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Lie Algebras

The Lie algebra $\mathfrak{g}$ is the tangent space to the Lie group $G$ at the identity. It is a vector space equipped with a bracket $[\cdot,\cdot]$ that captures the non-commutativity of the group. For physicists, the generators are the observables — charge, angular momentum, color — and their commutation relations determine the entire representation theory.

Key Concepts

Lie Algebra g\mathfrak{g}
The tangent space TeGT_e G at the identity of a Lie group, equipped with the Lie bracket [X,Y][X,Y]. As a vector space, dimg=dimG\dim\mathfrak{g} = \dim G.
Generator
Ta=ig/αaα=0T^a = -i\,\partial g / \partial\alpha_a|_{\alpha=0}. For unitary groups, generators are Hermitian. The {Ta}\{T^a\} are a basis for g\mathfrak{g}.
Structure Constants
fabcf^{abc} defined by [Ta,Tb]=ifabcTc[T^a, T^b] = if^{abc}T^c. Totally antisymmetric: fabc=fbacf^{abc}=-f^{bac}. Completely characterize the Lie algebra.
Rank
The dimension of the maximal abelian subalgebra (Cartan subalgebra). For su(n)\mathfrak{su}(n): rank =n1= n-1. Equals the number of simultaneously diagonalizable generators.
Killing Form
B(X,Y)=Tr(adXadY)B(X,Y) = \text{Tr}(\text{ad}_X \circ \text{ad}_Y). Negative definite for compact semisimple Lie algebras. Used to raise/lower structure constant indices.

Key Equations

Lie Algebra Commutation Relations
[Ta,Tb]=ifabcTc[T^a,\, T^b] = i\,f^{abc}\,T^c
The structure constants fabcf^{abc} are antisymmetric and satisfy the Jacobi identity.
Jacobi Identity
[A,[B,C]]+[B,[C,A]]+[C,[A,B]]=0[A,[B,C]] + [B,[C,A]] + [C,[A,B]] = 0
Automatically satisfied in any Lie algebra. Corresponds to the associativity constraint.
Normalization (Fundamental Rep)
Tr(TaTb)=12δab\mathrm{Tr}(T^a T^b) = \tfrac{1}{2}\,\delta^{ab}
Standard normalization for generators in the fundamental representation of SU(n)SU(n).
Worked Example

Structure Constants of su(2)\mathfrak{su}(2)

Problem

The generators of SU(2)SU(2) are Ti=σi/2T^i = \sigma^i/2. Using the known Pauli matrix commutator [σi,σj]=2iεijkσk[\sigma^i, \sigma^j] = 2i\varepsilon^{ijk}\sigma^k, find f123f^{123}.

Solution

[T1,T2]=[σ1/2,σ2/2]=14[σ1,σ2]=14(2iσ3)=iσ32=iT3[T^1, T^2] = [\sigma^1/2,\, \sigma^2/2] = \tfrac{1}{4}[\sigma^1,\sigma^2] = \tfrac{1}{4}(2i\sigma^3) = \tfrac{i\sigma^3}{2} = iT^3.

From the definition [Ta,Tb]=ifabcTc[T^a,T^b] = if^{abc}T^c: [T1,T2]=if123T3[T^1,T^2] = if^{123}T^3.

Comparing: iT3=if123T3iT^3 = if^{123}T^3, so f123=1f^{123} = 1.

More generally, fijk=εijkf^{ijk} = \varepsilon^{ijk} for su(2)\mathfrak{su}(2) (the Levi-Civita symbol).

Answer f123=1f^{123} = 1.
Practice

Exercises

7 problems
1 of 7

For SU(2)SU(2) generators with fijk=εijkf^{ijk}=\varepsilon^{ijk}, what is f231f^{231}?

2 of 7

The rank of su(n)\mathfrak{su}(n) is n1n-1. What is the rank of su(5)\mathfrak{su}(5)?

3 of 7

For Ti=σi/2T^i = \sigma^i/2, the normalization gives Tr(TaTb)=12δab\mathrm{Tr}(T^a T^b) = \frac{1}{2}\delta^{ab}. What is 2Tr((T1)2)2\,\mathrm{Tr}((T^1)^2)?

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4 of 7

How many generators does SU(2)SU(2) have?

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5 of 7

Structure constants are totally antisymmetric: fabc=fbacf^{abc} = -f^{bac}. If f123=1f^{123} = 1 for su(2)\mathfrak{su}(2), what is f321f^{321}?

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6 of 7

How many generators does SU(3)SU(3) have? (SU(n)SU(n) has n21n^2-1 generators.)

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7 of 7

How many diagonal Gell-Mann matrices are there? (Equals the rank of su(3)\mathfrak{su}(3).)

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Key Takeaways

  • The Lie algebra g\mathfrak{g} is the tangent space at the identity of GG. It is a vector space with a bracket [,][\cdot,\cdot] encoding the local structure of the group.
  • Structure constants fabcf^{abc} defined by [Ta,Tb]=ifabcTc[T^a,T^b]=if^{abc}T^c are totally antisymmetric and satisfy the Jacobi identity.
  • For su(2)\mathfrak{su}(2): fijk=εijkf^{ijk}=\varepsilon^{ijk} (angular momentum algebra). For su(3)\mathfrak{su}(3): 28 independent non-zero fabcf^{abc}.
  • The rank of su(n)\mathfrak{su}(n) is n1n-1: the number of simultaneously diagonalizable generators (conserved, commuting charges).