In mathematics, the adjoint representation (or adjoint action) 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: . For any Lie group, this natural representation is obtained by linearizing (i.e. taking the differential of) the action of G on itself by conjugation. The adjoint representation can be defined for linear algebraic groups over arbitrary fields. Representation theory and Lie group#The Lie algebra associated with a Lie group Let G be a Lie group, and let be the mapping g ↦ Ψg, with Aut(G) the automorphism group of G and Ψg: G → G given by the inner automorphism (conjugation) This Ψ is a Lie group homomorphism. For each g in G, define Adg to be the derivative of Ψg at the origin: where d is the differential and is the tangent space at the origin e (e being the identity element of the group G). Since is a Lie group automorphism, Adg is a Lie algebra automorphism; i.e., an invertible linear transformation of to itself that preserves the Lie bracket. Moreover, since is a group homomorphism, too is a group homomorphism. Hence, the map is a group representation called the adjoint representation of G. If G is an immersed Lie subgroup of the general linear group (called immersely linear Lie group), then the Lie algebra consists of matrices and the exponential map is the matrix exponential for matrices X with small operator norms. Thus, for g in G and small X in , taking the derivative of at t = 0, one gets: where on the right we have the products of matrices. If is a closed subgroup (that is, G is a matrix Lie group), then this formula is valid for all g in G and all X in . Succinctly, an adjoint representation is an isotropy representation associated to the conjugation action of G around the identity element of G.

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Representation theory
Representation theory is a branch of mathematics that studies abstract algebraic structures by representing their elements as linear transformations of vector spaces, and studies modules over these abstract algebraic structures. In essence, a representation makes an abstract algebraic object more concrete by describing its elements by matrices and their algebraic operations (for example, matrix addition, matrix multiplication).
Semisimple Lie algebra
In mathematics, a Lie algebra is semisimple if it is a direct sum of simple Lie algebras. (A simple Lie algebra is a non-abelian Lie algebra without any non-zero proper ideals). Throughout the article, unless otherwise stated, a Lie algebra is a finite-dimensional Lie algebra over a field of characteristic 0. For such a Lie algebra , if nonzero, the following conditions are equivalent: is semisimple; the Killing form, κ(x,y) = tr(ad(x)ad(y)), is non-degenerate; has no non-zero abelian ideals; has no non-zero solvable ideals; the radical (maximal solvable ideal) of is zero.
Cartan subalgebra
In mathematics, a Cartan subalgebra, often abbreviated as CSA, is a nilpotent subalgebra of a Lie algebra that is self-normalising (if for all , then ). 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 . In a finite-dimensional semisimple Lie algebra over an algebraically closed field of characteristic zero (e.g., ), a Cartan subalgebra is the same thing as a maximal abelian subalgebra consisting of elements x such that the adjoint endomorphism is semisimple (i.
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