A nonassociative algebra obeyed by objects such as the Lie bracket and Poisson bracket. Elements f, g, and h of a Lie algebra satisfy
[f,f]==0
(1)
[f g,h]==[f,h] [g,h],
(2)

and
[f,[g,h]] [g,[h,f]] [h,[f,g]]==0
(3)

(the Jacobi identity). The relation [f,f]==0 implies
[f,g]==-[g,f].
(4)

For characteristic not equal to two, these two relations are equivalent.

The binary operation of a Lie algebra is the bracket
[fg,h]==f[g,h] [f,h]g.
(5)

An associative algebra A with associative product xy can be made into a Lie algebra A^- by the Lie product
[x,y]==xy-yx.
(6)

Every Lie algebra L is isomorphic to a subalgebra of some A^- where the associative algebra A may be taken to be the linear operators over a vector space V (the Poincaré-Birkhoff-Witt theorem; Jacobson 1979, pp. 159-160). If L is finite dimensional, then V can be taken to be finite dimensional (Ado’s theorem for characteristic p==0; Iwasawa’s theorem for characteristic p!=0).

The classification of finite dimensional simple Lie algebras over an algebraically closed field of characteristic 0 can be accomplished by (1) determining matrices called Cartan matrices corresponding to indecomposable simple systems of roots and (2) determining the simple algebras associated with these matrices (Jacobson 1979, p. 128). This is one of the major results in Lie algebra theory, and is frequently accomplished with the aid of diagrams called Dynkin diagrams.

Btw, Miro, koho by takato matematika nebavila? :)