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Research article

Smash product construction of modular lattice vertex algebras

  • Received: 08 August 2021 Revised: 17 November 2021 Accepted: 17 November 2021 Published: 24 December 2021
  • Motivated by a work of Li, we study nonlocal vertex algebras and their smash products over fields of positive characteristic. Through smash products, modular vertex algebras associated with positive definite even lattices are reconstructed. This gives a different construction of the modular vertex algebras obtained from integral forms introduced by Dong and Griess in lattice vertex operator algebras over a field of characteristic zero.

    Citation: Qiang Mu. Smash product construction of modular lattice vertex algebras[J]. Electronic Research Archive, 2022, 30(1): 204-220. doi: 10.3934/era.2022011

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  • Motivated by a work of Li, we study nonlocal vertex algebras and their smash products over fields of positive characteristic. Through smash products, modular vertex algebras associated with positive definite even lattices are reconstructed. This gives a different construction of the modular vertex algebras obtained from integral forms introduced by Dong and Griess in lattice vertex operator algebras over a field of characteristic zero.



    It is well known that there are three important classes of rational vertex operator algebras over the field of complex numbers; namely, affine vertex operator algebras, Virasoro vertex operator algebras and lattice vertex operator algebras (see [1]). It is natural to study the corresponding vertex algebra structures over fields of prime characteristic first.

    There have already been some works on modular vertex algebras and their representations. For example, modular A(V) theory and An(V) theory were studied in [2,3], modular Virasoro vertex operator algebras were studied in [4], and framed vertex operator algebras were studied in [5]. Modular vertex algebras obtained from integral forms in some vertex operator algebras over the field of complex numbers were used to study modular moonshine in [6,7,8].

    Dong and Griess introduced an integral form of the vertex algebras associated with positive definite even lattices over a field of characteristic zero in [9], and the related modular vertex algebras were studied in [10].

    In a series of papers (see [11,12,13]), Li studied nonlocal vertex algebras over a field of characteristic zero. In particular, in [13] Li introduced a smash product construction of nonlocal vertex algebras and used smash product to give a different construction of lattice vertex algebras and their modules (cf. [1,14]). Motivated by [13], in this paper we study nonlocal vertex algebras and the smash product construction over fields of prime characteristic. As an application, modular vertex algebras associated with positive definite even lattices are reconstructed by using smash products. This gives another construction of the modular vertex algebras obtained from integral forms introduced by Dong and Griess of lattice vertex operator algebras over a field of characteristic zero.

    This paper is organized as follows: In Section 2, we present some basic results on modular nonlocal vertex algebras and give the smash product construction of nonlocal vertex algebras. In Section 3, we use the smash product to construct the vertex algebras associated with positive definite even lattices.

    In this section, we first present some basic results on modular nonlocal vertex algebras. Then we give the smash product construction of modular nonlocal vertex algebras. The proofs for most of the results in this section are the same as those for characteristic zero (see [11,12,13]).

    Let F be an algebraically closed field of an odd prime characteristic p, which is fixed throughout this paper. All vector spaces, including algebras, are considered to be over F. We use Z for the integers, Z+ for the positive integers, and N for the nonnegative integers.

    Note that for any mZ, kN,

    (mk)=m(m1)(m+1k)k!Z.

    Then we shall also view (mk) as an element of F. Furthermore, for mZ we have

    (x±z)m=kN(mk)(±1)kxmkzkF[x,x1][[z]].

    The following definition is the same as in characteristic zero (see [11,12,13]).

    Definition 2.1. A nonlocal vertex algebra is a vector space V endowed with a distinguished vector 1, called the vacuum vector, and endowed with a linear map

    Y(,x):V(EndV)[[x,x1]]vY(v,x)=nZvnxn1 (2.1)

    such that for u,vV,

    unv=0for   n sufficiently large, (2.2)
    Y(1,x)=1, (2.3)
    Y(v,x)1V[[x]]andlimx0Y(v,x)1=vfor vV (2.4)

    and for u,v,wV, there exists a nonnegative integer l such that

    (x0+x2)lY(u,x0+x2)Y(v,x2)w=(x0+x2)lY(Y(u,x0)v,x2)w. (2.5)

    As in [15], define B to be the bialgebra with a basis {D(r)rN}, where

    D(m)D(n)=(m+nn)D(m+n),D(0)=1,Δ(D(n))=ni=0D(ni)D(i),ε(D(n))=δn,0

    for m,nN. Set

    exD=nNxnD(n)B[[x]]. (2.6)

    The bialgebra structure of B can be described in terms of the generating functions as

    exDezD=e(x+z)D,Δ(exD)=exDexD,ε(exD)=1, (2.7)

    in particular, we have exDexD=1.

    Remark 2.2. Let U be any vector space. Then U[[x,x1]] is a B-module with D(n) for nN acting as the n-th Hasse differential operator (n)x with respect to x, which is defined by

    (n)xxm=(mn)xmnfor mZ. (2.8)

    Set ezx=nNzn(n)x. Then

    f(x+z)=ezxf(x)for f(x)U[[x,x1]]. (2.9)

    As in the case of characteristic zero, we have (cf. [13]):

    Lemma 2.3. Let V be a nonlocal vertex algebra.Then V is naturally a B-module with

    D(n)u=un11 (2.10)

    for uV and nN.Furthermore,

    ex0DY(u,x2)ex0D=Y(ex0Du,x2)=Y(u,x2+x0)=ex0x2Y(u,x2). (2.11)

    Proof. Let uV. By (2.4) and (2.10), we have

    exDu=Y(u,x)1, (2.12)

    and in particular, D(0)=1 on V.

    Let lN be such that

    (x0+x2)lY(Y(u,x0)1,x2)1=(x0+x2)lY(u,x0+x2)Y(1,x2)1.

    As Y(1,x)=1 and Y(u,x)1 only involves nonnegative powers of x, we have

    (x0+x2)lY(Y(u,x0)1,x2)1=(x0+x2)lY(u,x0+x2)1=(x0+x2)lY(u,x2+x0)1.

    Multiplying both sides by (x2+x0)l we obtain

    Y(Y(u,x0)1,x2)1=Y(u,x2+x0)1.

    Using (2.12) and the equation above, we have

    ex2D(ex0Du)=Y(ex0Du,x2)1=Y(Y(u,x0)1,x2)1=Y(u,x2+x0)1=e(x2+x0)Du.

    Therefore V is a B-module.

    Let u,vV. Then there is lN such that

    (x0+x2)lY(Y(u,x0)1,x2)v=(x0+x2)lY(u,x0+x2)Y(1,x2)v=(x0+x2)lY(u,x0+x2)v.

    We may assume that xlY(u,x)vV[[x]] by replacing l with a bigger integer if necessary, so that

    (x0+x2)lY(u,x0+x2)v=(x0+x2)lY(u,x2+x0)v.

    Then

    (x2+x0)lY(Y(u,x0)1,x2)v=(x2+x0)lY(u,x2+x0)v.

    Multiplying both sides by (x2+x0)l we have

    Y(ex0Du,x2)v=Y(Y(u,x0)1,x2)v=Y(u,x2+x0)v=ex0x2Y(u,x2)v.

    Let u,vV and let lN be such that

    (x0+x2)lY(Y(u,x0)v,x2)1=(x0+x2)lY(u,x0+x2)Y(v,x2)1.

    Since Y(Y(u,x0)v,x2)1 involves only nonnegative powers of x2, we can multiply both sides by (x0+x2)l to get

    Y(Y(u,x0)v,x2)1=Y(u,x0+x2)Y(v,x2)1.

    Then

    ex2DY(u,x0)v=Y(Y(u,x0)v,x2)1=Y(u,x0+x2)Y(v,x2)1=Y(u,x0+x2)ex2Dv,

    that is,

    ex2DY(u,x0)=Y(u,x0+x2)ex2D

    on V. Applying ex2D from left, as ex2Dex2D=1, we have

    ex2DY(u,x0)ex2D=Y(u,x0+x2).

    Thus (2.11) holds.

    The following two results of [11] are valid here with the same proof.

    Lemma 2.4. For any subset S of a nonlocal vertex algebra V, the subalgebra S generated by S is linearly spanned by vectors

    v(1)n1v(2)n2v(r)nr1

    for rN, v(i)S, niZ.

    Let V be a nonlocal vertex algebra. For u,vV, we say u,v are mutually local if there exists kN such that

    (x1x2)kY(u,x1)Y(v,x2)=(x1x2)kY(v,x2)Y(u,x1). (2.13)

    A subset S of V is said to be local if every pair of elements of S are mutually local.

    Lemma 2.5. Let V be a nonlocal vertex algebra and let S be a local subset of V.Then the subalgebra S of V generated by S is a vertex algebra.

    Definition 2.6. Let V be a nonlocal vertex algebra. A V-module is a vector space W endowed with a linear map

    YW(,x):V(EndW)[[x,x1]]vYW(v,x)=nZvnxn1 (2.14)

    such that for vV and wW,

    vnw=0for n sufficiently large,  (2.15)
    YW(1,x)=1, (2.16)

    and for u,vV and wW, there exists a nonnegative integer l such that

    (x0+x2)lYW(u,x0+x2)YW(v,x2)w=(x0+x2)lYW(Y(u,x0)v,x2)w. (2.17)

    A unital associative algebra A is called a B-module algebra if A is a B-module such that

    h(ab)=(h(1)a)(h(2)b),h1=ε(h)1 (2.18)

    for hB and a,bA, where Δ(h)=h(1)h(2) is in the Sweedler notation.

    Example 2.7. Let A be a B-module algebra. Then A has a nonlocal vertex algebra structure with 1 as the vacuum vector and

    Y(a,x)b=(exDa)bfor a,bA.

    Furthermore, on any module W for A as an associative algebra, there exists a module structure YW for A with YW(a,x)w=(exDa)w for aA, wW.

    Remark 2.8. Let A and B be B-module algebras. Then AB is a B-module algebra with exD=exDAexDB.

    Let V and U be nonlocal vertex algebras. A linear map f from V to U is a homomorphism of nonlocal vertex algebras if

    f(1)=1,fY(u,x)v=Y(f(u),x)f(v)for u,vV.

    It is straightforward to show that fexDV=exDUf if f is a homomorphism from V to U. A homomorphism of nonlocal vertex algebras from V to V is called an endomorphism of V.

    Remark 2.9. Let A and B be B-module algebras. Then a linear map f from A to B is a homomorphism of nonlocal vertex algebras from A to B if and only if f is a homomorphism of algebras and of B-modules, that is, fexDA=exDBf.

    As in the case of characteristic zero, we have:

    Lemma 2.10. Let V and U be nonlocal vertex algebras and let f be a linear map from V to U.If

    f(1)=1,fY(u,x)v=Y(f(u),x)f(v)for  uT,vV,

    where T is a generating subset of V, then f is a homomorphism of nonlocal vertex algebras.

    Proof. Set

    S={uV|f(Y(u,x)w)=Y(f(u),x)f(w) for wV}.

    We must show that V=S. Since TS and T generates V, it suffices to show that S is a nonlocal vertex subalgebra of V. As 1S, it remains to show that for u,vS and nZ we have unvS, that is,

    f(Y(Y(u,x0)v,x2)w)=Y(f(Y(u,x0)v),x2)f(w) (2.19)

    for wV. Let lN be such that

    (x0+x2)lY(u,x0+x2)Y(v,x2)w=(x0+x2)lY(Y(u,x0)v,x2)w,(x0+x2)lY(f(u),x0+x2)Y(f(v),x2)f(w)=(x0+x2)lY(Y(f(u),x0)f(v),x2)f(w).

    Since u,vS, we have

    (x0+x2)lfY(Y(u,x0)v,x2)w=(x0+x2)lfY(u,x0+x2)Y(v,x2)w=(x0+x2)lY(f(u),x0+x2)fY(v,x2)w=(x0+x2)lY(f(u),x0+x2)Y(f(v)v,x2)f(w)=(x0+x2)lY(Y(f(u),x0)f(v),x2)f(w)=(x0+x2)lY(f(Y(u,x0)v),x2)f(w).

    Multiplying both sides by (x2+x0)l, we obtain (2.19).

    Let V be a nonlocal vertex algebra and let A be a B-module algebra. Following [13], we consider V as a subalgebra of VA by the natural embedding, and consider VA as an A-module with A acting on the second factor. Then

    HomF(V,VA)=EndA(VA)

    as A-modules and as spaces. We also consider any linear map from V to VA or from V to V as an A-linear endomorphism of VA. Then we consider the vertex operator map Y of V as an A-linear map from VA to (End(VA))[[x,x1]], that is,

    Y(va,x)=Y(v,x)afor vV, aA.

    We denote by Yten the vertex operator map of VA.

    Lemma 2.11. Let V be a nonlocal vertex algebra, let A be a B-module algebra, and let f be a linear map from V to VA.Then f is a homomorphism of nonlocal vertex algebras if and only if

    f(1)=1,fY(v,x)=Y((1exD)f(v),x)ffor    vV.

    Proof. For any uV and aA, we see that

    Yten(ua,x)=Y(u,x)Y(a,x)=Y(u,x)(exDa)=Y((1exD)(ua),x).

    It follows that

    Yten(f(v),x)=Y((1exD)f(v),x)for vV.

    Then for vV, we see fY(v,x)=Yten(f(v),x)f is equivalent to

    fY(v,x)=Y((1exD)f(v),x)f.

    Thus our assertion follows.

    We denote by F((x)) the B-module algebra F((x)) with D(n) acting as (1)n(n)x for nN. Now we consider the special case with A=F((x)).

    Definition 2.12. Let V be a nonlocal vertex algebra. We define PEnd(V) to be the subspace of HomF(V,VF((x))) consisting of the elements f(x) such that

    f(x)1=1,f(x1)Y(u,x2)=Y(f(x1x2)u,x2)f(x1)for uV.

    Lemma 2.13. Let V be a nonlocal vertex algebra and let f(x)HomF(V,VF((x))).Then f(x)PEnd(V) if and only if f(x) is a homomorphism of nonlocal vertex algebrasfrom V to VF((x)).Furthermore,

    ezDVf(x)ezDV=f(x+z)for  f(x)PEnd(V). (2.20)

    Proof. Since ex2xg(x)=g(xx2) for g(x)F((x)), we have

    f(xx2)u=(1ex2x)f(x)ufor uV.

    Thus the first assertion follows from Lemma 2.11.

    For f(x)PEnd(V), since f(x) is a homomorphism of nonlocal vertex algebras, we have

    f(x)ezDV=(ezDVezx)f(x)=ezDVf(x+z).

    Then (2.20) holds.

    Let V be a nonlocal vertex algebra. We say a subset U of Hom(V,VF((x))) is Δ-closed if for every a(x)U, there exist elements a(1i)(x),a(2i)(x)U, i=1,2,,r, such that

    a(x1)Y(u,x2)=ri=1Y(a(1i)(x1x2)u,x2)a(2i)(x1)for uV. (2.21)

    We denote by B(V) the sum of all the Δ-closed subspaces U of Hom(V,VF((x))) such that

    a(x)1F1for a(x)U.

    Using the same arguments in [13, Proposition 3.4] we have:

    Lemma 2.14. Let V be a nonlocal vertex algebra.Then B(V) is Δ-closed and B(V) is a B-module algebra with D(n) acting as (n)x for nN.Furthermore, V is a module for B(V) as a nonlocal vertex algebra with YV(a(x),x0)=a(x0) for a(x)B(V).

    The following notion is the modular counterpart of the notion of differential bialgebra in [13].

    Definition 2.15. A B-module bialgebra is a bialgebra (B,Δ,ε) endowed with a B-module structure such that εexD=ε and ΔexD=(exDexD)Δ.

    We shall need the following notion (see [13]).

    Definition 2.16. A nonlocal vertex algebra V endowed with a coalgebra structure (V,Δ,ε) is called a vertex bialgebra if Δ and ε are homomorphisms of nonlocal vertex algebras.

    Let (B,Δ,ε) be a B-module bialgebra. Then B is a B-module algebra, and we have a nonlocal vertex algebra B by Example 2.7. From definition we have Δ(1)=11 and ε(1)=1. Furthermore,

    ε(Y(a,x)b)=ε((exDa)b)=ε(exDa)ε(b)=ε(a)ε(b)=Y(ε(a),x)ε(b),Δ(Y(a,x)b)=Δ((exDa)b)=Δ(exDa)Δ(b)=((exDexD)Δ(a))Δ(b)=Y(Δ(a),x)Δ(b)

    for a,bB. Then Δ and ε are nonlocal vertex algebra homomorphisms. Thus B is a vertex bialgebra.

    Definition 2.17. Let H be a vertex bialgebra. A nonlocal vertex H-module-algebra is a nonlocal vertex algebra V endowed with an H-module structure on V such that

    Y(h,x)uVF((x)),Y(h,x)1V=ε(h)1V,Y(h,x1)Y(v,x2)u=Y(Y(h(1),x1x2)v,x2)Y(h(2),x1)u

    for hH, u,vV.

    The following results of [13] hold with the same arguments.

    Lemma 2.18. Let H be a vertex bialgebra, let T be a generating subset of H as a nonlocal vertex algebra, let V be a nonlocal vertex algebra, and let (V,YHV) be an H-module.Suppose that

    YHV(h,x)Hom(V,VF((x))),YHV(h,x)1=ε(h)1,YHV(h,x1)Y(v,x2)u=Y(YHV(h(1),x1x2)v,x2)YHV(h(2),x1)u

    for hT and u,vV.Then V is a nonlocal vertex H-module-algebra.

    Theorem 2.19. Let H be a vertex bialgebra, and let V be a nonlocal vertex H-module-algebra.We define VH=VH as a vector space and define

    Y(uh,x)(vk)=Y(u,x)Y(h(1),x)vY(h(2),x)k.

    for u,vV and h,kH.Then (VH,Y) is a nonlocal vertex algebra.Furthermore,

    Y(h,x1)Y(v,x2)=Y(Y(h(1),x1x2)v,x2)Y(h(2),x1)

    for hH and vV.

    In [9], Dong and Griess introduced an integral form of vertex operator algebras associated to even lattices over the complex field, from which one can define modular lattice vertex algebras. In this section, we construct the modular lattice vertex algebras through smash product.

    Let L be a positive definite even lattice with a basis {γ1,,γd} and let L be the dual lattice of L. Let AL denote the d×d matrix (γi,γj)1i,jd. Note that det(AL) is independent of the choice of a basis for L. Let ϵ:L×LF× be a map such that

    ϵ(α,0)=ϵ(0,α)=1,ϵ(α,β+γ)ϵ(β,γ)=ϵ(α+β,γ)ϵ(α,β)

    for α,β,γL. Denote by Fϵ[L] the ϵ-twisted group algebra of L with F-basis {eααL} and multiplication

    eαeβ=ϵ(α,β)eα+βfor α,βL.

    Next, recall from [9] the ring M(1)Z. Denote by M(1) the polynomial algebra generated by sα,n for α{γ1,,γd} and nZ+. Set sα,0=1 for α{γ1,,γd}. For α{γ1,,γd}, we set

    E(α,x)=nNsα,nxnM(1)[[x]].

    Note that E(α,x) is an invertible element of M(1)[[x]] as sα,0=1. For a general element α=k1γ1+k2γ2++kdγdL, where k1,,kdZ, we define

    E(α,x)=di=1E(γi,x)kiM(1)[[x]].

    Then for α,βL,

    E(α,x)E(β,x)=E(α+β,x),E(0,x)=1.

    As M(1) is isomorphic to the universal enveloping algebra of the abelian Lie algebra with basis {sα,nα{γ1,,γd},nZ+}, we see M(1) is naturally a bialgebra with

    ε(E(α,x))=1, (3.1)
    Δ(E(α,x))=E(α,x)E(α,x) (3.2)

    for αL.

    Define a B-action on M(1) by ezD1=1 and

    ezDri=1E(αi,xi)=ri=1E(αi,xi+z)E(αi,z) (3.3)

    for rZ+, αi{γ1,,γd}. Then (3.3) holds for rZ+, αiL. It is straightforward to check

    e(z+z0)D=ezDez0Don M(1),ezD(ab)=(ezDa)(ezDb)for a,bM(1).

    Then M(1) is a B-module algebra. Furthermore, for rZ+, αiL, we have

    εezDri=1E(αi,xi)=εri=1E(αi,xi+z)E(αi,z)=1=εri=1E(αi,xi),

    and

    ΔezDri=1E(αi,xi)=Δri=1E(αi,xi+z)E(αi,z)=(ri=1E(αi,xi+z)E(αi,z))(ri=1E(αi,xi+z)E(αi,z))=(ezDri=1E(αi,xi))(ezDri=1E(αi,xi))=(ezDezD)Δri=1E(αi,xi).

    Therefore, (M(1),Δ,ε) is a B-module bialgebra.

    For α{γ1,γ2,,γd}, we inductively define linear operators rα,n for nN on M(1) by

    rα,n1=δn,01, (3.4)
    rα,nri=1sβi,mi=j1,,jrN(ri=1(1)ji(α,βiji)sβi,miji)rα,nj1jr1 (3.5)

    for βi{γ1,γ2,,γd}, miN, where rα,m is understood to be zero if m<0. From (3.5), we see

    rα,nsβ,m=iN(1)i(α,βi)sβ,mirα,nion M(1) (3.6)

    for β{γ1,γ2,,γd} and mN. For α{γ1,γ2,,γd}, we set

    E+(α,x)=nNrα,nxn(EndM(1))[[x1]].

    Furthermore, for α=k1γ1+k2γ2++kdγdL, where k1,,kdZ, we define

    E+(α,x)=di=1E+(γi,x)ki(EndM(1))[[x1]].

    Then for α,βL,

    E+(α,x)E+(β,x)=E(α+β,x),E+(0,x)=1,

    and furthermore,

    E+(α,x1)E(β,x2)=(1x2x1)α,βE(β,x2)E+(α,x1). (3.7)

    Lemma 3.1. In the B-module algebra M(1), we have

    Δ(E(α,x)E+(α,x)u)=(E(α,x)E+(α,x)E(α,x))Δu (3.8)

    for αL and uM(1).

    Proof. We use induction on m to show (3.8) holds for u=sα1,n1sα2,n2sαm,nm with mN, αiL, niN. For u=1, we have

    ΔE(α,x)E+(α,x)1=ΔE(α,x)=E(α,x)E(α,x)=(E(α,x)E+(α,x)E(α,x))(11)=(E(α,x)E+(α,x)E(α,x))Δ1.

    The induction step is given by

    ΔE(α,x)E+(α,x)E(β,z)u=(1zx)α,βΔE(β,z)E(α,x)E+(α,x)u=(1zx)α,β(ΔE(β,z))(ΔE(α,x)E+(α,x)u)=(1zx)α,β(E(β,z)E(β,z))(E(α,x)E+(α,x)E(α,x))Δu=(1zx)α,β(E(β,z)E(α,x)E+(α,x)E(β,z)E(α,x))Δu=(E(α,x)E+(α,x)E(β,z)E(α,x)E(β,z))Δu=(E(α,x)E+(α,x)E(α,x))ΔE(β,z)u.

    This completes the induction. As M(1) is spanned by elements of the form

    sα1,n1sα2,n2sαm,nm,

    our assertion follows.

    Set

    BL,ϵ=Fϵ[L]M(1), (3.9)

    an associative algebra.

    Lemma 3.2. For αL and uM(1), define

    exD(eαu)=eαE(α,x)exDu.

    Then BL,ϵ is a B-module algebra.

    Proof. For eαu,eβvBL,ϵ, we have

    exD((eαu)(eβv))=ϵ(α,β)exD(eα+βuv)=ϵ(α,β)eα+βE(αβ,x)exD(uv)=eαeβE(α,x)E(β,x)(exDu)(exDv)=(eαE(α,x)(exDu))(eβE(β,x)(exDv))=(exDeαu)(exDeβv).

    Thus BL,ϵ is a B-module algebra.

    Set

    BL=F[L]M(1), (3.10)

    a unital commutatively associative algebra. As in the case of characteristic zero (see [13]), we have the following universal property of BL:

    Lemma 3.3. Let A be a B-module algebra and let f:F[L]A be a homomorphism of algebras.Then f can be extended uniquely to a homomorphism of B-module algebras from BL to A.

    Proof. For α{γ1,γ2,,γd}, define

    fE(α,x)=(feα)exDfeα. (3.11)

    Since M(1) is freely generated by sα,n for α{γ1,γ2,,γd} and nZ+, it follows that f can be extended to a homomorphism of algebras.

    Now, we show that in fact (3.11) holds for all αL. Let P be the subset of L consisting of α such that (3.11) holds for all nN. From definition, we have γiP for 1id. Assume α,βP. Then we get

    fE(αβ,x)=f(E(α,x)E(β,x))=(feα)(exDfeα)(feβ)(exDfeβ)=(feα)(feβ)(exDfeα)(exDfeβ)=(feαβ)exD((feα)(feβ))=(feαβ)exD(feα+β),

    proving α+βP.

    Now, assume αP. As E(α,x)E(α,x)=1 and (exDfeα)(exDfeα)=exD1=1, we have

    fE(α,x)=(fE(α,x))1=((feα)exDfeα)1=(feα)exDfeα,

    proving αP. Thus P=L, that is, (3.11) holds for all αL.

    Next we show that f is a homomorphism of B-modules. For αL, we have

    fexD(eα)=f(eαE(α,x))=(feα)(feα)exD(feα)=exD(feα).

    Using the equation above and (3.3), we have

    exDfE(α,z)=exD((feα)ezDfeα)=(exDfeα)(exDezDfeα)=(feα)(exDfeα)(feα)(e(z+x)Dfeα)=f(E(α,x))f(E(α,z+x))=f(E(α,x)E(α,z+x))=fexDE(α,z).

    Since BL as an algebra is generated by sα,n and eα for αL and nN, it follows that fexD=exDf. Thus f is a B-module homomorphism.

    For αL, we define xα(EndVL)[x,x1] by

    xα(eβu)=xα,β(eβu) (3.12)

    for βL and uM(1).

    Lemma 3.4. For αL, we have

    E+(α,x)xαPEnd(BL,ϵ).

    Proof. For βL, we have

    (ex2DE+(α,x1x2)(x1x2)αeβ)E+(α,x1)xα1=(x1x2)α,β(ex2Deβ)E+(α,x1)xα1=(x1x2)α,βE(β,x2)eβE+(α,x1)xα1=(x1x2)α,βE(β,x2)E+(α,x1)eβxα1=(x1x2)α,β(1x2x1)α,βE+(α,x1)E(β,x2)eβxα1=xα,β1(x1x2)α,β(1x2x1)α,βE+(α,x1)E(β,x2)xα1eβ=E+(α,x1)E(β,x2)xα1eβ=E+(α,x1)xα1ex2Deβ.

    Since L generates VL,ϵ as a nonlocal vertex algebra, it follows from Lemma 2.10 that E+(α,x)xα is a homomorphism of nonlocal vertex algebras. By Lemma 2.13, we see that E+(α,x)xαPEnd(BL,ϵ).

    Lemma 3.5. There exists a unique BL-module structure YM on BL,ϵ such that

    YM(eα,x)=E+(α,x)xαfor  αL,

    and (BL,ϵ,YM) is a nonlocal vertex BL-module-algebra.

    Proof. Denote Φα(x)=E+(α,x)xα for αL. By Lemma 3.4, we have Φα(x)PEnd(BL,ϵ). Clearly Φ0(x)=1 and

    Φα(x)Φβ(x)=Φα+β(x)for α,βL.

    Let A be the subalgebra of B(BL,ϵ) generated by (n)xΦα(x) for nN, αL. Clearly A is a commutative B-module algebra. By Lemma 3.3, there exists a homomorphism f of B-module algebras from BL to A such that f(eα)=Φα(x) for all αL. Then by Lemma 2.18 we see that BL,ϵ is a nonlocal vertex BL-module-algebra.

    As BL,ϵ is a nonlocal vertex BL-module-algebra by Lemma 3.5, we have the nonlocal vertex algebra BL,ϵBL by Theorem 2.19.

    Theorem 3.6. Denote

    U=αLF(eαeα)Δ(M(1)),

    a subspace of BL,ϵBL.Then U is a vertex subalgebra of the nonlocal vertex algebra BL,ϵBL, and the linear map

    π:VLU,eαu(eαeα)Δ(u)

    for αL and uM(1) is a vertex algebra homomorphism.Furthermore, if det(AL)0(modp), the map π is an isomorphism.

    Proof. This is a slight modification of the proof in [13]. As Δ is a homomorphism from M(1) to M(1)M(1), we see that π is a linear homomorphism. We then show that π is a vertex algebra homomorphism. Let α,βL and uM(1). Then we have

    YVL(eα,x)(eβu)=xα,βϵ(α,β)(eα+βE(α,x)E+(α,x)u).

    By Lemma 3.1, we have

    π(YVL(eα,x)(eβu))=xα,βϵ(α,β)(eα+βeα+β)Δ(E(α,x)E+(α,x)u)=xα,βϵ(α,β)(eα+βeα+β)(E(α,x)E+(α,x)E(α,x))Δ(u).

    Since Δ(eα)=eαeα, by Lemma 3.2 we have

    Y(eαeα,x)=YBL,ϵ(eα,x)YM(eα,x)YBL(eα,x)=E(α,x)eαE+(α,x)xαE(α,x)eα.

    Then

    Y(eαeα,x)π(eβu)=E(α,x)eαE+(α,x)xαE(α,x)eα(eβeβ)Δ(u)=xα,βϵ(α,β)(eα+βeα+β)(E(α,x)E+(α,x)E(α,x))Δ(u).

    Therefore

    π(YVL(eα,x)(eβu))=Y(eαeα,x)π(eβu)

    for α,βL and uM(1). Since L generates VL as a vertex algebra by [10, Theorem 1], it follows from Lemma 2.10 that π is a nonlocal vertex algebra homomorphism. As VL is a vertex algebra, we see that π is a vertex algebra homomorphism. If det(AL)0(modp), it follows from [10, Theorem 13] that VL is a simple vertex algebra, then π is an isomorphism.

    Extend ϵ to a map from L×L to F× such that

    ϵ(α,β)ϵ(α+β,γ)=ϵ(α,β+γ)ϵ(β,γ)

    for α,βL and γL (see [14]). Define an Fϵ[L]-module structure on F[L] by

    eαeγ=ϵ(α,γ)eα+γfor αL,γL.

    Set

    VL=F[L]M(1).

    By the same proof of [13, Proposition 5.8], we have:

    Proposition 3.7. There exists a unique VL-module structure on VL such that

    Y(eα,x)=E(α,x)E+(α,x)eαxα

    for αL.

    The author was supported by the China NSF (grant 11571391) and the Heilongjiang Provincial NSF (grant JQ2020A002).

    The authors declare there is no conflicts of interest.



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