Startseite Mathematik Irreducible modules with highest weight vectors over modular Witt and special Lie superalgebras
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Irreducible modules with highest weight vectors over modular Witt and special Lie superalgebras

  • Keli Zheng EMAIL logo und Yongzheng Zhang
Veröffentlicht/Copyright: 19. November 2019

Abstract

Let 𝔽 be an arbitrary field of characteristic p > 2. In this paper we study irreducible modules with highest weight vectors over Witt and special Lie superalgebras of 𝔽. The same irreducible modules of general and special linear Lie superalgebras, which are the 0-th part of Witt and special Lie superalgebras in certain ℤ-grading, are also considered. Then we establish a certain connection called a P-expansion between these modules.

MSC 2010: 17B10; 17B50; 17B70

1 Introduction

Let 𝔽 be an arbitrary field of characteristic p > 2 and ℤ2 = {0̄, 1̄} be the residue class ring mod 2. Throughout this paper we have assumed that all vector spaces, linear mappings and tensor products are over the underlying base field 𝔽. Assume that x is a ℤ2-homogeneous element and d(x) is the ℤ2-degree of x, if d(x) occurs in an expression.

In 1967, Rudakov and Shafarevich [1] described all the irreducible representations of 𝔰𝔩(2) over an algebraically closed field 𝔽 of characteristic p > 2. They demonstrated that in addition to the p-representations known since 1930s, all of which possess a highest and lowest weight and are labeled by one integer, there are other representations that form a variety of dimension 3. They described the 𝔤-modules not possessing a p-structure for Lie algebras 𝔤 with Cartan matrix. In 1974, Rudakov [2] described irreducible 𝔤-modules, where 𝔤 is a simple Lie algebras of vector fields over ℂ, for modules dual to modules of (formal) tensor fields. For a review of similar results and the importance of this particular type of module, we refer the readers to the papers [3, 4]. In the 1980s, Krylyuk [5, 6] studied the highest weight modules over the algebras of vector fields of series W and S possessing a p-structure. Shu [7] discussed the representations of Cartan type Lie algebras in characteristic p > 2 from the viewpoint of reducing rank. Zhang [8] constructed the simple L-modules with nonsingular characters and some simple modules with singular characters, where L is a restricted simple Lie algebra of Cartan type.

Since the classification of all the finite-dimensional simple complex Lie superalgebras was done by Kac [9], the problems of constructing a unified representation theory for all the types of simple Lie superalgebras has become more important than ever. Kac obtained essential results for the highest weight representations of classical Lie superalgebras [10, 11]. Most of Kac’s results can also be extended to the remaining classical series of Lie superalgebras [12, 13, 14], while the representations of Lie superalgebras of Cartan type have been studied in [15, 16]. Recent work on the representation theory of modular Lie superalgebras of Cartan type can also be found in [17, 18, 19].

The structure of gradation plays a critical role in the research of Lie algebras and superalgebras. Shen [20, 21, 22] introduced an important notion which is called the mixed product and realized the graded modules over Lie algebras of Cartan type. The method of the mixed product can also be applied to Lie superalgebras of Cartan type over fields of characteristic zero [23]. In the case of modular Lie superalgebras, Zhang [24] has obtained the ℤ-graded modules over finite-dimensional Hamiltonian Lie superalgebras.

This paper generalizes some of Shen’s results in [20, 21, 22]. A brief summary of the relevant concepts in generalized Witt and special modular Lie superalgebras is presented in Section 2. Section 3 gives some properties of the graded modules over modular Lie superalgebras. In Section 4, the certain connection which is called a P-expansion between irreducible highest weight representations of generalized Witt and special modular Lie superalgebras, and the same irreducible highest weight representations of general linear Lie superalgebras 𝔤𝔩(m, n) and special linear Lie superalgebras 𝔰𝔩(m, n), is established.

2 Generalized Witt and special modular Lie superalgebras

In addition to the standard notation ℤ, ℕ and ℕ0 is used for the set of positive integers and the set of nonnegative integers, respectively. Generally, let m, n denote fixed integers in ℕ ∖ {1, 2}. For α = (α1, …, αm) ∈ N0m , we put |α| := i=1m αi. Following [25], let 𝓞(m) denote the divided power algebra over 𝔽 with an 𝔽-basis {x(α) | α N0m }. For εi := (δi1, …, δim), we abbreviate {x(εi)} to xi, i = 1, 2, …, m, where δij is Kronecker delta. Let Λ(n) be the exterior superalgebra over 𝔽 in n variables xm+1, xm+2, …, xm+n and 𝓞(m, n) denote the tensor product 𝓞(m) ⊗𝔽 Λ(n) . Clearly, 𝓞(m, n) is an associative superalgebra with a ℤ2-gradation induced by the trivial ℤ2-gradation of 𝓞(m) and the natural ℤ2-gradation of Λ(n). Moreover, 𝓞(m, n) is super-commutative. For g ∈ 𝓞(m), fΛ(n), we write gf for gf. The following formulae hold in 𝓞(m, n):

x(α)x(β)=α+βαx(α+β) for α,βN0m,xixj=xjxi for i,j=m+1,,m+n,x(α)xj=xjx(α) for αN0m,j=m+1,,m+n,

where α+βα:=i=1mαi+βiαi. Put Y0 := {1, 2, …, m}, Y1 := {m + 1, m + 2, …, m + n} and Y := Y0 ∪ Y1. Set

Bk:=i1,i2,,ikm+1i1<i2<<ikm+n

and B:=k=0nBk, where 𝔹0 := ∅. For u = 〈i1, i2, …, ik〉 ∈ 𝔹k, set |u| := k, |∅| := 0, x := 1, xu := xi1 xi2xik and xE := xm+1 xm+2xm+n. Clearly, {x(α)xu | α N0m , u ∈ 𝔹} constitutes an 𝔽-basis of 𝓞(m, n). Let D1, D2, …, Dm+n be the linear transformations of 𝓞(m, n) such that

Dr(x(α)xu)=x(αεr)xu,rY0,x(α)(xu)/xr,rY1,

where / xr is the superderivation of Λ(n) such that xs/ xr = δrs for r, s ∈ Y1. For more details on superderivations for Lie superalgebras, the reader is referred to [9, 26]. D1, D2, …, Dm+n are superderivations of the superalgebra 𝓞(m, n). Let

W(m,n):={rYfrDr|frO(m,n)}.

Then W(m, n) is a Lie superalgebra, which is contained in Der(𝓞(m, n)), where Der(𝓞(m, n)) denotes the superderivation space of 𝓞(m, n). Obviously, d(Di) = τ(i), where

τ(i):=0¯,iY0,1¯,iY1.

An easy verification shows that

[fD,gE]=fD(g)E(1)d(fD)d(gE)gE(f)D+(1)d(D)d(g)fg[D,E]

for f, g ∈ 𝓞(m, n), D, E ∈ Der(𝓞(m, n)). In particular, the following formula holds in W(m, n):

[fDr,gDs]=fDr(g)Ds(1)d(fDr)d(gDs)gDs(f)Dr

for f, g ∈ 𝓞(m, n), r, s ∈ Y.

Let

t:=(t1,t2,,tm)Nm,π:=(π1,π2,,πm),

where πi := pti − 1, i ∈ Y0. Let 𝔸 := {α N0m | αiπi, i = 1, 2, …, m}. Then

O(m,n,t):=spanFx(α)xuαA,uB

is a finite-dimensional subalgebra of 𝓞(m, n) with a natural ℤ-gradation 𝓞(m, n, t) = r=1ξ 𝓞(m, n, t)r by putting

O(m,n,t)r:=spanFx(α)xu|α|+|u|=r,ξ:=|π|+n.

Set

W(m,n,t):={rYfrDr|frO(m,n,t)}.

Then W(m, n, t) is called the generalized Witt modular Lie superalgebra and it is a subalgebra of W(m, n). In particular, it is a finite-dimensional simple Lie superalgebra (see [27]). Clearly, W(m, n, t) is a free 𝓞(m, n, t)-module with basis {Dr | r ∈ Y}. Note that W(m, n, t) possesses a standard 𝔽-basis {x(α) xu Dr | α ∈ 𝔸, u ∈ 𝔹, r ∈ Y}.

Let r, s ∈ Y and Drs : 𝓞(m, n, t) → W(m, n, t) be a linear mapping such that

Drs(f)=(1)τ(r)τ(s)Dr(f)Ds(1)(τ(r)+τ(s))d(f)Ds(f)Dr, (1)

where f ∈ 𝓞(m, n, t) and r, s ∈ Y. Then the following equation holds:

[Dk,Drs(f)]=(1)τ(k)τ(r)Drs(Dk(f)),fO(m,n,t);k,r,sY.

Put

S(m,n,t):=spanFDrs(f)fO(m,n,t);r,sY.

Then S(m, n, t) is called the special modular Lie superalgebra. S(m, n, t) is also a finite-dimensional simple Lie superalgebra (see [27]).

Let div : W(m, n, t) → 𝓞(m, n, t) be the divergence such that

divrYfrDr=rY(1)τ(r)d(fr)Dr(fr).

It follows that

div[D,E]=Ddiv(E)(1)d(D)d(E)Ediv(D) for any D,EW(m,n,t).

Then div is a superderivation from W(m, n, t) to 𝓞(m, n, t). Following [1], put

S¯(m,n,t):=DW(m,n,t)div(D)=0.

Then S(m, n, t) is contained in S(m, n, t) and S(m, n, t) is a subalgebra of W(m, n, t). The ℤ-gradation of 𝓞(m, n, t) induces naturally ℤ-gradation structures of W(m, n, t) = i=1ξ1 W(m, n, t)i and S(m, n, t) = i=1ξ2 S(m, n, t)i, where

W(m,n,t)i:=spanFfDrrY,fO(m,n,t)i+1,S(m,n,t)i:=spanFDrs(f)r,sY,fO(m,n,t)i+2.

In addition, S(m, n, t) is also a ℤ-graded subalgebra of W(m, n, t). For convenience, W(m, n, t), S(m, n, t), S(m, n, t) and 𝓞(m, n, t) will be denoted by W, S, S and 𝓞, respectively.

3 Graded modules over modular Lie superalgebras

Let 𝔤𝔩(m, n) = 𝔤𝔩(m, n) ⊕ 𝔤𝔩(m, n) be the general linear Lie superalgebra of all s × s matrices over 𝔽 (see [9]), where s = m + n. Set 𝔤𝔩(m, n, t) = 𝓞 ⊗ 𝔤𝔩(m, n). Define the operation [ , ] in 𝔤𝔩(m, n, t) as follows:

[ax,by]=(1)d(x)d(b)ab[x,y], (2)

where a, b ∈ 𝓞, x, y ∈ 𝔤𝔩(m, n). Then 𝔤𝔩(m, n, t) is a Lie superalgebra. For AW, define A ⊗ 1 ∈ End(𝔤𝔩(m, n, t)) by

(A1)(ax)=A(a)x,aO,xgl(m,n). (3)

Let P ∈ 𝔤𝔩(m, n) be an s × s invertible matrix. Suppose that A = i=1s ai DiWα, where α ∈ ℤ2. Let

A~=k,j=1s(1)τ(k)τ(j)+τ(j)+τ(k)α(Dkaj)P1EkjP, (4)

where Ekj is an s × s matrix whose (i, l)-entry is δkiδjl. Then 𝔤𝔩(m, n, t)α. By virtue of the definition of superderivation we have

Dk(ab)=(Dka)b+(1)τ(k)d(a)a(Dkb), (5)

where a, b ∈ 𝓞, k = 1, …, s.

Let A = i=1s ai DiWα and B = i=1s bj DjWβ, where α, β ∈ ℤ2. Then

[A,B]=j=1sqjDj, where qj=i=1s(ai(Dibj)(1)αβ(bi(Diaj)). (6)

Using the formulae from (2) to (6), a direct calculation shows the following proposition.

Proposition 3.1

([24], Formula (7)). Suppose that AWα and BWβ, where α, β ∈ ℤ2. If C = [A, B], then

C~=[A~,B~]+(A1)(B~)(1)αβ(B1)(A~). (7)

Suppose that L is a subalgebra of 𝔤𝔩(m, n) and L(P) = {P–1 AP | AL}. Then L(P) is a subalgebra of 𝔤𝔩(m, n). Let Ω = ΩΩ, where

Ωα={AWαA~OL(P)},αZ2.

If A, BΩ, then [, ] ∈ Ω. The formula (7) shows that Ω is a subalgebra of modular Witt Lie superalgebras W. The subalgebra Ω is called the P-expansion of L into W. Then the P-expansion of 𝔤𝔩(m, n) into W is exactly W.

The special linear Lie superalgebra 𝔰𝔩(m, n) = {A ∈ 𝔤𝔩(m, n) | str(A) = 0} is a subalgebra of 𝔤𝔩(m, n) (see [9]). Let Ω is the P-expansion of 𝔰𝔩(m, n) into W. If A = i=1s ai DiW, then, for α ∈ ℤ2,

AΩαA~(Osl(m,n))αk=1mj=1s(1)τ(j)(Dkaj)Ekj(1)αk=m+1sj=1s(Dkaj)Ekj(Osl(m,n))αk=1m(Dkak)Ekk(1)αk=m+1s(Dkak)Ekk(Osl(m,n))α(k=1s(1)τ(k)d(ak)(Dkak))E11(Osl(m,n))αk=1s(1)τ(k)d(ak)(Dkak)=0 and DkakOαAS¯α.

Hence Ωα = Sα. It follows that Ω = S.

Let ρ be a representation of L(P) on ℤ2-graded space V. Then ρ can be expanded to a representation ρ1 of 𝓞 ⊗ L(P) on the space 𝓞 ⊗ V, defined by

ρ1(ax)(bv)=(1)d(x)d(b)abρ(x)(v), (8)

where a, b ∈ 𝓞, xL(P), vV.

Proposition 3.2

([24], Proposition 2). Let Ω be the P-expansion of L into W. Then

ρ~(A)=ρ1(A)+A1,AΩ (9)

defines a representation ρ͠ of Ω on2-graded space 𝓞 ⊗ V.

By Proposition 3.2, 𝓞 ⊗ V which will be denoted by is a Ω-module. In [20] the module is called the mixed product of 𝓞 and the module V.

A ℤ-graded module V of X is called positively graded if V = i0 Vi and LjViVi+j, where X is a ℤ-graded Lie superalgebra.

Let i = 〈av | a ∈ 𝓞i, vV〉. Then = i=0ξ i, where ξ = i=1m πi + n. Put i = 0 for i > ξ. A direct verification shows that Ωiji+j. Hence is a positively graded Ω-module. Since the P-expansion of 𝔤𝔩(m, n) and 𝔰𝔩(m, n)) into W are, respectively, W and S, Proposition 3.2 shows the following corollary.

Corollary 3.3

The following statements hold:

  1. If V is a 𝔤𝔩(m, n)-module, then the mixed product is a ℤ-graded W-module.

  2. If V is an 𝔰𝔩(m, n)-module, then the mixed product is a ℤ-graded S-module and so is a ℤ-graded S-module.

If V is an irreducible L(P)-module with a highest weight λ, then denote by (λ). Furthermore, the weight vector associated with the highest weight λ is denoted by vλ, where vλ(λ). Similar to [21, Theorem 1.2] one may obtain that (λ) has an unique irreducible submodule U(L)(1 ⊗ V), where U(L) is the universal enveloping algebra of L. We customarily denote the unique irreducible submodule by V. Then x(α) xuvλV for all α = (α1, …, αm) ∈ 𝔸, u = (i1, …, ir) ∈ 𝔹.

Suppose that π = (π1, …, πm), E = (m + 1, …, s), then π ∈ 𝔸, E ∈ 𝔹. Since Lie superalgebra W0 is isomorphic to 𝔤𝔩(m, n), the element i,j=1s aij Eij of L(P) can be identified as the element i,j=1s aijxiDj of W, where aij ∈ 𝔽. Hence x(π) xEV can be regarded as an L(P)-module. Similarly, by [21, Proposition 2.4], we can prove that V is an irreducible L(P)-module if and only if x(π) xEV is an irreducible L(P)-module. The following proposition is the analogue of [21, Proposition 2.1].

Proposition 3.4

Suppose that V is an irreducible L(P)-module, vλ is the weight vector associated with the highest weight λ and V is the unique irreducible submodule of (λ), where L = 𝔤𝔩(m, n) or 𝔰𝔩(m, n), then

  1. V contains 1 ⊗ V as a submodule.

  2. If x(π) xEvλV, then V = (λ), that is (λ) is an irreducible Ω-module, where Ω is the P-expansion of L(P) into W.

Proof

Recall that Ω = W if L = 𝔤𝔩(m, n) and Ω = S if L = 𝔰𝔩(m, n).

  1. Without loss of generality we suppose that x(α) xuvλV, then

    1vλ=D1α1DmαmDi1Dir(x(α)xuvλ)V¯.

    Because V is an irreducible L(P)-module, 1 ⊗ V is an irreducible Ω0-module. Then 1 ⊗ V = U(Ω0)(1 ⊗ vλ) ⊆ V, where U(Ω0) is the universal enveloping algebra of Ω0.

  2. Since module V is non-trivial, (λ)ξ is non-trivial. Let x(π) xEV′ be a proper Ω0-submodule of (λ)ξ = x(π) xEV. Then 1 ⊗ V′ is a proper Ω0-submodule of 1 ⊗ V. Hence V′ is a proper L(P)-submodule of V, which contradicts that V is irreducible. Since (λ)ξ is an irreducible Ω0-module, we have

    U(Ω0)(x(π)xEvλ)=x(π)xEVV¯.

    Let α ∈ 𝔸, u ∈ 𝔹. Assuming that (β1, …, βm) = π-α and w = (j1, …, jk) ∈ 𝔹 such that {w} = {E} ∖ {u}, then

    x(α)xuvλ=D1β1DmβmDj1Djk(x(π)xEvλ)V¯.

    Hence V = (λ). □

4 Irreducibility of module (λ) over W and S

Let V be an irreducible 𝔰𝔩(m, n)-module with the highest weight λ. Proposition 3.2 shows that (λ) is an S-module. Clearly, it is also an S-module. Assuming that V is irreducible as an S-module and if x(π) xEvλV, then it follows that V = (λ) from the similar methods used in Proposition 3.4 (ii). Therefore, (λ) is an irreducible S-module.

We know that the standard Cartan subalgebra H of S is 〈hi | i = 1, 2, …, s – 1〉, where

hi=Eii(1)τ(i)+τ(i+1)Ei+1i+1,i=1,2,,s1.

Let Λi be the linear function on 〈E11, …, Ess〉 such that Λi(Ejj) = δij, where i, j = 1, 2, …, s. Set

λi=j=1iΛj,i=1,2,,m1,λm=j=m+1sΛj,λi=j=1mΛj+j=m+1iΛj,i=m+1,,s.

Then λi, i = 1, 2, …, s – 1, is a fundamental weight of 𝔰𝔩(m, n) and λi(hj) = δij. We know that ΛiΛj is a positive root of 𝔰𝔩(m, n) and the corresponding vectors of the positive root are Eij, where 1 ≤ i < js.

If V is a finite-dimensional irreducible 𝔰𝔩(m, n)-module, then λ = i=1s1 ciλi, where ci ∈ 𝔽. Let λ|m = i=1m1 ciλi and λ|+m = i=m+1s1 ciλi. Then λ = λ|m + cm λm + λ|+m. Also, assuming that ρ and ρ͠ are representations corresponding with the modules V and (λ), respectively.

Lemma 4.1

Assuming that λ|m ≠ 0. If λλi, i = 1, 2, …, m – 1, then (λ) is an irreducible S-module.

Proof

Since λ|m ≠ 0 and λλi, i = 1, 2, …, m – 1, it was observed that λ must be one of the two cases: (1) λ|m = λi and cmλm + λ|+m ≠ 0, (2) λ|mλi, i = 1, 2, …, m – 1.

  1. If λ|m = λi and cmλm + λ|+m ≠ 0, where 1 ≤ im – 1, then ci ≠ 0 for mis – 1. Let ck be the first non-zero element of {cm, cm+1, …, cs−1}. If k > m, then by virtue of formulae (1), (2), (8) and (9) and

    ρ(EiiEk+1k+1)vλ=ρ(j=imhjj=m+1khj)vλ=(1ck)vλ,

    where vλ is a weight vector associated with the highest weight λ,

    ρ~(Dik+1(x(π)xE))(1vλ)=ρ~(x(πεi)xEDk+1(1)n+kmx(π)xEk+1Di)(1vλ)=ρ1(j=1mDj(x(πεi)xE)Ejk+1(1)n1j=m+1sDj(x(πεi)xE)Ejk+1)(1vλ)(1)n+kmρ1(j=1mDj(x(π)xEk+1)Eji+(1)n1j=m+1sDj(x(π)xEk+1Eji))(1vλ)=(1)n+kmx(πεi)xEk+1(1ck)vλ+j=k+2s(1)n+jmx(πεi)xEjρ(Ejk+1)vλ(1)n+kmj=i+1mx(πεj)xEk+1ρ(Eji)vλ+j=m+1k(1)k+jx(πεi)xEjk+1ρ(Eji)vλ+j=k+2s(1)j+kx(πεi)xEk+1jρ(Eji)vλ. (10)

    Applying the formulae (8), (9) and (10) and

    ρ(Eii+1Ei+1i)vλ=ρ(EiiEi+1i+1)vλ=vλ,

    we get

    ρ~(Dii+1(x(2εi)xi+1xk+1))ρ~(Dik+1(x(π)xE))(1vλ)=(1)nx(π)xEvλ(1)n(1ck)x(π)xEρ(EiiEi+1i+1)vλ=(1)nckx(π)xEvλ.

    By Proposition 3.4 (i), we know that 1 ⊗ vλV. Since ck ≠ 0, it shows x(π) xEvλV. Hence (λ) is an irreducible S-module.

  2. If λ|mλi, i = 1, 2, …, m – 1, then

    ρ~(Di+1i(x(2εi+2εi+1)))ρ~(Dii+1(x(π)xE))(1vλ)=(ci2+ci)x(π)xEvλ.

    If ci ≠ 0 or 1, then x(π) xEvλV and (λ) is an irreducible S-module. So it was assumed that ck = 0 or 1, where k = 1, 2, …, m – 1. Since λ|m ≠ 0 and λ|mλi, there exist at least two k ∈ {1, 2, …, m – 1} such that ck = 1. Without loss of generality we assumed that ci and cj, i < j, are the first and second coefficients which are equal to 1. Then

    ρ~(Dij+1(x(2εi+2εj+1)))ρ~(Dij+1(x(π)xE))(1vλ)=((ci+cj)2+(ci+cj))x(π)xEvλ=2x(π)xEvλ.

    Therefore, x(π) xEvλV and (λ) is an irreducible S-module. □

Lemma 4.2

Suppose that n is odd. If cm ≠ – 1 or 0, then (λ) is an irreducible S-module.

Proof

If cm+1cm + 1, then cm(1 + cmcm+1) ≠ 0. A direct computation shows that

ρ~(Dmm+1(x(2εm)xm+1xm+2))ρ~(Dmm+1(x(π)xE))(1vλ)=cm(1(1)n(cmcm+1))x(π)xEvλ=cm(1+cmcm+1)x(π)xEvλ.

Then x(π) xEvλV and (λ) is an irreducible S-module. If cm+1 = cm + 1, then

ρ~(Dmm+2(x(2εm)xm+1xm+2))ρ~(Dmm+1(x(π)xE))(1vλ)=((cmcm+1)(1)ncm+1+(1)ncm(cmcm+1))x(π)xEvλ=(2+2cm)x(π)xEvλ.

Since cm ≠ –1, we have 2 + 2cm ≠ 0. Therefore, x(π) xEvλV and (λ) is irreducible.□

Lemma 4.3

Suppose that n is odd and cm ≠ 0. If λ ≠ –λm, then (λ) is an irreducible S-module.

Proof

If cm ≠ –1, then Lemma 4.2 shows that (λ) is irreducible. If cm = –1 and λ|m ≠ 0, then Lemma 4.1 shows that (λ) is irreducible. Suppose that cm = –1, λ|m = 0 and λ|+m ≠ 0. Let ck be the first non-zero element of {cm+1, cm+2, …, cs−1}. Then

ρ~(Dmk(x(2εm)xkxk+1))ρ~(Dmk+1(x(π)xE))(1vλ)=(cm(1)n(cmck)cm)x(π)xEvλ=ckx(π)xEvλ.

Hence x(π) xEvλV. Consequently, the module (λ) is an irreducible S-module.□

Lemma 4.4

Suppose that λ|m = 0, cm ≠ 0 and λ|+m ≠ 0. If (λ) is a reducible S-module, then there exists k ∈ {m + 1, m + 2, …, s – 2} such that λ = ckλk – (ck + 1)λk+1.

Proof

Since λ|+m ≠ 0, the elements cm+1, …, cs−1 of 𝔽 are not all zero. So we may suppose that ck is the first non-zero element of {cm+1, cm+2, …, cs−1}. Assuming that there exists a ck+i ≠ 0, where i > 1. A direct computation shows that

ρ~(Dk+ik+i+1(xkxk+1xk+ixk+i+1))ρ~(Dkk+1(x(π)xE))(1vλ)=(1)nckck+ix(π)xEvλ.

As ckck+i ≠ 0, we have x(π) xEvλV. But this conclusion confutes that (λ) is a reducible S-module. As ck+i = 0, i > 1 and λ = ckλk + ck+1 λk+1. Then

ρ~(Dk1k+2(xk1xkxk+1xk+2))ρ~(Dkk+1(x(π)xE))(1vλ)=(1)nck(1+ck+ck+1)x(π)xEvλ,m+2ks2;(1)nck(1+ck+ck+1)x(π)xEvλ,k=m+1.

Since (λ) is a reducible S-module, we have 1 + ck + ck+1 = 0. Therefore, ck+1 = –(ck + 1) and λ = ckλk – (ck + 1)λk+1.□

Theorem 4.5

Let V be a finite-dimensional irreducible 𝔰𝔩(m, n)-module with a non-zero highest weight λ. Suppose that n is odd. If λ ≠ –λm or (–1)τ(i) λi, i = 1, …, m – 1, m + 2, …, s – 1, then (λ) is an irreducible S-module.

Proof

Assume that (λ) is a reducible S-module. It suffices to prove λ = –λm or (–1)τ(i) λi, where i = 1, …, m – 1, m + 2, …, s – 1.

If λ|m ≠ 0, by Lemma 4.1, then λ = λi = (–1)τ(i) λi, where i ∈ {1, …, m – 1}.

Suppose that λ|m = 0. If cm ≠ 0, by Lemma 4.3, then λ = –λm.

Suppose that λ|m = 0 and cm = 0. Then λ|m ≠ 0. Lemma 4.4 shows that λ = ciλi – (ci + 1)λi+1, where i ∈ {m + 1, …, s – 2}. A direct computation shows that

ρ~(Dmi+1(x(2εm)xi+1xi+2))ρ~(Dmi+2(x(π)xE))(1vλ)=2cix(π)xEvλ.

Since (λ) is a reducible S-module, we have x(π) xEvλV. Therefore, ci = 0 and λ = –λi+1 = (–1)τ(i+1) λi+1, where i ∈ {m + 1, …, s – 2}, that is λ = (–1)τ(i) λi, where i ∈ {m + 1, …, s – 2}. The proof is completed.□

The W-module (λ) will be discussed in the following theorem.

Theorem 4.6

Let V be a finite-dimensional irreducible 𝔤𝔩(m, n)-module with the non-zero highest weight λ. Suppose that n is odd. If λ ≠ –λm, (–1)τ(i) λi, i = 1, …, m – 1, m + 2, …, s – 1, then (λ) is an irreducible W-module.

Proof

We may suppose that λ = j=1s cj λj, where cj ∈ 𝔽, and ρ is the representation corresponding to the module V. Assume that (λ) is a reducible W-module. It suffices to prove λ = –λm or (–1)τ(i) λi, where i = 1, …, m – 1, m + 2, …, s – 1. Clearly, (λ) is also a reducible S-module. By Theorem 4.5, we know that λ|H, the restriction of λ to the Cartan subalgebra H of 𝔰𝔩(m, n), is equal to –λm or (–1)τ(i) λi, where i = 1, …, m – 1, m + 2, …, s – 1.

If λ|H = –λm, then λ|H(hi) = –λm(hi), i = 1, …, s – 1. Hence

λ=cj=1mΛj+(1+c)j=m+1sΛj,

where c ∈ 𝔽. A direct computation shows that

ρ~(x(2ε1)D1)ρ~(x(π)xED1)(1vλ)=(cc2)x(π)xEvλ.

Since (λ) is reducible, we have cc2 = 0. It follows c = 0 or 1. By virtue of

ρ~(x(2ε1)D1)ρ~(x(π)xEDm+1)(1vλ)=(1)n1(1+c)cx(π)xEvλ

and (λ) is reducible, we have (1 + c)c = 0. Then c = 0 and λ = j=m+1s Λj = –λm.

If λ|H = (–1)τ(i) λi, where i = 1, …, m – 1, then λ|H = λi. Since λ(hj) = λi(hj), j = 1, 2, …, s – 1, we have

λ=cj=1iΛj+(c1)j=i+1mΛj+(c1)j=m+1sΛj,

where c ∈ 𝔽. It follows that c = 0 or 1 from

ρ~(x(2ε1)D1)ρ~(x(π)xEDm)(1vλ)=(cc2)x(π)xEvλ

and (λ) is reducible. But the equation

ρ~(x(2εm)Dm)ρ~(x(π)xEDm)(1vλ)=((c1)2+(c1))x(π)xEvλ,

shows that c ≠ 0. Hence c = 1 and λ = λi = (–1)τ(i) λi, where i = 1, …, m – 1.

If λ|H = (–1)τ(i) λi, where i = m + 2, …, s – 1, then λ|H = –λi. Since λ(hj) = –λi(hj), j = 1, 2, …, s – 1, we have

λ=cj=1mΛjcj=m+1iΛj+(1c)j=i+1sΛj,

where c ∈ 𝔽. It follows that c = 0 or 1 from

ρ~(x(2ε1)D1)ρ~(x(π)xED1)(1vλ)=(cc2)x(π)xEvλ

and (λ) is reducible. Furthermore, the equation

ρ~(x1xj+1D1)ρ~(x(π)xEDj+1)(1vλ)=(1)n(1c)2x(π)xEvλ,

shows that c = 1. Hence

λ=j=1mΛjj=m+1iΛj=λi=(1)τ(i)λi,

where i = m + 2, …, s – 1.

In conclusion, the proof is completed.□

Acknowledgement

This work was supported by the Fundamental Research Funds for the Central Universities (No.2572018BC15) and the National Natural Science Foundation of China (No.11171055).

References

[1] Rudakov A., Shafarevich I., Irreducible representations of a simple three-dimensional Lie algebra over a field of finite characteristic, Math. Notes., 1967, 2(5), 760–767.10.1007/BF01093935Suche in Google Scholar

[2] Rudakov A., Irreducible representations of infinite-dimensional Lie algebras of Cartan type, Math. USSR Izv., 1974, 8(4), 836–866.10.1070/IM1974v008n04ABEH002129Suche in Google Scholar

[3] Grozman P., Leites D., Shchepochkina I., Invariant operators on supermanifolds and standard models, Multiple facets of quantization and supersymmetry, 2002, 508–555.10.1142/9789812777065_0031Suche in Google Scholar

[4] Olshanetsky M., Lie algebroids as gauge symmetries in topological field theories, Multiple facets of quantization and supersymmetry, 2002, 205–232.10.1142/9789812777065_0020Suche in Google Scholar

[5] Krylyuk Ya., Maximum dimension of irreducible representations of simple Lie p-algebras of Cartan series S and H, Mat. Sb. (N.S.), 1984, 123(165)(1), 108-119 (Russian)Suche in Google Scholar

[6] Krylyuk Ya., On the index of algebras of Cartan type in finite characteristic, Math. USSR. Izv., 1987, 28, 381–399.10.1070/IM1987v028n02ABEH000888Suche in Google Scholar

[7] Shu B., Representations of Cartan type Lie algebras in characteristic p, J. Algebra, 2002, 256(1), 7–27.10.1016/S0021-8693(02)00035-2Suche in Google Scholar

[8] Zhang C., Representations of the restricted Lie algebras of Cartan type, J. Algebra, 2005, 290(2), 408–432.10.1016/j.jalgebra.2005.04.012Suche in Google Scholar

[9] Kac V., Lie superalgebras, Adv. Math., 1977, 26, 8–96.10.1016/0001-8708(77)90017-2Suche in Google Scholar

[10] Kac V., Characters of typical representations of classical Lie superalgebras, Comm. Algebra, 1977, 5(8), 889–897.10.1080/00927877708822201Suche in Google Scholar

[11] Kac V., Representations of classical Lie superalgebras, Lect. Notes Math., Springer, Berlin, 1978, 676, 597–626.10.1007/BFb0063691Suche in Google Scholar

[12] Serganova V., Kazhdan-Lusztig polynomials for Lie superalgebra gl(m|n), Adv. Soviet Math., 1993, 16(2), 151–165.10.1090/advsov/016.2/05Suche in Google Scholar

[13] Su Y., Some results on finite dimensional representations of general linear Lie superalgebras, Adv. Lect. Math., 2008, 6, 374–439.Suche in Google Scholar

[14] Van der Jeugt J., Hughes J., King R., Thierry-Mieg J., Character formulas for irreducible modules of the Lie superalgebras sl(m/n), J. Math. Phys., 1990, 31(9), 2278–2304.10.1063/1.528637Suche in Google Scholar

[15] Bernstein J., Leites D., Irreducible representations of finite-dimensional Lie superalgebras of series W and S, C. R. Acad. Bulgare Sci., 1979, 32(3), 277–278.Suche in Google Scholar

[16] Shapovalov A., Finite-dimensional irreducible representations of Hamiltonian Lie superalgebras, Mat.Sb.(N.S.), 1978, 107(149)(2), 259–274. (Russian)Suche in Google Scholar

[17] Shu B., Yao Y., Character formulas for restricted simple modules of the special superalgebras, Math. Nachr., 2012, 285(8-9), 1107–1116.10.1002/mana.201000064Suche in Google Scholar

[18] Shu B., Zhang C., Restricted representations of the Witt superalgebras, J. Algebra, 2010, 324(4), 652–672.10.1016/j.jalgebra.2010.04.032Suche in Google Scholar

[19] Yao Y., Shu B., Restricted representations of Lie superalgebras of Hamiltonian type, Algebr. Represent. Theory, 2013, 16(3), 615–632.10.1007/s10468-011-9322-2Suche in Google Scholar

[20] Shen G., Graded modules of graded Lie algebras of Cartan type I: Mixed products of modules, Sci. Sinica Ser. A., 1986, 29(6), 570–581.Suche in Google Scholar

[21] Shen G., Graded modules of graded Lie algebras of Cartan type II: Positive and negative graded modules, Sci. Sinica Ser. A., 1986, 29(10), 1009–1019.Suche in Google Scholar

[22] Shen G., Graded modules of graded Lie algebras of Cartan type III: Irreducible modules, Chin. Ann. Math. Ser. B., 1988, 9(4), 404–417.Suche in Google Scholar

[23] Zhang Y., ℤ-graded module of Lie superalgebra H(n) of Cartan type, Chin. Sci. Bull., 1996, 41(10), 813–817.Suche in Google Scholar

[24] Zhang Y., Fu H., Finite-dimensional Hamiltonian Lie superalgebra, Comm. Algebra, 2002, 30(6), 2651–2673.10.1081/AGB-120003981Suche in Google Scholar

[25] Strade H., Simple Lie algebras over fields of positive characteristic, I, Structure Theory, Walter de Gruyter, Berlin, New York, 2004.10.1515/9783110197945Suche in Google Scholar

[26] Scheunert M., Theory of Lie superalgebras, Springer-Verlay, Berlin, Heidelberg and New York, 1979.10.1007/BFb0070929Suche in Google Scholar

[27] Zhang Y., Finite-dimensonal Lie superalgebras of Cartan-type over fields of prime characteristic, Chin. Sci. Bull., 1997, 42, 720–724.10.1007/BF03186962Suche in Google Scholar

Received: 2019-01-15
Accepted: 2019-10-15
Published Online: 2019-11-19

© 2019 Keli Zheng and Yongzheng Zhang, published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 Public License.

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