Survey
* Your assessment is very important for improving the work of artificial intelligence, which forms the content of this project
* Your assessment is very important for improving the work of artificial intelligence, which forms the content of this project
PARTIAL ENTWINING STRUCTURES
S. CAENEPEEL AND K. JANSSEN
Abstract. We introduce partial (co)actions of a Hopf algebra on an
algebra A. To this end, we introduce first the notion of lax coring,
generalizing Wisbauer’s notion of weak coring. We also have the dual
notion of lax ring. We then introduce partial and lax entwining structures. Several duality results are given, and we develop Galois theory
for partial entwining structures.
Introduction
Partial group actions were considered first by Exel [15], in the context of
operator algebras. A treatment from a purely algebraic point of view was
given recently in [11, 12, 13, 14]. In particular, Galois theory over commutative rings can be generalized to partial group actions, see [13] (at least
under the additional assumption that the associated ideals are generated by
idempotents).
The following questions arise naturally: can we develop a theory of partial
(co)actions of Hopf algebras? Is it possible to generalize Hopf-Galois theory
to the partial situation? The aim of this paper is to give a positive answer
to these questions.
Partial group actions were studied from the point of view of corings by the
first author and De Groot in [6]. Namely, a partial group action in the sense
of [13] gives rise to a coring. The Galois theory of [13] can then be considered as a special case of the Galois theory of corings (see [2, 3, 4, 18]). There
is a remarkable analogy with the Galois theory that can be developed for
weak Hopf algebras (see [7]): in both cases, the associated coring is a direct
factor of the tensor product of the Galois extension A, and a coalgebra. In
the partial group action case, the coalgebra is the dual of the group algebra,
in the other case it is the weak Hopf algebra that we started with. The right
A-module structure of the coring is induced by a kind of entwining map. In
the weak Hopf algebra case, it is a weak entwining map, as introduced in
[5]. The map in the partial group action case, however, does not satisfy the
axioms of a weak entwining structure.
Wisbauer [17] introduces weak entwining structures from the point of view
of weak corings; these are corings with a bimodule structure that is not necessarily unital. If C is a left-unital weak A-coring, then C1A is an A-coring
2000 Mathematics Subject Classification. 16W30.
Key words and phrases. coring, entwining structure, smash product, Galois extension.
1
2
S. CAENEPEEL AND K. JANSSEN
that is a direct summand of C. Weak entwining structures are then in oneto-one correspondence with left-unital weak A-coring structures on A ⊗ C,
where A is an algebra, and C is a coalgebra.
If a finite group G acts partially on an algebra A, then we can define a leftunital A-bimodule structure on A ⊗ (kG)∗ , such that (A ⊗ (kG)∗ )1A is an
A-coring, and a direct factor of A ⊗ (kG)∗ . But A ⊗ (kG)∗ does not satisfy
Wisbauer’s axioms of a weak coring. This observation has lead us to the
introduction of lax corings. The counit property of a lax coring is weaker
than that of a weak coring, but it is still designed in such a way that C1A is
a coring.
Our next step is then to examine lax coring structures on A ⊗ C. A subtlety that appears is that we have two possible choices for the counit: we
can consider A ⊗ and (A ⊗ ) ◦ π, where is the counit on C, and π is
the projection of A ⊗ C onto (A ⊗ C)1A . This leads to the introduction of
lax and partial entwining structures. The notion of lax entwining structure
is the most general, and includes partial and weak entwining structures as
special cases. If (A, C, ψ) is at the same time a partial and weak entwining
structure, then it is an entwining structure.
Now let C = H be a Hopf algebra, and consider a map ρ : A → A ⊗ H. We
call A a right partial (resp. lax) H-comodule algebra if (A, C, ψ), with ψ
given by the formula ψ(h ⊗ a) = a[0] ⊗ ha[1] is a partial (resp. lax) entwining
structure.
We have a dual theory: we can introduce lax A-rings, and lax and partial
smash product structures. We then obtain the definition of partial (resp.
lax) H-module algebra. In the case where H is a group algebra, we recover
the definition of partial group action. We also discuss duality results. For
example, if C is a finitely generated projective coalgebra, then we have a
bijective correspondence between lax (resp. partial) entwining structures of
the form (A, C, ψ) and lax (resp. partial) smash product structures of the
form (Aop , C ∗ , R) (see Theorem 5.7). In the final Section 7, we applied the
theory of Galois corings to corings arising from partial entwining structures.
1. Lax rings and corings
In this Section, A is a ring with unit. A-modules will not necessarily be
unital.
Proposition 1.1. Let P be an unital left A-module. There is a bijective
correspondence between
(1) (non-unital) right A-module structures on P making P an A-bimodule;
(2) unital right A-module structures on left A-linear direct factors P of
P , making P a unital A-bimodule.
Proof. Let P be an A-bimodule as in (1). The map π : P → P , π(p) = p1A
is a left A-linear projection. The right A-action on P restricts to a unital
right A-action on P = Im (π).
PARTIAL ENTWINING STRUCTURES
3
Conversely, let π : P → P be a left A-linear projection, and let P be an
unital A-bimodule. We extend the right A-action from P to P as follows:
pa = π(p)a ∈ P . This action is associative, since (pa)b = (π(p)a)b =
π(p)(ab) = p(ab).
We observe that π is then also right A-linear, so P is an A-bimodule direct
factor of P . The inclusion ι : P → P is a right inverse of π.
Recall that an A-coring (C, ∆, ε) is a coalgebra in the monoidal category
A MA of unital A-bimodules. This means that C is an unital A-bimodule,
and that ∆ : C → C ⊗A C and ε : C → A are A-bimodule maps such that
(1)
(∆ ⊗A C) ◦ ∆ = (C ⊗A ∆) ◦ ∆
and
(2)
(ε ⊗A C) ◦ ∆ = (C ⊗A ε) ◦ ∆ = C.
We will often use the Sweedler-Heyneman notation
∆(c) = c(1) ⊗A c(2) ,
where summation is implicitly understood.
Now take a left unital A-bimodule C and two A-bimodule maps ∆ : C →
C ⊗A C and ε : C → A satisfying (1). We consider the projection π : C →
C = C1 and its right inverse ι. For all c ∈ C, we have that
∆(c1) = ∆(c)1 = c(1) ⊗A 1c(2) 1 = c(1) 1 ⊗A c(2) 1 ∈ C ⊗A C,
so ∆ restricts to a map ∆ : C → C ⊗A C. ε ◦ ι is then the restriction of ε to
C.
• We call (C, ∆, ε) a left unital lax A-coring if (C, ∆, ε◦ι) is an A-coring;
this is equivalent to
(3)
c = ε(c(1) )c(2) = c(1) ε(c(2) ),
for all c ∈ C.
• Following [17], we call (C, ∆, ε) a left unital weak A-coring if
(4)
c1A = ε(c(1) )c(2) = c(1) ε(c(2) ),
for all c ∈ C.
It is clear that weak corings are lax corings.
Recall that an A-ring (R, µ, η) is an algebra in the category A MA of unital
A-bimodules. This means that µ : R ⊗A R → R and η : A → R are
A-bimodule maps such that
(5)
µ ◦ (µ ⊗A R) = µ ◦ (R ⊗A µ)
and
(6)
µ ◦ (η ⊗A R) = µ ◦ (R ⊗A η) = R.
4
S. CAENEPEEL AND K. JANSSEN
Then R is a ring with unit η(1A ), and η : A → R is a ring morphism. It
follows from (6) that the A-bimodule structure on R is induced by η. So an
A-ring is a ring R together with a ring morphism η : A → R.
Let R be a left unital A-bimodule, and consider the projection π : R → R =
R1, and an A-bimodule map µ : R ⊗A R → R satisfying (5). µ restricts to
a map µ : R ⊗A R → R, since µ(r1A ⊗A s1A ) = µ(r1A ⊗A s)1A ∈ R, for
all r, s ∈ R. We will write µ(r ⊗A s) = rs, as usual. Let η : A → R be an
A-bimodule map, and write η(1A ) = 1R . Then π(1R ) = 1R 1A = η(1A )1A =
η(1A ) = 1R , so that π ◦ η is the corestriction of η to R.
• (R, µ, η) is called a left unital lax A-ring if (R, µ, π ◦ η) is an A-ring,
that is,
(7)
r = 1R r = r1R ,
for all r ∈ R;
• (R, µ, η) is called a left unital weak A-ring if
(8)
r1A = 1R r = r1R ,
for all r ∈ R.
In what follows we will also need a right unital version of lax and weak
A-ring.
Let R be a right unital A-bimodule, put R = 1R, and consider an Abimodule map µ : R ⊗A R → R satisfying (5). As before µ restricts to a
map µ : R ⊗A R → R, and an A-bimodule map η : A → R corestricts to
the map π ◦ η : A → R.
• (R, µ, η) is called a right unital lax A-ring if (R, µ, π ◦ η) is an A-ring,
that is, condition (7) is fulfilled, for all r ∈ R;
• (R, µ, η) is called a right unital weak A-ring if
(9)
1A r = 1R r = r1R ,
for all r ∈ R.
Duality. Let C be a left unital A-bimodule. Then ∗ C =
right unital A-bimodule, with A-action
A Hom(C, A)
is a
(af b)(c) = f (ca)b,
for all a, b ∈ A, c ∈ C and f ∈ ∗ C. If ∆ : C → C ⊗A C is a coassociative
A-bimodule map, then µ : ∗ C ⊗A ∗ C → ∗ C, µ(f ⊗A g) = f #g given by
(f #g)(c) = g(c(1) f (c(2) )),
for all c ∈ C, is an associative A-bimodule map: we compute easily that
(f #g#h)(c) = h(c(1) g(c(2) f (c(3) ))).
PARTIAL ENTWINING STRUCTURES
5
Let ε : C → A be an A-bimodule map. For all a ∈ A and c ∈ C, we have
that
(aε)(c) = (εa)(c) = ε(c)a,
so η : A → ∗ C, η(a) = aε = εa, is an A-bimodule map.
For all f ∈ ∗ C and c ∈ C, we compute that
(ε#f )(c) = f (c(1) ε(c(2) ))
and
(f #ε)(c) = ε(c(1) f (c(2) )) = ε(c(1) )f (c(2) ) = f (ε(c(1) )c(2) ).
Proposition 1.2. If (C, ∆, ε) is a left unital weak (resp. lax) A-coring, then
(∗ C, µ, η) is a right unital weak (resp. lax) A-ring. The A-rings 1A ∗ C and
∗ (C1 ) are isomorphic.
A
Proof. Let (C, ∆, ε) be a left unital weak A-coring. For all f ∈ ∗ C and c ∈ C,
we have
(4)
(ε#f )(c) = f (c(1) ε(c(2) )) = f (c1A ) = (1A f )(c);
(4)
(f #ε)(c) = f (ε(c(1) )c(2) ) = f (c1A ) = (1A f )(c).
Thus (9) holds, and (∗ C, µ, η) is a right unital weak A-ring.
Now assume that (C, ∆, ε) is a left unital lax A-coring. For all f = 1A f ∈
1A ∗ C = ∗ C and c ∈ C, we have
(ε#f )(c) = (ε#1A f )(c) = (1A f )(c(1) ε(c(2) ))
(3)
= f (c(1) ε(c(2) )1A ) = f (c(1) ε(c(2) )) = f (c1A ) = (1A f )(c)
(f #ε)(c) = ε(c(1) (1A f )(c(2) )) = ε(c(1) f (c(2) 1A ))
(3)
= ε(c(1) )f (c(2) 1A ) = f (ε(c(1) )c(2) 1A ) = f (c1A ) = (1A f )(c).
So ε#f = f #ε = f , and (7) holds, and it follows that (∗ C, µ, η) is a right
unital lax A-ring.
To prove the final statement, we observe first that f ∈ 1A ∗ C if and only if
1 · f = f , or f (c · 1) = f (c), for all c ∈ C. The map
α : 1A ∗ C → ∗ (C1A ), α(f ) = f|C1A
has an inverse β, defined by the formula
β(g)(c) = g(c · 1A ),
for all g ∈ ∗ (C1A ). It is clear that β(g) ∈ 1A ∗ C, and
β(α(f ))(c) = α(f )(c · 1A ) = f (c · 1A ) = f (c),
for all f ∈ 1A ∗ C, and
α(β(g))(c · 1) = β(g)(c · 1) = g(c · 1),
for all g ∈ ∗ (C1A ).
6
S. CAENEPEEL AND K. JANSSEN
2. Partial entwining structures
Let k be a commutative ring, A a k-algebra, and M a k-module. A ⊗ M is
then an unital left A-module, with left A-action induced by multiplication
on A. For a k-linear map ψ : M ⊗ A → A ⊗ M , we will adopt the notation
ψ(m ⊗ a) = aψ ⊗ mψ = aΨ ⊗ mΨ ,
for all a ∈ A and m ∈ M . Summation is implicitly understood.
Lemma 2.1. There is a bijective correspondence between
• (non-unital) right A-actions on A ⊗ M , compatible with the left Aaction;
• k-linear maps ψ : M ⊗ A → A ⊗ M satisfying the condition
(ab)ψ ⊗ mψ = aψ bΨ ⊗ mψΨ ,
(10)
for all a, b ∈ A and m ∈ M .
Then A ⊗ M = (A⊗M )1A is an unital A-bimodule, and we have a projection
π : A ⊗ M → A ⊗ M, π(a ⊗ m) = (a ⊗ m)1 = a1ψ ⊗ mψ .
A ⊗ M is right A-unital if
1ψ ⊗ mψ = 1 ⊗ m,
(11)
for all m ∈ M .
Proof. Given a right A-action, we define ψ : M ⊗A → A⊗M by the formula
ψ(m ⊗ a) = (1 ⊗ m)a.
(10) follows from the associativity of the right A-action. Conversely, given
ψ, we define a right A-action by (a ⊗ m)b = abψ ⊗ mψ .
Now let (C, δ, ) be a k-coalgebra, and ψ : C ⊗ A → A ⊗ C a k-linear map
satisfying (10). Consider the maps
∼ A ⊗ C ⊗ C,
∆ = (π ⊗ C) ◦ (A ⊗ δ) : A ⊗ C → A ⊗ C ⊗A A ⊗ C =
ψ
∆(a ⊗ c) = (a ⊗ c(1) ) ⊗A (1 ⊗ c(2) ) ∼
= a1ψ ⊗ c(1) ⊗ c(2) ,
ε = A ⊗ : A ⊗ C → A, ε(a ⊗ c) = (c)a,
ε = (A ⊗ ) ◦ π : A ⊗ C → A, ε(a ⊗ c) = (cψ )a1ψ .
We will now investigate when (A ⊗ C, ∆, ε) and (A ⊗ C, ∆, ε) are left unital
weak, resp. lax A-corings. Then ∆ and ε (or ε) have to be right A-linear.
Lemma 2.2. Let A be a k-algebra, C a k-coalgebra, and ψ : C ⊗A → A⊗C
a k-linear map satisfying (10).
(1) ∆ is right A-linear if and only if
(12)
ψ
ψ
Ψ
aψ 1Ψ ⊗ (cψ )Ψ
(1) ⊗ (c )(2) = aψΨ ⊗ c(1) ⊗ c(2) ,
for all a ∈ A and c ∈ C.
PARTIAL ENTWINING STRUCTURES
7
(2) ε is right A-linear if and only if
(cψ )1ψ a = (cψ )aψ ,
(13)
for all a ∈ A and c ∈ C.
(3) ε is right A-linear if and only if ε = ε, that is
(c)a = (cψ )aψ ,
(14)
for all a ∈ A and c ∈ C.
Proof. 1) ∆ is right A-linear if and only if
ψ
Ψ
∼
∆(1 ⊗ c)a = (1 ⊗ c(1) ) ⊗A (aψ ⊗ cψ
(2) ) = aψΨ ⊗ c(1) ⊗ c(2)
equals
∆((1 ⊗ c)a) = ∆(aψ ⊗ cψ )
ψ
= (aψ ⊗ (cψ )(1) ) ⊗A (1 ⊗ (cψ )(2) ) ∼
= aψ 1Ψ ⊗ (cψ )Ψ
(1) ⊗ (c )(2) .
2) ε is right A-linear if and only if ε(b ⊗ c)a = (cψ )b1ψ a equals ε((b ⊗ c)a) =
(cψ )baψ , for all a, b ∈ A and c ∈ C, and this is equivalent to (13).
3) ε is right A-linear if and only if ε(b ⊗ c)a = (c)ba equals ε((b ⊗ c)a) =
(cψ )baψ , and this is equivalent to (14).
If ∆ is right A-linear, then ∆ restricts to a map ∆ : A ⊗ C → A ⊗ C ⊗A
A ⊗ C.
Proposition 2.3. Let A be a k-algebra, C a k-coalgebra, and ψ : C ⊗ A →
A ⊗ C a k-linear map. The following assertions are equivalent:
(1) (A ⊗ C, ∆, ε) is a left unital weak A-coring;
(2) the conditions (10,12,13) and
(15)
1ψ ⊗ cψ = (cψ
(1) )1ψ ⊗ c(2)
are satisfied for all a, b ∈ A and c ∈ C;
(3) the conditions (10,13,15) and
(16)
ψ
aψ ⊗ δ(cψ ) = aψΨ ⊗ cΨ
(1) ⊗ c(2) ,
are satisfied for all a, b ∈ A and c ∈ C.
We then say that (A, C, ψ) is a weak entwining structure.
Proof. If (A ⊗ C, ∆, ε) is a left unital weak A-coring, then (10,12,13) hold,
by Lemmas 2.1 and 2.2.
Assume that (10,12,13) are satisfied. The left counit property (ε⊗A C)◦∆ =
π (cf. (4)) holds if and only if
ε(a ⊗ c(1) )(1 ⊗ c(2) ) = (cψ
(1) )a1ψ ⊗ c(2)
equals
(a ⊗ c)1 = a1ψ ⊗ cψ ,
8
S. CAENEPEEL AND K. JANSSEN
for all a ∈ A and c ∈ C, if and only if (15) holds for all c ∈ C. This proves
that (1) ⇒ (2). It also proves that (2) ⇒ (1), if we can show that the right
counit condition is satisfied. Indeed,
(a ⊗ c(1) )ε(1 ⊗ c(2) ) = (cψ
(2) )(a ⊗ c(1) )1ψ
=
(12)
Ψ
(cψ
(2) )(a1ψΨ ⊗ c(1) )
=
((cψ )(2) )a1ψ 1Ψ ⊗ (cψ )Ψ
(1)
=
a1ψ 1Ψ ⊗ cψΨ
(10)
=
a1ψ ⊗ cψ = (a ⊗ c)1.
(2) ⇔ (3). We will prove that the left hand sides of the formulas (12) and
(16) are equal if ψ satisfies (10) and (15). Indeed,
(15)
ψ
ψ Ψ
ψ
ψ
aψ 1Ψ ⊗ (cψ )Ψ
(1) ⊗ (c )(2) = aψ (c )(1) 1Ψ ⊗ (c )(2) ⊗ (c )(3)
(15)
aψ 1Ψ ⊗ (cψΨ )(1) ⊗ (cψΨ )(2)
(10)
aψ ⊗ (cψ )(1) ⊗ (cψ )(2) = aψ ⊗ δ(cψ ).
=
=
Weak entwining structures were first introduced by the first author and
De Groot [5], and the defining axioms are (10,13,15) and (16). Wisbauer
[17] introduced weak corings, and proved the equivalence of (1) and (2) in
Proposition 2.3 (see [17, 4.1]). So his axioms characterizing weak entwining
structures are (10,12,13) and (15). In a remark following 4.1 in [17], it is
observed that the defining axioms in [5] and [17] are not the same. It follows
from Proposition 2.3 that the two sets of axioms are equivalent.
Proposition 2.4. Let A be a k-algebra, C a k-coalgebra, and ψ : C ⊗ A →
A ⊗ C a k-linear map. The following assertions are equivalent:
(1) (A ⊗ C, ∆, ε) is an A-coring;
(2) (A ⊗ C, ∆, ε) is a left unital weak A-coring;
(3) (A, C, ψ) is an entwining structure; this means that the conditions
(10,11,14) and (16) are satisfied.
Proof. (1) ⇒ (2) is trivial.
(2) ⇒ (3). It follows from Lemmas 2.1 and 2.2 that (10,12,14) hold. Using
(4), we find
a1ψ ⊗ cψ = (a ⊗ c)1 = ε(a ⊗ c(1) )(1 ⊗ c(2) ) = (c(1) )a ⊗ c(2) = a ⊗ c,
and (11) follows after taking a = 1. (16) follows easily from (11) and (12).
(3) ⇒ (1) is well-known (see e.g. [2]).
Proposition 2.5. Let A be a k-algebra, C a k-coalgebra, and ψ : C ⊗ A →
A ⊗ C a k-linear map. The following assertions are equivalent:
(1) (A ⊗ C, ∆, ε) is a left unital lax A-coring;
PARTIAL ENTWINING STRUCTURES
9
(2) the conditions (10,12,13) and
ψ
1ψ ⊗ cψ = (cΨ
(1) )1ψΨ ⊗ c(2) ,
(17)
are satisfied for all a, b ∈ A and c ∈ C;
(3) the conditions (10,12,13) and
ψ
1ψ ⊗ cψ = (cΨ
(1) )1Ψ 1ψ ⊗ c(2) ,
(18)
are satisfied for all a, b ∈ A and c ∈ C.
We then say that (A, C, ψ) is a lax entwining structure.
Proof. (1) ⇒ (2). It follows from Lemmas 2.1 and 2.2 that (10,12,13) hold.
Take 1ψ ⊗ cψ ∈ A ⊗ C. Then
∆(1ψ ⊗ cψ ) = (1ψ ⊗ (cψ )(1) ) ⊗A (1 ⊗ (cψ )(2) )
ψ
= (1ψ 1Ψ ⊗ (cψ )Ψ
(1) ) ⊗A (1 ⊗ (c )(2) ).
From the left counit property in (3), it follows that
1ψ ⊗ cψ = ((ε ◦ ι) ⊗A A ⊗ C)∆(1ψ ⊗ cψ )
=
ψ
(A ⊗ )(1ψ 1Ψ ⊗ (cψ )Ψ
(1) )(1 ⊗ (c )(2) )
=
ψ
((cψ )Ψ
(1) )1ψ 1Ψ ⊗ (c )(2)
(12)
=
ψ
(cΨ
(1) )1ψΨ ⊗ c(2) ,
so (17) holds.
(2) ⇒ (1). If (A, C, ψ) satisfies (10,12,13,17), then ∆ is a coassociative comultiplication on A ⊗ C. One equality in (3) is equivalent to (17), and the
other one can be proved as follows: we have shown in the proof of Proposition 2.3 that (10) and (12) imply that
((A ⊗ C) ⊗A ε) ◦ ∆ = π.
This entails that
((A ⊗ C) ⊗A (ε ◦ ι)) ◦ ∆ = A ⊗ C.
(2) ⇔ (3). Using (13), we find that (17) is equivalent to (18) (take a = 1ψ
in (13)).
Proposition 2.6. Let A be a k-algebra, C a k-coalgebra, and ψ : C ⊗ A →
A ⊗ C a k-linear map. The following assertions are equivalent:
(1) (A ⊗ C, ∆, ε) is a left unital lax A-coring;
(2) (A, C, ψ) is a lax entwining structure and
(19)
(cψ )1ψ = (c)1,
for all c ∈ C;
(3) The conditions (10,12) and (14) are satisfied, for all a ∈ A and
c ∈ C.
We then say that (A, C, ψ) is a partial entwining structure.
10
S. CAENEPEEL AND K. JANSSEN
Proof. (1) ⇒ (2). It follows from Lemma 2.2 that (14) holds; taking a = 1,
we find (19). It is clear that (A, C, ψ) is a lax entwining structure.
(2) ⇒ (1). From (19) it follows that ε = ε, and thus (A ⊗ C, ∆, ε = ε) is a
left-unital lax A-coring.
(2) ⇒ (3). Combining (19) and (13), we find (14).
(3) ⇒ (2). Taking a = 1 in (14), we find (19). (13) then follows from (19)
and (14). Also (18) follows easily:
(19)
ψ
ψ
ψ
(cΨ
(1) )1Ψ 1ψ ⊗ c(2) = (c(1) )11ψ ⊗ c(2) = 1ψ ⊗ c .
Proposition 2.7. (A, C, ψ) is an entwining structure if and only if it is at
the same time a partial and weak entwining structure.
Proof. One implication is obvious. Conversely, if (A, C, ψ) is a weak entwining structure, then, by Proposition 2.3, (10,15,16) are satisfied. If (A, C, ψ)
is a partial entwining structure, then (14) holds, by Proposition 2.6. Then
(11) can be shown as follows:
(15)
(14)
1ψ ⊗ cψ = (cψ
(1) )1ψ ⊗ c(2) = (c(1) )1 ⊗ c(2) = 1 ⊗ c.
The lax Koppinen smash product. Let (A, C, ψ) be a weak (or lax) entwining
structure, i.e. (C = A ⊗ C, ∆, ε) is a (left unital) weak (or lax) A-coring.
Given the k-module isomorphism
∗
C = A Hom(A ⊗ C, A) ∼
= Hom(C, A), f 7→ f ◦ (ηA ⊗ C),
the (right unital) weak (or lax) A-ring structure on ∗ C (see Proposition 1.2)
induces a (right unital) weak (or lax) A-ring structure on Hom(C, A). It is
given by the following formulas, for all a, b ∈ A, c ∈ C and f, g ∈ Hom(C, A):
(af b)(c) = aψ f (cψ )b,
(f #g)(c) = f (c(2) )ψ g(cψ
(1) ),
and
η : A → Hom(C, A), η(a)(c) = (cψ )aψ .
Hom(C, A) with this weak A-ring structure (but with slightly modified multiplication) is called in [5] the weak Koppinen smash product; when it is
equipped with the lax A-ring structure, we will call it the lax Koppinen
smash product. It is usually denoted by #(C, A).
The left dual of the corresponding A-coring C = C1A is then isomorphic to
#(C, A) = 1A #(C, A) = {f ∈ #(C, A) | f (c) = 1ψ f (cψ ), for all c ∈ C}.
PARTIAL ENTWINING STRUCTURES
11
3. Lax entwined modules
Let (A, C, ψ) be a lax entwining structure, C = A ⊗ C the associated lax
A-coring, and C = (A ⊗ C)1A the associated A-coring. For a k-linear
map ρ : M → M ⊗ C, we will adopt the notation ρ(m) = m[0] ⊗ m[1] ,
(ρ ⊗ C)(ρ(m)) = ρ2 (m) = m[0] ⊗ m[1] ⊗ m[2] , etc. We do not assume that ρ
is coassociative.
A lax entwined module is a right A-module M , together with a k-linear
map ρ : M → M ⊗ C such that the following conditions are satisfied, for
all m ∈ M :
(20)
m[0] (m[1] ) = m;
(21)
ρ2 (m) = m[0] 1ψΨ ⊗ (m[1](1) )Ψ ⊗ (m[1](2) )ψ ;
(22)
ρ(ma) = m[0] aψ ⊗ mψ
[1] .
A morphism between two lax entwined modules M and N is a right A-linear
map f : M → N such that f (m[0] )⊗m[1] = f (m)[0] ⊗f (m)[1] , for all m ∈ M .
M(ψ)C
A will denote the category of lax entwined modules.
Proposition 3.1. For a lax entwining structure (A, C, ψ), the categories
MC and M(ψ)C
A are isomorphic.
Proof. Let M be a right A-module. We will first show that HomA (M, M ⊗A
C) is isomorphic to the submodule of Hom(M, M ⊗ C) consisting of maps
ρ satisfying (22). Take ρ : M → M ⊗ C satisfying (22), and define α(ρ) :
M → M ⊗A C as follows:
α(ρ)(m) = m[0] ⊗A (1ψ ⊗ mψ
[1] ).
α(ρ) is right A-linear since
α(ρ)(ma) = m[0] aΨ ⊗A (1ψ ⊗ mΨψ
[1] )
=
(10)
m[0] ⊗A (aΨ 1ψ ⊗ mΨψ
[1] )
=
m[0] ⊗A (aψ ⊗ mψ
[1] )
=
m[0] ⊗A (1ψ ⊗ mψ
[1] )a = (α(ρ)(m))a.
Conversely, take ρ̃ ∈ HomA (M, M ⊗A C), and define β(ρ̃) ∈ Hom(M, M ⊗ C)
as follows: for m ∈ M , there exist (a finite number of) mi ∈ M and ci ∈ C
P
such that ρ̃(m) = i mi ⊗A (1ψ ⊗ cψ
i ); then we define
X
β(ρ̃)(m) =
mi 1ψ ⊗ cψ
i .
i
P
ψΨ
β(ρ̃) satisfies (22): ρ̃(ma) = i mi ⊗A (aψ ⊗ cψ
i mi aψ ⊗A (1Ψ ⊗ ci ),
i )=
hence
X
X
β(ρ̃)(ma) =
mi aψ 1Ψ ⊗ cψΨ
=
mi 1ψ aΨ ⊗ cψΨ
i
i .
P
i
i
12
S. CAENEPEEL AND K. JANSSEN
α and β are inverses:
α(β(ρ̃))(m) =
X
mi 1ψ ⊗A (1Ψ ⊗ cψΨ
i )
i
=
X
mi ⊗A (1ψ ⊗ cψ
i ) = ρ̃(m)
i
(22)
β(α(ρ))(m) = m[0] 1ψ ⊗ mψ
[1] = ρ(m).
Now take ρ : M → M ⊗ C satisfying (22) and the corresponding right
A-linear map ρ̃. We claim that ρ̃ is coassociative if and only if ρ satisfies
(21). First compute
ψ
1
ρ̃2 (m) = m[0] ⊗A (1Ψ1 ⊗ mΨ
[1] ) ⊗A (1ψ ⊗ m[2] );
ψ
((M ⊗A ∆) ◦ ρ̃)(m) = m[0] ⊗A (1ψ ⊗ (mψ
[1] )(1) ) ⊗A (1 ⊗ (m[1] )(2) ).
If ρ̃ is coassociative, then it follows that
ψ
1Ψ
m[0] 1Ψ1 1ψΨ ⊗ mΨ
[1] ⊗ m[2]
(10)
ψ
m[0] 1ψΨ ⊗ mΨ
[1] ⊗ m[2]
(22)
ρ(m[0] 1ψ ) ⊗ mψ
[1] = ρ(m[0] ) ⊗ m[1]
=
=
(22)
equals
ψ
Ψ
m[0] 1ψ 1Ψ ⊗ (mψ
[1] )(1) ⊗ (m[1] )(2)
(12)
=
m[0] 1ψΨ ⊗ (m[1](1) )Ψ ⊗ (m[1](2) )ψ ,
and (21) follows. Conversely, if (21) holds, then
((M ⊗A ∆) ◦ ρ̃)(m)
=
(12)
ψ
Ψ
m[0] ⊗A (1ψ 1Ψ ⊗ (mψ
[1] )(1) ) ⊗A (1 ⊗ (m[1] )(2) ) · 1
=
m[0] ⊗A (1ψΨ ⊗ (m[1](1) )Ψ ) ⊗A (1 ⊗ (m[1](2) )ψ ) · 1
=
m[0] 1ψΨ ⊗A (1 ⊗ (m[1](1) )Ψ ) · 1 ⊗A (1 ⊗ (m[1](2) )ψ ) · 1
(21)
=
m[0] ⊗A (1 ⊗ m[1] ) · 1 ⊗A (1 ⊗ m[2] ) · 1 = ρ̃2 (m),
so ρ̃ is coassociative. Finally, ρ̃ satisfies the counit property if and only if
(22)
m = m[0] (mψ
[1] )1ψ = m[0] (m[1] ).
Remark 3.2. Let (A, C, ψ) be a weak entwining structure. Using (16), we
find that (21) is equivalent to
(22)
ρ2 (m) = m[0] 1ψ ⊗ δ(mψ
[1] ) = m[0] ⊗ δ(m[1] ),
so (20,21) are equivalent to saying that M is a right C-comodule. We then
recover [2, Prop. 2.3(3)].
PARTIAL ENTWINING STRUCTURES
13
4. Partial coactions
Let k be a commutative ring, A a k-algebra and H a k-bialgebra. Consider
a map
ρ : A → A ⊗ H, ρ(a) = a[0] ⊗ a[1] .
To ρ, we associate a map
(23)
ψ : H ⊗ A → A ⊗ H, ψ(h ⊗ a) = a[0] ⊗ ha[1] = aψ ⊗ hψ .
Lemma 4.1. ψ satisfies (10) if and only if
(24)
ρ(ab) = a[0] b[0] ⊗ a[1] b[1] ;
ψ satisfies (11) if and only if
(25)
ρ(1A ) = 1A ⊗ 1H ;
ψ satisfies (12) if and only if
(26)
ρ(a[0] ) ⊗ a[1] = a[0] 1[0] ⊗ a[1](1) 1[1] ⊗ a[1](2) ;
ψ satisfies (13) if and only if
(27)
(a[1] )a[0] = (1[1] )1[0] a;
ψ satisfies (14) if and only if
(28)
(a[1] )a[0] = a;
ψ satisfies (15) if and only if
(29)
ρ(1A ) = (1[1] )1[0] ⊗ 1H ;
ψ satisfies (16) if and only if
(30)
ρ(a[0] ) ⊗ a[1] = a[0] ⊗ δ(a[1] );
ψ satisfies (17) if and only if
(31)
ρ(1A ) = (1[0][1] )1[0][0] ⊗ 1[1] ;
ψ satisfies (18) if and only if
(32)
ρ(1A ) = (1[10 ] )1[00 ] 1[0] ⊗ 1[1] ;
ψ satisfies (19) if and only if
(33)
(1[1] )1[0] = 1A .
Proof. Let us show the equivalence between (12) and (26); the proof of the
other equivalences is similar. (12) holds if and only if
a[0][0] ⊗ h(1) a[0][1] ⊗ h(2) a[1] = a[0] 1[0] ⊗ h(1) a[1](1) 1[1] ⊗ h(2) a[1](2) ,
and this is equivalent with (26).
14
S. CAENEPEEL AND K. JANSSEN
It follows immediately from Lemma 4.1 that (A, H, ψ) is an entwining structure if and only if A is a right H-comodule algebra. It follows also that
(A, H, ψ) is a partial entwining structure if and only if (24,26,28) hold. We
will then say that H coacts partially on A, or that A is a right partial Hcomodule algebra. Similarly, we say that H is a right lax H-comodule algebra
if (A, H, ψ) is a lax entwining structure, i.e. (24,26,27), and (31) or (32) are
satisfied.
Example 4.2. Let e ∈ H be an idempotent such that e ⊗ e = ∆(e)(e ⊗ 1)
and (e) = 1. Then we can define the following partial H-coaction on A = k:
ρ(x) = x ⊗ e ∈ k ⊗k H.
It is straightforward to verify that (24,26,28) hold:
ρ(x)ρ(y) = xy ⊗ e2 = xy ⊗ e = ρ(xy);
ρ(x[0] ) ⊗ x[1] = x ⊗ e ⊗ e = x ⊗ e(1) e ⊗ e(2) = x[0] 1[0] ⊗ x[1](1) 1[1] ⊗ x[1](2) ;
x(e) = x.
Such an idempotent e exists in a finite dimensional semisimple Hopf algebra.
There exists a left integral t such that (t) = 1. t is an idempotent, since
t2 = (t)t = t, and ∆(t)(t ⊗ 1) = t(1) t ⊗ t(2) = (t(1) )t ⊗ t(2) = t ⊗ t.
The proof of our next result is left to the reader.
Proposition 4.3. Let H be a k-bialgebra, C a k-coalgebra, and consider a
map
κ : C ⊗ H → C, κ(c ⊗ h) = c · h,
and define ψ : C ⊗ H → H ⊗ C by the formula
ψ(c ⊗ h) = h(1) ⊗ c · h(2) .
Then (H, C, ψ) is a partial entwining structure if and only if
(34)
(35)
(c · h) · k = c · (hk);
(c · h)(1) · 1H ⊗ (c · h)(2) = c(1) · h(1) ⊗ c(2) · h(2) ;
(36)
C (c · h) = C (c)H (h),
for all c ∈ C, h, k ∈ H. We then call C a right partial H-module coalgebra.
We are now able to define partial Doi-Hopf data.
Proposition 4.4. Let H be a k-bialgebra, A a right partial H-comodule
algebra, and C a right partial H-module coalgebra. Consider the map
ψ : C ⊗ A → A ⊗ C, ψ(c ⊗ a) = a[0] ⊗ c · a[1] .
Then (A, C, ψ) is a partial entwining structure. We will say that (H, A, C)
is a (right-right) partial Doi-Hopf structure.
PARTIAL ENTWINING STRUCTURES
15
Proof. Clearly the conditions (10,14) are satisfied. Let us show that (12)
holds.
ψ
aψ 1Ψ ⊗ (cψ )Ψ
(1) ⊗ (c )(2) = a[0] 1[0] ⊗ (c · a[1] )(1) · 1[1] ⊗ (c · a[1] )(2)
(34)
=
(35)
=
(34)
=
(26)
=
a[0] 1[0] ⊗ ((c · a[1] )(1) · 1H ) · 1[1] ⊗ (c · a[1] )(2)
a[0] 1[0] ⊗ (c(1) · a[1](1) ) · 1[1] ⊗ c(2) · a[1](2)
a[0] 1[0] ⊗ c(1) · (a[1](1) 1[1] ) ⊗ c(2) · a[1](2)
ψ
a[0][0] ⊗ c(1) · a[0][1] ⊗ c(2) · a[1] = aψΨ ⊗ cΨ
(1) ⊗ c(2) .
Remark 4.5. In a similar way, we can define lax H-module coalgebras and
lax Doi-Hopf data.
5. Partial smash products
Let A and B be k-algebras, and R : B ⊗ A → A ⊗ B a k-linear map. We
use the notation
R(b ⊗ a) = aR ⊗ bR = ar ⊗ br .
We assume that A⊗B is a left unital A-bimodule under the action c0 (a⊗b)c =
c0 acR ⊗ bR . Then the following condition is satisfied, for all a, c ∈ A and
b ∈ B (see (10)):
(ac)R ⊗ bR = aR cr ⊗ bRr .
(37)
The map µ : (A ⊗ B) ⊗A (A ⊗ B) → A ⊗ B,
µ((a ⊗ b) ⊗A (c ⊗ d)) = acR ⊗ bR d
is well-defined since
µ((a ⊗ b)a0 ⊗A (c ⊗ d)) = µ((aa0R ⊗ bR ) ⊗A (c ⊗ d)) = aa0R cr ⊗ bRr d
(37)
=
a(a0 c)R ⊗ bR d = µ((a ⊗ b) ⊗A (a0 c ⊗ d)).
A#B will be our notation for A ⊗ B together with the multiplication µ. We
then write
µ((a ⊗ b) ⊗A (c ⊗ d)) = (a#b)(c#d).
We also consider the maps
η = A ⊗ ηB : A → A ⊗ B, η(a) = a ⊗ 1B ;
η = π ◦ η : A → A ⊗ B, η(a) = a1R ⊗ 1R .
Lemma 5.1. Assume that R : B ⊗ A → A ⊗ B satisfies (37).
(1) µ is right A-linear if and only if µ is associative if and only if
(38)
(acR )r ⊗ br dR = aR cr ⊗ (bR d)r ,
for all a, c ∈ A and b, d ∈ B.
16
S. CAENEPEEL AND K. JANSSEN
(2) η is right A-linear if and only if
a ⊗ 1 = aR ⊗ 1R ,
(39)
for all a ∈ A.
(3) η is right A-linear if and only if
a1R ⊗ 1R = aR ⊗ 1R ,
(40)
for all a ∈ A.
Proof. 1) µ is right A-linear if and only if
(a0 #b)((a#d)c) = (a0 #b)(acR #dR ) = a0 (acR )r #br dR
equals
((a0 #b)(a#d))c = (a0 aR #bR d)c = a0 aR cr #(bR d)r ,
for all a0 , a, c ∈ A and b, d ∈ B. This is equivalent to (38). It is obvious that
µ is associative if and only if µ is right A-linear.
2) η is right A-linear if and only if η(a) = a ⊗ 1 equals η(1)a = (1 ⊗ 1)a =
aR ⊗ 1R .
3) η is right A-linear if and only if η(a) = a1R ⊗ 1R equals
(37)
η(1)a = (1R ⊗ 1R )a = 1R ar ⊗ 1Rr = aR ⊗ 1R .
Proposition 5.2. Let A and B be k-algebras, and R : B ⊗ A → A ⊗ B a
k-linear map. The following assertions are equivalent:
(1) (A#B, µ, η) is a left unital weak A-ring;
(2) the conditions (37,38,40) and
(41)
1R ⊗ bR = 1R ⊗ 1R b
are satisfied, for all a, c ∈ A and b, d ∈ B;
(3) (A, B, R) is a weak smash product structure in the sense of [5], that
is, the conditions (37,40,41) and
(42)
aRr ⊗ br dR = aR ⊗ (bd)R
are satisfied, for all a, c ∈ A and b, d ∈ B.
Proof. (1) ⇒ (2). (37,38,40) follow from Lemma 5.1. From (8), it follows
that
(1#b)1 = 1R #bR
equals
(37)
(1R #1R )(1#b) = 1R 1r #1Rr b = 1R #1R b,
and (41) follows.
(2) ⇒ (1). If (37,38,40) hold, then we only need to verify (8), by Lemma 5.1.
PARTIAL ENTWINING STRUCTURES
17
We compute that
(37)
(1R #1R )(a#b) = 1R ar #1Rr b = aR #1R b
(40)
=
(41)
a1R #1R b = a1R #bR = (a#b)1;
(a#b)(1R #1R ) = a1Rr #br 1R = a(11R )r #br 1R
(38)
=
(37)
a1R 1r #(bR 1)r = a1R 1r #bRr = a1R #bR = (a#b)1.
(2) ⇒ (3). Replacing b by bd in (41), we obtain
1R ⊗ (bd)R = 1R ⊗ 1R bd.
(43)
Taking a = 1 in (38), we obtain
(38)
(41)
cRr ⊗ br dR = 1R cr ⊗ (bR d)r = 1R cr ⊗ (1R bd)r
(43)
=
(37)
1R cr ⊗ (bd)Rr = cR ⊗ (bd)R ,
and (42) follows.
(3) ⇒ (2). We have to show that (38) holds. Indeed,
(37)
0
(42)
(acR )r ⊗ br dR = ar cRr0 ⊗ brr dR = ar cR ⊗ (br d)R .
Proposition 5.3. Let A and B be k-algebras, and R : B ⊗ A → A ⊗ B a
k-linear map. The following assertions are equivalent:
(1) (A#B, µ, η) is an A-ring;
(2) (A#B, µ, η) is a left unital weak A-ring;
(3) (A, B, R) is a smash product structure; this means that the following
conditions hold: (37,39,42) and
1 ⊗ b = 1R ⊗ bR ,
(44)
for all b ∈ B.
Proof. (1) ⇒ (2) is trivial.
(2) ⇒ (3). It follows from Lemma 5.1 that (37,38,39) hold. Using (8), we
find that
(39)
1R #bR = (1#b)1 = (1#1)(1#b) = 1R #1R b = 1#b,
proving (44). Taking a = 1 in (38) and using (44), we find (42).
(3) ⇒ (1) is well-known (and easy to prove).
Proposition 5.4. Let A and B be k-algebras, and R : B ⊗ A → A ⊗ B a
k-linear map. The following assertions are equivalent:
(1) (A#B, µ, η) is a left unital lax A-ring;
(2) the conditions (37,38,40) and
(45)
a1R ⊗ bR = (a1r )R ⊗ 1R br
are fulfilled, for all a, c ∈ A and b, d ∈ B;
18
S. CAENEPEEL AND K. JANSSEN
(3) the conditions (37,38,40) and
a1R ⊗ bR = aR 1r ⊗ (1R b)r
(46)
are fulfilled, for all a, c ∈ A and b, d ∈ B.
We then say that (A, B, R) is a lax smash product structure.
Proof. (1) ⇒ (2). (37,38,40) follow from Lemma 5.1. Using (7), we find
0
(37)
a1R #bR = (1r #1r )(a1R #bR ) = 1r (a1R )r0 #1rr bR = (a1R )r #1r bR ,
so (45) is satisfied.
(2) ⇒ (3). We compute that
(38)
a1R #bR = (a1R )r #1r bR = aR 1r #(1R b)r .
(3) ⇒ (1). It follows from the above computations that
a1R #bR = (1r #1r )(a1R #bR ).
We also have
0
(a1R #bR )(1r #1r ) = a1R 1rr0 #bRr 1r
(37)
(38)
(37)
= a(11r )R #bR 1r = a1R 1r #bRr = a1R #bR ,
as needed.
Proposition 5.5. Let A and B be k-algebras, and R : B ⊗ A → A ⊗ B a
k-linear map. The following assertions are equivalent:
(1) (A#B, µ, η) is a left unital lax A-ring;
(2) (A, B, R) is a lax smash product structure and
(47)
1 ⊗ 1 = 1 R ⊗ 1R ;
(3) the conditions (37,38,39) are satisfied.
We then say that (A, B, R) is a partial smash product structure.
Proof. (1) ⇒ (2). Let (A#B, µ, η) be a left unital lax A-ring. It follows
from Lemma 5.1 that (39) holds. (47) follows after we take a = 1 in (39).
(47) implies that η = η, so (A#B, µ, η) is a left unital lax A-ring.
(2) ⇒ (1) follows also from the fact that (47) implies that η = η.
(1) ⇒ (3) follows immediately from Lemma 5.1.
(3) ⇒ (1). We have to show that (7) holds:
(37)
(a1R #bR )(1#1) = a1R 1r #bRr = a1R #bR ;
(39)
(1#1)(a1R #bR ) = (a1R )r #1r bR = a1R #bR .
Proposition 5.6. (A, B, R) is a smash product structure if and only if it is
at the same time a weak and partial smash product structure.
PARTIAL ENTWINING STRUCTURES
19
Proof. One implication is obvious. Conversely, if (A, B, R) is a weak smash
product structure, then (37,40,41,42) are satisfied (cf. Proposition 5.2). If
(A, C, ψ) is a partial smash product structure, then (39) holds (cf. Proposition 5.5) and (44) can be computed as follows:
(41)
(47)
1R #bR = 1R #1R b = 1#b.
Theorem 5.7. Let A be a k-algebra, and C a finitely generated projective
k-coalgebra. Then there is a one-to-one correspondence between lax (resp.
partial) entwining structures of the form (A, C, ψ) and lax (resp. partial)
smash product structures of the form (Aop , C ∗ , R).
Proof. Let {ci , c∗i | i = 1, . . . , n} be a dual basis for C. Then it is well-known
(see for example [8, (1.5)]) that
X
X
(48)
∆(ci ) ⊗ c∗i =
ci ⊗ cj ⊗ c∗i ∗ c∗j .
i
i,j
We also have an isomorphism of k-modules
Hom(C ⊗ A, A ⊗ C) ∼
= Hom(C ∗ ⊗ A, A ⊗ C ∗ ).
The isomorphism can be described as follows. If R : C ∗ ⊗ A → A ⊗ C ∗
corresponds to ψ : C ⊗ A → A ⊗ C, then
X
∗
R(c∗ ⊗ a) = aR ⊗ (c∗ )R =
(49)
hc∗ , cψ
i iaψ ⊗ ci ;
i
ψ
ψ(c ⊗ a) = aψ ⊗ c =
(50)
X
h(c∗i )R , ciaR ⊗ ci .
i
Assume that (A, C, ψ) is a lax entwining structure; we will show that
(Aop , C ∗ , R) is a lax smash product structure. The multiplication in Aop will
be denoted by a dot: a · b = ba. We have to show that R satisfies (37,38,40)
and (45).
X
∗
aR · br ⊗ (c∗ )Rr = br aR ⊗ (c∗ )Rr =
h(c∗ )R , cψ
i ibψ aR ⊗ ci
i
=
X
(10)
X
∗ Ψ
hc∗j , cψ
i ihc , cj ibψ aΨ
i,j
=
⊗ c∗i =
X
∗
hc∗ , cψΨ
i ibψ aΨ ⊗ ci
i
∗
∗ R
∗ R
hc∗ , cψ
i i(ba)ψ ⊗ ci = (ba)R ⊗ (c ) = (a · b)R ⊗ (c ) ;
i
∗ r
(a · bR )r ⊗ (c ) ∗ (d∗ )R = (bR a)r ⊗ (c∗ )r ∗ (d∗ )R
X
∗ r
∗
=
hd∗ , cψ
i i(bψ a)r ⊗ (c ) ∗ ci
i
=
X
i,j
∗ Ψ
∗
∗
hd∗ , cψ
i ihc , cj i(bψ a)Ψ ⊗ cj ∗ ci
20
S. CAENEPEEL AND K. JANSSEN
(48)
=
X
(10)
=
X
(12)
=
X
(10)
=
X
=
X
=
X
∗ Ψ
∗
hd∗ , cψ
i(2) ihc , ci(1) i(bψ a)Ψ ⊗ ci
i
0
∗
∗ ΨΨ
0
hd∗ , cψ
i(2) ihc , ci(1) ibψΨ aΨ ⊗ ci
i
0
ψ ΨΨ
∗
∗
hd∗ , (cψ
i )(2) ihc , (ci )(1) ibψ 1Ψ aΨ0 ⊗ ci
i
ψ Ψ
∗
∗
hd∗ , (cψ
i )(2) ihc , (ci )(1) ibψ aΨ ⊗ ci
i
ψ
∗ Ψ
∗
∗
hd∗ , (cψ
i )(2) ihc , cj ihcj , (ci )(1) ibψ aΨ ⊗ ci
i,j
∗ Ψ
∗
hc∗j ∗ d∗ , cψ
i ihc , cj ibψ aΨ ⊗ ci
i,j
br aR ⊗ ((c∗ )R ∗ d∗ )r = aR · br ⊗ ((c∗ )R ∗ d∗ )r ;
X
∗
a · 1R ⊗ R = 1R a ⊗ R =
h, cψ
i i1ψ a ⊗ ci
=
i
(13)
=
X
h, cψ
i iaψ
⊗ c∗i = aR ⊗ R ;
i
∗ R
a · 1R ⊗ (c ) = 1R a ⊗ (c∗ )R =
X
∗
hc∗ , cψ
i i1ψ a ⊗ ci
i
Ψ
∗ ψ
h, ci(1) ihc , ci(2) i1Ψ 1ψ a
(18)
=
X
(13)
=
X
(48)
=
X
=
X
=
(1r a)R ⊗ R ∗ (c∗ )r = (a · 1r )R ⊗ R ∗ (c∗ )r .
⊗ c∗i
i
∗ ψ
∗
h, cΨ
i(1) ihc , ci(2) i(1ψ a)Ψ ⊗ ci
i
∗ ψ
∗
∗
h, cΨ
i ihc , cj i(1ψ a)Ψ ⊗ ci ∗ cj
i,j
∗
∗ r
h, cΨ
i i(1r a)Ψ ⊗ ci ∗ (c )
i
If (A, C, ψ) is a partial entwining structure, then (Aop , C ∗ , R) is a partial
smash product structure. It suffices to show that (47) holds.
X
∗
1R ⊗ R =
h, cψ
i i1ψ ⊗ ci
i
(19)
=
X
h, ci i1 ⊗ c∗i = 1 ⊗ .
i
Conversely, if (Aop , C ∗ , R) is a lax, resp. partial smash product structure,
then (A, C, ψ) is a lax, resp. partial entwining structure. The computations
are similar to the ones above, and are left to the reader.
PARTIAL ENTWINING STRUCTURES
21
Remark 5.8. Theorem 5.7 also holds for (weak) entwining structures versus
(weak) smash product structures. We refer to [8, Theorem 8] and to [5].
Proposition 5.9. Assume that C is finitely generated and projective as a
k-module. Let (A, C, ψ) be a lax entwining structure, and (Aop , C ∗ , R) the
corresponding lax smash product structure. Then ∗ (A ⊗ C)op is isomorphic
to Aop #C ∗ as left unital lax Aop -rings, and ∗ (A ⊗ C)op is isomorphic to
Aop #C ∗ as Aop -rings. Consequently the categories Aop #C ∗ M and M(ψ)C
A
are isomorphic.
Proof. We know from Section 2 that ∗ (A ⊗ C)op ∼
= #(C, A)op , with multiplication
(f • g)(c) = g(c(2) )ψ f (cψ
(1) )
in #(A, C)op . The map
α : Aop ⊗ C ∗ → Hom(C, A), α(a#c∗ )(c) = ahc∗ , ci
is an isomorphism of k-modules since C is finitely generated and projective.
The first statement follows after we show that α preserves the multiplication.
α((a#c∗ )(b#d∗ ))(c) = α(bR a#(c∗ )R ∗ d∗ )(c)
X
∗
∗
= bR ah(c∗ )R ∗ d∗ , ci =
hc∗ , cψ
i ibψ ahci ∗ d , ci
=
X
∗
hc
i
ψ
∗
, ci ibψ ahci , c(1) ihd∗ , c(2) i
∗
= bψ ahc∗ , cψ
(1) ihd , c(2) i
i
∗
∗
= (α(b#d∗ )(c(2) ))ψ α(a#c∗ )(cψ
(1) ) = (α(a#c ) • α(b#d ))(c).
Applying Proposition 1.2 we see that
∗
(A ⊗ C)op ∼
= (1A · ∗ (A⊗C))op = ∗ (A⊗C)op ·1A ∼
= (Aop #C ∗ )·1A = Aop #C ∗ .
6. Partial actions
Let k be a commutative ring, A a k-algebra and H a k-bialgebra. Consider
a map
κ : H ⊗ A → A, κ(h ⊗ a) = h · a.
To κ, we associate a map
(51)
R : H ⊗ A → A ⊗ H, R(h ⊗ a) = h(1) · a ⊗ h(2) = aR ⊗ hR .
Lemma 6.1. R satisfies (37) if and only if
(52)
h · (ac) = (h(1) · a)(h(2) · c);
R satisfies (38) if and only if
(53)
h · (a(k · c)) = (h(1) · a)((h(2) k) · c);
R satisfies (39) if and only if
(54)
1H · a = a;
22
S. CAENEPEEL AND K. JANSSEN
R satisfies (40) if and only if
(55)
a(1H · 1A ) = 1H · a;
R satisfies (41) if and only if
(56)
h · 1A = (h)1H · 1A ;
R satisfies (42) if and only if
(57)
h · (k · a) = (hk) · a;
R satisfies (44) if and only if
h · 1A = (h)1A ;
(58)
R satisfies (45) if and only if
(59)
a(h · 1A ) = 1H · (a(h · 1A ));
R satisfies (46) if and only if
(60)
a(h · 1A ) = (1H · a)(h · 1A );
R satisfies (47) if and only if
(61)
1H · 1A = 1A .
Proof. Let us show the equivalence between (38) and (53); the proof of the
other equivalences is similar. (38) holds if and only if
h(1) · (a(k(1) · c)) ⊗ h(2) k(2) = (h(1) · a)((h(2) k(1) ) · c) ⊗ h(3) k(2) ,
and this is equivalent with (53).
Remark 6.2. If (52) holds, then (53) is equivalent to
(62)
h · (k · a) = (h(1) · 1A )((h(2) k) · a).
It follows immediately from Lemma 6.1 that (A, H, R) is a smash product
structure if and only if A is a left H-module algebra. It follows also that
(A, H, R) is a partial smash product structure if and only if (52,62,54) hold.
We will then say that H acts partially on A, or that A is a left partial Hmodule algebra. Likewise we call A a left lax H-module algebra if (A, H, R) is
a lax smash product structure, i.e. (52,62,55), and (59) or (60) are satisfied.
We will investigate the former notion in the particular situation where H =
kG is a group algebra. We will recover the partial group actions introduced
in [13] and generalized in [6].
PARTIAL ENTWINING STRUCTURES
23
Partial group actions. Let G be a group, and A a k-algebra. A partial action
of G on A consists of a set of idempotents {eσ | σ ∈ G} ⊂ A, and a set of
isomorphisms ασ : eσ−1 A → eσ A such that
e1 = 1A ; α1 = A,
and
(63)
(64)
(65)
eσ αστ (eτ −1 σ−1 a) = ασ (eσ−1 ατ (eτ −1 a));
ασ (eσ−1 ab) = ασ (eσ−1 a)ασ (eσ−1 b);
ασ (eσ−1 ) = eσ ,
for all σ, τ ∈ G and a, b ∈ A. This slightly generalizes the
[13] and [6]: in [13], it is assumed that A is commutative
isomorphisms ασ are multiplicative; in [6], it is assumed that,
eσ is central and ασ is multiplicative. In both cases (64)
automatically satisfied.
definitions in
and that the
for all σ ∈ G,
and (65) are
Proposition 6.3. Let A be a k-algebra, and G a group. Then there is a
bijective correspondence between partial G-actions and partial kG-actions on
A.
Proof. Assume first that kG acts partially on A. For each σ ∈ G, let
eσ = σ · 1A .
Take a = c = 1A in (52); then it follows that e2σ = eσ . It follows from (54)
that e1 = 1 · 1A = 1A . From (62), it follows that
σ · (τ · a) = eσ ((στ ) · a).
(66)
We then compute
σ · eσ−1 = σ · (σ −1 · 1A ) = eσ 1A = eσ ,
(67)
and
(52)
σ · (eσ−1 a) = (σ · eσ−1 )(σ · a) = eσ (σ · a).
(68)
It follows that the map A → A, a 7→ σ · a restricts to a map
ασ : eσ−1 A → eσ A.
Observe that
(69)
(68)
(52)
σ · (eσ−1 a) = eσ (σ · a) = (σ · 1A )(σ · a) = σ · a.
Now
(68)
(69)
ασ−1 (ασ (eσ−1 a) = ασ−1 (eσ (σ · a)) = σ −1 · (σ · a)
(66)
=
(54)
eσ−1 ((σ −1 σ) · a) = eσ−1 a.
In a similar way, we find that ασ (ασ−1 (eσ a)) = eσ a, and it follows that
ασ : eσ−1 A → eσ A is an isomorphism. It is also clear that
(54)
α1 (a) = 1 · a = a,
24
S. CAENEPEEL AND K. JANSSEN
and
(67)
ασ (eσ−1 ) = σ · (eσ−1 ) = eσ .
(64) can be shown as follows:
ασ (eσ−1 a)ασ (eσ−1 b) = (σ · (eσ−1 a))(σ · (eσ−1 b))
(52)
= (σ · eσ−1 )(σ · a)(σ · eσ−1 )(σ · b) = eσ (σ · a)eσ (σ · b)
(52)
(69)
= (σ · 1A )(σ · a)(σ · 1A )(σ · b) = σ · (ab) = ασ (eσ−1 ab).
We are left to prove that (63) holds:
(69)
ασ (eσ−1 ατ (eτ −1 a)) = σ · (τ · a)
(66)
(69)
= eσ ((στ ) · a) = eσ αστ (eτ −1 σ−1 a).
Conversely, assume that G acts partially on A, and define an action of kG
on A by extending
σ · a = ασ (eσ−1 a) ∈ eσ A
linearly to kG. This defines a partial action of kG on A, since
(64)
σ · (ab) = ασ (eσ−1 ab) = ασ (eσ−1 a)ασ (eσ−1 b) = (σ · a)(σ · b);
(63)
σ · (τ · a) = ασ (eσ−1 ατ (eτ −1 a)) = eσ αστ (eτ −1 σ−1 a) = eσ ((στ ) · a);
1 · a = α1 (e1 a) = α1 (a) = a.
It is easy to check that condition (65) establishes the bijectivity of the correspondence.
A Frobenius property. Let i : R → S be a ring homomorphism. Recall
that i is called Frobenius (or we say that S/R is Frobenius) if there exists
a Frobenius system (ν,
This consists of an R-bimodule map ν : S → R
P e).
and P
an element e P
=
e1 ⊗R e2 ∈ S ⊗R S such that se = es, for all s ∈ S,
and
ν(e1 )e2 = e1 ν(e2 ) = 1.
A Hopf algebra H over a commutative ring k is Frobenius if and only if it is
finitely generated projective, and the space of integrals is free of rank one.
If H is Frobenius, then there exists a left integral t ∈ H and a left integral
ϕ ∈ H ∗ such that
(70)
hϕ, ti = 1.
The Frobenius system is (ϕ, t(2) ⊗ S(t(1) )). In particular, we have
(71)
hϕ, t(2) iS(t(1) ) = t(2) hϕ, S(t(1) )i = 1H .
For a detailed discussion, we refer to the literature, see for example [8, Sec.
3.2].
If t ∈ H is a left integral, then it is easy to prove that
(72)
t(2) ⊗ S(t(1) )h = ht(2) ⊗ S(t(1) ),
for all h ∈ H (see [8, Prop. 58] for a similar statement).
Assume that A is a left H-module algebra, and that H is Frobenius. Then
the ring homomorphism A → A#H is also Frobenius (see [8, Prop. 5.1]).
Similar properties hold for a module algebra over a weak Hopf algebra and
PARTIAL ENTWINING STRUCTURES
25
for an algebra with a partial group action (see [6, 7]). Our aim is now to
prove such a statement for a partial module algebra over a Frobenius Hopf
algebra H. Assume that we have an action of H on an algebra A satisfying
(52,62,54). The smash product A#H has multiplication rule
(73)
(a#h)(b#k) = a(h(1) · b)#h(2) k,
and A#H is the subalgebra generated by the elements of the form (a#h)1A =
a(h(1) · 1A )#h(2) .
Proposition 6.4. Let H be a Frobenius Hopf algebra, let t and ϕ be as
above, and take a left partial H-module algebra A. Suppose that h · 1A is
central in A, for every h ∈ H, and that t satisfies the following cocommutativity property:
(74)
t(1) ⊗ t(2) ⊗ t(3) ⊗ t(4) = t(1) ⊗ t(3) ⊗ t(2) ⊗ t(4) .
Then A#H/A is Frobenius, with Frobenius system
(ν = (A#ϕ) ◦ ι, e = (1A #t(2) )1A ⊗A (1A #S(t(1) ))1A ),
where ι : A#H → A#H is the inclusion map.
Proof. Applying ∆ to the first tensor factor of (74), we see that
(75)
t(1) ⊗ t(2) ⊗ t(3) ⊗ t(4) ⊗ t(5) = t(1) ⊗ t(2) ⊗ t(4) ⊗ t(3) ⊗ t(5) .
For all a ∈ A and h ∈ H, we have
(1A #t(2) )1A ⊗A (1A #S(t(1) ))1A (a#h)1A
=
(1A #t(2) ) ⊗A (1A #S(t(1) ))(a#h)1A
=
(1A #t(2) ) ⊗A ((1A #S(t(1) ))(a(h(1) · 1A )#h(2) ))1A
=
=
(1A #t(3) ) ⊗A (S(t(2) ) · (a(h(1) · 1A ))#S(t(1) )h(2) )1A
t(3) · (S(t(2) ) · (a(h(1) · 1A )))#t(4) ⊗A (1A #S(t(1) )h(2) )1A
(t(3) · 1A )((t(4) S(t(2) )) · (a(h(1) · 1A )))#t(5) ⊗A (1A #S(t(1) )h(2) )1A
(t(4) · 1A )((t(3) S(t(2) )) · (a(h(1) · 1A )))#t(5) ⊗A (1A #S(t(1) )h(2) )1A
(t(2) · 1A )a(h(1) · 1A )#t(3) ⊗A (1A #S(t(1) )h(2) )1A
a(h(1) · 1A )(t(2) · 1A )#t(3) ⊗A (1A #S(t(1) )h(2) )1A
a(h(1) · 1A )((h(2) t(2) ) · 1A )#h(3) t(3) ⊗A (1A #S(t(1) ))1A
=
(a(h(1) · 1A )#h(2) t(2) )1A ⊗A (1A #S(t(1) ))1A
=
(a#h)(1A #t(2) ) ⊗A (1A #S(t(1) ))1A
=
(a#h)1A (1A #t(2) )1A ⊗A (1A #S(t(1) ))1A .
=
(62)
=
(75)
=
=
=
(72)
Using the fact that ϕ is a left integral, we easily find that
(54)
ν((a#h)1A ) = hϕ, h(2) ia(h(1) · 1A ) = hϕ, hia(1H · 1A ) = hϕ, hia.
26
S. CAENEPEEL AND K. JANSSEN
The left A-linearity of ν is obvious, and the right A-linearity can be established as follows:
ν((a#h)1A b) = ν((a#h)b1A ) = ν((a(h(1) · b)#h(2) )1A )
=
(54)
=
hϕ, h(2) ia(h(1) · b) = hϕ, hia(1H · b)
hϕ, hiab = ν((a#h)1A )b.
Finally,
ν(1A #t(2) )1A )((1A #S(t(1) ))1A ) = (hϕ, t(2) i1A #S(t(1) ))1A
(71)
=
(1A #1H )1A = 1A #1H ;
(1A #t(2) )ν((1A #S(t(1) ))1A ) = (1A #t(2) )hϕ, S(t(1) )i1A
(71)
=
(1A #1H )1A = 1A #1H .
Remark 6.5. It follows from (74) that t is cocommutative. Obviously (74)
is satisfied if H is cocommutative.
7. Galois theory
Let (A, C, ψ) be a lax entwining structure, and consider the corresponding
A-coring C = A ⊗ C. The aim is to give a structure theorem for lax entwined
modules, based on the Galois theory for corings. To this end, we first study
the grouplike elements of C.
Proposition 7.1. Let (A, C, ψ) be a lax entwining structure, and g ∈ G(C).
The element x = 1ψ ⊗g ψ satisfies the equation ∆(x) = x⊗A x. x is grouplike
in the following situations:
• (A, C, ψ) is a partial entwining structure;
• C = H is a weak bialgebra, A is a right H-comodule algebra in the
sense of [1] or [5], and ψ : H ⊗ A → A ⊗ H is given by the formula
ψ(h ⊗ a) = a[0] ⊗ ha[1] , and g = 1H .
Proof.
ψ
∆(x) = (1ψ ⊗ (g ψ )(1) ) ⊗A (1 ⊗ (g ψ )(2) ) = (1ψ 1Ψ ⊗ (g ψ )Ψ
(1) ) ⊗A (1 ⊗ (g )(2) )
(12)
(10)
0
=
(1ψΨ ⊗ g Ψ ) ⊗A (1 ⊗ g ψ ) = (1Ψ 1ψΨ0 ⊗ g ΨΨ ) ⊗A (1 ⊗ g ψ )
=
(1Ψ ⊗ g Ψ ) ⊗A (1ψ ⊗ g ψ ) = x ⊗A x.
If (A, C, ψ) is a partial entwining structure, then
(19)
ε(x) = (g ψ )1ψ = (g)1 = 1.
If A is a comodule algebra over a weak bialgebra H, then A is, in particular,
an H-comodule (see [1] or or [5]). Then x = 1[0] ⊗1[1] , and ε(x) = (1[1] )1[0] =
1 (see also [7, Lemma 2.1]).
PARTIAL ENTWINING STRUCTURES
27
The situation where C = H is a weak bialgebra has been studied in [7]. Let
us here focus attention to the situation where (A, C, ψ) is a partial entwining
structure. We keep the notation from Proposition 7.1. Then A ∈ M(ψ)C
A,
with coaction
ρ(a) = aψ ⊗ g ψ .
Let
T = AcoC = {b ∈ A | b1ψ ⊗ g ψ = bψ ⊗ g ψ }.
We have a morphism of corings
can : A ⊗T A → A ⊗ C, can(a ⊗ b) = abψ ⊗ g ψ .
From [4, Sec. 1 and Prop. 3.8] and [18, Sec. 3] we obtain immediately the
following.
Proposition 7.2. Let (A, C, ψ) be a partial entwining structure, and g ∈
G(C). We have a pair of adjoint functors (F, G) between the categories MT
coC , and F (N ) = N ⊗ A with coaction ρ(n ⊗ a) =
and M(ψ)C
T
T
A . G = (−)
(n ⊗T aψ ) ⊗ g ψ . The following conditions are equivalent:
(1) can is an isomorphism and A is faithfully flat as a left T -module;
(2) (F, G) is an equivalence of categories and A is flat as a left T -module;
(3) A ⊗ C is flat as a left A-module, and A is a projective generator of
M(ψ)C
A.
In this situation, we will say that A is a faithfully flat partial coalgebra-Galois
extension of T .
From now on, we assume that C is finitely generated and projective as
a k-module, with finite dual basis {(ci , c∗i ) | i = 1, . . . , n}. If there exists
g ∈ G(C), then C is a k-progenerator: C is a generator, because (g) = 1 (see
for example [10, I.1] for a discussion of (pro)generator modules). Suppose
in addition that A is finitely generated and projective as a left T -module.
Then can is an isomorphism if and only if its left dual
∗
can : ∗ (A ⊗ C) ∼
= #(C, A) → ∗ (A ⊗T A) ∼
= T End(A)op
is an isomorphism. Viewed as a map #(C, A) → T End(A)op , ∗ can is given
by the formula ∗ can(f )(a) = aψ f (g ψ ). Composing ∗ can with the isomorphism ∗ (A ⊗ C)op ∼
= Aop #C ∗ (see Proposition 5.9), we obtain an Aop -ring
isomorphism θ : Aop #C ∗ → T End(A). We compute the map θ explicitly:
X
∗
θ((a#c∗ ) · 1)(b) = θ(1R a#(c∗ )R )(b) = θ(
1ψ a#hc∗ , cψ
i ici )(b)
i
=
X
∗
bΨ 1ψ ahc
∗ Ψ
, cψ
i ihci , g i
(10)
= bΨ 1ψ ahc∗ , g Ψψ i = bψ ahc∗ , g ψ i.
i
Recall (see [9, Sec. 3]) that we can associate a Morita context (T, ∗ C, A, Q, τ, µ)
to an A-coring C with a fixed grouplike element x. We will now compute this Morita context for C = A ⊗ C and x = 1ψ ⊗ g ψ , in the case
where (A, C, ψ) is a partial entwining structure. First recall that Q = {q ∈
28
S. CAENEPEEL AND K. JANSSEN
∗C
| c(1) q(c(2) ) = q(c)x, for all c ∈ C}. We first compute Q as a submodule
of #(C, A). q ∈ #(C, A) satisfies the equation
q(c) = 1ψ q(cψ ),
(76)
for all c ∈ C. Let ϕ be the map in ∗ (A ⊗ C) corresponding to q. For
γ = a1ψ ⊗ cψ ∈ A ⊗ C, we have that
ψ
∆(γ) = (a1ψΨ ⊗ cΨ
(1) ) ⊗A (1 ⊗ c(2) ),
hence q ∈ Q if and only if
ψ
ψ
ΨΨ
γ(1) ϕ(γ(2) ) = (a1ψΨ ⊗ cΨ
(1) )q(c(2) ) = a1ψΨ q(c(2) )Ψ0 ⊗ c(1)
(10)
0
(76)
Ψ
Ψ
a(1ψ q(cψ
(2) ))Ψ ⊗ c(1) = aq(c(2) )Ψ ⊗ c(1)
=
equals
ϕ(γ)x = a1ψ q(cψ )(1Ψ ⊗ g Ψ ) = aq(c)1ψ ⊗ g ψ ,
for all a ∈ A and c ∈ C. We conclude that Q is the submodule of #(C, A)
consisting of the maps q that satisfy (76) and
ψ
q(c(2) )ψ ⊗ cψ
(1) = q(c)1ψ ⊗ g ,
(77)
for all c ∈ C.
NowP
we want to describe Q as a submodule of Aop #C ∗ ∼
= #(C, A)op . Take
k = j aj #d∗j ∈ Aop #C ∗ corresponding to q ∈ #(C, A)op . Then
X
X
(78)
aj #d∗j =
1R aj #(d∗j )R ,
j
j
where R is the map from the partial smash product structure corresponding
to (A, C, ψ), cf. Theorem 5.7. Then k ∈ Q if and only if
X
X
ajψ hd∗j , c(2) i ⊗ cψ
aj hd∗j , ci1ψ ⊗ g ψ ,
(1) =
j
j
for all c ∈ C. This is equivalent to stating that
X
X
∗
ajψ hd∗j , c(2) ihc∗ , cψ
ajψ hd∗j , c(2) ihc∗ , cψ
i ihci , c(1) i
(1) i =
j
i,j
(49)
=
X
ajR hd∗j , c(2) ih(c∗ )R , c(1) i
=
j
X
ajR h(c∗ )R ∗ d∗j , ci
j
equals
X
aj 1ψ hd∗j , cihc∗ , g ψ i =
j
X
∗
aj 1ψ hd∗j , cihc∗ , cψ
i ihci , gi
i,j
(49)
=
X
j
aj 1R hd∗j , cih(c∗ )R , gi,
PARTIAL ENTWINING STRUCTURES
29
for all
c∗ ∈ C ∗ . We conclude that Q consists of the elements
P c ∈ C ∗ and op
k = j aj #dj ∈ A #C ∗ satisfying (78) and
X
X
(79)
ajR #((c∗ )R ∗ d∗j ) =
aj 1R #h(c∗ )R , gid∗j ,
j
j
for all c∗ ∈ C ∗ .
It follows from [9, Lemma 3.1] that Q is a (#(C, A), T )-bimodule. The left
action is given by the multiplication in #(C, A). We also know (cf. [9, Prop.
2.2]) that A is a (T, #(C, A))-bimodule, with right #(C, A)-action given by
the formula a · f = aψ f (g ψ ). We have well-defined maps
τ : A ⊗#(C,A) Q → T, τ (a ⊗ q) = a · q = aψ q(g ψ );
µ : Q ⊗T A → #(C, A), µ(q ⊗ a)(c) = q(c)a.
(T, #(C, A), A, Q, τ, µ) is a Morita context. The map τ is surjective if and
only if there exists q ∈ Q such that q(g) = 1.
Theorem 7.3. Let (A, C, ψ) be a partial entwining structure, g ∈ G(C),
and assume that C is finitely generated and projective as a k-module. Then
the following assertions are equivalent.
(1)
(2)
(3)
(4)
A is a faithfully flat partial coalgebra-Galois extension of T ;
θ is an isomorphism and A is a left T -progenerator;
the Morita context (T, #(C, A), A, Q, τ, µ) is strict;
(F, G) is an equivalence of categories.
Proof. Since C is finitely generated projective as a k-module, A⊗C is finitely
generated and projective as a left A-module. Being a direct factor of A ⊗ C,
A ⊗ C is also finitely generated and projective as a left A-module. A ⊗ C is
a left A-generator since
(14)
ε(1ψ ⊗ g ψ ) = 1ψ (g ψ ) = 1(g) = 1.
It follows that A ⊗ C is a left A-progenerator, and the result then follows
immediately from [4, Theorem 4.7].
We now consider the situation where C = H is a finitely generated projective
Hopf algebra, g = 1H , A is a right partial H-comodule algebra, and ψ is
given by the formula (23). We will compute the corresponding partial smash
product structure (Aop , H ∗ , R) (see Theorem 5.7), and show that it comes
from a left partial H ∗cop -action on Aop , given by the formula
h∗ *a = hh∗ , a[1] ia[0] .
Proposition 7.4. With notation and assumptions as above, Aop is a left
partial H ∗cop -module algebra, and (Aop , H ∗ , R) is the corresponding smash
product structure, as discussed in Section 6.
30
S. CAENEPEEL AND K. JANSSEN
Proof. We compute R using (49):
X
R(h∗ ⊗ a) =
hh∗ , hi a[1] ia[0] ⊗ h∗i
i
=
X
hh∗(1) , hi ihh∗(2) , a[1] ia[0] ⊗ h∗i = h∗(2) *a ⊗ h∗(1) .
i
It follows that R is given by formula (51), starting from the Hopf algebra
H ∗cop . From Theorem 5.7, it follows that (Aop , H ∗ , R) is a partial smash
product structure. Hence, by definition, Aop is a left partial H ∗cop -module
algebra. It is also possible to verify (52,62,54) directly.
Assume that H is Frobenius. Then H ∗cop is also Frobenius. Assume, moreover, that
a1[0] ⊗ 1[1] = 1[0] a ⊗ 1[1] and hϕ, hklmi = hϕ, hlkmi,
for all a ∈ A and h, k, l, m ∈ H. Then it follows from Proposition 6.4
that Aop #H ∗cop /Aop is Frobenius. The Morita context (T, #(H, A) ∼
=
op
op
∗cop
, A, Q, τ, µ) is the Morita context associated to the A -ring
A #H
Aop #H ∗cop , see [9, Theorem 3.5]. It follows from [9, Theorem 2.7] that
Q∼
= A as k-modules. So we conclude that the Morita context is of the form
(T, Aop #H ∗cop , A, A, τ, µ).
References
[1] G. Böhm, Doi-Hopf modules over weak Hopf algebras, Comm. Algebra 28 (2000),
4687–4698.
[2] T. Brzeziński, The structure of corings. Induction functors, Maschke-type theorem,
and Frobenius and Galois properties, Algebr. Representat. Theory 5 (2002), 389–410.
[3] T. Brzeziński and R. Wisbauer, “Corings and comodules”, London Math. Soc. Lect.
Note Ser. 309, Cambridge University Press, Cambridge, 2003.
[4] S. Caenepeel, Galois corings from the descent theory point of view, Fields Inst. Comm
43 (2004), 163–186.
[5] S. Caenepeel and E. De Groot, Modules over weak entwining structures, Contemp.
Math. 267 (2000), 31–54.
[6] S. Caenepeel, E. De Groot, Corings applied to partial Galois theory, in ”Proceedings
of the International Conference on Mathematics and its Applications, ICMA 2004”,
S.L. Kalla and M.M. Chawla (Eds.), Kuwait University, Kuwait, 2005, 117–134.
[7] S. Caenepeel, E. De Groot, Galois theory for weak Hopf algebras, Rev. Roumaine
Math. Pures Appl., to appear.
[8] S. Caenepeel, G. Militaru and Shenglin Zhu, “Frobenius and separable functors for
generalized module categories and nonlinear equations”, Lect. Notes in Math. 1787,
Springer Verlag, Berlin, 2002.
[9] S. Caenepeel, J. Vercruysse and Shuanhong Wang, Morita theory for corings and cleft
entwining structures, J. Algebra 276 (2004), 210–235.
[10] F. DeMeyer, E. Ingraham, Separable algebras over commutative rings, Lecture Notes
in Math. 181, Springer Verlag, Berlin, 1971.
[11] M. Dokuchaev, R. Exel, and P. Piccione, Partial representations and partial group
algebras, J. Algebra 226 (2000), 251–268.
PARTIAL ENTWINING STRUCTURES
31
[12] M. Dokuchaev and R. Exel, Associativity of crossed products by partial actions,
enveloping actions and partial representations, Trans. Amer. Math. Soc. 357 (2005),
1931–1952.
[13] M. Dokuchaev, M. Ferrero, and A. Pacques, Partial Galois theory of commutative
rings, J. Pure Appl. Algebra, to appear.
[14] M. Dokuchaev, N. Zhukavets, On finite degree partial representations of groups, J.
Algebra 274 (2004), 309–334.
[15] R. Exel, Twisted partial actions: a classification of regular C ∗ -algebraic bundels,
Proc. London Math. Soc. 74 (1997), 417–443.
[16] M. E. Sweedler, The predual Theorem to the Jacobson-Bourbaki Theorem, Trans.
Amer. Math. Soc. 213 (1975), 391–406.
[17] R. Wisbauer, Weak corings, J. Algebra 245 (2001), 123–160.
[18] R. Wisbauer, On Galois corings, in “Hopf algebras in non-commutative geometry and
physics”, Caenepeel S. and Van Oystaeyen, F. (eds.), Lect. Notes Pure Appl. Math.
239, Dekker, New York, 2004.
Faculty of Engineering, Vrije Universiteit Brussel, B-1050 Brussels, Belgium
E-mail address: [email protected]
URL: http://homepages.vub.ac.be/~scaenepe/
Faculty of Engineering, Vrije Universiteit Brussel, B-1050 Brussels, Belgium
E-mail address: [email protected]
URL: http://homepages.vub.ac.be/~krjansse/