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The free Hopf module over a group algebra

Example

Let G be any group, k a field, and V a k-vector space. Write kG for the vector space of finite formal sums of elements of G, with multiplication extended from G. Give it the Hopf structure Δ(g)=g⊗g, ε(g)=1, and S(g)=g−1 on each g∈G. On V⊗kG use the free action and coaction. Then its coinvariants are V⊗1, P(v⊗g)=v⊗1, and the inverse decomposition sends v⊗g to (v⊗1)⊗g.

Facts & Assumptions

Given: A group G, a field k, and a k-vector space V.

[F1]

A right-right Hopf module has compatibility ρ(xh)=∑x0h1⊗x1h2 and coinvariants ρ(x)=x⊗1 (Right-right Hopf modules and coinvariants).

[F2]

The free structure on V⊗H is (v⊗h)g=v⊗hg and ρ(v⊗h)=∑(v⊗h1)⊗h2 (The free right-right Hopf module on a vector space).

[F3]

The projection is P(x)=∑x0S(x1), and the inverse theorem map is β(x)=∑P(x0)⊗x1 (The coinvariant projection of a right-right Hopf module, The fundamental theorem of right-right Hopf modules).

Verification

1.1givenalgebra

Multiplication on kG is associative and unital because the group multiplication is; on each basis element, Δ(gh)=gh⊗gh=(g⊗g)(h⊗h) and ε(gh)=1=ε(g)ε(h). Coassociativity and both counit identities hold on g since Δ(g)=g⊗g and ε(g)=1. Finally, gS(g)=gg−1=1=S(g)g, so both antipode equations hold on each basis vector. All structure identities extend by linearity or bilinearity to finite sums, making kG a Hopf algebra.

1.2F1F2algebra

Every z∈V⊗kG has finite support and can be written z=∑gvg⊗g; the coefficients are unique because applying id⁡V⊗δg, where δg extracts the g-coefficient, recovers vg. If z is coinvariant, then ∑gvg⊗g⊗g=∑gvg⊗g⊗e. Applying id⁡V⊗δg⊗δg shows vg=0 for g≠e. Conversely v⊗e is coinvariant, so the coinvariants are exactly V⊗e.

2.1F1F2step 1.1

For v∈V and g,a∈G, the free structure gives ρ((v⊗g)a)=ρ(v⊗ga)=(v⊗ga)⊗ga, while the compatibility right side is (v⊗g)a⊗ga=(v⊗ga)⊗ga. Bilinearity extends this equality to every h∈kG, so the pair is a Hopf module.

3.1F2F3step 1.2step 2.1∎

For a basis tensor v⊗g, P(v⊗g)=(v⊗g)g−1=v⊗e. Hence β(v⊗g)=(v⊗e)⊗g and α((v⊗e)⊗g)=v⊗g. Finite-sum linearity gives the formulas on every element; these are the projection and inverse decomposition from [F3].

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