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+xn−y)[d−12]∑i=0(−1)i(d−1−ii)xniyd−1−2i=0, for d≥2;(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 d≤4, of tame type if d=5, and of wild type if d≥6. 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 n≥1, 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|1≤i≤n}. For any 1≤i,j,k≤n, if
ai⋅aj=n∑k=1γ(k)i,jak, |
where γ(k)i,j∈R≥0, 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 (0≤i≤2n−1) with a basis {νi} is an Hn-module with the action of Hn:
x⋅νi=ηiνi,y⋅νi=(1+ηi)νi,z⋅νi=0. |
(2) The K-space V1 with a basis {θ1,θ2} is an Hn-module with the action of Hn:
x⋅θ1=−θ1,y⋅θ1=0,z⋅θ1=0,x⋅θ2=−θ2,y⋅θ2=θ1,z⋅θ2=0. |
(3) The K-space V2 with a basis {ξ1,ξ2} is an Hn-module with the action of Hn:
x⋅ξ1=ξ1,y⋅ξ1=ξ2,z⋅ξ1=ξ1,x⋅ξ2=ξ2,y⋅ξ2=2ξ2,z⋅ξ2=2ξ1. | (2.1) |
(4) The K-space V3 with a basis {μj∣0≤j≤2n−1} is an Hn-module with the action of Hn:
x⋅μj=μj+1(mod2n),y⋅μj=0,z⋅μj=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⋯(x⏟2n⋅ξi)⋯))=ξi.(i=1,2), |
Then, the straightforward verification shows that
y⋅(y⋅ξ1)=2ξ2=x⋅(y⋅ξ1)+y⋅ξ1,y⋅(y⋅ξ2)=4ξ2=x⋅(y⋅ξ2)+y⋅ξ2, |
and
y⋅(x⋅ξ1)=ξ2=x⋅(y⋅ξ1),y⋅(x⋅ξ2)=2ξ2=x⋅(y⋅ξ2). |
Moreover, it is obvious that
z⋅(z⋅ξ1)=ξ1=z⋅ξ1,z⋅(z⋅ξ2)=2ξ1=z⋅ξ2, |
and
x⋅(z⋅ξ1)=ξ1=z⋅ξ1=z⋅(x⋅ξ1), |
x⋅(z⋅ξ2)=2ξ1=z⋅ξ1=z⋅(x⋅ξ1). |
Finally, we see that
z⋅(y⋅ξ1)=2ξ1=2z⋅ξ1,z⋅(y⋅ξ2)=4ξ1=2z⋅ξ2. |
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|0≤i≤2n−1,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|0≤i≤2n−1,j,k=0,1}. |
Therefore, it is sufficient to prove that the set
{xiyj,ykz|0≤i≤2n−1,j,k=0,1} |
consists of linearly independent elements.
Now, we assume the following:
2n−1∑i=0aixi+2n−1∑j=0bjxjy+1∑k=0ckykz=0.(I) |
Acting on μ0 by the both sides of (I), we have 2n−1∑i=0aiμi=0 and
ai=0,0≤i≤2n−1. |
It yields that
2n−1∑j=0bjxjy+1∑k=0ckykz=0.(II) |
Acting on {ν0,⋯,νn−1,θ2,νn+1,⋯ν2n−1} by the both sides of (II), we have
(2n−1∑j=0bjxjy+1∑k=0ckykz)⋅θ2=(2n−1∑j=0bjxj)⋅θ1=2n−1∑j=0(−1)jbjθ1=0 |
and
(2n−1∑j=0bjxjy+1∑k=0ckykz)⋅νi=(2n−1∑j=0bjxj)⋅(1+ηi)νi=(1+ηi)2n−1∑j=0ηijbjνi=0. |
Hence, obtain the following:
2n−1∑j=0(−1)jbj=0 and 2n−1∑j=0ηijbj=0(i≠n), |
since 1+ηi≠0.
Thus,
(1⋯111…1⋮⋯⋮⋮⋮⋯⋮1⋯(ηn−1)n−1(ηn−1)n(ηn−1)n+1…(η2n−1)i1⋯(−1)n−1(−1)n(−1)n+1…−11⋯(ηn+1)n−1(ηn+1)n(ηn+1)n+1…(η2n−1)i⋮⋯⋮⋮⋮⋯⋮1⋯(η2n−1)n−1(η2n−1)n(η2n−1)n+1…(η2n−1)2n−1)(b0⋮bn−1bnbn+1⋮b2n−1)=(0⋮000⋮0). |
It is easy to see that the determinant of the coefficient matrix is nonzero; thus, we have the following:
bj=0 for 0≤j≤2n−1. |
Moreover, it yields that
1∑k=0ckykz=0.(III) |
Acting on {ξ1} by the both sides of (III), we have
1∑k=0ckykz⋅ξ1=c0ξ1+c1ξ2=0, |
and c0=c1=0.
In summary,
{xiyj,ykz|0≤i≤2n−1,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 0≤i≤2n−1, N0=z and N1=yz. Let
B={Li,Mi,Nk|0≤i≤2n−1,k=0,1}. |
Then, B is a basis of Hn.
Proposition 2.4. For 0≤i,j≤2n−1, we have the following:
(1) Li⋅Lj=Lj⋅Li=Li+j(mod2n);
(2) Li⋅Mj=Mj⋅Li=Mi+j(mod2n);
(3) Mi⋅Mj=Mj⋅Mi=Mi+j(mod2n)+Mi+j+1(mod2n);
(4) N0⋅N0=N0⋅Li=Li⋅N0=N0;
(5) N0⋅N1=N0⋅Mi=2N0;
(6) N1⋅N0=Mi⋅N0=N1⋅Li=Li⋅N1=N1;
(7) N1⋅N1=N1⋅Mi=Mi⋅N1=2N1.
Proof. For 0≤i,j≤2n−1, by a straightforward verification, we have
Li⋅Lj=xixj=xi+j(mod2n)=Li+j(mod2n)=Lj⋅Li |
and
Li⋅Mj=xixjy=xi+j(mod2n)y=Mi+j(mod2n)=Mj⋅Li, |
since x2n=1,xy=yx.
Hence, (1) and (2) hold.
(3) By y2=xy+y, we have the following:
Mi⋅Mj=xiyxjy=xixjy2=xixj(xy+y)=xi+j(mod2n)y+xi+j+1(mod2n)y=Mi+j(mod2n)+Mi+j+1(mod2n)=Mj⋅Mi. |
(4) By z2=z, we have
Li⋅N0=N0⋅Li=xiz=zxi=z=N0 |
and
N0⋅N0=z2=z=N0. |
(5) By zy=2z, we have
N0⋅N1=zyz=2z2=2z=2N0 |
and
N0⋅Mi=zxiy=zy=2z=2N0. |
(6) First, we have
N1⋅N0=yzz=yz2=yz=N1 |
and
N1⋅Li=yzxi=yz=N1. |
Moreover, we have
Mi⋅N0=xiyz=yxiz=yz=N1 |
and
Li⋅N1=xiyz=yxiz=yz=N1. |
Therefore, N1⋅N0=Mi⋅N0=N1⋅Li=Li⋅N1=N1. (7) First, we have
N1⋅N1=yzyz=2yz2=2yz=2N1 |
and
N1⋅Mi=yzxiy=yzy=2yz=2N1, |
since zy=2z.
Moreover, we have the following:
Mi⋅N1=xiyyz=xi(xy+y)z=xixyz+xiyz=xi+1yz+xiyz=yxi+1z+yxiz=yz+yz=2N1. |
Hence, N1⋅N1=N1⋅Mi=Mi⋅N1=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|0≤i≤2n−1,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,y2−xy−y=0, |
has 4n−1 distinct solutions given by the following:
Γ={(ηi,0)|0≤i≤2n−1}∪{(ηj,1+ηj)|0≤j≤2n−1,j≠n}. |
For each solution (x1,x2)∈Γ, we can define a simple A-module by
x⋅v=x1v,y⋅v=x2v. |
Hence, we have the following Lemma.
Lemma 3.1. (1) For 0≤i≤2n−1, there are 2n non-isomorphic 1-dimensional A-modules Si with the basis {vi}. The action of A is given by the following:
x⋅vi=ηivi,y⋅vi=0. |
(2) For 0≤i≤2n−1 and i≠n, there are 2n−1 non-isomorphic 1-dimensional A-modules Wi with the basis {vi}. The action of A is given by the following:
x⋅vi=ηivi,y⋅vi=(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:
x⋅v1=−v1,y⋅v1=0,x⋅v2=−v2,y⋅v2=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 d≥2. Then, EndV is local and EndV/radEndV≅K. Accordingly, we can assume that the matrices of x and y acting on some suitable basis of V are X=ηiEd and
Y=(λ10⋯000λ1⋯00⋮⋮⋮⋯⋮000⋯λ1000⋯0λ)d×d,λ∈K, |
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 V≅D.
In the following, set
ei=12n2n−1∑k=0η−ikxk |
for 0≤i≤2n−1.
One can easily check that {e0,e1,...,e2n−1} is a set of central idempotents of Hn, and
z(e0−z)=(e0−z)z=0,zei=eiz=0 for 1≤i≤2n−1. |
Therefore, we have the following:
Hn=Hnz⊕Hn(e0−z)⊕Hne1⊕⋯⊕Hne2n−1. |
Now, we can deduce the simple modules and indecomposable modules of Hn by Lemma 3.1 and Proposition 3.2:
(1) For 0≤i≤2n−1, let Si be a 1-dimensional Hn-module with the basis {vi}; the action of Hn is given by
x⋅vi=ηivi,y⋅vi=0,z⋅vi=0. |
(2) For 0≤i≤2n−1 and i≠n, let Wi be a 1-dimensional Hn-module with the basis {vi}; the action of Hn is given by
x⋅vi=ηivi,y⋅vi=(1+ηi)vi,z⋅vi=0. |
(3) The indecomposable Hn-module V1 is produced by extending D, which is given in Lemma 2.2.
Corollary 3.3. V1≅Hnen 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
x⋅yen=−yen,y⋅yen=0,z⋅yen=0,x⋅en=−en,y⋅en=yen,z⋅en=0. |
Hence, it is easy to obtain V1≅Hnen and Sn=topV1 by Lemma 2.2.
The proof is finished.
Lemma 3.4. Hnz≅V2 is a 2-dimensional indecomposable projective Hn-module.
Proof. First, it is easy to have Hnz is projective, since Hn=Hnz⊕Hn(1−z). 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
x⋅z=z,y⋅z=yz,z⋅z=z,x⋅yz=yz,y⋅yz=2yz,z⋅yz=2z. |
By Lemma 2.2, it is easy to obtain that Hnz≅V2.
Suppose that V2=A1⊕A2, where A1 and A2 are nonzero. One has 0≠φ=k1z+k2yz∈A1 for some k1≠0 or k2≠0. Then,
y⋅φ=(k1+2k2)yz∈A1,z⋅φ=(k1+2k2)z∈A1. |
If k1+2k2=0, we get that φ=k2(2z−yz)∈A1 with k2≠0 and 2z−yz∈A1. Accordingly, the decomposition yz=(yz−2z)+2z implies that 2z∈A2 and y⋅z=yz∈A2. Hence, A2=V2, which is a contradiction. This implies that k1+2k2≠0, yz∈A1 and z∈A1. Thus, we have A1=V2, which is also a contradiction.
Therefore, Hnz≅V2 is an indecomposable projective module.
Assume S=Kv is a 1-dimensional Hn-module defined by
x⋅v=v,y⋅v=2v,z⋅v=v. | (3.1) |
Reviewing the action of Hn on V2, we let ξ′1=2ξ1−ξ2, ξ′2=ξ2; then the action of Hn can be written as follows:
x⋅ξ′1=ξ′1,y⋅ξ′1=0,z⋅ξ′1=0,x⋅ξ′2=ξ′2,y⋅ξ′2=2ξ′2,z⋅ξ′2=ξ′1+ξ′2. | (3.2) |
We get that S=topV2 and the exact sequence
0→S0→V2→S→0. |
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) 4n−2 projective simple modules Si and Wi, where 0≤i≤2n−1 and i≠n.
We also need more preparations to list all the indecomposable Hn-modules.
Lemma 3.6. Hn(e0−z)=S0⊕W0.
Proof. For 0≤i≤2n−1, we have
xi(e0−z)=xie0−xiz=e0−z, |
xiy(e0−z)=yxie0−yxiz=ye0−yz, |
and
z(e0−z)=ze0−z2=0,yz(e0−z)=yz−yz2=0. |
Set v1=2e0−2z−ye0+yz, v2=ye0−yz; then, {v1,v2} is a basis of Hn(e0−z) and
x⋅v1=v1,y⋅v1=0,z⋅v1=0,x⋅v2=v2,y⋅v2=2v2,z⋅v2=0. |
By Lemma 2.2, Hn(e0−z)=S0⊕W0.
The result follows.
Lemma 3.7. For 1≤i≤2n−1, 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 1≤i≤2n−1.
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 V2⊕S0 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=V2⊕S0.
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:
0→S0→V2→S→0. |
Assume that
0→S0→Q→S→0 |
is another extension of S0 by S, where Q is indecomposable of the basis {v1,v2}; the action of Hn is given by
x⋅v1=v1,y⋅v1=0,z⋅v1=0,x⋅v2=v2,y⋅v2=2v2,z⋅v2=kv1+v2, |
with k≠0.
Now, let h:V2→Q, which is given by ξ′1↦kv1, ξ′2↦v2. 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,S∣0≤i,j≤2n−1,j≠n}∪{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|i∈I} with the identity a1 of A. For i,j∈I, set
i⋆j={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 s∈I such that j∈s⋆i, then we denoted it by i≤Lj. For i,j∈I, if i≤Lj and j≤Li, we denote it by i∼Lj, which is an equivalent relation. The associated equivalence class is referred to as a left cell. Moreover, we write i<Lj, provided that i≤lj and i≁Lj.
Assume that L is a left cell in I, and let ¯L be the union of all left cells L′ in I such that L′≥L. Set ¯L_=¯L∖L. 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 NL⊂ML. 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|0≤i,j≤2n−1,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,i∈Z2n};
(2) L2={j|j is the index of Mj,j∈Z2n};
(3) L3={k|k is the index of Nk,k=0,1}.
Proof. (1) Set i,i′∈Z2n and i<i′. We obtain Li′−i⋅Li=Li′ by Proposition 2.4. It follows that i′∈(i′−i)⋆i, which implies that i≤Li′. Similarly, we have L2n−i′+i⋅Li′=Li; then, i∈(2n−i′+i)⋆i′ and i′≤Li. The equivalent relation i∼Li′ holds and L1 is a left cell.
(2) Set j,j′∈Z2n and j<j′. We have j′∈(j′−j)⋆j and j≤Lj′, since Mj′−j⋅Mj=Mj′+Mj′+1. Similarly, we obtain that j∈(2n+j−j′)⋆j′ and j′≤Lj. Hence, L2 is a left cell.
(3) By Proposition 2.4, it is obvious that N0⋅N1=2N0 and N1⋅N0=N1. Thus, we have 1≤L0 and 0≤L1. 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,j∈Z2n, we have Mj⋅Li=Mi+j(mod2n) by Proposition 2.4. It is clear that L1<LL2.
Furthermore, by Proposition 2.4, it is easy to see that
N0⋅Mj=N0+N0,N1⋅Mj=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|i∈Z2n}, where ¯Li=Li+NL1, NL1=Span{Mj,Nk|j∈Z2n,k=0,1};
(2) CL2=Span{¯Mj|j∈Z2n}, 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=L1∪L2∪L3,¯L1_=L2∪L3. |
By Proposition 4.1, it follows that
ML1=Span{Li,Mj,Nk|i,j∈Z2n,k=0,1}, |
and
NL1=Span{Mj,Nk|j∈Z2n,k=0,1}. |
Hence,
CL1=ML1/NL1=Span{¯Si|i∈Z2n}. |
(2) By Corollary 4.2, we have
¯L2=L2∪L3,¯L2_=L3. |
It follows that
ML2=Span{Mj,Nk|j∈Z2n,k=0,1}, |
and
NL2=Span{Nk|k=0,1}. |
Therefore,
CL2=ML2/NL2=Span{¯Mj|j∈Z2n}. |
(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|i∈Z2n} and write μi=¯Li with 0≤i≤2n−1. Then, the action of Hn on CL1 is defined by
x⋅μi=μi+1(mod2n),y⋅μi=0,z⋅μi=0. |
Now, set
χi=12n(μ0+η−iμ1+η−2iμ2+⋯+η−(2n−1)iμ2n−1), |
where 0≤i≤2n−1.
A straightforward calculation shows that
x⋅χi=ηiχi,y⋅χi=0,z⋅χi=0. |
Theorem 4.4. CL1 is decomposable and
CL1≅S0⊕S1⊕⋯⊕S2n−1. |
Proof. By Lemma 2.2, the 1-dimensional Hn-module Kχi=Si. Hence, Si is a submodule of CL1. We easily see that
dimK(S0⊕S1⊕⋯⊕S2n−1)=dimKCL1, |
and conclude
CL1≅S0⊕S1⊕⋯⊕S2n−1. |
The proof is completed.
For the left cell module CL2, we have CL2=Span{¯Mj|j∈Z2n} and denote νj=¯Mj with 0≤j≤2n−1. It is easy to see that
x⋅νj=νj+1(mod2n),y⋅νj=νj+νj+1(mod2n),z⋅νj=0. |
Set
ωj=12n(ν0+η−jν1+η−2jν2+⋯+η−(2n−1)jν2n−1) |
for 0≤j≤2n−1.
Then, a straightforward calculation shows that
x⋅ωj=ηjωj,y⋅ωj=(1+ηj)ωj,z⋅ωj=0. |
Theorem 4.5. CL2 is decomposable and
CL2≅W0⊕⋯⊕Wn−1⊕Sn⊕Wn+1⊕⋯⊕W2n−1. |
Proof. On the one hand, by Lemma 2.2, we see that the Hn-module Kωj≅Wj when j≠n, and Kωn≅Sn. Hence, Wj is a submodule of CL2 for 0≤j≤2n−1 and j≠n.
On the other hand, it is easy to see that
dimK(W0⊕⋯⊕Wn−1⊕Sn⊕Wn+1⊕⋯⊕W2n−1)=dimKCL2. |
Hence,
CL2≅W0⊕⋯⊕Wn−1⊕Sn⊕Wn+1⊕⋯⊕W2n−1. |
The proof is finished.
Theorem 4.6. CL3≅V2 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
x⋅N0=N0,y⋅N0=N1,z⋅N0=N0,x⋅N1=N1,y⋅N1=2N1,z⋅N1=2N0. |
Hence, CL3≅V2 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 s∈I such that j∈i⋆s, then one can denote it by i≤Rj. If i≤Rj and j≤Ri, then one can denote it by i∼Rj, 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,i∈Z2n};
(2) R2={j|j is the index of Mj,j∈Z2n};
(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|i∈Z2n}, on which the action of Hn is given by
μi⋅x=μi+1(mod2n),μi⋅y=0,μi⋅z=0. |
(2) CR2=Span{νj|j∈Z2n}, on which the action of Hn is given by
νj⋅x=νj+1(mod2n),νj⋅y=νj+νj+1(mod2n),νj⋅z=0. |
(3) CR3=Span{ξ1}, on which the action of Hn is given by
ξ1⋅x=ξ1,ξ1⋅y=2ξ1,ξ1⋅z=ξ1. |
(4) CR4≅CR3.
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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