In this article, I will introduce Lie algebra, which essentially is related to the Poisson brackets we studied before.

Definition

Lie Algebra

For a vector space V defined on field F , a Lie algebra is tuple V,[,] , where [,] is a bilinear mapping: [,]:V×VV , s.t. all of the 3 following conditions are fulfilled:

  1. Bilinearity:
[ax+by,z]=a[x,z]+b[y,z],x,y,zV.
  1. Anti-Symmetry:
[x,x]=0,xV.

If the field F does not have character 2 , we also have

[x,y]=[y,x],x,yV.
  1. Jacobi Identity:
[x,[y,z]]+[y,[z,x]]+[z,[x,y]]=0,x,y,zV.

Comment: The character of a field F is defined as:

char(F)=argminn>0(1+1+...+1n times=0),

if n= , char(F):=0 .

Why Poisson brackets have Lie algebra structure

What is Poisson bracket

See the link.