Loading [MathJax]/jax/output/SVG/jax.js
Theory article

Derivations of finite-dimensional modular Lie superalgebras ¯K(n,m)

  • Received: 28 February 2023 Revised: 08 May 2023 Accepted: 22 May 2023 Published: 01 June 2023
  • This paper is aimed at determining the derivation superalgebra of modular Lie superalgebra ¯K(n,m). To that end, we first describe the Z-homogeneous derivations of ¯K(n,m). Then we obtain the derivation superalgebra Der(¯K). Finally, we partly determine the derivation superalgebra Der(K) by virtue of the invariance of K(n,m) under Der(¯K).

    Citation: Dan Mao, Keli Zheng. Derivations of finite-dimensional modular Lie superalgebras ¯K(n,m)[J]. Electronic Research Archive, 2023, 31(7): 4266-4277. doi: 10.3934/era.2023217

    Related Papers:

    [1] Baoling Guan, Xinxin Tian, Lijun Tian . Induced 3-Hom-Lie superalgebras. Electronic Research Archive, 2023, 31(8): 4637-4651. doi: 10.3934/era.2023237
    [2] Yusi Fan, Chenrui Yao, Liangyun Chen . Structure of sympathetic Lie superalgebras. Electronic Research Archive, 2021, 29(5): 2945-2957. doi: 10.3934/era.2021020
    [3] Ying Hou, Liangyun Chen . Constructions of three kinds of Bihom-superalgebras. Electronic Research Archive, 2021, 29(6): 3741-3760. doi: 10.3934/era.2021059
    [4] Ying Hou, Liangyun Chen, Keli Zheng . Super-bimodules and O-operators of Bihom-Jordan superalgebras. Electronic Research Archive, 2024, 32(10): 5717-5737. doi: 10.3934/era.2024264
    [5] Hongliang Chang, Yin Chen, Runxuan Zhang . A generalization on derivations of Lie algebras. Electronic Research Archive, 2021, 29(3): 2457-2473. doi: 10.3934/era.2020124
    [6] Wen Teng, Xiansheng Dai . Nonabelian embedding tensors on 3-Lie algebras and 3-Leibniz-Lie algebras. Electronic Research Archive, 2025, 33(3): 1367-1383. doi: 10.3934/era.2025063
    [7] Kailash C. Misra, Sutida Patlertsin, Suchada Pongprasert, Thitarie Rungratgasame . On derivations of Leibniz algebras. Electronic Research Archive, 2024, 32(7): 4715-4722. doi: 10.3934/era.2024214
    [8] Margarida Camarinha . A natural 4th-order generalization of the geodesic problem. Electronic Research Archive, 2024, 32(5): 3396-3412. doi: 10.3934/era.2024157
    [9] Jinguo Jiang . Algebraic Schouten solitons associated to the Bott connection on three-dimensional Lorentzian Lie groups. Electronic Research Archive, 2025, 33(1): 327-352. doi: 10.3934/era.2025017
    [10] Shanshan Liu, Abdenacer Makhlouf, Lina Song . The full cohomology, abelian extensions and formal deformations of Hom-pre-Lie algebras. Electronic Research Archive, 2022, 30(8): 2748-2773. doi: 10.3934/era.2022141
  • This paper is aimed at determining the derivation superalgebra of modular Lie superalgebra ¯K(n,m). To that end, we first describe the Z-homogeneous derivations of ¯K(n,m). Then we obtain the derivation superalgebra Der(¯K). Finally, we partly determine the derivation superalgebra Der(K) by virtue of the invariance of K(n,m) under Der(¯K).



    Lie superalgebras, which originated from the research of quantum physics (see [1]), can be considered as the natural generalization of Lie algebras. Lie superalgebras are closely connected with mathematical physics as well as numerous branches of mathematics (see [2,3]). Based on the study of Lie algebras, the theory of Lie superalgebras developed rapidly, including the completed classification of finite dimensional simple Lie superalgebras in 1977 (see [4]). However, the classification of finite dimensional simple modular Lie superalgebras has not been accomplished up to now. Since the main difference between modular Lie superalgebras and Lie superalgebras in characteristic zero is the algebras of cartan type, we pay more attention to the related researches on modular Lie superalgebras of Cartan type. In [5,6], authors investigated the associative forms of modular Lie superalgebras of Cartan type. The natural filtrations (see [7,8,9,10]) and automorphisms (see [10,11]) of some Cartan type modular Lie superalgebras are studied. In addition, the cohomologies (see [6,12,13]) of some modular Lie superalgebras have also been determined.

    It is known to all that the determination of derivation superalgebras is crucial to Lie superalgebras. The related research results in Cartan type modular Lie superalgebras are also quite rich. The derivation superalgebras of some finite dimensional simple modular Lie superalgebras of Cartan type such as K(m,n,t_), W(m,n,t_), S(m,n,t_), HO(n,n;t_), KO(n,n+1,t_), SHO(m,m,t_)(2) (see [14,15,16,17,18]) are determined, respectively. Moreover, the derivation superalgebras of some nonsimple ones are also described, where we are most interested in the correlative results of ¯W(n,m), H(n,m) and S(n,m) (see [19,20,21]). They all possess the derivation of Θ-type. In [22], we have constructed a class of finite dimensional modular Lie superalgebra of Contact type which is denoted by ¯K(n,m). This paper is aimed at determining the derivation superalgebras of ¯K(n,m).

    The present paper is arranged as follows. In Section 2, certain essential notations and concepts are recalled. In Section 3, the Z-homogeneous components of Der(¯K), the derivation superalgebras of ¯K(n,m), are described, respectively. Therefore, we determine Der(¯K). In order to give a description of Der(¯K), we prove that K(n,m) is invariant under Der(¯K).

    Hereafter F denotes a field of characteristic p3; Z2={¯0,¯1} is the ring of integers modulo 2. Apart from the standard notation Z, let N and N0 denote the sets of positive integers and nonnegative integers, respectively. A simple description of construction of the modular Lie superalgebra ¯K(n,m) in [22] will be given.

    Let Λ(n) be the Grassmann algebra over F in n variables x1,x2,,xn. Suppose that Bk={i1,i2,,ik1i1<i2<<ikn} and B(n)=nk=0Bk, where B0=. For u=i1,i2,,ikBk, set |u|=k, {u}={i1,i2,,ik} and xu=xi1xi2xik (||=0,x=1). Then {xu|uB(n)} is an F-basis of Λ(n).

    Let U=Λ(n)T(m) be the tensor product, where T(m) is the truncated polynomial algebra satisfying ypi=1 for all i=1,2,,m (see [20]). Then U is an associative superalgebra with Z2-gradation, which is induced by the trivial Z2-gradation of T(m) and the natural Z2-gradation of Λ(n). Namely, U=U¯0U¯1, where U¯0=Λ(n)¯0T(m) and U¯1=Λ(n)¯1T(m).

    For fΛ(n) and αT(m), we abbreviate fα as fα. Then the elements xuyλ with uB(n) and λG form an F-basis of U. Obviously, U=ni=0Ui is a Z-graded superalgebra, where Ui=spanF{xuyλuB(n),|u|=i,λG}. In particular, U0=T(m) and Un=spanF{xπyλλG}, where π:=1,2,,nB(n).

    In this paper, let hg(A)=Aˉ0Aˉ1, where A=Aˉ0Aˉ1 is a superalgebra. If x is a Z2-homogeneous element of A, then degx denotes the Z2-degree of x.

    Set Y={1,2,,n}. Given iY, let /xi be the partial derivative on Λ(n) with respect to xi. For iY, let Di be the linear transformation on U such that Di(xuyλ)=(xu/xi)yλ for all uB(n) and λG. Let DerU denote the derivation superalgebra of U(see [12]). Then DiDerˉ1U for all iY since /xiDerˉ1(Λ(n)) (see [23]).

    Suppose that uBkB(n) and iY. When i{u}, ui denotes the uniquely determined element of Bk1 satisfying {ui}={u}{i}.Then the number of integers less than i in {u} is denoted by τ(u,i). When i{u}, we set τ(u,i)=0 and xui=0. Therefore, Di(xu)=(1)τ(u,i)xui for all iY and uB(n).

    We define (fD)(g)=fD(g) for f,ghg(U) and Dhg(DerU). Since the multiplication of U is supercommutative, fD is a derivation of U. Let

    W(n,m)=spanF{xuyλDiuB(n),λG,iY}.

    Then W(n,m) is a finite dimensional Lie superalgebra contained in DerU. A direct computation shows that

    [fDi,gDj]=fDi(g)Dj(1)deg(fDi)deg(gDj)gDj(f)Di.

    where f,ghg(U) and i,jY.

    Set J={1,...,n1}. Let ˜Dk:UW(n,m) be the linear map such that

    ˜Dk(f)=iJfiDi+fnxnDn,

    where fhg(U), fi=(1)degf(xixnDn(f)+Di(f)),iJ and fn=2fiJxiDi(f).

    Let ¯K(n,m) = spanF{˜Dk(f)|fU}. Then ¯K(n,m) is a subspace of W(n,m).

    Let

    Gi=Di+xixnDn,iJ,Gn=2xnDn.

    By direct calculation, we have

    [Gi,Gj]=δijGn,[Gn,Gj]=0,

    where i,jJ and δij is Kronecker delta.

    It is easy to prove that ˜Dk(f)=iJ(1)degfGi(f)Gi+fGn

    For fUθ and gUμ, where θ,μZ2, set f,g=˜Dk(f)(g)Gn(f)(g). In [22], we have proved that [˜Dk(f),˜Dk(g)]=˜Dk(f,g). Namely, ¯K(n,m) is a subalgebra of W(n,m).

    If we define an operator [,] in U such that [f,g]=˜Dk(f)(g)Gn(f)(g) for any f,gU. Then ¯K(n,m)(U,[,]). Moreover, for any f,g¯K(n,m), we have

    [f,g]=(2fiJxiDi(f))xnDn(g)(1)deg(f)deg(g)(2giJxiDi(g))xnDn(f)+iJ(1)degfDi(f)Di(g).

    Let K(n,m) be the derived algebra of ¯K(n,m), then K(n,m)=spanF{xuyλ|xuyλU,xuyλxˆuyλ}, where ˆu=1,...,n1. By [22], we know that modular Lie superalgebra K(n,m) is not simple.

    In this section, we will abbreviate ¯K(n,m), K(n,m) as ¯K and K, respectively.

    In [22], we proved that K(n,m) does not possess a Z-graded structure as W(n,m) (see [19]). In fact, ¯K(n,m) does not possess Z-gradation in the ordinary sense as well. If ¯K=si=r¯Ki, then it does not satisfy that

    [¯Ki,¯Kj]¯Ki+j,i,j{r,r+1,...,s}.

    Now we give a "formal" Z-gradation of ¯K(n,m):

    ¯K(n,m)=n2i=2¯K(n,m)i,

    where ¯K(n,m)i=spanF{xuyλ|uB(n),|u|=i+2,λG}. Let

    Dert(¯K)={φDer(¯K)|φ(¯Ki)¯Kt+i,iZ}.

    It is easy to prove that Der(¯K)=tZDert(¯K) is a Z-graded Lie superalgebra (see [24]).

    Lemma 3.1. Let φDer(¯K), f¯K and [f,xi]=bi, iJ. If φ(xi)=φ(bi)=0, iJ, then φ(f)¯K2.

    Proof. By applying φ to [f,xi]=bi, we obtain [φ(f),xi]+(1)degφdegf[f,φ(xi)]=φ(bi). Since φ(xi)=φ(bi)=0, we have [φ(f),xi]=0, iJ. Note that

    [φ(f),1]=[φ(f),[x1,x1]]=[φ(f),[x1,x1]]=([[φ(f),x1],x1]+[x1,[φ(f),x1]])=0.

    Therefore, 2xnDn(φ(f))=[φ(f),1]=0. Then Dn(φ(f))=0. For all iJ,

    [φ(f),xi]=(2φ(f)tJxtDt(φ(f)))xnDn(xi)(1)deg(φ(f))deg(xi)(2xitJxtDt(xi))xnDn(φ(f))+tJ(1)degφ(f)Dt(φ(f))Dt(xi)=(1)degφ(f)Di(φ(f)).

    Since [φ(f),xi]=0, we obtain Di(φ(f))=0,iJ. Therefore, φ(f)¯K2.

    Lemma 3.2. Let φDert(¯K), t2. If φ(¯Kt2)=0, then φ=0.

    Proof. If s<t2, then φ(¯Ks)¯Kst={0}.

    When st2, we will use induction on s to prove that φ(¯Ks)=0. For s=t2, we have φ(¯Ks)=0 with the hypothesis of the lemma. Suppose s>t2. For any y¯Ks, iJ, set [y,Di]=yi. Then yi¯Ks, where s<s. According to the hypothesis of induction, we have φ(yi)=0. Noting that φ(Di)=0, we obtain φ(y)¯K2. Therefore, φ(y)¯K2¯Kst={0}. Namely, φ(y)=0. Then φ(¯Ks)=0. It follows that φ=0.

    Proposition 3.3. Dert(¯K)=0, t2.

    Proof. Let φDert(¯K),t2. We will prove φ(¯Kt2)=0, where

    ¯Kt2=spanF{xu1xnyλ,xu2yη|u1,u2B(n),|u1|=t1,|u2|=t,λ,ηG}.

    Note that φ(¯Kt2)¯K2. Without loss of generality, we put φ(xu1xnyλ)=ayμ, φ(xu2yη)=byμ, where a,bF, μG. Applying φ to [xn,xu1xnyλ]=0, we obtain

    [φ(xn),xu1xnyλ]+(1)degφdegxn[xn,φ(xu1xnyλ)]=0. (3.1)

    Since φ(xn)¯Kt1={0}, which combined with (3.1) yields [xn,φ(xu1xnyλ)]=0. Namely, [xn,ayμ]=0. In fact, [xn,ayμ]=2ayμxn. Therefore, 2ayμxn=0. Then

    φ(xu1xnyλ)=ayμ=0. (3.2)

    For i{u2}, we have

    [xixn,xu2yη]=(1)τ(u2,i)xu2ixnyη. (3.3)

    Without loss of generality, let xu2ixnyη=xuxnyη, where |u|=t1. Then we may write the Eq (3.3) as

    [xixn,xu2yη]=(1)τ(u2,i)xuxnyη. (3.4)

    By virtue of the Eq (3.2), we have φ(xuxnyη)=0. Applying φ to the Eq (3.4), we obtain

    [φ(xixn),xu2yη]+(1)degφdeg(xixn)[xixn,φ(xu2yη)]=0. (3.5)

    If t=2, it follows from the Eq (3.2) that φ(xixn)=0. If t>2, then φ(xixn)¯Kt={0}. Consequently, φ(xixn)=0. Therefore, by virtue of the Eq (3.5), we have [xixn,φ(xu2yη)]=0. Namely, [xixn,byμ]=0. In fact, [xixn,byμ]=2byμxixn. Therefore, 2byμxixn=0. Then

    φ(xu2yη)=byμ=0. (3.6)

    It follows from the Eqs (3.2) and (3.6) that φ(¯Kt2)=0. By virtue of Lemma 3.2, we have φ=0. Therefore, Dert(¯K)=0, t2.

    Lemma 3.4. Let φDert(¯K), tZ. Suppose that φ(¯Kj)=0, j=2,1,...,l. If t+l2, then φ=0.

    Proof. By virtue of Lemma 3.1, the proof is completely analogous to [24, Lemma 2.8].

    Proposition 3.5. Der1(¯K)=0.

    Proof. Let φDer1(¯K). Then φ(¯K2)=0. In order to prove φ=0, we need to obtain φ(¯K1)=0. Without loss of generality, we put φ(xnyλ)=ayμ, where aF,μG. Applying φ to [1,xnyλ]=2xnyλ yields (1)degφdeg1[1,ayμ]=2ayμ. Therefore, 2ayμ=0. Then φ(xnyλ)=ayμ=0. Similarly, we can prove that φ(xiyλ)=0, iJ. Therefore, φ(¯K1)=0. Then φ=0.

    Let Θ=T(m)×...×T(m). For every θ=(h1(y),...,hm(y))Θ, we define ˜θ:GT(m). (see [20]) For every θΘ,we define Dθ:¯K¯K such that Dθ(˜Dk(xuyλ))=˜θ(λ)˜Dk(xuyλ), for xuyλU. A direct computation shows that DθDer¯0(¯K), for all θΘ. Put Ω={Dθ|θΘ}.

    Proposition 3.6. Der0(¯K)=ad¯K2+Ω.

    Proof. Assume that yλ¯K2. For f¯Kj,j{2,1,...,n2}, we have

    (adyλ)(f)=[yλ,f]=(2yλiJxiDi(yλ))xnDn(f)(1)deg(yλ)deg(f)(2fiJxiDi(f))xnDn(yλ)+iJ(1)degyλDi(yλ)Di(f)=2yλxnDn(f)¯Kj.

    Therefore, ad¯K2Der0(¯K). Obviously, ΩDer0(¯K). It follows that ad¯K2+ΩDer0(¯K).

    Conversely, let φDer0(¯K). It is obvious that there exist yμ¯K2 and DθΩ such that (φadyμDθ)(¯K2)=0. Consequently, by lemma 3.4, we have φadyμDθ=0. Then φ=adyμ+Dθad¯K2+Ω. Thus, Der0(¯K)ad¯K2+Ω.

    Lemma 3.7. Let h1,...,hn be the nonzero elements of U. If Gi(hj)=Gj(hi) for all distinct i,jY, then there exists nonzero element hU such that Gi(h)=hi, for iJ and Gn(h)=hn.

    Proof. We use induction to prove there exist nonzero element hU such that Gi(h)=hi for all iJ.

    When n1=1, let h=x1h10. Then

    G1(h)=(D1+x1xnDn)(x1h1)=h1.

    Suppose that there exists 0gU such that Gi(g)=hi for all i{1,...,n2}. For i{1,...,n2},

    Gi(hn1)=Gn1(hi)=Gn1(Gi(g))=Gi(Gn1(g)).

    Therefore, Gi(hn1Gn1(g))=0. Let h=g+xn1(hn1Gn1(g)). For i{1,...,n2},

    Gi(h)=Gi(g)+Gi(xn1(hn1Gn1(g))=Gi(g)=hi.

    On the other hand,

    Gn1(h)=Gn1(g)+Gn1(xn1(hn1Gn1(g))=hn1.

    Consequently, we have Gi(h)=hi, for all i{1,...,n1}. For i{1,...,n1},

    Gi(hn)=Gn(hi)=Gn(Gi(h))=Gi(Gn(h)).

    Then Gi(hn+Gn(h))=0. Therefore, hn+Gn(h)=0. Namely, Gn(h)=hn. Consequently, the assertion follows from h=h.

    Lemma 3.8. Let φh(Dert(¯K)), tN. If φ(Gj)=0, jY, then there exists θΘ such that φ(˜Dk(yλ))=Dθ(˜Dk(yλ)), for λG.

    Proof. Assume that for every iY, φ(yλGi)=nk=1gkiλGk, where gkiλU. Applying φ to [Gi,yλGn]=0, iY yields gknλT(m). Let g(y)knλ=gknλ. Then φ(yλGn)=nk=1g(y)knλGk. Note that [Gj,yλGi]=0 and [Gi,yλGi]=yλGn for all iJ, ijY. Applying φ to these equations, we know that gkiλ contains at most xi in Λ(n). Let gkiλ=g(xi,y)kiλ, iJ. For jJ, let ˜Dk(xj)=nk=1akGk. Since [Gj,Gj]=Gn and [Gj,˜Dk(xj)]=0, we obtain

    [Gj,Gj+˜Dk(xj)]=Gn. (3.7)

    Applying φ to (3.7) yields (1)degφ[Gj,φ(Gj+˜Dk(xj))]=0. Then [Gj,φ(˜Dk(xj))]=0. Namely, [Gj,nk=1akGk]=0. Therefore, Gj(ak)=0,kY. Applying φ to [yλGj,Gj+˜Dk(xj)]=yλGn yields

    [φ(yλGj),Gj+˜Dk(xj)]+(1)degφ[yλGj,φ(˜Dk(xj))]=φ(yλGn).

    Therefore, [φ(yλGj),Gj+˜Dk(xj)]=φ(yλGn). Namely,

    [nk=1g(xj,y)kjλGk,Gj+˜Dk(xj)]=nk=1g(y)knλGk.

    A direct computation shows that g(y)knλ=0, kJ and g(xj,y)jjλ=g(y)nnλ. Then φ(yλGn)=g(y)nnλGn. We abbreviate g(y)nnλ as g(y)nλ. Let hnλ(y)=g(y)nλyλ. Then φ(yλGn)=hnλ(y)yλGn. Let φ(˜Dk(xjyη))=nk=1bkGk, where bkU. Note that

    [Gj,yηGj+˜Dk(xjyη)]=yηGn (3.8)

    Applying φ to (3.8) yields

    (1)degφ[Gj,φ(yηGj)+nk=1bkGk]=φ(yηGn). (3.9)

    Since g(xj,y)jjλ=g(y)nnλ, we know g(xj,y)jjηT(m). We may abbreviate g(xj,y)jjη as g(y)jη. Let hjη(y)=g(y)jηyη. It follows from (3.9) that

    (1)degφhjη(y)yηGn+(1)degφnk=1Gj(bk)Gk=hnη(y)yηGn.

    Then Gj(bn)=(hjη(y)+(1)degφhnη(y))yη and Gj(bi)=0,iJ. Therefore, bn=(hjη(y)+(1)degφhnη(y))yηxj+qn with Gj(qn)=0. Then

    φ(˜Dk(xjyη))=nk=1bkGk=(hjη(y)+(1)degφhnη(y))yηxjGn+qnGn+iJbiGi.

    Applying φ to [yλG,yηGj+˜Dk(xjyη)]=yλ+ηGn yields

    [φ(yλG),yηGj+˜Dk(xjyη)]+(1)degφ[yλG,φ(yηGj)+φ(˜Dk(xjyη))]=φ(yλ+ηGn).

    A calculation shows that

    hjλ(y)+hnη(y)=hn(λ+η)(y). (3.10)

    Particularly, hjλ(y)+hnλ(y)=hn(2λ)(y)=hnλ(y)+hnλ(y). Therefore, hjλ(y)=hnλ(y) for jJ. Consequently, we may abbreviate hiλ(y) as hλ(y) for iY. Then the Eq (3.10) can be equivalent to

    hλ(y)+hη(y)=hλ+η(y), (3.11)

    for λ,ηG. Therefore, for kY,cΠ, we have

    hczk(y)=chzk(y). (3.12)

    Let λ=mj=1λjzjG. It follows from (3.11) and (3.12) that

    hλ(y)=hλ1z1+...+λmzm(y)=mj=1λjhzj(y). (3.13)

    We abbreviate hzj(y) as hj(y) for j=1,...,m. Let θ=(h1(y),...,hm(y))Θ. It follows from (3.13) that hλ(y)=mj=1λjhzj(y)=˜θ(λ). Therefore,

    φ(˜Dk(yλ))=φ(yλGn)=hλ(y)yλGn=˜θ(λ)yλGn=Dθ(˜Dk(yλ)).

    Lemma 3.9. Let φh(Dert(¯K)), tN. Then there exist BNorW(¯K)={xW|[x,¯K]¯K} and θΘ such that φ=adB+Dθ.

    Proof. Assume that for every kJ, φ(Gk)=ni=1fikGi, where fikU and φ(Gn)=(1)degφni=1finGi, where finU. For klY, applying φ to [Gk,Gl]=0 yields

    Gl(fik)=Gk(fil)

    for all iY. It follows from lemma 3.7 that there exist gi(i=1,...,n) such that

    Gk(gi)=fik,kJ,Gn(gi)=fin.

    Let B=(1)degφni=1giGi. Then for any kJ,

    adB(Gk)=[B,Gk]=ni=1fikGi=φ(Gk),adB(Gn)=[B,Gn]=(1)degφni=1finGi=φ(Gn).

    Therefore, φ(Gj)=adB(Gj) for all jY. Namely, (φadB)(Gj)=0 for all jY. According to lemma 3.8, there exists θΘ such that

    (φadB)(˜Dk(yλ))=Dθ(˜Dk(yλ))

    for all λG. Let ϕ=φadBDθ. We use induction on j to prove ϕ(¯Kj)=0,j=2,1,0,...,n2. A direct computation shows that ϕ(¯K2)=0. Assume that j1. For any ξ¯Kj, let [ξ,Gn]=ξ1. Applying ϕ to this equation, we obtain

    [ϕ(ξ),Gn]+(1)degϕdegξ[ξ,ϕ(Gn)]=ϕ(ξ1).

    It follows from the induction hypothesis that ϕ(ξ1)=0. Since ϕ(Gn)=0, we have [ϕ(ξ),Gn]=0. Then ϕ(ξ)¯K1¯Kj+t={0}. Therefore, ϕ(ξ)=0. Since the choice of ξ was arbitrary, we have ϕ(¯Kj)=0. Consequently, φ=adB+Dθ.

    Lemma 3.10. Let ˆK(n,m)={jYfjGjW|Gi(fj)=Gj(fi)+(1)degfδijGn(f),i,jJ}. Then ¯K(n,m)=ˆK(n,m).

    Proof. Assume that jYfjGjˆK(n,m). According to lemma 3.7, there exists 0fU such that Gi(f)=fi for all iJ. Therefore, jYfjGj=jJGj(f)Gj+fnGn¯K(n,m). Then ˆK(n,m)¯K(n,m).

    Conversely, let ˜Dk(f)=ni=1fiGi¯K(n,m). For i,jJ,

    Gi(fj)=Gi((1)degfGj(f))=(1)degf(GjGi(f)+δijGn(f))=Gj((1)degfGi(f))+(1)degfδijGn(f)=Gj(fi)+(1)degfδijGn(f).

    Therefore, ˜Dk(f)ˆK(n,m). Then ¯K(n,m)ˆK(n,m).

    Consequently, ¯K(n,m)=ˆK(n,m).

    Proposition 3.11. Let tN. Then Dert(¯K)=ad(¯Kt)+Ω.

    Proof. It suffices to prove that Dert(¯K)ad(¯Kt)+Ω. Let φDert(¯K). By virtue of Lemma 3.9, there exists BNorW(¯K) such that φ(Gk)=adB(Gk), for kY. Assume that B=nj=1gjGj and plug it into the following equation, i.e.,

    (1)degBdegGj[Gj,[Gi,B]]+(1)degGjdegGi[Gi,[B,Gj]],+(1)degGidegB[B,[Gj,Gi]]=0

    for i,jJ. Accordingly, we have Gi(fj)+Gj(fi)(1)degfδijGn(f)=0,i,jJ. Therefore, B¯K(n,m). By virtue of Lemma 3.9, φ=adB+Dθad¯K+Ω. Then Dert(¯K)ad(¯Kt)+Ω. Consequently, Dert(¯K)=ad(¯Kt)+Ω.

    Lemma 3.12. The following statements hold:

    (1) Ω is a subspace of Der(¯K).

    (2) ad(¯K)Ω={0}.

    Proof. The proof is completely analogous to [20, Lemma 3.11].

    Theorem 3.13. Der(¯K)=ad(¯K)Ω, where ¯K=¯K2n2i=1¯Ki.

    Proof. By virtue of Propositions 3.3, 3.5, 3.6, 3.11 and Lemma 3.12, this theorem can be easily proved.

    Proposition 3.14. K(n,m) is invariant under Der(¯K).

    Proof. Let ϕΩ. Obviously, ϕ(K)K.

    Let ϕad(¯K). Without loss of generality, we may suppose that ϕ=adf, where f¯K¯K. Since K is a derived algebra of ¯K, K is an ideal of ¯K. Therefore, ϕ(K)=adf(K)=[f,K]K.

    Since Der(¯K)=ad(¯K)Ω, we have ϕ(K)K for any ϕDer(¯K). Namely, K(n,m) is invariant under Der(¯K).

    An immediate corollary of this proposition is the following.

    Corollary 3.15. Der(¯K)|KDer(K).

    Remark. If m=0, then derivation superalgebras of modular Lie superalgebras K(n), which were mentioned in [22], will be obtained.

    The authors give special thanks to referees for many helpful suggestions. This work was supported by the Fundamental Research Funds for the Central Universities (No.2572021BC02) and the National Natural Science Foundation of China (Grant No.11626056)

    The authors declare there is no conflicts of interest.



    [1] B. DeWitt, Supermanifolds, 2nd edition, Cambridge University Press, Cambridge, 1992.
    [2] P. Fayet, S. Ferrara, Supersymmetry, Phys. Rep., 32 (1977), 249–334. https://doi.org/10.1016/0370-1573(77)90066-7 doi: 10.1016/0370-1573(77)90066-7
    [3] V. S. Varadarajan, Supersymmetry for Mathematicians: An Introduction, American Mathematical Society, Rhode Island, 2004
    [4] V. G. Kac, Lie Superalgebras, Adv. Math., 26 (1977), 8–96. https://doi.org/10.1016/0001-8708(77)90017-2 doi: 10.1016/0001-8708(77)90017-2
    [5] Y. Wang, Y. Zhang, The associative forms of the graded Lie superalgebras, Adv. Math., 29 (2000), 65–70.
    [6] J. Yuan, W. Liu, W. Bai, Associative forms and second cohomologies of Lie superalgebras HO and KO, J. Lie Theory, 23 (2009), 203–215.
    [7] Q. Mu, Y. Zhang, Infinite-dimensional Hamiltonian Lie superalgebras, Sci. China Math., 53 (2010), 1625–1634. https://doi.org/10.1007/s11425-010-3142-4 doi: 10.1007/s11425-010-3142-4
    [8] K. Zheng, Y. Zhang, The natural filtration of finite dimensional modular Lie superalgebras of special type, Abstr. Appl. Anal., 2013 (2013), 891241. https://doi.org/10.1155/2013/891241 doi: 10.1155/2013/891241
    [9] K. Zheng, Y. Zhang, W. Song, The natural filtrations of finite-dimensional modular Lie superalgebras of Witt and Hamiltonian type, Pac. J. Math., 269 (2014), 199–218. https://doi.org/10.2140/pjm.2014.269.199 doi: 10.2140/pjm.2014.269.199
    [10] J. Yuan, W. Liu, Filtration, automorphisms, and classification of infinite-dimensional odd contact superalgebras, Front. Math. China, 8 (2013), 203–216. https://doi.org/10.1007/s11464-012-0185-6 doi: 10.1007/s11464-012-0185-6
    [11] W. Liu, Y. Zhang, Automorphism groups of restricted cartan-type Lie superalgebras, Commun. Algebr., 34 (2006), 3767–37842. https://doi.org/10.1080/00927870600862615 doi: 10.1080/00927870600862615
    [12] W. Xie, Y. Zhang, Second cohomology of the modular Lie superalgebra of cartan type k, Algebr. Colloq., 16 (2009), 309–324. https://doi.org/10.1142/S1005386709000303 doi: 10.1142/S1005386709000303
    [13] S. Bouarroudj, P. Grozman, A. Lebedev, D. Leites, Divided power (co)homology. Presentations of simple finite dimensional modular Lie superalgebras with Cartan matrix, Homol. Homotopy Appl., 12 (2010), 237–278. https://doi.org/10.4310/HHA.2010.v12.n1.a13 doi: 10.4310/HHA.2010.v12.n1.a13
    [14] F. Ma, Q. Zhang, The derivation algebra of modular Lie superalgebra k-type, J. Math., 20 (2000), 431–435. https://doi.org/10.13548/j.sxzz.2000.04.015 doi: 10.13548/j.sxzz.2000.04.015
    [15] Q. Zhang, Y. Zhang, Derivation algebras of modular Lie superalgebras W and S of Cartan type, Acta Math. Sci., 20 (2000), 137–144. https://doi.org/10.1016/s0252-9602(17)30743-9 doi: 10.1016/s0252-9602(17)30743-9
    [16] W. Liu, Y. Zhang, X. Wang, The derivation algebra of the Cartan-type Lie superalgebra HO, J. Algebr., 273 (2004), 176–205. https://doi.org/10.1016/j.jalgebra.2003.10.019 doi: 10.1016/j.jalgebra.2003.10.019
    [17] J. Fu, Q. Zhang, C. Jiang, The Cartan-type modular Lie superalgebra KO, Commun. Algebr., 34 (2006), 107–128. https://doi.org/10.1080/00927870500346065 doi: 10.1080/00927870500346065
    [18] W. Bai, W. Liu, Superderivations for modular graded lie superalgebras of cartan-type, Algebr. Represent. Theor., 17 (2014), 69–86. https://doi.org/10.1007/s10468-012-9387-6 doi: 10.1007/s10468-012-9387-6
    [19] S. Awuti, Y. Zhang, Modular Lie superalgebra ¯W(n,m), Northeast Norm. Univ. (Nat. Sci. Ed.), 40 (2008), 7–11.
    [20] L. Ren, Q. Mu, Y. Zhang, A class of finite-dimensional Lie superalgebras of hamiltonian type, Algebr. Colloq., 18 (2011), 347–360. https://doi.org/10.1142/S1005386711000241 doi: 10.1142/S1005386711000241
    [21] K. Zheng, Y. Zhang, J. Zhang, A class of finite dimensional modular Lie superalgebras of special type, Bull. Malays. Math. Sci. Soc., 39 (2016), 381–390. https://doi.org/10.1007/s40840-015-0177-2 doi: 10.1007/s40840-015-0177-2
    [22] D. Mao, K. Zheng, Constructions and properties for a finite-dimensional modular Lie superalgebra K(n,m), J. Math., 2021 (2021), 7069556. https://doi.org/10.1155/2021/7069556 doi: 10.1155/2021/7069556
    [23] Y. Zhang, Finite-dimensional Lie superalgebras of Cartan type over fields of prime characteristic, Chin. Sci. Bull., 42 (1997), 720–724. https://doi.org/10.1007/BF03186962 doi: 10.1007/BF03186962
    [24] Y. Zhang, W. Liu, Modular Lie Superalgebras, Science Press, Beijing, 2004.
  • Reader Comments
  • © 2023 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(1300) PDF downloads(41) Cited by(0)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog