Hopf Algebras & Quantum Groups

comodule

A module is a vector space acted on by an algebra: the algebra reaches in and moves vectors around. A comodule is the mirror image: instead of being acted on, the space coacts onto itself tensored with a coalgebra, recording 'where each vector could come from.' If a module is how a symmetry pushes a space, a comodule is how a space resolves itself into pieces labelled by a coalgebra.

Formally, a right comodule over a coalgebra C is a vector space M with a linear coaction ρ : M -> M ⊗ C satisfying coassociativity (ρ ⊗ id) ∘ ρ = (id ⊗ Δ) ∘ ρ and counitality (id ⊗ ε) ∘ ρ = id (after M ⊗ k ≅ M). One uses a Sweedler-style notation ρ(m) = Σ m(0) ⊗ m(1), with the (0)-leg in M and the (1)-leg in C.

Comodules are dual to modules and often closer to geometry. A comodule over the coordinate Hopf algebra O(G) of an algebraic group G is precisely a rational (algebraic) representation of G, whereas modules over O(G) are far more rigid. So the comodule language is the natural home for representations of affine group schemes and, after deformation, for representations of quantum groups.

Every comodule over C is the directed union of its finite-dimensional subcomodules — comodules are locally finite, mirroring the Fundamental Theorem of Coalgebras. This is false for modules over algebras, and it is the technical reason representations of algebraic groups are built from finite-dimensional ones.