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Automorphism group and twisted modules of the twisted Heisenberg-Virasoro vertex operator algebra

  • We first determine the automorphism group of the twisted Heisenberg-Virasoro vertex operator algebra VL(123,0). Then, for any integer t>1, we introduce a new Lie algebra Lt, and show that σt-twisted VL(123,0)(2=0)-modules are in one-to-one correspondence with restricted Lt-modules of level 13, where σt is an order t automorphism of VL(123,0). At the end, we give a complete list of irreducible σt-twisted VL(123,0)(2=0)-modules.

    Citation: Hongyan Guo. Automorphism group and twisted modules of the twisted Heisenberg-Virasoro vertex operator algebra[J]. Electronic Research Archive, 2021, 29(4): 2673-2685. doi: 10.3934/era.2021008

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  • We first determine the automorphism group of the twisted Heisenberg-Virasoro vertex operator algebra VL(123,0). Then, for any integer t>1, we introduce a new Lie algebra Lt, and show that σt-twisted VL(123,0)(2=0)-modules are in one-to-one correspondence with restricted Lt-modules of level 13, where σt is an order t automorphism of VL(123,0). At the end, we give a complete list of irreducible σt-twisted VL(123,0)(2=0)-modules.



    Let L be the twisted Heisenberg-Virasoro algebra. It is the universal central extension of the Lie algebra of differential operators on a circle of order at most one (cf. [3]):

    {f(t)ddt+g(t) | f(t),g(t)C[t,t1]}.

    L contains an infinite-dimensional Heisenberg algebra and the Virasoro algebra as subalgebras (cf. [3], [4]). The induced module VL(123,0)=U(L)U(L(1))C123 is a vertex operator algebra of central charge 1 with conformal vector ω=L21 (cf. [12]). VL(123,0) is a nonrational vertex operator algebra and is not C2-cofinite. The structure theory and representation theory of the twisted Heisenberg-Virasoro vertex operator algebra VL(123,0) are closely related to the three scalars 1,2,3 (cf. [3], [1], [2], [4], [5], [8], [12], etc.).

    Determining the automorphism group Aut(V) of a vertex operator algebra V is an important subject in vertex operator algebra theory. It is related to the orbifold theory which studies the fixed point subalgebras of vertex operator algebras and their modules under certain finite subgroups of the full automorphism groups. The orbifold conjecture says that under some conditions on V, every simple VG-module is contained in some g-twisted V-module, where G is a finite subgroup of Aut(V), gG, VG is the fixed point subalgebra of V under the group G.

    The automorphism group of the twisted Heisenberg-Virasoro algebra L has been studied in [15]. In this paper, we study the automorphism group of the twisted Heisenberg-Virasoro vertex operator algebra VL(123,0). We know that VL(123,0) is generated by ω=L21 and I11. By definition, any homomorphism of a vertex operator algebra (V,Y,1,ω) takes ω to ω. Therefore, it suffices to determine the action on the generator I11. It turns out that automorphisms of the twisted Heisenberg-Virasoro vertex operator algebra VL(123,0) depend on the numbers 2 and 3, and there exists automorphism of order other than 2, which makes the study of twisted modules for VL(123,0) interesting.

    In [12], all irreducible modules for the vertex operator algebra VL(123,0) are classified: that is, every irreducible module for VL(123,0) is isomorphic to some LL(123,h1,h2), h1,h2C. In this paper, for any integer t>1, we classify σt-twisted irreducible modules for VL(123,0), where σt is an order t automorphism of VL(123,0). The way we deal with this problem is similar to the one used for modules of vertex algebra (cf. [10], [11], [12], [13], etc.), but in the context of twisted modules. We first introduce another Lie algebra Lt. It is a Lie algebra with basis {Ln,In+1t,k1,k3 | nZ}, and Lie brackets

    [Lm,Ln]=(mn)Lm+n+δm+n,0m3m12k1,
    [Lm,In+1t]=(n+1t)Im+n+1t,
    [Im+1t,In+1t]=(m+1t)δm+n+2t,0δt,2k3,[Lt,ki]=0,i=1,3.

    Note that when t2, {In+1t | nZ} is an abelian Lie algebra. Then we construct irreducible Lt-modules LLt(k1,k3,h) as quotient of the induced modules MLt(k1,k3,h), where k1,k3,hC. We show that σt-twisted VL(123,0)-modules (2=0) are in one-to-one correspondence with restricted Lt-modules of level 13. Using this result, we get a complete list of irreducible σt-twisted VL(123,0)-modules, where 2=0, 1, 3C. Let VL(123,0)σt be the fixed point subalgebra of VL(123,0) under the automorphism σt. VL(123,0)σt is a vertex operator subalgebra of VL(123,0). It is important and meaningful to study the representations of the fixed point subalgebra VL(123,0)σt. We remark at the end of the paper that except for the case of order 2, the complete list of irreducible modules for VL(123,0)σt needs to be further investigated.

    This paper is organized as follows. In Section 2, we review the notions and some results of vertex operator algebras, automorphisms and twisted modules for vertex operator algebras. In Section 3, we study the automorphism group of the twisted Heisenberg-Virasoro vertex operator algebra VL(123,0). In Section 4, we first study the twisted modules of VL(123,0)(2=0) under an order t automorphism σt for any integer t>1. Then we give a complete list of irreducible σt-twisted VL(123,0)(2=0)-modules.

    For later use, we recall the following result (cf. Proposition 2.3.7 of [13]).

    Lemma 2.1.

    (x1x2)m(x2)nx11δ(x2x1)=0 (2.1)

    for m>n, m,nN, where δ(x1x2)=nZxn1xn2.

    Let (V,Y,ω,1) be a vertex operator algebra (cf. Definition 3.1.22 of [13]). Then, a priori, (V, Y, 1) is a vertex algebra (cf. Definition 3.1.1 of [13]). Let D be the endomorphism of the vertex algebra V defined by D(v)=v21 for vV. We have Y(Dv,x)=ddxY(v,x). Denote by L(n)=ωn+1 for any nZ. It can be proved that 1V(0) and D=L(1).

    Definition 2.2. An automorphism of a vertex operator algebra (V,Y,ω,1) is a linear isomorphism σ of V such that

    σ(1)=1,σ(ω)=ωandσ(unv)=σ(u)nσ(v)

    for any u,vV, nZ.

    The group of all automorphisms of a vertex operator algebra V is denoted by Aut(V). Any automorphism of a vertex operator algebra V is grading-preserving, i.e. it preserves each homogeneous subspace V(n) of V, nZ. Let σ be an order t automorphism of a vertex operator algebra V, t is a positive integer. Then σ acts semisimply on V. Therefore

    V=V0V1Vt1,

    where Vk is the eigenspace of V for σ with eigenvalues ηk, where η=exp(2π1t), k=0,,t1. It is easy to see that the fixed points set V0:=Vσ={vV | σ(v)=v} is a vertex operator subalgebra of V

    Now we recall some notions regarding to twisted modules from [14].

    Definition 2.3. Let (V,1,Y) be a vertex algebra with an automorphism σ of order t. A σ-twisted V-module is a triple (W,d,YW) consisting of a vector space W, an endomorphism d of W and a linear map

    YW(,z):V(EndW)[[z1t,z1t]]

    satisfying the following conditions:

    (TW1) For any vV,wW, vnw=0forn1tZsufficiently large;

    (TW2) YW(1,z)=IdW;

    (TW3) [d,YW(v,z)]=YW(D(v),z)=ddzYW(v,z)for anyvV;

    (TW4) For any u,vV, the following σ-twisted Jacobi identity holds:

    z10δ(z1z2z0)YW(u,z1)YW(v,z2)z10δ(z2z1z0)YW(v,z2)YW(u,z1)=z121tt1k=0δ((z1z0z2)1t)YW(Y(σku,z0)v,z2).

    If V is a vertex operator algebra, a σ-twisted V-module for V as a vertex algebra is called a σ-twisted weak module for V as a vertex operator algebra.

    Definition 2.4. For V a vertex operator algebra, a σ-twisted V-module W is a σ-twisted weak module for V as a vertex algebra and W=hCW(h) such that

    (TW5) L(0)w=hwforhC,wW(h);

    (TW6) For any fixed h,W(h+n)=0forn1tZsufficiently small;

    (TW7) dimW(h)<for anyhC.

    Remark 2.5. Let W be a σ-twisted V-module. Then

    [L(0),YW(v,z)]=zYW(L(1)v,z)+YW(L(0)v,z) (2.2)

    for vV. Hence, if vV is homogeneous,

    vnW(h)W(h+wtvn1)forn1tZ,hC.

    It follows that a σ-twisted V-module W decomposes into twisted submodules corresponding to the congruence classes mod 1tZ: For hC/1tZ, let

    W[h]=α+1tZ=hW(α). (2.3)

    Then

    W=hC/1tZW[h]. (2.4)

    In particular, if W is irreducible, then

    W=W[h] (2.5)

    for some h.

    Remark 2.6. Let W be a σ-twisted V-module. For uVk, vV, there is the following twisted iterate formula (cf. (2.32) of [14])

    YW(Y(u,z0)v,z2)=Resz1(z1z0z2)ktX, (2.6)

    where

    X=z10δ(z1z2z0)YW(u,z1)YW(v,z2)z10δ(z2z1z0)YW(v,z2)YW(u,z1).

    Then it can be easily deduced that for any nZ,

    YW(unv,z)=Resz1j=0(1)j(ktj)zktj1zktYj, (2.7)

    where

    Yj=((z1z)n+jYW(u,z1)YW(v,z)(z+z1)n+jYW(v,z)YW(u,z1)),

    (ktj)=kt(kt1)(ktj+1)j!. Note that when k=0, kt=0, we have j=0, and then (2.7) is the usual formula for (untwisted) V-modules (cf. (3.8.16) of [13]).

    Definition 2.7. A homomorphism between two σ-twisted weak V-modules M and W is a linear map f:MW such that for any vV,

    fYM(v,z)=YW(v,z)f. (2.8)

    If V is a vertex operator algebra, then a V-module homomorphism f is compatible with the gradings:

    f(M(h))W(h)forhC. (2.9)

    Using the formula (2.7), similarly as Proposition 4.5.1 of [13], there is the following result.

    Proposition 2.8. Let W1 and W2 be σ-twisted V-modules and let ψHomC(W1,W2). Suppose that

    Y(a,z)ψ=ψY(a,z)foraS,

    where S is a given generating set of V. Then ψ is a σ-twisted V-module homomorphism.

    In the following, we review from Section 3 of [14] the local systems of twisted vertex operators.

    Definition 2.9. Let W be a vector space, let t be a fixed positive integer. A Zt-twisted weak vertex operator on W is a formal series a(z)=n1tZanzn1(EndW)[[z1t,z1t]] such that for any wW, anw=0 for n1tZ sufficiently large.

    Definition 2.10. Two Zt-twisted weak vertex operators a(z) and b(z) are said to be mutually local if there is a positive integer n such that

    (z1z2)na(z1)b(z2)=(z1z2)nb(z2)a(z1).

    A Zt-twisted weak vertex operator is called a Zt-twisted vertex operator if it is local with itself.

    Denote by F(W,t) the space of all Zt-twisted weak vertex operators on W. Let σ be the endomorphism of (EndW)[[z1t,z1t]] defined by: σf(z1t)=f(η1z1t). Denote by F(W,t)k={f(z)F(W,t) | σf(z)=ηkf(z)} for 0kt1. For any mutually local Zt-twisted vertex operators a(z),b(z) on W, define a(z)nb(z) as follows (cf. Definition 3.7 of [14]).

    Definition 2.11. Let W be a vector space and let a(z) and b(z) be mutually local Zt-twisted vertex operators on W such that a(z)F(W,t)k. Then for any integer n we define a(z)nb(z) as an element of F(W,t) as follows:

    a(z)nb(z)=Resz1Resz0(z1z0z)ktzn0X, (2.10)

    where

    X=z10δ(z1zz0)a(z1)b(z)z10δ(zz1z0)b(z)a(z1).

    For any set S of mutually local Zt-twisted vertex operators on W, by Zorn's Lemma, there exists a local system A of Zt-twisted vertex operators on W (cf. Section 3 of [14]). Denote by S the vertex algebra generated by S inside A via the operations a(z)nb(z), nZ.

    In this section, we first recall the definition of the twisted Heisenberg-Virasoro algebra L and the construction of the twisted Heisenberg-Virasoro vertex operator algebra VL(123,0). Then we determine the automorphism group of the vertex operator algebra VL(123,0).

    Recall the definition of the twisted Heisenberg-Virasoro algebra L (see [3] or [4]).

    Definition 3.1. The twisted Heisenberg-Virasoro algebra L is a Lie algebra with basis {Ln,In,c1,c2,c3 | nZ}, and the following Lie brackets:

    [Lm,Ln]=(mn)Lm+n+δm+n,0m3m12c1, (3.1)
    [Lm,In]=nIm+nδm+n,0(m2+m)c2, (3.2)
    [Im,In]=mδm+n,0c3,[L,ci]=0,i=1,2,3. (3.3)

    Clearly, Span{Ln,c1 | nZ} is a Virasoro algebra, Span{In,c3 | nZ{0}} is an infinite-dimensional Heisenberg algebra, we denote them by Vir, H respectively.

    Let

    L(z)=nZLnzn2,I(z)=nZInzn1,

    then the defining relations of L become to be

    [L(z1),L(z2)]=m,nZ(mn)Lm+nzm21zn22+mZm3m12c1zm21zm22=ddz2(L(z2))z11δ(z2z1)+2L(z2)z2z11δ(z2z1)+c112(z2)3z11δ(z2z1), (3.4)
    [L(z1),I(z2)]=m,nZnIm+nzm21zn12mZ(m2+m)c2zm21zm12=ddz2(I(z2))z11δ(z2z1)+I(z2)z2z11δ(z2z1)(z2)2z11δ(z2z1)c2, (3.5)
    [I(z1),I(z2)]=mZmc3zm11zm12=z2z11δ(z2z1)c3. (3.6)

    We recall the construction of the twisted Heisenberg-Virasoro vertex operator algebra VL(123,0) from [12]. Let

    L(1)=n1CLnn0CIn3i=1Cci,
    L(2)=n2CLnn1CIn.

    They are graded subalgebras of L and

    L=L(1)L(2).

    Let i,i=1,2,3, be any complex numbers. Consider C as an L(1)-module with ci acting as the scalar i,i=1,2,3, and with n1CLnn0CIn acting trivially. Denote this L(1)-module by C123. Form the induced module

    VL(123,0)=U(L)U(L(1))C123, (3.7)

    where U() denotes the universal enveloping algebra of a Lie algebra. Set 1=11VL(123,0). VL(123,0) is a vertex operator algebra with vacuum vector 1 and conformal vector ω=L21. And {ω=L21,I:=I11} is a generating subset of VL(123,0). Recall the grading on VL(123,0):

    VL(123,0)=n0VL(123,0)(n),

    where VL(123,0)(0)=C and VL(123,0)(n), n1, has a basis consisting of the vectors

    Ik1IksLm1Lmr1

    for r,s0, m1mr2, k1ks1 with ri=1mi+sj=1kj=n.

    Now we give our first main result. The automorphism group of VL(123,0) is determined in the following theorem.

    Theorem 3.2. (1) If 20, then Aut(VL(123,0))={id}.

    (2) If 2=0 and 30, then Aut(VL(123,0))Z2.

    (3) If both 2 and 3 are 0, then Aut(VL(123,0))C×=C{0}.

    Proof. Let

    φ:VL(123,0)VL(123,0)

    be an automorphism of the vertex operator algebra VL(123,0). Then φ(1)=1 and φ(ω)=ω. Since VL(123,0) is generated by ω and I=I11, it suffices to determine φ(I). φ is grading-preserving, so φ(I)=aI for some aC×.

    Then, on the one hand, we have

    φ(L1I)=aL1I=a[L1,I1]1=2a21,

    on the other hand, we have

    φ(L1I)=φ([L1,I1]1)=221.

    Therefore if 20, we get that a=1, i.e. when 20, Aut(VL(123,0))={id} only consists of the identity map.

    Suppose now 2=0. Let's consider φ(I1I). On the one hand,

    φ(I1I)=φ(I)1φ(I)=a2I1I11=a2[I1,I1]1=a231,

    on the other hand,

    φ(I1I)=φ([I1,I1]1)=31.

    So if 30, we get a2=1, i.e. a=1 or a=1, then Aut(VL(123,0))Z2.

    Now let 2=0and3=0, then a can be any nonzero complex number, so Aut(VL(123,0))C×.

    In this section, we always assume 2=0. We study twisted modules for the vertex operator algebra VL(123,0). More precisely, for any integer t>1, we introduce an infinite-dimensional Lie algebra Lt. We show that there is a one-to-one correspondence between restricted Lt-modules of level 13 and σt-twisted VL(123,0)-modules, where σt is an order t automorphism of VL(123,0). And we give a complete list of irreducible σt-twisted VL(123,0)-modules.

    Note that if 2=0 and 30, then t can only be the integer 2 (Theorem 3.2). As we need, we introduce the following Lie algebra.

    Definition 4.1. Let Lt be a Lie algebra with basis {Ln,In+1t,k1,k3 | nZ}, and the Lie brackets are given by:

    [Lm,Ln]=(mn)Lm+n+δm+n,0m3m12k1, (4.1)
    [Lm,In+1t]=(n+1t)Im+n+1t, (4.2)
    [Im+1t,In+1t]=(m+1t)δm+n+2t,0δt,2k3,[Lt,ki]=0,i=1,3. (4.3)

    Note that if t2, then [Im+1t,In+1t]=0 for any m,nZ.

    Form the generating function as

    L(z)=nZLnzn2,Iσt(z)=nZIn+1tzn1t1.

    Then the defining relations (4.1), (4.2), (4.3) amount to:

    [L(z1),L(z2)]=ddz2(L(z2))z11δ(z2z1)+2L(z2)z2z11δ(z2z1)+112(z2)3z11δ(z2z1)k1, (4.4)
    [L(z1),Iσt(z2)]=m,nZ(n+1t)Im+n+1tzm21zn1t12=ddz2(Iσt(z2))z11δ(z2z1)+Iσt(z2)z2z11δ(z2z1), (4.5)
    [Iσt(z1),Iσt(z2)]=mZ(m+1t)zm1t11zm+1t12δt,2k3=z2(z11δ(z2z1)(z2z1)1t)δt,2k3. (4.6)

    Now we construct irreducible Lt-modules (cf. [12], [13], etc.). Let

    (Lt)0=(m0CLm)(n0CIn+1t)Ck1Ck3.

    It is a subalgebra of Lt.

    Let C be an (Lt)0-module, where Lm, In+1t act trivially for all m1, n0, and L0,k1,k3 act as scalar multiplications by h,k1,k3 respectively. Denote this (Lt)0-module by Ck13,h. Form the induced module

    MLt(k1,k3,h)=U(Lt)U((Lt)0)Ck13,h.

    Set

    1k13,h=1Ck13,hMLt(k1,k3,h).

    Then MLt(k1,k3,h) is C-graded by L0-eigenvalues:

    MLt(k1,k3,h)=n0MLt(k1,k3,h)n+h,

    where MLt(k1,k3,h)(h)=Ck13,h and MLt(k1,k3,h)(n+h) is the L0-eigenspace of eigenvalue n+h for n>0. MLt(k1,k3,h)(n+h) has a basis consisting of

    Ik1+1tIks+1tLm1Lmr1k13,h

    for r,s0, m1mr1, k1ks1 with ri=1mi+sj=1(kj1t)=n, n>0.

    Remark 4.2. As a module for Lt, MLt(k1,k3,h) is generated by 1k13,h with the relations

    L01k13,h=h1k13,h,ki=ki,i=1,3,

    and

    Lm1k13,h=0,In+1t1k13,h=0form1,n0.

    MLt(k1,k3,h) is universal in the sense that for any Lt-module W of level k13 equipped with a vector v such that L0v=hv,Lmv=0,In+1tv=0form1,n0, there exists a unique Lt-module map MLt(k1,k3,h)W sending 1k13,h to v.

    In general, MLt(k1,k3,h) as an Lt-module may be reducible. Since Ck13,h generate MLt(k1,k3,h) as Lt-module, for any proper submodule U of MLt(k1,k3,h), U(h)=UMLt(k1,k3,h)(h)=0. Hence there exists a maximal proper Lt-submodule TLt(k1,k3,h). Set

    LLt(k1,k3,h)=MLt(k1,k3,h)/TLt(k1,k3,h).

    Then LLt(k1,k3,h) is an irreducible Lt-module.

    Definition 4.3. An Lt-module W is said to be restricted if for any wW,nZ, Lnw=0 and In+1tw=0 for n sufficiently large. We say an Lt-module W is of level k13 if the central element ki acts as scalar ki for i=1,3.

    It is easy to see that MLt(k1,k3,h), LLt(k1,k3,h) are restricted Lt-modules of level k13 for any hC. Now we are going to relate Lt-modules with twisted VL(123,0)-modules. On the one hand, we have

    Theorem 4.4. If W is a restricted Lt-module of level 13, then W is a σt-twisted VL(123,0)-module for VL(123,0) as a vertex algebra with

    Yσt(L21,z)=L(z)=nZLnzn2,
    Yσt(I11,z)=Iσt(z)=nZIn+1tzn1t1.

    Proof. Let UW={L(z),Iσt(z),1W}, where 1W is the identity operator on W. Clearly, L(z),Iσt(z) are Zt-twisted weak vertex operators on W. From (4.4), (4.5), (4.6), using (2.1), we see that L(z),Iσt(z) are mutually local Zt-twisted vertex operators on W. Hence, by Corollary 3.15 of [14], UW is a vertex algebra with W a faithful σ-twisted module, where σ is an order t automorphism of the vertex algebra UW. To say that W is a σt-twisted module for VL(123,0), from Proposition 3.17 of [14], it suffices to show that there exists a vertex algebra homomorphism from VL(123,0) to UW.

    By Lemma 2.11 of [14], Y(L(z),z1) and Y(Iσt(z),z1) satisfy the twisted Heisenberg-Virasoro algebra relations (3.4), (3.5), (3.6). Then UW is an L-module with Ln,In acting as L(z)n+1, Iσt(z)n for nZ, ci acting as i with 2=0, i=1,2,3.

    By the universal property of VL(123,0) (c.f. Remark 2.7 of [12]), there exists a unique L-module homomorphism

    ψ:VL(123,0)UW;11W.

    Then

    ψ(ωnv)=L(z)nψ(v)=ψ(ω)nψ(v),
    ψ(Inv)=Iσt(z)nψ(v)=ψ(I)nψ(v)

    for all vVL(123,0), nZ. Hence ψ is a vertex algebra homomorphism. Therefore, W is a weak σt-twisted VL(123,0)-module with Yσt(L21,z)=L(z), Yσt(I11,z)=Iσt(z).

    Conversely, we have

    Theorem 4.5. If W is a σt-twisted VL(123,0) (2=0)-module, then W is a restricted Lt-module of level 13 with L(z)=YW(L21,z), Iσt(z)=YW(I11,z).

    Proof. Let W be a σt-twisted VL(123,0)(2=0)-module. Recall the following formula (c.f. (2.40) of [14])

    [YW(a,z1),YW(b,z2)]=j=01j!((z2)jz11δ(z2z1)(z2z1)kt)YW(ajb,z2),

    where k is determined by a. In our case, when a=L21, k=0, when a=I11, k=1. For a=b=L21, we have ((2.21) of [12])

    (L21)jL21=(j+1)Lj31+δj3,0(j1)3(j1)12c11,

    so

    [YW(L21,z1),YW(L21,z2)]=YW(L31,z2)z12δ(z1z2)+2YW(L21,z2)(z1)z12δ(z1z2)+112(z1)3z12δ(z1z2)11. (4.7)

    For a=L21,b=I11, we have ((2.22) of [12] with 2=0)

    (L21)jI11=Ij21,

    so

    [YW(L21,z1),YW(I11,z2)]=YW(I21,z2)z11δ(z2z1)+YW(I11,z2)(z2)z11δ(z2z1). (4.8)

    For a=b=I11, we have ((2.23) of [12])

    (I11)jI11=jδj1,0c31,

    so

    [YW(I11,z1),YW(I11,z2)]=(z2)z11δ(z2z1)(z2z1)1t31. (4.9)

    Note that for t2, we have to require 3=0 (Theorem 3.2). Therefore, with (4.4), (4.5) and (4.6), W is a Lt-module with L(z)=YW(L21,z), Iσt(z)=YW(I11,z), ki=i, i=1,3. Then W is restricted of level 13 is clear.

    Let

    L(0)t=CL0Ck1Ck3,L(n)t=CLnfor0nZ,
    L(1t+n)t=CIn+1t,L(k)t=0fork1tZ,kZ,1t+Z.

    Then L=nZL(nt)t is a 1tZ-graded Lie algebra, and the grading is given by adL0-eigenvalues.

    By Theorem 4.4 and Theorem 4.5 we have the following result.

    Theorem 4.6. The σt-twisted modules for VL(123,0) (2=0) viewed as a vertex operator algebra (i.e. C-graded by L0-eigenvalues and with the two grading restrictions (TW6), (TW7)) are exactly those restricted modules for the Lie algebra Lt of level 13 that are C-graded by L0-eigenvalues and with the two grading restrictions. Furthermore, for any σt-twisted VL(123,0)-module W, the σt-twisted VL(123,0)-submodules of W are exactly the submodules of W for Lt, and these submodules are in particular graded.

    Hence irreducible restricted Lt-modules of level 13 corresponds to irreducible σt-twisted VL(123,0)-modules. Recall that for any hC, LLt(1,3,h) is an irreducible restricted Lt-module of level 13, so it is an irreducible σt-twisted VL(123,0)-module with 2=0.

    Now we give the complete list of irreducible σt-twisted VL(123,0)-modules.

    Theorem 4.7. Let 2=0, 1,3C. Then {LLt(1,3,h) | hC} is a complete list of irreducible σt-twisted VL(123,0)-modules.

    Proof. Let W=rCW(r) be an irreducible σt-twisted VL(123,0)-module. By Theorem 4.6, W is an irreducible restricted Lt-module of level 13. So ki acts on W as a scalar i for i=1,3. From Remark 2.5, there exists hC such that W(h)0 and W(hn)=0 for all n1tZ1. Let 0wW(h). Then

    L0w=hw,Lmw=0,In+1tw=0

    for m1,n0. In view of Remark 4.2, there is a unique Lt-module homomorphism

    φ:MLt(1,3,h)W

    such that φ(1k13,h)=w. By Proposition 2.8, φ is a σ-twisted UW-module homomorphism (since Lt generates the vertex algebra UW), where σ is an order t automorphism of the vertex algebra UW. Recall that MLt(1,3,h) is a weak σt-twisted VL(123,0)-module via the vertex algebra homomorphism ψ in Theorem 4.4. So φ can be viewed as a σt-twisted VL(123,0)-module homomorphism. Since W is irreducible and TLt(1,3,h) is the (unique) largest proper submodule of MLt(1,3,h), it follows that

    φ(MLt(1,3,h))=W

    and

    Kerφ=TLt(1,3,h).

    Thus φ reduces to a σt-twisted VL(123,0)-module isomorphism from LLt(1,3,h) to W.

    It is interesting and important to classify the irreducible modules for the fixed point subalgebra VL(123,0)σt:={vVL(123,0) | σt(v)=v}, tZ1. In the case of 2=0 and 30, we have t=2. Then σt is the order 2 automorphism of VL(123,0) which is induced from its Heisenberg vertex operator subalgebra. Denote by σ2=σ. Precisely, the automorphism

    σ:VL(123,0)VL(123,0)

    is defined on the basis elements by

    Ik1IksLm1Lmr1(1)sIk1IksLm1Lmr1,

    and extended linearly, where r,s1, m1mr2, k1ks1. Let

    VL(123,0)+={vVL(123,0) | σ(v)=v}

    be the fixed point subalgebra under σ.

    For 30, denote by

    c~Vir=11+12223.

    Let VH(3,0) be the vertex operator algebra constructed from the Heisenberg subalgebra H which is equipped with the nonstandard conformal vector ωH=123I1I11+23I21 (of central charge 112223). Let ~Vir be the Virasoro algebra constructed by ˜ω=ωωH. Let V~Vir(c~Vir,0) be the corresponding Virasoro vertex operator algebra. Recall that when 30, we have (cf. Theorem 3.16 of [12])

    VL(123,0)VH(3,0)V~Vir(c~Vir,0)

    as vertex operator algebras.

    It is well known that there exists an order 2 isomorphism of the Heisenberg vertex operator algebra VH(3,0). Let again

    σ:VH(3,0)VH(3,0)

    be the order 2 automorphism which is defined on the basis elements by

    Ik1Iks1(1)sIk1Iks1

    and extended linearly, where s1, k1ks1. The fixed point subalgebra VH(3,0)+={vVH(3,0) | σ(v)=v} has beed extensively studied (cf. [6] etc.).

    Then it is immediate to see that when 30 and 2=0, we have an isomorphism of vertex operator algebras

    VL(123,0)+VH(3,0)+V~Vir(c~Vir,0).

    Up to isomorphism, irreducible modules for the vertex operator algebra VH(3,0)+ are (cf. [6], etc.) VH(3,0)±,VH(3,0)(σ)±,VH(3,λ)VH(3,λ) for any 0λC. Up to isomorphism, irreducible modules for the Virasoro vertex operator algebra V~Vir(c~Vir,0) are L~Vir(c~Vir,h) for all hC (cf. [9], [16], etc.). Therefore, in the case of 2=0 and 30, irreducible modules of VL(123,0)+ are one-to-one correspond to the tensor product of irreducible modules of VH(3,0)+ and irreducible modules of V~Vir(c~Vir,0) (cf. Proposition 4.7.2 and Theorem 4.7.4 of [7]).

    For other automorphism σt, the complete list of irreducible VL(123,0)σt-modules remains to be investigated.



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