亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        Gorenstein dimensions for weak Hopf-Galois extensions

        2021-01-12 12:17:16

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

        Abstract:The 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 A?B- 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 words:weak Hopf algebra; integral; weak Hopf-Galois extension; Gorenstein dimension

        The study of Gorenstein projective modules can be traced back to Ref.[1], where theG-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 ofG-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. LetHbe a weak Hopf algebra with a bijective antipode,Aa weak rightH-comodule algebra andBtheH-coinvariant subalgebra ofA. After recalling some basic definitions and giving a summary of the fundamental properties concerned with weak Hopf algebras, we study some properties of Gorenstein projectiveH-modules in representation category, and find that the Gorenstein global dimension ofHis 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 projectiveA-module is a projectiveB-module; on the other hand, we describe the separability of the functorA?B- and that of the restriction of scalar functionB(-). Consequently, we investigate the Gorenstein global dimension of a weak Hopf-Galois extension.

        1 Preliminaries

        Throughout this article,kdenotes a fixed field, and we will always work overk. The tensor product ?:=?kand Hom-functor are always assumed to be overk. We also use Sweedler’s notations for the terminologies on coalgebras and comodules. For a coalgebraC, we write the comultiplicationΔ(c)=∑c1?c2for anyc∈C. For a rightC-comoduleM, we denote its coaction byρ(m)=∑m(0)?m(1)for anym∈M. For any unexplained definitions and notations, one may refer to Ref.[4] or Ref.[5].

        Definition1[3]A weak Hopf algebraHis 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)(1H?Δ(1H))=

        (1H?Δ(1H))(Δ(1H)?1H)

        (3)

        and there exists a linear mapS:H→H, called an antipode, satisfying

        (4)

        LetHbe a weak Hopf algebra. The imagesHt=εt(h) andHs=εs(h) of the projectionsεt,εs:H→Hdefined by

        εt(h)=∑ε(11h)12,εs(h)=∑11ε(h12)

        are both separable subalgebras ofHand commute with each other[3].HtandHsare called left and right unital subalgebras, respectively.

        Definition2[3]A left integral inHis an element l∈Hsatisfyinghl=εt(h)lfor allh∈H. Furthermore, ifεt(l)=1H, then it is said to be normalized. A normalized right integral is defined similarly. A left or right integral inHis called non-degenerate if it defines a non-degenerate functional onH*, the dual space ofH.

        ∑S(hl1)?l2=∑l1?hl2

        (5)

        ∑h1λ(gh2)=∑λ(g2h)S(g1)

        (6)

        ∑λ(S-1(l)h)=ε(h)

        (7)

        LetHbe a weak Hopf algebra with an antipodeS. According to Refs.[8-9], we have

        (8)

        (9)

        (10)

        (11)

        Definition3[10]LetHbe a weak Hopf algebra, andAa rightH-comodule, which is also an associative algebra. We callAa weak rightH-comodule algebra if

        ρ(ab)=ρ(a)ρ(b)

        (12)

        ∑a1(0)?1(1)=∑a(0)?εt(a(1))

        (13)

        for alla,b∈A.

        LetHbe a weak Hopf algebra, andAa weak rightH-comodule algebra. Then, according to Ref.[8], we obtain that

        ∑a1(0)?εs(1(1))

        (14)

        Define theH-coinvariant subalgebra ofAas

        Then, we know from Ref.[11] that

        Definition4[12]LetAbe a weak rightH-comodule algebra andBtheH-coinvariant subalgebra ofA. The extensionA/Bis said to be weak Hopf-Galois, if the canonical map

        β:A?BA→A?sH,β(a?Bb)=∑ab(0)?sb(1)

        2 Gorenstein Global Dimensions for Weak Hopf Algebras

        For a ringR, we denote the class of projective leftR-modules by P, and for an objectMinRM, the category of leftR-modules, we denote the projective and injective dimension ofMbyp.dimRMandi.dimRM, respectively.

        Definition5[13]A leftR-moduleMis Gorenstein projective if there exists anRHom(-,P)-exact sequence

        …→P1→P0→P0→P1→…

        such thatM=Ker(P0→P1), where everyPiandPiare projective.

        Dually, Gorenstein injective leftR-modules can be defined.

        Definition6For a leftR-moduleM, the Gorenstein projective dimension G.p.dimRMis at mostnif there is an exact sequence

        0→Gn→Gn-1→…→G1→G0→M→0

        where everyGiis Gorenstein projective.

        Dually, the Gorenstein injective dimension G.i.dimRMcan be defined.

        For any ringR, Ref.[14] shows us that

        sup{G.p.dimRM|M∈RM}=sup{G.i.dimRM|M∈RM}

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

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

        In what follows, we always assume thatHis a weak Hopf algebra with a bijective antipodeS. Then, the leftH-module categoryHM, called the representation category, is an abelian monoidal category[17-18]such that

        ?Htis the unit object with a leftH-action viah·x=εt(hx) for allh∈Handx∈Ht;

        ? ForM,N∈HM, the tensor product isM?tN:=M?HtN, where the rightHt-module structure onMis defined bym·x=S-1(x)·mfor allm∈Mandx∈Ht;

        ? The leftH-module structure onM?tNis defined by the following diagnosing actionh·(m?tn)=h1·m?th2·n, for allh∈H,m∈M,n∈N;

        ? ForM,N∈HM, a homomorphism betweenMandNis leftH-linear.

        Proposition1IfPis a Gorenstein projective leftH-module, then so isP?tXfor any leftH-moduleX.

        ProofIfPis a Gorenstein projective leftH-module, then there is anHHom(-,P)-exact sequence

        P:…→P1→P0→P0→P1→…

        such thatM=Ker(P0→P1), where everyPiandPiare projective. AsHtis separable, we can obtain an exact sequence

        P?tX:…→P?tX→P0?tX→P0?tX→P1?tX→…

        such thatM?tX=Ker(P0?tX→P1?tX). Meanwhile, everyPi?tXandPi?tXare projective leftH-modules[19]. For any projective leftH-moduleQ,

        HHom(P?tX,Q)?HtHom(X,HHom(P,Q))

        Hence,HHom(P?tX,Q) is exact, as desired.

        Theorem1LetHbe a weak Hopf algebra with a bijective antipodeS. Then, G.gl.dim(H)=G.p.dimHHt.

        ProofObviously, 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→Gn→Gn-1→…→G1→G0→Ht→0

        where everyGiis Gorenstein projective. For any leftH-moduleX, we obtain an exact sequence

        0→Gn?tX→Gn-1?tX→…→G1?tX→

        G0?tX→Ht?tX→0

        AsHt?tX?X, and everyGi?tXis 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

        β-1(1A?sh)=∑ili(h)?Bri(h)∈A?BA

        such that

        ∑∑ili(h)ri(h)(0)?sri(h)(1)=1A?sh(15)

        by definition. Such elements enjoy the following properties.

        Lemma1[20]For alla∈Aandh∈H, 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:

        A?B-:BM→AM,NA?BN

        B(-):AM→BM,MBM

        whereB(-) is the restriction of the scalars functor.

        Lemma2(A?B-,B(-)) and (B(-),A?B-) are double adjunctions.

        ProofNote that the element ∑λ(a(1))a(0)∈B[21]fora∈A. Then, for allN∈BM, we have a well-defined mapφ:A?BN→BHom(A,N) given by

        φ(a?Bn)(b)=∑λ(b(1)a(1))b(1)a(0)·n

        a,b∈A,n∈N

        Then, it is easy to check thatφis a morphism of leftA-modules, whereBHom(A,N)∈AMvia (a·f)(b)=f(ba) for alla,b∈Aandf∈BHom(A,N). Meanwhile, we claim thatφis a bijection with the inverse given by

        φ:BHom(A,N)→A?BN

        φ(f)=∑li(S-1(l ))?Bf(ri(S-1(l )))

        Indeed, on the one hand, for alla,b∈Aandn∈N, by Lemma 1, we have

        φφ(a?Bn)=

        ∑∑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(l2))ri(S-1(12))a(0)λ(S-1(l1)a(1))?Bn=

        ∑1(0)a(0)λ(S-1(l )1(1)a(1))?Bn

        On the other hand, for allb∈Aandf∈BHom(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)l2)f(b(0)li(S-1(l1))ri(S-1(l1)))=

        ∑λ(l2)ε(S-1(l1)b(1)1(1))f(b(0)1(0))=

        ∑λ(l2)ε(S-1(l1)b(1))f(b(0))n=f(b)

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

        By Lemma 2, we have the following assertion.

        Corollary1IfP∈BMis projective, thenA?BP∈AMis projective.

        Lemma3IfHis semisimple andP∈AM, thenPis projective as a leftA-module if and only ifPis projective as a leftB-module.

        ∑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.

        for allp∈P.

        ∑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)

        Conversely, suppose thatPis projective as a leftA-module. It follows from Lemma 2 that (A?B-,B(-)) is an adjoint pair. SinceAis projective as a rightB-module[22], we obtain that the functorA?B- is exact. Hence,B(-) preserves projective objects. Therefore,Pis projective asB-module.

        Lemma41) IfHis semisimple, thenB(-) is separable.

        2) IfH*is semisimple, thenA?B- is separable.

        Corollary21) IfHis semisimple, thenMis a left A-module direct summand ofA?BMfor allM∈AM.

        2) IfH*is semisimple, thenNis a leftB-module direct summand ofA?BNfor allN∈BM.

        Proof1) AsHis semisimple, we know from Lemma 4 thatB(-) is separable. Hence, the counit:of the adjunction (A?B-,B(-)) is a cosplit epimorphism[11], that is, there is a natural transformationfor allM∈AM. Thus,Mis a leftA-module direct summand ofA?BM.

        Lemma5IfN∈BMis Gorenstein projective, thenA?BN∈AMis Gorenstein projective.

        ProofSuppose thatNis a Gorenstein projective leftB-module. Then, there is aBHom(-,P)-exact sequence

        P:…→P1→P0→P0→P1→…

        such thatN=Ker(P0→P1), where everyPiandPiare projective. SinceAis projective as a rightB-module, we obtain thatA?BPis exact andA?BN=Ker(A?BP0→A?BP1). We also obtain thatA?BPiis projective for everyibecause of the assertion thatB(-) is exact andA?B- is a left adjoint[12].

        Let us suppose finally thatQ∈AMis Gorenstein projective. Then,

        AHom(A?BP,Q)?BHom(P,Q)

        However,BQis projective sinceB(-) is a left adjoint ofA?B- which is exact. Thus,BHom(P,Q) is exact sinceNis Gorenstein projective, and so,AHom(A?BP,Q) is also exact, which implies thatA?BNis Gorenstein projective.

        Theorem2IfHis a semisimple and cosemisimple weak Hopf algebra, then G.gl.dim(A)=G.gl.dimB.

        ProofAssume that G.gl.dimB=n<+∞. For anyM∈AM, as a leftB-module, there is a Gorenstein projective resolution:

        0→Gn→Gn-1→…→G1→G0→M→0

        where everyGiis Gorenstein projective. Since the functorA?B- is exact, it induces a leftA-module exact sequence

        0→A?BGn→A?BGn-1→…→

        A?BG1→A?BG0→A?BM→0

        From Lemma 5, we know that everyA?BGiis Gorenstein projective, and thus, G.gl.dimA(A?BM)≤n. SinceMis a direct summand ofA?BMas leftA-modules by Corollary 2, G.gl.dimAM≤n[26]. Hence, G.gl.dim(A)≤n.

        Suppose that G.gl.dim(A)=q≤n=G.gl.dimB. Then, G.gl.dimB(A?BN)≤qfor anyN∈BM. Therefore,BExti(A?BN,U)=0 for alli>qand all projective leftB-moduleU[26]. SinceNis a leftB-module direct summand ofA?BNand the functorBExt(-,U) preserves finite direct sums,BExt(N,U)=0 for alli>qand all projective leftB-moduleU, and, hence, G.gl.dimBN≤q. 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.

        Corollary3LetHbe a semisimple and cosemisimple weak Hopf algebra. Then,Ais quasi-Frobenius (rep. left Gorenstein hereditary) if and only if so isB.

        In particular, ifR#His a weak smash product of a weak leftH-module algebraR(see Ref.[24] for the definitions), thenR#His quasi-Frobenius (rep. left Gorenstein hereditary) if and only if so isR.

        日本在线视频网站www色下载 | 国外亚洲成av人片在线观看| 日本韩国一区二区三区| 在线一区二区三区免费视频观看| 精品一区中文字幕在线观看| 国产女人高潮叫床免费视频| 九九视频免费| 亚洲素人av在线观看| 丰满精品人妻一区二区| 国产精品欧美福利久久| 亚洲成人观看| 日韩字幕无线乱码免费| 性高朝久久久久久久3小时| 97伦伦午夜电影理伦片| 亚洲网站免费看| 爱爱免费视频一区二区三区| 人妻少妇精品无码专区| 成人免费ā片在线观看| 中国老太老肥熟女视频| 最新日本人妻中文字幕| 18禁黄久久久aaa片| 亚洲色成人网一二三区| 亚洲综合小综合中文字幕| 国产极品视觉盛宴| 国产精品麻花传媒二三区别 | 高潮毛片无遮挡高清免费| 中文字幕精品亚洲无线码二区 | 日日摸夜夜添无码无码av| 亚洲AV色欲色欲WWW| 就爱射视频在线视频在线| 闺蜜张开腿让我爽了一夜| 国产精品18久久久久网站| 亚洲av一区二区在线| 国精品人妻无码一区二区三区性色 | 亚洲成av人片乱码色午夜| 久草热8精品视频在线观看| 喷潮出白浆视频在线观看| 手机看片久久第一人妻| 亚洲熟少妇在线播放999| 国产成人精品无码一区二区老年人| 精品国产乱子伦一区二区三|