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Lie Groups

A Lie group is simultaneously a group and a smooth manifold: its elements can be continuously varied, and both the multiplication and inverse maps are smooth. Lie groups describe continuous symmetries in physics — rotations, Lorentz boosts, gauge transformations — and their dimension (the number of continuous parameters) directly determines how many conserved quantities and gauge bosons arise.

Key Concepts

Lie Group
A group GG that is also a smooth manifold, with group multiplication G×G→GG\times G\to G and inversion G→GG\to G both smooth maps. Examples: SO(n)SO(n), SU(n)SU(n), U(n)U(n), GL(n,R)GL(n,\mathbb{R}).
Dimension
The dimension of GG as a manifold: the number of real parameters needed to specify a group element. Equals the number of independent generators in the Lie algebra.
Compactness
SO(n)SO(n), SU(n)SU(n), U(n)U(n) are compact (closed and bounded as matrix groups). Compact groups have finite-dimensional unitary representations. GL(n,R)GL(n,\mathbb{R}) is not compact.
Simply Connected
SU(n)SU(n) is simply connected (π1=0\pi_1=0). SO(n)SO(n) for n≥2n\geq2 is not — its fundamental group is Z2\mathbb{Z}_2, which is why spinors require SU(2)SU(2) rather than SO(3)SO(3).
Double Cover
There is a 2-to-1 group homomorphism SU(2)→SO(3)SU(2) \to SO(3). The two elements ±I∈SU(2)\pm I \in SU(2) both map to the identity in SO(3)SO(3). Spin-12\frac{1}{2} particles require the full SU(2)SU(2).

Key Equations

Dimensions of Classical Lie Groups
dim⁡SO(n)=n(n−1)2,dim⁡SU(n)=n2−1,dim⁡U(n)=n2\dim SO(n) = \frac{n(n-1)}{2}, \quad \dim SU(n) = n^2-1, \quad \dim U(n) = n^2
The most-used dimension formulas in particle physics.
Exponential Map
g(α)=exp⁡ ⁣(i αa Ta)∈Gg(\alpha) = \exp\!\left(i\,\alpha_a\, T^a\right) \in G
Every element near the identity is an exponential of a Lie algebra element. The TaT^a are generators and αa\alpha_a are real parameters.
Worked Example

Dimension of SO(4)SO(4)

Problem

How many independent parameters are needed to specify a rotation in 4-dimensional Euclidean space? In other words, what is dim⁡SO(4)\dim SO(4)?

Solution

SO(n)SO(n) consists of n×nn\times n orthogonal matrices with det =1=1. The independent degrees of freedom are the number of independent planes of rotation.

Use dim⁡SO(n)=n(n−1)/2\dim SO(n) = n(n-1)/2.

dim⁡SO(4)=4×32=6\dim SO(4) = \frac{4 \times 3}{2} = 6
Answer dim⁡SO(4)=6\dim SO(4) = 6.
Practice

Exercises

7 problems
1 of 7

What is dim⁡SU(4)\dim SU(4)? Use dim⁡SU(n)=n2−1\dim SU(n) = n^2 - 1.

2 of 7

What is dim⁡SO(5)\dim SO(5)? Use dim⁡SO(n)=n(n−1)/2\dim SO(n) = n(n-1)/2.

3 of 7

What is dim⁡U(4)\dim U(4)? Use dim⁡U(n)=n2\dim U(n) = n^2.

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4 of 7

What is dim⁡SU(2)\dim SU(2)?

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5 of 7

The Lorentz group SO(3,1)SO(3,1) has the same number of generators as SO(4)SO(4). What is dim⁡SO(4)\dim SO(4)?

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6 of 7

What is dim⁡SU(3)\dim SU(3)?

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7 of 7

What is dim⁡SU(5)\dim SU(5)? (SU(5)SU(5) is the simplest candidate grand unified theory group.)

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Key Takeaways

  • A Lie group is a smooth manifold that is also a group. Its dimension equals the number of independent continuous parameters — and the number of generators.
  • dim⁡SO(n)=n(n−1)/2\dim SO(n)=n(n-1)/2, dim⁡SU(n)=n2−1\dim SU(n)=n^2-1, dim⁡U(n)=n2\dim U(n)=n^2. Memorize these — they appear constantly in particle physics.
  • SU(2)SU(2) is the simply-connected double cover of SO(3)SO(3). Spin-12\frac{1}{2} particles are representations of SU(2)SU(2), not SO(3)SO(3).
  • The number of gauge bosons of a gauge theory with symmetry group GG equals dim⁡G\dim G: 1 photon (U(1)U(1)), 3 weak bosons (SU(2)SU(2)), 8 gluons (SU(3)SU(3)).