Regular element of a Lie algebra

Last updated

In mathematics, a regular element of a Lie algebra or Lie group is an element whose centralizer has dimension as small as possible.

Contents

Basic case

In the specific case of matrices over an algebraically closed field (such as the complex numbers), an element is regular if and only if its Jordan normal form contains a single Jordan block for each eigenvalue. In that case, the centralizer is the set of polynomials of degree less than evaluated at the matrix , and therefore the centralizer has dimension (but it is not necessarily an algebraic torus).

If the matrix is diagonalisable, then it is regular if and only if there are different eigenvalues. To see this, notice that will commute with any matrix that stabilises each of its eigenspaces. If there are different eigenvalues, then this happens only if is diagonalisable on the same basis as ; in fact is a linear combination of the first powers of , and the centralizer is an algebraic torus of complex dimension (real dimension ); since this is the smallest possible dimension of a centralizer, the matrix is regular. However if there are equal eigenvalues, then the centralizer is the product of the general linear groups of the eigenspaces of , and has strictly larger dimension, so that is not regular.

For a connected compact Lie group , the regular elements form an open dense subset, made up of -conjugacy classes of the elements in a maximal torus which are regular in . The regular elements of are themselves explicitly given as the complement of a set in , a set of codimension-one subtori corresponding to the root system of . Similarly, in the Lie algebra of , the regular elements form an open dense subset which can be described explicitly as adjoint -orbits of regular elements of the Lie algebra of , the elements outside the hyperplanes corresponding to the root system. [1]

Definition

Let be a finite-dimensional Lie algebra over an infinite field. [2] For each , let

be the characteristic polynomial of the adjoint endomorphism of . Then, by definition, the rank of is the least integer such that for some and is denoted by . [3] For example, since for every x, is nilpotent (i.e., each is nilpotent by Engel's theorem) if and only if .

Let . By definition, a regular element of is an element of the set . [3] Since is a polynomial function on , with respect to the Zariski topology, the set is an open subset of .

Over , is a connected set (with respect to the usual topology), [4] but over , it is only a finite union of connected open sets. [5]

A Cartan subalgebra and a regular element

Over an infinite field, a regular element can be used to construct a Cartan subalgebra, a self-normalizing nilpotent subalgebra. Over a field of characteristic zero, this approach constructs all the Cartan subalgebras.

Given an element , let

be the generalized eigenspace of for eigenvalue zero. It is a subalgebra of . [6] Note that is the same as the (algebraic) multiplicity [7] of zero as an eigenvalue of ; i.e., the least integer m such that in the notation in § Definition. Thus, and the equality holds if and only if is a regular element. [3]

The statement is then that if is a regular element, then is a Cartan subalgebra. [8] Thus, is the dimension of at least some Cartan subalgebra; in fact, is the minimum dimension of a Cartan subalgebra. More strongly, over a field of characteristic zero (e.g., or ), [9]

A regular element in a Cartan subalgebra of a complex semisimple Lie algebra

For a Cartan subalgebra of a complex semisimple Lie algebra with the root system , an element of is regular if and only if it is not in the union of hyperplanes . [10] This is because: for ,

This characterization is sometimes taken as the definition of a regular element (especially when only regular elements in Cartan subalgebras are of interest).

Notes

  1. Sepanski, Mark R. (2006). Compact Lie Groups. Springer. p. 156. ISBN   978-0-387-30263-8.
  2. Editorial note: the definition of a regular element over a finite field is unclear.
  3. 1 2 3 Bourbaki 1981 , Ch. VII, § 2.2. Definition 2.
  4. Serre 2001 , Ch. III, § 1. Proposition 1.
  5. Serre 2001 , Ch. III, § 6.
  6. This is a consequence of the binomial-ish formula for ad.
  7. Recall that the geometric multiplicity of an eigenvalue of an endomorphism is the dimension of the eigenspace while the algebraic multiplicity of it is the dimension of the generalized eigenspace.
  8. Bourbaki 1981 , Ch. VII, § 2.3. Theorem 1.
  9. Bourbaki 1981 , Ch. VII, § 3.3. Theorem 2.
  10. Procesi 2007 , Ch. 10, § 3.2.

Related Research Articles

In the mathematical field of representation theory, a weight of an algebra A over a field F is an algebra homomorphism from A to F, or equivalently, a one-dimensional representation of A over F. It is the algebra analogue of a multiplicative character of a group. The importance of the concept, however, stems from its application to representations of Lie algebras and hence also to representations of algebraic and Lie groups. In this context, a weight of a representation is a generalization of the notion of an eigenvalue, and the corresponding eigenspace is called a weight space.

Adjoint representation

In mathematics, the adjoint representation of a Lie group G is a way of representing the elements of the group as linear transformations of the group's Lie algebra, considered as a vector space. For example, if G is , the Lie group of real n-by-n invertible matrices, then the adjoint representation is the group homomorphism that sends an invertible n-by-n matrix to an endomorphism of the vector space of all linear transformations of defined by: .

In the mathematical theory of compact Lie groups a special role is played by torus subgroups, in particular by the maximal torus subgroups.

In mathematics, the Cartan decomposition is a decomposition of a semisimple Lie group or Lie algebra, which plays an important role in their structure theory and representation theory. It generalizes the polar decomposition or singular value decomposition of matrices. Its history can be traced to the 1880s work of Élie Cartan and Wilhelm Killing.

In mathematics, a Kac–Moody algebra is a Lie algebra, usually infinite-dimensional, that can be defined by generators and relations through a generalized Cartan matrix. These algebras form a generalization of finite-dimensional semisimple Lie algebras, and many properties related to the structure of a Lie algebra such as its root system, irreducible representations, and connection to flag manifolds have natural analogues in the Kac–Moody setting.

Cartan subalgebra Nilpotent subalgebra of a Lie algebra


In mathematics, a Cartan subalgebra, often abbreviated as CSA, is a nilpotent subalgebra of a Lie algebra that is self-normalising. They were introduced by Élie Cartan in his doctoral thesis. It controls the representation theory of a semi-simple Lie algebra over a field of characteristic .

Semisimple Lie algebra Direct sum of simple Lie algebras

In mathematics, a Lie algebra is semisimple if it is a direct sum of simple Lie algebras.

Solvable Lie algebra

In mathematics, a Lie algebra is solvable if its derived series terminates in the zero subalgebra. The derived Lie algebra of the Lie algebra is the subalgebra of , denoted

Verma modules, named after Daya-Nand Verma, are objects in the representation theory of Lie algebras, a branch of mathematics.

In mathematics, specifically the theory of Lie algebras, Lie's theorem states that, over an algebraically closed field of characteristic zero, if is a finite-dimensional representation of a solvable Lie algebra, then stabilizes a flag ; "stabilizes" means for each and i.

Hermitian symmetric space Manifold with inversion symmetry

In mathematics, a Hermitian symmetric space is a Hermitian manifold which at every point has an inversion symmetry preserving the Hermitian structure. First studied by Élie Cartan, they form a natural generalization of the notion of Riemannian symmetric space from real manifolds to complex manifolds.

In mathematics, the Weyl character formula in representation theory describes the characters of irreducible representations of compact Lie groups in terms of their highest weights. It was proved by Hermann Weyl. There is a closely related formula for the character of an irreducible representation of a semisimple Lie algebra. In Weyl's approach to the representation theory of connected compact Lie groups, the proof of the character formula is a key step in proving that every dominant integral element actually arises as the highest weight of some irreducible representation. Important consequences of the character formula are the Weyl dimension formula and the Kostant multiplicity formula.

In mathematics, the Jordan–Chevalley decomposition, named after Camille Jordan and Claude Chevalley, expresses a linear operator as the sum of its commuting semisimple part and its nilpotent part. The multiplicative decomposition expresses an invertible operator as the product of its commuting semisimple and unipotent parts. The decomposition is easy to describe when the Jordan normal form of the operator is given, but it exists under weaker hypotheses than the existence of a Jordan normal form. Analogues of the Jordan-Chevalley decomposition exist for elements of linear algebraic groups, Lie algebras, and Lie groups, and the decomposition is an important tool in the study of these objects.

In mathematics, a toral subalgebra is a Lie subalgebra of a general linear Lie algebra all of whose elements are semisimple. Equivalently, a Lie algebra is toral if it contains no nonzero nilpotent elements. Over an algebraically closed field, every toral Lie algebra is abelian; thus, its elements are simultaneously diagonalizable.

Index of a Lie algebra

In algebra, let g be a Lie algebra over a field K. Let further be a one-form on g. The stabilizer gξ of ξ is the Lie subalgebra of elements of g that annihilate ξ in the coadjoint representation. The index of the Lie algebra is

In mathematics, symmetric cones, sometimes called domains of positivity, are open convex self-dual cones in Euclidean space which have a transitive group of symmetries, i.e. invertible operators that take the cone onto itself. By the Koecher–Vinberg theorem these correspond to the cone of squares in finite-dimensional real Euclidean Jordan algebras, originally studied and classified by Jordan, von Neumann & Wigner (1934). The tube domain associated with a symmetric cone is a noncompact Hermitian symmetric space of tube type. All the algebraic and geometric structures associated with the symmetric space can be expressed naturally in terms of the Jordan algebra. The other irreducible Hermitian symmetric spaces of noncompact type correspond to Siegel domains of the second kind. These can be described in terms of more complicated structures called Jordan triple systems, which generalize Jordan algebras without identity.

In mathematics, Lie group–Lie algebra correspondence allows one to study Lie groups, which are geometric objects, in terms of Lie algebras, which are linear objects. In this article, a Lie group refers to a real Lie group. For the complex and p-adic cases, see complex Lie group and p-adic Lie group.

Glossary of Lie groups and Lie algebras Wikipedia glossary

This is a glossary for the terminology applied in the mathematical theories of Lie groups and Lie algebras. For the topics in the representation theory of Lie groups and Lie algebras, see Glossary of representation theory. Because of the lack of other options, the glossary also includes some generalizations such as quantum group.

In abstract algebra, specifically the theory of Lie algebras, Serre's theorem states: given a root system , there exists a finite-dimensional semisimple Lie algebra whose root system is the given .

Representation theory of semisimple Lie algebras

In mathematics, the representation theory of semisimple Lie algebras is one of crowning achievements of the theory of Lie groups and Lie algebras. The theory was worked out mainly by E. Cartan and H. Weyl and because of that, the theory is also known as the Cartan–Weyl theory. The theory gives the structural description and classification of a finite-dimensional representation of a semisimple Lie algebra ; in particular, it gives a way to parametrize irreducible finite-dimensional representations of a semisimple Lie algebra, the result known as the theorem of the highest weight.

References