ConceptComplete

Compact Lie Groups - Examples and Constructions

Explicit examples of compact Lie groups demonstrate the diversity of structures while illustrating unifying principles. These examples form the foundation for applications in geometry, topology, and physics.

Example

The torus Tn=S1Γ—β‹―Γ—S1⏟nΒ timesT^n = \underbrace{S^1 \times \cdots \times S^1}_{n \text{ times}}

The nn-torus is the fundamental abelian compact Lie group. It appears as:

  • Maximal torus in any rank-nn compact group
  • Classifying space for Zn\mathbb{Z}^n lattices
  • Phase space in classical mechanics

Lie algebra: tn=Rn\mathfrak{t}^n = \mathbb{R}^n (tangent space at identity)

Example

Special unitary group SU(n)SU(n):

Matrices A∈Mn(C)A \in M_n(\mathbb{C}) satisfying Aβˆ—A=IA^* A = I and det⁑(A)=1\det(A) = 1. This is:

  • Simply connected for all nn (universal cover of PSU(n)PSU(n))
  • Dimension n2βˆ’1n^2 - 1
  • Rank nβˆ’1n - 1
  • Compact (unitary matrices have norm-bounded entries)

Fundamental group: Ο€1(SU(n))=0\pi_1(SU(n)) = 0 (simply connected)

Example

Special orthogonal group SO(n)SO(n):

Real orthogonal matrices with determinant 1. Properties:

  • Connected for nβ‰₯2n \geq 2
  • Simply connected for nβ‰₯3n \geq 3: Ο€1(SO(n))=0\pi_1(SO(n)) = 0
  • For SO(3)SO(3): Ο€1(SO(3))=Z/2Z\pi_1(SO(3)) = \mathbb{Z}/2\mathbb{Z} (double covered by SU(2)SU(2))
  • Dimension n(nβˆ’1)2\frac{n(n-1)}{2}

Physical interpretation: rotations in nn-dimensional space.

Remark

The spin group Spin(n)Spin(n) is the universal cover of SO(n)SO(n), a double cover for nβ‰₯3n \geq 3. For n=3n = 3: Spin(3)=SU(2)Spin(3) = SU(2), the group of unit quaternions.

Example

Symplectic group Sp(n)Sp(n) (compact form):

Quaternionic unitary matrices. Can be realized as: Sp(n)=U(2n)∩Sp2n(C)Sp(n) = U(2n) \cap Sp_{2n}(\mathbb{C}) where Sp2n(C)Sp_{2n}(\mathbb{C}) preserves a complex symplectic form.

Properties:

  • Dimension n(2n+1)n(2n+1)
  • Rank nn
  • Simply connected

Exceptional compact groups:

Example

The exceptional compact Lie groups corresponding to G2,F4,E6,E7,E8G_2, F_4, E_6, E_7, E_8:

  • G2G_2: Compact form of 14-dimensional exceptional algebra (automorphisms of octonions)
  • F4F_4: 52-dimensional, related to exceptional Jordan algebra
  • E6,E7,E8E_6, E_7, E_8: Simply connected compact groups of dimensions 78, 133, 248

These appear in:

  • String theory (heterotic E8Γ—E8E_8 \times E_8)
  • Exceptional holonomy manifolds
  • Moonshine phenomena

Product constructions: The product GΓ—HG \times H of compact groups is compact. For example:

  • U(1)Γ—SU(n)β†’U(n)U(1) \times SU(n) \to U(n) (covering with finite kernel)
  • SO(m)Γ—SO(n)β†’SO(m+n)SO(m) \times SO(n) \to SO(m+n) (block diagonal embedding)
Remark

Homogeneous spaces: Quotients G/HG/H for compact GG and closed subgroup HH yield important geometric spaces:

  • Spheres: Sn=SO(n+1)/SO(n)S^n = SO(n+1)/SO(n)
  • Complex projective space: CPn=SU(n+1)/(SU(n)Γ—U(1))\mathbb{CP}^n = SU(n+1)/(SU(n) \times U(1))
  • Grassmannians: Gr(k,n)=U(n)/(U(k)Γ—U(nβˆ’k))Gr(k,n) = U(n)/(U(k) \times U(n-k))

These examples demonstrate that compact Lie groups naturally appear wherever continuous symmetries of bounded geometric objects arise.