nLab bialgebroid

Redirected from "associative bialgebroid".

Context

Algebra

Group theory

Ring theory

Module theory

Gebras

higher algebra

universal algebra

Algebraic theories

Algebras and modules

Higher algebras

Model category presentations

Geometry on formal duals of algebras

Theorems

Contents

Idea

A bialgebroid may be viewed as a multiobject generalization of a concept of a bialgebra, or a possibly noncommutative generalization of a space-algebra dual version of the concept of an internal category in spaces.

Nomenclature

This entry is about “associative” bialgebroid, see also the different concept of a Lie bialgebroid.

Motivation in Tannakian formalism

When a monoidal category has a fiber functor to a category of vector spaces over a field, one tries to “reconstruct” the category as the category of representations of the endomorphism object of a fiber functor. One often does not have a fiber functor to vector spaces but only to bimodules over some base algebra AA. Sometimes in such cases, the object of endomorphisms of the fiber functor form a bialgebroid over AA and the category is equivalent to the category of representations of that bialgebroid.

Definition

Via monoidal categories

Given a unital (possibly noncommutative) ring RR an RR-bialgebroid is an RR-RR-bimodule HH (object of R R{}_R \mathcal{M}_R) equipped with a structure of a comonoid in R R{}_R \mathcal{M}_R (i.e. an RR-coring) and of a monoid in R e R e{}_{R^e}\mathcal{M}_{R^e} (i.e. an R eR^e-ring), where R e=R opRR^e = R^{op}\otimes R is the enveloping ring of RR; and the structures of a monoid and a comonoid satisfy certain compatibility conditions. These compatibility conditions are equivalent to the fact that the monad R eH: R e R e{}_{\otimes_{R^e}} H : \mathcal{M}_{R^e}\to \mathcal{M}_{R^e} is opmonoidal. The category of RR-comodules is by definition the category of comodules over the underlying RR-coring.

An explicit definition

If AA is an associative algebra over some ground field kk, then a left associative AA-bialgebroid is another associative kk-algebra HH together with the following additional maps: an algebra map α:AH\alpha:A\to H called the source map, an algebra map β:A opH\beta:A^{op}\to H called the target map, so that the elements of the images of α\alpha and β\beta commute in HH, therefore inducing an AA-bimodule structure on HH via the rule a.h.b=α(a)β(b)ha.h.b = \alpha(a)\beta(b) h for a,bA,hHa,b\in A, h\in H; an AA-bimodule morphism Δ:HH AH\Delta:H\to H\otimes_A H which is required to be a counital coassociative comultiplication on HH in the monoidal category of AA-bimodules with monoidal product A\otimes_A. The map HAhaϵ(hα(a))H\otimes A\ni h\otimes a\mapsto \epsilon(h\alpha(a))\in must be a left action extending the multiplication AAAA\otimes A\to A along αid A\alpha\otimes id_A. Furthermore, a compatibility between the comultiplication Δ\Delta and multiplications on HH and on HHH\otimes H is required. For a noncommutative LL the tensor square H AH\otimes_A is not an algebra, hence asking for a bialgebra-like compatibility that Δ:HH AH\Delta:H\to H\otimes_A H is a morphism of kk-algebras does not make sense. Instead, one requires that H AHH\otimes_A H has a kk-subspace TT which contains the image of Δ\Delta and has a well-defined multiplication induced from its preimage under the projection from the usual tensor square algebra HHH\otimes H. Then one requires that the corestriction Δ| T:HT\Delta|^T :H\to T is a homomorphism of unital algebras. Under these conditions, one can make a canonical choice for TT, namely the so called Takeuchi’s product H× AHH AHH\times_A H\subset H\otimes_A H, which always inherits an associative multiplication along the projection from HHH\otimes H.

Via AA opA\otimes A^{op}-rings

All modules and morphisms will be over a fixed ground commutative ring kk.

A left AA-bialgebroid is an A kA opA\otimes_k A^{op}-ring (H,μ H,η)(H,\mu_H,\eta), together with the AA-bimodule map “comultiplication” Δ:HH AH\Delta : H\to H\otimes_A H, which is coassociative and counital with a counit ϵ\epsilon, such that

(i) the AA-bimodule structure used on HH is a.h.a:=s(a)t(a)ha.h.a':= s(a)t(a')h, where s:=η(1 A):AHs := \eta(-\otimes 1_A):A\to H and t:=η(1 A):A opHt:=\eta(1_A\otimes -):A^{op}\to H are the algebra maps induced by the unit η\eta of the AA opA\otimes A^{op}-ring HH

(ii) the coproduct Δ:HH AH\Delta : H\to H\otimes_A H corestricts to the Takeuchi product and the corestriction Δ:HH× AH\Delta : H\to H\times_A H is a kk-algebra map, where the Takeuchi product H× AHH\times_A H has a multiplication induced factorwise

(iii) ϵ\epsilon is a left character on the AA-ring (H,μ H,s)(H,\mu_H,s).

Notice that H AHH\otimes_A H is in general not an algebra, just an AA-bimodule. That is why (ii) is needed. An equivalent condition to (ii) is the following: the formula h.( ik il i)= ih (1)k ih (2)l ih.(\sum_i k_i \otimes l_i) = \sum_i h_{(1)}\cdot k_i \otimes h_{(2)} \cdot l_i defines a well-defined action of HH on H AHH\otimes_A H.

The definition of a right AA-bialgebroid differs by the AA-bimodule structure on HH given instead by a.h.a:=hs(a)t(a)a.h.a':= h s(a')t(a) and the counit ϵ\epsilon is a right character on the AA-coring (H,μ H,t)(H,\mu_H,t) (tt and ss can be interchanged in the last requirement).

Literature

Related notions: Hopf algebroid

Commutative case

The commutative case is rather classical. See for example the appendix to

  • Douglas C. Ravenel, Complex cobordism and stable homotopy groups of spheres, Pure and Applied Mathematics 121. Academic Press Inc., Orlando, FL, 1986.

Noncommutative case

The first version of a bialgebroid over a noncommutative base was more narrow:

  • M. Sweedler, Groups of simple algebras, Publ. IHES 44:79–189, 1974, numdam

A modern generality, but in different early formalism, is due to Takeuchi (who was motivated to generalize the results from the Sweedler’s paper), under the name of × A\times_A-bialgebra (as it involves the × A\times_A-product, nowdays called Takeuchi product):

  • M. Takeuchi, Groups of algebras over A×A¯A \times \bar{A}, J. Math. Soc. Japan 29, 459–492, 1977, MR0506407, euclid

Lu introduces the name bialgebroid for a structure which is equivalent to the Takeuchi’s × A\times_A-bialgebra (though differently axiomatized there):

Modern treatments are in

There is also a notion of quasibialgebroid, where the coassociativity is weakened by a bialgebroid 3-cocycle. See also Hopf algebroid.

Last revised on September 28, 2024 at 13:58:07. See the history of this page for a list of all contributions to it.