Research article Special Issues

Representations of a non-pointed Hopf algebra

  • In this paper, we construct all the indecomposable modules of a class of non-pointed Hopf algebras, which are quotient Hopf algebras of a class of prime Hopf algebras of GK-dimension one. Then the decomposition formulas of the tensor product of any two indecomposable modules are established. Based on these results, the representation ring of the Hopf algebras is characterized by generators and some relations.

    Citation: Ruifang Yang, Shilin Yang. Representations of a non-pointed Hopf algebra[J]. AIMS Mathematics, 2021, 6(10): 10523-10539. doi: 10.3934/math.2021611

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  • In this paper, we construct all the indecomposable modules of a class of non-pointed Hopf algebras, which are quotient Hopf algebras of a class of prime Hopf algebras of GK-dimension one. Then the decomposition formulas of the tensor product of any two indecomposable modules are established. Based on these results, the representation ring of the Hopf algebras is characterized by generators and some relations.



    There are a lot of works about classification of Hopf algebras or Nichols algebras of finite GK-dimension. For example, the readers can refer to [1,2]. In the paper [2], Liu tried to classify all prime Hopf algebras of GK-dimension one and constructed a series of new examples of non-pointed Hopf algebras D(m_,d,γ). As a by-product, a series of finite-dimensional non-semisimple quotient Hopf algebras are obtained, which have no Chevalley property. To understand this new class of quotient Hopf algebras, we see that those quotient Hopf algebras under the conditions that n is odd and d=2n, denoted by D(n), are just isomorphic to an extension of the generalized quaternion group algebra kQ4n equipped with a nontrivial suitable coalgebraic structure. It is well known that the representations of the generalized quaternion group Q4n have been known for a long time. In [3,4], all the irreducible representations of Q4n are given. As applications, [5] determined the complex representation rings of Q4n and gave the isomorphism class of the n-th augmentation quotient of the augmentation ideal. In [6] the group code over the generalized quaternion group Q4n is studied, which is based on representations of Q4n. It is important in cryptography.

    The task of this paper is to classify all the indecomposable modules of D(n) explicitly. The decomposition formulas of the tensor products of them are established. Finally, we describe the representation ring of D(n) by generators and generating relations. There is much effort to put into understanding and classifying all indecomposable modules of algebras of finite representation type. The readers can refer to the books [7,8] for the representation theory of algebras and some newest results [9,10] for example. In [11], Yang determined the representation type of a class of pointed Hopf algebras and classified all indecomposable modules of simple-pointed Hopf algebra R(q,α). In the paper [12], the representations of the half of the small quantum group uq(sl2) were constructed by the technique of the deformed preprojective algebras. Furthermore, a lot of papers investigated the representation rings of various Hopf algebras, the readers can refer to [13,14,15,16,17]. By techniques of generators and generating relations, Su and Yang described representation rings of the weak generalized Taft Hopf algebras as well as some small quantum groups in [15,16]. Sun et al. described the representation rings of Drinfeld doubles of Taft algebras in [17]. Motivated by the above works, we shall establish the decomposition formulas of the tensor products of the indecomposable D(n)-modules and determine the representation ring of D(n). This can help us to understand the structure and representation theory of D(n) in a better way.

    The paper is organized as follows. In Section 2, we review the definition of D(n) and show that D(n) is of finite representation type. In Section 3, we shall construct all the indecomposable D(n)-modules and establish all the decomposition formulas of the tensor product of two indecomposable D(n)-modules. In Section 4, we characterize the representation ring of D(n) by three generators and some generating relations.

    For the theories of Hopf algebras and representation theory, we refer to [7,8,18,19].

    Throughout this paper, we work over an algebraic closed field k of characteristic 0. Unless otherwise stated, all algebras, Hopf algebras, and modules are finite-dimensional over k, all maps are k-linear, dim and stand for dimk and k, respectively. In this paper, we describe the representations of a quotient of the Hopf algebra D(m_,d,γ) for the case of m=2.

    Firstly, we review the definition of the Hopf algebra D(2_,d,γ) in [2]. Let 2|d. As an algebra, it is generated by a±1,b±1,c,u0,u1, subject to the following relations

    aa1=a1a=1,bb1=b1b=1,a2d=b2,c2=1a2d, (2.1)
    ab=ba,ac=ca,cb=bc,auk=uka1(k=1,2), (2.2)
    cu0=2u1=ωadu0c,cu1=0=u1c,u0b=a2dbu0,u1b=a2dbu1, (2.3)
    u20=a3d2b,u21=0,u0u1=12ωa3d2cb,u1u0=12a3d2cb, (2.4)

    where ωk is a primitive 4-th root of unity. The comultiplication Δ, the counit ϵ and the antipode S of D(2_,d,γ) are given by

    Δ(a)=aa,Δ(b)=bb,Δ(c)=cb+1c,Δ(u0)=u0u0u1adbu1,Δ(u1)=u0u1+u1adbu0,ϵ(a)=ϵ(b)=ϵ(u0)=1,ϵ(c)=ϵ(u0)=0,S(a)=a1,S(b)=b1,S(c)=cb1,S(u0)=a3d2bu0,S(u1)=ωad2u1.

    From now on, assume that n is odd and d=2n. Let D(n) be the quotient Hopf algebra

    D(n)=:D(2_,d,γ)/(an1).

    We claim that the Hopf algebra D(n) can be viewed as the Hopf algebra generated by x,y,z satisfying the following relations

    x2n=1,y2=0,xn=z2,xy=yx,xz=zx1,yz=ωzy.

    The comultiplication Δ, the counit ϵ and the antipode S are given by

    Δ(x)=xx,Δ(y)=1y+yz2,Δ(z)=zz+yzyz1,
    ϵ(x)=ϵ(z)=1,ϵ(y)=0,S(x)=x1,S(y)=yz2,S(z)=z1.

    Indeed, we define the maps φ and ψ as

    φ:axz2,bz2,c2y,u0z,u1yz

    and

    ψ:xab,y12c,zu0,

    respectively. It is straightforward to check that φ and ψ are Hopf algebra isomorphisms and ψφ=id. Hence we have the claim.

    Now, we use the later generators and relations to define the Hopf algebra D(n). Actually, D(n) is a class of non-pointed Hopf algebras.

    It is noted that the generalized quaternion group algebra kQ4n of order 4n is defined as

    kQ4n=kx,z|x2n=1,xn=z2,xz=zx1.

    Obviously, it can be embedded into the algebra D(n) as an algebra, but not as a Hopf algebra.

    Firstly, we determine the representation type of D(n) as an algebra.

    Lemma 2.1. The algebra D(n) is of finite representation type.

    Proof. Let Q4n be the generalized quaternion group

    x,z|x2n=1,xn=z2,xz=zx1,

    and A=ky|y2=0 a k-algebra. It is obvious that A is of finite representation type. Define

    yx=y,yz=ωy.

    Since (yx)(yx)=0,(yz)(yz)=0, Q4n can be viewed as subgroup of AutAlg(A). Therefore, we have the skew group algebra Q4nA, whose multiplication is given by

    (ha)(kb)=hk(ak)b

    for any h,kQ4n,a,bA.

    It is easy to see that A can be viewed as the subalgebra of Q4nA and

    (x1)(1y)=xy,(1y)(x1)=x(yx)=xy,
    (z1)(1y)=zy,(1y)(z1)=z(yz)=ωzy,

    and D(n)Q4nA as an algebra. Consequently, D(n) is of finite representation type as an algebra by [20,Theorem 1.1,Theorem 1.3(a)].

    In this section, we mainly construct all the indecomposable D(n)-modules and establish their tensor products. It is remarked that the simple modules of the algebra GB are completely understood, and coincide with those of the group G for which B acts as zero (see [21]).

    Firstly we classify all the indecomposable modules of D(n). Let ξk be a primitive 2n-th root of unity.

    Theorem 3.1. (a) There are 4 pairwise non-isomorphic 1-dimensional D(n)-modules Si with basis {vi} for 0i3, the action of D(n) is defined by

    xvi=(1)ivi,yvi=0,zvi=ωivi.

    (b) There are n1 pairwise non-isomorphic 2-dimensional simple D(n)-modules Mj with basis {v1j,v2j} for 1jn1, the action of D(n) is defined by

    xv1j=ξjv1j,xv2j=ξjv2j,yv1j=0,yv2j=0,zv1j=v2j,zv2j=(1)jv1j.

    (c) There are 4 pairwise non-isomorphic 2-dimensional indecomposable projective D(n)-modules Pi with basis {μ1i,μ2i} for 0i3, the action of D(n) is defined by

    xμ1i=(1)iμ1i,xμ2i=(1)i+1μ2i,yμ1i=μ2i,yμ2i=0,zμ1i=ωiμ1i,zμ2i=ωi+1μ2i.

    (d) There are n1 pairwise non-isomorphic 4-dimensional indecomposable projective D(n)-modules Tj with basis {ϑ1j,ϑ2j,ϑ3j,ϑ4j} for 1jn1, the action of D(n) is defined by

    xϑ1j=ξjϑ1j,xϑ2j=ξjϑ2j,xϑ3j=ξjϑ3j,xϑ4j=ξjϑ4j,yϑ1j=ϑ3j,yϑ2j=ϑ4j,yϑ3j=0,yϑ4j=0,zϑ1j=ϑ2j,zϑ2j=(1)jϑ1j,zϑ3j=ωϑ4j,zϑ4j=ω(1)j+1ϑ3j.

    Proof. The results of (a), (b) are showed in [5,6,21].

    Firstly, we construct the 2-dimensional indecomposable non-simple D(n)-modules. Let xμi=λiμi for i=1,2,λik and yμ10. Suppose that yμ1=ˉμ1, it is obvious that ˉμ1 and μ1 are linearly independent. We might let yμ1=ˉμ1=:μ2 as well, then yμ2=0. Since xμ2=x(yμ1)=y(xμ1)=λ1μ2, there is λ2=λ1. Now consider zμ1. If zμ1 and μ1,μ2 are linearly dependent, let zμ1=p1μ1+p2μ2,p1,p2k, then zμ2=z(yμ1)=ωy(zμ1)=ωp1μ2. By z2=xn, it's easy to see (1+ω)p1p2=0 and p21=λn1, so p2=0 for p10. Since λ2n1=1,λn1=p21=±1. When λn1=1, p1=±1, there is λ1=λ11 by xz=zx1, thus λ1=±1. But if λ1=1, then λn1=11, which is a contradiction. Thus λ1=1. Similarly, if λn1=1, then λ1=1, it also gets a contradiction. Hence we get (c).

    Next, let xv1=ξiv1 for some iZ2n, zv1=v2, yv1=v3, here ξ is a primitive 2n-th root of unity. Then

    xv2=x(zv1)=zx1v1=ξizv1=ξiv2

    and

    xv3=ξiv3,yv2=ωzv3,yv3=0,zv2=(1)iv1.

    Obviously, zv30.

    If zv3 and v1,v2,v3 are linearly dependent, let zv3=av1+bv2+cv3,a,b,ck. By xz=zx1, it's easy to get that a=b=0. Since z4=1, we can set zv3=ωkv3 for some kZ4, where ω is a primitive 4-th root of unity, then yv2=ωk+1v3. At this time, the matrices of x,y,z acting on {v1,v2,v3} are

    x(ξi000ξi000ξi),y(0000001ωk+10),z(0(1)i010000ωk),

    respectively. It is directly checked that all the generating relations are satisfied only when i=0 or i=n. If i=0, then

    x(100010001),y(0000001±10),z(01010000ω);

    If i=n, then

    x(100010001),y(0000001±ω0),z(01010000±1).

    Now we use a unified expression to describe such modules Vk with a basis {ν1k,ν2k,ν3k} for 0k3, and the matrices of x,y,z acting on this basis are

    x((1)k000(1)k000(1)k+1),y(0000001ωk0),z(0(1)k010000ωk1),

    respectively. In fact, these modules are decomposable. For, let

    {ω1k:=ωkν1k+ν2k,ω2k:=12((1)kν1k+ωkν2k),ω3k:=ν3k|0k3}

    be another basis, then the matrices of x,y,z acting on {ω1k,ω2k,ω3k} are

    x((1)k000(1)k000(1)k+1),y(000000010),z(ωk000ωk000ωk1),

    respectively. Thus we get that

    Vk=k{ω1k}k{ω2k,ω3k}Sk+2Pk.

    Moreover, if zv3 and v1,v2,v3 are linearly independent, let zv3=v4, then

    xv4=ξiv4,yv2=ωv4,yv4=0,zv4=(1)i+1v3,

    and the matrices of x,y,z acting on {v1,v2,v3,v4} are

    x(ξi0000ξi0000ξi0000ξi),y(0000000010000ω00),z(0(1)i001000000(1)i+10010),

    respectively. We set v4=ωv4 to get the result (d). It is noted that when n<i<2n, let ˉv1:=v2,ˉv2:=(1)iv1,ˉv3:=v4,ˉv4:=(1)iv3, then the matrices of x,y,z acting on this basis are

    x(ξ2ni0000ξi2n0000ξ2ni0000ξi2n),y(0000000010000100),
    z(0(1)i001000000ω(1)i+100ω0),

    respectively. Therefore when n<i<2n, the modules are isomorphic to the case of 2ni. Furthermore, when i=0,

    we choose the basis

    {ˉv1:=v1+v2,ˉv2:=v3+v4,ˉv3:=v1v2,ˉv4:=v3v4},

    then the matrices of x,y,z acting on this basis are

    x(1000010000100001),y(0000100000000010),z(10000ω000010000ω),

    respectively. Hence it is decomposable and isomorphic to P0P2. Similarly, for the case i=n, the module is decomposable and isomorphic to P1P3. Indeed, we choose the basis

    {ˉv1:=v1+ωv2,ˉv2:=v3+ωv4,ˉv3:=v1ωv2,ˉv4:=v3ωv4},

    then the matrices of x,y,z acting on this basis are

    x(1000010000100001),y(0000100000000010),z(ω000010000ω00001),

    respectively. Therefore, we get the result (d).

    Then we claim that Pi(0i3) and Tj(1jn1) are indecomposable projective modules.

    In fact, we know that the primitive idempotents of D(n) are listed in [6] as

    e0=14n2n1k=0xk(1+z),e1=14n2n1k=0(x)k(1iz),
    e2=14n2n1k=0xk(1z),e3=14n2n1k=0(x)k(1+iz).

    Since

    xe0=e0,xe1=e1,xe2=e2,xe3=e3,

    and

    ze0=e0,ze1=ωe1,ze2=e2,ze3=ωe3,

    then k{ei,yei|0i3} consist of four indecomposable modules of D(n) and are isomorphic to Pi, respectively. Thus D(n)eiPi is an indecomposable projective module.

    For 0j2n1, set

    θj=12n2n1r=0ξjrxr,

    then {θ0,θ1,,θ2n1} is a set of orthogonal idempotents of D(n). Since xθj=ξjθj, the matrices of x,y,z act on {θj,zθj,yθj,yzθj}, are

    x(ξj0000ξj0000ξj0000ξj),y(0000000010000100),z(0(1)j001000000ω(1)j+100ω0),

    respectively. By the result of (d), we know that k{θj,zθj,yθj,yzθj}Tj for 1jn1, so D(n)θjTj is an indecomposable projective module.

    The straightforward verification shows that Pi(0i3) and Tj(1jn1) are uniserial, that is 0Si1(mod4)Pi and 0MnjTj are the unique composition series of Pi and Tj, respectively. Since D(n) is a Frobenius algebra and thus is self-injective, we get that all the indecomposable projective modules are indecomposable injective modules. Therefore D(n) is a Nakayama algebra. By [8,Theorem V.3.5], the modules listed above are all the indecomposable modules of D(n).

    The proof is completed.

    Corollary 3.2. (1) For all 0i3,Pi is the projective cover of Si.

    (2) For all 1jn1,Tj is the projective cover of Mj.

    Proof. The results is directly obtained by [8,Lemma 5.6].

    Let H be a Hopf algebra, M and N be left H-modules. It has been known that MkN is a left H-module defined by

    h(mn)=(h)h(1)mh(2)n

    for all hH,mM and nN, where Δ(h)=(h)h(1)h(2).

    The remaining of this section is devoted to establishing all the decomposition formulas of the tensor products of two indecomposable D(n)-modules.

    Theorem 3.3. (1) (a) For 0i,j3,

    SiSjSjSiSi+j(mod4).

    (b) For 1jn1,

    SiMjMjSi{Mj,i=0,2,Mnj,i=1,3.

    (c) For 0i,j3,

    SiPjPjSiPi+j(mod4).

    (d) For 1jn1,

    SiTjTjSi{Tj,i=0,2,Tnj,i=1,3.

    (2) (a) For 1i,jn1,

    MiMj{Mi+jM|ij|,0<i+j<n,ijM2n(i+j)M|ij|,n<i+j<2n,ijM|ij|S1S3,i+j=n,ijMi+jS0S2,i=j,0<i+j<n,M2n(i+j)S0S2,i=j,n<i+j<2n.

    (b) For 1in1,0j3,

    MiPjPjMi{Ti,j=0,2,Tni,j=1,3.

    (c) For 1i,jn1,

    MiTjTjMi{Ti+jT|ij|,0<i+j<n,ijT2n(i+j)T|ij|,n<i+j<2n,ijP1P3T|ij|,i+j=n,ijTi+jP0P2,i=j,0<i+j<n,T2n(i+j)P0P2,i=j,n<i+j<2n.

    (3) (a) For 0i,j3,

    PiPjPjPiPi+j(mod4)Pi+j+1(mod4).

    (b) For 1jn1,0i3,

    PiTjTjPiTjTnj.

    (4) For 1i,jn1,

    TiTj{Ti+jT|ij|Tn(i+j)Tn|ij|,0<i+j<n,ijT2n(i+j)T|ij|T(i+j)nTn|ij|,n<i+j<2n,ijP0P1P2P3T|ij|Tn|ij|,i+j=n,ijP0P1P2P3Ti+jTn(i+j),i=j,0<i+j<n,P0P1P2P3T2n(i+j)T(i+j)n,i=j,n<i+j<2n.

    Proof. For SiSj, let vij:=vivj, then

    xvij=(1)i+jvij,yvij=0,zvij=ωi+jvij,

    thus SiSjSi+j(mod4)SjSi.

    For SiMj, let v1ij:=viv1j,v2ij:=viv2j, then

    xv1ij=(1)iξjv1ij,yv1ij=0,zv1ij=ωiv2ij,xv2ij=(1)iξjv2ij,yv2ij=0,zv2ij=(1)jωiv1ij,

    thus SiMjMj when i=0,2 and SiMjMnj when i=1,3. Similarly, we can get the same results of MjSi.

    For SiPj, let μ1ij:=viμ1j,μ2ij:=viμ2j, then

    xμ1ij=(1)i+jμ1ij,yμ1ij=μ2ij,zμ1ij=ωi+jμ2ij,xμ2ij=(1)i+j+1μ2ij,yμ2ij=0,zμ2ij=ωi+j+1μ1ij,

    thus SiPjPi+j(mod4). The same results of PjSi can be obtained in the same way.

    For SiTj, let ϑ1ij:=viϑ1j,ϑ2ij:=viϑ2j,ϑ3ij:=viϑ3j,ϑ4ij:=viϑ4j, then

    xϑ1ij=(1)iξjϑ1ij,yϑ1ij=ϑ3ij,zϑ1ij=ωiϑ2ij,xϑ2ij=(1)iξjϑ2ij,yϑ2ij=ϑ4ij,zϑ2ij=(1)jωiϑ1ij,xϑ3ij=(1)i+1ξjϑ3ij,yϑ3ij=0,zϑ3ij=ωi+1ϑ4ij,xϑ4ij=(1)i+1ξjϑ4ij,yϑ4ij=0,zϑ4ij=(1)j+1ωi+1ϑ3ij,

    thus SiTjTj when i=0,2 and SiTjTnj when i=1,3. Similarly, we get the same results of TjSi.

    For MiMj, let ω1ij:=v1iv1j,ω2ij:=v1iv2j,ω3ij:=v2iv1j,ω4ij:=v2iv2j, then

    xω1ij=ξi+jω1ij,yω1ij=0,zω1ij=ω4ij,xω2ij=ξijω2ij,yω2ij=0,zω2ij=(1)jω3ij,xω3ij=ξjiω3ij,yω3ij=0,zω3ij=(1)iω2ij,xω4ij=ξ(i+j)ω4ij,yω4ij=0,zω4ij=(1)i+jω1ij.

    Obviously, when 0<i+j,ij<n,MiMjMi+jMij. Besides, we need to note that when n<i+j<2n, let ˉω1ij:=ω4ij,ˉω2ij:=(1)i+jω1ij, then

    xˉω1ij=ξ2n(i+j)ˉω1ij,yˉω1ij=0,zˉω1ij=ˉω2ij,xˉω2ij=ξi+j2nˉω2ij,yˉω2ij=0,zˉω2ij=(1)i+jˉω1ij.

    Therefore, k{ˉω1ij,ˉω2ij}Mi+j. When n<ij<0,n<ij+2n<2n, using the previous conclusion, we directly get that k{ˉω3ij:=ω3ij,ˉω4ij:=(1)iω2ij}Mji.

    In particular, when i+j=n, the matrices of x,y,z acting on the basis {ˉω1ij,ˉω2ij} are simultaneously diagonalizable. Thus the modules are isomorphic to S1S3; when ij=0, the matrices of x,y,z acting on the basis {ˉω3ij,ˉω4ij} are also simultaneously diagonalizable and isomorphic to S0S2. In fact we might assume that ij since the result of MjMi are the same as MiMj.

    For MiPj, let ˉν1ij:=v1iμ1j,ˉν2ij:=ωjv2iμ1j,ˉν3ij:=v1iμ2j,ˉν4ij:=ωjv2iμ2j, then

    xˉν1ij=(1)jξiˉν1ij,yˉν1ij=ˉν3ij,zˉν1ij=ˉν2ij,xˉν2ij=(1)jξiˉν2ij,yˉν2ij=ˉν4ij,zˉν2ij=(1)i+jˉν1ij,xˉν3ij=(1)j+1ξiˉν3ij,yˉν3ij=0,zˉν3ij=ωˉν4ij,xˉν4ij=(1)j+1ξiˉν4ij,yˉν4ij=0,zˉν4ij=ω(1)i+j+1ˉν3ij.

    Thus when j=0,2,MiPjPjMiTi; when j=1,3,MiPjPjMiTni,

    For MiTj, let {ˉϑ1ij:=v1iϑ1j,ˉϑ2ij:=v2iϑ2j,ˉϑ3ij:=v1iϑ3j,ˉϑ4ij:=v2iϑ4j,ˉϑ5ij:=v1iϑ2j,ˉϑ6ij:=(1)jv2iϑ1j,ˉϑ7ij:=v1iϑ4j,ˉϑ8ij:=(1)jv2iϑ3j}, then

    xˉϑ1ij=ξi+jˉϑ1ij,yˉϑ1ij=ˉϑ3ij,zˉϑ1ij=ˉϑ2ij,xˉϑ2ij=ξ(i+j)ˉϑ2ij,yˉϑ2ij=ˉϑ4ij,zˉϑ2ij=(1)i+jˉϑ1ij,xˉϑ3ij=ξi+jˉϑ3ij,yˉϑ3ij=0,zˉϑ3ij=ωˉϑ4ij,xˉϑ4ij=ξ(i+j)ˉϑ4ij,yˉϑ4ij=0,zˉϑ4ij=ω(1)i+j+1ˉϑ3ij,xˉϑ5ij=ξijˉϑ5ij,yˉϑ5ij=ˉϑ7ij,zˉϑ5ij=ˉϑ6ij,xˉϑ6ij=ξjiˉϑ6ij,yˉϑ6ij=ˉϑ8ij,zˉϑ6ij=(1)ijˉϑ5ij,xˉϑ7ij=ξijˉϑ7ij,yˉϑ7ij=0,zˉϑ7ij=ωˉϑ8ij,xˉϑ8ij=ξjiˉϑ8ij,yˉϑ8ij=0,zˉϑ8ij=ω(1)ij+1ˉϑ7ij.

    Obviously, when 0<i+j,ij<n,MiTjTi+jTij. It has been shown that in Theorem 3.1 when n<i+j<2n, these modules k{ˉϑ1ij,ˉϑ2ij,ˉϑ3ij,ˉϑ4ij} are isomorphic to the cases of 2n(i+j). When n<ij<0,n<ij+2n<2n, it's clear to get that the modules are isomorphic to the case of 2n(ij+2n)=ji.

    For PiPj, we have known that 0Si1(mod4)Pi is the unique composition series of Pi for 0i3. Thus there is an exact sequence

    0Si1(mod4)PiSi0.

    By Corollary 3.2, Pi=P(Si), so there is a split exact sequence

    0Si1(mod4)PjPiPjSiPj0.

    Hence

    PiPjSi1(mod4)PjSiPjPi+j1(mod4)Pi+j(mod4).

    For PiTj, similarly, we have the split exact sequence

    0Si1(mod4)TjPiTjSiTj0.

    Hence

    PiTjSi1(mod4)TjSiTjTjTnj.

    For TiTj,i>j, the unique composition series of Ti is 0MniTi for 1in1, and there is an exact sequence

    0MniTiMi0

    and the split exact sequence

    0MniTjTiTjMiTj0

    for Tj=P(Mj). Hence

    TiTjMniTjMiTjTni+jTnijTi+jTij.

    Then applying the result of (2)(c), we get the result (4). For i<j, the result is similar.

    The proof is finished.

    Corollary 3.4. The tensor product of any two D(n)-modules is commutative.

    Let H be a finite dimensional Hopf algebra and F(H) the free abelian group generated by the isomorphic classes [M] of finite dimensional H-modules M. The abelian group F(H) becomes a ring if we endow F(H) with a multiplication given by the tensor product [M][N]=[MN]. The representation ring (or Green ring) r(H) of the Hopf algebra H is defined to be the quotient ring of F(H) modulo the relations [MN]=[M]+[N]. It follows that the representation ring r(H) is an associative ring with identity given by [kε], the trivial 1-dimensional H-module. Note that r(H) has a Z-basis consisting of isomorphic classes of finite dimensional indecomposable H-modules. In this section we will describe the representation ring r(D(n)) of the Hopf algebra D(n) explicitly by the generators and the generating relations.

    Let Fq(y,z) be the generalized Fibonacci polynomials defined by

    Fq+2(y,z)=zFq+1(y,z)yFq(y,z)

    for q1, while F0(y,z)=0,F1(y,z)=1,F2(y,z)=z. These generalized Fibonacci polynomials appeared in [13,14].

    Lemma 4.1. [13,Lemma 3.11] Let Z[y,z] be the polynomial algebra over Z in two variables y and z. Then for any q1, we have

    Fq(y,z)=[q12]i=0(1)i(q1ii)yizq12i,

    where [q12] denotes the biggest integer which is not bigger than q12.

    Let [S1]=α, [M1]=β and [P0]=γ. In the following the sum mi=0 disappears if m<0.

    Lemma 4.2. The following statements hold in r(D(n)).

    1. α4=1,α2β=β,αγ=γ(γ1);

    2. [Si]=αi, [Pi]=αiγ(0i3);

    3. For 1jn1,

    [Mj]={j12i=0(1)i(jii)βj2ij32i=0(1)i(j2ii)βj22i,jis odd,j2i=0(1)i(jii)βj2ij42i=0(1)i(j2ii)βj22i+(1)j2α2,jis even; (4.1)
    [Tj]={j12i=0(1)i(jii)βj2iγj32i=0(1)i(j2ii)βj22iγ,jis odd,j2i=0(1)i(jii)βj2iγj42i=0(1)i(j2ii)βj22iγ+(1)j2α2γ,jis even. (4.2)

    Proof. The results of (1), (2) are easy to get from Theorem 3.3(1)(a)–(c) and (3)(a).

    We prove (3) by induction. By Theorem 3.3(2)(a), there is

    [M2]=β2(1+α2)=F3(1,β)α2

    and

    [M3]=[M1][M2][M1]=β32βα2β=β33β=F4(1,β)F2(1,β).

    Suppose that (4.1) holds for j1 being odd and j being even, then for j+1 we have

    [Mj+1]=[Mj][M1][Mj1]=(Fj+1(1,β)α2Fj1(1,β))β(Fj(1,β)Fj2(1,β))=(Fj+1(1,β)βFj(1,β))α2(Fj1(1,β)βFj2(1,β))=Fj+2(1,β)α2Fj(1,β)=j2i=0(1)i(j+1ii)βj+12iα2j22i=0(1)i(j1ii)βj12i=j2i=0(1)i(j+1ii)βj+12ij22i=0(1)i(j1ii)βj12i.

    Similarly, suppose that (4.1) holds for j1 being even and j being odd, then for j+1 we directly get that

    [Mj+1]=j+12i=0(1)i(j+1ii)βj+12iα2j12i=0(1)i(j1ii)βj12i=j+12i=0(1)i(j+1ii)βj+12ij32i=0(1)i(j1ii)βj12i(1)j12α2.

    By Theorem 3.3(2)(b), we know that MjP0Tj, thus the Eq (4.2) is obvious to be obtained.

    Corollary 4.3. Keep the notations above.

    1. If n12 is odd, then

    n+14i=0(1)i(n+12ii)βn+122in74i=0(1)i(n32ii)βn322i+(1)n+14α2=αn34i=0(1)i(n12ii)βn122iαn74i=0(1)i(n52ii)βn522i.

    2. If n12 is even, then

    n14i=0(1)i(n+12ii)βn+122in54i=0(1)i(n32ii)βn322i=αn14i=0(1)i(n12ii)βn122iαn94i=0(1)i(n52ii)βn522i+(1)n14α3.

    Proof. Since [S1][Mn12]=[Mn+12] by Theorem 3.3(1)(b), and using the equations of (4.1) in Lemma 4.2, we can easily get the results.

    Corollary 4.4. Keep notations as above, then the sets

    {αiγk0i3,0k1}{αiβjγk0i1,1jn12,0k1}

    form a Z-basis of r(D(n)).

    Proof. By Lemma 4.1, α4=1, and there is a one-to-one correspondence between the set {αi,αiγ0i3} and the set of D(n)-modules {[Si],[Pi]0i3}. By the Eq (4.1), we know that [Mj] is a Z-polynomial with α and β, and when jn+12,[Mj]=[S1][Mnj]. By Corollary 4.3, we know that the highest degree of β in this polynomial is n12, and {[Mj]1jn1} is a Z-linear combination of {αi0i3}, {αβj1jn12} and {βj1jn12}. Consequently, [Tj] is a Z-polynomial with α,β,γ and the highest degree of γ in this polynomial is 1 since γ2=αγ+γ. Therefore [Tj] is a Z-linear combination of {αi0i3}, {αβjγ1jn12} and {βjγ1jn12}.

    The result is obtained.

    Theorem 4.5. The representation ring r(D(n)) is a commutative ring generated by a,b,c, subject to the following relations

    a4=1,a2b=b,ac=c(c1)

    and

    bn+12=n+14i=1(1)i(n+12ii)bn+122i+n74i=0(1)i(n32ii)bn322i+(1)n+54a2+an34i=0(1)i(n12ii)bn122ian74i=0(1)i(n52ii)bn522i

    if n12 is odd, or

    bn+12=n14i=1(1)i(n+12ii)bn+122i+n54i=0(1)i(n32ii)bn322i+(1)n14a3+an14i=0(1)i(n12ii)bn122ian94i=0(1)i(n52ii)bn522i

    if n12 is even.

    Proof. By Corollary 3.4, we know that the ring r(D(n)) is a commutative ring generated by α, β and γ, there is a unique ring epimorphism

    Φ:Z[a,b,c]r(D(n))

    from Z[a,b,c] to r(D(n)) such that

    Φ(a)=α,Φ(b)=β,Φ(c)=γ.

    By Lemma 4.1, there is

    α4=1,α2β=β,αγ=γ(γ1),

    thus we have

    Φ(a41)=0,Φ(a2bb)=0,Φ(acc(c1))=0.

    Note that by Corollary 4.3,

    βn+12=n+14i=1(1)i(n+12ii)βn+122i+n74i=0(1)i(n32ii)βn322i+(1)n+54α2+αn34i=0(1)i(n12ii)βn122iαn74i=0(1)i(n52ii)βn522i

    when n12 is odd, or

    βn+12=n14i=1(1)i(n+12ii)βn+122i+n54i=0(1)i(n32ii)βn322i+(1)n14α3+αn14i=0(1)i(n12ii)βn122iαn94i=0(1)i(n52ii)βn522i

    when n12 is even. Thus Φ maps

    bn+12+n+14i=1(1)i(n+12ii)bn+122in74i=0(1)i(n32ii)bn322i(1)n+54a2a[n34]i=0(1)i(n12ii)bn122i+an74i=0(1)i(n52ii)bn522i

    or

    bn+12+n14i=1(1)i(n+12ii)bn+122in54i=0(1)i(n32ii)bn322i(1)n14a3an14i=0(1)i(n12ii)bn122i+an94i=0(1)i(n52ii)bn522i

    to 0. It follows that Φ(I)=0, and Φ induces a ring epimorphism

    ¯Φ:Z[a,b,c]/Ir(D(n))

    such that ¯Φ(¯ν)=Φ(ν) for all νZ[a,b,c], where ¯ν=π(ν) and π is the natural epimorphism Z[a,b,c]Z[a,b,c]/I. Note that the ring r(D(n)) is a free Z-module of rank 2n+6 with the Z-basis {αiγk0i3,0k1}{αiβjγk0i1,1jn12,0k1}, so we can define a Z-module homomorphism

    Ψ:r(D(n))Z[a,b,c]/Iαiγk¯ai¯ck(0i3,0k1),αiβjγk¯ai¯bj¯ck(0i1,1jn12,0k1).

    On the other hand, as a free Z-module, Z[a,b,c]/I is generated by elements aick(0i3,0k1) and aibjck(0i1,1jn12,0k1), we have

    Ψ¯Φ(¯aick)=ΨΦ(aick)=Ψ(αiγk)=¯ai¯ck,
    Ψ¯Φ(¯aibjck)=ΨΦ(aibjck)=Ψ(αiβjγk)=¯ai¯bj¯ck.

    Hence Ψ¯Φ=id, and ¯Φ is injective. Thus, ¯Φ is a ring isomorphism.

    The proof is finished.

    Example 4.6. We have the following examples.

    The representation ring r(D(3)) is a commutative ring generated by a,b,c, subject to the following relations

    a4=1,a2b=b,ac=c(c1),b2=ab+a2+1.

    The representation ring r(D(5)) is a commutative ring generated by a,b,c, subject to the following relations

    a4=1,a2b=b,ac=c(c1),b3=ab2+3ba3a.

    We have constructed all the indecomposable modules of the non-pointed Hopf algebra D(n) and established the decomposition formulas of the tensor product of any two indecomposable modules. The representation ring r(D(n)) has been characterized by generators and relations. In the further work, we hope to construct all the simple Yetter-Drinfeld modules of D(n) and classify all the finite-dimensional Nichols algebras and finite-dimensional Hopf algebras over D(n).

    This work was supported by the National Natural Science Foundation of China (11671024).

    The authors declare that they have no competing interests.



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