Gorenstein dimensions for weak Hopf-Galois extensions

Wang Zhongwei

(School of Mathematics, Southeast University, Nanjing 211189, China)(School of Science, Jinling Institute of Technology, Nanjing 211169, China)

AbstractThe representation of weak Hopf algebras is studied by investigating the Gorenstein dimensions of weak Hopf algebras and weak Hopf-Galois extensions. Let H be a weak Hopf algebra with a bijective antipode, A a weak right H-comodule algebra and B the H-coinvariant subalgebra of A. First, some properties of Gorenstein projective H-modules in the representation category are studied, and the fact that Gorenstein global dimension of H is the same as the Gorenstein projective dimension of its left unital subalgebra is demonstrated. Secondly, by applying the integral theory of weak Hopf algebras, on the one hand, a sufficient and necessary condition that a projective A-module is a projective B-module is given; on the other hand, the separability of the functor AB- and that of the restriction of scalar function B(-) are described, respectively. Finally, as a mean result, the Gorenstein global dimension of a weak Hopf-Galois extension is investigated under the condition that H is both semisimple and cosemisimple.

Key wordsweak Hopf algebra; integral; weak Hopf-Galois extension; Gorenstein dimension

The study of Gorenstein projective modules can be traced back to Ref.[1], where the G-dimension of a finitely generated module over a two-sided Noetherian ring was introduced. Furthermore, the definition of Gorenstein projective modules was given in Ref.[2]. We knew already that a module of G-dimension zero is actually a Gorenstein projective module. Gorenstein projective modules play an important role in many areas. For example, they are widely used in the representation theory of Artin algebras, the theory of stable and singularity categories, and the cohomology theory of commutative rings, and so on.

Weak bialgebras and weak Hopf algebras introduced in Ref.[3] generalized the ordinary bialgebras and Hopf algebras by weakening the comultiplication of unit and the multiplication of counit. Comultiplication is allowed to be non-unital, but it is still coassociative. In exchange for coassociativity, the multiplicativity of the counit is replaced by a weaker condition, implying that the unit representation is not necessarily one-dimensional and irreducible. Weak Hopf algebras can provide us with a good framework for studying the symmetries of certain quantum field theories. Groupoid algebras, face algebras and generalized Kac algebras are examples of weak Hopf algebras.

The main purpose of this paper is to study the representation of weak Hopf algebras by investigating the Gorenstein dimensions of weak Hopf algebras and weak Hopf-Galois extensions. Let H be a weak Hopf algebra with a bijective antipode, A a weak right H-comodule algebra and B the H-coinvariant subalgebra of A. After recalling some basic definitions and giving a summary of the fundamental properties concerned with weak Hopf algebras, we study some properties of Gorenstein projective H-modules in representation category, and find that the Gorenstein global dimension of H is the same as the Gorenstein projective dimension of its left unital subalgebra. By applying the integral theory of weak Hopf algebras, on the one hand, we give a sufficient and necessary condition that a projective A-module is a projective B-module; on the other hand, we describe the separability of the functor AB- and that of the restriction of scalar function B(-). Consequently, we investigate the Gorenstein global dimension of a weak Hopf-Galois extension.

1 Preliminaries

Throughout this article, k denotes a fixed field, and we will always work over k. The tensor product ⊗:=⊗k and Hom-functor are always assumed to be over k. We also use Sweedler’s notations for the terminologies on coalgebras and comodules. For a coalgebra C, we write the comultiplication Δ(c)=∑c1c2 for any cC. For a right C-comodule M, we denote its coaction by ρ(m)=∑m(0)m(1) for any mM. For any unexplained definitions and notations, one may refer to Ref.[4] or Ref.[5].

Definition 1[3] A weak Hopf algebra H is an algebra (H,μ,η) and a coalgebra (H,Δ,ε) such that

Δ(xy)=Δ(x)Δ(y)

(1)

ε(xyz)=∑ε(xy1)ε(y2z)=∑ε(xy2)ε(y1z) (2)

Δ2(1H)=(Δ(1H)⊗1H)(1HΔ(1H))=

(1HΔ(1H))(Δ(1H)⊗1H)

(3)

and there exists a linear map S: HH, called an antipode, satisfying

(4)

for all x, y, zH, where Δ(1H)=∑11⊗12,

Let H be a weak Hopf algebra. The images Ht=εt(h) and Hs=εs(h) of the projections εt,εs: HH defined by

εt(h)=∑ε(11h)12, εs(h)=∑11ε(h12)

are both separable subalgebras of H and commute with each other[3]. Ht and Hs are called left and right unital subalgebras, respectively.

Definition 2[3] A left integral in H is an element l∈H satisfying hl=εt(h)lfor all hH. Furthermore, if εt(l)=1H, then it is said to be normalized. A normalized right integral is defined similarly. A left or right integral in H is called non-degenerate if it defines a non-degenerate functional on H*, the dual space of H.

The spaces of left and right integrals in H are denoted as and respectively.

S(hl1)⊗l 2=∑l1hl 2

(5)

for all hH. Meanwhile, according to Ref.[6], the left integral λ satisfies the following invariant properties for all h,gH,

h1λ(gh2)=∑λ(g2h)S(g1)

(6)

If a weak Hopf algebra H is finite dimensional, then it has a bijective antipode S[6], in which inverse is denoted as S-1 in the following, and there exist non-degenerate left integrals such that ∑l1λ(l 2)=1H[7]. Furthermore, the quasi-basis of λ is ∑l2S-1(l1)[3]. Therefore, for all hH,

λ(S-1(l)h)=ε(h)

(7)

Let H be a weak Hopf algebra with an antipode S. According to Refs.[8-9], we have

(8)

(9)

(10)

(11)

Definition 3[10] Let H be a weak Hopf algebra, and A a right H-comodule, which is also an associative algebra. We call A a weak right H-comodule algebra if

ρ(ab)=ρ(a)ρ(b)

(12)

a1(0)⊗1(1)=∑a(0)εt(a(1))

(13)

for all a,bA.

Let H be a weak Hopf algebra, and A a weak right H-comodule algebra. Then, according to Ref.[8], we obtain that

a1(0)εs(1(1))

(14)

Define the H-coinvariant subalgebra of A as

Then, we know from Ref.[11] that

Definition 4[12] Let A be a weak right H-comodule algebra and B the H-coinvariant subalgebra of A. The extension A/B is said to be weak Hopf-Galois, if the canonical map

β:ABAAsH, β(aBb)=∑ab(0)sb(1)

is an isomorphism, where ⊗s:=⊗Hs is the relative tensor product over Hs is a right Hs-module via y·a=∑ε(ya(1))a(0) for all yHs, aA, and H is a left Hs-module via its multiplication).

2 Gorenstein Global Dimensions for Weak Hopf Algebras

For a ring R, we denote the class of projective left R-modules by P, and for an object M in RM, the category of left R-modules, we denote the projective and injective dimension of M by p.dimRM and i.dimRM, respectively.

Definition 5[13] A left R-module M is Gorenstein projective if there exists an RHom(-,P)-exact sequence

…→P1P0P0P1→…

such that M=Ker(P0P1), where every Pi and Pi are projective.

Dually, Gorenstein injective left R-modules can be defined.

Definition 6 For a left R-module M, the Gorenstein projective dimension G.p.dimRM is at most n if there is an exact sequence

0→GnGn-1→…→G1G0M→0

where every Gi is Gorenstein projective.

Dually, the Gorenstein injective dimension G.i.dimRM can be defined.

For any ring R, Ref.[14] shows us that

sup{G.p.dimRM|MRM}=sup{G.i.dimRM|MRM}

The common value is called the left Gorenstein global dimension of R and denoted as G.gl.dim(R).

We know that G.gl.dim(R)=0 if and only if the ring R is quasi-Frobenius[15]. In addition, R is left Gorenstein hereditary if every submodule of a projective left R-module is Gorenstein projective[16], i.e., G.gl.dim(R)≤1.

In what follows, we always assume that H is a weak Hopf algebra with a bijective antipode S. Then, the left H-module category HM, called the representation category, is an abelian monoidal category[17-18] such that

Ht is the unit object with a left H-action via h·x=εt(hx) for all hH and xHt;

• For M,NHM, the tensor product is MtN:=MHtN, where the right Ht-module structure on M is defined by m·x=S-1(xm for all mM and xHt;

• The left H-module structure on MtN is defined by the following diagnosing action h·(mtn)=h1·mth2·n, for all hH, mM, nN;

• For M,NHM, a homomorphism between M and N is left H-linear.

Proposition 1 If P is a Gorenstein projective left H-module, then so is PtX for any left H-module X.

Proof If P is a Gorenstein projective left H-module, then there is an HHom(-,P)-exact sequence

P:…→P1P0P0P1→…

such that M=Ker(P0P1), where every Pi and Pi are projective. As Ht is separable, we can obtain an exact sequence

PtX:…→PtXP0tXP0tXP1tX→…

such that MtX=Ker(P0tXP1tX). Meanwhile, every PitX and PitX are projective left H-modules[19]. For any projective left H-module Q,

HHom(PtX,Q)≅HtHom(X,HHom(P,Q))

Hence, HHom(PtX,Q) is exact, as desired.

Theorem 1 Let H be a weak Hopf algebra with a bijective antipode S. Then, G.gl.dim(H)=G.p.dimHHt.

Proof Obviously, G.gl.dim(H)≥G.p.dimHHt. Hence, we shall prove the reverse inequality. Assume that G.p.dimHHt=n<+∞. Then, there is an exact sequence

0→GnGn-1→…→G1G0Ht→0

where every Gi is Gorenstein projective. For any left H-module X, we obtain an exact sequence

0→GntXGn-1tX→…→G1tX

G0tXHttX→0

As HttXX, and every GitX is Gorenstein projective by Proposition 1, we obtain G.gl.dim(H)≤n. This shows that G.gl.dim(H)≤G.p.dimHHt.

3 Gorenstein Global Dimensions for Weak Hopf-Galois Extensions

Throughout this section,H is always assumed to be a weak Hopf algebra with a bijective antipode S, unless otherwise stated. Then, let be two non-degenerate left integrals such that ∑l1λ(l2)=1H, and we fix a weak Hopf-Galois extension A/B and use the following formal notation for the inverse of β for all hH,

β-1(1Ash)=∑ili(h)⊗Bri(h)∈ABA

such that

∑∑ili(h)ri(h)(0)sri(h)(1)=1Ash (15)

by definition. Such elements enjoy the following properties.

Lemma 1[20] For all aA and hH, we have

ili(h)ri(h)=∑ε(h1(1))1(0)

∑∑ili(h)⊗Bri(h)(0)sri(h)(1)=

∑∑ili(h1)⊗Bri(h1)⊗sh2

∑∑ili(h)(0)Bri(h)⊗sli(h)(1)=

∑∑ili(h2)⊗Bri(h2)⊗sS(h1)

Consider the two functors:

AB-:BMAM, NABN

B(-):AMBM, MBM

where B(-) is the restriction of the scalars functor.

Lemma 2 (AB-,B(-)) and (B(-),AB-) are double adjunctions.

Proof Note that the element ∑λ(a(1))a(0)B[21] for aA. Then, for all NBM, we have a well-defined map φ:ABNBHom(A,N) given by

φ(aBn)(b)=∑λ(b(1)a(1))b(1)a(0)·n

a,bA, nN

Then, it is easy to check that φ is a morphism of left A-modules, where BHom(A,N)∈AM via (a·f)(b)=f(ba) for all a,bA and fBHom(A,N). Meanwhile, we claim that φ is a bijection with the inverse given by

φ:BHom(A,N)→ABN

φ(f)=∑li(S-1(l ))⊗Bf(ri(S-1(l )))

Indeed, on the one hand, for all a,bA and nN, by Lemma 1, we have

φφ(aBn)=

∑∑ili(S-1(l ))⊗Bλ(ri(S-1a(1))ri(S-1a(0)·n=

∑∑ili(S-1(l ))ri(S-1a(0)λ(ri(S-1a(1))⊗Bn=

∑∑ili(S-1(l 2))ri(S-1(12))a(0)λ(S-1(l 1)a(1))⊗Bn=

∑1(0)a(0)λ(S-1(l )1(1)a(1))⊗Bn

On the other hand, for all bA and fBHom(A,N), by Lemma 1, we have

φφ(f)(b)=

∑∑iλ(b(1)li(S-1(l ))(1))b(0)li(S-1(l ))(0)·

f(ri(S-1(l )))n=

∑∑iλ(b(1)l 2)f(b(0)li(S-1(l 1))ri(S-1(l 1)))=

λ(l 2)ε(S-1(l 1)b(1)1(1))f(b(0)1(0))=

λ(l 2)ε(S-1(l 1)b(1))f(b(0))n=f(b)

Hence, the adjoint isomorphism theorem, (AB-,B(-)) and (B(-),AB-) are double adjunctions[12].

By Lemma 2, we have the following assertion.

Corollary 1 If PBM is projective, then ABPAM is projective.

Lemma 3 If H is semisimple and PAM, then P is projective as a left A-module if and only if P is projective as a left B-module.

Proof As H is semisimple, we know that H is finite dimensional and there is which is normalized[3], i.e., εs(J)=1H. Then, for all aA,

iali(J)⊗Bri(J)=∑ili(J)⊗Bri(J)a

(16)

In fact, by Lemma 1, we have

∑∑iali(J)ri(J)(0)sri(J)(1)=

∑∑iali(J1)ri(J1)⊗s2J2=

as needed.

Consider that P is a projective left B-module and let M,NAM. Suppose that δ:MN and ξ:PN are left A-module morphisms such that δ is surjective. Since P is projective as a left B-module, there is a left B-module morphism f:PM such that Define

·f(ri(J)·p)

for all pP.

Obviously, is a morphism of left A-modules by (16). Moreover,

ili(J)ri(J)·ξ(p)=∑ε(J1(1))1(0)·ξ(p)=

ε(εs(J)1(1))1(0)·ξ(p)=∑ε(1(1))1(0)·ξ(p)=

1A·ξ(p)=ξ(p)

where the third equality follows[8]. Hence, Thus, P is projective as a left A-module.

Conversely, suppose that P is projective as a left A-module. It follows from Lemma 2 that (AB-,B(-)) is an adjoint pair. Since A is projective as a right B-module[22], we obtain that the functor AB- is exact. Hence, B(-) preserves projective objects. Therefore, P is projective as B-module.

Definition 7[23] Let C and D be categories. A covariant functor F:C→D is separable if for all objects M,NC, there are maps satisfying the following conditions:

1) For α∈HomC(M,N), we have

2) Given M′,N′∈C, f∈HomD(F(M),F(N)),g∈HomD(F(M′),F(N′)), α∈HomC(M,M′), β∈HomC(N,N′), we have

Lemma 4 1) If H is semisimple, then B(-) is separable.

2) If H* is semisimple, then AB- is separable.

Proof 1) Let J∈ such that εs(J)=1H. By the proof of Lemma 3, we can know that the element ∑ili(J)⊗Bri(J) is exactly the separability idempotent, i.e., the extension A/B is separable. Hence, the restriction of scalars functor B(-) is separable[23].

2) Note that A is a weak left H*-module algebra under the action φa=∑φ(a(1))a(0) for aA, φH*[24]. As H* is semisimple, there exists a normalized left integral Then, λ⇀1A=1A, and the map F:AB defined by F(a)=λa is a B-bimodule projection[21]. This assumes that B is a direct summand of A as a B-bimodule. Hence, the unit of the adjunction (AB-,B(-)) is a split monomorphism[25]. So, the induction function AB- is separable[11].

Corollary 2 1) If H is semisimple, then M is a left A-module direct summand of ABM for all MAM.

2) If H* is semisimple, then N is a left B-module direct summand of ABN for all NBM.

Proof 1) As H is semisimple, we know from Lemma 4 that B(-) is separable. Hence, the counit : of the adjunction (AB-,B(-)) is a cosplit epimorphism[11], that is, there is a natural transformation for all MAM. Thus, M is a left A-module direct summand of ABM.

2) As H* is semisimple, we have that AB- is separable by Lemma 4. Hence, we also know that the counit of the adjunction (B(-),AB-) is a cosplit epimorphism[11]. Thus, N is a left B-module direct summand of ABN for all NBM.

Lemma 5 If NBM is Gorenstein projective, then ABNAM is Gorenstein projective.

Proof Suppose that N is a Gorenstein projective left B-module. Then, there is a BHom(-,P)-exact sequence

P:…→P1P0P0P1→…

such that N=Ker(P0P1), where every Pi and Pi are projective. Since A is projective as a right B-module, we obtain that ABP is exact and ABN=Ker(ABP0ABP1). We also obtain that ABPi is projective for every i because of the assertion that B(-) is exact and AB- is a left adjoint[12].

Let us suppose finally that QAM is Gorenstein projective. Then,

AHom(ABP,Q)≅BHom(P,Q)

However, BQ is projective since B(-) is a left adjoint of AB- which is exact. Thus, BHom(P,Q) is exact since N is Gorenstein projective, and so, AHom(ABP,Q) is also exact, which implies that ABN is Gorenstein projective.

Theorem 2 If H is a semisimple and cosemisimple weak Hopf algebra, then G.gl.dim(A)=G.gl.dimB.

Proof Assume that G.gl.dimB=n<+∞. For any MAM, as a left B-module, there is a Gorenstein projective resolution:

0→GnGn-1→…→G1G0M→0

where every Gi is Gorenstein projective. Since the functor AB- is exact, it induces a left A-module exact sequence

0→ABGnABGn-1→…→

ABG1ABG0ABM→0

From Lemma 5, we know that every ABGi is Gorenstein projective, and thus, G.gl.dimA(ABM)≤n. Since M is a direct summand of ABM as left A-modules by Corollary 2, G.gl.dimAMn[26]. Hence, G.gl.dim(A)≤n.

Suppose that G.gl.dim(A)=qn=G.gl.dimB. Then, G.gl.dimB(ABN)≤q for any NBM. Therefore, BExti(ABN,U)=0 for all i>q and all projective left B-module U[26]. Since N is a left B-module direct summand of ABN and the functor BExt(-,U) preserves finite direct sums, BExt(N,U)=0 for all i>q and all projective left B-module U, and, hence, G.gl.dimBNq. This implies that G.gl.dim(A)≤G.gl.dimB. Therefore, in view of the above discussion, we have G.gl.dim(A)=G.gl.dimB.

Corollary 3 Let H be a semisimple and cosemisimple weak Hopf algebra. Then, A is quasi-Frobenius (rep. left Gorenstein hereditary) if and only if so is B.

In particular, if R#H is a weak smash product of a weak left H-module algebra R (see Ref.[24] for the definitions), then R#H is quasi-Frobenius (rep. left Gorenstein hereditary) if and only if so is R.

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弱Hopf-Galois扩张的Gorenstein维数

王忠伟

(东南大学数学学院, 南京 211189)(金陵科技学院理学院, 南京 211169)

摘要:通过讨论弱Hopf代数和弱Hopf-Galois扩张的Gorenstein整体维数,研究了弱Hopf代数的表示. 设H是带有双射对积的弱Hopf代数,A是弱右H-余模代数,BA的余不变子代数. 首先,通过讨论Gorenstein投射H-模在表示范畴中的性质,证明了H的Gorenstein整体维数等于其左单位子代数的Gorenstein投射维数;其次,利用弱Hopf代数的积分理论,给出了投射A-模是投射B-模的刻画,并讨论了函子AB-和标量函子的限制B(-)的可分性;最后,研究了H是半单且余半单弱Hopf代数条件下的弱Hopf-Galois扩张的Gorenstein整体维数.

关键词:弱Hopf代数;积分;弱Hopf-Galois扩张;Gorenstein维数

DOI:10.3969/j.issn.1003-7985.2020.04.014

Received 2020-03-30,Revised 2020-06-20.

BiographyWang Zhongwei (1984—), male, doctor, associate professor, wangzhongwei@jit.edu.cn.

Foundation items:The National Natural Science Foundation of China (No.11601203), the China Postdoctoral Science Foundation (No.2018M642128), Qing Lan Project of Jiangsu Province, the Natural Science Foundation of Jiangsu Province (No.BK20150113).

CitationWang Zhongwei. Gorenstein dimensions for weak Hopf-Galois extensions[J].Journal of Southeast University (English Edition),2020,36(4):483-488.DOI:10.3969/j.issn.1003-7985.2020.04.014.

中图分类号:O153.3