This paper classifies all pointed Hopf algebras over an algebraically closed field of characteristic p with dimension p^2q, revealing finitely many classes including new examples not generated by group-like or skew-primitive elements.
Contribution
It provides a complete classification of pointed Hopf algebras of dimension p^2q in characteristic p, identifying new examples and the structure of isomorphism classes.
Findings
01
Finitely many isomorphism classes of such Hopf algebras.
02
10 classes are not generated by group-like or skew-primitive elements.
03
Discovery of many new finite-dimensional pointed Hopf algebras.
Abstract
Let \mathdsk be an algebraically closed field of characteristic p. We give the complete classification of pointed Hopf algebras over \mathdsk of dimension p2q for a prime number q. The result shows that there are finitely many isomorphism classes, including 10 classes that are not generated by group-like elements and skew-primitive elements. In particular, there are many new examples of finite-dimensional pointed Hopf algebras.
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Taxonomy
TopicsAlgebraic structures and combinatorial models · Finite Group Theory Research · Advanced Topics in Algebra
Full text
Pointed Hopf algebras of dimension p2q in characteristic p
Rongchuan Xiong
Department of Mathematics, Changzhou University, Changzhou 213164, China
Let \mathdsk be an algebraically closed field of characteristic p. We give the complete classification of pointed Hopf algebras over \mathdsk of dimension p2q for a prime number q. The result shows that there are finitely many isomorphism classes, including 10 classes that are not generated by group-like elements and skew-primitive elements. In particular, there are many new examples of finite-dimensional pointed Hopf algebras.
Let \mathdsk be an algebraically closed field of characteristic p. This work is devoted to the classification of pointed Hopf algebras over \mathdsk of a given dimension. In general, it is a hard and challenging question even for too many small dimensions. Until now, the complete classifications have been done only for connected Hopf algebras of dimension p2 [39], p3 [20, 21] and pointed ones of dimension p2 [38], 8 [22].
There are some results with some properties. G. Henderson classified cocommutative connected Hopf algebras of dimension p2 and p3 [14]; S. Scherotzke classified rank one pointed Hopf algebras that are generated by the first term of the coalgebra filtration [29]; The author classified non-connected pointed Hopf algebras of dimension 16 that are generated by group-like elements and skew-primitive elements [40]; N. Hu et al. constructed examples of pointed Hopf algebras of dimension pn [15, 16, 32, 33]; C. Cibils et al. [12] and N. Andruskiewitsch et al. [2, 3, 4] gave examples of those whose diagrams are Nichols algebras of non-diagonal type. We mention that the classification of Hopf algebras of some prime dimensions has been completed in [19].
Now we study the classification of pointed Hopf algebras over \mathdsk of dimension p2m with p∤m. N. Andruskiewitsch and S. Natale [6] classified all pointed Hopf algebras of dimension p2q in characteristic zero. The results showed that there are 4(p−1) isomorphism classes and all are generated by group-like elements and skew-primitive elements. As far as we know, it is still an open question to classify those in characteristic zero when m is not a prime number, see e.g. [10] for more details.
Our strategy follows the Lifting Method [7] and the Hochschild cohomology of coalgebras [31], which are proposed to classify pointed Hopf algebras in characteristic zero of dimension p3 and subsequently used in a lot of papers. Let H be a pointed Hopf algebra and grH be the graded Hopf algebra of H associated to the coradical filtration. Then grH≅R♯H0 [24, Theorem 2], where R is a strictly graded Hopf algebra in H0H0YD. The subalgebra of R generated by the space R(1) is the so-called Nichols algebra B(R(1)) (also called quantum shuffle algebra [27]), which plays a key role in the classification of pointed complex Hopf algebras under the following
Conjecture 1**.**
[8, Conjecture 2.7]**
Assume that the base field \mathdsk has characteristic zero. Any finite-dimensional connected graded braided Hopf algebra R=⊕i≥0R(i) in H0H0YD
satisfying P(R)=R(1) is generated by R(1).
As well-known, Conjecture 1 is true for abelian
groups in characteristic zero [9] but it fails in positive characteristic, see e.g. [8, Example 2.5]. Indeed, there are infinitely many examples of pointed Hopf algebras over \mathdsk of dimension pn whose diagrams are not Nichols algebras, see e.g. [39, 20, 21, 22, 41]. The
second Hochschild cohomology groups of coalgebras can control the coproducts of the generators which are not group-like elements and skew-primitive elements, see e.g. [22, Theorem 2.7].
In this paper, we first classify coradically graded pointed Hopf algebras of a given dimension, including classes that are not generated by group-like elements and skew-primitive elements, then compute the liftings and finally determine the isomorphism classes. The lifting procedure is highly non-trivial and computationally challenging especially when the diagrams R are not Nichols algebras or the relations of R(1)♯H0 admit non-trivial deformations. Our main result is
Let H be a pointed Hopf algebra over \mathdsk of dimension p2q. If H is generated by group-like elements and skew-primitive elements, then H is one of the algebras listed in Propositions 5.2 and 5.3; otherwise H is one of the algebras listed in Proposition 5.5.
The result shows that there are finitely many classes of pointed Hopf algebras over \mathdsk of dimension p2q. The Hopf algebras listed in Proposition 5.2 are rank-one pointed Hopf algebras of the second type and the third type in [29]. In Proposition 5.3, except for the classes described in (27)–(28), (33) and (40), they are Radford biproducts of restricted universal enveloping algebras of dimension p2 by \mathdsk[Zq]. We mention that restricted universal enveloping algebras may be not Hopf subalgebras of H. Contrary to the situation in characteristic zero [6], there are 10 classes that are not generated by group-like elements and skew-primitive elements listed in Proposition 5.5.
See Sec. 5.1 for details.
Besides, we also give the complete classification of pointed Hopf algebras of dimension pq and pqr for distinct prime numbers p,q,r, see Corollaries 3.8 and 3.9. Furthermore, we classify pointed Hopf algebras of dimension p2m with abelian coradical, where m is square-free and char\mathdsk=p∤m.
Let m be square-free and char\mathdsk=p∤m. Let H be a pointed Hopf algebra of dimension p2m with abelian coradical. Then H is isomorphic to one of the following Hopf algebras:
(i)
AG(H)k(g,χ,f)* for k∈I1,2 and AG(H)3(g,f) (see Definition 3.1);*
(ii)
\mathdsHk(D)* for k∈I1,8 (see Definition 3.13);*
(iii)
HG(H)k(g,χ)* for k∈I1,4 (see Theorem 4.14).*
The Hopf algebras listed in (i) are rank-one pointed Hopf algebras of the second type and the third type in [29]. The Hopf algebras listed in (ii) are also generated by group-like elements and skew-primitive elements. Among them, \mathdsHk(D) for k∈I1,5 are Radford biproducts of connected (braided) Hopf algebra of dimension p2 by \mathdsk[G(H)], see Remark 3.16 for details. The Hopf algebras listed in (iii) are not generated by group-like elements and skew-primitive elements. Among them, HG(H)k(g,χ) for k∈I1,3 are Radford biproducts of connected Hopf algebras of dimension p2 classified in [39, Lemma 7.3] by \mathdsk[G(H)], see Remark 4.15 for details. To the best of our knowledge, \mathdsHk(D) for k∈I6,8 and HG(H)4(g,χ) constitute new examples of pointed Hopf algebras.
The paper is organized as follows: In Sec. 2, we introduce some necessary notations and concepts. In Sec. 3, we study the classification when the diagrams are Nichols algebras of dimension p or p2. In Sec. 4, we study the classification when diagrams are not Nichols algebras and have dimension p2. In Sec. 5, we give the main results on pointed Hopf algebras of dimension p2m. It seems much more hard to classify pointed Hopf algebras of dimension p2m without the assumptions. Indeed, we are working on the classification of pointed Hopf algebras of dimension p2q2. It turns out that there are examples whose diagrams are braided (not usual) Hopf algebras of dimension pq that are not Nichols algebras.
2. Preliminaries
Conventions
We work over an algebraically closed field \mathdsk. Denote by char\mathdsk the characteristic of \mathdsk, by \mathdsN the set of natural numbers, and by Zn the cyclic group of order n. \mathdsk×=\mathdsk−{0}. Given n≥k≥0, Ik,n={k,k+1,…,n}.
For a Hopf algebra H, G(H):={h∈H∣Δ(h)=h⊗h,ϵ(h)=1} is the group of group-like elements of H. For any g∈G(H), denote by ∣g∣ or ord(g) the order of g. H is said to be pointed if the coradical H0=\mathdsk[G(H)]. Unless otherwise stated, “pointed” means “non-cosemisimple pointed” in our context.
For any g,h∈G(H), Pg,h(H):={c∈H∣Δ(c)=c⊗g+h⊗c} is the set of (g,h)-skew primitive elements of H. In particular, P(H):=P1,1(H) is the space of primitive elements of H.
2.1. q-binomial coefficients
We follow [25] to introduce necessary results on q-binomial coefficients and refer to [25, 26] and the reference therein for more details.
For any given q∈\mathdsk, i≤n∈\mathdsN, denote by ∣q∣ or ord(q) the multiplicative order. The q-number and q-factorial are defined by
[TABLE]
For 0≤i≤n, the q-binomial coefficient is defined inductively by
[TABLE]
In particular, if n≥1 and (n−1)q!=0, then
[TABLE]
Theorem 2.1**.**
[25, Lemma 3]**
Suppose that A is an algebra over \mathdsk and x,y∈A satisfy xy=qyx, where q∈\mathdsk×. Then
[TABLE]
In particular, if char\mathdsk=0, ord(q)=n, or char\mathdsk=p>0, pkord(q)=n, for k∈\mathdsN, then
[TABLE]
2.2. Yetter-Drinfeld modules and bosonizations
Suppose that the Hopf algebra H has bijective antipode. Then the category HHYD of Yetter-Drinfeld modules over H is rigid braided monoidal, where the braiding c is determined by
[TABLE]
and the left dual V∗ is defined by
[TABLE]
Remark 2.2**.**
Suppose that V:=\mathdsk{v} is an object of dimension one in HHYD. By definition, there is an algebra map χ:H→\mathdsk and g∈G(H) satisfying
[TABLE]
such that δ(v)=g⊗v, h⋅v=χ(h)v. Moreover, g lies in the center Z(G(H)) of G(H). Such a triple (G(H),g,χ) is called a YD-triple for convenience.
Remark 2.3**.**
[8, Remark 1.5]**
Denote by GGYD the category \mathdsk[G]\mathdsk[G]YD for short, where \mathdsk[G] is the group algebra of G. For V∈GGYD, set Vg:={v∈V∣δ(v)=g⊗v} for any g∈G. Then as a G-comodule, V:=⊕g∈GVg is a G-graded vector space. Assume in addition that the action of G is diagonalizable, that is, V=⊕χ∈GVχ, where Vχ:={v∈V∣g⋅v=χ(g)v,∀g∈G}. Then
[TABLE]
Let R be a braided Hopf algebra in HHYD and denote ΔR(r)=r(1)⊗r(2) to avoid confusions. The bosonization or Radford biproduct of R by H, denoted by R♯H, is a usual Hopf algebra, whose multiplication and comultiplication are determined by the smash product and smash coproduct, respectively:
[TABLE]
Clearly, the inclusion ι:H→R♯H,h↦1♯h,∀h∈H and the projection
π:R♯H→H,r♯h↦ϵR(r)h,∀r∈R,h∈H are both morphisms of Hopf algebras such that π∘ι=idH.
Furthermore, R=(R♯H)coH={x∈R♯H∣(id⊗π)Δ(x)=x⊗1}.
Conversely, for Hopf algebras A and H, if there are Hopf algebra morphisms π:A→H and ι:H→A such that π∘ι=idH, then A≃R♯H, where R=AcoH is a braided Hopf algebra in HHYD. See [26, pp. 380-384] for details.
2.3. Nichols algebras and Lifting Method
For V∈HHYD, the Nichols algebraB(V) of V is a strictly \mathdsN-graded Hopf algebra B(V)=⊕n≥0Bn(V) in HHYD that is generated as an algebra by V. Namely, B(V) is a \mathdsN-graded Hopf algebra R=⊕n≥0R(n) in HHYD such that
[TABLE]
Furthermore, B(V) depends only on (V,cV,V) and the same braided vector space can be realized in HHYD in many ways and for many H’s.
Remark 2.4**.**
We say that a braided vector space (V,c) of rank m is of diagonal type, if there is a basis {xi}i∈I1,m of V and (qi,j)i,j∈I1,m such that c(xi⊗xj)=qijxj⊗xi, see [1] for details. In char\mathdsk=p>0, if V is of rank 1 with trivial braiding, that is, V=\mathdsk{x} with c(x⊗x)=x⊗x, then B(V)≅\mathdsk[x]/(xp).
Remark 2.5**.**
Let V:=\mathdsk{x1,x2} be a braided vector space of diagonal type with the braiding (qi,j)i,j∈I1,2 satisfying qi,j=1. Then B(V)≅\mathdsk[x,y]/(xp,yp), where x,y are primitive elements. See [37, 35, 36] for more details.
Following the Lifting Method [7], we explain how the Nichols algebra enters into the classification program of pointed Hopf algebra. Let A be a pointed Hopf algebra and {An}n=0∞ the coradical filtration of A, in which
An=A0⋀An−1={a∈A∣Δ(a)∈A0⊗A+A⊗An−1}. Consider the associated graded coalgebra grA, that is, grA=⊕n=0∞grnA with gr0A=A0
and grnA=An/An−1. It is well-known that grA is a Hopf algebra admitting the Hopf
algebra projection of grA onto A0, which is denoted by π:grA↠A0.
Then π splits the inclusion i:A0↪grA. Therefore, grA≅R♯A0, where R=(grA)coA0 is a Hopf algebra
in A0A0YD. Furthermore, R has the following properties:
(1)
R=⊕n=0∞R(n) is a graded Hopf algebra in A0A0YD, where R(n)=R∩H(n);
(2)
R is connected, that is, R(0)≅\mathdsk;
(3)
P(R)=R(1).
Definition 2.6**.**
With the notations as above, the algebra R and the part R(1) are called the diagram and the infinitesimal braiding of A, respectively.
Furthermore, the subalgebra of R generated by
R(1) is the Nichols algebra of R(1), which
plays a key role in the classification of pointed complex Hopf algebra under
the following
Conjecture 2**.**
[8, Conjecture 2.7]**
Let A be a finite-dimensional pointed complex Hopf algebra and keep the notations as above. Then the diagram R is a Nichols algebra.
Remark 2.7**.**
To the best of our knowledge, all examples of finite-dimensional Hopf algebras with char\mathdsk=0 support Conjecture 2. However, it is not always true in positive characteristic, see e.g. [8, Example 2.5]. Furthermore, there are infinite families of pointed Hopf algebras of dimension pn whose diagrams are not Nichols algebras. See e.g. [20, 21, 22, 41] for details.
2.4. The Hochschild cohomology
We introduce some basic concepts on the Hochschild cohomology of coalgebras and explain how it enters into the classification program. See [31, 34, 39, 22]) for more details.
Definition 2.8**.**
[31, Sec. 1]**
Let C be a pointed coalgebra and
(M,δL,δR) a C-bicomodule. Set idn:=idC⊗n. The Hochschild cohomologyH∙(M,C) of C with coefficients in M is defined by the homology of the complex (Cn(M,C),dn)n∈\mathdsN, where Cn(M,C)=Hom\mathdsk(M,C⊗n) and
[TABLE]
Set Zn(M,C):=Ker∂n, Bn(M,C):=Im∂n−1 and Hn(M,C):=Zn(M,C)/Bn(M,C). Furthermore,
Proposition 2.9**.**
[31, Proposition 1.4]**
Hn(M,C)≅Hn(C∗,M∗), where M∗ is endowed with a natural C∗-bimodule structure.
For g,h∈G(C) and M:=g\mathdskh with δL(k)=h⊗k and δR(k)=k⊗g, for k∈\mathdsk, H∙(g\mathdskh,C) can be computed as the homology of the complex (C⊗n,dg,hn), whose differentials are given by
[TABLE]
Set dn:=d1,1n, Zn(\mathdsk,C):=Zn(1\mathdsk1,C), Bn(\mathdsk,C):=Bn(1\mathdsk1,C) and Hn(\mathdsk,C):=Hn(1\mathdsk1,C) for short.
Remark 2.10**.**
The differentials in low degrees are explicitly given as follows:
[TABLE]
There is a close connection between the Hochschild cohomology of a pointed coalgebra and its coradical filtration.
Theorem 2.11**.**
[31, Theorem 1.2]**
Let C be a pointed coalgebra. Then
(1)
Pg,h(C)/\mathdsk(g−h)≅H1(g\mathdskh,C).
2. (2)
Cng,h/Cn−1≅ker[H2(g\mathdskh,Cn−1)→H2(g\mathdskh,C)]* for any n>1, where Cng,h={x∈C∣Δ(x)=x⊗g+h⊗x+ω,ω∈Cn−1⊗Cn−1}.*
As an application, we have the following result (see also [34, Lemma 2.3]).
Proposition 2.12**.**
[31, Corollary 1.3]**
Let C be a pointed coalgebra, D a subcoalgebra of C and g,h∈G(C). Suppose that there is n>0 such that Dn=Cn. Then the differential dg,h1 induces an injective map
[TABLE]
In particular, if H2(g\mathdskh,D)=0, then Dn+1g,h=Cn+1g,h.
Consider a strictly graded pointed coalgebra C=∑i=0nC(n), then H∙(g\mathdskh,C) admits a bi-grading structure with the homological grading and the Adams grading, that is, Hi(g\mathdskh,C)=⊕j=0nHi,j(g\mathdskh,C),
where Hi,j(g\mathdskh,C)⊂Hi(g\mathdskh,C) consists of homogeneous elements whose Adams grading is j.
Now we introduce the following braided version of Proposition 2.12 due to [19, Theorem 2.7]:
Theorem 2.13**.**
Let R=⊕n≥0R(n) be a strictly graded Hopf algebra in GGYD and S be a graded Hopf subalgebra of R in GGYD. Suppose that there exists n>1∈\mathdsN satisfying R(k)=S(k) for k∈I0,n. Then d1 induces an injective map in GGYD
[TABLE]
Proof.
For any r∈R(n+1), by assumptions,
[TABLE]
Furthermore, from the coassociativity of ΔR, we have d2∣S(d1(r))=0 and hence d1(r)∈Z2(\mathdsk,S). Consequently, d1 is well-defined in GGYD.
Now assume that d1(r)=0 in H2(\mathdsk,S). Then there exists s∈S such that d1(r)=d1(s), that is, Δ(r−s)=(r−s)⊗1+1⊗(r−s). Hence r−s∈P(R)=R(1)=S(1)⊂S and so r∈S(n+1). This completes the proof.
∎
2.5. Useful results in positive characteristic
Now we introduce some useful results, which shall be used hereafter. Denote (adLx)(y):=[x,y] and (x)(adRy)=[x,y].
Proposition 2.14**.**
[17, pp.186–187]**
Let A be an associative algebra with char\mathdsk=p>0 and a,b∈A. Then
[TABLE]
Furthermore,
[TABLE]
where ksk(a,b) is the coefficient of λk−1 in (a)(adRλa+b)p−1, λ an indeterminate.
Remark 2.15**.**
s1(a,b)=(a)(adRb)p−1=∑i=0p−1biabp−1−i.**
Lemma 2.16**.**
Let H be a pointed Hopf algebra over \mathdsk, x∈Hg,h,and y∈H1,k for some g,h,k∈G(H). Assume that g,h,k,x generate a commutative Hopf subalgebra A of H and d1,k1(y)∈A. Then
[TABLE]
Proof.
It follows by a direct computation that
[TABLE]
∎
The following lemma is due to [29, Corollary 4.10] and [38] (also [22, Lemma 5.1(1)]).
Lemma 2.17**.**
Let A be an associative algebra over \mathdsk with generators g, x, subject to the relations gn=1,gx−xg=g(1−g). Assume that char\mathdsk=p>0. Then
**(1): **
gix=xgi+igi−igi+1. In particular, gpx=xgp.
**(2): **
(g)(adRx)p−1=g−gp, (g)(adRx)p=[g,x].
**(3): **
(adLx)p−1(g)=g−gp, [xp,g]=(adLx)p(g)=[x,g].
Proof.
**(1): **
Note that (g)(adRx)=[g,x]=g−g2. Then (adRx):\mathdsk⟨g⟩→\mathdsk⟨g⟩ is a derivation. It follows that [gi,x]=igi−1[g,x]=igi−igi+1.
**(2): **
This is [22, Lemma 5.1(1)] when n=pk for k>0. As stated in the proof of [22, Lemma 4.0.1(1)], the linear map (adRx):\mathdsk⟨g⟩→\mathdsk⟨g⟩ is diagonalizable with eigenvalues 0,1,…,n−1. Then by Fermat’s little Theorem, (adRx)p=adRx. Moreover, after a direct computation, (g)(adRx)p−1=g−gp.
**(3): **
The proof follows the same line of (2).
∎
The following result is useful to determine when a coalgebra map is one-one.
Proposition 2.18**.**
[26, Proposition 4.3.3]**
Let C,D be coalgebras over \mathdsk and f:C→D is a coalgebra map. Assume that C is pointed. Then the following are equivalent:
(a)
f* is one-one.*
(b)
For any g,h∈G(C), f∣Pg,h(C) is one-one.
(c)
f∣C1* is one-one.*
3. The diagrams are Nichols algebras
Let char\mathdsk=p>0 and p∤m. In this section, we study the classification of pointed Hopf algebras whose diagrams are Nichols algebras of dimension p or p2 to obtain our main results. In particular, we give the complete classification of pointed Hopf algebras of dimension pq and pqr for distinct prime numbers p,q,r.
3.1. The diagram has dimension p
We determine finite-dimensional pointed Hopf algebras whose diagrams have dimension p, which were essentially classified in [29] in a different way. As a byproduct, we give the complete classification of pointed Hopf algebras of dimension pq and pqr.
Definition 3.1**.**
Let (G,g,χ) be a YD triple such that χ(g)=1,
where G is a group of order n with generators h1,⋯,ht and a fixed set of defining relations Rt. Let f be a map from G to \mathdsk such that f(hk)=χ(k)f(h)+f(k) for any h,k∈G, with condition: f is the zero map if g=1. Let
(1)
AG1(g,χ,f):=\mathdsk⟨h1,⋯,ht,x⟩/(Rt,h1x−χ(h1)xh1−f(h1)(1−g),⋯,htx−χ(ht)xht−f(ht)(1−g),xp), if f(h)(1−gp)=0 for any h∈G and f(g)=0;
(2)
AG2(g,χ,f):=\mathdsk⟨h1,⋯,ht,x⟩/(Rt,h1x−χ(h1)xh1−f(h1)(1−g),⋯,htx−χ(ht)xht−f(ht)(1−g),xp−x), if χp−1=ϵ, gp−1=1, f(g)=0 and f(h)p=f(h) for any h∈G;
(3)
AG3(g,f):=\mathdsk⟨h1,⋯,ht,x⟩/(Rt,h1x−xh1−f(h1)h1(1−g),⋯,htx−xht−f(ht)ht(1−g),xp−f(g)x), if p∣ord(g), χ=ϵ, f(g)=1 and f(h)p=f(h) for any h∈G.
They admit a Hopf algebra structure given by Δ(h)=h⊗h for h∈G and Δ(x)=x⊗1+g⊗x.
Remark 3.2**.**
(1)
*For any n∈\mathdsN and h∈G, f(hn)=∑i=0n−1χ(h)if(h). From which, f(hq)=0 when χ(h) is a primitive *qth root of unity. Furthermore,
[TABLE]
If χ(h)=1 and p∤ord(h), then f(h)=0. In particular, the case f(g)=0 occurs only when g=1 and p∣ord(g).
(2)
If χ=ϵ, then f is a morphism of groups from G to (\mathdsk,+). Furthermore, if χ=ϵ and p∤ord(G), then f must be the zero map (we write f=0 for short).
(3)
Let A be one of the Hopf algebras in Definition 3.1. If g=1, then f=0; otherwise there is an exact sequence of \mathdsk[G]-modules:
[TABLE]
For any fixed h∈G, if p∤ord(h), then as ⟨h⟩-modules, the exact sequence is split and hence we can choose f(h)=0. Furthermore, we can take f=0 when p∤ord(G).
(4)
The Hopf algebras AGi(g,χ,f) for i∈I1,2 and AG3(g,f) are rank-one pointed Hopf algebras of the second type and third type in **[29]**, respectively.
(5)
In what follows, denote AGi(g,χ):=AGi(g,χ,0) with i∈I1,2 for short.
Remark 3.3**.**
(i)
It is clear that {xih,h∈G,i∈I0,p−1} is a basis of AGk(g,χ) for k∈I1,2. Then one can check easily that π:AGk(g,χ)→\mathdsk[G],xih→h is a bialgebra map admitting a bialgebra
section ι:\mathdsk[G]→AGk(g,χ) such that π∘ι=id. Therefore, Ak(g,χ)≅R♯\mathdsk[G] for k∈I1,2, where R≅\mathdsk[x]/(xp) or \mathdsk[x]/(xp−x).
(ii)
Here \mathdsk[x]/(xp) and \mathdsk[x]/(xp−x) are usual Hopf algebras of dimension p appeared in **[39]**. Furthermore, they are dual Hopf algebras of \mathdsk[T]/(Tp) and \mathdsk[X]/(Xp−1), respectively, where Δ(T)=T⊗1+1⊗T and Δ(X)=X⊗X (See **[39, Corollary 7.2]**). In particular, up to isomorphism, they are regarded as Hopf subalgebras of the algebra of distributions on Ga and Gm, respectively
(see **[18, 7.8 and 7.10]**).
(iii)
For k∈I1,2, by **[5, 2.2]**, AGk(χ,g)∗≅R∗♯(\mathdsk[G])∗, where R∗≅\mathdsk[T]/(Tp) or \mathdsk[X]/(Xp−X) with T∈P(R∗) and X∈G(R∗), respectively.
Proposition 3.4**.**
grAGi(g,χ,f)≅\mathdsk[x]/(xp)♯\mathdsk[G]* for i∈I1,2 and grAG3(g,f)≅\mathdsk[x]/(xp)♯\mathdsk[G].*
Proof.
Let A be one of the Hopf algebras in Definition 3.1. It is easy to check that A0=\mathdsk[G] and Ai=Ai−1+\mathdsk[G]{xi} for i∈I1,p−1. Therefore, grA≅R♯\mathdsk[G], where R≅\mathdsk[x]/(xp).
∎
Proposition 3.5**.**
(1)
AG1(g,χ,f)≅AG1(g′,χ′,f′)* if and only if there exists F∈Aut(G) such that F(g)=g′, χ⋅F−1=χ′ and αf′F−f+β(χ−ϵ)=0 for some α∈\mathdsk×,β∈\mathdsk satisfying β(1−gp)=0.*
(2)
AG2(g,χ,f)≅AG2(g′,χ′,f′)* if and only if there exists F∈Aut(G) such that F(g)=g′, χ⋅F−1=χ′ and αf′F−f+β(χ−ϵ)=0 for some α∈\mathdsk×,β∈\mathdsk satisfying αp=α and (βp−β)(1−g)=0.*
(3)
AG3(g,f)≅AG3(g′,f′)* if and only if there exists F∈Aut(G) such that F(g)=g′ and f⋅F−1=f′.*
Proof.
(1)-(2):
Suppose that there is a Hopf algebra isomorphism ϕ:AGi(g,χ,f)→AGi(g′,χ′,f′), then by Proposition 2.18, ϕ∣G∈Aut(G) and ϕ(P1,g(AGi(g,χ)))=P1,g′(AGi(g′,χ′)). Hence we assume that ϕ(g)=g′ and ϕ(x)=αx′+β(1−g′) for α=0,β∈\mathdsk. If g′=1, then we assume that β=0. Since ϕ(hxh−1−χ(h)x−f(h)(1−g))=0, it follows that χ′⋅ϕ=χ and [αf′ϕ−f+β(χ−ϵ)](h)(1−g′)=0. Applying ϕ to the relation xp=(i−1)x, we have (i−1)(αp−α)=0 and βp(1−(g′)p)=(i−1)β(1−g′).
If g′=1, then g=1, f=0=f′ and (i−1)(αp−α)=0. If g′=1 and (g′)p=g′, then i=1 and αf′ϕ−f+β(χ−ϵ)=0 satisfying βp(1−(g′)p)=0. If g′=1 and (g′)p=g′, then αf′F−f+β(χ−ϵ)=0 for some α∈\mathdsk×,β∈\mathdsk satisfying (i−1)(αp−α)=0 and βp=(i−1)β.
Conversely, let ψ be the algebra morphism determined by ψ(h)=F(h),ψ(x)=αx′+β(1−g′), then it is clear that ψ is a Hopf algebra isomorphism.
As Hopf algebras, AG1(g,χ,f), AG2(g,χ,f) and AG3(g,f) are pairwise non-isomorphic.
Proof.
We first claim that AG1(g,χ,f)≅AG2(g,χ,f). Indeed, if there is a Hopf algebra isomorphism ϕ:AG1(g,χ,f)→AG2(g,χ,f), then ϕ∣G∈Aut(G) and ϕ(P1,g(AG1(g,χ,f)))=P1,g′(AG2(g′,χ′,f′)), which implies that ϕ(g)=g′ and ϕ(x)=αx′+β(1−g′) for α=0. On the other hand, we have α=0 when applying ϕ to the relations hx−χ(h)x=f(h)h(1−g) and xp=0 in AG1(g,χ,f), a contradiction. Consequently, the claim follows.
Similarly, AGk(g,χ,f)≅AG3(g,f) for k∈I1,2.
∎
Now we introduce the following result, which is essentially appeared in [29] in a different way.
Theorem 3.7**.**
Let H be a finite-dimensional pointed Hopf algebra whose diagram has dimension p. Then there exists a tuple (G(H),g,χ,f) such that H is isomorphic to AG(H)1(g,χ,f), AG(H)2(g,χ,f) or AG(H)3(g,f).
Proof.
Since x∈P1,g(H), it follows that hx−χ(h)xh∈Ph,hg(H)∩H0. If g=1, then Ph,h(H)∩H0=0; otherwise Ph,hg(H)∩H0=\mathdsk{h(1−g)}. Hence hx−χ(h)xh=f(h)h(1−g), where f is a map from G(H) to \mathdsk with condition: f=0 when g=1. Then consider the conjugation of \mathdsk[G], we have f(hk)=χ(k)f(h)+f(k). If f(g)=0 and g=1, then applying f to the relation gk=kg for any k∈G(H), we have χ(g)f(k)+f(g)=χ(k)f(g)+f(k), which implies that χ=ϵ and thereby f(hk)=f(h)+f(k).
Observe that gx−xg=f(g)g(1−g). Then by Proposition 2.14 and Lemma 2.17,
[TABLE]
which implies that xp−f(g)p−1x∈P1,gp(H)∩Hp−1.
Assume that gp=g. Then xp=λ2x+λ3(1−gp) for λ2,λ3∈\mathdsk and f(g)=0. By induction, hxn=[χ(h)x+f(h)(1−g)]nh for n∈\mathdsN and h∈G(H). In particular,
[TABLE]
The verification of h(xp)=(hx)xp−1 imposes the conditions:
[TABLE]
Let A(g,χ,f,λ2,λ3) be the Hopf algebra described as above. Then consider the translation x↦x+a(1−g) satisfying ap−λ2a=λ3, we have A(g,χ,f,λ2,λ3)≅A(g,χ,f+a(ϵ−χ),λ2,0).
If λ2=0, then clearly f+a(ϵ−χ)=0 and so A(g,χ,f,λ2,λ3)≅AG(H)1(g,χ). If λ2=0, then χp−1=ϵ and by the translation x↦b−1x satisfying bp−1=λ2, we have
[TABLE]
Assume that gp=g. Then xp−f(g)p−1x=λ4(1−gp). Furthermore,
[TABLE]
If f(g)=0, then from (hx)xp−1=h(xp), we have [λ4(χp−ϵ)(h)+f(h)p](1−gp)=0; otherwise χ=ϵ and then we have
[TABLE]
Similar to the last case, we may choose λ4=0 by the translation x↦x+a(1−g) satisfying ap−f(g)p−1a=λ4.
If f(g)=0, then f(h)(1−gp)=0 and H≅AG(H)1(g,χ,f); otherwise we have χ=ϵ, f(g)p−1f(h)=f(h)p and then by the translation x↦f(g)−1x, we can take f(g)=1 and thereby H≅AG(H)3(g,f).
∎
Corollary 3.8**.**
Set Zq:=⟨g⟩ and Zq:=⟨χ⟩. Let H be a pointed Hopf algebra of dimension pq for a prime number q. Then H is isomorphic to AZq1(1,ϵ), AZq2(1,ϵ), AZq1(g,ϵ), AZq2(g,ϵ), AZq1(1,χ) or AZq2(1,χ).
Proof.
Let R be the diagram of H and V:=R(1). We claim that G(H)≅Zq. By Nichols-Zoeller Theorem [23], dimH0∣dimH, which implies that dimH0=p,q. If dimH0=p, that is, H0≅\mathdsk[Zp], then there must be an element x∈Vgϵ for some g∈G(H) with trivial braiding. Hence \mathdsk[x]/(xp) is a braided Hopf subalgebra of R. Then by [13] or [28, Proposition 2.16], dim\mathdsk[x]/(xp)=p must divide dimR=q, a contradiction.
Consequently, dimH0=q, that is, G(H)≅Zq.
Since G(H)≅Zq:=⟨g⟩, it follows that dimR=p. Then by Theorem 3.7, H≅AZqk(gi,χj) for k∈I1,2 and some i,j∈I0,q−1 such that ξij=1, where χ(g)=ξ is a primitive qth root of unity. Furthermore, ξij=1 yields i=0 or j=0. If i=0, then up to change the character χ, we can take j∈I0,1. If j=0, then we can take i∈I0,1. This completes the proof.
∎
Corollary 3.9**.**
Set Zqr:=⟨g⟩, Zqr:=⟨χ⟩ and Zq⋊Zr:=⟨τ⟩. Let H be a pointed Hopf algebra of dimension pqr for distinct prime numbers p,q,r. Then H is isomorphic to AZqr1(1,χj), AZqr2(1,χj) for j∈{0,1,q,r}, AZqr1(gi,ϵ), AZqr2(gi,ϵ) for i∈{1,q,r}, AZq⋊Zr1(1,τ) or AZq⋊Zr2(1,τ).
Proof.
Let R be the diagram of H and V:=R(1).
We claim that dimH0=qr. Indeed, by Nichols-Zoeller Theorem [23], dimH0∣dimH, which implies that dimH0=p,q,r,pq,qr,pr. If dimH0=pq, then G(H)≅Zpq:=⟨ζ⟩ and dimR=r. Hence dimR(1)=1 with a basis {x}. Furthermore, x∈Vgζi,i∈I0,q−1 with g∈G(H), which implies that c(x⊗x)=ζi(g)x⊗x. Therefore, R contains a braided Hopf subalgebra of dimension p or q, a contradiction. Hence dimH0=pq. Similarly, we have dimH0=pr,qr,p,q,r. Therefore, the claim follows.
Assume that G(H)=Zqr=⟨g⟩. Then dimR=p and hence dimV=1 with trivial braiding. Let V:=\mathdsk{x} and G(H)=⟨χ⟩, where χ(g)=θ is a primitive qrth root of unity. Then by Remark 2.2, x∈Vgiχj for some i,j∈I0,qr−1 such that θij=1, which implies that qr∣ij. Hence i=0 or j=0. If i=0, then by Proposition 3.5, we can take j∈{0,1,q,r}. If j=0, then we can take i∈{0,1,q,r}.
Assume that G(H)=Zq⋊Zr. Then dimR=p and hence dimV=1 with trivial braiding. Let V:=\mathdsk{x} and G(H)=⟨τ⟩, where τ(g)=ξ is a primitive qth root of unity, and τ(h)=1. Since the center of G(H) is trivial, by Remark 2.2, x∈V1τi for some i∈I0,q−1. By Proposition 3.5, we can take i∈I0,1.
[38, Theorem 3.3]**
Let H be a non-connected pointed Hopf algebra of dimension p2 and g a generator of Zp. Then H is isomorphic to AZp1(1,ϵ), AZp2(1,ϵ), AZp1(g,ϵ) or AZp3(g,f).
Proof.
Let R be the diagram of H. By assumptions, dimH0=p and hence G(H)≅Zp and R≅\mathdsk[x]/(xp) with Yetter-Drinfeld module structure given by g⋅x=x,δ(x)=gi⊗x for i∈I0,p−1. By changing the generator, we may choose i∈I0,1.
Observe that f=0 when f(g)=0. If i=0, then by Theorem 3.7, H is isomorphic to AZp1(1,ϵ) or AZp2(1,ϵ); otherwise H is isomorphic to AZp1(g,ϵ) or AZp3(g,f).
∎
3.2. Liftings of quantum
planes
We determine liftings of quantum
planes of dimension p2.
Definition 3.11**.**
A QPYD-datum D(G,χ1,χ2,g1,g2) consists of a group G of order m, characters χ1,χ2∈G and g1,g2∈Z(G) satisfying χ1(g1)=1=χ2(g2)=χ1(g2)χ2(g1). We write D:=D(G,χ1,χ2,g1,g2) for short.
Lemma 3.12**.**
Let V:=\mathdsk{x,y} and D a QPYD-datum. Then (V,D)∈GGYD with x∈Vg1χ1, y∈Vg2χ2. Furthermore, dimB(V,D)=p2.
Proof.
It follows by the fact that (V,D) is a quantum plane.
∎
Now we determine liftings of B(V,D)♯\mathdsk[G].
For a QPYD datum D:=D(G,χ1,χ2,g1,g2), we set qij:=χj(gi) and [x,y]c=xy−q12yx for short.
Definition 3.13**.**
For k∈I1,8,
[TABLE]
where Ik is the ideal given as follows:
•
I1:=([x,y]c,xp,yp);
•
I2:=([x,y]c,xp−x,yp), if χ1p−1=ϵ, g1p−1=1;
•
I3:=([x,y],xp−y,yp), if χ1p=χ2, g1p=g2;
•
I4:=([x,y]c,xp−x,yp−y), if χ1p−1=ϵ=χ2p−1, g1p−1=1=g2p−1;
•
I5:=([x,y]−y,xp−x,yp), if χ1=ϵ, g1=1;
•
I6:=([x,y]−(1−g1g2),xp,yp), if χ1χ2=ϵ, g1g2=1;
•
I7:=([x,y]−y−(1−g2),xp−x,yp), if χ1=ϵ=χ2, g1=1, g2=1;
•
I8:=([x,y],xp−y,yp−x), if χ1p=χ2, χ2p=χ1, g1p=g2, g2p=g1 and g1=g2 or χ1p=χ2, χ2p=χ1, g1=g2, g1p−1=1 and χ1=χ2.
If no confusions, we also denote \mathdsHk(χ1,χ2,g1,g2):=\mathdsHk(D) for k∈I1,8.
Lemma 3.14**.**
For k∈I1,8, \mathdsHk(D) is a Hopf algebra with
[TABLE]
Proof.
It follows by direct computations that Δ(Ik)⊂\mathdsHk(D)⊗Ik+Ik⊗\mathdsHk(D) and ϵ(Ik)=0.
∎
Lemma 3.15**.**
For k∈I1,8, dim\mathdsHk(D)=p2m.
Proof.
Applying the Diamond Lemma [11], it suffices to verify the following overlaps:
[TABLE]
are resolvable with the order y<x<g, where g∈G with order mg. We omit the details to save spaces, since it is tedious but straightforward.
∎
Remark 3.16**.**
Observe that {yixjh,h∈G,i,j∈I0,p−1} is a basis of \mathdsHk(D). For k∈I1,8−{6,7}, it is easy to see that the projection π:\mathdsHk(D)→\mathdsk[G],yjxih→h is a bialgebra map admitting a bialgebra
section ι:\mathdsk[G]→\mathdsHk(D) such that π∘ι=id. Then \mathdsHk(D)≅R♯\mathdsk[G] for k∈I1,8−{6,7}, where R≅T(V)/Ik is a (maybe not usual) connected Hopf algebra of dimension p2. If χ2(g1)=1 (e.g. k∈{3,5}), then R is one of the restricted universal enveloping algebras of 2-dimensional restricted Lie algebras classified in [39, Proposition A.3].
Proposition 3.17**.**
For k∈I1,8, gr\mathdsHk(D)=B(V,D)♯\mathdsk[G].
Proof.
Let F(n):=F(n−1)+\mathdsk[G]{yixj∣i+j=n,i,j∈I0,p−1 with F(0)=\mathdsk[G].
It is easy to check that the filtration {F(n),n∈I0,p2−1} is a Hopf algebra filtration. Therefore, (\mathdsHk(D))0=\mathdsk[G] and hence \mathdsHk(D) is a pointed Hopf algebra with coradical \mathdsk[G]. Furthermore, grF\mathdsHk(D)=R♯\mathdsk[G], where grF\mathdsHk(D) is the graded Hopf algebra associated to the filtration {F(n),n∈I0,p2−1}. Clearly, V⊂P(R). Since dimR=dimB(V)=p2, it follows that R=B(V,D). Therefore, the filtration {F(n),n∈I0,p2−1} is the coradical filtration of \mathdsHk(D).
∎
Proposition 3.18**.**
Let D:=D(G,χ1,χ2,g1,g2) and D′:=D(G,χ1′,χ2′,g1′,g2′).
For k∈I1,8, \mathdsHk(D)≅\mathdsHk(D′) if and only if there exists f∈Aut(G) and σ∈S2 such that f(gσ(i))=gi′ and χσ(i)⋅f−1=χi′.
Proof.
Set x1:=x and x2:=y for convenience. Suppose that ψ:\mathdsH1(D)→\mathdsHk(D′) is an isomorphism of Hopf algebras. Then ψ∣G∈Aut(G) and ψ(xi)∈P1,ψ(gi)(\mathdsHk(D′)).
If χ1′=χ2′=χ and g1′=g2′=g, then ψ(g1)=g=ψ(g2), which implies that g1=g2. Furthermore, there exist some αi,βi∈\mathdsk for i∈I1,3 such that
[TABLE]
If g=1, we let α3=0=β3. Since hxih−1=χi(h)xi for all h∈G, we see that
[TABLE]
Hence χ1=χ⋅ψ∣G=χ2.
If χ1′=χ2′ or g1′=g2′, then there is σ∈S2 and α1,α2∈\mathdsk−{0},β1,β2∈\mathdsk such that
[TABLE]
where βi=0, if gσ(i)′=1. Indeed, if g1′=g2′, then dimP1,gi′(\mathdsH(D′))=1 and hence the claim follows; if g1′=g2′ and χ1′=χ2′, then using the adjoint action of \mathdsk[G], one can check easily that the claim follows.
Consequently, applying ψ to the relations hxih−1=χi(h)xi for all h∈G, we have χi=χσ(i)′⋅ψ∣G.
Conversely, let f∈Aut(G) and σ∈S2 such that f(gσ(i))=gi′ and χσ(i)⋅f−1=χi′. Then one can extend f to a Hopf algebra isomorphism from \mathdsHk(D) to \mathdsHk(D′) by f(xi)=xσ−1(i)′.
∎
Proposition 3.19**.**
Let D:=D(G,χ1,χ2,g1,g2), D′:=D(G,χ1′,χ2′,g1′,g2′) and i,j∈I1,8.
If i=j, then \mathdsHi(D)≅\mathdsHj(D′) as Hopf algebras.
Proof.
We show that \mathdsH1(D)≅\mathdsHk(D′) for k∈I2,8. Set x1:=x and x2:=y for convenience. Assume that ψ:\mathdsH1(D)→\mathdsHk(D′) for k∈I2,8 is an isomorphism of Hopf algebras. Then ψ∣G∈Aut(G) and ψ(xi)∈P1,ψ(gi)(\mathdsHk(D′)).
If χ1′=χ2′=χ and g1′=g2′=g, then as shown in the proof of Proposition 3.18, g1=g2 and χ1=χ2 and there exist some αi,βi∈\mathdsk for i∈I1,3 such that
[TABLE]
with conditions: α3=0=β3 if g=1. Applying ϕ to the relations [x1,x2]=0, x1p=0 and x2p=0, we see that
[TABLE]
Then from the defining relations in \mathdsHk(D′), one can check easily that α1β2−α2β1=0, a contradiction.
If χ1′=χ2′ or g1′=g2′, then there is σ∈S2 and α1,α2∈\mathdsk−{0},β1,β2∈\mathdsk such that
[TABLE]
where βi=0, if gσ(i)′=1. Since (x1′)p=0, (x2′)p=0 or [x1′,x2′]c=0, from [x1,x2]=0, x1p=0 and x2p=0, we have
α1α2=0, a contradiction.
Similarly, for any i∈I2,7, one can show that \mathdsHi(D)≅\mathdsHk(D′) for all k∈Ii+1,8.
∎
Definition 3.20**.**
For a QPYD-datum D:=D(G,χ1,χ2,g1,g2) with p∤ord(G), let \mathdsH be a Hopf algebra such that gr\mathdsH≅B(V,D)♯\mathdsk[G].
Lemma 3.21**.**
There exists an epimorphism of Hopf algebras from T(V,D)♯\mathdsk[G] to \mathdsH.
Proof.
Set x1:=x and x2=y for convenience. Since xi∈P1,gi(\mathdsH) for i∈I1,2, it follows that there exist two maps f1,f2 from G to \mathdsk such that hxih−1=χi(h)xi+fi(h)(1−gi) with conditions: fi=0 if gi=1.
If gi=1 and g1=g2, then there is an exact sequence of G-modules:
[TABLE]
Since p∤ord(G)=m, \mathdsk[G] is semisimple and so the sequence is split, which implies that P1,gi(\mathdsH)=\mathdsk{1−gi}⊕\mathdsk{xi} as G-modules. Hence we can choose fi=0.
If g1=g2=1, then there is an exact sequence of G-modules:
[TABLE]
The sequence is also split since \mathdsk[G] is semisimple, and hence we can choose f1=f2=0.
∎
Remark 3.22**.**
By Lemma 3.21, it remains to determine liftings of the relations in B(V,D).
Lemma 3.23**.**
(i)
[x,y]c∈P1,g1g2(\mathdsH).
(ii)
xp∈P1,g1p(\mathdsH), yp∈P1,g2p(\mathdsH).
Proof.
Since x∈P1,g1(\mathdsH) and y∈P1,g2(\mathdsH), it follows that xy−q12yx∈P1,g1g2(\mathdsH). By Lemma 3.21, we have g1x=xg1 and g2y=yg2. Then by Theorem 2.1, xp∈P1,g1p(\mathdsH), yp∈P1,g2p(\mathdsH).
∎
Proposition 3.24**.**
Assume that dimP(\mathdsH)=2. Then there exists k∈I1,8−{6,7} such that \mathdsH≅\mathdsHk(D).
Proof.
By assumption, we have g1=g2=1 and so P(\mathdsH)=V. Then by Lemma 3.23, xy−yx,xp,yp∈P(\mathdsH). Since P(\mathdsH)=\mathdsk{x,y}, there exist α1,α2,β1,β2,γ1,γ2∈\mathdsk such that
[TABLE]
Consider the adjoint action of \mathdsk[G], we have the following conditions:
•
α1=0, if χ1p−1=ϵ;
•
α2=0, if χ1p=χ2;
•
β1=0, if χ2p=χ1;
•
β2=0, if χ2p−1=ϵ;
•
γ1=0, if χ2=ϵ;
•
γ2=0, if χ1=ϵ.
Let K be the subalgebra of \mathdsH generated by P(\mathdsH). Then Lemma 3.21 and equations (8) imply that K is a Hopf subalgebra of \mathdsH. Furthermore, \mathdsH≅K♯\mathdsk[G]. Observe that K is a usual connected Hopf algebras of dimension p2. Indeed, K is isomorphic to the restricted universal enveloping algebra U(P(H)) of P(H). Then by [39, Proposition A.3], K is isomorphic to one of the following Hopf algebras
(1)
\mathdsk[x,y]/(xp,yp),
2. (2)
\mathdsk[x,y]/(xp−x,yp),
3. (3)
\mathdsk[x,y]/(xp−y,yp),
4. (4)
\mathdsk[x,y]/(xp−x,yp−y),
5. (5)
\mathdsk⟨x,y⟩/(xp−x,yp,[x,y]−y).
**Case 1: ** Assume that χ1=χ2=ϵ. Then by Lemma 3.21, for any h∈G, hx=xh and hy=yh. Therefore, \mathdsH≅U(P(H))⊗\mathdsk[G] and consequently \mathdsH≅\mathdsHi(χ1,χ2,g1,g2) for i∈I1,5.
**Case 2: ** Assume that χ1=ϵ and χ2=ϵ(χ2p=ϵ). Then α2=γ1=0=β1, that is, xp=α1x, yp=β2y and xy−yx=γ2y.
By induction, we have
[TABLE]
In particular, xpy=yxp+γ2py and xyp=ypx. Then
[TABLE]
Hence the verification of (xp)y=xp−1(xy), x(yp)=(xy)yp−1 and (yp)y=y(yp) imposes the conditions
[TABLE]
If γ2=0, then we can take α1,β2∈I0,1 by rescaling x,y. If α1=β2∈I0,1, then \mathdsH≅\mathdsH1(χ1,χ2,g1,g2) or \mathdsH4(χ1,χ2,g1,g2). If α1−1=0=α2, then \mathdsH≅\mathdsH2(χ1,χ2,g1,g2). If α1=0=α2−1, then χ2p−1=ϵ and hence \mathdsH≅\mathdsH2(χ2,χ1,g2,g1).
If γ2=0, then β2=0 and α1=γ2p−1. Hence we can take α1=γ1=1 via the linear translation x↦γ2−1x and hence \mathdsH≅\mathdsH5(χ1,χ2,g1,g2).
**Case 3: ** Assume that χ1=ϵ and χ2=ϵ. Then by swapping (χ1,g1,x) and (χ2,g2,y), it is the last case.
**Case 4: ** Assume that χ1=χ2=ϵ. Then γ1=γ2=0, that is, xp=α1x+α2y, yp=β1x+β2y, xy−yx=0. If χ1p−1=ϵ, then αi=βi=0 for i∈I1,2 and hence \mathdsH≅\mathdsH1(χ1,χ2,g1,g2).
If χ1p−1=ϵ, then one can check easily that for any isomorphism ψ∈Aut(U(P(\mathdsH))), there is ϕ∈Aut(\mathdsH) (e.g. ψ♯id) such that ϕ∣U(P(H)=ψ, and then by [39, Proposition A.3.], \mathdsH≅\mathdsHi(χ1,χ2,g1,g2) for i∈I1,4. Indeed, for any ψ∈Aut(U(P(\mathdsH))), there are some a1,a2,b1,b2∈\mathdsk such that
[TABLE]
Since x,y,xp,yp∈P(\mathdsH)χ1={t∈P(\mathdsH)∣hth−1=χ1(h)t,∀h∈G}, it follows that ψ is also an isomorphism of Hopf algebras in GGYD and hence ψ♯id∈Aut(\mathdsH).
**Case 5: ** Assume that χ1=ϵ,χ2=ϵ and χ1=χ2. Then γ1=0=γ2. that is, xp=α1x+α2y, yp=β1x+β2y, xy−yx=0.
If χ1p−1=ϵ=χ2p−1, then χ1p=χ1=χ2 and χ2p=χ2=χ1. Hence α2=β1=0, and by rescaling x,y, we can take α1,β2∈I0,1. If α1=β2∈I0,1, then \mathdsH≅\mathdsH1(χ1,χ2,g1,g2) or \mathdsH4(χ1,χ2,g1,g2). If α1−1=0=α2, then \mathdsH≅\mathdsH2(χ1,χ2,g1,g2). If α1=0=α2−1, then \mathdsH≅\mathdsH2(χ2,χ1,g2,g1).
If χ1p−1=ϵ and χ2p−1=ϵ, then χ1p=χ2 and χ2p=χ1. Indeed, if χ2p=χ1, then χ2p=χ1p and so χ1=χ2, a contradiction. Therefore, α2=0=β2=β1. Then by rescaling x, we take α1∈I0,1 and hence \mathdsH≅\mathdsHi(χ1,χ2,g1,g2) for i∈I1,2.
If χ1p−1=ϵ and χ2p−1=ϵ, then by swapping (χ1,g1,x) and (χ2,g2,y), it is the last case.
If χ1p−1=ϵ and χ2p−1=ϵ, then α1=β2=0. If χ1p=χ2 and χ2p=χ1, then α2=0=β1 and hence \mathdsH≅\mathdsH1(χ1,χ2,g1,g2).
If χ1p=χ2 and χ2p=χ1, then β1=0 and α2∈I0,1 by rescaling x, which implies that \mathdsH≅\mathdsHi(χ1,χ2,g1,g2) for i∈{0,3}. If χ1p=χ2 and χ2p=χ1, then by swapping (χ1,g1,x) and (χ2,g2,y), it is the last case. If χ1p=χ2 and χ2p=χ1, then xp=α2y and yp=β1x for α2,β1∈\mathdsk. If α2=0, then by rescaling y, we can take β1∈I0,1 and hence \mathdsH≅\mathdsHk(χ1,χ2,g1,g2) for k∈{1,3}.
If β1=0, then by swapping x and y, it is the last case.
If α2=0 and β1=0, then we can take α2=1=β1 via the linear translation
x↦a−1x,y↦b−1y satisfying ap=α2b and bp=β1a and hence \mathdsH≅\mathdsH8(χ1,χ2,g1,g2).
∎
Proposition 3.25**.**
Assume that dimP(\mathdsH)=1. Then there is k∈I1,7 such that \mathdsH≅\mathdsHk(D).
Proof.
By assumption, we may assume that g1=1 and g2=1. By Lemma 3.23, xy−yx∈P1,g2(\mathdsH), xp∈P(\mathdsH) and yp∈P1,g2p(\mathdsH). Since P(\mathdsH)=\mathdsk{x} and P1,g2(\mathdsH)=\mathdsk{1−g2,y},
[TABLE]
for some λ2,λ3,λ4∈\mathdsk. Consider the adjoint action of \mathdsk[G], we have the conditions
•
λ2=0, if χ1p−1=ϵ;
•
λ3=0, if χ1=ϵ;
•
λ4=0, if χ1χ2=ϵ.
Now we determine liftings of yp=0 in gr\mathdsH. Since p∤ord(G(\mathdsH)), it follows that g2p=1. Therefore, there are the follows two cases.
**Case 1: ** Suppose that g2p−1=1, that is, g2p=g2. Then yp=λ5y+λ6(1−g2p) for some λ5,λ6∈\mathdsk. Consider the adjoint action of \mathdsk[G], we have conditions:
•
λ5=0, if χ2p−1=ϵ;
•
λ6=0, if χ2=ϵ.
By induction, for n>0, we have
[TABLE]
In particular, we have
[TABLE]
Then
[TABLE]
Then the overlaps x(yyp−1)=(xy)yp−1,xp−1(xy)=(xp−1x)y gives the conditions
[TABLE]
It is easy to check that other overlaps are resolvable and give no conditions.
Assume that λ2=0. Then equations (9) imply that λ3=0 and we can choose λ6=0 via the linear translation y↦y−a(1−g) satisfying ap−λ5a=λ6. Furthermore, we can also take λ4,λ5∈I0,1 by rescaling x,y. Observe that λ4λ5=0.
If λ4=0=λ5, then \mathdsH≅\mathdsH1(χ1,χ2,g1,g2); if λ4=0=λ5−1, then χ2p−1=ϵ, g2p=g2 and hence \mathdsH≅\mathdsH2(χ2,χ1,g2,g1); if λ4−1=0=λ5, then χ1χ2=ϵ and \mathdsH≅\mathdsH6(χ1,χ2,g1,g2)
Assume that λ2=0. Then χ1p−1=ϵ and we can take λ2=1 by rescaling x. If λ5=0, then χ2p−1=ϵ and equations (9) imply that λ3=λ4=0. By rescaling y, we can take λ5=1. Furthermore, we can choose λ6=0 via the linear translation y↦y+a(1−g2) satisfying ap−a=λ6. Hence \mathdsH≅\mathdsH4(χ1,χ2,g1,g2).
If λ5=0, then λ3p=λ3, (1−λ3p−1)λ4=0 and hence we can take λ3∈I0,1 by rescaling x and take λ6=0 via the linear translation y↦y−a(1−g) satisfying ap=λ6. If λ3=0, then λ4=0 and hence \mathdsH≅\mathdsH2(χ1,χ2,g1,g2). If λ3=1, then we take λ4∈I0,1 and hence \mathdsH≅\mathdsHi(χ1,χ2,g1,g2) for i∈{5,7}.
**Case 2: ** Suppose that g2p−1=1, that is, g2p=g2. Then yp=λ7(1−g2p) for some λ7∈\mathdsk with conditions: λ7=0 if χ2=ϵ.
Similar to the last case, we have
[TABLE]
Applying the Diamond Lemma, the verification of overlaps (3)–(6) amounts to conditions:
[TABLE]
We take λ7=0 via the linear translation y↦y+a(1−g) satisfying ap=λ7.
If λ2=0, then λ3=0 and we can take λ4∈I0,1 by rescaling x.
Hence \mathdsH≅\mathdsHi(χ1,χ2,g1,g2) for i∈{1,6}.
If λ2=0, then we can take λ2=1 by rescaling x. Hence λ3p=λ3 and (λ3p−1−1)λ4=0. We can take λ3∈I0,1 by rescaling x. If λ3=0, then λ4=0 and hence \mathdsH≅\mathdsH2(χ1,χ2,g1,g2). If λ3=1, then we take λ4∈I0,1 by rescaling y and hence \mathdsH≅\mathdsHi(χ1,χ2,g1,g2) for i∈{5,7}.
∎
Proposition 3.26**.**
Assume that dimP1,g(\mathdsH)=2 for some g=1. Then there exists k∈I1,8−{5,7} such that \mathdsH≅\mathdsHk(D).
Proof.
By assumption, we may assume that g1=g2=g=1. Then by Lemma 3.23, xp,yp∈P1,g1p(\mathdsH) and [x,y]∈P1,g1g2(\mathdsH). Observe that P1,g1(\mathdsH)=\mathdsk{x}⊕\mathdsk{y}⊕\mathdsk{1−g1} and P1,g1g2(\mathdsH)=\mathdsk{1−g1g2}. Hence
[TABLE]
where λ3,…,λ9∈\mathdsk with conditions: λ3=λ4=λ6=λ7=0, if g1p−1=1. Consider the adjoint action of \mathdsk[G], we have the following conditions:
Similarly, the overlaps (3), (4), (5) are resolvable and give no conditions. The verification of (7) amounts to the condition
[TABLE]
We can choose λ9∈I0,1 by rescaling x,y.
If λ9=0, then we can take λ5=0=λ8 via the linear translation x↦x+α1(1−g),y↦y+α2(1−g) satisfying
[TABLE]
Indeed, since \mathdsk is algebraically closed, equations have the solutions. If g1p−1=1, then λ3=λ4=λ6=λ7=0 and hence \mathdsH≅\mathdsH1((χ1,χ2,g1,g2). Now we assume that g1p−1=1.
Assume that χ1=χ2. If χ1p=χ1, then χ1p=χ2 and χ2p=χ1, which implies that λ4=0=λ6. Indeed, if χ2p=χ1, then χ1p=χ2p and so χ1=χ2, a contradiction. By rescaling x,y, we can take λ3,λ7∈I0,1 and hence \mathdsH≅\mathdsHi(χ1,χ2,g1,g2) for i∈{1,2,4}. If χ2p=χ2, then by exchanging x with y, we have \mathdsH≅\mathdsHi(χ1,χ2,g1,g2) for i∈{1,2,4}. If χ1p=χ1 and χ2p=χ2, then λ3=0=λ7. If λ4=0, then by rescaling y, we can take λ6∈I0,1 and hence \mathdsH≅\mathdsHk(χ1,χ2,g1,g2) for k∈{1,3}. If λ6=0, then by swapping x and y, it is the last case.
If λ4=0 and λ6=0, then we can take λ4=1=λ6 by rescaling x,y and hence \mathdsH≅\mathdsH8(χ1,χ2,g1,g2).
Assume that χ1=χ2. If χ1p=χ1, then χ1p=χ2, χ2p=χ1 and χ2p=χ2 and hence λ3=λ4=λ6=λ7=0, which implies that \mathdsH≅\mathdsH1(χ1,χ2,g1,g2).
If χ1p=χ1, then χ1p=χ2p=χ1=χ2.
It is clear that \mathdsH=S(λ3,λ4,λ6,λ7)♯\mathdsk[G], where S(λ3,λ4,λ6,λ7):=\mathdsk[x,y]/(xp−(λ3x+λ4y),yp−(λ6x+λ7y))∈GGYD with
[TABLE]
Let S:=S(λ4,λ5,λ6,λ7) for short. Clearly, S is a usual connected Hopf algebra of dimension p2. Observe that x,y,xp,yp∈P1,g1χ1(\mathdsH)={t∈P1,g(\mathdsH)∣hth−1=χ1(h)t,∀h∈G}. Then one can easily check that for any isomorphism ψ∈Aut(S), ψ is also an isomorphism of Hopf algebras in GGYD and hence there is ϕ∈Aut(\mathdsH) (e.g. ψ♯id) such that ϕ∣S=ψ; Then by [39, Proposition A.3], \mathdsH≅\mathdsHi(χ1,χ2,g1,g2) for i∈I1,4.
If λ9=1, then χ1χ2=ϵ, λ3=0=λ7 and λ4=0=λ6. Furthermore, we can take λ5=0=λ8 via the linear translation x↦x−a(1−g),y↦y−b(1−g) satisfying ap=λ5 and bp=λ8. Hence \mathdsH≅\mathdsH6(χ1,χ2,g1,g2).
∎
Proposition 3.27**.**
Assume that g1=1,g2=1,g1=g2. Then there exists k∈I1,8−{5,7} such that \mathdsH≅\mathdsHk(D).
Proof.
By assumption, g1g2−1=1, P1,g1(\mathdsH)=\mathdsk{x}⊕\mathdsk{1−g1} and P1,g2(\mathdsH)=\mathdsk{y}⊕\mathdsk{1−g2} and P1,g1g2(\mathdsH)=\mathdsk{1−g1g2}. By Lemma 3.23, xp∈P1,g1p(\mathdsH),yp∈P1,g2p(\mathdsH) and [x,y]c∈P1,g1g2(\mathdsH). Then
[TABLE]
for λ0∈\mathdsk. Consider the adjoint action of \mathdsk[G], we have the condition: λ0=0 if χ1χ2=ϵ. Furthermore, if χ1χ2=ϵ, then χ1(g2)=χ2(g1)=1.
**Case 1: ** Suppose that g1p=g1(=g2). Then g2p=g1. Indeed, if g2p=g1, then g1p=g2p, that is, (g1g2−1)p=1, which implies that p∣m=∣G∣, a contradiction. Therefore, there are λ2,λ3,λ4,λ5∈\mathdsk such that
[TABLE]
with conditions:
•
λ1=0, if χ1p−1=ϵ;
•
λ2=0, if χ1p−1=ϵ or g2p−1=1;
•
λi+2=0, if χi=ϵ for i∈I1,2.
Furthermore, if λ3=0 or λ4=0, then χ1(g2)=χ2(g1)=1. Then we can take λ3=0=λ4 via the linear translation x↦x+a(1−g1),y↦b(1−g2) satisfying ap−λ1a=λ3,bp−λ2b=λ4. We can take λ1,λ2∈I0,1 by rescaling x,y.
If λ1=λ2∈I0,1, then \mathdsH≅\mathdsH1(χ1,χ2,g1,g2) or \mathdsH4(χ1,χ2,g1,g2). If λ1−1=0=λ2, then \mathdsH≅\mathdsH2(χ1,χ2,g1,g2). If λ1=0=λ2−1, then \mathdsH≅\mathdsH2(χ2,χ1,g2,g1).
**Case 2: ** Suppose that g1p=g2(=g1). Then χ1(g2)=1=χ2(g1) and g2p=g2. Indeed, if g2p=g2, then g1p=g2p and hence g1=g2, a contradiction. Therefore,
[TABLE]
for λ2,λ3,λ4,λ5∈\mathdsk with conditions:
•
λ1=0, if χ1p=χ2;
•
λ2=0, if χ2p=χ1 or g2p=g1;
•
λi+2=0, if χi=ϵ for i∈I1,2.
The verification of [xp,x]=0 and [yp,y]=0 amounts to the conditions
[TABLE]
If λ2=0, then we can take λ3=0=λ4 via the linear translation x↦x+a(1−g1),y↦b(1−g2) satisfying ap−λ1b=λ3,bp=λ4. Then we can take λ0,λ1∈I0,1 by rescaling x,y. If λ0=0, then λ1∈I0,1 and hence \mathdsH≅\mathdsH1(χ1,χ2,g1,g2) or \mathdsH3(χ1,χ2,g1,g2). If λ0=1, then λ1=0 and hence \mathdsH≅\mathdsH6(χ1,χ2,g1,g2).
If λ2=0, then λ0=0, χ2p=χ1 and g2p=g1. Furthermore, we can take λ3=0=λ4 via the linear translation x↦x+a(1−g1),y↦y+b(1−g2) satisfying ap−λ1b=λ3,bp−λ2a=λ4.
Then we can take λ2=1 and λ1∈I0,1 by rescaling x,y. Therefore, \mathdsH≅\mathdsH3(χ2,χ1,g2,g1) or \mathdsH8(χ1,χ2,g1,g2).
**Case 3: ** Suppose that g1p=g1,g1p=g2. If g2p=g2, then by swapping x and y, it is the case 1. If g2p=g1, then by swapping x and y, it is the case 2. Therefore, we may assume that g2p=g1,g1p=g2 and hence there exist λ3,λ4∈\mathdsk such that
[TABLE]
If χ1χ2=ϵ, then χ1(g2)=χ2(g1)=1 and we can take λ3=0=λ4 via the linear translation x↦x+a(1−g1),y↦y+b(1−g2) satisfying ap=λ3,bp=λ4. Therefore, \mathdsH≅\mathdsH1(χ1,χ2,g1,g2) or \mathdsH6(χ1,χ2,g1,g2).
If χ1χ2=ϵ, then λ0=0 and λ3λ4=0. If χ1=ϵ or χ2=ϵ, then χ1(g2)=χ2(g1)=1 and we can take λ3=0=λ4 via the linear translation x↦x+a(1−g1),y↦y+b(1−g2) satisfying ap=λ3,bp=λ4; otherwise consider the adjoint action of \mathdsk[G], we have λ3=0=λ4. Consequently, \mathdsH≅\mathdsH1(χ1,χ2,g1,g2).
∎
Theorem 3.28**.**
There exists k∈I1,8 and a QPYD-datum D such that \mathdsH≅\mathdsHk(D) as Hopf algebras.
Proof.
By definition, \mathdsH≅gr\mathdsH as coalgebras. According to the spaces of skew-primitive elements, there are four possibilities: (1) dimP(\mathdsH)=2, (2) dimP(\mathdsH)=1, (3) dimP1,g(\mathdsH)=2 for some g=1∈G, (4) dimP1,g1(\mathdsH)=1=dimP1,g2(\mathdsH) with g1=1,g2=1. Consequently, it follows by Propositions 3.24, 3.25, 3.26 and 3.27.
∎
4. The diagrams are not Nichols algebras
Let char\mathdsk=p>0. In this section, we study pointed Hopf algebras of dimension p2m whose diagrams are not Nichols algebras and have dimension p2. We first classify the coradically graded ones, then determine the liftings and finally determine the isomorphism classes.
4.1. The coradically graded pointed Hopf algebras of dimension p2m
Let H be a coradically graded pointed Hopf algebra of dimension p2m that is not generated by group-like elements and skew-primitive elements, where G(H) is of order m with (p,m)=1. We study the structure of H.
Lemma 4.1**.**
[22, 4.2 Case (C)]**
Let char\mathdsk=p>0 and B(V)=\mathdsk[x]/(xp) with V:=\mathdsk{x}. Then dimH2(\mathdsk,B(V))=1 with a generator ω0(x), where
[TABLE]
Lemma 4.2**.**
Let R:=⊕n=0∞R(n) be a strictly graded Hopf algebra in GGYD for some group algebra \mathdsk[G] such that B(R(1))=p. Assume that R is not a Nichols algebra. Then R contains a Hopf subalgebra S of dimension p2, where S≅\mathdsk[x,y]/(xp,yp)∈GGYD with
[TABLE]
with x∈R(1)gχ and y∈R(p)gpχp for some g∈Z(G(H)) and χ∈G(H) satisfying χ(g)=1.
Proof.
Let V:=R(1) for short. By assumption, dimV=1 with trivial braiding. Set V:=\mathdsk{x}. Then B(V)=\mathdsk[x]/(xp), which is a usual connected Hopf algebra of dimension p. Furthermore, by Remark 2.2, B(V)∈GGYD with x∈Vgχ, where g lies in the center of G, χ∈G satisfying χ(g)=1.
By Lemma 4.1, dimH2(\mathdsk,B(V))=1 with a generator ω0(x). Since ω0(x)∈∑i=1p−1R(i)⊗R(p−i) and {xi}i=0p−1 is a basis of B(V), the total degree of ω0(x) is p and B(V)(p)=0.
Then by Theorem 2.13, there is an isomorphism in GGYD:
[TABLE]
Therefore, dimR(p)=1 and there exists a basis {y} of R(p) such that d1(y)=ω0(x), that is,
[TABLE]
Furthermore, for any h∈G,
[TABLE]
Then using the braiding formula in GGYD, we have c(a⊗b)=b⊗a for a,b∈{x,y}. Furthermore, it follows by a direct computation that xy−yx∈P(R)=R(1)∩R(p+1) and hence xy−yx=0 in R. Then
[TABLE]
which implies that yp∈R(1)∩R(p2) and hence yp=0 in R. Consequently, S:=K[x,y]/(xp,yp) is the Hopf subalgebra of R generated by x and y in GGYD.
∎
Corollary 4.3**.**
With the notations in Lemma 4.2, p2∣dimR. In particular, if dimR=p2, then R≅S in GGYD.
Proof.
It follows directly by Lemma 4.2 and [28, Proposition 2.16].
∎
Remark 4.4**.**
The Hopf algebra S:=\mathdsk[xp,yp] in GGYD is a usual co-commutative graded connected Hopf algebra of dimension p2 classified in [14] (see also [39, 22]).
Theorem 4.5**.**
Let H be a coradically graded pointed Hopf algebra with char\mathdsk=p of dimension p2m such that dimH0=m. Suppose that H is not generated by group-like elements and skew-primitive elements. Then
H is generated by generators of G(H), and x,y, subject to the relations in G(H) and the following:
[TABLE]
where x∈P1,g(H) for some g∈Z(G(H)) and χ∈G(H) such that χ(g)=1 and
[TABLE]
Proof.
By assumption, H≅R♯H0, where R=HcoH0 is a strictly graded Hopf algebra of dimension p2 in H0H0YD. Since R is not a Nichols algebra, it follows that dimB(R(1))=p. Consequently, the assertion follows by Lemma 4.2 and Corollary 4.3.
∎
4.2. Liftings of H
Suppose that char\mathdsk=p and p∤m. Let H be a pointed Hopf algebra with abelian coradical such that grH≅H as Hopf algebras and H≅H as coalgebras.
By Theorem 4.5, H is generated by h1,h2,⋯,ht, x and y, where hi,i∈I1,t generate the group G(H) of order m, x∈P1,g(H) for some g∈Z(G(H)) and
[TABLE]
Now we determine defining relations of H. Set ωg(x):=∑i=1p−1i!(p−i)!(p−1)!xigp−i⊗xp−i for short in what follows.
Lemma 4.6**.**
The relation hx−χ(h)h=0 for h∈G(H) holds in H.
Proof.
If g=1, then we have P(H)≅\mathdsk{x} as G(H)-modules, otherwise as well-known, there is an exact sequence of G(H)-modules:
[TABLE]
By the assumption that (m,p)=1, \mathdsk[G(H)] is semisimple and so the exact sequence is split, which implies that P1,g(H)≅\mathdsk{1−g}⊕\mathdsk{x} as G(H)-modules. Consequently, the relation hx−χ(h)xh=0 holds in H for h∈G(H).
∎
Lemma 4.7**.**
The relation hy−χp(h)yh=0 for h∈G(H) holds in H.
Proof.
By Lemma 4.6, hx−χ(h)xh=0 for h∈G(H) in H. Observe that Δ(h)ωg(x)=χp(h)ωg(x)Δ(h). Then it follows by a direct computation that
[TABLE]
Therefore, hy−χp(h)yh∈Ph,gph(H)∩Hp−1.
Assume that gp−1=1. Then Ph,gph(H)=\mathdsk{h(1−gp)} and there is a map λ:G(H)→\mathdsk such that hy−χp(h)yh=λhh(1−gp). Then consider the conjugation of G(H), we have λhk=χp(k)λh+λk. Observe that G(H) is abelian. Then from λhk=λkh, we have [1−χp(h)]λk=[1−χp(k)]λh.
If χp(h)=1, then we can take λh=0 via the linear translation y↦y−α(1−gp) satisfying (1−χp(h))α=λh. If χp(h)=1, then
0=[1,y]=[hmh,y]=mhλh(1−gp) and so λh=0.
Assume that gp−1=1. Then Ph,gph(H)=\mathdsk{h(1−gp),xh} and there are two map λ,γ from G(H) to \mathdsk such that hy−χp(h)yh=λhxh+γhh(1−gp). If g=1, then set γh=0. Then consider the conjugation of G(H), we have λhk=χp(k)λh+χ(h)λk and γhk=χp(k)γh+γk. From λhk=λkh and γhk=γkh, we have [χ(h)−χp(h)]λk=[χ(k)−χp(k)]λh and [1−χp(h)]γk=[1−χp(k)]γh.
Let ξ=χ(h) for short. By induction, we have
[TABLE]
Then from [hmh,y]=[1,y]=0 for mh=ord(h), we have
[TABLE]
If χp(h)=1, that is, ξp=1, then we have γh=0 since (mh,p)=1; otherwise,
we can take
γh=0 via the linear translation y↦y−α(1−gp) satisfying (1−χp(h))α=λh.
If χp−1(h)=1, that is, ξ1−p=1, then λh=0; otherwise we can take
λh=0 via the linear translation y↦y−αx satisfying αχ(h)(1−χp−1(h))=λh. One can directly verify the translations as described above are isomorphisms of Hopf algebras.
∎
Lemma 4.8**.**
There exists λ∈I0,1 such that xp=λx in H with condition: λ=0 if gp−1=1 or χp−1=ϵ.
Assume that gp−1=1. Then P1,gp(H)=\mathdsk{1−gp} and hence xp=λ1(1−gp) for some λ1∈\mathdsk. If χ=ϵ, then consider the adjoint action of \mathdsk[G(H)], we have λ1=0, otherwise we can take λ1=0 via the translation x↦x−a(1−g) satisfying ap=λ1.
Assume that gp−1=1. Then P1,gp(H)=\mathdsk{1−gp,x} and hence xp=λ2x+λ3(1−gp) for some λ2,λ3∈\mathdsk.
If χp=χ, then consider the adjoint action of \mathdsk[G(H)], we have λ2=0=λ3. If χp=χ=ϵ, then λ3=0. If χ=ϵ, then we can take λ3=0 via the linear translation x↦x−a(1−g) satisfying ap−λ2a=λ3.
By rescaling x, we can take λ2∈I0,1.
∎
Lemma 4.9**.**
There exist λ,γ∈\mathdsk such that
[TABLE]
in H with the conditions: λ=0 if g=1 or χ=ϵ; γ=0 if χp+1=ϵ or gp+1=1. In particular, λγ=0.
Proof.
Observe that Δ(x)ωg(x)=ωg(x)Δ(x). Then
[TABLE]
that is, xy−yx∈P1,gp+1(H).
Assume that g=1. Then P1,gp+1(H)=P(H)=\mathdsk{x} and so [x,y]=λx for λ∈\mathdsk.
If χp=ϵ, that is, χ=ϵ, then consider the adjoint action of \mathdsk[G(H)], we have λ=0.
Assume that g=1. Then P1,gp+1(H)=\mathdsk{1−gp+1} and so [x,y]=γ(1−gp+1) for some λ∈\mathdsk. If χp+1=ϵ, then consider the adjoint action of \mathdsk[G(H)], then γ=0.
∎
Lemma 4.10**.**
Assume the situation described as above, for n>0,
[TABLE]
Proof.
It follows by induction on n.
∎
The following result generalizes the relative results in [22, Case C].
Let Y:=yp−([x,y]xp−1)(adRy)p−2. If gp−1=1 and χp−1=ϵ, then xp=λx for λ∈I0,1 and Y−λpy∈P1,gp2(H)=P1,g(H); otherwise Y∈P1,gp2(H).
Proof.
If gp−1=1 and χp−1=ϵ, then by Lemma 4.8, xp=λx for λ∈I0,1. Since Δ(y)=y⊗1+gp⊗y+ωg(x) and ωg(xp)=ωg(λx), it follows that Y−λpy∈P1,gp2(H)=P1,g(H). Otherwise xp=0 in H and so ωg(xp)=0, which implies that Y∈P1,gp2(H).
∎
Theorem 4.14**.**
Let RG be the set of defining relations of G:=G(H) and hx=χ(h)xh,hy=χp(h)yh for h∈G(H). Then H is isomorphic to one of the following Hopf algebras:
HG2(g,χ):=\mathdsk⟨h1,⋯,ht,x,y⟩/(RG,[x,y],xp,yp−x), if χp−1=ϵ and gp−1=1;
(3)
HG3(g,χ):=\mathdsk⟨h1,⋯,ht,x,y⟩/(RG,[x,y],xp−x,yp−y), if χp−1=ϵ and gp−1=1;
(4)
HG4(g,χ):=\mathdsk⟨h1,⋯,ht,x,y⟩/(RG,[x,y]−1+gp+1,xp,yp+(1−gp+1)p−1x−x), if gp−1=1, χp−1=ϵ, gp+1=1 and χp+1=ϵ;
where hi∈G(H) for i∈I1,t, x∈P1,g(H) for some g∈Z(G(H)) and χ∈G(H) such that χ(g)=1 and
[TABLE]
Proof.
By Lemmas 4.6, 4.7 and 4.8, the following relations hold in H:
[TABLE]
for λ1∈I0,1 with conditions: λ1=0, if gp−1=1 or χp−1=ϵ.
**Case 1. ** Assume that g=1. Then by Lemma 4.9, [x,y]=λ2x for λ2∈\mathdsk with conditions: λ2=0, if g=1 or χ=ϵ.
Observe that ([x,y]xp−1)(adRy)p−2=(λ2xp)(adRy)p−2=λ1λ2p−1x. Then by Corollary 4.13,
yp−λ1λ2p−1x−λ1py∈P(H)∩Hp−1 and hence yp−λ1py=λ3x for λ3∈\mathdsk. Consider the adjoint action of \mathdsk[G(H)], we have λ3=0 if χp−1=ϵ.
By Lemma 4.10, xpy=yxp, xyp=ypx+λ2px.
Then
the verification of [xp,y]=(adLx)p(y) and [x,yp]=(x)(adRy)p gives the conditions
[TABLE]
If λ1=0, then we can choose λ3∈I0,1 by rescaling x,y and obtain two classes described in (1)–(2).
If λ1=1, then gp−1=1, χp−1=1 and so we can take λ3=0 via the linear translation y↦y−bx satisfying bp−b=λ3, which gives one class of H described in (3).
Case 2. Assume that g=1. Then by Lemma 4.9, [x,y]=λ2(1−gp+1) for λ2∈\mathdsk with conditions: λ2=0, if gp+1=1 or χp+1=ϵ. Observe that ([x,y]xp−1)(ady)p−2=(p−1)![x,y]p−1x=(p−1)!λ2p−1(1−gp+1)p−1x.
**Case 2a. ** If gp−1=1 and χp−1=ε, then by Corollary 4.13, yp−([x,y]xp−1)(ady)p−2−λ1py∈P1,g(H). Therefore,
[TABLE]
If χ=ϵ, then consider the adjoint action of \mathdsk[G(H)], we have ν2=0; otherwise we take ν2=0 via the linear translation y↦y−a(1−g) satisfying ap−λ1pa=ν2.
Observe that (p−1)!=−1. The verification of [xp,y]=(adLx)p(y), [x,yp]=(x)(adRy)p and [y,yp]=0 amounts to the conditions
[TABLE]
If λ1=1, then λ2=0. We can take ν1=0 via the linear translation y↦y−ax satsifying ap=ν1, which gives one class described in (3).
If λ1=0=λ2, then we take ν1∈I0,1 by rescaling x,y, which gives two classes described in (1)−(2).
If λ1=0 and λ2=0, then gp+1=1 and χp+1=ϵ. Furthermore, we take λ2=1 via the linear translation x↦a−1x,y↦a−py satisfying ap+1=λ2, and hence ν1=1, which gives one class described in (4).
**Case 2b. ** If gp−1=1 or χp−1=1, then xp=0 and hence yp−([x,y]xp−1)(ady)p−2=ν(1−gp2).
The verification of [y,yp]=0 amounts to the condition λ2=0. Then we can take ν=0 via the linear translation y↦y−a(1−gp) satisfying ap=ν, which gives one class of H described in (1).
∎
Remark 4.15**.**
It is clear that {yixjh,h∈G,i,j∈I0,p−1} is a basis of HGk(g,χ) for k∈I1,3. One can check easily that π:HGk(g,χ)→\mathdsk[G],yixjh→h is a bialgebra map admitting a bialgebra
section ι:\mathdsk[G]→HGk(g,χ) such that π∘ι=id. Then Hk(g,χ)≅R♯\mathdsk[G] for k∈I1,3, where R is one of connected Hopf algebras of dimension p2 classified in [39, Lemma 7.3].
Remark 4.16**.**
(i)
As Hopf algebras, HG1(1,ϵ)≅\mathdsk[G(H)]⊗\mathdsk[x,y]/(xp,yp), HG2(1,ϵ)≅\mathdsk[G(H)]⊗\mathdsk[x,y]/(xp,yp−x), HG3(1,ϵ)≅\mathdsk[G(H)]⊗\mathdsk[x,y]/(xp−x,yp−y).
(ii)
The Hopf subalgebra generated by x,y appeared in **[39]** as examples of connected Hopf algebras of dimension p2. Among them, \mathdsk[x,y]/(xp,yp) and \mathdsk[x,y]/(xp−x,yp−y) are dual Hopf algebras of \mathdsk[T]/(Tp2) and \mathdsk[X]/(Xp2−1), respectively, where Δ(T)=T⊗1+1⊗T and Δ(X)=X⊗X (see **[39, Corollary 7.5]**). In particular, up to isomorphism, they are regarded as Hopf subalgebras of the algebra of distributions on Ga and Gm, respectively (see **[18, 7.8 ]**).
Proposition 4.17**.**
The Hopf algebras HG1(g,χ), HG2(g,χ), HG3(g,χ) and HG4(g,χ) are pairwise non-isomorphic.
Proof.
We first show that HG1(g,χ)≅HG2(g′,χ′). Suppose that there is a Hopf algebra isomorphism ϕ:HG1(g,χ)→HG2(g′,χ′), then ϕ∣G∈Aut(G) and by Proposition 2.18ϕ(P1,g(HG1(g,χ)))=P1,g′(HG2(g′,χ′)). Therefore, ϕ(g)=g′ and ϕ(x)=αx′+β(1−g′) for some α∈\mathdsk×,β∈\mathdsk.
Applying ϕ to the relations hx−χ(h)x=0 and xp=0 in HG1(g,χ), we have β=0.
Consider grϕ:grHG1(g,χ)→grHG2(g′,χ′) which is induced by ϕ. Then there exist βi∈\mathdsk such that
[TABLE]
Then from Δgrϕ(y)=(grϕ⊗grϕ)Δ(y),
we deduce βi=0 if gi′=1.
Hence grϕ(y)=β0y′. Then ϕ(y)=β0y′+ω, where ω belongs to the subalgebra generated by the first term of the coradical filtration. From Δϕ(y)=(ϕ⊗ϕ)Δ(y), we have
[TABLE]
Thus ω=γ1x′+γ2(1−g′) and ϕ(y)=αpy′+γ1x′+γ2(1−g′). From yp=0 in HG1(g,χ), we deduce α=0, a contradiction. Hence HG1(g,χ)≅HG2(g′,χ′).
Similarly, one can check that HG1(g,χ)≅HG3(g,χ), HG1(g,χ)≅HG4(g,χ), HG2(g,χ)≅HG3(g,χ), HG2(g,χ)≅HG4(g,χ) and HG3(g,χ)≅HG4(g,χ).
∎
Proposition 4.18**.**
HGi(g,χ)≅HGi(g′,χ′)* for i∈I1,4 if and only if there exists f∈Aut(G) such that f(g)=g′ and χ⋅f−1=χ′.*
Proof.
Let ψ:HG1(g,χ)→HG1(g′,χ′) be a Hopf algebra isomorphism. Then ψ∣G∈Aut(G) and ψ(P1,g(HG1(g,χ))=P1,g′(HG1(g′,χ′)). Therefore,
[TABLE]
Since ψ(hxh−1−χ(h)x)=0, it follows that χ′⋅ψ=χ and β(χ−ϵ)=0. Applying ψ to the relation xp=0, we have β=0.
Consider grψ:grHG1(g,χ)→grHG1(g′,χ′) which is induced by ψ. Then there exist βi∈\mathdsk such that
[TABLE]
Then from Δgrψ(y)=(grψ⊗grψ)Δ(y),
we deduce βi=0 if gi′=1.
Hence grψ(y)=β0y′. Then ϕ(y)=β0y′+ω, where ω belongs to the subalgebra generated by the first term of the coradical filtration. From Δψ(y)=(ϕ⊗ψ)Δ(y), we have
[TABLE]
Thus ω=γ1x′+γ2(1−g′) and ϕ(y)=αpy′+γ1x′+γ2(1−g′). From hy−χp(h)yh=0 and yp=0 in HG1(g,χ), we have γ2(1−g′)=0 and (χp−1−ϵ)γ1=0.
Conversely, if there exists f∈Aut(G) such that f(g)=g′ and χ⋅f−1=χ′. Then f can extend to an isomorphism of Hopf algebras from HG1(g,χ) to HG1(g′,χ′) by f(x)=x′ and f(y)=y′.
The proof of the remaining cases follows the same line of the last case.
∎
4.3. Classification results: diagrams are not Nichols algebras
We classify pointed Hopf algebras of dimension p2m whose diagrams are not Nichols algebras and the coradicals have dimension m.
Lemma 4.19**.**
*Let A be the Hopf subalgebra of H generated by group-like elements and skew-primitive elements. Then there exists a YD-triple (G(H),g,χ) and k∈I1,2 such that A≅AG(H)k(g,χ) (see Definition 3.1).
*
Proof.
By assumption and Theorem 4.14, A is a pointed Hopf algebra of dimension pm whose diagram has dimension p with p∤m. Then by Theorem 3.7, there exists a tuple (G(H),g,χ,f) and k∈I1,2 such that A≅AG(H)1(g,χ,f). Since p∤m=∣G(A)∣, by Remark 3.2(3), we have f=0. This completes the proof.
∎
Proposition 4.20**.**
dimH2(1\mathdskgp,A)=1* with a basis {ωg(x)}.*
Proof.
We first claim that ωg(x)=0 in H2(1\mathdskgp,A). Indeed, it is easy to see that ωg(x)∈Z2(1\mathdskg2,A). Suppose that ωg(x)∈B2(1\mathdskgp,A). Then there is an element a∈A such that −d1,gp1(a)=ωg(x), that is, Δ(a)=a⊗1+gp⊗a+ωg(x).
On one hand, a=∑i=0p−1gixi for some gi∈\mathdsk[G] and so Δ(a)∈∑k=0p−1Ak⊗Ap−1−k. On the other hand, ωg(x)∈∑k=1p−1Ak⊗Ap−k. Therefore, ωg(x)∈B2(1\mathdskgp,A) and so dimH2(1\mathdskgp,A)≥1.
By Remark 3.3(iii), A∗≅R∗♯(\mathdsk[G])∗ and as algebras, R∗≅\mathdsk[Zp]. By Proposition 2.9,
[TABLE]
Since (\mathdsk[G])∗ is semisimple, it follows by [30, Theorem 3.3 and Eq. (3.6.1)], H2(R∗♯(\mathdsk[G])∗,\mathdsk)≅H2(R∗,\mathdsk)(\mathdsk[G])∗, where H2(R∗,\mathdsk)(\mathdsk[G])∗ is the space of (\mathdsk[G])∗)-invariant, see [30] for details. Then
[TABLE]
Therefore, dimH2(1\mathdskgp,A)=1 with a basis ωg(x).
∎
Let H be the Hopf algebra such that grH≅H in Theorem 4.5. Proposition 4.20 shows that Δ(y) does not admit non-trivial deformations in the lifting procedure. Namely, there does not exist an element ω=ωg(x) in H2(1\mathdskgp,A) such that ΔH(y)=y⊗1+gp⊗y+ω.
Theorem 4.21**.**
Let char\mathdsk=p. Let H be a pointed Hopf algebra with abelian coradical of dimension p2m such that the diagram has dimension p2. Suppose that H is not generated by group-like elements and skew-primitive elements. Then
H is isomorphic to HG(H)k(g,χ) for some k∈I1,4 in Theorem 4.14. Furthermore, HG(H)i(g,χ)≅HG(H)i(g′,χ′) for i∈I1,4 if and only if there exists f∈Aut(G(H)) such that f(g)=g′ and χ⋅f−1=χ′.
Proof.
By assumption, it is clear that grH≅grH≅H in Theorem 4.5. By Proposition 4.20, there exists some y∈H−A such that Δ(y)=y⊗1+gp⊗y+ωg(x), that is, H≅H as Hopf algebras. Therefore, the assertion follows by Theorem 4.14, Propositions 4.17 and 4.18.
∎
5. Main results
Let char\mathdsk=p>0. In this section, we introduce our main classification results. We give the complete classification of pointed Hopf algebras of dimension p2q. Besides, we classify pointed Hopf algebras of dimension p2m with abelian coradicals, where m is square-free and p∤m.
5.1. Isomorphism classes of pointed Hopf algebras of dimension p2q
We give a complete list of isomorphism classes of pointed Hopf algebras over \mathdsk of dimension p2q.
Lemma 5.1**.**
Let H be a pointed Hopf algebra with char\mathdsk=p of dimension p2q and R the diagram of H. Then dimH0=pq or q.
Proof.
Let R be the diagram of H and V:=R(1)≅P(R). By Nichols-Zoeller Theorem [23], dimH0∣dimH and dimH=dimRdimH0. Thus we have the following possibilities:
(1)
dimH0=p2. Then ∣G(H)∣=p2 and dimR=q, which implies that dimV=1. Let V:=\mathdsk{x}. Since G(H)={ϵ}, x∈Vϵ and hence c(x⊗x)=x⊗x. Therefore, R contains a braided Hopf algebra \mathdsk[x]/(xp) of dimension p, a contradiction.
2. (2)
dimH0=p. Then G(H)≅Zp and dimR=pq. It is impossible. Indeed, if dimV=1, then dimB(V)=p and hence R is not a Nichols algebra; by Lemma 4.2, p2∣dimR, a contradiction. If dimV≥2, then from the proof of [40, Lemma 3.1], we have p2∣dimR, a contradiction. Indeed, there must be a two-dimensional subobject W⊂V, which is of diagonal type with trivial braiding or of Jordan type, which implies that dimB(W)∣dimB(V).
3. (3)
dimH0=pq. Then ∣G(H)∣=pq and dimR=p. Furthermore, R≅\mathdsk[x]/(xp).
4. (4)
dimH0=q. Then ∣G(H)∣=q and dimR=p2.
∎
Proposition 5.2**.**
Let H be a pointed Hopf algebra over \mathdsk of dimension p2q whose diagram R has dimension p. Then H is isomorphic to one of the following Hopf algebras:
**(1): **
\mathdsk[Zpq]⊗\mathdsk[x]/(xp), with x∈P(H);
**(2): **
\mathdsk[Zpq]⊗\mathdsk[x]/(xp−x), with x∈P(H);
**(3): **
\mathdsk⟨g,x⟩/(gpq−1,gx−ξxg,xp)*, ξ a primitive *qth root of unity, with g∈G(H), x∈P(H);
**(4): **
\mathdsk⟨g,x⟩/(gpq−1,gx−ξxg,xp−x), q∣p−1, with g∈G(H), x∈P(H);
**(5): **
\mathdsk⟨g,x⟩/(gpq−1,gx−ξxg,xp), with g∈G(H), x∈P1,gq(H);
**(6): **
\mathdsk[g,x]/(gpq−1,xp), with g∈G(H), x∈P1,g(H);
**(7): **
\mathdsk⟨g,x⟩/(gpq−1,[g,x]−g+g2,xp−x), with g∈G(H), x∈P1,g(H);
**(8): **
\mathdsk[g,x]/(gpq−1,xp), with g∈G(H), x∈P1,gq(H);
**(9): **
\mathdsk⟨g,x⟩/(gpq−1,[g,x]−g+gq+1,xp−qp−1x), with g∈G(H), x∈P1,gq(H);
**(10): **
\mathdsk[g,x]/(gpq−1,xp), with g∈G(H), x∈P1,gp(H);
**(11): **
\mathdsk[g,x]/(gpq−1,xp−x), q∣p−1, with g∈G(H), x∈P1,gp(H);
**(12): **
\mathdsk⟨g,x⟩/(gpq−1,[g,x]−g+gp+1,xp−x), q∣p−1, with g∈G(H), x∈P1,gp(H);
**(13): **
\mathdsk[Zp⋊Zq]⊗\mathdsk[x]/(xp), with x∈P(H);
**(14): **
\mathdsk[Zp⋊Zq]⊗\mathdsk[x]/(xp−x), with x∈P(H);
**(15): **
\mathdsk⟨g,h,x⟩/(gq−1,hp−1,ghg−1−ht,gx−ξxg,hx−xh,xp), with g,h∈G(H), x∈P(H);
**(16): **
\mathdsk⟨g,h,x⟩/(gq−1,hp−1,ghg−1−ht,gx−ξxg,hx−xh,xp−x), with g,h∈G(H), x∈P(H);
**(17): **
\mathdsk[Zq⋊Zp]⊗\mathdsk[x]/(xp), with x∈P(H);
**(18): **
\mathdsk[Zq⋊Zp]⊗\mathdsk[x]/(xp−x), with x∈P(H).
Proof.
Let V:=R(1). By assumption, R≅\mathdsk[x]/(xp) with x∈Vhτ, where g∈Z(G(H)) and τ∈G(H) such that τ(h)=1.
Furthermore, G(H) is isomorphic either to Zpq, Zp⋊Zq, Zq⋊Zp. Therefore, by Theorem 3.7, there exists a tuple (G(H),h,τ,f) such that H≅AG(H)k(h,τ,f) for k∈I1,2 or AG(H)3(h,f). Now we determine isomorphism classes.
Assume that G(H)≅Zpq:=⟨g⟩. Observe that Z(G(H))=Zpq and G(H):=⟨χ⟩, where χ(g)=ξ is a primitive qth root of unity. Hence x∈Vgiχj for some i∈I0,pq−1,j∈I0,q−1 such that χj(gi)=ξij=1, which implies that q∣ij, that is, q∣i or j=0. If j=0, then by changing the generator of Zpq, we can take i∈{0,1,p,q}. If i=0, then we can take j∈I0,1. If i=0,j=0, then q∣i; we can take i=q. Therefore, up to isomorphism, we may restrict to the following realization of R:
[TABLE]
If (i,j)∈{(0,0),(0,1)}, then h=1 and hence H≅AZpqk(1,χj) for k∈I1,2, which are described in (1)–(4).
If (i,j)∈{(q,j),j∈I1,q−1}, then ord(h)=p, τ=ϵ. Since χj(g) is a primitive qth root of unity, it follows by Remark 3.2 (1), f(h)=f(gq)=0. Hence H≅AZpq1(gq,χj,f). Observe that the value of f(k) for any k∈Zpq is determined by f(g). Then by Proposition 3.5, we have AZpq1(gq,χj,f)≅AZpq1(gq,χj) via the linear translation x↦x+α(1−gq) satisfying f(g)=α(χj−ϵ)(g), which gives the one class descried in (5).
If (i,j)=(1,0), then τ=ϵ, ord(h)=pq. From which, we have hp−1=1 and hp=1. Therefore, H≅AZpq1(g,ϵ) or AZpq3(g,f) with f(g)=1, which are described in (6)–(7).
If (i,j)=(q,0), then τ=ϵ, ord(h)=p. By Remark 3.2 (2), we have f=0 when f(gq)=0. Consequently, H≅AZpq1(gq,ϵ) or AZpq3(gq,f) with f(g)=1, which are described in (8)–(9).
If (i,j)=(p,0), then ord(h)=q, and τ=ϵ. From which, we have p∤ord(h) and hp=1. Therefore, H≅AZpqk(gp,ϵ) for k∈I1,2 or AZpq2(gp,ϵ,f) with f(g)=1, which are described in (10)–(12). From the commutativity, the Hopf algebras described in (11) and (12) are non-isomorphic.
Assume that G(H)=Zp⋊Zq. Since the center of G(H) is trivial, x∈V1χi for some i∈I0,q−1. Up to change the character χ, we take i∈I0,1. Therefore, H≅AZp⋊Zqk(1,χi) for k∈I1,2, which are described in (13)–(16).
Assume that G(H)≅Zq⋊Zp. Since the center of G(H) and G(H) is trivial, x∈V1ϵ. Therefore, H≅AZq⋊Zpk(1,ϵ) for k∈I1,2, which are described in (17)–(18).
∎
Proposition 5.3**.**
Let H be a pointed Hopf algebra over \mathdsk of dimension p2q such that the diagram R has dimension p2. Then H is isomorphic to one of the following Hopf algebras:
**(1): **
\mathdsk[Zq]⊗\mathdsk[x,y]/(xp,yp), with x,y∈P(H);
**(2): **
\mathdsk[Zq]⊗\mathdsk[x,y]/(xp−x,yp), with x,y∈P(H);
**(3): **
\mathdsk[Zq]⊗\mathdsk[x,y]/(xp−y,yp), with x,y∈P(H);
**(4): **
\mathdsk[Zq]⊗\mathdsk[x,y]/(xp−x,yp−y), with x,y∈P(H);
**(5): **
\mathdsk[Zq]⊗\mathdsk⟨x,y⟩/(xp−x,yp,[x,y]−y), with g∈G(H), x,y∈P(H);
**(6): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−xg,gy−ξyg,xp,yp,[x,y]),* with g∈G(H), x,y∈P(H);*
**(7): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−xg,gy−ξyg,xp−x,yp,[x,y]),* with g∈G(H), x,y∈P(H);*
**(8): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−xg,gy−ξyg,xp,yp−y,[x,y]),* q∣p−1, with g∈G(H), x,y∈P(H);*
**(9): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−xg,gy−ξyg,xp−x,yp−y,[x,y]),* q∣p−1, with g∈G(H), x,y∈P(H);*
**(10): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−xg,gy−ξyg,xp−x,yp,[x,y]−y),* with g∈G(H), x,y∈P(H);*
**(11): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξyg,xp,yp,[x,y]),* with g∈G(H), x,y∈P(H);*
**(12): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξyg,xp−x,yp,[x,y]),* q∣p−1, with g∈G(H), x,y∈P(H);*
**(13): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξyg,xp−y,yp,[x,y]),* q∣p−1, with g∈G(H), x,y∈P(H);*
**(14): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξyg,xp−x,yp−y,[x,y]),* q∣p−1, with g∈G(H), x,y∈P(H);*
**(15): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξνyg,xp,yp,[x,y]),* ν∈I2,q−1, with g∈G(H), x,y∈P(H);*
**(16): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξνyg,xp−x,yp,[x,y]),* q∣p−1, ν∈I2,q−1, with g∈G(H), x,y∈P(H);*
**(17): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξνyg,xp,yp−y,[x,y]),* q∣p−1, ν∈I2,q−2, with g∈G(H), x,y∈P(H);*
**(18): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξνyg,xp−y,yp,[x,y]),* q∣p−ν, ν∈I2,q−1, with g∈G(H), x,y∈P(H);*
**(19): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξνyg,xp,yp−x,[x,y]),* q∣pν−1, ν∈I2,q−2, with g∈G(H), x,y∈P(H);*
**(20): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξνyg,xp−x,yp−y,[x,y]),* q∣p−1, ν∈I2,q−1, with g∈G(H), x,y∈P(H);*
**(21): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−ξxg,gy−ξ−1yg,xp−y,yp−x,[x,y]),* q∤p−1, q∣p+1, with g∈G(H), x,y∈P(H);*
**(22): **
\mathdsk[g,x,y]/(gq−1,xp,yp), with g∈G(H), x∈P(H), y∈P1,g(H);
**(23): **
\mathdsk[g,x,y]/(gq−1,xp−x,yp), with g∈G(H), x∈P(H), y∈P1,g(H);
**(24): **
\mathdsk[g,x,y]/(gq−1,xp,yp−y),q∣p−1, with g∈G(H), x∈P(H), y∈P1,g(H);
**(25): **
\mathdsk[g,x,y]/(gq−1,xp−x,yp−y), q∣p−1, with g∈G(H), x∈P(H), y∈P1,g(H);
**(26): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−xg,gy−yg,xp−x,yp,[x,y]−y),* with g∈G(H), x∈P(H), y∈P1,g(H);*
**(27): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−xg,gy−yg,xp,yp,[x,y]−1+g),* with g∈G(H), x∈P(H), y∈P1,g(H);*
**(28): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−xg,gy−yg,xp−x,yp,[x,y]−y−1+g),* with g∈G(H), x∈P(H), y∈P1,g(H);*
**(29): **
\mathdsk[g,x,y]/(gq−1,xp,yp), with g∈G(H), x,y∈P1,g(H);
**(30): **
\mathdsk[g,x,y]/(gq−1,xp−x,yp), q∣p−1, with g∈G(H), x,y∈P1,g(H);
**(31): **
\mathdsk[g,x,y]/(gq−1,xp−y,yp), q∣p−1, with g∈G(H), x,y∈P1,g(H);
**(32): **
\mathdsk[g,x,y]/(gq−1,xp−x,yp−y), q∣p−1, with g∈G(H), x,y∈P1,g(H);
**(33): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−xg,gy−yg,xp,yp,[x,y]−1+g2),q=2,
with g∈G(H), x,y∈P1,g(H).
**(34): **
\mathdsk[g,x,y]/(gq−1,xp,yp), with g∈G(H), x∈P1,g(H), y∈P1,gν(H),ν∈I2,q−1;
**(35): **
\mathdsk[g,x,y]/(gq−1,xp−x,yp), q∣p−1, with g∈G(H), x∈P1,g(H), y∈P1,gν(H),ν∈I2,q−1;
**(36): **
\mathdsk[g,x,y]/(gq−1,xp,yp−y), q∣p−1, with g∈G(H), x∈P1,g(H), y∈P1,gν(H),ν∈I2,q−2;
**(37): **
\mathdsk[g,x,y]/(gq−1,xp−y,yp), q∣p−ν, with g∈G(H), x∈P1,g(H), y∈P1,gν(H),ν∈I2,q−1;
**(38): **
\mathdsk[g,x,y]/(gq−1,xp,yp−x), q∣pν−1, with g∈G(H), x∈P1,g(H), y∈P1,gν(H),ν∈I2,q−2;
**(39): **
\mathdsk[g,x,y]/(gq−1,xp−x,yp−y), q∣p−1, with g∈G(H), x∈P1,g(H), y∈P1,gν(H),ν∈I2,q−1;
**(40): **
\mathdsk⟨g,x,y⟩/(gq−1,gx−xg,gy−yg,xp,yp,[x,y]−1+gν+1), with g∈G(H), x∈P1,g(H), y∈P1,gν(H),ν∈I2,q−2;
**(41): **
\mathdsk[g,x,y]/(gq−1,xp−y,yp−x), q∤p−1, q∣p+1, with g∈G(H), x∈P1,g(H), y∈P1,g−1(H).
Proof.
By assumption, G(H)≅Zq with generator g. Let G(H)≅⟨χ⟩, such that χ(g)=ξ is a primitive qth root of unity. Then by Lemma 5.8, R≅B(V,D) for some QPYD-datum D:=D(Zq,χi,χl,gj,gk) with i,j,k,l∈I0,q−1. Since χi(gj)=1=χl(gk)=χi(gk)χl(gj), it follows that
q∣ij, q∣kl and q∣kj+li. Therefore, ij=0, kl=0 and kj+li=0. Observe that Aut(Zq)≅Zq−1. Let Ω:={(i,l,j,k)∣ij=0,kl=0,kj+li=0,i,j,j,l∈I0,q−1}. Then consider the action of Aut(Zq)×S2 on Ω defined by Proposition 3.18,
we restrict to consider the cases:
(1)
V=V1ϵ.
2. (2)
V=V1ϵ⊕V1χ.
3. (3)
V=V1χ⊕V1χν,ν∈I1,q−1.
4. (4)
V=V1ϵ⊕Vgϵ.
5. (5)
V=Vgϵ⊕Vgνϵ,ν∈I1,q−1.
**Case (1) ** By Proposition 3.24, H≅\mathdsHk(Zq,ϵ,ϵ,1,1) for k∈I1,5, which are the non-isomorphic classes described in (1)–(5).
**Case (2) ** By Proposition 3.24, H≅\mathdsHk(Zq,χ,ϵ,1,1) for k∈{1,2,4} or H≅\mathdsHk(Zq,ϵ,χ,1,1) for k∈{1,2,4,5}. It is clear that \mathdsHk(Zq,ϵ,χ,1,1)≅\mathdsHk(Zq,χ,ϵ,1,1) for k∈{1,4} by exchanging x with y. Hence we obtain five classes, which are described in (6)-(10).
We claim that the Hopf algebras described in (6)-(10) are pairwise non-isomorphic. Indeed, by Proposition 3.19, it remains to show that the Hopf algebras described in (7)-(8) are non-isomorphic. Denote by H7 and H8 the Hopf algebras described in (7)–(8) respectively. If there is an isomorphism of Hopf algebras ϕ:H7→H8, then by Proposition 2.18ϕ(P(H7))=P(H8) and hence we have
[TABLE]
From gx=xg, gy=ξyg in H7, we deduce that α2=0=β1. From xp=x in H7, we have that α1=0, a contradiction. Hence H7≅H8.
Case (3). Suppose that ν=1. Then by Proposition 3.24, H≅\mathdsHk(Zq,χ,χ,1,1) for k∈I1,4, which are described in (11)–(14).
Suppose that ν=1. Then by Proposition 3.24, H≅\mathdsHk(Zq,χ,χν,1,1) or \mathdsHk(Zq,χν,χ,1,1) for k∈{1,2,3,4,8}. It is clear that \mathdsHk(Zq,χ,χν,1,1)≅\mathdsHk(Zq,χν,χ,1,1) for k∈{1,4,8} by exchanging x with y. Furthermore, if \mathdsH≅\mathdsH8(Zq,χν,χ,1,1), then from the conditions: χpν=χ, χp=χν and χν=χ, we see that q∤p−1, q∣p+1 and ν=q−1. Hence we obtain seven classes, which are described in (15)-(21).
Similar to Case (2), the Hopf algebras described in (15)-(21) are pairwise non-isomorphic, except for the following two cases:
•
the Hopf algebras described in (16) and (17) are isomorphic if and only if ν=q−1. Indeed, if there is a Hopf algebra isomorphism ϕ then by Proposition 2.18, there are α1,α2,β1,β2 such that
[TABLE]
Applying ϕ to the relations xp−x=0,yp=0,[x,y]=0, it follows that α1=β2=0 and α2p−α2=0. Then applying ϕ to the rest of the defining relations, we have ξν2−1=1, that is, ν=q−1. If ν=q−1, then by swapping x and y, the Hopf algebras described in (16) and (17) are isomorphic.
•
if q∣p−ν and q∣pν−1, the Hopf algebras described in (18) and (19) are isomorphic if and only if ν=q−1.
Case (4). By Proposition 3.25, H≅\mathdsHk(Zq,ϵ,ϵ,g,1) for k∈I1,7−{3,5,7} or H≅\mathdsHk(Zq,ϵ,ϵ,1,g) for k∈I1,7−{3}. It is clear that \mathdsHk(Zq,ϵ,χ,g,1)≅\mathdsHk(Zq,χ,ϵ,1,g) for k∈{1,4,6} by exchanging x with y. Hence we obtain seven classes, which are described in (22)–(28).
It is clear that Hopf algebras described in (23)–(24) are pairwise non-isomorphic. Then by Proposition 3.19, the Hopf algebras described in (22)–(28) are pairwise non-isomorphic.
Case (5).
Suppose that ν=1. Then by Proposition 3.26, H≅\mathdsHk(Zq,ϵ,ϵ,g,g) for k∈I1,6−{5}, which are described in (29)-(33).
Suppose that ν=1. Then by Proposition 3.27, H≅\mathdsHk(Zq,ϵ,ϵ,g,gν) or H≅\mathdsHk(Zq,ϵ,ϵ,gν,g) for k∈I1,8−{5,7}. It is clear that \mathdsHk(Zq,ϵ,ϵ,g,gν)≅\mathdsHk(Zq,ϵ,ϵ,gν,g) for k∈{1,4,6,8} by exchanging x with y. Furthermore, if \mathdsH≅\mathdsH8(Zq,ϵ,ϵ,g,gν), then from the conditions: gpν=g, gp=gν and gν=g, we see that q∤p−1, ν=q−1 and q∣p+1. Hence we obtain the classes described in (34)–(41).
Following the same lines of the last case, one can show that the Hopf algebras described in (35) and (36) are isomorphic if ν=q−1; if q∣p−ν and q∣pν−1, then the Hopf algebras described in (37) and (38) are isomorphic if and only if ν=q−1; otherwise the Hopf algebras described in (34)–(41) are pairwise non-isomorphic.
∎
Remark 5.4**.**
In Proposition 5.3, the Hopf algebras described in (26)–(27), (33) and (40) are noncommutative and noncocommutative, which constitute new examples of non-commutative non-cocommutative pointed Hopf algebras. By Remark 3.16, the rest are Radford biproducts of restricted universal enveloping algebras of dimension p2 by \mathdsk[Zq].
Proposition 5.5**.**
Let H be a pointed Hopf algebra over \mathdsk of dimension p2q whose diagram R is not a Nichols algebra. Then H is isomorphic to one of the following Hopf algebras
(1)
\mathdsk[Zq]⊗\mathdsk[x,y]/(xp,yp), with g=1;
(2)
\mathdsk[Zq]⊗\mathdsk[x,y]/(xp,yp−x), with g=1;
(3)
\mathdsk[Zq]⊗\mathdsk[x,y]/(xp−x,yp−y), with g=1;
(4)
\mathdsk⟨h,x,y⟩/(hq−1,hx−ξxh,hy−ξpyh,[x,y],xp,yp), with g=1;
(5)
\mathdsk⟨h,x,y⟩/(hq−1,hx−ξxh,hy−ξpyh,[x,y],xp,yp−x), q∣p−1, with g=1;
(6)
\mathdsk⟨h,x,y⟩/(hq−1,hx−ξxh,hy−ξpyh,[x,y],xp−x,yp−y), q∣p−1, with g=1;
(7)
\mathdsk[h,x,y]/(hq−1,xp,yp), with g=h;
(8)
\mathdsk[h,x,y]/(hq−1,xp,yp−x), q∣p−1, with g=h;
(9)
\mathdsk[h,x,y]/(hq−1,xp−x,yp−y), q∣p−1, with g=h;
(10)
\mathdsk⟨h,x,y⟩/(hq−1,[h,x],[h,y],[x,y]−1+hp+1,xp,yp+(1−hp+1)p−1x−x), q∣p−1, q∤p+1, with g=h;
where ξ is a primitive qth root of unity, h∈G(H), x∈P1,g(H) and Δ(y)=y⊗1+gp⊗y+ωg(x).
Proof.
By assumption and Lemma 5.1, G(H)≅Zq with generator h. Then dimB(R(1))=p and hence dimR(1)=1. Let V:=R(1)=\mathdsk{x}.
Then \mathdsk{x}∈G(H)G(H)YD by
•
x∈Vhjχi for i,j∈I0,q−1, where χ∈G satisfying χ(h)=ξ.
Hence ξij=1, that is, q∣ij, which implies that i=0 or j=0. Up to change the character χ and the element h
we may restrict to consider the cases: (i,j)=(0,0),(1,0),(0,1).
Then by Theorem 4.21, H is isomorphic to HZqk(1,ϵ), HZqk(1,χ) for k∈I1,3 or HZqk(g,ϵ) for k∈I1,4.
∎
Remark 5.6**.**
By Propositions 4.17, 4.18 and 5.5, there are 10 isomorphism classes of pointed Hopf algebras of dimension p2q whose diagrams are not Nichols algebras. By Remark 4.15, the classes described in (1)-(9) are Radford biproducts of connected Hopf algebras of dimension p2 [39] by \mathdsk[Zq]; the class described in (10) is the unique non-commutative non-cocommutative pointed Hopf algebra of dimension p2q whose diagram is not a Nichols algebra, which constitute new examples of non-commutative non-cocommutative pointed Hopf algebras.
Theorem 5.7**.**
Let H be a pointed Hopf algebra over \mathdsk of dimension p2q. If H is generated by group-like elements and skew-primitive elements, then H is one of the algebras listed in Propositions 5.2 and 5.3; otherwise H is one of the algebras listed in Proposition 5.5.
Proof.
By Lemma 5.1, the diagram of H has dimension p or p2. Therefore, it follows by Propositions 5.2, 5.3 and 5.5.
∎
5.2. On pointed Hopf algebras of dimension p2m
Let m be square-free and p∤m. Now we first give a classification of pointed Hopf algebras of dimension p2m with abelian coradicals whose diagrams are Nichols algebras.
Lemma 5.8**.**
Suppose that char\mathdsk=p, m is square-free and p∤m. Let H be a pointed Hopf algebra over \mathdsk of dimension p2m whose diagram is a Nichols algebra. Then dimR=p or p2. Furthermore,
(1)
If dimR=p, then R≅\mathdsk[x]/(xp) with x∈R(1)gχ satisfying χ(g)=1 for some g∈Z(G(H)) and χ∈G(H);
(2)
If dimR=p2, then R≅B(V,D) for some QPYD-datum D:=D(G(H),χ1,χ2,g1,g2).
Proof.
We first claim that p∣dimR. Let dimH0=pkn with p∤n for k∈I0,2. Then dimR=p2−km/n. By assumption, there is an element x∈R(1)gχ for some YD-pair (g,χ) such that c(x⊗x)=χ(g)x⊗x. Then B(\mathdsk{x}) is a Hopf subalgebra of R in G(H)G(H)YD and hence dimB(\mathdsk{x})∣dimR. Suppose that χ(g)=1. Then χ(g)=ξi for i∈I1,n−1, where ξ is a primitive nth root of unity and hence ord(ξi)∣n, which implies that ord(ξi)∤m/n. On the other hand, dimB(\mathdsk{x})=ord(ξi)∣m/n, a contradiction. Consequently, χ(g)=1 and hence p=dimB(\mathdsk{x})∣dimR.
Since p∣dimR, it follows that the order of G(H) is square-free and G(H)≅Zpkn for k∈I0,1.
We claim that p2∣dimR when dimR=p. Assume that dimR=p. If \mathdsk{x} is a subobject of some non-simple indecomposable object V, then by [40, Example 2.2] p2∣dimR, which implies that p∤dimH0 and so H0H0YD are semisimple, a contradiction. Then there is an element y∈R(1)−\mathdsk{x} such that y∈R(1)g′χ′. Furthermore, χ′(g′)=1. Let W:=\mathdsk{x,y}. Then
B(W) is of diagonal type whose braiding (qi,j)i,j∈I1,2 is given by qi,i=1. Then by [37, Theorem 5.1], B(W) is finite-dimensional if and only if q1,2q2,1=1. Hence B(W)=\mathdsk[x,y]/(xp,yp) and then p2∣dimR.
If dimR=p, then p2∣dimR and hence G(H)≅Zn. Similarly, if dimR∈{p,p2}, then p3∣dimR, a contradiction. Consequently, dimR=p or p2.
∎
Lemma 5.9**.**
Suppose that char\mathdsk=p, m is square-free and p∤m. Let H be a pointed Hopf algebra over \mathdsk of dimension p2m whose diagram is not a Nichols algebra. Then dimR=p2.
Proof.
By Lemma 5.8, B(R(1))≅\mathdsk[x]/(xp), where R(1):=\mathdsk{x}. Then by Corollary 4.3, p2∣dimR.
If dimR=p2, then by [41, Lemma 3.2], there are a braided Hopf subalgebra of dimension p3, which is isomorphic to \mathdsk[x,y,x]/(xp,yp,zp) with
[TABLE]
which implies that p3∣dimR, a contradiction. Consequently, we have dimR=p2.
∎
Theorem 5.10**.**
Suppose that char\mathdsk=p, m is square-free and p∤m. Let H be a pointed Hopf algebra over \mathdsk of dimension p2m with abelian coradical. Then H is isomorphic to one of the following Hopf algebras:
(i)
AG(H)k(g,χ,f)* for k∈I1,2 and AG(H)3(g,f);*
(ii)
\mathdsHk(D)* for k∈I1,8;*
(iii)
HG(H)k(g,χ)* for k∈I1,4.*
Furthermore,
•
AG1(g,χ,f)≅AG1(g′,χ′,f′)* if and only if there exists F∈Aut(G) such that F(g)=g′, χ⋅F−1=χ′ and αf′F−f+β(χ−ϵ)=0 for some α∈\mathdsk×,β∈\mathdsk satisfying β(1−gp)=0.*
•
AG2(g,χ,f)≅AG2(g′,χ′,f′)* if and only if there exists F∈Aut(G) such that F(g)=g′, χ⋅F−1=χ′ and αf′F−f+β(χ−ϵ)=0 for some α∈\mathdsk×,β∈\mathdsk satisfying αp=α and (βp−β)(1−g)=0.*
•
AG(H)3(g,η)≅AG(H)3(g′,η′)* if and only if there exists F∈Aut(G(H)) such that F(g)=g′ and f⋅F−1=f′;*
•
\mathdsHk(D)≅\mathdsHk(D′)* for k∈I1,8 if and only if there are F∈Aut(G(H)) and σ∈S2 such that F(gσ(i))=gi′ and χσ(i)⋅F−1=χi′;*
•
HG(H)i(g,χ)≅HG(H)i(g′,χ′)* for i∈I1,4 if and only if there exists F∈Aut(G(H)) such that F(g)=g′ and χ⋅F−1=χ′.*
Proof.
If the diagram is a Nichols algebra, then it follows by Lemma 5.8, Theorems 3.7, 3.28; otherwise it follows by Lemma 5.9 and Theorem 4.21.
∎
Acknowledgements
The author is grateful to Prof. V. C. Nguyen for her suggestions and comments on earlier draft of this article and to Profs. Quanshui Wu and Xingting Wang so much for the help and encouragement during his visiting at the Shanghai Center for Mathematical Sciences. The author would like to thank the referee for many helpful comments and suggestions that improved the exposition.
Bibliography41
The reference list from the paper itself. Each links out to its DOI / PubMed record.
1[1] N. Andruskiewitsch and I. E. Angiono, On finite dimensional Nichols algebras of diagonal type, Bulletin of Mathematical Sciences 7 (3) (2017), 353–573.
2[2] N. Andruskiewitsch, I. Angiono and I. Heckenberger, Examples of finite-dimensional pointed Hopf algebras in positive characteristic . Preprint: ar Xiv:1905.03074.
3[3] N. Andruskiewitsch, D. Bagio, S. D. Flora and D. Flres, Examples of finite-dimensional pointed Hopf algebras in characteristic 2 , Glasgow Math. J. 64 (2022), 65–78.
4[4] N. Andruskiewitsch and H. Pena Pollastri, On the restricted Jordan plane in odd characteristic , J. Algebra Appl. 20 (1) (2021), 2140012
5[5] N. Andruskiewitsch and M. Graña, Braided Hopf algebras over non abelian finite groups , Bol. Acad. Nac. Cienc. Cordoba 63 (1999), 46–78.
6[6] N. Andruskiewitsch and S. Natale, Counting arguments for Hopf algebras of low dimension , Tsukuba Math J. 25 (1) (2001), 187–201.
7[7] N. Andruskiewitsch and H. J. Schneider, Lifting of quantum linear spaces and pointed Hopf algebras of order p 3 superscript 𝑝 3 p^{3} , J. Algebra 209 (1998), 658–691.
8[8] N. Andruskiewitsch and H. J. Schneider, Pointed Hopf algebras , New directions in Hopf algebras, 1–68, Math. Sci. Res. Inst. Publ., 43, Cambridge Univ. Press, Cambridge, 2002.