Lie Algebra

A vector space with a bilinear bracket operation that is antisymmetric and satisfies the Jacobi identity.
Lie Algebra

A Lie algebra is a g\mathfrak{g} (typically over R\mathbb{R} or C\mathbb{C}) equipped with a bilinear map

[ , ]:g×gg, [\ ,\ ]:\mathfrak{g}\times\mathfrak{g}\to\mathfrak{g},

called the , such that for all X,Y,ZgX,Y,Z\in\mathfrak{g}:

  1. Alternating / antisymmetry: [X,X]=0[X,X]=0 (equivalently [X,Y]=[Y,X][X,Y]=-[Y,X]).
  2. Jacobi identity: [X,[Y,Z]]+[Y,[Z,X]]+[Z,[X,Y]]=0. [X,[Y,Z]]+[Y,[Z,X]]+[Z,[X,Y]]=0.

Examples

  • Any associative algebra becomes a Lie algebra with commutator [A,B]=ABBA[A,B]=AB-BA, e.g. matrix Lie algebras gl(n,R)\mathfrak{gl}(n,\mathbb{R}).
  • The space of on a manifold with the commutator bracket.
  • An is one with [X,Y]=0[X,Y]=0 for all X,YX,Y.

Maps and structure

A structure-preserving map is a ; bijective ones are .

Important substructures include , , and the .

Many classification notions are defined in terms of the bracket, such as , , , , and Lie algebras.