLIC SUBGROUPS, PARABOLIC SUBALGEBRAS. Alfred G. Noël Department of Mathematics Northeastern University Boston, MA

ON THE CONSTRUCTIVE INVERSE PROBLEM IN DIFFERENTIAL GALOIS THEORY #

Weyl group representations on zero weight spaces

Cartan s Criteria. Math 649, Dan Barbasch. February 26

Combinatorics and geometry of E 7

Transcription:

About polynomiality of the Poisson semicentre for parabolic subalgebras University of Saint-Etienne, ICJ, LYON - France The Canicular Days - Haifa - July 2017 - Celebrating A. Joseph s 75th birthday

Aim. Let a be a complex algebraic Lie algebra and A be its adjoint group. Denote by S(a) the symmetric algebra of a. We want to study the polynomiality of the algebra of invariants S(a) A = S(a) a =: Y (a), especially when a is a (truncated) parabolic subalgebra. Results where polynomiality holds (the list is not exhaustive!). When a is semisimple, then Y (a) is polynomial in rank a homogeneous generators (Chevalley, 1968). When a = p Λ is the canonical truncation of a (bi)-parabolic subalgebra of g simple of type A or C, then Y (a) is polynomial in ind p Λ rank g homogeneous generators (Joseph - F-M, 2005). When a = g x (centralizer of x g), with g simple of type A or C and x is any nilpotent element of g or when g is simple (outside type E 8 ) and x is the highest root vector of g, then Y (a) is polynomial in rank g homogeneous generators (Panyushev - Premet - Yakimova, 2007).

Where polynomiality holds. When a = p (g/p) a (parabolic contraction) and p a parabolic subalgebra of g simple of type A or C, or when p = b the Borel subalgebra of g simple of any type, then Y (a) is polynomial in rank g homogeneous generators (Panyushev - Yakimova, 2012, 2013).

Counter-examples. When a = p Λ = g x is the centralizer of the highest root vector in g simple of type E 8, then Y (a) is not polynomial (Yakimova, 2007). When a = g x is the centralizer of some x g with g simple of type D 7, then Y (a) is not polynomial (Charbonnel - Moreau, 2016).

The case of parabolic subalgebras. From now on, we focus on a parabolic subalgebra p of a complex simple Lie algebra g. Set, for λ p, S(p) λ := {s S(p) x p, (ad x)(s) = λ(x) s}. Then the Poisson semicentre of S(p) is Sy(p) = λ p S(p) λ, while the Poisson centre is Y (p) = S(p) 0. We have that Sy(p) = S(p) p where p = [p, p] and Y (p) Sy(p). If p = g, then Y (g) = Sy(g). Otherwise Y (p) = C Sy(p). Denote by p Λ the canonical truncation of p, that is, the largest subalgebra of p which vanishes on each weight of Sy(p). Then Sy(p Λ ) = Y (p Λ ) = Sy(p).

Notations. Fix a Cartan subalgebra h of g simple, and a set π of simple roots. The set of roots of g is denoted by = + and the root subspace of g corresponding to α is denoted by g α. Then g = n h n, where n, resp. n, is the largest nilpotent subalgebra of g corresponding to, resp. to +. Fix a subset π π and denote by + π the subset of + generated by π. Let p = n h n π be a parabolic subalgebra of g where n π is the largest nilpotent subalgebra of g corresponding to + π. Then the canonical truncation p Λ of p verifies p Λ = n h Λ n π with h Λ h.

Lower and upper bounds for Sy(p). For any h-module M = ν h M ν with finite dimensional weight subspaces M ν, we define its formal character ch M = ν h dim M ν e ν. Theorem 1 (Joseph - F-M, 2005) There are two polynomial algebras A and B, which are also h-modules, such that ch A ch Sy(p) ch B. Moreover if ch A = ch B, then Sy(p) is a polynomial algebra. It is in particular the case when g is simple of type A or C.

Criterion There is a combinatorial criterion, which establishes when ch A = ch B, so when Sy(p) = Y (p Λ ) is a polynomial algebra. In particular, the bounds coincide for any parabolic subalgebra of g simple of type A or C. When g is simple of type B or D and p is a maximal parabolic subalgebra, then the bounds coincide in roughly half of the cases. Note that this criterion is not a necessary condition for polynomiality of Sy(p). For instance, when p = b, then the criterion does not hold in g simple of type outside A or C, but Sy(b ) is a polynomial algebra (Joseph, 1977).

The Kostant slice Theorem 2 (Kostant, 1963) Assume that g is a complex simple Lie algebra. Then there exists a principal sl 2 -triple (x, h, y) with h h, x, y regular nilpotent in g, such that [h, x] = x and [h, y] = y and we have the following. Restriction of functions gives an algebra isomorphism Y (g) R[y + g x ] where R[y + g x ] is the algebra of regular functions on the affine variety y + g x. The degree of each homogeneous generator of Y (g) is equal to one plus the eigenvalue of ad h on each element of a basis of g x. Every G-orbit in G(y + g x ) meets y + g x transversally at exactly one point and G(y + g x ) = g (the affine subspace y + g x is called an affine slice to the coadjoint action of g).

Adapted pair When the algebraic Lie algebra a is not semisimple, there exists no principal sl 2 -triple in general in a. Definition 3 (Joseph, 2007) An adapted pair for a is a pair (h, y) a a, with h ad-semisimple, y regular in a (that is, the coadjoint orbit A.y is of minimal codimension, the index of a) and (ad h)(y) = y. Remarks 4 Adapted pairs were constructed for all truncated (bi)parabolic subalgebras in g simple of type A (Joseph, 2008). Adapted pairs need not exist (for instance for b Λ in g simple of type B, D, E, F, G).

An improved upper bound. Lemma 5 (Joseph, 2008) Assume that there exists an adapted pair (h, y) h Λ p Λ for the canonical truncation p Λ of p such that y = γ S x γ with x γ g γ \ {0}, S + π and that S hλ is a basis for h Λ. Then there exists an improved upper bound b such that ch Sy(p) b. Moreover if equality holds, then restriction of functions gives an isomorphism of algebras Sy(p) R[y + V ] where (ad p Λ )(y) V = p Λ and V is an h-stable vector space. Such an affine subspace y + V is called a Weierstrass section or an algebraic slice.

Theorem 6 (Joseph - Shafrir, 2010) Assume that Sy(p) = Y (p Λ ) is a polynomial algebra in l := ind p Λ generators and that p Λ admits an adapted pair (h, y) h Λ p Λ. Then y + V is a Weierstrass section and it is also an affine slice to the coadjoint action of p Λ (where V is an h-stable complement of (ad p Λ )(y) in p Λ ). If {m i } l i=1 are the eigenvalues of ad h on a basis of V, then {m i + 1} l i=1 are the degrees of the generators of Y (p Λ). In particular, m i 0.

Maximal parabolic subalgebras. This is a joint work with Polyxeni Lamprou. From now on, we focus on maximal parabolic subalgebras p of g simple of type B or D. That is, p = n h n π with π = π \ {α s }. In this case the canonical truncation p Λ of p is such that p Λ = n h n π with h = h [p, p]. By the criterion of Theorem 1, we obtain that Sy(p) is a polynomial algebra when s is odd (with Bourbaki s labeling). Then it remains the case s even, which we will treat by constructing an adapted pair for p Λ and then use Lemma 5, showing that the improved upper bound is reached.

Constructing an adapted pair. Definition 7 Let γ. An Heisenberg set Γ γ of centre γ is a subset of such that 1 γ Γ γ 2 for all α Γ γ \ {γ} there exists α Γ γ such that α + α = γ. Example 0.1 Let = i be a root system, i irreducible root systems and β i the unique highest root of i. Take ( i ) βi := {α i (α, β i ) = 0} and decompose it into irreducible root systems ij with highest roots β ij. Continuing we obtain a set of strongly orthogonal positive roots β K, indexed by elements K N N 2. The sets H βk := {α K (α, β K ) > 0} are Heisenberg sets of centre β K.

A criterion of regularity. For A, denote by g A := α A g α with g α the root subspace of g corresponding to α. Let S be a subset of + π. We choose for all γ S an Heisenberg set Γ γ + π such that all Γ γ s are disjoint. We set O = γ S Γ0 γ (with Γ0 γ = Γ γ \ {γ}) and o = g O.

A criterion of regularity. Lemma 8 Assume that 1 y = γ S x γ, with x γ g γ \ {0} for all γ S. 2 + π = γ S Γ γ T. 3 T = ind p Λ. 4 S hλ is a basis for h Λ. 5 The restriction of Φ y : g g C defined by Φ y (x, x ) = K(y, [x, x ]) (with K the Killing form of g) to o o is non-degenerate. Then y is regular in p Λ and (h, y) is an adapted pair for p Λ (where h h Λ is defined by γ(h) = 1 for all γ S).

A criterion of non-degeneracy. We set S = S + S S m with S +, resp. S, being the subset of S containing those γ S such that Γ γ +, resp. Γ γ π. Set O ± = γ S ± Γ0 γ, Om = γ S m Γ0 γ and O = O+ O O m. Lemma 9 (Generalization of a lemma of Joseph.) Assume that 1 y = γ S x γ, with x γ g γ \ {0} for all γ S. 2 S hλ is a basis for h Λ. 3 If α Γ 0 γ, with γ S +, is such that there exists β O +, with α + β S, then β Γ 0 γ and α + β = γ. 4 If α Γ 0 γ, with γ S, is such that there exists β O, with α + β S, then β Γ 0 γ and α + β = γ. 5 Additional technical conditions for all α O such that there exists β O m, with α + β S. Then the restriction of Φ y to o o is non-degenerate.

Example for B 6 with π = π \ {α 4 }. We choose S = {β 1 = ε 1 + ε 2, β 2 = β 2 α 4 = ε 3 + ε 5, ε 4, β = β + α 3 = ε 3 ε 1, β = ε 5 ε 6 } T = {α 1, β 2, α 3, α 3 + α 4, α 5 } (roots in blue) β 1 positive roots β 2 ε 4 negative roots β β

Example for D 6 with π = π \ {α 4 }. We choose S = {β 1 = ε 1 + ε 2, β 2 = β 2 α 4 = ε 3 + ε 5, β = β + α 3 = ε 3 ε 1, γ 1 = ε 4 + ε 6, γ 2 = ε 4 ε 6 } T = {α 1, β 2, α 3, α 3 + α 4, α 5 } (roots in blue) β 1 positive roots β 2 γ 1 γ 2 negative roots β

Polynomiality of Sy(p) for a maximal parabolic subalgebra p. Theorem 10 (F-M - Lamprou, arxiv 2017) Let p be any maximal parabolic subalgebra of a simple Lie algebra g of type B, D or E 6. Then Sy(p) is a polynomial algebra and there exists a Weierstrass section (given by an adapted pair for the canonical truncation p Λ ) which is also an affine slice to the coadjoint action of p Λ.

Remarks 11 For the cases when lower and upper bounds ch A and ch B of Theorem 1 coincide, we have constructed an adapted pair for p Λ (F-M - Lamprou, 2016) (in this case, the subset S m = ). Then we apply Theorem 6. When lower and upper bounds of Theorem 1 donnot coincide, we have also constructed an adapted pair for p Λ (in this case, adapted pairs are more complicated to construct than in the previous case, and in particular the subset S m and then the additional conditions of Lemma 9 are needed). Then we have computed the improved upper bound b and have shown that b = ch A. Applying Lemma 5, we conclude that Sy(p) is a polynomial algebra, whose degrees of generators can be computed by Theorem 6. For type E 6, when lower and upper bound donnot coincide, an adapted pair was found by computer calculations.

Further. For other parabolic subalgebras when the bounds in Theorem 1 donnot coincide, we hope to find an adapted pair (h, y) for the canonical truncation p Λ.

The strategy. Theorem 12 (Joseph - F-M, 2016) Every second element of an adapted pair for the canonical truncation p Λ of a (bi)parabolic subalgebra of g simple of type A is the restriction to p Λ of a regular nilpotent element of g. In particular, this gives an element w of the Weyl group of g which sends the set π of simple roots of g to a new system of simple roots. The previous theorem is motivated by the following theorem. Theorem 13 (Joseph, 2011) Thanks to an element of the Weyl group which is roughly the square root of the longest element of the Weyl group of g, there is a combinatorial receipt which gives Weierstrass sections for the Borel subalgebra of g (for almost all simple Lie algebras g).

Example Now assume that g is simple of type B n and embed g in sl 2n+1. Let p be a maximal parabolic subalgebra of g and consider the adapted pair (h, y) for p Λ we have constructed. Then applying the method of Theorem 12 in type A, one may compute a regular nilpotent element y of g such that y is its restriction to p Λ. This provides a new set of simple roots π and then an element of the Weyl group of g which sends π to π. One may hope to generalize such an element of the Weyl group to other parabolic subalgebras of g, which are not maximal and then get an adapted pair for p Λ, for example when π = π \ {α s, α s+2 }, with s even.