Research article

A new family of positively based algebras Hn

  • Received: 25 October 2023 Revised: 04 December 2023 Accepted: 10 December 2023 Published: 26 December 2023
  • MSC : 16D80, 16G60

  • In this paper, we introduce a new family of algebras Hn, which are generated by three generators x,y,z, with the following relations: (1) x2n=1, y2=xy+y, xy=yx; and (2) z2=z, xz=zx=z, zy=2z. First, it shows that Hn is a positively based algebra. Then, all the indecomposable modules of Hn are constructed. Additionally, it shows that the dimension of each indecomposable Hn-module is at most 2. Finally, all the left (right) cells and left (right) cell modules of Hn are described, and the decompositions of the decomposable left cell modules are also obtained.

    Citation: Shiyu Lin, Shilin Yang. A new family of positively based algebras Hn[J]. AIMS Mathematics, 2024, 9(2): 2602-2618. doi: 10.3934/math.2024128

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  • In this paper, we introduce a new family of algebras Hn, which are generated by three generators x,y,z, with the following relations: (1) x2n=1, y2=xy+y, xy=yx; and (2) z2=z, xz=zx=z, zy=2z. First, it shows that Hn is a positively based algebra. Then, all the indecomposable modules of Hn are constructed. Additionally, it shows that the dimension of each indecomposable Hn-module is at most 2. Finally, all the left (right) cells and left (right) cell modules of Hn are described, and the decompositions of the decomposable left cell modules are also obtained.



    An algebra A is called a positively based algebra if it has a positive basis. By the latter, we mean that a set of bases with all the structure constants with respect to this basis are non-negative real numbers. The concept of a positive basis can be traced back to the work of Schur on the centralizer algebra of a transitive permutation representation of a finite group in [16,17]. Since then, variations of the positively based algebras have been discovered in many different fields (see [1,3,15]). Examples of positively based algebras include the group algebras, semigroup algebras, table algebras, and Hecke algebras corresponding to Coxeter groups with respect to the Kazhdan-Lusztig basis. As an interesting infinite dimensional example, Thurston proved that the Kauffman bracket skein algebra for a compact oriented surface has a natural positive basis in [19], which generalized the positivity conjecture in cluster algebra. In [14], Mazorchuk et al. defined the cell 2-representations of finitary 2-categories. It turns out that the cell 2-representation is a based module over some finite-dimensional positively based algebras on the level of the Grothendieck group. In addition, in the perspective of representation theory, Green algebra of a bialgebra is a central instance of positively based algebras. For example, Cao et al. [4] studied the cell modules of the Green algebra of the generalized Taft Hopf algebras, in which the approach depends on the Green ring.

    In [10], Lin and Yang introduced a class of positively based algebras An,d over the subring K of the complex field C; all indecomposable modules and cell modules of An,d are classified and constructed. It is noted that An,d can be regarded as the Green algebra of weak Hopf algebras w1n,d constructed from the generalized Taft algebra (see [18]). In the present paper, we introduce the K-algebra Hn, which is generated by x,y,z with the relations (1) and (2); since we can construct a set of positive bases of Hn, we can conclude that Hn is a positively based algebra. The algebra Hn can be viewed as the extension of the Green ring of the weak Hopf algebra wH4n, which is constructed from neither the pointed nor the semisimple Hopf algebra H4n (see [5]). Recall that An,d in [10,Definition 2.1] is generated by x,y,z with the following relations:

    (1)xnd=1, xy=yx;(2)(1+xny)[d12]i=0(1)i(d1ii)xniyd12i=0, for  d2;(3)z2=z, xz=zx=z, yz=2z.

    We see that the generating relations of An,d and Hn are strongly different. For instance, the representation type of An,d depends on d, and it is of finite representation type if d4, of tame type if d=5, and of wild type if d6. However, the algebra Hn is only of finite representation type. Up to now, there is a limited number of works that classifies the representations of this family of positively based algebras. This provides a good chance to understand the representation theory of Hn. In this paper, as the analog of the method in [10], we first construct a set of positive basis of Hn and show that Hn is a positively based algebra. Then, we make efforts to classify all the indecomposable modules of Hn by utilizing the representation theory of a quiver. It is easily seen that the algebra Hn is of finite representation type, and thus all the indecomposable modules of Hn are constructed. Finally, all the left (right) cells and left cell (right) modules of Hn are constructed. Moreover, the decompositions of the left cell modules are provided.

    Let us describe the arrangement of this paper. In Section 2, we introduce the algebra Hn by generators and generating relations, and show that Hn is a positively based algebra. In Section 3, we focus on constructing all indecomposable modules of Hn and we see that Hn is of finite representation type. In Section 4, we classify all the left (right) cells and left (right) cell modules of Hn.

    Throughout the paper and unless otherwise stated, C, R, Z and N, stand for the field of complex numbers, the field of real numbers, the ring of integers, and the set of natural numbers, respectively. Fixing an integer n1, we always suppose that K is an unital subring of C containing the primitive 2n-th root of the unity:

    η=cosπn+isinπn.

    Let A be a K-algebra of finite free rank n with a basis B={ai|1in}. For any 1i,j,kn, if

    aiaj=nk=1γ(k)i,jak,

    where γ(k)i,jR0, then B is said to be a positive basis of A, and A is called a positively based algebra.

    Now, we define the algebra Hn and describe its basic properties.

    Definition 2.1. The K-algebra Hn is generated by x,y,z with the following relations:

    (1) x2n=1, y2=xy+y, xy=yx;

    (2) z2=z, xz=zx=z, zy=2z.

    It is easy to see that Hn is noncommutative, and it is noted that when K=C, the algebra Hn is just the Green algebra of the weak Hopf algebra wH4n (see [5]).

    In the following, we construct a set of positive bases of Hn to show that Hn is a positively based algebra. For this purpose, we list one lemma as follows.

    Lemma 2.2. (1) The K-space Wi (0i2n1) with a basis {νi} is an Hn-module with the action of Hn:

    xνi=ηiνi,yνi=(1+ηi)νi,zνi=0.

    (2) The K-space V1 with a basis {θ1,θ2} is an Hn-module with the action of Hn:

    xθ1=θ1,yθ1=0,zθ1=0,xθ2=θ2,yθ2=θ1,zθ2=0.

    (3) The K-space V2 with a basis {ξ1,ξ2} is an Hn-module with the action of Hn:

    xξ1=ξ1,yξ1=ξ2,zξ1=ξ1,xξ2=ξ2,yξ2=2ξ2,zξ2=2ξ1. (2.1)

    (4) The K-space V3 with a basis {μj0j2n1} is an Hn-module with the action of Hn:

    xμj=μj+1(mod2n),yμj=0,zμj=0.

    Proof. In the following, we only prove the statement (3); the proofs of the other statements are similar.

    First, it is easy to see that

    (x(x(x2nξi)))=ξi.(i=1,2),

    Then, the straightforward verification shows that

    y(yξ1)=2ξ2=x(yξ1)+yξ1,y(yξ2)=4ξ2=x(yξ2)+yξ2,

    and

    y(xξ1)=ξ2=x(yξ1),y(xξ2)=2ξ2=x(yξ2).

    Moreover, it is obvious that

    z(zξ1)=ξ1=zξ1,z(zξ2)=2ξ1=zξ2,

    and

    x(zξ1)=ξ1=zξ1=z(xξ1),
    x(zξ2)=2ξ1=zξ1=z(xξ1).

    Finally, we see that

    z(yξ1)=2ξ1=2zξ1,z(yξ2)=4ξ1=2zξ2.

    It follows that the generators x,y and z acting on V2 keep the defining relations.

    Hence, the actions of x,y and z on V2 define an Hn-module.

    Proposition 2.3. The set {xiyj,ykz|0i2n1,j,k=0,1} forms a basis of Hn.

    Proof. By the defining relations of Hn, one can see that Hn are spanned by the following:

    {xiyj,ykz|0i2n1,j,k=0,1}.

    Therefore, it is sufficient to prove that the set

    {xiyj,ykz|0i2n1,j,k=0,1}

    consists of linearly independent elements.

    Now, we assume the following:

    2n1i=0aixi+2n1j=0bjxjy+1k=0ckykz=0.(I)

    Acting on μ0 by the both sides of (I), we have 2n1i=0aiμi=0 and

    ai=0,0i2n1.

    It yields that

    2n1j=0bjxjy+1k=0ckykz=0.(II)

    Acting on {ν0,,νn1,θ2,νn+1,ν2n1} by the both sides of (II), we have

    (2n1j=0bjxjy+1k=0ckykz)θ2=(2n1j=0bjxj)θ1=2n1j=0(1)jbjθ1=0

    and

    (2n1j=0bjxjy+1k=0ckykz)νi=(2n1j=0bjxj)(1+ηi)νi=(1+ηi)2n1j=0ηijbjνi=0.

    Hence, obtain the following:

    2n1j=0(1)jbj=0 and 2n1j=0ηijbj=0(in),

    since 1+ηi0.

    Thus,

    (111111(ηn1)n1(ηn1)n(ηn1)n+1(η2n1)i1(1)n1(1)n(1)n+111(ηn+1)n1(ηn+1)n(ηn+1)n+1(η2n1)i1(η2n1)n1(η2n1)n(η2n1)n+1(η2n1)2n1)(b0bn1bnbn+1b2n1)=(00000).

    It is easy to see that the determinant of the coefficient matrix is nonzero; thus, we have the following:

    bj=0 for 0j2n1.

    Moreover, it yields that

    1k=0ckykz=0.(III)

    Acting on {ξ1} by the both sides of (III), we have

    1k=0ckykzξ1=c0ξ1+c1ξ2=0,

    and c0=c1=0.

    In summary,

    {xiyj,ykz|0i2n1,j,k=0,1}

    is a linearly independent set. Hence, it is a basis of Hn.

    The proof is finished.

    Set Li=xi, Mi=xiy for 0i2n1, N0=z and N1=yz. Let

    B={Li,Mi,Nk|0i2n1,k=0,1}.

    Then, B is a basis of Hn.

    Proposition 2.4. For 0i,j2n1, we have the following:

    (1) LiLj=LjLi=Li+j(mod2n);

    (2) LiMj=MjLi=Mi+j(mod2n);

    (3) MiMj=MjMi=Mi+j(mod2n)+Mi+j+1(mod2n);

    (4) N0N0=N0Li=LiN0=N0;

    (5) N0N1=N0Mi=2N0;

    (6) N1N0=MiN0=N1Li=LiN1=N1;

    (7) N1N1=N1Mi=MiN1=2N1.

    Proof. For 0i,j2n1, by a straightforward verification, we have

    LiLj=xixj=xi+j(mod2n)=Li+j(mod2n)=LjLi

    and

    LiMj=xixjy=xi+j(mod2n)y=Mi+j(mod2n)=MjLi,

    since x2n=1,xy=yx.

    Hence, (1) and (2) hold.

    (3) By y2=xy+y, we have the following:

    MiMj=xiyxjy=xixjy2=xixj(xy+y)=xi+j(mod2n)y+xi+j+1(mod2n)y=Mi+j(mod2n)+Mi+j+1(mod2n)=MjMi.

    (4) By z2=z, we have

    LiN0=N0Li=xiz=zxi=z=N0

    and

    N0N0=z2=z=N0.

    (5) By zy=2z, we have

    N0N1=zyz=2z2=2z=2N0

    and

    N0Mi=zxiy=zy=2z=2N0.

    (6) First, we have

    N1N0=yzz=yz2=yz=N1

    and

    N1Li=yzxi=yz=N1.

    Moreover, we have

    MiN0=xiyz=yxiz=yz=N1

    and

    LiN1=xiyz=yxiz=yz=N1.

    Therefore, N1N0=MiN0=N1Li=LiN1=N1. (7) First, we have

    N1N1=yzyz=2yz2=2yz=2N1

    and

    N1Mi=yzxiy=yzy=2yz=2N1,

    since zy=2z.

    Moreover, we have the following:

    MiN1=xiyyz=xi(xy+y)z=xixyz+xiyz=xi+1yz+xiyz=yxi+1z+yxiz=yz+yz=2N1.

    Hence, N1N1=N1Mi=MiN1=2N1.

    Theorem 2.5. The algebra Hn is a positively based algebra.

    Proof. By Proposition 2.4, one can easily check that

    B={Li,Mi,Nk|0i2n1,k=0,1}

    is a set of positive bases of Hn.

    The theorem follows.

    From this section, we always assume that K is a subfield of C containing η.

    The aim of section is to construct all indecomposable modules of Hn with the help of the representation theory of a quiver. For this purpose, we first consider an algebra A over the field K, which is generated by x,y with the following relations:

    x2n=1,y2=xy+y,xy=yx.

    By a straightforward calculation, we see that the following system of equations

    {x2n=1,y2xyy=0,

    has 4n1 distinct solutions given by the following:

    Γ={(ηi,0)|0i2n1}{(ηj,1+ηj)|0j2n1,jn}.

    For each solution (x1,x2)Γ, we can define a simple A-module by

    xv=x1v,yv=x2v.

    Hence, we have the following Lemma.

    Lemma 3.1. (1) For 0i2n1, there are 2n non-isomorphic 1-dimensional A-modules Si with the basis {vi}. The action of A is given by the following:

    xvi=ηivi,yvi=0.

    (2) For 0i2n1 and in, there are 2n1 non-isomorphic 1-dimensional A-modules Wi with the basis {vi}. The action of A is given by the following:

    xvi=ηivi,yvi=(1+ηi)vi.

    Proof. It is obvious.

    In the following, we describe all indecomposable modules of A.

    Let D be a 2-dimensional vector space with the basis {v1,v2}. We define an action of A on D as follows:

    xv1=v1,yv1=0,xv2=v2,yv2=v1.

    Then, D is an indecomposable A-module.

    Proposition 3.2. Any d-dimensional, non-simple, indecomposable A-module V is isomorphic to D.

    Proof. Assume that V is a d-dimensional, non-simple, indecomposable module with d2. Then, EndV is local and EndV/radEndVK. Accordingly, we can assume that the matrices of x and y acting on some suitable basis of V are X=ηiEd and

    Y=(λ10000λ100000λ10000λ)d×d,λK,

    respectively, since x2n=1 and xy=yx.

    One can easily see that matrices X and Y satisfy the following:

    (Y(1+ηi)Ed)Y=0.

    It follows that i=n, d=2 and λ=1+ηi=0. Thus, we have VD.

    In the following, set

    ei=12n2n1k=0ηikxk

    for 0i2n1.

    One can easily check that {e0,e1,...,e2n1} is a set of central idempotents of Hn, and

    z(e0z)=(e0z)z=0,zei=eiz=0 for 1i2n1.

    Therefore, we have the following:

    Hn=HnzHn(e0z)Hne1Hne2n1.

    Now, we can deduce the simple modules and indecomposable modules of Hn by Lemma 3.1 and Proposition 3.2:

    (1) For 0i2n1, let Si be a 1-dimensional Hn-module with the basis {vi}; the action of Hn is given by

    xvi=ηivi,yvi=0,zvi=0.

    (2) For 0i2n1 and in, let Wi be a 1-dimensional Hn-module with the basis {vi}; the action of Hn is given by

    xvi=ηivi,yvi=(1+ηi)vi,zvi=0.

    (3) The indecomposable Hn-module V1 is produced by extending D, which is given in Lemma 2.2.

    Corollary 3.3. V1Hnen is the projective cover of Sn.

    Proof. First, by a straightforward calculation, we have

    xien=(1)ien,xiyen=(1)iyen,zen=0,yzen=0.

    It follows that {yen,en} is a basis of Hnen; the action of Hn is given by

    xyen=yen,yyen=0,zyen=0,xen=en,yen=yen,zen=0.

    Hence, it is easy to obtain V1Hnen and Sn=topV1 by Lemma 2.2.

    The proof is finished.

    Lemma 3.4. HnzV2 is a 2-dimensional indecomposable projective Hn-module.

    Proof. First, it is easy to have Hnz is projective, since Hn=HnzHn(1z). Moreover, we have

    xiz=z,xiyz=yxiz=yz,z2=z,yzz=yz.

    It follows that {z,yz} is a basis of Hnz; the action of Hn is given by

    xz=z,yz=yz,zz=z,xyz=yz,yyz=2yz,zyz=2z.

    By Lemma 2.2, it is easy to obtain that HnzV2.

    Suppose that V2=A1A2, where A1 and A2 are nonzero. One has 0φ=k1z+k2yzA1 for some k10 or k20. Then,

    yφ=(k1+2k2)yzA1,zφ=(k1+2k2)zA1.

    If k1+2k2=0, we get that φ=k2(2zyz)A1 with k20 and 2zyzA1. Accordingly, the decomposition yz=(yz2z)+2z implies that 2zA2 and yz=yzA2. Hence, A2=V2, which is a contradiction. This implies that k1+2k20, yzA1 and zA1. Thus, we have A1=V2, which is also a contradiction.

    Therefore, HnzV2 is an indecomposable projective module.

    Assume S=Kv is a 1-dimensional Hn-module defined by

    xv=v,yv=2v,zv=v. (3.1)

    Reviewing the action of Hn on V2, we let ξ1=2ξ1ξ2, ξ2=ξ2; then the action of Hn can be written as follows:

    xξ1=ξ1,yξ1=0,zξ1=0,xξ2=ξ2,yξ2=2ξ2,zξ2=ξ1+ξ2. (3.2)

    We get that S=topV2 and the exact sequence

    0S0V2S0.

    It concludes the following theorem.

    Theorem 3.5. The following is a complete set of all simple Hn-modules up to isomorphism:

    (1) One non-projective simple module Sn with the projective cover V1;

    (2) One non-projective simple module S with the projective cover V2;

    (3) 4n2 projective simple modules Si and Wi, where 0i2n1 and in.

    We also need more preparations to list all the indecomposable Hn-modules.

    Lemma 3.6. Hn(e0z)=S0W0.

    Proof. For 0i2n1, we have

    xi(e0z)=xie0xiz=e0z,
    xiy(e0z)=yxie0yxiz=ye0yz,

    and

    z(e0z)=ze0z2=0,yz(e0z)=yzyz2=0.

    Set v1=2e02zye0+yz, v2=ye0yz; then, {v1,v2} is a basis of Hn(e0z) and

    xv1=v1,yv1=0,zv1=0,xv2=v2,yv2=2v2,zv2=0.

    By Lemma 2.2, Hn(e0z)=S0W0.

    The result follows.

    Lemma 3.7. For 1i2n1, we have the following:

    (1) HomHn(Hnei,Hne0)=0;

    (2) HomHn(Hne0,Hnei)=0.

    Proof. (1) By [2,Lemma 4.2], we have

    HomHn(Hnei,Hne0)=eiHne0=0,

    since eie0=e0ei=0, and xy=yx,xz=zx for 1i2n1.

    The proof of (2) is similar to (1).

    Lemma 3.8. (1) HomHn(V2,W0)=0, HomHn(V2,Sn)=0;

    (2) HomHn(S0,V2)0, HomHn(W0,V2)=0.

    Proof. (1) By Lemmas 3.4 and 3.8, we have

    HomHn(V2,W0)=HomHn(Hnz,W0)=zW0=0.

    Similarly,

    HomHn(V2,S0)=S0=0.

    (2) By (3.2), S0 is the socle of V2. Thus,

    HomHn(S0,V2)0.

    For W0, the result is obvious.

    According to Lemmas 3.6–3.8, one can easily see that V2S0 is a block of Hn. Meanwhile, the indecomposable modules of other blocks are either 1-dimensional or 2-dimensional. Therefore, we only need to consider the indecomposable modules of the block C=V2S0.

    Proposition 3.9. The quiver of the block C is as follows:

    Proof. On the one hand, V2 is the projective cover of S, and S0 is projective by Lemma 3.4. Therefore,

    Ext1Hn(S0,S)=0.

    On the other hand, we have the following extension of S0 by S:

    0S0V2S0.

    Assume that

    0S0QS0

    is another extension of S0 by S, where Q is indecomposable of the basis {v1,v2}; the action of Hn is given by

    xv1=v1,yv1=0,zv1=0,xv2=v2,yv2=2v2,zv2=kv1+v2,

    with k0.

    Now, let h:V2Q, which is given by ξ1kv1, ξ2v2. Then, h is an isomorphism. It follows that

    dimExt1Hn(S,S0)=1.

    The result follows.

    Theorem 3.10. The algebra Hn has 4n+2 pairwise, non-isomorphic, indecomposable modules:

    {Si,Wj,S0i,j2n1,jn}{V1,V2}.

    Proof. By Proposition 3.9, the quiver of block C is as follows:

    It is easy to see that this block has non-isomorphic, indecomposable modules S0, S and V2. By Theorem 3.5, we get 4n+2 pairwise, non-isomorphic, indecomposable modules of Hn as the aforementioned list.

    Let A be a positively based algebra with a fixed positive basis B={ai|iI} with the identity a1 of A. For i,jI, set

    ij={k|γ(k)i,j>0}.

    This defines an associative multi-valued operation on the set I and turns the latter set into a finite multi-semigroup, see [9,Subsection 3.7]. If there is an sI such that jsi, then we denoted it by iLj. For i,jI, if iLj and jLi, we denote it by iLj, which is an equivalent relation. The associated equivalence class is referred to as a left cell. Moreover, we write i<Lj, provided that ilj and iLj.

    Assume that L is a left cell in I, and let ¯L be the union of all left cells L in I such that LL. Set ¯L_=¯LL. Let ML be the vector space spanned by aj, where j¯L, and NR be the vector space spanned by aj with j¯L_. According to [8,Proposition 1], ML and NL are submodules of AA and NLML. It allows us to define the cell module CR=ML/NL. Especially, if ¯L_=, denote it by NL=0. For the study of cells and cell modules, the readers can refer to [6,7,8,11,12,13].

    Now, we investigate the left (right) cells and left (right) cell modules of Hn. By Theorem 2.5,

    B={Li,Mj,Nk|0i,j2n1,k=0,1}

    is a positive basis of Hn.

    Proposition 4.1. The algebra Hn has three left cells L1, L2 and L3, as listed in the following;

    (1) L1={i|i  is  the  index  of  Li,iZ2n};

    (2) L2={j|j  is  the  index  of  Mj,jZ2n};

    (3) L3={k|k  is  the  index  of  Nk,k=0,1}.

    Proof. (1) Set i,iZ2n and i<i. We obtain LiiLi=Li by Proposition 2.4. It follows that i(ii)i, which implies that iLi. Similarly, we have L2ni+iLi=Li; then, i(2ni+i)i and iLi. The equivalent relation iLi holds and L1 is a left cell.

    (2) Set j,jZ2n and j<j. We have j(jj)j and jLj, since MjjMj=Mj+Mj+1. Similarly, we obtain that j(2n+jj)j and jLj. Hence, L2 is a left cell.

    (3) By Proposition 2.4, it is obvious that N0N1=2N0 and N1N0=N1. Thus, we have 1L0 and 0L1. Therefore, L3 is a left cell.

    The proof is completed.

    Corollary 4.2. For the left cells of Hn, we have L1<LL2<LL3.

    Proof. For i,jZ2n, we have MjLi=Mi+j(mod2n) by Proposition 2.4. It is clear that L1<LL2.

    Furthermore, by Proposition 2.4, it is easy to see that

    N0Mj=N0+N0,N1Mj=N1+N1.

    Thus, L2<LL3 holds.

    Consequently, we have L1<LL2<LL3.

    Proposition 4.3. For the left cells L1, L2 and L3, the corresponding left cell modules CL1, CL2 and CL3 are given as follows:

    (1) CL1=Span{¯Li|iZ2n}, where ¯Li=Li+NL1, NL1=Span{Mj,Nk|jZ2n,k=0,1};

    (2) CL2=Span{¯Mj|jZ2n}, where ¯Mj=Mj+NL2, and

    NL2=Span{Nk|k=0,1};

    (3) CL3=Span{Nk|k=0,1}, where NL3={0}.

    Proof. (1) As is shown in Corollary 4.2, we have

    ¯L1=L1L2L3,¯L1_=L2L3.

    By Proposition 4.1, it follows that

    ML1=Span{Li,Mj,Nk|i,jZ2n,k=0,1},

    and

    NL1=Span{Mj,Nk|jZ2n,k=0,1}.

    Hence,

    CL1=ML1/NL1=Span{¯Si|iZ2n}.

    (2) By Corollary 4.2, we have

    ¯L2=L2L3,¯L2_=L3.

    It follows that

    ML2=Span{Mj,Nk|jZ2n,k=0,1},

    and

    NL2=Span{Nk|k=0,1}.

    Therefore,

    CL2=ML2/NL2=Span{¯Mj|jZ2n}.

    (3) By Proposition 4.1 and Corollary 4.2, we have

    ¯L3=L3, and  ¯L3_=.

    It follows that

    ML3=Span{Nk|k=0,1}, and NL3={0}.

    Hence,

    CL3=ML3/NL3=Span{Nk|k=0,1}.

    The proof is finished.

    By Proposition 4.3, we see that CL1=Span{¯Li|iZ2n} and write μi=¯Li with 0i2n1. Then, the action of Hn on CL1 is defined by

    xμi=μi+1(mod2n),yμi=0,zμi=0.

    Now, set

    χi=12n(μ0+ηiμ1+η2iμ2++η(2n1)iμ2n1),

    where 0i2n1.

    A straightforward calculation shows that

    xχi=ηiχi,yχi=0,zχi=0.

    Theorem 4.4. CL1 is decomposable and

    CL1S0S1S2n1.

    Proof. By Lemma 2.2, the 1-dimensional Hn-module Kχi=Si. Hence, Si is a submodule of CL1. We easily see that

    dimK(S0S1S2n1)=dimKCL1,

    and conclude

    CL1S0S1S2n1.

    The proof is completed.

    For the left cell module CL2, we have CL2=Span{¯Mj|jZ2n} and denote νj=¯Mj with 0j2n1. It is easy to see that

    xνj=νj+1(mod2n),yνj=νj+νj+1(mod2n),zνj=0.

    Set

    ωj=12n(ν0+ηjν1+η2jν2++η(2n1)jν2n1)

    for 0j2n1.

    Then, a straightforward calculation shows that

    xωj=ηjωj,yωj=(1+ηj)ωj,zωj=0.

    Theorem 4.5. CL2 is decomposable and

    CL2W0Wn1SnWn+1W2n1.

    Proof. On the one hand, by Lemma 2.2, we see that the Hn-module KωjWj when jn, and KωnSn. Hence, Wj is a submodule of CL2 for 0j2n1 and jn.

    On the other hand, it is easy to see that

    dimK(W0Wn1SnWn+1W2n1)=dimKCL2.

    Hence,

    CL2W0Wn1SnWn+1W2n1.

    The proof is finished.

    Theorem 4.6. CL3V2 is indecomposable.

    Proof. By Proposition 4.3, for the left cell module CL3, we have CL3=Span{Nk|k=0,1}, on which the action of Hn is given by

    xN0=N0,yN0=N1,zN0=N0,xN1=N1,yN1=2N1,zN1=2N0.

    Hence, CL3V2 by Lemma 3.4.

    The result follows.

    Finally, we give some remarks for the right cell modules of Hn. For the positive basis B, if there is an sI such that jis, then one can denote it by iRj. If iRj and jRi, then one can denote it by iRj, which is an equivalent relation. The equivalence class is called a right cell. The similar statement to Proposition 4.1 shows that Hn has the following four right cells:

    (1) R1={i|i is the index of Si,iZ2n};

    (2) R2={j|j is the index of Mj,jZ2n};

    (3) R3={0|0 is the index of N0};

    (4) R4={1|1 is the index of N1}.

    We see that R1<RR2<RR3 and R1<RR2<RR4. Consequently, we get the following:

    (1) CR1=Span{μi|iZ2n}, on which the action of Hn is given by

    μix=μi+1(mod2n),μiy=0,μiz=0.

    (2) CR2=Span{νj|jZ2n}, on which the action of Hn is given by

    νjx=νj+1(mod2n),νjy=νj+νj+1(mod2n),νjz=0.

    (3) CR3=Span{ξ1}, on which the action of Hn is given by

    ξ1x=ξ1,ξ1y=2ξ1,ξ1z=ξ1.

    (4) CR4CR3.

    In the paper, all indecomposable modules of Hn, a family of positively based algebras, are constructed and classified. Also, their left cell modules are described. In our further study, we will focus on the family of positive based algebras associated to the Green algebras of the dual of the generalized Taft algebra. These results may help us to understand the general representation theory of a positive based algebra.

    All authors declare they have not used Artificial Intelligence (AI) tools in the creation of this article.

    All authors declare no conflict of interest in this paper.



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