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The two standard bialgebra compatibility formulations are equivalent
Statement
Let be a -vector space with a unital associative algebra structure and a counital coassociative coalgebra structure . Give the tensor-product coalgebra structure of The tensor product of two coalgebras is a coalgebra, and give its coalgebra structure , . Then the following are equivalent:
- and are unital algebra homomorphisms, where has multiplication .
- and 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.
A coalgebra map is linear and satisfies and (Coalgebra and coalgebra map over a field).
Every element of 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).
A bialgebra over requires and to be unital algebra homomorphisms, using the tensor-product algebra multiplication (Bialgebras and bialgebra maps).
The tensor-product coalgebra has and (The tensor product of two coalgebras is a coalgebra).
The tensor-product algebra multiplication satisfies with unit (The tensor product of -algebras has multiplication ).
The unit isomorphism sends to (The regular module is a tensor unit: and ).
The associator on iterated tensor products is coherent (Associator naturality, pentagon, unit triangle and symmetry hexagons on elementary tensors).
Linear maps induce tensor-product linear maps by , uniquely and functorially (Module homomorphisms induce tensor-product homomorphisms functorially).
Proof
The stated maps make a coalgebra: for , both iterated coproducts of equal under the coherent associator [F7], and either counit contraction equals under the unit isomorphism [F6]. The induced tensor maps are well-defined by [F8].
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 , , , and .
The comultiplication equation for to be a coalgebra map [F1], evaluated on , is . By [F4]–[F5], this is exactly . Both sides are linear in and elementary tensors span by [F2], while is well-defined by [F8]. Thus the map equation holds exactly when that multiplicativity equation holds for all .
The counit equation for to be a coalgebra map [F1] is , which by [F4] is . Since elementary tensors span [F2], equality on all of them is equivalent to equality of the linear maps.
For , the coalgebra-map equations [F1] at are and . By linearity and the formulas in the Statement, these become and , using the source coalgebra established in step 1.1. They hold for every exactly when and . Steps 1.3–1.4 show that 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.
Depends on
- Bialgebras and bialgebra maps
- Coalgebra and coalgebra map over a field
- Scalars, tensor powers, the empty tensor, opposite algebras and finite sums
- Associator naturality, pentagon, unit triangle and symmetry hexagons on elementary tensors
- The tensor product of two coalgebras is a coalgebra
- Module homomorphisms induce tensor-product homomorphisms functorially
- The tensor product of $R$-algebras has multiplication $(a\otimes b)(a'\otimes b')=aa'\otimes bb'$
- The regular module is a tensor unit: $R\otimes_RN\cong N$ and $M\otimes_RR\cong M$
Used by
Nothing in the library uses this result yet.
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Sources
- Hans-Jürgen Schneider, Lectures on Hopf algebras, notes by Sonia Natale (standard reference, not scraped)
- Thomas Rüd, Hopf Algebras and rooted trees, Practical work in mathematics (standard reference, not scraped)