Let GG be a Lie group with Lie algebra g\mathfrak{g}. The assigns to each g∈Gg\in G an automorphism Adg:g→g\mathrm{Ad}_g:\mathfrak{g}\to\mathfrak{g}. The coadjoint action is the action of GG on the dual g∗\mathfrak{g}^* (canonically analogous to a fiber of a ) defined by

Adg∗:g∗→g∗,Adg∗(λ):=λ∘Adg−1.\mathrm{Ad}^*_g:\mathfrak{g}^*\to\mathfrak{g}^*, \qquad \mathrm{Ad}^*_g(\lambda) := \lambda\circ \mathrm{Ad}_{g^{-1}}.
Equivalent characterizations

Equivalently, Adg∗\mathrm{Ad}^*_g is characterized by the pairing identity

⟨Adg∗λ, X⟩=⟨λ, Adg−1X⟩(λ∈g∗, X∈g).\langle \mathrm{Ad}^*_g\lambda,\, X\rangle = \langle \lambda,\, \mathrm{Ad}_{g^{-1}}X\rangle \quad (\lambda\in\mathfrak{g}^*,\, X\in\mathfrak{g}).

The assignment g↦Adg∗g\mapsto \mathrm{Ad}^*_g is a smooth group homomorphism G→GL(g∗)G\to \mathrm{GL}(\mathfrak{g}^*).

Examples
  1. Abelian groups. If GG is abelian, then Ad\mathrm{Ad} is trivial, hence Ad∗\mathrm{Ad}^* is also trivial: Adg∗=id\mathrm{Ad}^*_g=\mathrm{id} for all gg.
  2. Compact rotations. For G=SO(3)G=\mathrm{SO}(3), using the standard inner product to identify so(3)≅so(3)∗≅R3\mathfrak{so}(3)\cong\mathfrak{so}(3)^*\cong\mathbb{R}^3, the coadjoint action corresponds to the usual rotation action on R3\mathbb{R}^3.
  3. Matrix groups with trace pairing. For G=GL(n,R)G=\mathrm{GL}(n,\mathbb{R}), identify gl(n,R)∗\mathfrak{gl}(n,\mathbb{R})^* with matrices by ⟨A,B⟩=tr⁡(ATB)\langle A,B\rangle=\operatorname{tr}(A^\mathsf{T}B). Under this identification,
    Ad⁡g∗A=g−TAgT.\operatorname{Ad}_g^*A=g^{-\mathsf{T}}Ag^\mathsf{T}.