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Quantum projective planes as certain graded twisted tensor products

Abstract.

Let 𝕂\mathbb{K} be an algebraically closed field. Building upon previous work, we classify, up to isomorphism of graded algebras, quadratic graded twisted tensor products of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z]. When such an algebra is Artin-Schelter regular, we identify its point scheme and type, in the sense of [5]. We also describe which three-dimensional Sklyanin algebras contain a subalgebra isomorphic to a quantum β„™1{\mathbb{P}}^{1}, and we show that every algebra in this family is a graded twisted tensor product of π•‚βˆ’1​[x,y]\mathbb{K}_{-1}[x,y] and 𝕂​[z]\mathbb{K}[z].

Key words and phrases:
Artin-Schelter regular algebras, noncommutative algebraic geometry, twisted tensor products, Sklyanin algebras
2010 Mathematics Subject Classification:
16S37, 16W50

Andrew Conner


Department of Mathematics and Computer Science

Saint Mary’s College of California

Moraga, CA 94575


Peter Goetz


Department of Mathematics

Humboldt State University

Arcata, California 95521


1. Introduction

In [11], Čap, Schichl, and Vanžura were led to define the notion of a twisted tensor product of algebras over a field as an answer to the following question from noncommutative differential geometry:

Given two algebras that represent noncommutative spaces, what is an appropriate representative of a noncommutative product of those spaces?

This paper is motivated by a related question in noncommutative projective geometry. If AA is a noetherian graded 𝕂\mathbb{K}-algebra, finitely generated in degree 1, the noncommutative projective scheme (Proj ​A,π’ͺ)(\hbox{Proj }A,\mathcal{O}) is, by definition, the quotient category Proj ​A=GrMod​(A)/Tors​(A)\hbox{Proj }A={\rm GrMod}(A)/{\rm Tors}(A) of graded right modules, modulo torsion modules, with π’ͺ\mathcal{O} the image of AAA_{A} in Proj ​A\hbox{Proj }A. In light of Serre’s theorem in commutative algebraic geometry, the category Proj ​A\hbox{Proj }A can be considered as the category of quasi-coherent sheaves on an imagined noncommutative scheme. In this context, we say Proj ​A\hbox{Proj }A (or just AA) is a quantum projective space if AA is a quadratic Artin-Schelter regular algebra; more precisely, if AA has global dimension n+1n+1, then we say that Proj ​A\hbox{Proj }A (or AA) is a quantum β„™n{\mathbb{P}}^{n}. We raise the following natural question:

Which quantum projective spaces are isomorphic to graded twisted tensor products of other quantum projective spaces?

It is not hard to show that every quantum β„™1{\mathbb{P}}^{1} is a graded twisted tensor product of 𝕂​[x]\mathbb{K}[x] and 𝕂​[y]\mathbb{K}[y]. One of our main results in this paper is the determination of all of the quantum β„™2{\mathbb{P}}^{2}’s that are isomorphic as graded algebras to graded twisted tensor products of the β€œclassical” β„™1{\mathbb{P}}^{1}, 𝕂​[x,y]\mathbb{K}[x,y], with 𝕂​[z]\mathbb{K}[z]. This builds upon results in [4], where all graded twisted tensor products of 𝕂​[x,y]\mathbb{K}[x,y] with 𝕂​[z]\mathbb{K}[z] were classified up to a notion of equivalence stronger than that of graded algebra isomorphism.

An intriguing aspect of Artin-Schelter regular algebras is the extent to which their algebraic properties are encoded geometrically. To every quantum β„™2{\mathbb{P}}^{2}, one can associate a subscheme EβŠ‚β„™2E\subset{\mathbb{P}}^{2} and an automorphism Οƒ:Eβ†’E\sigma:E\to E which determine the algebra up to isomorphism. In characterizing which quantum β„™2{\mathbb{P}}^{2}’s are graded twisted tensor products of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z], we also determine this geometric data.

The first classification results on quantum β„™2{\mathbb{P}}^{2} are due to Artin and Schelter in [2] and Artin-Tate-van den Bergh in [1]. These results provide a β€œgeneric” classification up to algebra isomorphism which has subsequently been refined through the work of many authors; we refer the reader to [5] for details. In characteristic 0, a classification of three-dimensional quadratic Artin-Schelter regular algebras up to isomorphism and Morita equivalence has recently been completed [5, 6] using the theory of geometric algebras developed in [7] and [8]. Though we do not assume char​𝕂=0{\rm char}\ \mathbb{K}=0 in this paper, we adopt the naming conventions introduced by these authors, in which the types of algebras are differentiated according to the geometric data (E,Οƒ)(E,\sigma), see Section 2. Detailed mappings from the classification of [4] to types from [5] are provided in Sections 3, 4, and 5.

Theorem 1.1 (Theorem 3.1, Theorem 4.1, Theorem 5.2).

Assume char​𝕂≠2{\rm char}\ \mathbb{K}\neq 2. Let TT be an Artin-Schelter regular graded twisted tensor product of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z].

  1. (1)

    If TT is of type E​CEC, then the point scheme EE is an elliptic curve, and the automorphism Οƒ\sigma is multiplication by βˆ’1-1 in the group law on EE. (TT is of type BB.)

  2. (2)

    If TT is not of type E​CEC, then TT belongs to one of the following types:

    P1,P2,S1,S1β€²,S2,S2β€²,T1,Tβ€²,W​L1,W​L2,W​L3,T​L1,T​L2,T​L4,N​C2.P_{1},P_{2},S_{1},S_{1}^{\prime},S_{2},S_{2}^{\prime},T_{1},T^{\prime},WL_{1},WL_{2},WL_{3},TL_{1},TL_{2},TL_{4},NC_{2}.

Moreover, each type listed above is the type of an Artin-Schelter regular graded twisted tensor product of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z].

Comparing Theorem 1.1 to the results of [5, 6] shows that, in characteristic 0, not all quantum β„™2{\mathbb{P}}^{2}’s can be expressed as graded twisted tensor products of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z], even up to graded Morita equivalence. We summarize this comparison as follows.

Theorem 1.2.

Assume char​𝕂=0{\rm char}\ \mathbb{K}=0. Let AA be a three-dimensional quadratic Artin-Schelter regular algebra.

  1. (1)

    (Remarks 3.7, 4.2, 5.3) If AA belongs to one of the following types:

    E​C​ (subtypeΒ B), ​S2β€²,T1,W​L2,W​L3,T​L4,N​C2,EC\text{ (subtype $B$), }S^{\prime}_{2},T_{1},WL_{2},WL_{3},TL_{4},NC_{2},

    then AA is isomorphic to a graded twisted tensor product of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z].

  2. (2)

    (Remark 5.26) If AA belongs to one of the following types:

    P,S,Sβ€²,T,Tβ€²,W​L,T​L,P,S,S^{\prime},T,T^{\prime},WL,TL,

    then AA is graded Morita equivalent to a graded twisted tensor product of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z].

  3. (3)

    If AA is of type C​CCC, then AA is not graded Morita equivalent to a graded twisted tensor product of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z].

Not every Morita equivalence class of quantum β„™2{\mathbb{P}}^{2}’s contains a graded twisted tensor product of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z]. By [5, Theorem 3.2], the only ones that do not are of Type NC, CC or EC. However, the unique isomorphism class of Type CC is a graded Ore extension of the Jordan plane, and every algebra of Type N​C1NC_{1} is a graded Ore extension of a skew polynomial algebra 𝕂a​[x,y]\mathbb{K}_{a}[x,y]. Since graded Ore extensions are twisted tensor products, Theorem 1.2 and the preceding observations imply that every quantum β„™2{\mathbb{P}}^{2} that is not of type EC is graded Morita equivalent to a twisted tensor product (in fact, a graded Ore extension) of some quantum β„™1{\mathbb{P}}^{1} with 𝕂​[z]\mathbb{K}[z].

In the last section of the paper, we prove there are quantum β„™2{\mathbb{P}}^{2}’s that are not (Morita equivalent to) graded twisted tensor products of any quantum β„™1{\mathbb{P}}^{1} with 𝕂​[z]\mathbb{K}[z]. Our results in this direction concern the three-dimensional Sklyanin algebras S​(a,b,c)S(a,b,c), see Section 6 for the relevant definitions. We argue first, using noncommutative algebraic geometry, that π•‚βˆ’1​[x,y]\mathbb{K}_{-1}[x,y] is the only quantum β„™1{\mathbb{P}}^{1} that can arise as a subalgebra of S​(a,b,c)S(a,b,c), when the point scheme of S​(a,b,c)S(a,b,c) is an elliptic curve, and this can only occur when a=ba=b.

Theorem 1.3 (Theorem 6.2, Proposition 6.5).

Assume char​𝕂≠2,3{\rm char}\ \mathbb{K}\neq 2,3. Let S​(a,b,c)S(a,b,c) be a three-dimensional Sklyanin algebra of type EC.Β Then S​(a,b,c)S(a,b,c) contains a subalgebra isomorphic to a quantum β„™1{\mathbb{P}}^{1} if and only if a=ba=b. The only quantum β„™1{\mathbb{P}}^{1} contained in S​(a,a,c)S(a,a,c) is π•‚βˆ’1​[x,y]\mathbb{K}_{-1}[x,y].

Thus, when char​𝕂≠2,3{\rm char}\ \mathbb{K}\neq 2,3, a Sklyanin algebra of type EC is graded Morita equivalent to a graded twisted tensor product of a quantum β„™1{\mathbb{P}}^{1} with 𝕂​[z]\mathbb{K}[z] only if it is graded Morita equivalent to S​(1,1,c)S(1,1,c) where cβ‰ 0c\neq 0 and (3​c)3β‰ (2+c3)3(3c)^{3}\neq(2+c^{3})^{3}.

Finally, we show that, in characteristic 0, every three-dimensional Sklyanin algebra of type EC that contains a subalgebra isomorphic to π•‚βˆ’1​[x,y]\mathbb{K}_{-1}[x,y] is a graded twisted tensor product of π•‚βˆ’1​[x,y]\mathbb{K}_{-1}[x,y] and 𝕂​[z]\mathbb{K}[z].

Theorem 1.4 (Theorem 6.13).

Assume char​𝕂=0{\rm char}\ \mathbb{K}=0. A three-dimensional Sklyanin algebra S​(1,1,c)S(1,1,c) of type EC is isomorphic as a graded algebra to a twisted tensor product P​(a)P(a) for some aβˆˆπ•‚βˆ’{0,1}a\in\mathbb{K}-\{0,1\}.

The outline of the paper is as follows. Definitions and notation related to twisted tensor products and types of Artin-Schelter regular algebras are given in Section 2. In particular, the three main families of graded twisted tensor products from [4] are described. In Sections 3, 4, and 5, algebras from these three families are classified up to isomorphism, and the associated geometric data is computed. Finally, results related to the three-dimensional Sklyanin algebras of type EC are the subject of Section 6.

2. Preliminaries

In this paper we work with algebras over a field 𝕂\mathbb{K}. We assume throughout that 𝕂\mathbb{K} is algebraically closed and char​𝕂≠2{\rm char}\,\mathbb{K}\neq 2. The tensor product of 𝕂\mathbb{K}-vector spaces VV and WW is denoted VβŠ—WV\otimes W, and when VV and WW are β„•{\mathbb{N}}-graded, the space VβŠ—WV\otimes W is graded by the formula

(VβŠ—W)m=⨁k+β„“=mVkβŠ—Wβ„“.(V\otimes W)_{m}=\bigoplus_{k+\ell=m}V_{k}\otimes W_{\ell}.

We write Vβˆ—V^{*} for the linear dual of the 𝕂\mathbb{K}-vector space VV.

By a graded 𝕂\mathbb{K}-algebra, we mean a connected, β„•{\mathbb{N}}-graded, locally finite-dimensional 𝕂\mathbb{K}-algebra, generated in degree 1. We require morphisms of graded algebras and vector spaces to preserve degree. We call a graded 𝕂\mathbb{K}-algebra AA quadratic if there exists a finite dimensional 𝕂\mathbb{K}-vector space VV and a subspace RβŠ†VβŠ—VR\subseteq V\otimes V such that Aβ‰…T​(V)/⟨R⟩A\cong T(V)/\langle R\rangle as graded algebras, where T​(V)T(V) is the tensor algebra.

2.1. Graded twisted tensor products

Let AA and BB be graded 𝕂\mathbb{K}-algebras. A graded twisted tensor product of AA and BB is a triple (C,iA,iB)(C,i_{A},i_{B}) where CC is a graded 𝕂\mathbb{K}-algebra and iA:Aβ†’Ci_{A}:A\to C and iB:Bβ†’Ci_{B}:B\to C are graded algebra inclusions such that the 𝕂\mathbb{K}-linear map AβŠ—Bβ†’CA\otimes B\to C given by aβŠ—b↦iA​(a)​iB​(b)a\otimes b\mapsto i_{A}(a)i_{B}(b) is an isomorphism. In this paper we are primarily concerned with the setting where A=𝕂​[x,y]A=\mathbb{K}[x,y], B=𝕂​[z]B=\mathbb{K}[z], and CC is a quadratic algebra.

A graded twisted tensor product imparts the structure of an associative algebra to AβŠ—BA\otimes B, implicitly determining a product map (AβŠ—B)βŠ—2β†’AβŠ—B(A\otimes B)^{\otimes 2}\to A\otimes B. The product can be described somewhat more directly via the notion of a twisting map. Given any 𝕂\mathbb{K}-linear map Ο„:BβŠ—Aβ†’AβŠ—B\tau:B\otimes A\to A\otimes B, one can define ΞΌΟ„:(AβŠ—B)βŠ—2β†’AβŠ—B\mu_{\tau}:(A\otimes B)^{\otimes 2}\to A\otimes B by ΞΌΟ„=(ΞΌAβŠ—ΞΌB)​(1βŠ—Ο„βŠ—1)\mu_{\tau}=(\mu_{A}\otimes\mu_{B})(1\otimes\tau\otimes 1). However, ΞΌΟ„\mu_{\tau} does not define an associative product, in general.

A (unital) graded twisting map for AA and BB is a graded 𝕂\mathbb{K}-linear map Ο„:BβŠ—Aβ†’AβŠ—B\tau:B\otimes A\to A\otimes B such that τ​(1βŠ—a)=aβŠ—1\tau(1\otimes a)=a\otimes 1, τ​(bβŠ—1)=1βŠ—b\tau(b\otimes 1)=1\otimes b, and

τ​(ΞΌBβŠ—ΞΌA)=(ΞΌAβŠ—ΞΌB)​(1βŠ—Ο„βŠ—1)​(Ο„βŠ—Ο„)​(1βŠ—Ο„βŠ—1)\tau(\mu_{B}\otimes\mu_{A})=(\mu_{A}\otimes\mu_{B})(1\otimes\tau\otimes 1)(\tau\otimes\tau)(1\otimes\tau\otimes 1)

where ΞΌA\mu_{A} and ΞΌB\mu_{B} denote the product maps on AA and BB, respectively. This condition is precisely what is required for ΞΌΟ„\mu_{\tau} to satisfy associativity.

Proposition 2.1.

[3, Proposition 2.3] Let AA and BB be graded algebras and Ο„:BβŠ—Aβ†’AβŠ—B\tau:B\otimes A\to A\otimes B a graded 𝕂\mathbb{K}-linear map. Then Ο„\tau is a graded twisting map if and only if (AβŠ—B,ΞΌΟ„)(A\otimes B,\mu_{\tau}) is an associative graded kk-algebra.

In particular, if Ο„:BβŠ—Aβ†’AβŠ—B\tau:B\otimes A\to A\otimes B is a graded twisting map, the graded algebra AβŠ—Ο„B=(AβŠ—B,ΞΌΟ„)A\otimes_{\tau}B=(A\otimes B,\mu_{\tau}), together with the canonical inclusions of AA and BB, is a graded twisted tensor product of AA and BB. If AβŠ—Ο„Bβ‰…AβŠ—Ο„β€²BA\otimes_{\tau}B\cong A\otimes_{\tau^{\prime}}B as graded 𝕂\mathbb{K}-algebras, it does not necessarily follow that Ο„=Ο„β€²\tau=\tau^{\prime}. In [11], the authors define a notion of isomorphism that uniquely identifies twisted tensor products by their twisting maps. In [4], we classified quadratic twisted tensor products 𝕂​[x,y]βŠ—Ο„π•‚β€‹[z]\mathbb{K}[x,y]\otimes_{\tau}\mathbb{K}[z] up to a notion of equivalence weaker than that of [11], yet stronger than graded algebra isomorphism. The precise definitions of these notions are not needed in this paper.

By [3, Theorem 1.2], a quadratic twisted tensor product 𝕂​[x,y]βŠ—Ο„π•‚β€‹[z]\mathbb{K}[x,y]\otimes_{\tau}\mathbb{K}[z] is uniquely determined by τ​(zβŠ—x)\tau(z\otimes x) and τ​(zβŠ—y)\tau(z\otimes y), and by [3, Proposition 2.5] we have

C=𝕂​[x,y]βŠ—Ο„π•‚β€‹[z]β‰…π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​xβˆ’Ο„β€‹(z​x),z​yβˆ’Ο„β€‹(z​y)⟩.C=\mathbb{K}[x,y]\otimes_{\tau}\mathbb{K}[z]\cong\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zx-\tau(zx),zy-\tau(zy)\rangle.

Here τ​(z​x)\tau(zx) and τ​(z​y)\tau(zy) are the images of τ​(zβŠ—x)\tau(z\otimes x) and τ​(zβŠ—y)\tau(z\otimes y) in π•‚β€‹βŸ¨x,y,z⟩\mathbb{K}\langle x,y,z\rangle under the obvious identification with T​(C1)T(C_{1}). A main result from [4] is the following, which does not require any restrictions on the characteristic of 𝕂\mathbb{K}.

Theorem 2.2.

[4, Theorem 1.4] Let 𝕂\mathbb{K} be an algebraically closed field. A quadratic twisted tensor product of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z] is equivalent to one determined by

τ​(z​x)\displaystyle\tau(zx) =a​x2+b​x​y+c​y2+d​x​z+e​y​z+f​z2\displaystyle=ax^{2}+bxy+cy^{2}+dxz+eyz+fz^{2}
τ​(z​y)\displaystyle\tau(zy) =A​x2+B​x​y+C​y2+D​y​z\displaystyle=Ax^{2}+Bxy+Cy^{2}+Dyz

where e,f,A∈{0,1}e,f,A\in\{0,1\}.

We alert the reader to a small notational shift from [4]: in [4, Theorem 1.4] we wrote EE instead of DD in the τ​(z​y)\tau(zy) equation. In this paper EE always refers to a point scheme, as defined below. When comparing results of this paper with corresponding results in [4] one should replace DD with EE.

We divided the algebras of Theorem 2.2 into three families: Ore type (when f=0f=0), reducible type (when f=1,A=0f=1,A=0) and elliptic type (when f=1,A=1f=1,A=1). Not all values of the other parameters yield twisted tensor products; complete descriptions are provided at the beginning of the section in which a family is discussed.

2.2. Noncommutative projective geometry

We review some basic definitions and results from [1] and [7]. Let A=T​(V)/⟨R⟩A=T(V)/\langle R\rangle be a quadratic algebra. An element f∈Td​(V)f\in T_{d}(V) determines a multilinear form f~:(Vβˆ—)Γ—d→𝕂\tilde{f}:(V^{*})^{\times d}\to\mathbb{K}. Let Ξ“=Γ​(A)βŠ†β„™β€‹(Vβˆ—)×ℙ​(Vβˆ—)\Gamma=\Gamma(A)\subseteq{\mathbb{P}}(V^{*})\times{\mathbb{P}}(V^{*}) denote the scheme of zeros of the multilinearizations of the elements of RR. Let pri:ℙ​(Vβˆ—)×ℙ​(Vβˆ—)→ℙ​(Vβˆ—){\rm pr}_{i}:{\mathbb{P}}(V^{*})\times{\mathbb{P}}(V^{*})\to{\mathbb{P}}(V^{*}) for i=1,2i=1,2 denote the canonical projections. Let EiE_{i} be the scheme-theoretic image of Ξ“\Gamma under pri{\rm pr}_{i}. We denote pri|Ξ“{\rm pr}_{i}|_{\Gamma} by Ο€i:Ξ“β†’Ei\pi_{i}:\Gamma\to E_{i}.

Definition 2.3.

We say that the algebra AA is semi-standard if E1E_{1} and E2E_{2} are equal as subschemes of ℙ​(Vβˆ—){\mathbb{P}}(V^{*}).

If the algebra AA is semi-standard, let E=E1=E2E=E_{1}=E_{2}. Then one may view Γ\Gamma as the graph of a correspondence E→EE\to E via the closed immersion (π1,π2):Γ→E×E(\pi_{1},\pi_{2}):\Gamma\to E\times E.

Definition 2.4.

Let AA be a semi-standard algebra. We say that AA is nondegenerate if Γ\Gamma is the graph of a scheme automorphism σ:E→E\sigma:E\to E. Otherwise we say that AA is degenerate.

If AA is semi-standard and nondegenerate, then we call the scheme EE the point scheme of AA. In [1] it is shown that the point scheme parametrizes the so-called point modules of AA. We refer the reader to [1] for the definition of a point module of a graded algebra.

The pair (E,Οƒ)(E,\sigma) encodes important information about the algebra AA. We use the notion of a geometric algebra developed in [7]. Let i:E→ℙ​(Vβˆ—)i:E\to{\mathbb{P}}(V^{*}) be the natural embedding, and set β„’=iβˆ—β€‹π’ͺℙ​(Vβˆ—){\mathcal{L}}=i^{*}{\mathcal{O}}_{{\mathbb{P}}(V^{*})}. There is a natural map of 𝕂\mathbb{K}-vector spaces:

ΞΌ:H0​(E,β„’)βŠ—H0​(E,β„’)β†’H0​(E,β„’βŠ—π’ͺEΟƒβˆ—β€‹β„’).{\mu}:H^{0}(E,{\mathcal{L}})\otimes H^{0}(E,{\mathcal{L}})\to H^{0}(E,{\mathcal{L}}\otimes_{{\mathcal{O}}_{E}}\sigma^{*}{\mathcal{L}}).
Definition 2.5.

[7, Definition 4.3] Let A=T​(V)/⟨R⟩A=T(V)/\langle R\rangle be a quadratic algebra. We say that AA is geometric if there is a pair (E,Οƒ)(E,\sigma), where EβŠ‚β„™β€‹(Vβˆ—)E\subset{\mathbb{P}}(V^{*}) is a closed subscheme and Οƒ:Eβ†’E\sigma:E\to E is an automorphism such that:

  • (i)

    Ξ“\Gamma is the graph of Οƒ\sigma,

  • (ii)

    R=ker​μR=\hbox{ker}\ {\mu} under the canonical identification H0​(E,β„’)=VH^{0}(E,{\mathcal{L}})=V.

We make frequent use of the following well-known result.

Theorem 2.6.

[7, Remark 4.9] Suppose that AA and Aβ€²A^{\prime} are geometric algebras associated to (E,Οƒ)(E,\sigma) and (Eβ€²,Οƒβ€²)(E^{\prime},\sigma^{\prime}), respectively. Then Aβ‰…Aβ€²A\cong A^{\prime} as graded 𝕂\mathbb{K}-algebras if and only if A1=A1β€²A_{1}=A_{1}^{\prime} and there is a scheme automorphism ψ\psi of ℙ​(A1){\mathbb{P}}(A_{1}) which restricts to an isomorphism ψ:Eβ†’Eβ€²\psi:E\to E^{\prime} such that the following diagram commutes.

E\textstyle{E\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ψ\scriptstyle{\psi}Οƒ\scriptstyle{\sigma}Eβ€²\textstyle{E^{\prime}\ignorespaces\ignorespaces\ignorespaces\ignorespaces}Οƒβ€²\scriptstyle{\sigma^{\prime}}E\textstyle{E\ignorespaces\ignorespaces\ignorespaces\ignorespaces}ψ\scriptstyle{\psi}Eβ€²\textstyle{E^{\prime}}

Some care must be taken in using the β€œif direction” of Theorem 2.6 when the schemes E,Eβ€²E,E^{\prime} are not reduced. In the sequel, we do not use this part of the theorem in such cases.

In [2] the following notion of regularity for graded 𝕂\mathbb{K}-algebras was introduced.

Definition 2.7.

[2] A finitely-presented graded 𝕂\mathbb{K}-algebra AA is Artin-Shelter regular (AS-regular) of dimension dd if:

  • (i)

    the global dimension of AA is dd;

  • (ii)

    the Gelfand-Kirillov dimension of AA is finite;

  • (iii)

    AA is Gorenstein: ExtAn​(𝕂,A)=0\hbox{\rm Ext}^{n}_{A}(\mathbb{K},A)=0 if nβ‰ dn\neq d, and ExtAd​(𝕂,A)≅𝕂\hbox{\rm Ext}^{d}_{A}(\mathbb{K},A)\cong\mathbb{K}.

Let us now restrict to the case we study in this paper and assume that A=T​(V)/⟨R⟩A=T(V)/\langle R\rangle is a quadratic algebra with dim𝕂V=dim𝕂R=3\dim_{\mathbb{K}}V=\dim_{\mathbb{K}}R=3. In [1] it is shown that if AA is AS-regular, then AA is semi-standard and nondegenerate. Not all semi-standard, nondegenerate quadratic algebra are AS-regular, however. Following [1] we say that AA is exceptional if the point scheme EE is the union of a line and a conic in β„™2{\mathbb{P}}^{2} and the automorphism Οƒ:Eβ†’E\sigma:E\to E interchanges these components. In [1, Proposition 4.11] it is proven that an exceptional algebra is not AS-regular. Finally, by [1, Theorem 1, Theorem 6.8], every quadratic AS-regular algebra of global dimension 33 is geometric.

Suppose that RβŠ‚VβŠ—VR\subset V\otimes V has {r1,r2,r3}\{r_{1},r_{2},r_{3}\} as a 𝕂\mathbb{K}-basis. Using xi,yi,zix_{i},y_{i},z_{i}, i=0,1i=0,1, as coordinates on the i+1i+1st factor of ℙ​(Vβˆ—)×ℙ​(Vβˆ—){\mathbb{P}}(V^{*})\times{\mathbb{P}}(V^{*}), we can factor the multilinearizations r1~,r2~,r3~\widetilde{r_{1}},\widetilde{r_{2}},\widetilde{r_{3}} in two ways:

(1) M​[x1y1z1]=[r1~r2~r3~],[x0y0z0]​N=[r1~r2~r3~],M\begin{bmatrix}x_{1}\\ y_{1}\\ z_{1}\end{bmatrix}=\begin{bmatrix}\widetilde{r_{1}}\\ \widetilde{r_{2}}\\ \widetilde{r_{3}}\end{bmatrix},\qquad\begin{bmatrix}x_{0}&y_{0}&z_{0}\end{bmatrix}N=\begin{bmatrix}\widetilde{r_{1}}&\widetilde{r_{2}}&\widetilde{r_{3}}\end{bmatrix},

where MM is a 3Γ—33\times 3 matrix with entries consisting of linear forms in x0,y0,z0x_{0},y_{0},z_{0} and NN is a 3Γ—33\times 3 matrix with entries consisting of linear forms in x1,y1,z1x_{1},y_{1},z_{1}. Then it is straightforward to prove that the set of closed points of the scheme E1E_{1} is the zero locus of detM\det M, 𝒡​(detM)\mathcal{Z}(\det M), in β„™2{\mathbb{P}}^{2}. Similarly, the set of closed points of E2E_{2} is equal to 𝒡​(detN)\mathcal{Z}(\det N) in β„™2{\mathbb{P}}^{2}. When AA is semi-standard, we often identify corresponding coordinate functions by suppressing the subscripts. It is easy to show that a semi-standard algebra is nondegenerate if and only if the rank of the matrix MM is 22 at every closed point of EE. Moreover, the automorphism Οƒ:Eβ†’E\sigma:E\to E can be computed on closed points by taking the cross product of two linearly independent rows of MM; see [1, Section 1], for example.

For each AS-regular twisted tensor product in our classification, AA, we determine the pair (E,Οƒ)(E,\sigma) for a particular representative of the graded isomorphism class of AA. We adopt the terminology of [8] and [5] to describe the types of pairs that are possible. In [8] and [5] the ground field, 𝕂\mathbb{K}, is assumed to be algebraically closed with char​𝕂=0{\rm char}\,\mathbb{K}=0. Though we assume only that 𝕂\mathbb{K} is algebraically closed and char​𝕂≠2{\rm char}\,\mathbb{K}\neq 2, these are sufficient for our purposes.

  • β€’

    Type P{\rm P}: E=β„™2E={\mathbb{P}}^{2}; ΟƒβˆˆAut𝕂​ℙ2β‰…PGL3​(𝕂)\sigma\in{\rm Aut}_{\mathbb{K}}{\mathbb{P}}^{2}\cong{\rm PGL}_{3}(\mathbb{K}),

  • β€’

    Type S1{\rm S}_{1}: EE is a triangle; Οƒ\sigma stabilizes each component,

  • β€’

    Type S2{\rm S}_{2}: EE is a triangle; Οƒ\sigma interchanges two components,

  • β€’

    Type S3{\rm S}_{3}: EE is a triangle; Οƒ\sigma cyclically permutes the components,

  • β€’

    Type S1β€²{\rm S}_{1}^{\prime}: EE is a union of a line and a conic meeting at two points; Οƒ\sigma stabilizes each component and the intersection points,

  • β€’

    Type S2β€²{\rm S}_{2}^{\prime}: EE is a union of a line and a conic meeting at two points; Οƒ\sigma stabilizes each component and interchanges the intersection points,

  • β€’

    Type T1{\rm T}_{1}: EE is a union of three lines meeting at one point; Οƒ\sigma stabilizes each component,

  • β€’

    Type T2{\rm T}_{2}: EE is a union of three lines meeting at one point; Οƒ\sigma interchanges two components,

  • β€’

    Type T3{\rm T}_{3}: EE is a union of three lines meeting at one point; Οƒ\sigma cyclically permutes the components,

  • β€’

    Type Tβ€²{\rm T}^{\prime}: EE is a union of a line and a conic meeting at one point; Οƒ\sigma stabilizes each component,

  • β€’

    Type CC{\rm CC}: EE is a cuspidal cubic curve,

  • β€’

    Type NC{\rm NC}: EE is a nodal cubic curve,

  • β€’

    Type WL{\rm WL}: EE is a union of a double line and a line,

  • β€’

    Type TL{\rm TL}: EE is a triple line,

  • β€’

    Type EC{\rm EC}: EE is an elliptic curve.

Note that some of the schemes described here are reducible and/or non-reduced. Furthermore, [5] divides these types into subtypes: Type P into Type Pi{\rm P}_{i} for i=1,2,3i=1,2,3; Type NC into Type NCi{\rm NC}_{i} for i=1,2i=1,2; Type WL into Type WLi{\rm WL}_{i} for i=1,2,3i=1,2,3; and Type TL into Type TLi{\rm TL}_{i} for i=1,2,3,4i=1,2,3,4.

In [1, 4.13], the authors identified four subtypes of Type EC, denoted A,B,E,A,B,E, and HH, which were defined in terms of the automorphism Οƒ\sigma. In [6], Matsuno completed the classification of algebras of Type EC up to graded algebra isomorphism in characteristic 0, showing that there are no additional subtypes.

3. Elliptic-type twisted tensor products

Since we assume char​𝕂≠2{\rm char}\ \mathbb{K}\neq 2, [4, Lemma 5.2] implies that any elliptic-type twisted tensor product is isomorphic to an algebra in the family

T​(g,h)=π•‚β€‹βŸ¨x,y,z⟩⟨x​yβˆ’y​x,z​y+y​zβˆ’x2βˆ’g​y2,z2+h​y2⟩g,hβˆˆπ•‚.T(g,h)=\dfrac{\mathbb{K}\langle x,y,z\rangle}{\langle xy-yx,zy+yz-x^{2}-gy^{2},z^{2}+hy^{2}\rangle}\quad g,h\in\mathbb{K}.

In this section we show that all algebras in this family are semi-standard and nondegenerate. We describe the associated point schemes and describe the distinct graded algebra isomorphism classes in this family. Our results for elliptic-type twisted tensor products are summarized in Table 1 and the following theorem.

Table 1. Mapping of elliptic-type TTP cases
TTP Case Subcase Algebra Condition Type
T​(g,h)T(g,h) h​(g2+4​h)β‰ 0h(g^{2}+4h)\neq 0 T​(g2/h)T(g^{2}/h) g2/hβˆ‰{0,βˆ’4}g^{2}/h\notin\{0,-4\} EC, subtype B
T​(0,1)T(0,1)
hβ‰ 0=g2+4​hh\neq 0=g^{2}+4h T​(βˆ’4)T(-4) N​C2NC_{2}
h=0h=0 T​(g,0)T(g,0) g∈{0,1}g\in\{0,1\} exceptional
Theorem 3.1.

Every elliptic-type twisted tensor product is isomorphic as a graded algebra to T​(g,h)T(g,h) for some g,hβˆˆπ•‚.g,h\in\mathbb{K}. The algebras listed in Table 1 are pairwise non-isomorphic, and the table gives the types of AS-regular algebras.

The proof of Theorem 3.1 is at the end of this section.

In [4], we characterized when the algebras T​(g,h)T(g,h) are AS-regular. The first result in this section elaborates on that characterization, and describes the point scheme of T​(g,h)T(g,h) and the associated automorphism.

Proposition 3.2.

The algebra T​(g,h)T(g,h) is semi-standard and nondegenerate for any g,hβˆˆπ•‚g,h\in\mathbb{K}. Moreover, T​(g,h)T(g,h) is AS-regular if and only if hβ‰ 0h\neq 0. The point scheme of T​(g,h)T(g,h) is

E=𝒡​(h​y3+x2​zβˆ’y​z2+g​y2​z)βŠ‚β„™2.E=\mathcal{Z}(hy^{3}+x^{2}z-yz^{2}+gy^{2}z)\subset{\mathbb{P}}^{2}.

The automorphism Οƒ:Eβ†’E\sigma:E\to E switches the points [1:0:0][1:0:0] and [0:0:1][0:0:1]. If hβ‰ 0h\neq 0, Οƒ([x:y:z])=[xz:yz:βˆ’hy2]\sigma([x:y:z])=[xz:yz:-hy^{2}] if yβ‰ 0y\neq 0.

If h=0h=0, Οƒ\sigma interchanges the line z=0z=0 and the conic x2βˆ’y​z+g​y2=0x^{2}-yz+gy^{2}=0.

Proof.

The matrices MM and NN defined in equation (1) are

M=[βˆ’y0x00βˆ’x0z0βˆ’g​y0y00h​y0z0],N=[y1βˆ’x10βˆ’x1βˆ’g​y1+z1h​y10y1z1].M=\begin{bmatrix}-y_{0}&x_{0}&0\\ -x_{0}&z_{0}-gy_{0}&y_{0}\\ 0&hy_{0}&z_{0}\end{bmatrix},\ \ N=\begin{bmatrix}y_{1}&-x_{1}&0\\ -x_{1}&-gy_{1}+z_{1}&hy_{1}\\ 0&y_{1}&z_{1}\end{bmatrix}.

If we identify coordinate functions by suppressing subscripts, one checks that

detM=h​y3+x2​zβˆ’y​z2+g​y2​z=βˆ’detN.\det M=hy^{3}+x^{2}z-yz^{2}+gy^{2}z=-\det N.

It follows that T​(g,h)T(g,h) is semi-standard. It is easy to prove that rank​(M)β‰₯2\hbox{rank}(M)\geq 2 at all points of β„™2{\mathbb{P}}^{2}, so T​(g,h)T(g,h) is nondegenerate. By [4, Theorem 6.2], the algebras T​(g,h)T(g,h) are AS-regular if and only if hβ‰ 0h\neq 0.

The descriptions of Οƒ([x:y:z])\sigma([x:y:z]) when hβ‰ 0h\neq 0 and h=0h=0 are obtained by taking the cross product of appropriate rows in MM. ∎

The algebras T​(g,0)T(g,0) are exceptional in the sense of [1, Section 4.9]. We prove that up to isomorphism, there are only two such algebras in the family T​(g,h)T(g,h).

Proposition 3.3.

If gβ‰ 0g\neq 0, T​(g,0)β‰…T​(1,0)T(g,0)\cong T(1,0). Moreover, T​(1,0)≇T​(0,0)T(1,0)\ncong T(0,0).

Proof.

The first statement follows by rescaling z↦g​zz\mapsto gz and x↦g​xx\mapsto\sqrt{g}x. For the second statement, suppose there is an isomorphism Ο†:T​(1,0)β†’T​(0,0)\varphi:T(1,0)\to T(0,0). It is easy to check that, up to rescaling, zz is the only degree-1 element of T​(0,0)T(0,0) that squares to 0. Thus we may assume φ​(z)=z\varphi(z)=z.

It is also straightforward to check that if u,v∈T​(0,0)1u,v\in T(0,0)_{1} are linearly independent and commute, then u,v∈span𝕂​{x,y}u,v\in{\rm span}_{\mathbb{K}}\{x,y\}. Thus φ​(x)=Ξ±1​x+Ξ²1​y\varphi(x)=\alpha_{1}x+\beta_{1}y and φ​(y)=Ξ±2​x+Ξ²2​y\varphi(y)=\alpha_{2}x+\beta_{2}y for Ξ±1,Ξ±2,Ξ²1,Ξ²2βˆˆπ•‚\alpha_{1},\alpha_{2},\beta_{1},\beta_{2}\in\mathbb{K}. Now, a direct calculation shows that φ​(z​y+y​zβˆ’x2βˆ’y2)=0\varphi(zy+yz-x^{2}-y^{2})=0 implies φ​(x)\varphi(x) and φ​(y)\varphi(y) are linearly dependent, a contradiction. ∎

For the remainder of the section, we assume hβ‰ 0h\neq 0. As shown above, all algebras T​(g,h)T(g,h) are AS-regular in this case.

When hβ‰ 0h\neq 0, the closed points of EE describe the projectivization of a plane cubic curve. After the transformation x↦yx\mapsto y, yβ†¦βˆ’xy\mapsto-x, z↦h​zz\mapsto hz, we see that EE can be described in Weierstrass form by

y2​z=x3βˆ’g​x2​zβˆ’h​x​z2.y^{2}z=x^{3}-gx^{2}z-hxz^{2}.

Following the formulae in [9, III.1], the discriminant of the curve obtained by setting z=1z=1 is Δ​(g,h)=16​h2​(g2+4​h)\Delta(g,h)=16h^{2}(g^{2}+4h). Thus we see that EE is the projectivization of an elliptic curve if and only if g2+4​hβ‰ 0g^{2}+4h\neq 0. Furthermore, the jj-invariant of this elliptic curve is j​(g,h)=162​(g2+3​h)3h2​(g2+4​h)j(g,h)=\dfrac{16^{2}(g^{2}+3h)^{3}}{h^{2}(g^{2}+4h)}. Setting β„“=g2/h\ell=g^{2}/h yields the expression j​(β„“)=162​(β„“+3)3β„“+4j(\ell)=\dfrac{16^{2}(\ell+3)^{3}}{\ell+4}, which is sometimes more convenient. Recall that the jj-invariant classifies elliptic curves up to isomorphism, see [9, Proposition III.1.4 (b)].

The next result characterizes T​(g,h)T(g,h) when EE is a singular curve; the case where EE is an elliptic curve is described below.

Proposition 3.4.

If hβ‰ 0h\neq 0 and g2+4​h=0g^{2}+4h=0, then EE is a nodal cubic curve, and the automorphism Οƒ\sigma fixes the node. (type N​C2NC_{2})
In this case, T​(g,h)T(g,h) is isomorphic as a 𝕂\mathbb{K}-algebra to

π•‚β€‹βŸ¨x,y,z⟩⟨x​zβˆ’2​y​x+z​y,z​xβˆ’2​x​y+y​z,y2+x2⟩.\dfrac{\mathbb{K}\langle x,y,z\rangle}{\langle xz-2yx+zy,zx-2xy+yz,y^{2}+x^{2}\rangle}.
Proof.

Using the description of EE as 𝒡​(h​y3+x2​zβˆ’y​z2+g​y2​z)\mathcal{Z}(hy^{3}+x^{2}z-yz^{2}+gy^{2}z) from Theorem 3.2 we see that if hβ‰ 0h\neq 0 and g2+4​h=0g^{2}+4h=0, then EE is the projectivization of a nodal cubic curve:

x2​z=y​(2​zβˆ’g​y)24x^{2}z=\dfrac{y(2z-gy)^{2}}{4}

Evidently the node is [0:2:g][0:2:g], and by Theorem 3.2 we see that Οƒ([0:2:g])=[0:2g:βˆ’4h]=[0:2:g]\sigma([0:2:g])=[0:2g:-4h]=[0:2:g] since gβ‰ 0g\neq 0.

Let AA denote the algebra specified in the statement of the Proposition. The map determined by: x↦α1​(xβˆ’y)x\mapsto\alpha_{1}(x-y), y↦α2​(x+y+z)y\mapsto\alpha_{2}(x+y+z), zβ†¦βˆ’3​xβˆ’3​y+zz\mapsto-3x-3y+z where Ξ±2=βˆ’g/2​h\alpha_{2}=-g/2h and Ξ±12=βˆ’8​g/h\alpha_{1}^{2}=-8g/h, is an isomorphism T​(g,h)β†’AT(g,h)\to A. ∎

It remains to consider the case where the discriminant Δ​(g,h)β‰ 0\Delta(g,h)\neq 0. Our next result shows that in this case, T​(g,h)T(g,h) is a Type EC, subtype B algebra.

Theorem 3.5.

Suppose that Δ​(g,h)β‰ 0\Delta(g,h)\neq 0, so that EE is a nonsingular cubic curve. There exists an element O∈EO\in E such that for the corresponding group law on EE, the automorphism Οƒ:Eβ†’E\sigma:E\to E is given by σ​(P)+P=O\sigma(P)+P=O for all P∈EP\in E.

Proof.

It is straightforward to check that a point [x0:1:z0]∈E[x_{0}:1:z_{0}]\in E is a fixed point of Οƒ\sigma if and only if x02=2​z0βˆ’gx_{0}^{2}=2z_{0}-g and z02=βˆ’hz_{0}^{2}=-h. Let O∈EO\in E be any fixed point of Οƒ\sigma. Consider the corresponding group law on EE, see [9, III.2] for example.

The line y=0y=0 intersects EE in e1=[1:0:0]e_{1}=[1:0:0] and e3=[0:0:1]e_{3}=[0:0:1], and Οƒ\sigma interchanges these points. We claim that e1+e3=Oe_{1}+e_{3}=O in the group law. To see this, first observe that y=0y=0 is tangent to EE at e3e_{3}. The line LL through e3e_{3} and O=[x0:1:z0]O=[x_{0}:1:z_{0}] is x=x0​yx=x_{0}y. The point e1e_{1} is not on LL, and LL is not tangent to EE at e3e_{3}, so we can write e1+e3=[x0:1:z1]e_{1}+e_{3}=[x_{0}:1:z_{1}]. The condition that e1+e3e_{1}+e_{3} lies on 𝒡​(h​y3+x2​zβˆ’y​z2+g​y2​z)\mathcal{Z}(hy^{3}+x^{2}z-yz^{2}+gy^{2}z), and the fact that x02=2​z0βˆ’gx_{0}^{2}=2z_{0}-g and z02=βˆ’hz_{0}^{2}=-h implies

z12βˆ’2​z0​z1+z02=(z1βˆ’z0)2=0.z_{1}^{2}-2z_{0}z_{1}+z_{0}^{2}=(z_{1}-z_{0})^{2}=0.

Thus z1=z0z_{1}=z_{0} and e1+e3=0e_{1}+e_{3}=0 as desired.

The argument above also proves that x=x0​yx=x_{0}y is the tangent line to EE at OO. Since we assumed only that OO was a fixed point of Οƒ\sigma on EE, if [x1:1:z1]∈E[x_{1}:1:z_{1}]\in E is any other fixed point of Οƒ\sigma, the tangent line at that point is x=x1​yx=x_{1}y.

Let P=[x1:1:z1]∈Eβˆ’{e1,e3}P=[x_{1}:1:z_{1}]\in E-\{e_{1},e_{3}\} be arbitrary. Then Οƒ(P)=[x1z1:z1:βˆ’h]\sigma(P)=[x_{1}z_{1}:z_{1}:-h]. If σ​(P)β‰ P\sigma(P)\neq P, then z12β‰ βˆ’hz_{1}^{2}\neq-h. The line through PP and σ​(P)\sigma(P) is xβˆ’x1​y=0x-x_{1}y=0, and e3e_{3} is the third point of intersection between this line and EE. The line through e3e_{3} and OO is tangent to EE at OO, so P+σ​(P)=OP+\sigma(P)=O.

If σ​(P)=P\sigma(P)=P, then as observed above, the tangent line to EE at PP is the line xβˆ’x1​y=0x-x_{1}y=0. The calculation then proceeds as before, yielding P+σ​(P)=OP+\sigma(P)=O. ∎

Next we classify the algebras T​(g,h)T(g,h) with hβ‰ 0h\neq 0 up to graded algebra isomorphism.

Proposition 3.6.

If hβ‰ 0h\neq 0 and hβ€²β‰ 0h^{\prime}\neq 0, then T​(g,h)β‰…T​(gβ€²,hβ€²)T(g,h)\cong T(g^{\prime},h^{\prime}) if and only if g2​hβ€²=(gβ€²)2​hg^{2}h^{\prime}=(g^{\prime})^{2}h.

Proof.

Assume that g2​hβ€²=(gβ€²)2​hg^{2}h^{\prime}=(g^{\prime})^{2}h. If gβ‰ 0g\neq 0, then the map determined by x↦α​xx\mapsto\alpha x, y↦β​yy\mapsto\beta y, z↦zz\mapsto z, where Ξ±2=Ξ²\alpha^{2}=\beta and Ξ²=gβ€²/g\beta=g^{\prime}/g is an isomorphism T​(g,h)β†’T​(gβ€²,hβ€²)T(g,h)\to T(g^{\prime},h^{\prime}). If g=0g=0, then the map determined by x↦α​xx\mapsto\alpha x, y↦β​yy\mapsto\beta y, z↦zz\mapsto z, where Ξ±2=Ξ²\alpha^{2}=\beta and Ξ²2=hβ€²/h\beta^{2}=h^{\prime}/h is an isomorphism T​(g,h)β†’T​(gβ€²,hβ€²)T(g,h)\to T(g^{\prime},h^{\prime}).

Suppose, conversely, that Ο†:T​(gβ€²,hβ€²)β†’T​(g,h)\varphi:T(g^{\prime},h^{\prime})\to T(g,h) is an isomorphism. A calculation, using the bases {x2,x​y,x​z,y2,y​z,z​x}\{x^{2},xy,xz,y^{2},yz,zx\} in degree 22, shows that commuting, linearly independent degree-1 elements of T​(g,h)T(g,h) lie in span𝕂​{x,y}{\rm span}_{\mathbb{K}}\{x,y\}. Thus there is no loss of generality in assuming that

φ​(x)=Ξ±1​x+Ξ²1​y,φ​(y)=Ξ±2​x+Ξ²2​y,φ​(z)=Ξ±3​x+Ξ²3​y+z.\varphi(x)=\alpha_{1}x+\beta_{1}y,\quad\varphi(y)=\alpha_{2}x+\beta_{2}y,\quad\varphi(z)=\alpha_{3}x+\beta_{3}y+z.

Then

0=φ​(z2+h′​y2)\displaystyle 0=\varphi(z^{2}+h^{\prime}y^{2}) =(Ξ±32+Ξ²3+h′​α22)​x2+2​(Ξ±3​β3+h′​α2​β2)​x​y\displaystyle=(\alpha_{3}^{2}+\beta_{3}+h^{\prime}\alpha_{2}^{2})x^{2}+2(\alpha_{3}\beta_{3}+h^{\prime}\alpha_{2}\beta_{2})xy
+(Ξ²32+g​β3βˆ’h+h′​β22)​y2+Ξ±3​(x​z+z​x),\displaystyle\quad+(\beta_{3}^{2}+g\beta_{3}-h+h^{\prime}\beta_{2}^{2})y^{2}+\alpha_{3}(xz+zx),

so we have

Ξ±3=0Ξ²3=βˆ’h′​α22Ξ±2​β2=0Ξ²32+g​β3+h′​β22βˆ’h=0.\alpha_{3}=0\quad\beta_{3}=-h^{\prime}\alpha_{2}^{2}\quad\alpha_{2}\beta_{2}=0\quad\beta_{3}^{2}+g\beta_{3}+h^{\prime}\beta_{2}^{2}-h=0.

Since Ξ±3=0\alpha_{3}=0, the coefficient of x​zxz in φ​(z​y+y​zβˆ’x2βˆ’g′​y2)\varphi(zy+yz-x^{2}-g^{\prime}y^{2}) is Ξ±2\alpha_{2}, so Ξ±2=0\alpha_{2}=0, Ξ²3=0\beta_{3}=0, and h′​β22=hh^{\prime}\beta_{2}^{2}=h. Bearing these in mind, we have

φ​(z​y+y​zβˆ’x2βˆ’g′​y2)=(Ξ²2βˆ’Ξ±12)​x2βˆ’2​α1​β1​x​y+(g​β2βˆ’g′​β22βˆ’Ξ²12)​y2.\varphi(zy+yz-x^{2}-g^{\prime}y^{2})=(\beta_{2}-\alpha_{1}^{2})x^{2}-2\alpha_{1}\beta_{1}xy+(g\beta_{2}-g^{\prime}\beta_{2}^{2}-\beta_{1}^{2})y^{2}.

We cannot have Ξ±1=0\alpha_{1}=0, else Ξ²2=0\beta_{2}=0 and φ​(y)=0\varphi(y)=0, so Ξ²1=0\beta_{1}=0 and g​β2=g′​β22g\beta_{2}=g^{\prime}\beta_{2}^{2}. Since Ξ²2β‰ 0\beta_{2}\neq 0, we have h′​β22=hh^{\prime}\beta_{2}^{2}=h and g′​β2=gg^{\prime}\beta_{2}=g, and the result follows. ∎

Remark 3.7.

Proposition 3.6 motivates the following further simplification. For β„“βˆˆπ•‚βˆ—\ell\in\mathbb{K}^{*}, we define

T​(β„“)=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​y+y​zβˆ’x2βˆ’β„“β€‹y2,z2+ℓ​y2⟩.T(\ell)=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zy+yz-x^{2}-\ell y^{2},z^{2}+\ell y^{2}\rangle.

When g​hβ‰ 0gh\neq 0, it is easily shown that T​(g,h)β‰…T​(g2/h)T(g,h)\cong T(g^{2}/h) by rescaling x↦g/h​xx\mapsto\sqrt{g/h}x and y↦g​y/hy\mapsto gy/h. Proposition 3.6 then implies T​(β„“)β‰…T​(β„“β€²)T(\ell)\cong T(\ell^{\prime}) if and only if β„“=β„“β€²\ell=\ell^{\prime}.

Recall that the jj-invariant of the point scheme of T​(β„“)T(\ell) is given by j​(β„“)=162​(β„“+3)3β„“+4j(\ell)=\dfrac{16^{2}(\ell+3)^{3}}{\ell+4}. Setting l=0l=0 we see that j​(0)=123j(0)=12^{3}. The point scheme of T​(0,1)T(0,1) has j=123j=12^{3}; we β€œcompactify” the family of algebras T​(β„“)T(\ell), β„“βˆˆπ•‚βˆ—\ell\in\mathbb{K}^{*} by defining T​(0)=T​(0,1)T(0)=T(0,1). (The algebra obtained by setting β„“=0\ell=0 in the presentation above is T​(0,0)T(0,0), which is not AS-regular.)

The jj-invariant does not completely characterize the isomorphism type of the algebra T​(β„“)T(\ell). Setting t=β„“+3t=\ell+3 and considering the discriminant of the polynomial t3βˆ’(j/162)​(t+1),t^{3}-(j/16^{2})(t+1), we see that for a fixed elliptic curve EE, or equivalently for a fixed value of jj, there are three isomorphism classes of algebras T​(g,h)T(g,h) with point scheme equal to EE whenever jβˆ‰{0,123}j\notin\{0,12^{3}\}, two when j=123j=12^{3}, and one when j=0j=0.

Comparing the above to [6, Proposition 3.10] shows that in characteristic 0, every quadratic AS-regular algebra of type EC, subtype B, is isomorphic to a graded twisted tensor product of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z]. By [5, Theorem 3.1], there is only one isomorphism class of type N​C2NC_{2} algebras, and Proposition 3.4 shows these algebras are graded twisted tensor products of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z].

We conclude with a proof of Theorem 3.1.

Proof of Theorem 3.1.

Every elliptic-type twisted tensor product is isomorphic to T​(g,h)T(g,h) by [4, Lemma 5.2]. Proposition 3.2 shows that T​(g,h)T(g,h) is AS-regular if and only if hβ‰ 0h\neq 0. The algebras T​(g,0)T(g,0) are classified in Proposition 3.3.

When hβ‰ 0h\neq 0, the graded algebra isomorphism classes of T​(g,h)T(g,h) are described in Proposition 3.6. This classification is described in terms of the family T​(β„“)T(\ell), β„“β‰ 0\ell\neq 0, in Remark 3.7. The types of AS-regular algebras in the family T​(g,h)T(g,h) are characterized in Proposition 3.4 and Theorem 3.5. ∎

4. Reducible-type twisted tensor products

In this section, TT denotes a quadratic twisted tensor product of reducible type, in normal form [4, Section 4]. The results below classify TT up to graded algebra isomorphism. When TT is AS-regular, we identify its type. We assume char​𝕂≠2{\rm char}\ \mathbb{K}\neq 2.

By [4, Theorem 4.9] Tβ‰…π•‚β€‹βŸ¨x,y,z⟩/IT\cong\mathbb{K}\langle x,y,z\rangle/I where II is the graded ideal of π•‚β€‹βŸ¨x,y,z⟩\mathbb{K}\langle x,y,z\rangle generated by the elements

x​yβˆ’y​x,z​xβˆ’a​x2βˆ’b​x​yβˆ’c​y2βˆ’d​x​zβˆ’e​y​zβˆ’z2,z​yβˆ’B​x​yβˆ’C​y2βˆ’D​y​z,xy-yx,zx-ax^{2}-bxy-cy^{2}-dxz-eyz-z^{2},zy-Bxy-Cy^{2}-Dyz,

such that (a,d)(a,d) is not a zero of certain polynomials fn​(t,u)f_{n}(t,u) for all nβ‰₯1n\geq 1, and the parameters satisfy one of the following cases:

  • R(i):

    a=B​(1βˆ’dβˆ’B)a=B(1-d-B), b=c=e=C=D=0b=c=e=C=D=0;

  • R(ii):

    e=B=C=0e=B=C=0, D=1D=1;

  • R(iii):

    d=βˆ’1d=-1, B=2B=2, e=C=0e=C=0, D=βˆ’1D=-1;

  • R(iv):

    a=B​(1βˆ’dβˆ’B)a=B(1-d-B), b=1βˆ’dβˆ’2​Bb=1-d-2B, c=βˆ’1c=-1, C=1C=1, e=D=0e=D=0;

  • R(v):

    e=0e=0, d=D=βˆ’1d=D=-1, B=2B=2, C=1C=1.

  • R(vi):

    e=1e=1, d=D=0d=D=0, a=B​(1βˆ’B)a=B(1-B), b=Cβˆ’Bβˆ’2​B​Cb=C-B-2BC, c=βˆ’C​(1+C)c=-C(1+C);

  • R(vii):

    B=C=0B=C=0, e=d=D=1e=d=D=1.

We use the polynomials fn​(t,u)f_{n}(t,u) in the proof of Proposition 4.9 below. We note here that f1​(t,u)=1βˆ’tf_{1}(t,u)=1-t, so aβ‰ 1a\neq 1.

By [4, Theorem 6.2], no algebras in cases R(i), R(iv), R(vi) are AS-regular. After two preliminary results, the analyses in this section are divided into two subsections, according to whether or not TT is AS-regular. The results are summarized in Table 2 and the following theorem.

Table 2. Mapping of reducible-type TTP cases not isomorphic to an Ore-type TTP
TTP Case Subcase Algebra Type
R(iii) b2βˆ’4​a​c+4​c=0b^{2}-4ac+4c=0 UU S2S_{2}
b2βˆ’4​a​c+4​cβ‰ 0b^{2}-4ac+4c\neq 0 Uβ€²U^{\prime} S2β€²S_{2}^{\prime}
R(i) B+d=0B+d=0 R0R_{0} not AS-regular
B+dβ‰ 0B+d\neq 0 R​(q)R(q)
R(iv)
B+d=0B+d=0 R1R_{1}
Theorem 4.1.

Every reducible-type twisted tensor product is isomorphic as a graded algebra to one of the algebras listed in Table 2, or to a twisted tensor product of Ore type. The algebras listed in Table 2 are pairwise non-isomorphic, and the table gives the types of the AS-regular algebras.

The proof of Theorem 4.1 can be found at the end of the section.

Remark 4.2.

By [5, Theorem 3.1], in characteristic 0, the isomorphism classes of Type S2S_{2} AS-regular algebras are parametrized by points of β„™1{\mathbb{P}}^{1}, but there is only one isomorphism class of Type S2β€²S^{\prime}_{2}. We show in Section 5 that no other graded twisted tensor products of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z] are of Type S2S_{2}.

The first lemma, and the theorem that follows, show that only case R(iii) contains AS-regular algebras not isomorphic to a graded Ore extension of 𝕂​[x,y]\mathbb{K}[x,y]. (Ore-type twisted tensor products are discussed in Section 5.)

Lemma 4.3.

The following hold.

  • (1)

    Any twisted tensor product from case R(v) is isomorphic as a graded algebra to an algebra from case R(iii).

  • (2)

    Any twisted tensor product from case R(vii) is isomorphic to an algebra from case R(ii).

  • (3)

    Any twisted tensor product from case R(ii) is isomorphic to an Ore-type twisted tensor product.

Proof.

For (1), the map sending x↦xβˆ’y/2x\mapsto x-y/2 and fixing yy and zz identifies a case R(v) algebra with one from case R(iii).

For (2), the map sending z↦zβˆ’y/2z\mapsto z-y/2 and fixing xx and yy identifies a case R(vii) algebra with one from case R(ii).

For (3), If TT is a reducible-type twisted tensor product from case R(ii) with a=0a=0 and d=1d=1, then the map interchanging xx and zz, fixing yy, identifies TT with the Ore-type algebra with relations

x​yβˆ’y​x,z​yβˆ’y​z,z​x+x2+c​y2βˆ’x​zβˆ’b​y​z.xy-yx,zy-yz,zx+x^{2}+cy^{2}-xz-byz.

If TT is any other reducible-type twisted tensor product from case R(ii), the map sending xβ†’x+α​zx\to x+\alpha z and fixing yy and zz where Ξ±\alpha satisfies a​α2+(dβˆ’1)​α+1=0a\alpha^{2}+(d-1)\alpha+1=0 identifies a case R(ii) algebra with the algebra with relations

x​yβˆ’y​x,z​yβˆ’y​z,(1βˆ’a​α)​z​xβˆ’a​x2βˆ’b​x​yβˆ’c​y2βˆ’(d+a​α)​x​zβˆ’b​α​y​z.xy-yx,zy-yz,(1-a\alpha)zx-ax^{2}-bxy-cy^{2}-(d+a\alpha)xz-b\alpha yz.

Note that this algebra is an Ore-type twisted tensor product provided that 1βˆ’a​α≠01-a\alpha\neq 0. If a=0a=0, then this is clear. Suppose that aβ‰ 0a\neq 0. Let Ξ΄=(dβˆ’1)2βˆ’4​a\delta=(d-1)^{2}-4a be the discriminant of a​t2+(dβˆ’1)​t+1at^{2}+(d-1)t+1. If Ξ΄β‰ 0\delta\neq 0, then a​α2+(dβˆ’1)​α+1=0a\alpha^{2}+(d-1)\alpha+1=0 has two distinct solutions and we may choose Ξ±β‰ aβˆ’1\alpha\neq a^{-1}. Suppose that Ξ΄=0\delta=0 and Ξ±=aβˆ’1\alpha=a^{-1} is the unique solution of a​α2+(dβˆ’1)​α+1=0a\alpha^{2}+(d-1)\alpha+1=0. One checks that a=1a=1, but this contradicts the fact that TT is a twisted tensor product. ∎

Theorem 4.4.

Let TT be a reducible-type twisted tensor product in normal form. Consider the following statements.

  1. (1)

    a+d≠0≠Da+d\neq 0\neq D,

  2. (2)

    TT is AS-regular of dimension 3,

  3. (3)

    TT is semi-standard.

Then (1)⇒(2)⇒(3)⇒D≠0(1)\Rightarrow(2)\Rightarrow(3)\Rightarrow D\neq 0. If TT is semi-standard and a+d=0a+d=0, then TT is isomorphic as a graded algebra to an Ore-type twisted tensor product.

Proof.

The implication (1)β‡’(2)(1)\Rightarrow(2) follows from [4, Theorem 6.2(2)], and (2)β‡’(3)(2)\Rightarrow(3) is immediate. Assume TT is semi-standard. The matrices MM and NN of equation (1) for a reducible-type algebra are

M=[βˆ’y0x00z0βˆ’a​x0βˆ’b​x0βˆ’c​y0βˆ’d​x0βˆ’e​y0βˆ’z00z0βˆ’B​x0βˆ’C​y0βˆ’D​y0]M=\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}-ax_{0}&-bx_{0}-cy_{0}&-dx_{0}-ey_{0}-z_{0}\\ 0&z_{0}-Bx_{0}-Cy_{0}&-Dy_{0}\end{bmatrix}

and

N=[y1βˆ’a​x1βˆ’b​y1βˆ’d​z1βˆ’B​y1βˆ’x1βˆ’c​y1βˆ’e​z1βˆ’C​y1βˆ’D​z10x1βˆ’z1y1].N=\begin{bmatrix}y_{1}&-ax_{1}-by_{1}-dz_{1}&-By_{1}\\ -x_{1}&-cy_{1}-ez_{1}&-Cy_{1}-Dz_{1}\\ 0&x_{1}-z_{1}&y_{1}\end{bmatrix}.

Suppressing subscripts we have

detM\displaystyle\det M =βˆ’y((aDβˆ’dB)x2+(bDβˆ’eBβˆ’dC)xy+(cDβˆ’eC)y2\displaystyle=-y((aD-dB)x^{2}+(bD-eB-dC)xy+(cD-eC)y^{2}
+(dβˆ’Bβˆ’D)xz+(eβˆ’C)yz+z2),\displaystyle\quad+(d-B-D)xz+(e-C)yz+z^{2}),
detN\displaystyle\det N =y​((Bβˆ’a)​x2+(Cβˆ’b)​x​yβˆ’c​y2+(Dβˆ’dβˆ’B)​x​zβˆ’(e+C)​y​zβˆ’D​z2).\displaystyle=y((B-a)x^{2}+(C-b)xy-cy^{2}+(D-d-B)xz-(e+C)yz-Dz^{2}).

Since TT is semi-standard, we have detM=k​detN\det M=k\det N for some kβˆˆπ•‚k\in\mathbb{K}. Examining the coefficients of y​z2yz^{2}, we see that Dβ‰ 0D\neq 0, so TT belongs to case R(ii), R(iii), R(v), or R(vii). If TT is an algebra from case R(iii) or R(v), then d=βˆ’1d=-1. Since f1​(a,d)=1βˆ’aβ‰ 0f_{1}(a,d)=1-a\neq 0, it follows that a+dβ‰ 0a+d\neq 0. If TT is from case R(ii) or R(vii), then TT is isomorphic to an Ore-type twisted tensor product by Lemma 4.3. ∎

4.1. Twisted tensor products from case R(iii)

In case R(iii), a+d≠0a+d\neq 0, and Theorem 4.4 implies that all algebras in this family are AS-regular. If TT is an algebra from case R(iii), the matrix MM is

[βˆ’y0x00z0βˆ’a​x0βˆ’b​x0βˆ’c​y0x0βˆ’z00z0βˆ’2​x0y0],\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}-ax_{0}&-bx_{0}-cy_{0}&x_{0}-z_{0}\\ 0&z_{0}-2x_{0}&y_{0}\end{bmatrix},

so the point scheme of TT is

E=𝒡​(y​(z2βˆ’2​x​z+(2βˆ’a)​x2βˆ’b​x​yβˆ’c​y2)).E=\mathcal{Z}(y(z^{2}-2xz+(2-a)x^{2}-bxy-cy^{2})).

The automorphism, which has order 2, is

Οƒ([x:y:z])={[x:y:2​xβˆ’z]yβ‰ 0[zβˆ’x:0:zβˆ’a​x]y=0.\sigma([x:y:z])=\begin{cases}[x:y:2x-z]&y\neq 0\\ [z-x:0:z-ax]&y=0\\ \end{cases}.

As char​𝕂≠2{\rm char}\ \mathbb{K}\neq 2, the quadratic form z2βˆ’2​x​z+(2βˆ’a)​x2βˆ’b​x​yβˆ’c​y2z^{2}-2xz+(2-a)x^{2}-bxy-cy^{2} is reducible if and only if its discriminant, b2βˆ’4​a​c+4​c=0b^{2}-4ac+4c=0.

Despite the number of parameters, there are only two graded algebra isomorphism classes of case R(iii) algebras, according to whether or not b2βˆ’4​a​c+4​c=0b^{2}-4ac+4c=0, as the next result shows. This result also clarifies the action of Οƒ\sigma on EE. We define the two algebras as follows. Let

U=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’z​x,y​xβˆ’x​z,y2+z2⟩,U=\mathbb{K}\langle x,y,z\rangle/\langle xy-zx,yx-xz,y^{2}+z^{2}\rangle,

and

Uβ€²=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’z​x,y​xβˆ’x​z,x2+y2+z2⟩.U^{\prime}=\mathbb{K}\langle x,y,z\rangle/\langle xy-zx,yx-xz,x^{2}+y^{2}+z^{2}\rangle.
Proposition 4.5.

Let TT be a twisted tensor product from case R(iii). Let s=b2βˆ’4​a​c+4​cs=b^{2}-4ac+4c.

  • (1)

    If s≠0s\neq 0, then TT is isomorphic to the algebra U′U^{\prime}.

  • (2)

    If s=0s=0, then TT is isomorphic to the algebra UU.

Proof.

For (1), let Ξ±2=2​(1βˆ’a)β€‹βˆ’2/s\alpha_{2}=2(1-a)\sqrt{-2/s} and let Ξ±1=b​α22​(1βˆ’a)\alpha_{1}=\dfrac{b\alpha_{2}}{2(1-a)}. Since aβ‰ 1a\neq 1, we have Ξ±2β‰ 0\alpha_{2}\neq 0. Define a graded algebra homomorphism Ο†:π•‚β€‹βŸ¨x,y,zβŸ©β†’π•‚β€‹βŸ¨x,y,z⟩\varphi:\mathbb{K}\langle x,y,z\rangle\to\mathbb{K}\langle x,y,z\rangle by

φ​(x)\displaystyle\varphi(x) =Ξ±1​x+y+z\displaystyle=\alpha_{1}x+y+z
φ​(y)\displaystyle\varphi(y) =Ξ±2​x\displaystyle=\alpha_{2}x
φ​(z)\displaystyle\varphi(z) =Ξ±1​x+(1+aβˆ’1)​y+(1βˆ’aβˆ’1)​z.\displaystyle=\alpha_{1}x+(1+\sqrt{a-1})y+(1-\sqrt{a-1})z.

Since Ξ±2β‰ 0\alpha_{2}\neq 0, and aβˆ’1β‰ 0a-1\neq 0, the map Ο†\varphi is clearly bijective in degree 1, and hence is an isomorphism. It suffices to prove that that Ο†\varphi is a 𝕂\mathbb{K}-linear isomorphism from the quadratic relations space of TT to that of Uβ€²U^{\prime}. For ease of notation we define Ξ²3=1+aβˆ’1\beta_{3}=1+\sqrt{a-1} and Ξ΄3=1βˆ’aβˆ’1\delta_{3}=1-\sqrt{a-1}. By direct calculation we see that

φ​(x​yβˆ’y​x)=Ξ±2​(y​x+z​xβˆ’x​yβˆ’x​z)\varphi(xy-yx)=\alpha_{2}(yx+zx-xy-xz)

and

φ​(z​yβˆ’2​x​y+y​z)=Ξ±2​[(Ξ²3βˆ’2)​y​xβˆ’Ξ²3​z​x+Ξ²3​x​yβˆ’(Ξ²3βˆ’2)​x​z].\varphi(zy-2xy+yz)=\alpha_{2}\left[(\beta_{3}-2)yx-\beta_{3}zx+\beta_{3}xy-(\beta_{3}-2)xz\right].

Since Ξ²3β‰ 1\beta_{3}\neq 1, these two images span the same subspace as y​xβˆ’x​zyx-xz and z​xβˆ’x​yzx-xy. We consider φ​(z​xβˆ’a​x2βˆ’b​x​yβˆ’c​y2+x​zβˆ’z2)\varphi(zx-ax^{2}-bxy-cy^{2}+xz-z^{2}) modulo these two relations, and show that it is a nonzero scalar multiple of x2+y2+z2x^{2}+y^{2}+z^{2}. To that end,

φ​(z​xβˆ’z2)\displaystyle\varphi(zx-z^{2}) =(1βˆ’Ξ²3)​(Ξ±1​x+Ξ²3​y+Ξ΄3​z)​(yβˆ’z)\displaystyle=(1-\beta_{3})(\alpha_{1}x+\beta_{3}y+\delta_{3}z)(y-z)
=(1βˆ’Ξ²3)​(Ξ±1​x​yβˆ’Ξ±1​x​z+Ξ²3​y2βˆ’Ξ²3​y​z+Ξ΄3​z​yβˆ’Ξ΄3​z2),\displaystyle=(1-\beta_{3})(\alpha_{1}xy-\alpha_{1}xz+\beta_{3}y^{2}-\beta_{3}yz+\delta_{3}zy-\delta_{3}z^{2}),
φ​(βˆ’a​x2)\displaystyle\varphi(-ax^{2}) =βˆ’a​(Ξ±12​x2+2​α1​x​y+2​α1​x​z+y2+y​z+z​y+z2),\displaystyle=-a(\alpha_{1}^{2}x^{2}+2\alpha_{1}xy+2\alpha_{1}xz+y^{2}+yz+zy+z^{2}),
φ​(βˆ’b​x​y)\displaystyle\varphi(-bxy) =βˆ’b​α2​(Ξ±1​x2+x​z+x​y),\displaystyle=-b\alpha_{2}(\alpha_{1}x^{2}+xz+xy),
φ​(βˆ’c​y2)\displaystyle\varphi(-cy^{2}) =βˆ’c​α22​x2,\displaystyle=-c\alpha_{2}^{2}x^{2},
φ​(x​z)\displaystyle\varphi(xz) =(Ξ±1​x+y+z)​(Ξ±1​x+Ξ²3​y+Ξ΄3​z),\displaystyle=(\alpha_{1}x+y+z)(\alpha_{1}x+\beta_{3}y+\delta_{3}z),
=Ξ±12​x2+Ξ±1​(1+Ξ²3)​x​y+Ξ±1​(1+Ξ΄3)​x​z+Ξ²3​y2+Ξ΄3​y​z\displaystyle=\alpha_{1}^{2}x^{2}+\alpha_{1}(1+\beta_{3})xy+\alpha_{1}(1+\delta_{3})xz+\beta_{3}y^{2}+\delta_{3}yz
+Ξ²3​z​y+Ξ΄3​z2.\displaystyle\quad+\beta_{3}zy+\delta_{3}z^{2}.

Examining the coefficients of the sum of the terms above, and noting that 1βˆ’Ξ²3=Ξ΄3βˆ’11-\beta_{3}=\delta_{3}-1, we see that the coefficients of x​yxy and x​zxz both equal (2βˆ’2​a)​α1βˆ’b​α2(2-2a)\alpha_{1}-b\alpha_{2}, which vanishes by definition of Ξ±1\alpha_{1}. The coefficients of y​zyz and z​yzy both equal Ξ²32βˆ’2​β3+2βˆ’a\beta_{3}^{2}-2\beta_{3}+2-a, which vanishes by definition of Ξ²3\beta_{3}. The coefficients of y2y^{2} and z2z^{2} both equal 2βˆ’2​a2-2a, and the coefficient of x2x^{2} is (1βˆ’a)​α12βˆ’b​α2​α1βˆ’c​α22.(1-a)\alpha_{1}^{2}-b\alpha_{2}\alpha_{1}-c\alpha_{2}^{2}. Using the definitions of Ξ±1\alpha_{1} and Ξ±2\alpha_{2}, it is straightforward to show this expression also equals 2βˆ’2​a2-2a.

The proof of (2) is similar. Let Ξ΄1=b2​(1βˆ’a)\delta_{1}=\dfrac{b}{2(1-a)}. Define a graded algebra homomorphism Ο†:π•‚β€‹βŸ¨x,y,zβŸ©β†’π•‚β€‹βŸ¨x,y,z⟩\varphi:\mathbb{K}\langle x,y,z\rangle\to\mathbb{K}\langle x,y,z\rangle by

φ​(x)\displaystyle\varphi(x) =Ξ΄1​x+y+z\displaystyle=\delta_{1}x+y+z
φ​(y)\displaystyle\varphi(y) =x\displaystyle=x
φ​(z)\displaystyle\varphi(z) =Ξ΄1​z+(1+aβˆ’1)​x+(1βˆ’aβˆ’1)​y.\displaystyle=\delta_{1}z+(1+\sqrt{a-1})x+(1-\sqrt{a-1})y.

One then checks that this map induces the desired isomorphism Tβ†’UT\to U. The details are left to the reader. ∎

In light of Lemma 4.3 and Proposition 4.5, there are only two isomorphism classes of AS-regular twisted tensor products of reducible type that do not contain Ore-type twisted tensor products. The next result shows these isomorphism classes are distinct, and characterizes their types.

Proposition 4.6.

The algebras UU and Uβ€²U^{\prime} are AS-regular.

  • (1)

    The point scheme of Uβ€²U^{\prime} is a union of a line and an irreducible conic, meeting at two points. The automorphism Οƒ\sigma stabilizes the components and interchanges the intersection points. (type S2β€²S_{2}^{\prime})

  • (2)

    The point scheme of UU is a union of three lines meeting in three points, and Οƒ\sigma interchanges two of the lines, fixing y=0y=0. (type S2S_{2})

In either case, the automorphism Οƒ\sigma has order 2.

Proof.

By Proposition 4.5, both UU and Uβ€²U^{\prime} are isomorphic to case R(iii) algebras, which are all AS-regular by Theorem 4.4.

First consider the algebra Uβ€²U^{\prime}. The associated matrix MM of equation (1) is

[βˆ’z0x00y00βˆ’x0x0y0z0],\begin{bmatrix}-z_{0}&x_{0}&0\\ y_{0}&0&-x_{0}\\ x_{0}&y_{0}&z_{0}\end{bmatrix},

so the point scheme is E=𝒡​(x​(2​y​z+x2))E=\mathcal{Z}(x(2yz+x^{2})), a union of a line and an irreducible conic. The line x=0x=0 intersects the conic 2​y​z+x2=02yz+x^{2}=0 in [0:1:0][0:1:0] and [0:0:1][0:0:1]. The automorphism Οƒ\sigma is given by

Οƒ([x:y:z])={[x:z:y]xβ‰ 0[0:βˆ’z:y]x=0.\sigma([x:y:z])=\begin{cases}[x:z:y]&x\neq 0\\ [0:-z:y]&x=0.\\ \end{cases}

So Οƒ\sigma stabilizes the components of EE, interchanges [0:1:0][0:1:0] and [0:0:1][0:0:1], and has order 2.

Next consider the algebra UU. The matrix MM of equation (1) is

[βˆ’z0x00y00βˆ’x00y0z0],\begin{bmatrix}-z_{0}&x_{0}&0\\ y_{0}&0&-x_{0}\\ 0&y_{0}&z_{0}\end{bmatrix},

thus the point scheme is E=𝒡​(x​y​z)E=\mathcal{Z}(xyz), a union of three lines. The automorphism Οƒ\sigma is given by

Οƒ([0:y:z])\displaystyle\sigma([0:y:z]) =[0:βˆ’z:y]\displaystyle=[0:-z:y]
Οƒ([x:0:z])\displaystyle\sigma([x:0:z]) =[x:z:0]\displaystyle=[x:z:0]
Οƒ([x:y:0])\displaystyle\sigma([x:y:0]) =[x:0:y],\displaystyle=[x:0:y],

so Οƒ\sigma stabilizes x=0x=0 while interchanging y=0y=0 and z=0z=0. The automorphism Οƒ\sigma has order 2. ∎

4.2. Twisted tensor products from cases R(i), R(iv), R(vi)

Recall that, as noted above, none of the reducible-type algebras in cases R(i), R(iv) and R(vi) are AS-regular. It appears that the algebras in each respective case may depend, even up to isomorphism, on two parameters. However, we show that, up to isomorphism, the algebras in cases R(i), R(iv) and R(vi) constitute a 1-parameter family of algebras and two isolated algebras.

Lemma 4.7.

Any twisted tensor product from case R(vi) is isomorphic to an algebra from case R(i) or case R(iv).

Proof.

The defining relations of a twisted tensor product TT from case R(vi) are

x​yβˆ’y​x,z​yβˆ’B​x​yβˆ’C​y2,z​xβˆ’a​x2βˆ’b​x​yβˆ’c​y2βˆ’y​zβˆ’z2,xy-yx,zy-Bxy-Cy^{2},zx-ax^{2}-bxy-cy^{2}-yz-z^{2},

where a=B​(1βˆ’B)a=B(1-B), b=Cβˆ’Bβˆ’2​B​Cb=C-B-2BC, c=βˆ’C​(1+C)c=-C(1+C). The map fixing xx and yy, sending z↦z+C​yz\mapsto z+Cy is an isomorphism from TT to the algebra Tβ€²T^{\prime} with relations

x​yβˆ’y​x,z​yβˆ’B​x​y,z​xβˆ’a​x2+B​(1+C)​x​yβˆ’(1+C)​y​zβˆ’z2.xy-yx,zy-Bxy,zx-ax^{2}+B(1+C)xy-(1+C)yz-z^{2}.

If C=βˆ’1C=-1, this algebra belongs to case R(i) (d=0d=0). Otherwise, the map sending y↦y/(1+C)y\mapsto y/(1+C), z↦zβˆ’yz\mapsto z-y and fixing xx is an isomorphism from Tβ€²T^{\prime} to an algebra from case R(iv) (d=0d=0). ∎

For d,B,qβˆˆπ•‚d,B,q\in\mathbb{K} we define

T(i)​(d,B)=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​y,(1βˆ’B)​z​xβˆ’(d+B)​x​zβˆ’z2⟩,\displaystyle T_{(i)}(d,B)=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zy,(1-B)zx-(d+B)xz-z^{2}\rangle,
T(i​v)​(d,B)=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​y,(1βˆ’B)​z​xβˆ’(d+B)​x​zβˆ’y​zβˆ’z2⟩,\displaystyle T_{(iv)}(d,B)=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zy,(1-B)zx-(d+B)xz-yz-z^{2}\rangle,
R​(q)=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​y,q​z​xβˆ’x​zβˆ’z2⟩,\displaystyle R(q)=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zy,qzx-xz-z^{2}\rangle,
R0=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​y,z​xβˆ’z2⟩,\displaystyle R_{0}=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zy,zx-z^{2}\rangle,
R1=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​y,z​xβˆ’y​zβˆ’z2⟩.\displaystyle R_{1}=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zy,zx-yz-z^{2}\rangle.

We omit the straightforward verification of the following lemma.

Lemma 4.8.

As graded algebras, R​(q)β‰…R​(qβ€²)R(q)\cong R(q^{\prime}) if and only if q=qβ€²q=q^{\prime}. Furthermore, for all qβˆˆπ•‚q\in\mathbb{K}, the algebras R​(q)R(q), R0R_{0} and R1R_{1} are pairwise non-isomorphic.

We note that for any Ξ»βˆˆπ•‚\lambda\in\mathbb{K}, Ξ»β‰ 0\lambda\neq 0, R1β‰…π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​y,z​xβˆ’Ξ»β€‹y​zβˆ’z2⟩,R_{1}\cong\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zy,zx-\lambda yz-z^{2}\rangle, so one could also view R0R_{0} and R1R_{1} as members of a 1-parameter flat family.

Proposition 4.9.

An algebra TT is a twisted tensor product from case R(i) or R(iv) if and only if it is isomorphic as a graded algebra to one of R​(q)R(q), qβˆˆπ•‚q\in\mathbb{K}, R0R_{0}, or R1R_{1}.

Proof.

First, let TT be a twisted tensor product from case R(i) or case R(iv). If TT is from case R(i), then the map that fixes xx and yy and sends z↦B​x+zz\mapsto Bx+z is an isomorphism Tβ†’T(i)​(d,B)T\to T_{(i)}(d,B). If TT is from case R(iv), then the map that fixes xx and yy and sends z↦B​x+y+zz\mapsto Bx+y+z is an isomorphism Tβ†’T(i​v)​(d,B)T\to T_{(iv)}(d,B).

If B+dβ‰ 0B+d\neq 0, the map given by x↦x+yx\mapsto x+y, yβ†¦βˆ’(d+B)​yy\mapsto-(d+B)y, z↦zz\mapsto z is an isomorphism T(i​v)​(d,B)β†’T(i)​(d,B)T_{(iv)}(d,B)\rightarrow T_{(i)}(d,B). Rescaling xx by 1/(d+B)1/(d+B) and fixing yy and zz gives an isomorphism between T(i)T_{(i)} and R​(q)R(q), where q=(1βˆ’B)/(B+d)q=(1-B)/(B+d).

If B+d=0B+d=0, the requirement that a=B​(1βˆ’dβˆ’B)a=B(1-d-B) implies a=Ba=B, and since aβ‰ 1a\neq 1, it follows that Bβ‰ 1B\neq 1. Then one sees that T(i)​(d,B)β‰…R0T_{(i)}(d,B)\cong R_{0} and T(i​v)​(d,B)β‰…R1T_{(iv)}(d,B)\cong R_{1} by isomorphisms fixing yy and zz and sending x↦(1/(1βˆ’B))​xx\mapsto(1/(1-B))x.

For the converse, we first note that by [4, Lemma 3.3], fn​(a,βˆ’a)=(1βˆ’a)nf_{n}(a,-a)=(1-a)^{n} for all nβ‰₯0n\geq 0. Thus choosing a=βˆ’dβ‰ 1a=-d\neq 1 guarantees (a,d)(a,d) is not a zero of any fn​(t,u)f_{n}(t,u). Now it is clear that R0R_{0} and R1R_{1} are isomorphic to case R(i) and R(iv) twisted tensor products where, for example, a=B=βˆ’d=0a=B=-d=0. Similarly, R​(0)R(0) is isomorphic to a twisted tensor product from case R(i) where B=1B=1 and a=d=0a=d=0.

If qβˆˆπ•‚βˆ—q\in\mathbb{K}^{*}, put d=1/qd=1/q and a=B=0a=B=0. One can show that in this case fn​(a,d)=1f_{n}(a,d)=1 for all nβ‰₯0n\geq 0, so there exists a case R(i) twisted tensor product isomorphic to R​(q)R(q). ∎

We conclude this section with the proof of Theorem 4.1.

Proof of Theorem 4.1.

By Lemma 4.3(2,3), the algebras in cases R(ii) and R(vii) are isomorphic to Ore-type twisted tensor products. Lemma 4.3(1) and Lemma 4.7 imply that among the remaining cases, it suffices to classify R(i), R(iii), and R(iv).

Proposition 4.5 shows that every algebra in case R(iii) is isomorphic to UU or Uβ€²U^{\prime}. Proposition 4.6 shows these algebras are non-isomorphic and AS-regular, and identifies their types as S2S_{2} and S2β€²S_{2}^{\prime}, respectively.

By [4, Theorem 6.2], no algebras in case R(i) or R(iv) are AS-regular. These algebras are classified up to graded algebra isomorphism as R​(q)R(q), R0R_{0}, or R1R_{1} in Proposition 4.9, and are pairwise non-isomorphic by Lemma 4.8. ∎

5. Ore-type twisted tensor products

In this section, let TT denote a quadratic twisted tensor product of Ore type, in normal form. The results below classify TT up to isomorphism of graded algebras. If TT is AS-regular, we identify its type, as in [5]. We continue to assume char​𝕂≠2{\rm char}\ \mathbb{K}\neq 2.

We begin by recalling the description of Ore-type twisted tensor products from [4]. By [4, Theorem 4.3], Tβ‰…π•‚β€‹βŸ¨x,y,z⟩/IT\cong\mathbb{K}\langle x,y,z\rangle/I where II is the graded ideal of π•‚β€‹βŸ¨x,y,z⟩\mathbb{K}\langle x,y,z\rangle generated by the elements

x​yβˆ’y​x,z​xβˆ’a​x2βˆ’b​x​yβˆ’c​y2βˆ’d​x​zβˆ’e​y​z,z​yβˆ’A​x2βˆ’B​x​yβˆ’C​y2βˆ’D​y​z,xy-yx,zx-ax^{2}-bxy-cy^{2}-dxz-eyz,zy-Ax^{2}-Bxy-Cy^{2}-Dyz,

such that A,e∈{0,1}A,e\in\{0,1\} and a,b,c,d,B,C,Dβˆˆπ•‚a,b,c,d,B,C,D\in\mathbb{K} belong to one of the following cases.

  1. O(1):

    e=0e=0, A∈{0,1}A\in\{0,1\}, and if A=0A=0, then C∈{0,1}C\in\{0,1\}. Furthermore, one of the following holds:

    1. (i)

      d=D=1d=D=1,

    2. (ii)

      d≠1=Dd\neq 1=D, A=B=C=0A=B=C=0,

    3. (iii)

      d=1β‰ Dd=1\neq D, a=b=c=0a=b=c=0,

    4. (iv)

      dβ‰ 1β‰ Dd\neq 1\neq D, A=c=0A=c=0, a=B​(dβˆ’1)/(Dβˆ’1)a=B(d-1)/(D-1), b=C​(dβˆ’1)/(Dβˆ’1)b=C(d-1)/(D-1).

  2. O(2):

    e=1e=1, d=Dd=D and one of the following holds:

    1. (i)

      d=1d=1, A=B=C=0A=B=C=0,

    2. (ii)

      dβ‰ 1d\neq 1, A=0A=0, B=a=(bβˆ’C)​(dβˆ’1)B=a=(b-C)(d-1), c=C/(dβˆ’1)c=C/(d-1).

By [4, Proposition 4.2] every Ore-type twisted tensor product is a graded Ore extension of 𝕂​[x,y]\mathbb{K}[x,y]. If TT is in normal form, T≅𝕂​[x,y]​[z;Ξ½,Ξ΄]T\cong\mathbb{K}[x,y][z;\nu,\delta] where

ν​(x)\displaystyle\nu(x) =d​x+e​y\displaystyle=dx+ey δ​(x)\displaystyle\delta(x) =a​x2+b​x​y+c​y2\displaystyle=ax^{2}+bxy+cy^{2}
ν​(y)\displaystyle\nu(y) =D​y\displaystyle=Dy δ​(y)\displaystyle\delta(y) =A​x2+B​x​y+C​y2.\displaystyle=Ax^{2}+Bxy+Cy^{2}.
Theorem 5.1.

An Ore-type twisted tensor product TT is semi-standard, and the following are equivalent.

  1. (1)

    TT is nondegenerate,

  2. (2)

    TT is AS-regular,

  3. (3)

    Ξ½\nu is invertible.

To facilitate the proof, and for use below, we record the matrices MM and NN of equation (1) of Section 2 and their determinants for an Ore-type twisted tensor product.

M=[βˆ’y0x00z0βˆ’a​x0βˆ’b​x0βˆ’c​y0βˆ’d​x0βˆ’e​y0βˆ’A​x0z0βˆ’B​x0βˆ’C​y0βˆ’D​y0]M=\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}-ax_{0}&-bx_{0}-cy_{0}&-dx_{0}-ey_{0}\\ -Ax_{0}&z_{0}-Bx_{0}-Cy_{0}&-Dy_{0}\end{bmatrix}
N=[y1βˆ’a​x1βˆ’b​y1βˆ’d​z1βˆ’A​x1βˆ’B​y1βˆ’x1βˆ’c​y1βˆ’e​z1βˆ’C​y1βˆ’D​z10x1y1]N=\begin{bmatrix}y_{1}&-ax_{1}-by_{1}-dz_{1}&-Ax_{1}-By_{1}\\ -x_{1}&-cy_{1}-ez_{1}&-Cy_{1}-Dz_{1}\\ 0&x_{1}&y_{1}\end{bmatrix}
detM\displaystyle\det M =d​A​x3+(d​B+e​Aβˆ’a​D)​x2​y+(e​B+d​Cβˆ’b​D)​x​y2\displaystyle=dAx^{3}+(dB+eA-aD)x^{2}y+(eB+dC-bD)xy^{2}
+(e​Cβˆ’c​D)​y3+(Dβˆ’d)​x​y​zβˆ’e​y2​z\displaystyle\quad+(eC-cD)y^{3}+(D-d)xyz-ey^{2}z
detN\displaystyle\det N =A​x3+(Bβˆ’a)​x2​y+(Cβˆ’b)​x​y2βˆ’c​y3+(Dβˆ’d)​x​y​zβˆ’e​y2​z\displaystyle=Ax^{3}+(B-a)x^{2}y+(C-b)xy^{2}-cy^{3}+(D-d)xyz-ey^{2}z
Proof.

The fact that TT is semi-standard, that is, detM=k​detN\det M=k\det N for some kβˆˆπ•‚βˆ—k\in\mathbb{K}^{*}, is easily verified in each case listed above.

The statement (3)β‡’\Rightarrow(2) follows from [4, Theorem 6.2(i)], and (2)β‡’\Rightarrow(1) is [1, Theorem 5.1]. Thus it suffices to prove (1)β‡’\Rightarrow(3).

If either xx or yy is nonzero, then NN clearly has rank 2. If x=y=0x=y=0, then we may assume z=1z=1 and NN becomes

[0βˆ’d00βˆ’eβˆ’D000]\begin{bmatrix}0&-d&0\\ 0&-e&-D\\ 0&0&0\end{bmatrix}

which has rank 2 if and only if d​Dβ‰ 0dD\neq 0. This condition implies the endomorphism Ξ½:𝕂​[x,y]→𝕂​[x,y]\nu:\mathbb{K}[x,y]\to\mathbb{K}[x,y] is bijective in degree 1, so Ξ½\nu is an isomorphism. ∎

The analysis of the cases O(1)(i,ii,iii,iv), O(2)(i,ii) is more involved than for the reducible-type twisted tensor products of Section 4. Consequently, following two preliminary results, this section is divided into four subsections. Our classification results are summarized in Table 3, and in the following theorem. Double lines in Table 3 delineate the four subsections.

Table 3. Mapping of Ore-type TTP cases
TTP Case Subcase Algebra Condition IM-type
O(1)(i)
A=0β‰ Bβˆ’aA=0\neq B-a
(Cβˆ’b)2β‰ 4​c​(aβˆ’B)(C-b)^{2}\neq 4c(a-B)
T​(Ξ±,Ξ²,Ξ³)βˆ—T(\alpha,\beta,\gamma)^{*} Ξ±+Ξ²+Ξ³β‰ 0\alpha+\beta+\gamma\neq 0 T1T_{1}
A=0β‰ Bβˆ’aA=0\neq B-a (Cβˆ’b)2=4​c​(aβˆ’B)(C-b)^{2}=4c(a-B) W​(Ξ³,Ο΅)W(\gamma,\epsilon) Ο΅=0\epsilon=0 W​L2WL_{2}
Ο΅=1\epsilon=1 W​L3WL_{3}
A=0A=0 a=Ba=B Cβˆ’b=0β‰ cC-b=0\neq c a=b=0a=b=0 aβ‰ 0a\neq 0 a=0β‰ ba=0\neq b L​(0,0)L(0,0) T​L1TL_{1}
L​(1,0)L(1,0) T​L2TL_{2}
L​(0,1)L(0,1) T​L4TL_{4}
A=0=Bβˆ’aA=0=B-a Cβˆ’b=0=cC-b=0=c P​(Ο΅)P(\epsilon) Ο΅=1\epsilon=1 P2P_{2}
P​(Ο΅)P(\epsilon) Ο΅=0\epsilon=0 P1P_{1}
O(1)(iv) C=0C=0 S​(d,D)βˆ—βˆ—S(d,D)^{**} d=Dβˆ‰{0,1}d=D\notin\{0,1\}
d​D=0dD=0 not AS-regular
dβ‰ Dd\neq D, d,Dβˆ‰{0,1}d,D\notin\{0,1\} S1S_{1}
O(1)(ii) S′​(d,Ο΅)S^{\prime}(d,\epsilon) dβ‰ 0=Ο΅d\neq 0=\epsilon
d≠0d\neq 0, ϡ=1\epsilon=1 S1′S^{\prime}_{1}
d=0d=0 not AS-regular
O(2)(i) a≠0a\neq 0 WW T′T^{\prime}
O(2)(ii) W​(d)W(d) dβˆ‰{0,1}d\notin\{0,1\} W​L1WL_{1}
d=0d=0 not AS-regular

*isomorphism classes of T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma) are parametrized by points [Ξ±:Ξ²:Ξ³]βˆˆβ„™2[\alpha:\beta:\gamma]\in{\mathbb{P}}^{2} up to permutation of coordinates.

**isomorphism classes of S​(d,D)S(d,D) are parametrized by pairs (d,D)(d,D) up to permutation of coordinates.

Theorem 5.2.

Every Ore-type twisted tensor product is isomorphic as a graded algebra to one of the algebras listed in Table 3. The algebras listed in Table 3 are AS-regular and are pairwise non-isomorphic, except as noted. The table gives the types of the AS-regular algebras.

The proof of Theorem 5.2 can be found at the end of this section.

Remark 5.3.

Comparing the algebras listed in Table 3 with those of [5, Theorem 3.1] shows that when char​𝕂=0{\rm char}\ \mathbb{K}=0, all algebras of types T1,W​L2,W​L3,T_{1},WL_{2},WL_{3}, and T​L4TL_{4} are isomorphic to Ore-type twisted tensor products of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z].

We begin our classification of Ore-type twisted tensor products up to graded algebra isomorphism with case O(1). Recall that case O(1) has e=0e=0. We start with a few simple observations.

Lemma 5.4.
  1. (1)

    Any twisted tensor product from case O(1)(iii) is isomorphic as a graded algebra to one from case O(1)(ii).

  2. (2)

    Any twisted tensor product from case O(1)(iv) is isomorphic to one from case O(1)(iv) with C=0C=0.

Proof.

Given a twisted tensor product from case O(1)(iii), the isomorphism that interchanges xx and yy and fixes zz yields an algebra from case O(1)(ii).

Given an algebra from case O(1)(iv) with C=1C=1, the isomorphism that fixes xx and yy and maps z↦z+y/(1βˆ’D)z\mapsto z+y/(1-D) yields an algebra from case O(1)(iv) with C=0C=0. ∎

5.1. Twisted tensor products from case O(1)(iv)

For d,Dβˆˆπ•‚d,D\in\mathbb{K}, dβ‰ 1β‰ Dd\neq 1\neq D, define

S​(d,D)=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​xβˆ’d​x​z,z​yβˆ’D​y​z⟩.S(d,D)=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zx-dxz,zy-Dyz\rangle.

The definition of S​(d,D)S(d,D) obviously makes sense for all values of dd and DD. The restrictions are imposed to avoid redundancies with other families of algebras defined below, and to align with the values permitted in the corresponding case O(1)(iv).

Proposition 5.5.

Any twisted tensor product from case O(1)(iv) is isomorphic as a graded algebra to an algebra from the family S​(d,D)S(d,D). Conversely, S​(d,D)S(d,D) is a twisted tensor product belonging to case O(1)(iv).

Proof.

Given a twisted tensor product TT from case O(1)(iv), by Lemma 5.4, we may assume C=0C=0, so the relations of TT are

x​yβˆ’y​x,z​xβˆ’a​x2βˆ’d​x​z,z​yβˆ’B​x​yβˆ’D​y​z,xy-yx,zx-ax^{2}-dxz,zy-Bxy-Dyz,

where a​(Dβˆ’1)=B​(dβˆ’1)a(D-1)=B(d-1). In this case, dβ‰ 1β‰ Dd\neq 1\neq D. The map that fixes xx and yy, and sends zz to λ​x+z\lambda x+z where Ξ»=a1βˆ’d=B1βˆ’D\lambda=\dfrac{a}{1-d}=\dfrac{B}{1-D} is an isomorphism from TT to S​(d,D)S(d,D). The converse is immediate from the description of case O(1)(iv). ∎

Proposition 5.6.

The algebra S​(d,D)S(d,D) is AS-regular if and only if d​Dβ‰ 0dD\neq 0. When S​(d,D)S(d,D) is AS-regular, the point scheme EE and associated automorphism Οƒ\sigma are as follows.

  • (1)

    If d=Dd=D, E=β„™2E={\mathbb{P}}^{2} and the automorphism Οƒ\sigma is diagonal. (type P1P_{1})

  • (2)

    If d≠Dd\neq D, EE is the union of three distinct lines, and the automorphism σ\sigma stabilizes these lines. (type S1S_{1})

In either case, the order of Οƒ\sigma is the least common multiple of the orders of d,Dβˆˆπ•‚βˆ—d,D\in\mathbb{K}^{*}.

Moreover, the algebras S​(d,D)S(d,D) and S​(dβ€²,Dβ€²)S(d^{\prime},D^{\prime}) are graded isomorphic if and only if (dβ€²,Dβ€²)∈{(d,D),(D,d)}(d^{\prime},D^{\prime})\in\{(d,D),(D,d)\}.

Proof.

The statement that S​(d,D)S(d,D) is AS-regular if and only if d​Dβ‰ 0dD\neq 0 follows from Proposition 5.5 and Theorem 5.1. The matrix MM for S​(d,D)S(d,D) is

[βˆ’y0x00z00βˆ’d​x00z0βˆ’D​y0].\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}&0&-dx_{0}\\ 0&z_{0}&-Dy_{0}\end{bmatrix}.

The point scheme of S​(d,D)S(d,D) is E=𝒡​((Dβˆ’d)​x​y​z)E=\mathcal{Z}((D-d)xyz), which is reduced, and the automorphism Οƒ\sigma is given by

Οƒ([x:y:z])={[d​x:d​y:z]xβ‰ 0[0:D​y:z]x=0.\sigma([x:y:z])=\begin{cases}[dx:dy:z]&x\neq 0\\ [0:Dy:z]&x=0\\ \end{cases}.

Statements (1), (2) and the statement regarding the order of Οƒ\sigma are now clear.

The characterization of graded algebra isomorphism classes of the S​(d,D)S(d,D) is a special case of [7, Example 4.10], so the proof is omitted. ∎

5.2. Twisted tensor products from cases O(1)(ii), O(1)(iii)

By Lemma 5.4 (1) there is no loss of generality in analyzing case O(1)(ii). For Ο΅,dβˆˆπ•‚\epsilon,d\in\mathbb{K} such that ϡ∈{0,1}\epsilon\in\{0,1\} and dβ‰ 1d\neq 1, we define:

S′​(d,Ο΅)=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​yβˆ’y​z,z​xβˆ’d​x​z+ϡ​y2⟩.S^{\prime}(d,\epsilon)=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zy-yz,zx-dxz+\epsilon y^{2}\rangle.

As in the preceding subsection, we have imposed a restriction on dd to avoid redundancy and to align with the values permitted in the corresponding case.

Proposition 5.7.

Any twisted tensor product from case O(1)(ii) is isomorphic as a graded algebra to an algebra from the family S′​(d,Ο΅)S^{\prime}(d,\epsilon). Conversely, S′​(d,Ο΅)S^{\prime}(d,\epsilon) is a twisted tensor product belonging to case O(1)(ii).

Proof.

Given a twisted tensor product TT from case O(1)(ii), the relations of TT are

x​yβˆ’y​x,z​yβˆ’y​z,z​xβˆ’a​x2βˆ’b​x​yβˆ’c​y2βˆ’d​x​z,xy-yx,zy-yz,zx-ax^{2}-bxy-cy^{2}-dxz,

where dβ‰ 1d\neq 1. The graded algebra map which fixes xx and yy and sends zz to λ​x+μ​y+z\lambda x+\mu y+z, where Ξ»=a1βˆ’d\lambda=\dfrac{a}{1-d} and ΞΌ=b1βˆ’d\mu=\dfrac{b}{1-d}, is an isomorphism from TT to the algebra with relations x​yβˆ’y​x,z​yβˆ’y​z,z​xβˆ’d​x​z+c​y2xy-yx,zy-yz,zx-dxz+cy^{2}. If cβ‰ 0c\neq 0, rescaling yy yields the algebra S′​(d,1)S^{\prime}(d,1). The converse is immediate from the description of case O(1)(ii). ∎

Proposition 5.8.

An algebra S′​(d,Ο΅)S^{\prime}(d,\epsilon) is AS-regular if and only if dβ‰ 0d\neq 0. If S′​(d,Ο΅)S^{\prime}(d,\epsilon) is AS-regular, then the point scheme EE and associated automorphism Οƒ\sigma are as follows.

  • (1)

    If Ο΅=0\epsilon=0, EE is a union of three distinct lines, and Οƒ\sigma stabilizes the components. (type S1S_{1})

  • (2)

    If Ο΅β‰ 0\epsilon\neq 0, EE is a union of a line and a conic meeting at two points, and Οƒ\sigma stabilizes the components and the intersection points. (type S1β€²S^{\prime}_{1})

In either case, the order of Οƒ\sigma is the order of dβˆˆπ•‚βˆ—d\in\mathbb{K}^{*}.

The algebras S′​(d,Ο΅)S^{\prime}(d,\epsilon) and S′​(dβ€²,Ο΅β€²)S^{\prime}(d^{\prime},\epsilon^{\prime}) are isomorphic if and only if Ο΅β€²=Ο΅\epsilon^{\prime}=\epsilon and dβ€²=dd^{\prime}=d or, when dβ‰ 0d\neq 0, dβ€²=dβˆ’1d^{\prime}=d^{-1}. Moreover, S′​(d,0)S^{\prime}(d,0) is not isomorphic to an algebra belonging to the family S​(dβ€²,Dβ€²)S(d^{\prime},D^{\prime}).

Proof.

By definition of S′​(d,Ο΅)S^{\prime}(d,\epsilon), the matrix MM is

[βˆ’y0x00z0ϡ​y0βˆ’d​x00z0βˆ’y0].\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}&\epsilon y_{0}&-dx_{0}\\ 0&z_{0}&-y_{0}\end{bmatrix}.

Proposition 5.7 and Theorem 5.1 imply that S′​(d,Ο΅)S^{\prime}(d,\epsilon) is AS-regular if and only if dβ‰ 0d\neq 0. In this case the point scheme is E=𝒡​((1βˆ’d)​x​y​z+ϡ​y3)E=\mathcal{Z}((1-d)xyz+\epsilon y^{3}), which is reduced since dβ‰ 1d\neq 1, and the automorphism Οƒ\sigma is given by

Οƒ([x:y:z])={[x:y:z]yβ‰ 0[d​x:0:z]y=0.\sigma([x:y:z])=\begin{cases}[x:y:z]&y\neq 0\\ [dx:0:z]&y=0\\ \end{cases}.

The description of the point scheme of S′​(d,Ο΅)S^{\prime}(d,\epsilon) and the automorphism Οƒ\sigma follows.

Next, we characterize S′​(d,Ο΅)S^{\prime}(d,\epsilon) up to graded algebra isomorphism. For the β€œif” part of the statement, observe that if dβ‰ 0d\neq 0, then S′​(d,Ο΅)β‰…S′​(dβˆ’1,Ο΅)S^{\prime}(d,\epsilon)\cong S^{\prime}(d^{-1},\epsilon) via the isomorphism given by switching xx and zz and rescaling yβ†¦βˆ’d​yy\mapsto\sqrt{-d}y.

Conversely, suppose S′​(d,Ο΅)β‰…S′​(dβ€²,Ο΅β€²)S^{\prime}(d,\epsilon)\cong S^{\prime}(d^{\prime},\epsilon^{\prime}). Since S′​(d,Ο΅)S^{\prime}(d,\epsilon) is AS-regular if and only if dβ‰ 0d\neq 0, we need only consider two cases: d​dβ€²β‰ 0dd^{\prime}\neq 0 and d=dβ€²=0d=d^{\prime}=0. First assume d​dβ€²β‰ 0dd^{\prime}\neq 0 so S′​(d,Ο΅)S^{\prime}(d,\epsilon) and S′​(dβ€²,Ο΅β€²)S^{\prime}(d^{\prime},\epsilon^{\prime}) are AS-regular of dimension 3, and thus are geometric algebras. By considering types, the first part of the Proposition implies Ο΅=Ο΅β€²\epsilon=\epsilon^{\prime}.

Let ψ:β„™2β†’β„™2\psi:{\mathbb{P}}^{2}\to{\mathbb{P}}^{2} be an automorphism such that Οˆβ€‹Οƒ=Οƒβ€²β€‹Οˆ.\psi\sigma=\sigma^{\prime}\psi. Since dβ‰ 1d\neq 1, Οƒ\sigma and Οƒβ€²\sigma^{\prime} restrict to non-identity maps on y=0y=0. As Οƒ\sigma and Οƒβ€²\sigma^{\prime} are the identity when yβ‰ 0y\neq 0, ψ\psi stabilizes the y=0y=0 component.

Let [ψi​j]∈G​L3[\psi_{ij}]\in GL_{3} be a matrix representing ψ\psi, up to scaling. Since ψ\psi stabilizes the line y=0y=0, we have ψ21=ψ23=0\psi_{21}=\psi_{23}=0. Since Οƒ\sigma and Οƒβ€²\sigma^{\prime} fix [1:0:0][1:0:0] and [0:0:1][0:0:1], the condition Οˆβ€‹Οƒ=Οƒβ€²β€‹Οˆ\psi\sigma=\sigma^{\prime}\psi implies

[dβ€²Οˆ11:0:ψ31]=[ψ11:0:ψ31]and[dβ€²Οˆ13:0:ψ33]=[ψ13:0:ψ33].[d^{\prime}\psi_{11}:0:\psi_{31}]=[\psi_{11}:0:\psi_{31}]\quad\text{and}\quad[d^{\prime}\psi_{13}:0:\psi_{33}]=[\psi_{13}:0:\psi_{33}].

Since dβ€²β‰ 1d^{\prime}\neq 1, we have ψ11β€‹Οˆ31=ψ13β€‹Οˆ33=0\psi_{11}\psi_{31}=\psi_{13}\psi_{33}=0, and since ψ\psi is invertible, we have ψ11β€‹Οˆ33β‰ Οˆ13β€‹Οˆ31\psi_{11}\psi_{33}\neq\psi_{13}\psi_{31}. So either ψ11=ψ33=0\psi_{11}=\psi_{33}=0 or ψ13=ψ31=0\psi_{13}=\psi_{31}=0. In the former case, ψ13β‰ 0β‰ Οˆ31\psi_{13}\neq 0\neq\psi_{31}, and evaluating Οˆβ€‹Οƒ=Οƒβ€²β€‹Οˆ\psi\sigma=\sigma^{\prime}\psi at [1:0:1][1:0:1] yields

[ψ13:0:dψ31]=[dβ€²Οˆ13:0:ψ31],[\psi_{13}:0:d\psi_{31}]=[d^{\prime}\psi_{13}:0:\psi_{31}],

whence dβ€²=dβˆ’1d^{\prime}=d^{-1}. A similar argument in the case ψ13=ψ31=0\psi_{13}=\psi_{31}=0 yields d=dβ€²d=d^{\prime}. This completes the characterization of S′​(d,Ο΅)S^{\prime}(d,\epsilon) in the case d​dβ€²β‰ 0dd^{\prime}\neq 0.

For the case d=dβ€²=0d=d^{\prime}=0, note that the relation z​x=0zx=0 holds in S′​(0,0)S^{\prime}(0,0). It is easy to check that products of linear elements in S′​(0,1)S^{\prime}(0,1) are always nonzero, hence S′​(0,Ο΅)β‰…S′​(0,Ο΅β€²)S^{\prime}(0,\epsilon)\cong S^{\prime}(0,\epsilon^{\prime}) implies Ο΅=Ο΅β€²\epsilon=\epsilon^{\prime}.

Finally, observe that if the definition of S​(d,D)S(d,D) is extended to allow D=1D=1, then S′​(d,0)=S​(d,1)S^{\prime}(d,0)=S(d,1). The fact that S′​(d,0)≇S​(dβ€²,Dβ€²)S^{\prime}(d,0)\ncong S(d^{\prime},D^{\prime}) for Dβ€²β‰ 1D^{\prime}\neq 1 is therefore a consequence of [7, Example 4.10]. ∎

5.3. Twisted tensor products from case O(1)(i)

Among the algebras from case O(1), it remains to consider case O(1)(i). Recall that in this case d=D=1d=D=1; that is, the ring endomorphism Ξ½\nu defining the Ore-extension TT is the identity. So, by Theorem 5.1, the algebra TT is AS-regular. As such, the classification in this case is aided by consideration of the possible point schemes. The following reduction simplifies the point scheme calculations.

Lemma 5.9.

Any twisted tensor product from case O(1)(i) is isomorphic to one from case O(1)(i) with A=0A=0.

Proof.

Suppose TT is a twisted tensor product from case O(1)(i) with A=1A=1. Let p​(t)=c​t3+(bβˆ’C)​t2+(aβˆ’B)​tβˆ’1βˆˆπ•‚β€‹[t]p(t)=ct^{3}+(b-C)t^{2}+(a-B)t-1\in\mathbb{K}[t].

If p​(t)p(t) is non-constant, let Ξ»βˆˆπ•‚\lambda\in\mathbb{K} be a zero of p​(t)p(t). Then the linear map x↦xx\mapsto x, y↦λ​x+yy\mapsto\lambda x+y, z↦zz\mapsto z determines an isomorphism of TT with Tβ€²=π•‚β€‹βŸ¨x,y,z⟩/Iβ€²T^{\prime}=\mathbb{K}\langle x,y,z\rangle/I^{\prime} where Iβ€²I^{\prime} is generated by

x​yβˆ’y​x,z​xβˆ’(a+b​λ+c​λ2)​x2βˆ’(b+2​c​λ)​x​yβˆ’c​y2βˆ’x​z,xy-yx,zx-(a+b\lambda+c\lambda^{2})x^{2}-(b+2c\lambda)xy-cy^{2}-xz,
z​yβˆ’(B+(2​Cβˆ’b)β€‹Ξ»βˆ’2​c​λ2)​x​yβˆ’(Cβˆ’c​λ)​y2βˆ’y​z.zy-(B+(2C-b)\lambda-2c\lambda^{2})xy-(C-c\lambda)y^{2}-yz.

Rescaling yy, if necessary, this presentation satisfies the conditions of case O(1)(i).

If p​(t)p(t) is constant, then c=bβˆ’C=aβˆ’B=0c=b-C=a-B=0. Interchanging xx and yy yields the isomorphic algebra with relations

x​yβˆ’y​x,z​xβˆ’b​x2βˆ’a​x​yβˆ’y2βˆ’x​z,z​yβˆ’b​x​yβˆ’a​y2βˆ’y​z.xy-yx,zx-bx^{2}-axy-y^{2}-xz,zy-bxy-ay^{2}-yz.

Rescaling yy if necessary, this presentation satisfies the conditions of case O(1)(i). ∎

If TT is an algebra from case O(1)(i) with A=0A=0, then the point scheme of TT is

E=𝒡​(y​[(Bβˆ’a)​x2+(Cβˆ’b)​x​yβˆ’c​y2]).E=\mathcal{Z}(y\left[(B-a)x^{2}+(C-b)xy-cy^{2}\right]).

The automorphism Οƒ\sigma is given by

Οƒ([x:y:z])={[x:y:z+B​x+C​y]yβ‰ 0[x:0:a​x+z]y=0.\sigma([x:y:z])=\begin{cases}[x:y:z+Bx+Cy]&y\neq 0\\ [x:0:ax+z]&y=0\\ \end{cases}.

We see that whenever EE consists of multiple components, the automorphism Οƒ\sigma stabilizes the components, and the components intersect in a single point [0:0:1][0:0:1].

When the quadratic form

Q​(x,y)=(Bβˆ’a)​x2+(Cβˆ’b)​x​yβˆ’c​y2Q(x,y)=(B-a)x^{2}+(C-b)xy-cy^{2}

is a product of distinct linear factors, EE is either a union of three lines (when a≠Ba\neq B), or the union of the double line y2=0y^{2}=0 and another line. We describe the three line case next.

For Ξ±,Ξ²,Ξ³βˆˆπ•‚\alpha,\beta,\gamma\in\mathbb{K} such that Ξ±+Ξ²+Ξ³β‰ 0\alpha+\beta+\gamma\neq 0, define

T​(Ξ±,Ξ²,Ξ³)=π•‚β€‹βŸ¨x,y,z⟩⟨x​yβˆ’y​x,x​zβˆ’z​xβˆ’Ξ²β€‹x2+(Ξ²+Ξ³)​x​y,y​zβˆ’z​yβˆ’Ξ±β€‹y2+(Ξ±+Ξ³)​x​y⟩.T(\alpha,\beta,\gamma)=\dfrac{\mathbb{K}\langle x,y,z\rangle}{\langle xy-yx,xz-zx-\beta x^{2}+(\beta+\gamma)xy,yz-zy-\alpha y^{2}+(\alpha+\gamma)xy\rangle}.
Proposition 5.10.

An algebra TT is a twisted tensor product from case O(1)(i) with A=0A=0 and Bβˆ’aβ‰ 0β‰ (Cβˆ’b)2βˆ’4​c​(aβˆ’B)B-a\neq 0\neq(C-b)^{2}-4c(a-B) if and only if TT is isomorphic to an algebra from the family T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma).

Proof.

Suppose TT is an algebra as hypothesized in the statement. Choose Οβˆˆπ•‚\rho\in\mathbb{K} such that (aβˆ’B)2+(4​(aβˆ’B)​cβˆ’(bβˆ’C)2)​ρ2=0(a-B)^{2}+(4(a-B)c-(b-C)^{2})\rho^{2}=0 and let Ξ»=Bβˆ’a+(bβˆ’C)​ρ2​(Bβˆ’a)\lambda=\dfrac{B-a+(b-C)\rho}{2(B-a)}. Then x↦x+λ​yx\mapsto x+\lambda y, y↦ρ​yy\mapsto\rho y, z↦zz\mapsto z determines an isomorphism from TT to an algebra T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma) where Ξ±=βˆ’(C​ρ+B​λ)\alpha=-(C\rho+B\lambda), Ξ²=βˆ’a\beta=-a, and Ξ³=B​(1+Ξ»)+C​ρ\gamma=B(1+\lambda)+C\rho.

Conversely, it is straightforward to check that when Ξ±+Ξ²+Ξ³β‰ 0\alpha+\beta+\gamma\neq 0, the algebra T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma) belongs to case O(1)(i) and satisfies the stated conditions. ∎

Proposition 5.11.

The algebra T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma) is AS-regular. The point scheme of T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma) is a union of three distinct lines meeting at a point. The automorphism Οƒ\sigma stabilizes the components (type T1T_{1}), and the order of Οƒ\sigma is the least common multiple of the additive orders of Ξ±,Ξ²,Ξ³\alpha,\beta,\gamma in 𝕂\mathbb{K}.

Moreover, T​(Ξ±,Ξ²,Ξ³)β‰…T​(Ξ±β€²,Ξ²β€²,Ξ³β€²)T(\alpha,\beta,\gamma)\cong T(\alpha^{\prime},\beta^{\prime},\gamma^{\prime}) if and only if the coordinates of the point [Ξ±β€²:Ξ²β€²:Ξ³β€²]βˆˆβ„™2[\alpha^{\prime}:\beta^{\prime}:\gamma^{\prime}]\in{\mathbb{P}}^{2} are a permutation of those of [Ξ±:Ξ²:Ξ³][\alpha:\beta:\gamma].

Proof.

As noted above, AS-regularity of T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma) follows from Theorem 5.1, since the automorphism Ξ½\nu is the identity. The matrix MM is

[βˆ’y0x00z0+β​x0βˆ’(Ξ²+Ξ³)​x0βˆ’x0βˆ’(Ξ±+Ξ³)​x0z0+α​x0βˆ’y0],\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}+\beta x_{0}&-(\beta+\gamma)x_{0}&-x_{0}\\ -(\alpha+\gamma)x_{0}&z_{0}+\alpha x_{0}&-y_{0}\end{bmatrix},

so the point scheme of is E=𝒡​((Ξ±+Ξ²+Ξ³)​x​y​(xβˆ’y))E=\mathcal{Z}((\alpha+\beta+\gamma)xy(x-y)), which is reduced, and the automorphism is

Οƒ([0:y:z])\displaystyle\sigma([0:y:z]) =[0:y:z+Ξ±y]\displaystyle=[0:y:z+\alpha y]
Οƒ([x:0:z])\displaystyle\sigma([x:0:z]) =[x:0:z+Ξ²x]\displaystyle=[x:0:z+\beta x]
Οƒ([x:x:z])\displaystyle\sigma([x:x:z]) =[x:x:zβˆ’Ξ³x].\displaystyle=[x:x:z-\gamma x].

Noting that the lines x=0x=0, y=0y=0, and x=yx=y intersect in [0:0:1][0:0:1], the first part of the Corollary follows.

Since the algebras T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma) are AS-regular of dimension 3, they are geometric algebras. Suppose T​(Ξ±,Ξ²,Ξ³)β‰…T​(Ξ±β€²,Ξ²β€²,Ξ³β€²)T(\alpha,\beta,\gamma)\cong T(\alpha^{\prime},\beta^{\prime},\gamma^{\prime}) and let Οƒβ€²\sigma^{\prime} be the automorphism of the point scheme Eβ€²E^{\prime} of T​(Ξ±β€²,Ξ²β€²,Ξ³β€²)T(\alpha^{\prime},\beta^{\prime},\gamma^{\prime}). Then there exists an automorphism ψ:β„™2β†’β„™2\psi:{\mathbb{P}}^{2}\to{\mathbb{P}}^{2} such that Οˆβ€‹Οƒ=Οƒβ€²β€‹Οˆ\psi\sigma=\sigma^{\prime}\psi, and ψ\psi acts by a permutation on the triple of lines (x=0x=0, y=0y=0, x=yx=y). Applying the inverse of this permutation to the triple (Ξ±,Ξ²,Ξ³)(\alpha,\beta,\gamma) yields (Ξ±β€²,Ξ²β€²,Ξ³β€²)(\alpha^{\prime},\beta^{\prime},\gamma^{\prime}) up to a scalar. We verify this only in the case of a 3-cycle, the other cases follow by similar, and easier, arguments.

Assume that ψ\psi cyclically permutes the lines: (x=0)β†’(y=0)β†’(x=y)β†’(x=0)(x=0)\rightarrow(y=0)\rightarrow(x=y)\rightarrow(x=0). Let [ψi​j]∈G​L3[\psi_{ij}]\in GL_{3} represent the transformation ψ\psi up to rescaling. Without loss of generality we may assume

[ψi​j]=[1βˆ’10100ψ31ψ32ψ33][\psi_{ij}]=\begin{bmatrix}1&-1&0\\ 1&0&0\\ \psi_{31}&\psi_{32}&\psi_{33}\\ \end{bmatrix}

where ψ33β‰ 0\psi_{33}\neq 0. Evaluating the commutativity relation Οˆβ€‹Οƒ=Οƒβ€²β€‹Οˆ\psi\sigma=\sigma^{\prime}\psi at [0:1:0][0:1:0], [1:0:0][1:0:0] and [1:1:0][1:1:0] yields

Ξ²β€²=βˆ’Ξ±β€‹Οˆ33,Ξ³β€²=βˆ’Ξ²β€‹Οˆ33,Ξ±β€²=βˆ’Ξ³β€‹Οˆ33.\beta^{\prime}=-\alpha\psi_{33},\quad\gamma^{\prime}=-\beta\psi_{33},\quad\alpha^{\prime}=-\gamma\psi_{33}.

Hence [Ξ±β€²:Ξ²β€²:Ξ³β€²]=[Ξ³:Ξ±:Ξ²][\alpha^{\prime}:\beta^{\prime}:\gamma^{\prime}]=[\gamma:\alpha:\beta] as desired.

Conversely, suppose that [Ξ±:Ξ²:Ξ³]βˆˆβ„™2[\alpha:\beta:\gamma]\in{\mathbb{P}}^{2} and Ξ±+Ξ²+Ξ³β‰ 0\alpha+\beta+\gamma\neq 0. Let EE, Eβ€²E^{\prime} denote the point schemes of T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma), T​(Ξ³,Ξ±,Ξ²)T(\gamma,\alpha,\beta), with automorphisms Οƒ\sigma, Οƒβ€²\sigma^{\prime}, respectively. Define ψ∈Aut​(β„™2)\psi\in{\rm Aut}({\mathbb{P}}^{2}) by the matrix

[ψi​j]=[1βˆ’1010000βˆ’1].[\psi_{ij}]=\begin{bmatrix}1&-1&0\\ 1&0&0\\ 0&0&-1\\ \end{bmatrix}.

Then one checks that Οˆβ€‹Οƒ=Οƒβ€²β€‹Οˆ\psi\sigma=\sigma^{\prime}\psi, so, by Theorem 2.6, T​(Ξ±,Ξ²,Ξ³)β‰…T​(Ξ³,Ξ±,Ξ²)T(\alpha,\beta,\gamma)\cong T(\gamma,\alpha,\beta). Similarly, T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma) is isomorphic to T​(Ξ±β€²,Ξ²β€²,Ξ³β€²)T(\alpha^{\prime},\beta^{\prime},\gamma^{\prime}) whenever (Ξ±β€²,Ξ²β€²,Ξ³β€²)(\alpha^{\prime},\beta^{\prime},\gamma^{\prime}) is any permutation of (Ξ±,Ξ²,Ξ³)(\alpha,\beta,\gamma). ∎

When Bβˆ’a=0β‰ Cβˆ’bB-a=0\neq C-b, the quadratic form Q​(x,y)Q(x,y) has distinct linear factors, one of which is yy. These algebras are isomorphic to those where the form is a perfect square and are considered below.

Lemma 5.12.

A twisted tensor product from case O(1)(i) with A=0A=0 and Bβˆ’a=0β‰ Cβˆ’bB-a=0\neq C-b is isomorphic to an algebra from case O(1)(i) with A=0A=0 and Bβˆ’aβ‰ 0=(Cβˆ’b)2βˆ’4​(aβˆ’B)​cB-a\neq 0=(C-b)^{2}-4(a-B)c.

Proof.

An isomorphism is given by the mapping x↦y+β​xx\mapsto y+\beta x, y↦xy\mapsto x, z↦zz\mapsto z, where (Cβˆ’b)β€‹Ξ²βˆ’c=0(C-b)\beta-c=0. ∎

When Q​(x,y)Q(x,y) is the nonzero perfect square [2​(Bβˆ’a)​x+(Cβˆ’b)​y]2[2(B-a)x+(C-b)y]^{2}, the point scheme of TT is either the union of this double line with y=0y=0, or the triple line y3=0y^{3}=0. The next proposition simplifies the description of TT in the former case.

For Ξ³βˆˆπ•‚\gamma\in\mathbb{K} and ϡ∈{0,1}\epsilon\in\{0,1\}, define

W​(Ξ³,Ο΅)=π•‚β€‹βŸ¨x,y,z⟩⟨x​yβˆ’y​x,z​xβˆ’x​z+ϡ​x2+γ​x​y,z​yβˆ’y​z+ϡ​x​y+(1+Ξ³)​y2⟩.W(\gamma,\epsilon)=\dfrac{\mathbb{K}\langle x,y,z\rangle}{\left\langle xy-yx,zx-xz+\epsilon x^{2}+\gamma xy,zy-yz+\epsilon xy+(1+\gamma)y^{2}\right\rangle}.
Proposition 5.13.

An algebra TT is a twisted tensor product from case O(1)(i) with A=0A=0 and Bβˆ’aβ‰ 0=(Cβˆ’b)2βˆ’4​(aβˆ’B)​cB-a\neq 0=(C-b)^{2}-4(a-B)c if and only if TT is isomorphic to an algebra from the family W​(Ξ³,Ο΅)W(\gamma,\epsilon).

Proof.

Suppose TT is an algebra as hypothesized in the statement. The defining relations of TT are

x​yβˆ’y​x,z​xβˆ’a​x2βˆ’b​x​yβˆ’c​y2βˆ’x​z,z​yβˆ’B​x​yβˆ’C​y2βˆ’y​z.xy-yx,zx-ax^{2}-bxy-cy^{2}-xz,zy-Bxy-Cy^{2}-yz.

Let Ξ²\beta be the unique solution to (Bβˆ’a)​t2+(Cβˆ’b)​tβˆ’c=0.(B-a)t^{2}+(C-b)t-c=0. It follows that 2​(Bβˆ’a)​β+(Cβˆ’b)=02(B-a)\beta+(C-b)=0. The map sending x↦x+β​yx\mapsto x+\beta y and fixing yy and zz defines an isomorphism of TT to the algebra Tβ€²T^{\prime} with relations

x​yβˆ’y​x,z​xβˆ’x​zβˆ’a​x2βˆ’Ξ»β€‹x​y,z​yβˆ’y​zβˆ’B​x​yβˆ’Ξ»β€‹y2,xy-yx,zx-xz-ax^{2}-\lambda xy,zy-yz-Bxy-\lambda y^{2},

where Ξ»=C+β​B\lambda=C+\beta B. If Ξ»β‰ 0\lambda\neq 0, the map xβ†¦βˆ’yaβˆ’Bx\mapsto-\dfrac{y}{a-B}, yβ†¦βˆ’xΞ»y\mapsto-\dfrac{x}{\lambda}, z↦zz\mapsto z defines an isomorphism from Tβ€²T^{\prime} to the algebra W​(Ξ³,1)W(\gamma,1), where Ξ³=B/(aβˆ’B)\gamma=B/(a-B). If Ξ»=0\lambda=0, then xβ†¦βˆ’yaβˆ’Bx\mapsto-\dfrac{y}{a-B}, yβ†¦βˆ’xy\mapsto-x, z↦zz\mapsto z defines an isomorphism from Tβ€²T^{\prime} to the algebra W​(Ξ³,0)W(\gamma,0), where Ξ³=B/(aβˆ’B)\gamma=B/(a-B).

Conversely, for any Ξ³βˆˆπ•‚\gamma\in\mathbb{K} and ϡ∈{0,1}\epsilon\in\{0,1\}, W​(Ξ³,Ο΅)W(\gamma,\epsilon) satisfies the conditions of case O(1)(i) with A=0A=0, Bβˆ’a=0β‰ Cβˆ’bB-a=0\neq C-b. The result follows from Lemma 5.12. ∎

We use the following result to characterize isomorphism classes of Ore-type algebras in the cases where the point scheme is not reduced.

Recall that if Ξ»βˆˆπ•‚βˆ—\lambda\in\mathbb{K}^{*} and Ο†:Bβ†’Bβ€²\varphi:B\to B^{\prime} is an isomorphism of graded 𝕂\mathbb{K}-algebras, then the map φλ:Bβ†’Bβ€²\varphi_{\lambda}:B\to B^{\prime}, given by φλ​(b)=Ξ»i​b\varphi_{\lambda}(b)=\lambda^{i}b for all b∈Bib\in B_{i}, is also an isomorphism of graded 𝕂\mathbb{K}-algebras. We refer to φλ\varphi_{\lambda} as a scaling of Ο†\varphi.

Proposition 5.14.

Let AA be a graded 𝕂\mathbb{K}-algebra. Let A​[z,Ξ½,Ξ΄]A[z,\nu,\delta], A​[w,Ξ½β€²,Ξ΄β€²]A[w,\nu^{\prime},\delta^{\prime}] be graded Ore extensions with deg⁑z=deg⁑w=1\deg z=\deg w=1. Let Ο†:A​[z;Ξ½,Ξ΄]β†’A​[w;Ξ½β€²,Ξ΄β€²]\varphi:A[z;\nu,\delta]\to A[w;\nu^{\prime},\delta^{\prime}] be a graded 𝕂\mathbb{K}-algebra isomorphism.

  • (1)

    If φ​(A)=A\varphi(A)=A, then there exists a scaling of Ο†\varphi, φλ\varphi_{\lambda}, such that φλ​ν=ν′​φλ\varphi_{\lambda}\nu=\nu^{\prime}\varphi_{\lambda} and φλ​δ=δ′​φλ\varphi_{\lambda}\delta=\delta^{\prime}\varphi_{\lambda}.

  • (2)

    If A=𝕂​[x,y]A=\mathbb{K}[x,y] and Z​(A​[w;Ξ½β€²,Ξ΄β€²])1=0Z(A[w;\nu^{\prime},\delta^{\prime}])_{1}=0 then φ​(A)=A\varphi(A)=A.

Proof.

Assume that φ​(A)=A\varphi(A)=A. Since Ο†\varphi is surjective and degree-0, there exists kβˆˆπ•‚βˆ—k\in\mathbb{K}^{*} such that φ​(z)=aβ€²+k​w\varphi(z)=a^{\prime}+kw for aβ€²βˆˆA1a^{\prime}\in A_{1}. Scaling Ο†\varphi, if necessary, we may assume that k=1k=1. Then for any homogeneous a∈Aia\in A_{i} we have

0\displaystyle 0 =φ​(z​aβˆ’Ξ½β€‹(a)​zβˆ’Ξ΄β€‹(a))\displaystyle=\varphi(za-\nu(a)z-\delta(a))
=(aβ€²+w)​φ​(a)βˆ’Ο†β€‹(ν​(a))​(w+aβ€²)βˆ’Ο†β€‹(δ​(a))\displaystyle=(a^{\prime}+w)\varphi(a)-\varphi(\nu(a))(w+a^{\prime})-\varphi(\delta(a))
=[ν′​(φ​(a))βˆ’Ο†β€‹(ν​(a))]​w+a′​φ​(a)βˆ’Ο†β€‹(ν​(a))​aβ€²+δ′​(φ​(a))βˆ’Ο†β€‹(δ​(a)).\displaystyle=[\nu^{\prime}(\varphi(a))-\varphi(\nu(a))]w+a^{\prime}\varphi(a)-\varphi(\nu(a))a^{\prime}+\delta^{\prime}(\varphi(a))-\varphi(\delta(a)).

Since A​[w;Ξ½β€²,Ξ΄β€²]A[w;\nu^{\prime},\delta^{\prime}] is a free left AA-module on the basis {wi}\{w^{i}\}, AA is graded, deg⁑ν=0\deg\nu=0, and deg⁑δ=deg⁑δ′=1\deg\delta=\deg\delta^{\prime}=1, the first statement follows.

Now let A=𝕂​[x,y]A=\mathbb{K}[x,y] and suppose that Z​(A​[w;Ξ½β€²,Ξ΄β€²])1=0Z(A[w;\nu^{\prime},\delta^{\prime}])_{1}=0. Let ν′​(x)=m11​x+m12​y\nu^{\prime}(x)=m_{11}x+m_{12}y and ν′​(y)=m21​x+m22​y\nu^{\prime}(y)=m_{21}x+m_{22}y. Write φ​(x)=Ξ±1​x+Ξ²1​y+Ξ³1​w\varphi(x)=\alpha_{1}x+\beta_{1}y+\gamma_{1}w and φ​(y)=Ξ±2​x+Ξ²2​y+Ξ³2​w\varphi(y)=\alpha_{2}x+\beta_{2}y+\gamma_{2}w. Then

0=φ​(x​yβˆ’y​x)\displaystyle 0=\varphi(xy-yx) =[(Ξ±2​γ1βˆ’Ξ±1​γ2)​(m11βˆ’1)+(Ξ²2​γ1βˆ’Ξ²1​γ2)​m21]​x​w\displaystyle=[(\alpha_{2}\gamma_{1}-\alpha_{1}\gamma_{2})(m_{11}-1)+(\beta_{2}\gamma_{1}-\beta_{1}\gamma_{2})m_{21}]xw
+[(Ξ±2​γ1βˆ’Ξ±1​γ2)​(m12)+(Ξ²2​γ1βˆ’Ξ²1​γ2)​(m22βˆ’1)]​y​w\displaystyle+[(\alpha_{2}\gamma_{1}-\alpha_{1}\gamma_{2})(m_{12})+(\beta_{2}\gamma_{1}-\beta_{1}\gamma_{2})(m_{22}-1)]yw
+(Ξ±2​γ1βˆ’Ξ±1​γ2)​δ′​(x)+(Ξ²2​γ1βˆ’Ξ²1​γ2)​δ′​(y).\displaystyle+(\alpha_{2}\gamma_{1}-\alpha_{1}\gamma_{2})\delta^{\prime}(x)+(\beta_{2}\gamma_{1}-\beta_{1}\gamma_{2})\delta^{\prime}(y).

Let r=Ξ±2​γ1βˆ’Ξ±1​γ2r=\alpha_{2}\gamma_{1}-\alpha_{1}\gamma_{2} and s=Ξ²2​γ1βˆ’Ξ²1​γ2s=\beta_{2}\gamma_{1}-\beta_{1}\gamma_{2}. It follows from the calculation above and direct computation that r​x+s​yrx+sy is in Z​(A​[w;Ξ½β€²,Ξ΄β€²])1Z(A[w;\nu^{\prime},\delta^{\prime}])_{1}, hence r=s=0r=s=0. Thus both {(Ξ±1,Ξ±2),(Ξ³1,Ξ³2)}\{(\alpha_{1},\alpha_{2}),(\gamma_{1},\gamma_{2})\} and {(Ξ²1,Ξ²2),(Ξ³1,Ξ³2)}\{(\beta_{1},\beta_{2}),(\gamma_{1},\gamma_{2})\} are linearly dependent. If φ​(A)βŠ„A\varphi(A)\not\subset A, then (Ξ³1,Ξ³2)β‰ (0,0)(\gamma_{1},\gamma_{2})\neq(0,0) and {φ​(x),φ​(y)}\{\varphi(x),\varphi(y)\} is linearly dependent, a contradiction. ∎

Proposition 5.15.

The algebras W​(Ξ³,Ο΅)W(\gamma,\epsilon) and W​(Ξ³β€²,Ο΅β€²)W(\gamma^{\prime},\epsilon^{\prime}) are isomorphic if and only if Ο΅β€²=Ο΅\epsilon^{\prime}=\epsilon and Ξ³β€²=Ξ³\gamma^{\prime}=\gamma.

Proof.

First, if Ο΅=1\epsilon=1, or Ο΅=0\epsilon=0 and Ξ³βˆ‰{0,βˆ’1}\gamma\notin\{0,-1\}, then δ​(x)=βˆ’Ο΅β€‹x2βˆ’Ξ³β€‹x​y\delta(x)=-\epsilon x^{2}-\gamma xy and δ​(y)=βˆ’Ο΅β€‹x​yβˆ’(1+Ξ³)​y2\delta(y)=-\epsilon xy-(1+\gamma)y^{2} are linearly independent, and so Z​(W​(Ξ³,Ο΅))1=0Z(W(\gamma,\epsilon))_{1}=0. These W​(Ξ³,Ο΅)W(\gamma,\epsilon) are not isomorphic to W​(0,0)W(0,0) or W​(βˆ’1,0)W(-1,0) because xx or yy (respectively) is the unique central element in degree 1, up to scaling. Moreover, W​(0,0)W(0,0) and W​(βˆ’1,0)W(-1,0) are not isomorphic since it is clear that W​(0,0)/⟨x⟩W(0,0)/\langle x\rangle is not isomorphic to W​(βˆ’1,0)/⟨y⟩W(-1,0)/\langle y\rangle. Henceforth we assume that Ο΅=1\epsilon=1, or Ο΅=0\epsilon=0 and Ξ³βˆ‰{0,βˆ’1}\gamma\notin\{0,-1\}.

Suppose there is an isomorphism Ο†:W​(Ξ³,Ο΅)β†’W​(Ξ³β€²,Ο΅β€²)\varphi:W(\gamma,\epsilon)\to W(\gamma^{\prime},\epsilon^{\prime}). Then δ​(x)\delta(x) and δ​(y)\delta(y) are linearly independent elements of W​(Ξ³,Ο΅)W(\gamma,\epsilon) as are their counterparts δ′​(x)\delta^{\prime}(x) and δ′​(y)\delta^{\prime}(y) in W​(Ξ³β€²,Ο΅β€²)W(\gamma^{\prime},\epsilon^{\prime}). By Proposition 5.14 we may write φ​(x)=Ξ±1​x+Ξ²1​y\varphi(x)=\alpha_{1}x+\beta_{1}y and φ​(y)=Ξ±2​x+Ξ²2​y\varphi(y)=\alpha_{2}x+\beta_{2}y, and we may assume that Ο†\varphi commutes with Ξ΄\delta and Ξ΄β€²\delta^{\prime}. Equating coefficients of x2x^{2}, x​yxy and y2y^{2} in φ​(δ​(x))=δ′​(φ​(x))\varphi(\delta(x))=\delta^{\prime}(\varphi(x)) and φ​(δ​(y))=δ′​(φ​(y))\varphi(\delta(y))=\delta^{\prime}(\varphi(y)) yields the following:

Ξ±1​(ϡ​α1+γ​α2)\displaystyle\alpha_{1}(\epsilon\alpha_{1}+\gamma\alpha_{2}) =Ξ±1​ϡ′\displaystyle=\alpha_{1}\epsilon^{\prime} Ξ±2​(ϡ​α1+(1+Ξ³)​α2)\displaystyle\alpha_{2}(\epsilon\alpha_{1}+(1+\gamma)\alpha_{2}) =Ξ±2​ϡ′\displaystyle=\alpha_{2}\epsilon^{\prime}
Ξ²1​(ϡ​β1+γ​β2)\displaystyle\beta_{1}(\epsilon\beta_{1}+\gamma\beta_{2}) =Ξ²1​(1+Ξ³β€²)\displaystyle=\beta_{1}(1+\gamma^{\prime}) Ξ²2​(ϡ​β1+(1+Ξ³)​β2)\displaystyle\beta_{2}(\epsilon\beta_{1}+(1+\gamma)\beta_{2}) =Ξ²2​(1+Ξ³β€²)\displaystyle=\beta_{2}(1+\gamma^{\prime})
2​ϡ​α1​β1+γ​(Ξ±1​β2+Ξ±2​β1)=Ξ±1​γ′+Ξ²1​ϡ′2\epsilon\alpha_{1}\beta_{1}+\gamma(\alpha_{1}\beta_{2}+\alpha_{2}\beta_{1})=\alpha_{1}\gamma^{\prime}+\beta_{1}\epsilon^{\prime}
2​(1+Ξ³)​α2​β2+ϡ​(Ξ±1​β2+Ξ±2​β1)=Ξ±2​γ′+Ξ²2​ϡ′.2(1+\gamma)\alpha_{2}\beta_{2}+\epsilon(\alpha_{1}\beta_{2}+\alpha_{2}\beta_{1})=\alpha_{2}\gamma^{\prime}+\beta_{2}\epsilon^{\prime}.

Suppose that Ο΅=0\epsilon=0 and Ο΅β€²=1\epsilon^{\prime}=1. Considering the first two equations, we see that Ξ±1=0\alpha_{1}=0. The fifth and second equations then imply that Ξ²1=0\beta_{1}=0, so φ​(x)=0\varphi(x)=0, a contradiction. Thus we must have Ο΅=Ο΅β€²\epsilon=\epsilon^{\prime}.

When Ο΅=Ο΅β€²=0\epsilon=\epsilon^{\prime}=0, then Ξ±2=0\alpha_{2}=0 by the second equation, so Ξ±1β‰ 0β‰ Ξ²2\alpha_{1}\neq 0\neq\beta_{2}, else Ο†\varphi is not surjective. The fourth and fifth equations jointly imply that Ξ²2=1\beta_{2}=1, so Ξ³=Ξ³β€²\gamma=\gamma^{\prime}.

When Ο΅=Ο΅β€²=1\epsilon=\epsilon^{\prime}=1, we also have Ξ±2=0\alpha_{2}=0. If Ξ±1β‰ 0\alpha_{1}\neq 0, this follows from the first pair of equations. If Ξ±1=0\alpha_{1}=0, then Ξ²1β‰ 0\beta_{1}\neq 0 and (1+Ξ³)​α2=1(1+\gamma)\alpha_{2}=1. The fifth equation then simplifies to γ​α2=1\gamma\alpha_{2}=1, which implies that Ξ±2=0\alpha_{2}=0. A straightforward check shows that Ξ±2=0\alpha_{2}=0 implies Ξ³=Ξ³β€²\gamma=\gamma^{\prime}. ∎

Proposition 5.16.

The algebra W​(Ξ³,Ο΅)W(\gamma,\epsilon) is AS-regular. The point scheme of W​(Ξ³,Ο΅)W(\gamma,\epsilon) is the union of a line and a double line. The automorphism Οƒ\sigma stabilizes the components, and

  • (1)

    if Ο΅=0\epsilon=0, then Οƒ\sigma restricts to the identity on the double line (type W​L2WL_{2});

  • (2)

    if Ο΅=1\epsilon=1, then Οƒ\sigma has order char​𝕂{\rm char}\ \mathbb{K} on the double line. (type W​L3WL_{3})

Proof.

The algebra W​(Ξ³,Ο΅)W(\gamma,\epsilon) is AS-regular by Proposition 5.13 and Theorem 5.1. The matrix MM is

[βˆ’y0x00z0+ϡ​x0γ​x0βˆ’x00z0+ϡ​x0+(1+Ξ³)​y0βˆ’y0]\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}+\epsilon x_{0}&\gamma x_{0}&-x_{0}\\ 0&z_{0}+\epsilon x_{0}+(1+\gamma)y_{0}&-y_{0}\end{bmatrix}

so the point scheme is E=𝒡​(x​y2)E=\mathcal{Z}(xy^{2}) and the automorphism is

Οƒ([0:y:z])\displaystyle\sigma([0:y:z]) =[0:y:z+(1+Ξ³)y]\displaystyle=[0:y:z+(1+\gamma)y]
Οƒ([x:0:z])\displaystyle\sigma([x:0:z]) =[x:0:z+Ο΅x].\displaystyle=[x:0:z+\epsilon x].

The result follows immediately. ∎

For ϡ1,ϡ2∈{0,1}\epsilon_{1},\epsilon_{2}\in\{0,1\} we define

L​(Ο΅1,Ο΅2)=π•‚β€‹βŸ¨x,y,z⟩⟨x​yβˆ’y​x,z​xβˆ’x​z+Ο΅1​x​y+Ο΅2​x2,z​yβˆ’y​z+x2+Ο΅1​y2+Ο΅2​x​y⟩.L(\epsilon_{1},\epsilon_{2})=\dfrac{\mathbb{K}\langle x,y,z\rangle}{\langle xy-yx,zx-xz+\epsilon_{1}xy+\epsilon_{2}x^{2},zy-yz+x^{2}+\epsilon_{1}y^{2}+\epsilon_{2}xy\rangle}.
Proposition 5.17.

An algebra TT is a twisted tensor product from case O(1)(i) with A=0A=0 and Bβˆ’a=Cβˆ’b=0β‰ cB-a=C-b=0\neq c if and only if TT is isomorphic to one of L​(0,0),L​(0,1),L(0,0),L(0,1), or L​(1,0)L(1,0), no two of which are isomorphic.

Proof.

Suppose TT is an algebra as hypothesized in the statement. If aβ‰ 0a\neq 0, then x↦yβˆ’(b/a​c)​xx\mapsto y-(b/\sqrt{ac})x, y↦a/c​xy\mapsto\sqrt{a/c}x, zβ†¦βˆ’a​zz\mapsto-az determines an isomorphism from TT to L​(1,0)L(1,0). If a=b=0a=b=0, then xβ†¦βˆ’c​yx\mapsto-cy, y↦xy\mapsto x, z↦zz\mapsto z determines an isomorphism from TT to L​(0,0)L(0,0). If a=0β‰ ba=0\neq b, then x↦(c/b)​yx\mapsto(c/b)y, y↦xy\mapsto x, zβ†¦βˆ’b​zz\mapsto-bz determines an isomorphism from TT to L​(0,1)L(0,1). Conversely, it is clear that L​(0,0)L(0,0), L​(0,1)L(0,1) and L​(1,0)L(1,0) are algebras from case O(1)(i) of the stated form.

To see that the three algebras are pairwise non-isomorphic, first note that the degree-1 generator x∈L​(0,0)x\in L(0,0) is central, and L​(1,0)L(1,0) and L​(0,1)L(0,1) contain no central elements in degree 1. By Proposition 5.14, any isomorphism Ο†:L​(1,0)β†’L​(0,1)\varphi:L(1,0)\to L(0,1) must restrict to an automorphism of 𝕂​[x,y]\mathbb{K}[x,y] and commute with the respective derivations. An easy direct calculation in degree 1 shows that no such Ο†\varphi exists. ∎

Proposition 5.18.

The algebras L​(0,0)L(0,0), L​(0,1)L(0,1), and L​(1,0)L(1,0) are AS-regular, and the point scheme of each is a triple line. The order of the automorphism Οƒ\sigma is the order of Ο΅1\epsilon_{1} in the additive group (𝕂,+)(\mathbb{K},+).

Proof.

The algebras L​(0,0)L(0,0), L​(0,1)L(0,1), and L​(1,0)L(1,0) are AS-regular by Proposition 5.17 and Theorem 5.1. The matrix MM is

[βˆ’y0x00z0+Ο΅2​x0Ο΅1​x0βˆ’x0x0z0+Ο΅2​x0+Ο΅1​y0βˆ’y0]\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}+\epsilon_{2}x_{0}&\epsilon_{1}x_{0}&-x_{0}\\ x_{0}&z_{0}+\epsilon_{2}x_{0}+\epsilon_{1}y_{0}&-y_{0}\end{bmatrix}

so the point scheme of TT is E=𝒡​(x3)E=\mathcal{Z}(x^{3}) and the automorphism Οƒ\sigma is given by Οƒ([0:y:z])=[0:y:z+Ο΅1y].\sigma([0:y:z])=[0:y:z+\epsilon_{1}y]. The result follows. ∎

Remark 5.19.

The presentations of L​(0,0)L(0,0), L​(1,0)L(1,0), and L​(0,1)L(0,1) align with those of Types T​L1,T​L2,TL_{1},TL_{2}, and T​L4TL_{4} given in [5, Theorem 3.1]., respectively. We remark that Οƒ\sigma is the identity on closed points for both L​(0,0)L(0,0) and L​(0,1)L(0,1).

For ϡ∈{0,1}\epsilon\in\{0,1\} define

P​(Ο΅)=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​xβˆ’Ο΅β€‹x2βˆ’x​z,z​yβˆ’Ο΅β€‹x​yβˆ’y​z⟩.P(\epsilon)=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zx-\epsilon x^{2}-xz,zy-\epsilon xy-yz\rangle.
Proposition 5.20.

An algebra TT is a twisted tensor product from case O(1)(i) with Bβˆ’a=Cβˆ’b=c=0B-a=C-b=c=0 if and only if TT is isomorphic to P​(Ο΅)P(\epsilon).

Proof.

Suppose TT is an algebra as hypothesized in the statement. The defining relations of TT are

x​yβˆ’y​x,z​xβˆ’a​x2βˆ’b​x​yβˆ’x​z,z​yβˆ’a​x​yβˆ’b​y2βˆ’y​z.xy-yx,zx-ax^{2}-bxy-xz,zy-axy-by^{2}-yz.

If a=b=0a=b=0, then clearly T=P​(0)T=P(0). If aβ‰ 0a\neq 0, then the change of variables x↦xβˆ’(b/a)​yx\mapsto x-(b/a)y, y↦yy\mapsto y, z↦a​zz\mapsto az is an isomorphism from TT to the algebra P​(1)P(1). If a=0β‰ ba=0\neq b, then interchanging xx and yy yields an algebra of the form just considered.

Conversely, the algebras P​(0)P(0) and P​(1)P(1) clearly satisfy the conditions specified in this subcase of case O(1)(i). ∎

Proposition 5.21.

The algebras P​(0)P(0) and P​(1)P(1) are AS-regular. The point scheme of each is β„™2{\mathbb{P}}^{2}. The automorphism Οƒ\sigma is the identity for P​(0)P(0), and for P​(1)P(1) the order of Οƒ\sigma is the characteristic of 𝕂\mathbb{K}.

Proof.

The algebras P​(0)P(0) and P​(1)P(1) are AS-regular by Proposition 5.20 and Theorem 5.1. The matrix MM is

[βˆ’y0x00z0βˆ’Ο΅β€‹x00βˆ’x00z0βˆ’Ο΅β€‹x0βˆ’y0]\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}-\epsilon x_{0}&0&-x_{0}\\ 0&z_{0}-\epsilon x_{0}&-y_{0}\end{bmatrix}

so the point scheme of P​(Ο΅)P(\epsilon) is 𝒡​(0)=β„™2\mathcal{Z}(0)={\mathbb{P}}^{2} and the automorphism Οƒ\sigma is given by Οƒ([x:y:z])=[x:y:zβˆ’Ο΅x]\sigma([x:y:z])=[x:y:z-\epsilon x]. ∎

5.4. Twisted tensor products from cases O(2)(i), O(2)(ii)

Now we turn our attention to algebras from case O(2). Recall that in this case e=1e=1. Define

W=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​xβˆ’x​z+x2+y​z,z​yβˆ’y​z⟩.W=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zx-xz+x^{2}+yz,zy-yz\rangle.
Proposition 5.22.

Any twisted tensor product from case O(2)(i) with a=0a=0 is isomorphic to an algebra from case O(1)(i).

Any twisted tensor product from case O(2)(i) with a≠0a\neq 0 is isomorphic to WW.

Proof.

Let TT be a twisted tensor product from case O(2)(i). The defining relations of TT are

x​yβˆ’y​x,z​xβˆ’a​x2βˆ’b​x​yβˆ’c​y2βˆ’x​zβˆ’y​z,z​yβˆ’y​z.xy-yx,zx-ax^{2}-bxy-cy^{2}-xz-yz,zy-yz.

If a=0a=0, the map determined by xβ†¦βˆ’zx\mapsto-z, y↦yy\mapsto y, and z↦xβˆ’c​y+b​zz\mapsto x-cy+bz is an isomorphism from TT to the algebra with relations

x​yβˆ’y​x,z​xβˆ’x​yβˆ’x​z,z​yβˆ’y​z,xy-yx,zx-xy-xz,zy-yz,

which belongs to case O(1)(i).

If aβ‰ 0a\neq 0, the isomorphism given by xβ†¦βˆ’xx\mapsto-x, y↦yy\mapsto y, z↦a​zβˆ’c​y+b​xz\mapsto az-cy+bx identifies TT with the algebra WW defined above. ∎

Proposition 5.23.

The algebra WW is AS-regular. The point scheme of WW is the union of a line and an irreducible conic. The components meet at a single point, and Οƒ\sigma stabilizes the components (type Tβ€²T^{\prime}). The order of Οƒ\sigma is char​𝕂{\rm char}\ \mathbb{K}.

Proof.

By Proposition 5.22 and Theorem 5.1, WW is AS-regular. The matrix MM is

[βˆ’y0x00z0+x00βˆ’x0+y00z0βˆ’y0]\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}+x_{0}&0&-x_{0}+y_{0}\\ 0&z_{0}&-y_{0}\end{bmatrix}

so the point scheme of WW is 𝒡​(y​(x2+y​z))\mathcal{Z}(y(x^{2}+yz)). The components intersect in the point [0:0:1][0:0:1], and the automorphism is given by

σ([x:y:z])={[x:y:z]y≠0[x:0:x+z]y=0.\sigma([x:y:z])=\begin{cases}[x:y:z]&y\neq 0\\ [x:0:x+z]&y=0\\ \end{cases}.

The result follows. ∎

For dβˆˆπ•‚d\in\mathbb{K}, dβ‰ 1d\neq 1, define

W​(d)=π•‚β€‹βŸ¨x,y,z⟩/⟨x​yβˆ’y​x,z​xβˆ’d​x​zβˆ’y​z,z​yβˆ’d​y​z⟩.W(d)=\mathbb{K}\langle x,y,z\rangle/\langle xy-yx,zx-dxz-yz,zy-dyz\rangle.
Proposition 5.24.

A twisted tensor product TT belongs to case O(2)(ii) if and only if TT is isomorphic to W​(d)W(d) for some dβ‰ 1d\neq 1. Moreover, the algebras W​(d)W(d) and W​(dβ€²)W(d^{\prime}) are isomorphic if and only if dβ€²=dd^{\prime}=d.

Proof.

If TT is a twisted tensor product from case O(2)(ii), then the map x↦xx\mapsto x, y↦yy\mapsto y, z↦z+λ​xβˆ’c​yz\mapsto z+\lambda x-cy, where Ξ»=a1βˆ’d\lambda=\dfrac{a}{1-d}, is an isomorphism from TT to an algebra in the family W​(d)W(d). Conversely, it is clear that W​(d)W(d) is an algebra from case O(2)(ii).

For the last statement, since dβ‰ 1d\neq 1, one checks that Z​(W​(d))1=0Z(W(d))_{1}=0, so by Proposition 5.14, an isomorphism Ο†:W​(d)β†’W​(dβ€²)\varphi:W(d)\rightarrow W(d^{\prime}) would restrict to an automorphism of 𝕂​[x,y]\mathbb{K}[x,y] that commutes with Ξ½\nu and Ξ½β€²\nu^{\prime}. As the Jordan forms of Ξ½1\nu_{1} and Ξ½1β€²\nu^{\prime}_{1} are indecomposable, the condition φ​ν=ν′​φ\varphi\nu=\nu^{\prime}\varphi implies that d=dβ€²d=d^{\prime}. ∎

Proposition 5.25.

The algebra W​(d)W(d) is AS-regular if and only if dβ‰ 0.d\neq 0. If W​(d)W(d) is AS-regular, then the point scheme is the union of a line and a double line. The automorphism Οƒ\sigma restricts to the identity on the reduced line. When restricted to the double line, the order of Οƒ\sigma is the additive order of dβˆˆπ•‚d\in\mathbb{K}. (type W​L1WL_{1})

Proof.

By Proposition 5.24 and Theorem 5.1, W​(d)W(d) is AS-regular if and only if dβ‰ 0d\neq 0. The matrix MM is

[βˆ’y0x00z00βˆ’d​x0βˆ’y00z0βˆ’d​y0]\begin{bmatrix}-y_{0}&x_{0}&0\\ z_{0}&0&-dx_{0}-y_{0}\\ 0&z_{0}&-dy_{0}\end{bmatrix}

so the point scheme of W​(d)W(d) is 𝒡​(y2​z)\mathcal{Z}(y^{2}z). The automorphism Οƒ\sigma is given by

Οƒ([x:0:z])\displaystyle\sigma([x:0:z]) =[dx:0:z]\displaystyle=[dx:0:z]
Οƒ([x:y:0])\displaystyle\sigma([x:y:0]) =[x:y:0],\displaystyle=[x:y:0],

and the result follows. ∎

We conclude this section with a proof of Theorem 5.2.

Proof of Theorem 5.2.

First we consider case O(1)(i). In this case, every algebra is AS-regular by Theorem 5.1. Lemma 5.9 shows there is no loss of generality in assuming A=0A=0. We further divide case O(1)(i) into two subcases. Algebras from case O(1)(i) with A=0β‰ Bβˆ’aA=0\neq B-a are classified up to isomorphism as T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma) or W​(Ξ³,Ο΅)W(\gamma,\epsilon) in Propositions 5.10 and 5.13. Proposition 5.11 shows that T​(Ξ±,Ξ²,Ξ³)T(\alpha,\beta,\gamma) is of Type T1T_{1}, and Proposition 5.16 shows that W​(Ξ³,Ο΅)W(\gamma,\epsilon) is of Type W​L2WL_{2} when Ο΅=0\epsilon=0, and Type W​L3WL_{3} when Ο΅=1\epsilon=1.

Continuing with case O(1)(i), when A=0=Bβˆ’aA=0=B-a, Lemma 5.12 shows that no generality is lost in assuming b=Cb=C. Case O(1)(i) algebras with A=Bβˆ’a=Cβˆ’b=0A=B-a=C-b=0 are classified up to isomorphism as L​(0,0),L​(0,1),L​(1,0)L(0,0),L(0,1),L(1,0), or P​(Ο΅)P(\epsilon) in Propositions 5.17 and 5.20. Proposition 5.18 and Remark 5.19 show that L​(0,0),L​(1,0),L(0,0),L(1,0), and L​(0,1)L(0,1) are AS-regular of Type T​L1TL_{1}, T​L2TL_{2}, and T​L4TL_{4}, respectively. Proposition 5.21 proves that P​(Ο΅)P(\epsilon) is AS-regular of Type P1P_{1} when Ο΅=0\epsilon=0, and Type P2P_{2} when Ο΅=1\epsilon=1.

Algebras from case O(1)(ii) are isomorphic to algebras from the family S′​(d,Ο΅)S^{\prime}(d,\epsilon) by Proposition 5.7. Proposition 5.8 shows S′​(d,Ο΅)S^{\prime}(d,\epsilon) is AS-regular if and only if dβ‰ 0d\neq 0, and that the AS-regular algebras in this family are of Type S1S_{1} when Ο΅=0\epsilon=0, and Type S1β€²S^{\prime}_{1} when Ο΅=1\epsilon=1.

By Lemma 5.4(1), every algebra from case O(1)(iii) is isomorphic to an algebra from case O(1)(ii).

For case O(1)(iv), Lemma 5.4(2) shows that no generality is lost in assuming C=0C=0. These algebras are isomorphic to algebras from the family S​(d,D)S(d,D) by Proposition 5.5. Proposition 5.6 shows S​(d,D)S(d,D) is AS-regular if and only if d​Dβ‰ 0dD\neq 0, and proves that the AS-regular algebras in this family are of Type P1P_{1} when d=Dd=D, and of Type S1S_{1} when dβ‰ Dd\neq D. Proposition 5.21 shows that the Type P1P_{1} algebras isomorphic to S​(d,D)S(d,D) are not isomorphic to the algebra P​(0)P(0). Proposition 5.8 shows that the Type S1S_{1} algebras isomorphic to S​(d,D)S(d,D) are not isomorphic to Type S1S_{1} algebras from the family S′​(d,0)S^{\prime}(d,0).

In case O(2)(i), Proposition 5.22 shows that no generality is lost in assuming that a≠0a\neq 0 and shows that all algebras in this family are isomorphic to the algebra WW. Proposition 5.23 establishes that WW is AS-regular of Type T′T^{\prime}.

Finally, algebras from case O(2)(ii) are isomorphic to algebras from the family W​(d)W(d) by Proposition 5.24. Proposition 5.25 shows that W​(d)W(d) is AS-regular if and only if dβ‰ 0d\neq 0, and that the regular algebras in this family are of Type W​L1WL_{1}. ∎

Remark 5.26.

[5, Theorem 3.2] characterizes quadratic AS-regular algebras of non-EC type up to Morita equivalence. Types P,T,Tβ€²,W​L,T​LP,T,T^{\prime},WL,TL, each of which include algebras from Theorem 5.2, consist of a single Morita equivalence class. For Type SS, [5, Theorem 3.2] implies that every Morita equivalence class contains an algebra with Ξ²=Ξ³=1\beta=\gamma=1, Ξ±β‰ 0,1\alpha\neq 0,1. Such an algebra is the twisted tensor product S′​(Ξ±,0)S^{\prime}(\alpha,0) (see Subsection 5.2). Similarly for Type Sβ€²S^{\prime}, every Morita class contains an algebra with Ξ²=1\beta=1 and Ξ±β‰ 0,1\alpha\neq 0,1. After interchanging xx and yy and rescaling yy, we obtain the twisted tensor product S′​(1/Ξ±,1)S^{\prime}(1/\alpha,1).

6. Graded Twisted Tensor Products and Sklyanin Algebras

As the preceding sections show, the only graded twisted tensor products of 𝕂​[x,y]\mathbb{K}[x,y] and 𝕂​[z]\mathbb{K}[z] whose point schemes are elliptic curves are the algebras T​(g,h)T(g,h) (hβ‰ 0h\neq 0) of Section 3. These algebras belong to subtype B in the classification schemes of [1] and [6]. It is therefore natural to ask whether other subtypes of type-EC AS-regular algebras are graded twisted tensor products of the form AβŠ—π•‚β€‹[z]A\otimes\mathbb{K}[z], where AA is a two-dimensional quadratic AS-regular algebra. We answer this question for the well-known family of three-dimensional Sklyanin algebras.

By definition, a three-dimensional Sklyanin algebra is any algebra of the form

S​(a,b,c)=π•‚β€‹βŸ¨x,y,z⟩⟨a​y​z+b​z​y+c​x2,a​z​x+b​x​z+c​y2,a​x​y+b​y​x+c​z2⟩S(a,b,c)=\dfrac{\mathbb{K}\langle x,y,z\rangle}{\langle ayz+bzy+cx^{2},azx+bxz+cy^{2},axy+byx+cz^{2}\rangle}

such that [a:b:c]βˆˆβ„™2βˆ’π’Ÿ[a:b:c]\in{\mathbb{P}}^{2}-\mathcal{D}, where

π’Ÿ={[1:0:0],[0:1:0],[0:0:1]}βˆͺ{[a:b:c]:a3=b3=c3}.\mathcal{D}=\{[1:0:0],[0:1:0],[0:0:1]\}\cup\{[a:b:c]:a^{3}=b^{3}=c^{3}\}.

This family is defined over a field 𝕂\mathbb{K} of any characteristic. It is well known that S​(a,b,c)S(a,b,c) is AS-regular if and only if [a:b:c]βˆ‰π’Ÿ[a:b:c]\notin\mathcal{D}. If [a:b:c]βˆˆπ’Ÿ[a:b:c]\in\mathcal{D}, the algebra S​(a,b,c)S(a,b,c) is referred to as a degenerate Sklyanin algebra. Let

S1=π•‚β€‹βŸ¨u,v,w⟩⟨u2,v2,w2⟩,S2=π•‚β€‹βŸ¨u,v,w⟩⟨u​v,v​w,w​u⟩.S_{1}=\dfrac{\mathbb{K}\langle u,v,w\rangle}{\langle u^{2},v^{2},w^{2}\rangle},\qquad S_{2}=\frac{\mathbb{K}\langle u,v,w\rangle}{\langle uv,vw,wu\rangle}.

Smith [10] proved that if [a:b:c]βˆˆπ’Ÿ[a:b:c]\in\mathcal{D} and char​𝕂≠3{\rm char\ }\mathbb{K}\neq 3, then S​(a,b,c)β‰…S1S(a,b,c)\cong S_{1} if a=ba=b and S​(a,b,c)β‰…S2S(a,b,c)\cong S_{2} if aβ‰ ba\neq b.

The point scheme of the Sklyanin algebra S​(a,b,c)S(a,b,c) is

E=𝒡​((a3+b3+c3)​x​y​zβˆ’(a​b​c)​(x3+y3+z3)),E=\mathcal{Z}((a^{3}+b^{3}+c^{3})xyz-(abc)(x^{3}+y^{3}+z^{3})),

which describes an elliptic curve if and only if a​b​cβ‰ 0abc\neq 0 and (3​a​b​c)3β‰ (a3+b3+c3)3(3abc)^{3}\neq(a^{3}+b^{3}+c^{3})^{3}. When EE is an elliptic curve, the automorphism of EE can be described as translation by [a:b:c][a:b:c] in the group law, where the identity element is OE=[1:βˆ’1:0]O_{E}=[1:-1:0] (see [1, p. 38]). In this section we are concerned mainly with those S​(a,b,c)S(a,b,c) whose point scheme is an elliptic curve. We say that S​(a,b,c)S(a,b,c) is of type EC if this is the case.

If S​(a,b,c)β‰…AβŠ—π•‚β€‹[z]S(a,b,c)\cong A\otimes\mathbb{K}[z], then S​(a,b,c)S(a,b,c) contains a subalgebra isomorphic to AA, generated in degree 1. We begin by characterizing which S​(a,b,c)S(a,b,c) of type EC contain a one-generated subalgebra isomorphic to a skew polynomial ring 𝕂q​[r,s]\mathbb{K}_{q}[r,s], qβˆˆπ•‚βˆ—q\in\mathbb{K}^{*}, or the Jordan plane π•‚β€‹βŸ¨r,s⟩/⟨r​sβˆ’s​r+s2⟩\mathbb{K}\langle r,s\rangle/\langle rs-sr+s^{2}\rangle.

6.1. Three-dimensional Sklyanin algebras containing a quantum β„™1{\mathbb{P}}^{1}

If A=T​(V)/⟨R⟩A=T(V)/\langle R\rangle is a quadratic algebra, the quadratic dual algebra is defined to be the algebra A!=T​(Vβˆ—)/⟨RβŸ‚βŸ©A^{!}=T(V^{*})/\langle R^{\perp}\rangle where RβŸ‚βŠ‚Vβˆ—βŠ—Vβˆ—R^{\perp}\subset V^{*}\otimes V^{*} is the orthogonal complement to RR with respect to the natural pairing. Note that (A!)!(A^{!})^{!} is canonically isomorphic to AA. We establish a few facts about the schemes Γ​(S​(a,b,c)!)\Gamma(S(a,b,c)^{!}). Let e1=[1:0:0]e_{1}=[1:0:0], e2=[0:1:0]e_{2}=[0:1:0], e3=[0:0:1]e_{3}=[0:0:1].

Proposition 6.1.

Let A=S​(a,b,c)A=S(a,b,c) be a three-dimensional Sklyanin algebra.

  • (1)

    If cβ‰ 0c\neq 0, then Γ​(A!)\Gamma(A^{!}) is the empty scheme.

  • (2)

    Γ​(S​(a,βˆ’a,0)!)\Gamma(S(a,-a,0)^{!}) is the empty scheme.

  • (3)

    Γ​(S1!)={e1Γ—e1,e2Γ—e2,e3Γ—e3}.\Gamma(S_{1}^{!})=\{e_{1}\times e_{1},e_{2}\times e_{2},e_{3}\times e_{3}\}.

Proof.

(1) Assume that cβ‰ 0c\neq 0. Since Γ​(A!)\Gamma(A^{!}) is a projective scheme it is quasi-compact; as such, to prove the result, it suffices to show that Γ​(A!)\Gamma(A^{!}) has no closed points. Since cβ‰ 0c\neq 0, we can write the defining relations of A!A^{!} as

a​x2βˆ’c​y​za​y2βˆ’c​z​xa​z2βˆ’c​x​yb​x2βˆ’c​z​yb​y2βˆ’c​x​zb​z2βˆ’c​y​x.ax^{2}-cyz\qquad ay^{2}-czx\qquad az^{2}-cxy\qquad bx^{2}-czy\qquad by^{2}-cxz\qquad bz^{2}-cyx.

Multilinearizing these relations, we see that a closed point

[x0:y0:z0]Γ—[x1:y1:z1]βˆˆΞ“(A!)[x_{0}:y_{0}:z_{0}]\times[x_{1}:y_{1}:z_{1}]\in\Gamma(A^{!})

satisfies

a​x0​x1βˆ’c​y0​z1\displaystyle ax_{0}x_{1}-cy_{0}z_{1} =0(E1)\displaystyle=0\quad(E_{1}) b​x0​x1βˆ’c​z0​y1\displaystyle bx_{0}x_{1}-cz_{0}y_{1} =0(E2)\displaystyle=0\quad(E_{2})
a​y0​y1βˆ’c​z0​x1\displaystyle ay_{0}y_{1}-cz_{0}x_{1} =0(E3)\displaystyle=0\quad(E_{3}) b​y0​y1βˆ’c​x0​z1\displaystyle by_{0}y_{1}-cx_{0}z_{1} =0(E4)\displaystyle=0\quad(E_{4})
a​z0​z1βˆ’c​x0​y1\displaystyle az_{0}z_{1}-cx_{0}y_{1} =0(E5)\displaystyle=0\quad(E_{5}) b​z0​z1βˆ’c​y0​x1\displaystyle bz_{0}z_{1}-cy_{0}x_{1} =0(E6).\displaystyle=0\quad(E_{6}).

First assume a=0a=0. Since [a:b:c]βˆ‰π’Ÿ[a:b:c]\notin\mathcal{D}, we have b​cβ‰ 0bc\neq 0. It is easy to check that no point in β„™2Γ—β„™2{\mathbb{P}}^{2}\times{\mathbb{P}}^{2} satisfies all of the equations (Ei)(E_{i}). The case b=0b=0 is analogous.

Now assume that a​bβ‰ 0ab\neq 0. Let s:β„™2Γ—β„™2β†’β„™8s:{\mathbb{P}}^{2}\times{\mathbb{P}}^{2}\to{\mathbb{P}}^{8},

s([x0:y0:z0],[x1:y1:z1])=[x0​x1x0​y1x0​z1y0​x1y0​y1y0​z1z0​x1z0​y1z0​z1]s([x_{0}:y_{0}:z_{0}],[x_{1}:y_{1}:z_{1}])=\begin{bmatrix}x_{0}x_{1}&x_{0}y_{1}&x_{0}z_{1}\\ y_{0}x_{1}&y_{0}y_{1}&y_{0}z_{1}\\ z_{0}x_{1}&z_{0}y_{1}&z_{0}z_{1}\end{bmatrix}

be the Segre embedding. Let wi​jw_{ij}, 1≀i,j≀31\leq i,j\leq 3 be coordinates on β„™8{\mathbb{P}}^{8}. Recall that the image s​(β„™2Γ—β„™2)s({\mathbb{P}}^{2}\times{\mathbb{P}}^{2}) is the subscheme of β„™8{\mathbb{P}}^{8} cut out by the 2Γ—22\times 2 minors of the matrix [wi​j][w_{ij}]. Equations (Ei)(E_{i}), 1≀i≀61\leq i\leq 6 show that the closed points of s​(Γ​(A!))s(\Gamma(A^{!})) are the rank-1 matrices of the form

M=[c​w11a​w33b​w22b​w33c​w22a​w11a​w22b​w11c​w33].M=\begin{bmatrix}cw_{11}&aw_{33}&bw_{22}\\ bw_{33}&cw_{22}&aw_{11}\\ aw_{22}&bw_{11}&cw_{33}\end{bmatrix}.

Let Mi​jM_{ij}, 1≀i,j≀31\leq i,j\leq 3, denote the minors of MM. If M∈s​(Γ​(A!))M\in s(\Gamma(A^{!})), then consideration of the equations wi​i​Mi​i=0w_{ii}M_{ii}=0, for i=1,2,3i=1,2,3 shows that w113=w223=w333w_{11}^{3}=w_{22}^{3}=w_{33}^{3}. Note that since rank​(M)=1{\rm rank}(M)=1, w11​w22​w33β‰ 0w_{11}w_{22}w_{33}\neq 0. Furthermore, consideration of c​w33​M33=0cw_{33}M_{33}=0, b​w11​M32=0bw_{11}M_{32}=0, and a​w22​M31=0aw_{22}M_{31}=0 shows that

a3​w11​w22​w33=b3​w11​w22​w33=c3​w11​w22​w33.a^{3}w_{11}w_{22}w_{33}=b^{3}w_{11}w_{22}w_{33}=c^{3}w_{11}w_{22}w_{33}.

Since w11​w22​w33β‰ 0w_{11}w_{22}w_{33}\neq 0 we conclude that a3=b3=c3a^{3}=b^{3}=c^{3}. This contradicts the assumption that S​(a,b,c)S(a,b,c) is a three-dimensional Sklyanin algebra.

For (2), the algebra S​(a,βˆ’a,0)S(a,-a,0) is the polynomial algebra on three variables. Its quadratic dual is an exterior algebra, and it is straightforward to check that there are no closed points in Γ​(S​(a,βˆ’a,0)!)\Gamma(S(a,-a,0)^{!}).

For (3), a closed point [x0:y0:z0]Γ—[x1:y1:z1]βˆˆΞ“(S1!)[x_{0}:y_{0}:z_{0}]\times[x_{1}:y_{1}:z_{1}]\in\Gamma(S_{1}^{!}) satisfies

x0​y1=y0​x1=z0​x1=x0​z1=z0​y1=y0​z1=0.x_{0}y_{1}=y_{0}x_{1}=z_{0}x_{1}=x_{0}z_{1}=z_{0}y_{1}=y_{0}z_{1}=0.

It is then straightforward to verify that Γ​(S1!)={e1Γ—e1,e2Γ—e2,e3Γ—e3}.\Gamma(S_{1}^{!})=\{e_{1}\times e_{1},e_{2}\times e_{2},e_{3}\times e_{3}\}. ∎

The following theorem characterizes the S​(a,b,c)S(a,b,c) of type EC that contain a one-generated skew polynomial ring.

Theorem 6.2.

Let S​(a,b,c)S(a,b,c) be a three-dimensional Sklyanin algebra of type EC. Assume that char​𝕂≠2,3{\rm char}\ \mathbb{K}\neq 2,3.

  • (1)

    If r,s∈S​(a,b,c)1r,s\in S(a,b,c)_{1} are linearly independent and r​s=q​s​rrs=qsr for qβˆˆπ•‚βˆ—q\in\mathbb{K}^{*}, then q=βˆ’1q=-1 and a=ba=b.

  • (2)

    If the algebra S​(1,1,c)S(1,1,c) is of type EC, then there exist r,s∈S​(1,1,c)1r,s\in S(1,1,c)_{1} that are linearly independent and r​s=βˆ’s​rrs=-sr. More precisely, up to scaling in each component independently, the set of such pairs (r,s)(r,s) is in one-to-one correspondence with the closed points of the scheme Γ​(S​(βˆ’c,βˆ’c,2))\Gamma(S(-c,-c,2)).

Proof.

(1) Suppose that r,s∈S​(a,b,c)1r,s\in S(a,b,c)_{1} are linearly independent and r​s=q​s​rrs=qsr for some qβˆˆπ•‚βˆ—q\in\mathbb{K}^{*}. Since a​b​cβ‰ 0abc\neq 0, there is no loss of generality in assuming a=1a=1. We write r=Ξ±1​x+Ξ²1​y+Ξ³1​zr=\alpha_{1}x+\beta_{1}y+\gamma_{1}z and s=Ξ±2​x+Ξ²2​y+Ξ³2​zs=\alpha_{2}x+\beta_{2}y+\gamma_{2}z for Ξ±i,Ξ²i,Ξ³iβˆˆπ•‚\alpha_{i},\beta_{i},\gamma_{i}\in\mathbb{K}. The equation r​s=q​s​rrs=qsr implies the following identities hold in 𝕂\mathbb{K}:

(1βˆ’q)​α1​α2βˆ’c​β1​γ2+q​c​γ1​β2=0(E1)\displaystyle(1-q)\alpha_{1}\alpha_{2}-c\beta_{1}\gamma_{2}+qc\gamma_{1}\beta_{2}=0\quad(E_{1})
(1βˆ’q)​β1​β2βˆ’c​γ1​α2+q​c​α1​γ2=0(E2)\displaystyle(1-q)\beta_{1}\beta_{2}-c\gamma_{1}\alpha_{2}+qc\alpha_{1}\gamma_{2}=0\quad(E_{2})
(1βˆ’q)​γ1​γ2βˆ’c​α1​β2+q​c​β1​α2=0(E3)\displaystyle(1-q)\gamma_{1}\gamma_{2}-c\alpha_{1}\beta_{2}+qc\beta_{1}\alpha_{2}=0\quad(E_{3})
(1+b​q)​β1​α2βˆ’(q+b)​α1​β2=0(E4)\displaystyle(1+bq)\beta_{1}\alpha_{2}-(q+b)\alpha_{1}\beta_{2}=0\quad(E_{4})
(1+b​q)​α1​γ2βˆ’(q+b)​γ1​α2=0(E5)\displaystyle(1+bq)\alpha_{1}\gamma_{2}-(q+b)\gamma_{1}\alpha_{2}=0\quad(E_{5})
(1+b​q)​γ1​β2βˆ’(q+b)​β1​γ2=0(E6).\displaystyle(1+bq)\gamma_{1}\beta_{2}-(q+b)\beta_{1}\gamma_{2}=0\quad(E_{6}).

We refer to this set of equations as system (E)(E). We view system (E)(E) as the defining equations of Γ​(A)\Gamma(A), where AA is the quotient of π•‚β€‹βŸ¨x,y,z⟩\mathbb{K}\langle x,y,z\rangle by the relations:

(1βˆ’q)​x2βˆ’c​y​z+q​c​z​y,(1βˆ’q)​y2βˆ’c​z​x+q​c​x​z,(1βˆ’q)​z2βˆ’c​x​y+q​c​y​x,\displaystyle(1-q)x^{2}-cyz+qczy,\qquad(1-q)y^{2}-czx+qcxz,\qquad(1-q)z^{2}-cxy+qcyx,
(1+b​q)​y​xβˆ’(q+b)​x​y,(1+b​q)​x​zβˆ’(q+b)​z​x,(1+b​q)​z​yβˆ’(q+b)​y​z.\displaystyle(1+bq)yx-(q+b)xy,\qquad(1+bq)xz-(q+b)zx,\qquad(1+bq)zy-(q+b)yz.

Then we identify rr and ss with components of a closed point pβˆˆΞ“β€‹(A)p\in\Gamma(A). Observe that under this identification, if pβˆˆΞ”β€‹(β„™2)p\in\Delta({\mathbb{P}}^{2}), where Ξ”:β„™2β†’β„™2Γ—β„™2\Delta:{\mathbb{P}}^{2}\to{\mathbb{P}}^{2}\times{\mathbb{P}}^{2} is the diagonal embedding, then rr and ss are linearly dependent. We consider several cases.

First, if q=1q=1, then A=𝕂​[x,y,z]A=\mathbb{K}[x,y,z] is the polynomial ring on three variables. Since Γ​(𝕂​[x,y,z])=Δ​(β„™2)\Gamma(\mathbb{K}[x,y,z])=\Delta({\mathbb{P}}^{2}), any rr and ss whose coefficients satisfy system (E)(E) must be linearly dependent, a contradiction. We assume henceforth that qβ‰ 1q\neq 1.

If 1+b​q=q+b=01+bq=q+b=0, then q=βˆ’1q=-1 and b=1b=1, and we have the conclusion of (1). So we assume, henceforth, that 1+b​qβ‰ 01+bq\neq 0, or b+qβ‰ 0b+q\neq 0. Under this assumption it is clear that the six defining relations of AA are linearly independent. Consider the quadratic dual A!A^{!}; one checks that A!=S​(1+b​q,q+b,c​(1+q)).A^{!}=S(1+bq,q+b,c(1+q)). It is possible that this algebra is a degenerate Sklyanin algebra.

If q=βˆ’1q=-1 and bβ‰ 1b\neq 1, then Proposition 6.1(2) shows that system (E)(E) has no solutions, a contradiction. Hence, for the remainder of the proof, we assume that qβ‰ βˆ’1q\neq-1. If we suppose that A!A^{!} is not a degenerate Sklyanin algebra, then Proposition 6.1(1) shows that system (E)(E) has no solutions, a contradiction.

Finally, we rule out the possibility that A!A^{!} is a degenerate Sklyanin algebra. Suppose that this is the case. Note that c​(1+q)β‰ 0c(1+q)\neq 0, and recall that 1+b​qβ‰ 01+bq\neq 0, or b+qβ‰ 0b+q\neq 0, so [1+bq:b+q:c(1+q)]βˆ‰{e1,e2,e3}[1+bq:b+q:c(1+q)]\notin\{e_{1},e_{2},e_{3}\}. Hence, without loss of generality,

(1+b​q)3=(b+q)3=(c​(1+q))3=1.(1+bq)^{3}=(b+q)^{3}=(c(1+q))^{3}=1.

If 1+b​q=b+q1+bq=b+q, then A!β‰…S1A^{!}\cong S_{1}, and Proposition 6.1(3) implies that Γ​(A)\Gamma(A) is contained in Δ​(β„™2)\Delta({\mathbb{P}}^{2}), so rr and ss are linearly dependent, a contradiction. If 1+b​qβ‰ b+q1+bq\neq b+q, then A!β‰…S2A^{!}\cong S_{2}. Let Ξ±=1+b​q\alpha=1+bq, Ξ²=b+q\beta=b+q, Ξ³=c​(1+q)\gamma=c(1+q). Define elements of S​(1,b,c)S(1,b,c) by

r=Ξ±βˆ’1​x+Ξ²βˆ’1​y+Ξ³βˆ’1​z,s=Ξ²βˆ’1​x+Ξ±βˆ’1​y+Ξ³βˆ’1​z,t=α​β​γ​x+α​β​γ​y+z.r=\alpha^{-1}x+\beta^{-1}y+\gamma^{-1}z,\qquad s=\beta^{-1}x+\alpha^{-1}y+\gamma^{-1}z,\qquad t=\alpha\beta\gamma x+\alpha\beta\gamma y+z.

It is easy to check that {r,s,t}\{r,s,t\} is linearly independent and, using system (E)(E),

r​sβˆ’q​s​r=r​tβˆ’q​r​t=s​tβˆ’q​t​s=0.rs-qsr=rt-qrt=st-qts=0.

Hence S​(1,b,c)β‰…S​(1,βˆ’q,0)S(1,b,c)\cong S(1,-q,0). However, the point scheme of the algebra S​(1,βˆ’q,0)S(1,-q,0) is not an elliptic curve, a contradiction.

For (2), we assume S​(1,1,c)S(1,1,c) is a Sklyanin algebra of type EC. Therefore cβ‰ 0c\neq 0 and (3​c)3β‰ (2+c3)3(3c)^{3}\neq(2+c^{3})^{3}, so

(2+c3)3βˆ’(3​c)3=(c3βˆ’1)2​(c3+8)β‰ 0.(2+c^{3})^{3}-(3c)^{3}=(c^{3}-1)^{2}(c^{3}+8)\neq 0.

Setting a=b=1=βˆ’qa=b=1=-q, we see that the algebra AA defined above is S​(βˆ’c,βˆ’c,2)S(-c,-c,2). This algebra is a degenerate Sklyanin if and only if c3=βˆ’8c^{3}=-8, so S​(βˆ’c,βˆ’c,2)S(-c,-c,2) is a three-dimensional Sklyanin algebra. Moreover, S​(βˆ’c,βˆ’c,2)S(-c,-c,2) is also of type EC; for if (6​c2)3=(8βˆ’2​c3)3(6c^{2})^{3}=(8-2c^{3})^{3}, then

(6​c2)3βˆ’(8βˆ’2​c3)3=8​(c3βˆ’1)​(c3+8)2=0,(6c^{2})^{3}-(8-2c^{3})^{3}=8(c^{3}-1)(c^{3}+8)^{2}=0,

which contradicts the assumption that S​(1,1,c)S(1,1,c) is of type EC. The automorphism of the point scheme of S​(βˆ’c,βˆ’c,2)S(-c,-c,2) is translation by [βˆ’c:βˆ’c:2][-c:-c:2] in the group law with identity element [1:βˆ’1:0][1:-1:0], hence, no closed points of Γ​(S​(βˆ’c,βˆ’c,2))\Gamma(S(-c,-c,2)) lie on Δ​(β„™2)\Delta({\mathbb{P}}^{2}). We conclude that for every point

[Ξ±1:Ξ²1,Ξ³1]Γ—[Ξ±2:Ξ²2:Ξ³2]βˆˆΞ“(S(βˆ’c,βˆ’c,2)),[\alpha_{1}:\beta_{1},\gamma_{1}]\times[\alpha_{2}:\beta_{2}:\gamma_{2}]\in\Gamma(S(-c,-c,2)),

if r=Ξ±1​x+Ξ²1​y+Ξ³1​zr=\alpha_{1}x+\beta_{1}y+\gamma_{1}z and s=Ξ±2​x+Ξ²2​y+Ξ³2​zs=\alpha_{2}x+\beta_{2}y+\gamma_{2}z are elements in S​(1,1,c)1S(1,1,c)_{1}, then rr and ss are linearly independent and r​s=βˆ’s​rrs=-sr. Conversely, a pair (r,s)(r,s) of such rr and ss, up to scaling in each component independently, determines a unique closed point in Γ​(S​(βˆ’c,βˆ’c,2))\Gamma(S(-c,-c,2)). ∎

Remark 6.3.

The condition in Theorem 6.2 (2): S​(1,1,c)S(1,1,c) is of type EC is not necessary for the existence of stated rr and ss. For example, if c3=βˆ’8c^{3}=-8, then S​(1,1,c)S(1,1,c) is not of type EC, and A=S​(βˆ’c,βˆ’c,2)A=S(-c,-c,2) is a degenerate Sklyanin algebra. By [10], provided char​𝕂≠3{\rm char}\ \mathbb{K}\neq 3, Aβ‰…π•‚β€‹βŸ¨u,v,w⟩/⟨u2,v2,w2⟩A\cong\mathbb{K}\langle u,v,w\rangle/\langle u^{2},v^{2},w^{2}\rangle. One checks that AA is semi-standard, and Γ​(A)\Gamma(A) is a nonempty, non-identity relation on E=𝒡​(u​v​w)E=\mathcal{Z}(uvw). Thus Γ​(A)\Gamma(A) is not contained in Δ​(β„™2)\Delta({\mathbb{P}}^{2}), and one can use the isomorphism in [10] to find linearly independent r,s∈S​(1,1,c)1r,s\in S(1,1,c)_{1} such that r​s=βˆ’s​rrs=-sr.

Proposition 6.4.

Assume char​𝕂≠2,3{\rm char}\ \mathbb{K}\neq 2,3 and let jβˆˆπ•‚j\in\mathbb{K}. The number of distinct isomorphism classes of algebras S​(1,1,c)S(1,1,c) of type EC whose point scheme EE has j-invariant j​(E)=jj(E)=j is:

  • β€’

    three, if j≠0,123j\neq 0,12^{3},

  • β€’

    one, if j=0j=0,

  • β€’

    two, if j=123j=12^{3}.

Proof.

Observing that the automorphism Οƒ\sigma of the point scheme of S​(1,1,c)S(1,1,c) is translation by [1:1:c][1:1:c], a point of order 2, the proof is identical to that of [6, Proposition 3.10], with the obvious necessary change from type B to type A. ∎

We complete our characterization of when an algebra S​(a,b,c)S(a,b,c) of type EC contains a two-dimensional AS-regular subalgebra by showing that no three-dimensional Sklyanin algebras contain a Jordan plane generated in degree 1.

Proposition 6.5.

Let S​(a,b,c)S(a,b,c) be a three-dimensional Sklyanin algebra such that a​b​cβ‰ 0abc\neq 0. Assume char​𝕂≠2,3{\rm char}\ \mathbb{K}\neq 2,3. If r,s∈S​(a,b,c)1r,s\in S(a,b,c)_{1} satisfy r​s=s​rβˆ’s2rs=sr-s^{2}, then rr and ss are linearly dependent.

Proof.

Suppose r,s∈S​(a,b,c)1r,s\in S(a,b,c)_{1} satisfy r​s=s​rβˆ’s2rs=sr-s^{2}, and a​b​cβ‰ 0abc\neq 0. Without loss of generality, we assume a=1a=1 and write r=Ξ±1​x+Ξ²1​y+Ξ³1​zr=\alpha_{1}x+\beta_{1}y+\gamma_{1}z and s=Ξ±2​x+Ξ²2​y+Ξ³2​zs=\alpha_{2}x+\beta_{2}y+\gamma_{2}z for Ξ±i,Ξ²i,Ξ³iβˆˆπ•‚\alpha_{i},\beta_{i},\gamma_{i}\in\mathbb{K}. Examining the coefficients of x2x^{2}, y2y^{2}, z2z^{2} in the equation r​s=s​rβˆ’s2rs=sr-s^{2} implies the following identities hold in 𝕂\mathbb{K}:

Ξ±22βˆ’c​β1​γ2+c​γ1​β2βˆ’c​β2​γ2\displaystyle\alpha_{2}^{2}-c\beta_{1}\gamma_{2}+c\gamma_{1}\beta_{2}-c\beta_{2}\gamma_{2} =0(E1)\displaystyle=0\qquad(E_{1})
Ξ²22βˆ’c​γ1​α2+c​α1​γ2βˆ’c​α2​γ2\displaystyle\beta_{2}^{2}-c\gamma_{1}\alpha_{2}+c\alpha_{1}\gamma_{2}-c\alpha_{2}\gamma_{2} =0(E2)\displaystyle=0\qquad(E_{2})
Ξ³22βˆ’c​α1​β2+c​β1​α2βˆ’c​α2​β2\displaystyle\gamma_{2}^{2}-c\alpha_{1}\beta_{2}+c\beta_{1}\alpha_{2}-c\alpha_{2}\beta_{2} =0(E3).\displaystyle=0\qquad(E_{3}).

The linear combination Ξ±2​(E1)+Ξ²2​(E2)+Ξ³2​(E3)\alpha_{2}(E_{1})+\beta_{2}(E_{2})+\gamma_{2}(E_{3}) yields

(2) Ξ±23+Ξ²23+Ξ³23βˆ’3​c​α2​β2​γ2=0.\alpha_{2}^{3}+\beta_{2}^{3}+\gamma_{2}^{3}-3c\alpha_{2}\beta_{2}\gamma_{2}=0.

Examining the coefficients of z​yzy, x​zxz, y​xyx in the equation r​s=s​rβˆ’s2rs=sr-s^{2} implies:

(1+b)​γ1​β2βˆ’(1+b)​β1​γ2+(1βˆ’b)​β2​γ2\displaystyle(1+b)\gamma_{1}\beta_{2}-(1+b)\beta_{1}\gamma_{2}+(1-b)\beta_{2}\gamma_{2} =0(E1β€²)\displaystyle=0\qquad(E^{\prime}_{1})
(1+b)​α1​γ2βˆ’(1+b)​γ1​α2+(1βˆ’b)​α2​γ2\displaystyle(1+b)\alpha_{1}\gamma_{2}-(1+b)\gamma_{1}\alpha_{2}+(1-b)\alpha_{2}\gamma_{2} =0(E2β€²)\displaystyle=0\qquad(E^{\prime}_{2})
(1+b)​β1​α2βˆ’(1+b)​α1​β2+(1βˆ’b)​α2​β2\displaystyle(1+b)\beta_{1}\alpha_{2}-(1+b)\alpha_{1}\beta_{2}+(1-b)\alpha_{2}\beta_{2} =0(E3β€²).\displaystyle=0\qquad(E^{\prime}_{3}).

The linear combinations c​(Eiβ€²)βˆ’(1+b)​(Ei)c(E^{\prime}_{i})-(1+b)(E_{i}) for i=1,2,3i=1,2,3 show:

(1+b)​α22=2​c​β2​γ2,(1+b)​β22=2​c​α2​γ2,(1+b)​γ22=2​c​α2​β2.(1+b)\alpha_{2}^{2}=2c\beta_{2}\gamma_{2},\qquad(1+b)\beta_{2}^{2}=2c\alpha_{2}\gamma_{2},\qquad(1+b)\gamma_{2}^{2}=2c\alpha_{2}\beta_{2}.

If b=βˆ’1b=-1, then since cβ‰ 0c\neq 0, these equations imply that at least two of Ξ±2,Ξ²2,Ξ³2\alpha_{2},\beta_{2},\gamma_{2} are zero. It then follows from (E1)(E_{1}), (E2)(E_{2}), (E3)(E_{3}) that all of Ξ±2,Ξ²2,Ξ³2\alpha_{2},\beta_{2},\gamma_{2} are zero, so s=0s=0. Suppose that b+1β‰ 0b+1\neq 0. Note that the last three displayed equations show that

(1+b)​α23=2​c​α2​β2​γ2=(1+b)​β23=(1+b)​γ23.(1+b)\alpha_{2}^{3}=2c\alpha_{2}\beta_{2}\gamma_{2}=(1+b)\beta_{2}^{3}=(1+b)\gamma_{2}^{3}.

Thus Ξ±23=Ξ²23=Ξ³23\alpha_{2}^{3}=\beta_{2}^{3}=\gamma_{2}^{3} and equation (2) implies 3​(1βˆ’b)​α23=0.3(1-b)\alpha_{2}^{3}=0. If Ξ±2=0\alpha_{2}=0, then s=0s=0. If b=1b=1, equations (E1β€²)(E^{\prime}_{1}), (E2β€²)(E^{\prime}_{2}), (E3β€²)(E^{\prime}_{3}) simplify and show that all minors of

[Ξ±1Ξ²1Ξ³1Ξ±2Ξ²2Ξ³2]\begin{bmatrix}\alpha_{1}&\beta_{1}&\gamma_{1}\\ \alpha_{2}&\beta_{2}&\gamma_{2}\\ \end{bmatrix}

vanish, whence rr and ss are linearly dependent. ∎

6.2. Certain twisted tensor products as AS-regular algebras of type A

We introduce a one-parameter family of algebras, P​(a)P(a), aβˆˆπ•‚a\in\mathbb{K}. When aβ‰ 1a\neq 1, a member of this family is both a graded twisted tensor product of π•‚βˆ’1​[r,s]\mathbb{K}_{-1}[r,s] and 𝕂​[t]\mathbb{K}[t], and an AS-regular algebra. When aβ‰ 0,1a\neq 0,1, P​(a)P(a) is of type EC, subtype A. We show that every algebra in the family S​(1,1,c)S(1,1,c) of Sklyanin algebras is isomorphic to some P​(a)P(a), and hence is a graded twisted tensor product of π•‚βˆ’1​[r,s]\mathbb{K}_{-1}[r,s] and 𝕂​[t]\mathbb{K}[t].

Assuming that char​𝕂≠2{\rm char}\ \mathbb{K}\neq 2, for any aβˆˆπ•‚a\in\mathbb{K}, we define

P​(a)=π•‚β€‹βŸ¨r,s,t⟩⟨r​s+s​r,t​r+r​tβˆ’t2βˆ’a​r2,t​(rβˆ’s)+(rβˆ’s)​t+2​s2⟩.P(a)=\dfrac{\mathbb{K}\langle r,s,t\rangle}{\langle rs+sr,tr+rt-t^{2}-ar^{2},t(r-s)+(r-s)t+2s^{2}\rangle}.
Proposition 6.6.

The algebra P​(a)P(a) is a graded twisted tensor product of π•‚βˆ’1​[r,s]\mathbb{K}_{-1}[r,s] and 𝕂​[t]\mathbb{K}[t] if and only if aβ‰ 1a\neq 1. Moreover, when aβ‰ 1a\neq 1, r2,s2,r^{2},s^{2}, and t2t^{2} are central.

Proof.

Order monomials in the free algebra by left-lexicographic order via r<s<tr<s<t. Then in degree 2, the GrΓΆbner basis for the defining ideal of P​(a)P(a) is {s​r+r​s,t​sβˆ’t​r+s​tβˆ’r​tβˆ’2​s2,t2βˆ’t​rβˆ’r​t+a​r2}.\{sr+rs,ts-tr+st-rt-2s^{2},t^{2}-tr-rt+ar^{2}\}. Resolving the overlaps t​s​rtsr, t3t^{3}, and t2​st^{2}s via the Diamond Lemma yields two additional cubic GrΓΆbner basis elements:

t​r​s+t​r2βˆ’s​t​r+r​t​r+2​r​s2(1βˆ’a)​t​r2βˆ’(1βˆ’a)​r2​t.trs+tr^{2}-str+rtr+2rs^{2}\qquad(1-a)tr^{2}-(1-a)r^{2}t.

If a=1a=1, we have dim𝕂P​(a)3=11\dim_{\mathbb{K}}P(a)_{3}=11. However, any graded twisted tensor product of π•‚βˆ’1​[r,s]\mathbb{K}_{-1}[r,s] and 𝕂​[t]\mathbb{K}[t] has the same Hilbert series as π•‚βˆ’1​[r,s]βŠ—π•‚π•‚β€‹[t]\mathbb{K}_{-1}[r,s]\otimes_{\mathbb{K}}\mathbb{K}[t], namely (1βˆ’z)βˆ’3(1-z)^{-3}. Thus aβ‰ 1a\neq 1 is necessary for P​(a)P(a) to be a graded twisted tensor product, and we assume this condition holds for the remainder of the proof. It is now straightforward to check that the newly-introduced overlaps t2​r​st^{2}rs, t2​r2t^{2}r^{2}, and t​r​s​rtrsr resolve, hence

s​r+r​s,t​sβˆ’t​r+s​tβˆ’r​tβˆ’2​s2,t2βˆ’t​rβˆ’r​t+a​r2,sr+rs,\qquad ts-tr+st-rt-2s^{2},\qquad t^{2}-tr-rt+ar^{2},
t​r​s+r2​tβˆ’s​t​r+r​t​r+2​r​s2,t​r2βˆ’r2​ttrs+r^{2}t-str+rtr+2rs^{2},\qquad tr^{2}-r^{2}t

constitutes a GrΓΆbner basis for the defining ideal of P​(a)P(a), and

{ri​sj​(t​r)k​tΟ΅|i,j,kβ‰₯0,ϡ∈{0,1}}\{r^{i}s^{j}(tr)^{k}t^{\epsilon}\ |\ i,j,k\geq 0,\epsilon\in\{0,1\}\}

is a 𝕂\mathbb{K}-basis for P​(a)P(a). An easy counting argument shows the Hilbert series of P​(a)P(a) is (1βˆ’z)βˆ’3(1-z)^{-3}. It is also easy to check that r2,s2,r^{2},s^{2}, and t2t^{2} are central.

To complete the proof, we show that {ri​sj​tk|i,j,kβ‰₯0}\{r^{i}s^{j}t^{k}\ |\ i,j,k\geq 0\} is a spanning set for P​(a)P(a). Let UU be the 𝕂\mathbb{K}-linear subspace of P​(a)P(a) spanned by {ri​sj​tk|i,j,kβ‰₯0}\{r^{i}s^{j}t^{k}\ |\ i,j,k\geq 0\}. Given an arbitrary monomial m∈P​(a)m\in P(a) in the generators r,s,tr,s,t, we need to show that m∈Um\in U. Since rr and ss skew commute and t2t^{2} is central, it suffices to show that t​ri​sj∈Utr^{i}s^{j}\in U for all i,jβ‰₯0i,j\geq 0. Observe that the defining relations show that t​rtr and t​sts are both in UU. Write i=2​q+pi=2q+p, j=2​qβ€²+pβ€²j=2q^{\prime}+p^{\prime} for some integers p,pβ€²,q,qβ€²p,p^{\prime},q,q^{\prime} with p,pβ€²βˆˆ{0,1}p,p^{\prime}\in\{0,1\}. Using the fact that r2r^{2} and s2s^{2} are central, we have

t​ri​sj=t​r2​q​rp​s2​q′​spβ€²=r2​q​s2​q′​t​rp​spβ€².tr^{i}s^{j}=tr^{2q}r^{p}s^{2q^{\prime}}s^{p^{\prime}}=r^{2q}s^{2q^{\prime}}tr^{p}s^{p^{\prime}}.

If p=0p=0, it is clear that the last expression is in UU. If p=1p=1, then note that t​r​spβ€²=(a​r2βˆ’r​t+t2)​sp′≑r​t​sp′≑0(modU).trs^{p^{\prime}}=(ar^{2}-rt+t^{2})s^{p^{\prime}}\equiv rts^{p^{\prime}}\equiv 0\pmod{U}. ∎

Proposition 6.7.

The algebra P​(a)P(a) is AS-regular if and only if aβ‰ 1a\neq 1.

Proof.

Let S=P​(a)S=P(a) and let F=π•‚β€‹βŸ¨r,s,t⟩F=\mathbb{K}\langle r,s,t\rangle be the free algebra. The defining quadratic relations of P​(a)P(a) are:

f1=r​s+s​r,f2=t​r+r​tβˆ’t2βˆ’a​r2,f3=t​(rβˆ’s)+(rβˆ’s)​t+2​s2.f_{1}=rs+sr,\quad f_{2}=tr+rt-t^{2}-ar^{2},\quad f_{3}=t(r-s)+(r-s)t+2s^{2}.

We have M​[r​s​t]T=[f1​f2​f3]TM[r\ s\ t]^{T}=[f_{1}\ f_{2}\ f_{3}]^{T}, where

M=[sr0tβˆ’a​r0rβˆ’tt2​sβˆ’trβˆ’s].M=\begin{bmatrix}s&r&0\\ t-ar&0&r-t\\ t&2s-t&r-s\end{bmatrix}.

Let EE be the closed subscheme of β„™2{\mathbb{P}}^{2} determined by detM\det M. Recall that SS is nondegenerate provided that the rank of MM is equal to 22 at every closed point of EE. Let us write M​(p)M(p) for the matrix MM evaluated at a closed point p∈Ep\in E. If [r:s:t]∈E[r:s:t]\in E, rβ‰ 0r\neq 0 or sβ‰ 0s\neq 0, and rβ‰ sr\neq s or rβ‰ tr\neq t, then it is clear that rankM(r:s:t)=2{\rm rank\ }M(r:s:t)=2. If r=s=0r=s=0, the second and third rows of M(0:0:1)M(0:0:1) show that rankM(0:0:1)=2{\rm rank\ }M(0:0:1)=2. At the point [1:1:1]∈E[1:1:1]\in E,

M(1:1:1)=[1101βˆ’a00110],M(1:1:1)=\begin{bmatrix}1&1&0\\ 1-a&0&0\\ 1&1&0\end{bmatrix},

so the condition a≠1a\neq 1 is equivalent to rankM(1:1:1)=2{\rm rank\ }M(1:1:1)=2. We conclude that SS is nondegenerate if and only if a≠1a\neq 1.

Assume that a≠1a\neq 1. We now show that SS is a standard algebra. Let

P=[a​(sβˆ’r)tβˆ’2​s+a​rsβˆ’ttβˆ’2​s+a​rβˆ’2​t+4​sβˆ’2​rtβˆ’2​s+rsβˆ’ttβˆ’2​s+rsβˆ’r]P=\begin{bmatrix}a(s-r)&t-2s+ar&s-t\\ t-2s+ar&-2t+4s-2r&t-2s+r\\ s-t&t-2s+r&s-r\\ \end{bmatrix}

and define r1,r2,r3∈Fr_{1},r_{2},r_{3}\in F via P​[r​s​t]T=[r1​r2​r3]TP[r\ s\ t]^{T}=[r_{1}\ r_{2}\ r_{3}]^{T}. Note that P=PTP=P^{T} so the algebra Fβ€²=F/⟨r1,r2,r3⟩F^{\prime}=F/\langle r_{1},r_{2},r_{3}\rangle is standard. We shall prove that Fβ€²=P​(a)F^{\prime}=P(a). Since PP is symmetric, it suffices to show that the entries of [r​s​t]​P[r\ s\ t]P span the defining quadratic relations of P​(a)P(a). One checks that

[r​s​t]​P=[f1f2f3]​[aβˆ’211βˆ’10βˆ’12βˆ’1].[r\ s\ t]P=\begin{bmatrix}f_{1}&f_{2}&f_{3}\end{bmatrix}\begin{bmatrix}a&-2&1\\ 1&-1&0\\ -1&2&-1\end{bmatrix}.

Moreover, the determinant of the last matrix is equal to aβˆ’1a-1. Hence [r​s​t]​P[r\ s\ t]P spans the quadratic relations of P​(a)P(a). Therefore SS is standard. We conclude by [1, Theorem 1] that SS is AS-regular of dimension 3. ∎

Proposition 6.8.

Assume char​𝕂≠2,3{\rm char}\ \mathbb{K}\neq 2,3. Let aβˆˆπ•‚a\in\mathbb{K} such that aβ‰ 1a\neq 1.

  • (1)

    The point scheme of P​(a)P(a) is an elliptic curve if and only if aβ‰ 0a\neq 0.

  • (2)

    The automorphism of the point scheme of P​(a)P(a) has order 2.

  • (3)

    Every elliptic curve, up to isomorphism, is the point scheme of some P​(a)P(a).

Proof.

The condition aβ‰ 1a\neq 1, by Proposition 6.7, guarantees that P​(a)P(a) is AS-regular, and so the point scheme of P​(a)P(a) and its associated automorphism are defined. The matrix MM for P​(a)P(a) is given in the proof of Proposition 6.7. One then checks that the point scheme of P​(a)P(a) is given by Ea=𝒡​(F)E_{a}=\mathcal{Z}(F), where

F=detM=a​r3βˆ’a​r2​sβˆ’2​r​s2+2​r​s​t+2​s2​tβˆ’r​t2βˆ’s​t2.F=\det M=ar^{3}-ar^{2}s-2rs^{2}+2rst+2s^{2}t-rt^{2}-st^{2}.

We note that βˆ‚Fβˆ‚t=2​(r+s)​(sβˆ’t)\frac{\partial F}{\partial t}=2(r+s)(s-t), and it follows that the only points satisfying F=βˆ‚Fβˆ‚t=0F=\frac{\partial F}{\partial t}=0 are [0:0:1][0:0:1], [1:1:1][1:1:1] and [x:y:y][x:y:y] where a​x2=y2ax^{2}=y^{2}. One readily checks that none of these points are singular when a​(aβˆ’1)β‰ 0a(a-1)\neq 0. Conversely, if a=0a=0, then [1:0:0]∈Ea[1:0:0]\in E_{a} is singular. Therefore (1) holds.

The associated automorphism σa\sigma_{a} of EaE_{a} interchanges [0:0:1][0:0:1] and [1:1:1][1:1:1], and for r≠sr\neq s, computing the cross product of the first and third rows of MM shows

Οƒa([r:s:t])=[r:βˆ’s:(2s2βˆ’rtβˆ’st)/(rβˆ’s)].\sigma_{a}([r:s:t])=[r:-s:(2s^{2}-rt-st)/(r-s)].

It follows from an easy computation that Οƒa\sigma_{a} has order 2.

For (3), suppose that a​(aβˆ’1)β‰ 0a(a-1)\neq 0 so that the point scheme of P​(a)P(a) is the elliptic curve given by F=0F=0. A Weierstrass equation of this curve is

Y2​Z+2​X​Y​Zβˆ’4​(aβˆ’1)​Y​Z2=X3+(4βˆ’a)​X2​Zβˆ’4​(aβˆ’1)​X​Z2.Y^{2}Z+2XYZ-4(a-1)YZ^{2}=X^{3}+(4-a)X^{2}Z-4(a-1)XZ^{2}.

Using the formulae in [9, III.1] one checks that the jj-invariant is given by

ja=16​(a2+14​a+1)3a​(aβˆ’1)4.j_{a}=\frac{16(a^{2}+14a+1)^{3}}{a(a-1)^{4}}.

Since 𝕂\mathbb{K} is algebraically closed, this expression realizes every value in 𝕂\mathbb{K}. It is well known that the jj-invariant parametrizes elliptic curves up to isomorphism, see [9, Proposition III.1.4(b)] for example, hence (3) follows. ∎

Remark 6.9.

Suppose that aβˆˆπ•‚a\in\mathbb{K} satisfies a​(aβˆ’1)β‰ 0a(a-1)\neq 0. Let EaE_{a} denote the point scheme of the algebra P​(a)P(a). Then EaE_{a} is an elliptic curve by Proposition 6.8 (1). Let us define, for use below, points O=[0:0:1]O=[0:0:1], P=[1:1:1]P=[1:1:1] of EaE_{a}, and take OO as the identity element for the group law on EaE_{a}, for all aa. It is then straightforward, albeit tedious, to check that the automorphism Οƒa\sigma_{a} is translation by the point PP.

Theorem 6.10.

If a​(aβˆ’1)β‰ 0a(a-1)\neq 0, then P​(a)β‰…P​(aβ€²)P(a)\cong P(a^{\prime}) if and only if aβ€²βˆˆ{a,1/a}a^{\prime}\in\{a,1/a\}.

Proof.

Assume that aβˆˆπ•‚a\in\mathbb{K} and a​(aβˆ’1)β‰ 0a(a-1)\neq 0. Then P​(a)P(a) is AS-regular of type EC, and P​(a)P(a) is a geometric algebra. Clearly P​(a)≇P​(aβ€²)P(a)\ncong P(a^{\prime}) if aβ€²βˆˆ{0,1}a^{\prime}\in\{0,1\}, so suppose P​(a)β‰…P​(aβ€²)P(a)\cong P(a^{\prime}) for a′​(aβ€²βˆ’1)β‰ 0.a^{\prime}(a^{\prime}-1)\neq 0. By Theorem 2.6, it suffices to characterize projective equivalences ψ:Eaβ†’Eaβ€²\psi:E_{a}\to E_{a^{\prime}} such that Οˆβ€‹Οƒa=Οƒaβ€²β€‹Οˆ\psi\sigma_{a}=\sigma_{a^{\prime}}\psi. Let ψ\psi be such an equivalence.

The point O=[0:0:1]O=[0:0:1] is a flex point for both EaE_{a} and Eaβ€²E_{a^{\prime}}. It is well known that a projective equivalence preserves the set of flex points and that the set of flex points is equal to the set of 33-torsion points. Hence Οˆβ€‹(O)\psi(O) is a 3-torsion point for Eaβ€²E_{a^{\prime}}. Since translation by any 3-torsion point extends to an automorphism of β„™2{\mathbb{P}}^{2}, see [7, Lemma 5.3] for example, the map Οˆβ€²=Ο„βˆ’Οˆβ€‹(O)β€‹Οˆ:Eaβ†’Eaβ€²\psi^{\prime}=\tau_{-\psi(O)}\psi:E_{a}\to E_{a^{\prime}}, where Ο„βˆ’Οˆβ€‹(O)\tau_{-\psi(O)} is translation on Eaβ€²E_{a^{\prime}} by the point βˆ’Οˆβ€‹(O)-\psi(O), is a projective equivalence. Moreover, by Remark 6.9, Οƒaβ€²\sigma_{a^{\prime}} is a translation and one checks that Οˆβ€²β€‹Οƒa=Οƒaβ€²β€‹Οˆβ€²\psi^{\prime}\sigma_{a}=\sigma_{a^{\prime}}\psi^{\prime}. Therefore there is no loss of generality in assuming Οˆβ€‹(O)=O\psi(O)=O, and that ψ\psi is represented (up to scale) by an invertible matrix of the form

[a11a120a21a220a31a321].\begin{bmatrix}a_{11}&a_{12}&0\\ a_{21}&a_{22}&0\\ a_{31}&a_{32}&1\end{bmatrix}.

Since Οƒa([0:0:1])=[1:1:1]\sigma_{a}([0:0:1])=[1:1:1], we see ψ([1:1:1])=[1:1:1]\psi([1:1:1])=[1:1:1] and it follows that

a11+a12=a21+a22=a31+a32+1.a_{11}+a_{12}=a_{21}+a_{22}=a_{31}+a_{32}+1.

For the remainder of the proof we consider the action of ψ\psi on p∈Eaβˆ’{O,P}.p\in E_{a}-\{O,P\}. It is easy to check that [0:0:1][0:0:1] and [1:1:1][1:1:1] are the only points on EaE_{a} with r=sr=s, and [0:0:1][0:0:1] is the only point where r+s=0r+s=0. Thus p=[r:s:t]p=[r:s:t] with (rβˆ’s)​(r+s)β‰ 0(r-s)(r+s)\neq 0. The equation Οˆβ€‹Οƒa=Οƒaβ€²β€‹Οˆ\psi\sigma_{a}=\sigma_{a^{\prime}}\psi implies that there exists a scalar Kpβ‰ 0K_{p}\neq 0 such that

a11​rβˆ’a12​s=Kp​(a11​r+a12​s)\displaystyle a_{11}r-a_{12}s=K_{p}(a_{11}r+a_{12}s) (E1)\displaystyle(E_{1})
a21​rβˆ’a22​s=βˆ’Kp​(a21​r+a22​s)\displaystyle a_{21}r-a_{22}s=-K_{p}(a_{21}r+a_{22}s) (E2)\displaystyle(E_{2})
a31​rβˆ’a32​s+(2​s2βˆ’r​tβˆ’s​t)/(rβˆ’s)=Kp​(2​S2βˆ’R​Tβˆ’S​T)/(Rβˆ’S)\displaystyle a_{31}r-a_{32}s+(2s^{2}-rt-st)/(r-s)=K_{p}(2S^{2}-RT-ST)/(R-S) (E3),\displaystyle(E_{3}),

where R=a11​r+a12​s,R=a_{11}r+a_{12}s, S=a21​r+a22​sS=a_{21}r+a_{22}s, and T=a31​r+a32​s+tT=a_{31}r+a_{32}s+t. (The conditions a11+a12=a21+a22a_{11}+a_{12}=a_{21}+a_{22} and ψ\psi is invertible ensure that Rβˆ’Sβ‰ 0R-S\neq 0.) Since a11+a12=a21+a22a_{11}+a_{12}=a_{21}+a_{22}, subtracting (E2)(E_{2}) from (E1)(E_{1}) yields

(a11βˆ’a21)​(r+s)=Kp​[(a11+a21)​r+(a12+a22)​s].(a_{11}-a_{21})(r+s)=K_{p}[(a_{11}+a_{21})r+(a_{12}+a_{22})s].

Since ψ\psi is invertible and r+sβ‰ 0r+s\neq 0, the left side is nonzero, hence

Kp=(a11βˆ’a21)​(r+s)(a11+a21)​r+(a12+a22)​s.K_{p}=\dfrac{(a_{11}-a_{21})(r+s)}{(a_{11}+a_{21})r+(a_{12}+a_{22})s}.

Now equation (E1)(E_{1}) can be rewritten as a11​a21​r2βˆ’a12​a22​s2=0a_{11}a_{21}r^{2}-a_{12}a_{22}s^{2}=0. Since this homogeneous equation holds for all p∈Eaβˆ’{O,P}p\in E_{a}-\{O,P\}, we have a11​a21=a12​a22=0a_{11}a_{21}=a_{12}a_{22}=0. Thus either (i) a12=a21=0a_{12}=a_{21}=0, a11=a22β‰ 0a_{11}=a_{22}\neq 0, and Kp=1K_{p}=1, or (ii) a11=a22=0a_{11}=a_{22}=0, a12=a21β‰ 0a_{12}=a_{21}\neq 0, and Kp=βˆ’1K_{p}=-1.

In case (i), since equation (E3)(E_{3}) holds for all p∈Eaβˆ’{O,P}p\in E_{a}-\{O,P\}, we see that a31=0a_{31}=0 and a32=a11βˆ’1a_{32}=a_{11}-1. Then ψ([r:s:t])=[a11r:a11s:(a11βˆ’1)s+t]\psi([r:s:t])=[a_{11}r:a_{11}s:(a_{11}-1)s+t]. Using the assumption that [r:s:t]∈Ea[r:s:t]\in E_{a}, the condition ψ([r:s:t])∈Eaβ€²\psi([r:s:t])\in E_{a^{\prime}} is equivalent to

(a′​a112βˆ’a)​r3βˆ’(a′​a112βˆ’a)​r2​sβˆ’(a112βˆ’1)​r​s2+(a112βˆ’1)​s3=0.(a^{\prime}a_{11}^{2}-a)r^{3}-(a^{\prime}a_{11}^{2}-a)r^{2}s-(a_{11}^{2}-1)rs^{2}+(a_{11}^{2}-1)s^{3}=0.

This equation holds for all p∈Eaβˆ’{O,P}p\in E_{a}-\{O,P\} if and only if a=aβ€²a=a^{\prime} and a112=1a_{11}^{2}=1.

Similarly, in case (ii), considering (E3)(E_{3}) yields a31=a12a_{31}=a_{12} and a32=βˆ’1a_{32}=-1. So ψ([r:s:t])=[a12s:a12r:a12rβˆ’s+t]\psi([r:s:t])=[a_{12}s:a_{12}r:a_{12}r-s+t]. Using [r:s:t]∈Ea[r:s:t]\in E_{a}, the condition Ο•([r:s:t])∈Eaβ€²\phi([r:s:t])\in E_{a^{\prime}} is equivalent to

(a122βˆ’a)​r3βˆ’(a122βˆ’a)​r2​sβˆ’(a′​a12βˆ’1)​r​s2+(a′​a122βˆ’1)​s3=0.(a_{12}^{2}-a)r^{3}-(a_{12}^{2}-a)r^{2}s-(a^{\prime}a_{12}-1)rs^{2}+(a^{\prime}a_{12}^{2}-1)s^{3}=0.

This equation holds for all p∈Eaβˆ’{O,P}p\in E_{a}-\{O,P\} if and only if a212=aa_{21}^{2}=a and a′​a=1a^{\prime}a=1. The result follows. ∎

Corollary 6.11.

For jβˆˆπ•‚j\in\mathbb{K}, the number of distinct isomorphism classes of algebras P​(a)P(a) such that a​(aβˆ’1)β‰ 0a(a-1)\neq 0 and the point scheme EaE_{a} has j-invariant ja=jj_{a}=j is:

  • (1)

    three, if j≠0,123j\neq 0,12^{3},

  • (2)

    one, if j=0j=0, and

  • (3)

    two, if j=123j=12^{3}.

Proof.

Recall that for a​(aβˆ’1)β‰ 0a(a-1)\neq 0, the j-invariant of the elliptic curve EaE_{a} is given by ja=16​(a2+14​a+1)3/a​(aβˆ’1)4.j_{a}=16(a^{2}+14a+1)^{3}/a(a-1)^{4}. Observe that ja=j1/aj_{a}=j_{1/a}, so solutions to ja=jj_{a}=j occur in mutually inverse pairs. By Theorem 6.10, each pair corresponds to a single isomorphism class in the family P​(a)P(a).

If j=0j=0, then the equation ja=0j_{a}=0 has two distinct solutions, so (2) follows.

If j≠0j\neq 0, define a polynomial

fj​(x)=(x2+14​x+1)3βˆ’(j/16)​x​(xβˆ’1)4βˆˆπ•‚β€‹[t].f_{j}(x)=(x^{2}+14x+1)^{3}-(j/16)x(x-1)^{4}\in\mathbb{K}[t].

Observe that ja=jj_{a}=j if and only if aa is a zero of fj​(x)f_{j}(x). It is readily checked that

(x2+14​x+1)​fj′​(x)βˆ’6​(x+7)​fj​(x)=(j/16)​(xβˆ’1)3​(x+1)​(x2βˆ’34​x+1).(x^{2}+14x+1)f^{\prime}_{j}(x)-6(x+7)f_{j}(x)=(j/16)(x-1)^{3}(x+1)(x^{2}-34x+1).

Since jβ‰ 0j\neq 0 and fj​(1)β‰ 0f_{j}(1)\neq 0, if fj​(x)f_{j}(x) has a multiple root at x=ax=a, then we have (a+1)​(a2βˆ’34​a+1)=0(a+1)(a^{2}-34a+1)=0. For such an aa, fj​(a)=0f_{j}(a)=0 implies j=123j=12^{3}, so (1) follows. For (3), observe that ja=123j_{a}=12^{3} implies (a+1)2​(a2βˆ’34​a+1)2=0(a+1)^{2}(a^{2}-34a+1)^{2}=0. ∎

AS-regular algebras whose point schemes are elliptic curves have recently been classified up to isomorphism by Itaba and Matsuno in characteristic 0. In [5, Theorem 4.9], the authors provide a classification of geometric algebras whose point schemes are elliptic curves. However, not all algebras listed in [5, Theorem 4.9] are AS-regular. In [6, Theorem 3.13] (see also [6, Remark 3.9]) Matsuno completes the classification. We draw attention in particular to the family of algebras

R​(a,b,c)=π•‚β€‹βŸ¨x,y,z⟩⟨a​x​z+b​z​y+c​y​x,a​z​x+b​y​z+c​x​y,a​y2+b​x2+c​z2⟩R(a,b,c)=\frac{\mathbb{K}\langle x,y,z\rangle}{\langle axz+bzy+cyx,azx+byz+cxy,ay^{2}+bx^{2}+cz^{2}\rangle}

where [a:b:c]βˆˆβ„™2[a:b:c]\in{\mathbb{P}}^{2} is a point on EΞ»=𝒡​(x3+y3+z3βˆ’3​λ​x​y​z)E_{\lambda}=\mathcal{Z}(x^{3}+y^{3}+z^{3}-3\lambda xyz), Ξ»3β‰ 1\lambda^{3}\neq 1 such that a​b​cβ‰ 0abc\neq 0. When the jj-invariant of EΞ»E_{\lambda} is not equal to 0 or 12312^{3}, then these are the Type B algebras of [6, Table 1]; also see [5, Theorem 4.9].

Lemma 6.12.

Let [a:b:c]∈EΞ»[a:b:c]\in E_{\lambda}, Ξ»3β‰ 1\lambda^{3}\neq 1, such that a​b​cβ‰ 0abc\neq 0. If dim𝕂R​(a,b,c)3=10\dim_{\mathbb{K}}R(a,b,c)_{3}=10, then dim𝕂Z​(R​(a,b,c))2=2\dim_{\mathbb{K}}Z(R(a,b,c))_{2}=2.

Proof.

We calculate a GrΓΆbner basis to degree 3. Order monomials in the free algebra π•‚β€‹βŸ¨x,y,z⟩\mathbb{K}\langle x,y,z\rangle using left-lexicographic order based on x<y<zx<y<z. Without loss of generality assume that c=1c=1, and write the defining relations of R​(a,b,c)R(a,b,c) as:

z2+a​y2+b​x2z​y+bβˆ’1​y​x+a​bβˆ’1​x​zz​x+aβˆ’1​b​y​z+aβˆ’1​x​y.z^{2}+ay^{2}+bx^{2}\qquad zy+b^{-1}yx+ab^{-1}xz\qquad zx+a^{-1}byz+a^{-1}xy.

Then the overlaps in degree 33 are: z3,z2​y,z2​xz^{3},z^{2}y,z^{2}x. Resolving these yields:

aβˆ’2​(b3βˆ’a3)​[y2​zβˆ’a2​bβˆ’2​x2​z+bβˆ’1​y​x​yβˆ’a​bβˆ’2​x​y​x],\displaystyle a^{-2}(b^{3}-a^{3})[y^{2}z-a^{2}b^{-2}x^{2}z+b^{-1}yxy-ab^{-2}xyx],
bβˆ’2​(1βˆ’b3)​[y​x2βˆ’x2​y],\displaystyle b^{-2}(1-b^{3})[yx^{2}-x^{2}y],
aβˆ’2​(1βˆ’a3)​[x​y2βˆ’y2​x],\displaystyle a^{-2}(1-a^{3})[xy^{2}-y^{2}x],

respectively.

There are twelve cubic monomials in the free algebra π•‚β€‹βŸ¨x,y,z⟩\mathbb{K}\langle x,y,z\rangle that do not contain z2z^{2}, z​xzx or z​yzy as a submonomial. Assuming that dim𝕂R​(a,b,c)3=10\dim_{\mathbb{K}}R(a,b,c)_{3}=10, there must be exactly two linearly independent GrΓΆbner basis elements in degree 3. Therefore exactly one of: b3βˆ’a3b^{3}-a^{3}, 1βˆ’b31-b^{3}, 1βˆ’a31-a^{3} must be zero. We consider cases.

Case 1: b3βˆ’a3=0β‰ (1βˆ’b3)​(1βˆ’a3)b^{3}-a^{3}=0\neq(1-b^{3})(1-a^{3}).

The GrΓΆbner basis in degree 3 is spanned by: y​x2βˆ’x2​yyx^{2}-x^{2}y and y2​xβˆ’x​y2y^{2}x-xy^{2}. It is straightforward to check that {a2​bβˆ’2​x2+y2,x​y+y​x}\{a^{2}b^{-2}x^{2}+y^{2},xy+yx\} is a basis for Z​(R​(a,b,c))2Z(R(a,b,c))_{2}.

Case 2: 1βˆ’b3=0β‰ (b3βˆ’a3)​(1βˆ’a3)1-b^{3}=0\neq(b^{3}-a^{3})(1-a^{3}).

The GrΓΆbner basis in degree 3 is spanned by: y2​zβˆ’a2​bβˆ’2​x2​z+bβˆ’1​y​x​yβˆ’a​bβˆ’2​x​y​xy^{2}z-a^{2}b^{-2}x^{2}z+b^{-1}yxy-ab^{-2}xyx and y2​xβˆ’x​y2y^{2}x-xy^{2}. It is easy to check that {x​yβˆ’a​x​z+b​y​z,y2}\{xy-axz+byz,y^{2}\} is a basis for Z​(R​(a,b,c))2Z(R(a,b,c))_{2}.

The remaining case is analogous to Case 2. ∎

Theorem 6.13.

Let 𝕂\mathbb{K} be an algebraically closed field of characteristic 0. When a​(aβˆ’1)β‰ 0a(a-1)\neq 0, the twisted tensor product P​(a)P(a) is isomorphic as a graded algebra to a three-dimensional Sklyanin algebra S​(1,1,c)S(1,1,c) of type EC. Moreover, every algebra S​(1,1,c)S(1,1,c) of type EC is isomorphic to some P​(a)P(a) with a​(aβˆ’1)β‰ 0a(a-1)\neq 0.

Proof.

Assume a​(aβˆ’1)β‰ 0a(a-1)\neq 0. Proposition 6.6 ensures that P​(a)P(a) is a twisted tensor product of π•‚βˆ’1​[x,y]\mathbb{K}_{-1}[x,y] and 𝕂​[t]\mathbb{K}[t]. Moreover, by Proposition 6.7 and Proposition 6.8, P​(a)P(a) is AS-regular, its point scheme is an elliptic curve and the associated automorphism has order 2.

Combining [5, Theorem 4.9], [6, Remark 3.9], and [6, Theorem 3.13], it follows that P​(a)P(a) is isomorphic to a Sklyanin algebra S​(aβ€²,bβ€²,cβ€²)S(a^{\prime},b^{\prime},c^{\prime}) or to one of the algebras R​(aβ€²,bβ€²,cβ€²)R(a^{\prime},b^{\prime},c^{\prime}) defined above. We note that the Type E and Type H algebras in [6, Table 1] are ruled out, as the automorphisms for those types do not have order 2.

Since dim𝕂P​(a)3=10\dim_{\mathbb{K}}P(a)_{3}=10 and dim𝕂Z​(P​(a))2=3\dim_{\mathbb{K}}Z(P(a))_{2}=3, Lemma 6.12 implies P​(a)P(a) must be isomorphic to a three-dimensional Sklyanin algebra S​(aβ€²,bβ€²,cβ€²)S(a^{\prime},b^{\prime},c^{\prime}). Since P​(a)P(a) is of type EC, so is S​(aβ€²,bβ€²,cβ€²)S(a^{\prime},b^{\prime},c^{\prime}). Since P​(a)P(a) contains a subalgebra isomorphic to π•‚βˆ’1​[r,s]\mathbb{K}_{-1}[r,s], Theorem 6.2(1) implies P​(a)P(a) is isomorphic to S​(1,1,c)S(1,1,c).

Finally, the statement that every S​(1,1,c)S(1,1,c) of type EC is isomorphic to some P​(a)P(a) with a​(aβˆ’1)β‰ 0a(a-1)\neq 0 follows directly from Proposition 6.4 and Corollary 6.11.

∎

References

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