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Coconnected Hopf algebras give fixed vectors in every nonzero comodule

Statement

Let A be a coconnected commutative Hopf algebra over a field k, with filtration C0⊆C1⊆… as in Coconnected commutative Hopf algebras. If V≠0 is an A-comodule with coaction ρ:V→V⊗kA, then V has a nonzero vector v with ρ(v)=v⊗1.

In particular, if G is an affine algebraic group over k whose coordinate Hopf algebra O(G) is coconnected, then every nonzero rational representation of G has a nonzero fixed vector; that is, G is unipotent in the sense of Unipotent algebraic groups and unipotent representations.

Facts & Assumptions

Given: A field k, a coconnected commutative Hopf algebra A with filtration (Cr), and a nonzero A-comodule (V,ρ).

[F1]

C0=k⋅1A, ⋃rCr=A, and Δ(Cr)⊆∑i=0rCi⊗kCr−i for all r≥0. (Coconnected commutative Hopf algebras)

[F2]

A comodule structure is a k-linear map ρ:V→V⊗kA satisfying the counit identity (id⁡⊗ε)ρ=id⁡V and the coassociativity identity (ρ⊗id⁡)ρ=(id⁡⊗Δ)ρ. The linear span of the image of ρ lies in V⊗Cr for some r depending on the element. (Rational representations and comodules of an affine group scheme)

[F3]

Rational representations of an affine group scheme are exactly its comodules, with fixed vectors corresponding to elements with ρ(v)=v⊗1. (Rational representations of an affine group scheme are comodules of its coordinate Hopf algebra, Rational representations and comodules of an affine group scheme)

Proof

Given: A field k, a coconnected Hopf algebra A with filtration (Cr), and a nonzero comodule (V,ρ).

1.1F1F2

For r≥0 put Vr={v∈V:ρ(v)∈V⊗kCr}; these are k-linear subspaces of V with Vr⊆Vr+1 and, by [F1] and [F2], ⋃rVr=V. The space V0 consists exactly of the fixed vectors: if ρ(v)∈V⊗C0=V⊗k⋅1 then ρ(v)=w⊗1 for some w, and applying id⁡⊗ε gives v=w by the counit identity, so ρ(v)=v⊗1; conversely a fixed vector lies in V0.

2.1F1F2step 1.1

I claim that Vr=0 implies Vr+1=0 whenever r≥0. Let π:A→A/Cr be the quotient map. If v∈Vr+1, then ρ(v)∈V⊗Cr+1, and by [F1] every element of Cr+1 maps to zero under π⊗π applied to Δ, because Δ(Cr+1)⊆Cr⊗A+A⊗Cr; hence (id⁡⊗π⊗π)(id⁡⊗Δ)ρ(v)=0. By coassociativity [F2] this is (id⁡⊗π⊗π)(ρ⊗id⁡)ρ(v)=0. Choose a finite expansion (id⁡⊗π)ρ(v)=∑ivi⊗aˉi with the vi linearly independent, by taking a finite basis of the span of the first factors of any tensor expansion; then the last identity reads ∑i(id⁡⊗π)ρ(vi)⊗aˉi=0. The map (id⁡⊗π)ρ is injective on V when Vr=0, since its kernel is exactly Vr; therefore the elements (id⁡⊗π)ρ(vi) are linearly independent, so each aˉi=0, that is, (id⁡⊗π)ρ(v)=0 and hence ρ(v)∈V⊗Cr, i.e. v∈Vr=0. Thus Vr+1=0.

3.1F3step 1.1step 2.1∎

Since V≠0, [F2] gives an element v≠0 with ρ(v)∈V⊗Cr for some r, so Vr≠0. Iterating [step 2.1] downwards, V0≠0: if V0=0 then V1=0, then V2=0, and by induction Vr=0 for all r, contradicting Vr≠0. By [step 1.1] any nonzero element of V0 is a nonzero fixed vector, which proves the first assertion. The group-theoretic form follows from the comodule dictionary [F3], since for G with O(G)=A the rational representations of G are exactly the A-comodules and fixed vectors are the elements with coaction v⊗1.

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