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The two standard bialgebra compatibility formulations are equivalent

Statement

Let H be a k-vector space with a unital associative algebra structure (m,u) and a counital coassociative coalgebra structure (Δ,ε). Give H⊗H the tensor-product coalgebra structure of The tensor product of two coalgebras is a coalgebra, and give k its coalgebra structure Δk(λ)=λ(1⊗1), εk(λ)=λ. Then the following are equivalent:

  1. Δ:H→H⊗H and ε:H→k are unital algebra homomorphisms, where H⊗H has multiplication (a⊗b)(c⊗d)=ac⊗bd.
  2. m:H⊗H→H and u:k→H are coalgebra maps.

This equivalence is valid over every field and uses no dimension assumption.

Facts & Assumptions

Given: The algebra and coalgebra structure maps above, the tensor-product coalgebra formula, and the tensor-product algebra formula.

[F1]

A coalgebra map f:C→D is linear and satisfies ΔDf=(f⊗f)ΔC and εDf=εC (Coalgebra and coalgebra map over a field).

[F2]

Every element of V⊗W is a finite sum of elementary tensors, and tensor powers are associated using the displayed canonical associators (Scalars, tensor powers, the empty tensor, opposite algebras and finite sums).

[F3]

A bialgebra over k requires Δ and ε to be unital algebra homomorphisms, using the tensor-product algebra multiplication (Bialgebras and bialgebra maps).

[F4]

The tensor-product coalgebra has ΔH⊗H(a⊗b)=∑(a(1)⊗b(1))⊗(a(2)⊗b(2)) and εH⊗H(a⊗b)=ε(a)ε(b) (The tensor product of two coalgebras is a coalgebra).

[F5]

The tensor-product algebra multiplication satisfies (a⊗b)(c⊗d)=ac⊗bd with unit 1⊗1 (The tensor product of R-algebras has multiplication (a⊗b)(a′⊗b′)=aa′⊗bb′).

[F6]

The unit isomorphism k⊗k→k sends r⊗s to rs (The regular module is a tensor unit: R⊗RN≅N and M⊗RR≅M).

[F7]
[F8]

Linear maps induce tensor-product linear maps by (f⊗g)(v⊗w)=f(v)⊗g(w), uniquely and functorially (Module homomorphisms induce tensor-product homomorphisms functorially).

Proof

technique · direct
1.1givenF6F7F8algebra

The stated maps make k a coalgebra: for r∈k, both iterated coproducts of Δk(r)=r(1⊗1) equal r(1⊗1⊗1) under the coherent associator [F7], and either counit contraction equals r under the unit isomorphism [F6]. The induced tensor maps are well-defined by [F8].

1.2givenF3F5algebra

The maps in condition 1 are unital algebra homomorphisms exactly when they preserve products and units, as required in the bialgebra definition [F3]. With the tensor-product algebra [F5], these requirements are precisely Δ(ab)=Δ(a)Δ(b), Δ(1)=1⊗1, ε(ab)=ε(a)ε(b), and ε(1)=1.

1.3givenF1F2F4F5F8algebra

The comultiplication equation for m to be a coalgebra map [F1], evaluated on a⊗b, is Δ(m(a⊗b))=(m⊗m)ΔH⊗H(a⊗b)=∑a(1)b(1)⊗a(2)b(2). By [F4]–[F5], this is exactly Δ(ab)=Δ(a)Δ(b). Both sides are linear in a⊗b and elementary tensors span H⊗H by [F2], while m⊗m is well-defined by [F8]. Thus the map equation holds exactly when that multiplicativity equation holds for all a,b.

1.4givenF1F2F4

The counit equation for m to be a coalgebra map [F1] is ε(m(a⊗b))=εH⊗H(a⊗b), which by [F4] is ε(ab)=ε(a)ε(b). Since elementary tensors span [F2], equality on all of them is equivalent to equality of the linear maps.

2.1givenF1F8step 1.1step 1.2step 1.3step 1.4∎

For u:k→H, the coalgebra-map equations [F1] at λ∈k are Δ(u(λ))=(u⊗u)Δk(λ) and ε(u(λ))=εk(λ). By linearity and the formulas in the Statement, these become λΔ(1)=λ(1⊗1) and λε(1)=λ, using the source coalgebra established in step 1.1. They hold for every λ exactly when Δ(1)=1⊗1 and ε(1)=1. Steps 1.3–1.4 show that m is a coalgebra map exactly when the two product equations hold; the two unit equations supply the remaining equations in step 1.2. Therefore condition 2 holds exactly when condition 1 holds.

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