What is Lie algebra? A 5 Minute Introduction

Click For Summary
SUMMARY

A Lie algebra is a mathematical structure that serves as the generator of a Lie group, representing the tangent space around the identity element of the group. It features a binary, bi-linear, anti-symmetric operation known as commutation, where the commutator of two basis vectors results in a linear combination of the algebra's basis vectors, ensuring closure. Lie algebras are essential for studying Lie groups, particularly in representation theory, although caution is necessary as isomorphic algebras do not guarantee isomorphic groups, exemplified by SO(3) and SU(2).

PREREQUISITES
  • Understanding of Lie groups and their properties
  • Familiarity with linear algebra concepts, particularly vector spaces
  • Knowledge of commutative and non-commutative algebra
  • Basic grasp of representation theory in mathematics
NEXT STEPS
  • Study the properties of Lie groups and their relationship with Lie algebras
  • Explore the Jacobi identity and its implications in Lie algebra theory
  • Learn about the representation theory of Lie algebras
  • Investigate the differences between SO(3) and SU(2) in the context of Lie algebras
USEFUL FOR

Mathematicians, physicists, and students interested in advanced algebraic structures, particularly those focusing on the study of symmetry and group theory.

Messages
19,864
Reaction score
10,850
Definition/Summary
A Lie algebra (“Lee”) is a set of generators of a Lie group. It is a basis of the tangent space around a Lie group’s identity element, the space of differences between elements close to the identity element and the identity element itself.
Lie algebras include a binary, bi-linear, anti-symmetric operation: commutation. The commutator of two basis vectors is a linear combination of the algebra’s basis vectors (closure).
Lie algebras are valuable as a proxy for Lie groups. They are often more convenient to study than the groups that they generate, and much of what is known about Lie groups has come from studying their algebras, like their representation theory. One has to be careful about global properties, however; groups with isomorphic algebras need not be isomorphic, such as SO(3) and SU(2).
Equations
Commutator:
For matrices: [A,B] = A.B – B.A
For operators: [A,B](X) = A(B(X)) – B(A(X))
The commutator satisfies the Jacobi identity:
[A,[B,C]] + [B,[C,A]] +...

Continue reading...
 
Last edited:
Physics news on Phys.org

Similar threads

  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 5 ·
Replies
5
Views
4K
  • · Replies 15 ·
Replies
15
Views
3K
  • · Replies 20 ·
Replies
20
Views
4K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 19 ·
Replies
19
Views
3K
  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 0 ·
Replies
0
Views
3K