Yang–Mills equation

The Euler–Lagrange equation for the Yang–Mills functional, expressed as a covariant divergence-free condition on curvature.
Yang–Mills equation

Let PMP\to M be a principal GG-bundle over an oriented Riemannian manifold, and let AA be a with curvature FAF_A.

Theorem/Definition (Yang–Mills equation)

The Euler–Lagrange equation for the is

dA(FA)=0. d_A(*F_A)=0.

Here dAd_A is the covariant exterior derivative on Ad(P)\mathrm{Ad}(P)-valued forms, which extends the on ordinary forms and satisfies the Bianchi identity $d_A F_A=0.

A connection AA satisfying dA(FA)=0d_A(*F_A)=0 is called a Yang–Mills connection.

Examples

  1. Flat connections. If FA=0F_A=0 then dA(FA)=0d_A(*F_A)=0 automatically.
  2. Abelian reduction. For G=U(1)G=U(1), the equation becomes d(F)=0d(*F)=0, the source-free Maxwell equation for the curvature 2-form FF.
  3. Instantons in dimension 4. On a 4-manifold, any connection with self-dual or anti-self-dual curvature satisfies the Yang–Mills equation because FA=±FA*F_A=\pm F_A and the Bianchi identity gives dA(FA)=±dAFA=0d_A(*F_A)=\pm d_AF_A=0.