160
Views
0
CrossRef citations to date
0
Altmetric
Research Article

Generalized derivations of current Lie algebras

&
Received 16 Feb 2023, Accepted 03 May 2024, Published online: 10 Jun 2024

Abstract

Let L be a Lie algebra and let A be an associative commutative algebra with unity, both over the same field F. We consider the following question. Is every generalized derivation (resp. quasiderivation) of LA the sum of a derivation and a map from the centroid of LA, if the same holds true for L?

2020 Mathematics Subject Classification:

1 Introduction

Let L be a Lie algebra over a field F. A linear map d:LL is called a derivation if d([x,y])=[d(x),y]+[x,d(y)] for all x,yL. As usual, we denote the set of all derivations of L by Der(L). Obviously, Der(L) is a Lie subalgebra of the general linear algebra gl(L). There are several generalizations of the notion of a derivation. In this paper we consider generalized derivations and quasiderivations of Lie algebras as defined by Leger and Luks in [Citation6]. Let f:LL be a linear map. If there exist linear maps g,h:LL such that [f(x),y]+[x,g(y)]=h([x,y]) for all x,yL, then f is called a generalized derivation. In case there exists a linear map h:LL such that [f(x),y]+[x,f(y)]=h([x,y]) for all x,yL, then f is said to be a quasiderivation. By GDer(L) we shall denote the set of all generalized derivations of L and by QDer(L) the set of all quasiderivations of L. Obviously, QDer(L) and GDer(L) are Lie subalgebras of gl(L) such that Der(L)QDer(L)GDer(L)gl(L).

Yet another Lie subalgebra of gl(L) is the centroid of L, which is defined as Cent(L)={γgl(L)|γ([x,y])=[x,γ(y)] for all x,yL}.

For each map γCent(L) we have [γ(x),y]+[x,γ(y)]=2γ([x,y]) for all x,yL. Thus, Cent(L)QDer(L) and so Der(L)+Cent(L)QDer(L).

In several cases this is a strict inclusion. However, for some Lie algebras we have (1.1) Der(L)+Cent(L)=QDer(L)(1.1) or even (1.2) Der(L)+Cent(L)=GDer(L).(1.2)

Let us mention that Leger and Luks [Citation6, Corollary 4.16] proved that (1.1) holds true for each centerless Lie algebra L generated by special weight spaces. Examples of Lie algebras satisfying (1.2) can be found in Brešar’s paper [Citation1], where the structure of near-derivations was described for certain Lie algebras arising from associative ones. Note that the notion of a near-derivation, which was introduced in [Citation1], is even more general than the notion of a generalized derivation.

Suppose that L and A are algebras over a field F, where L is a Lie algebra and A is an associative commutative algebra with unity. The tensor product algebra LFA (or shortly LA) is also a Lie algebra over F, which is called a current Lie algebra. Recall that the Lie product on LA is defined as a bilinear map such that [xa,yb]=[x,y]ab for any simple tensors xa,ybLA.

The aim of this paper is to consider the following two questions.

  1. Does LA satisfy (1.1), if L satisfies (1.1)?

  2. Does LA satisfy (1.2), if L satisfies (1.2)?

Our research was motivated by [Citation6] and by Brešar’s papers [Citation2, Citation3], where the study of functional identities on tensor products of algebras was initiated.

2 The results

Let L be a Lie algebra over a field F. Recall that the center Z(L):={xL|[x,y]=0 for all yL} and the derived algebra [L,L]:=Span({[x,y]|x,yL}) are ideals of L. If Z(L)={0}, we say that L is centerless. For any subset S of L the set ZL(S):={xL|[x,s]=0 for all sS} is called the annihilator of S in L. If I is an ideal of L then ZL(I) is also an ideal of L. Thus, ZL([L,L]) is an ideal of L and Z(L)=ZL(L)ZL([L,L]).

Note that for any centerless Lie algebra L the sum Der(L)+Cent(L)=Der(L)Cent(L) is a direct sum of vector spaces. Recall that a Lie algebra L is prime, if L has no nonzero ideals I, J such that [I,J]=0. Clearly, all prime Lie algebras are centerless. A Lie algebra is said to be perfect if [L,L]=L. Let us state our main result on the form of quasiderivations of a current Lie algebra LA.

Theorem 2.1.

Let LA be a current Lie algebra over a field F, where L is centerless and char(F)2. Suppose that L is either perfect or prime. If QDer(L)=Der(L)Cent(L), then QDer(LA)=Der(LA)Cent(LA).

Another aim of this paper is to obtain a similar result for generalized derivations. Recall that the notion of a quasicentroid QCent(L) of a Lie algebra L was defined in [Citation6] as QCent(L)={fgl(L)|[f(x),y]=[x,f(y)] for all x,yL}.

Obviously, Cent(L)QCent(L) and (2.1) GDer(L)=QDer(L)+QCent(L)(2.1) (see [Citation6, Proposition 3.3]). Note that each commuting linear map f:LL (i.e. [f(x),x]=0 for all xL) belongs to QCent(L). Moreover, if char(F)2 then QCent(L) coincides with the set of all commuting linear maps of L.

Let L be a centerless Lie algebra over a field F with char(F)2. Suppose that L is either perfect or prime. Then ZL([L,L])=0 and hence the result of Brešar and Zhao [Citation4, Corollary 3.3] implies that the set of all commuting linear maps of L coincides with Cent(L). Thus, QCent(L)=Cent(L)QDer(L) and hence (2.1) implies GDer(L)=QDer(L). Since ZL([L,L])=0 it follows that ZLA([LA,LA])=0 and so GDer(LA)=QDer(LA) as well. Hence, Theorem 2.1 implies the following corollary.

Corollary 2.2.

Let LA be a current Lie algebra over a field F, where L is centerless and char(F)2. Suppose that L is either perfect or prime. Then GDer(L)=Der(L)Cent(L) implies GDer(LA)=Der(LA)Cent(LA).

If LA is a current Lie algebra, where A is finite dimensional, then we obtain the same conclusion assuming only that L is centerless.

Theorem 2.3.

Let LA be a current Lie algebra over a field F with char(F)2. Suppose that L is centerless and A is finite dimensional.

  1. If GenDer(L)=Der(L)Cent(L), then GenDer(LA)=Der(LA)Cent(LA).

  2. If QDer(L)=Der(L)Cent(L), then QDer(LA)=Der(LA)Cent(LA).

The proofs of Theorems 2.1 and 2.3 are given in the next section.

3 The proofs

Let L and A be algebras over a field F, where L is a Lie algebra and A is an associative commutative algebra with unity. Pick a basis B={bi|iI} of A. Hence every element in LA can be written uniquely in the form xi1bi1+xi2bi2++xinbin where n1 and xiL.

Let f:LALA be a linear map. For any element xL there exist unique elements fi(x)L, iI, such that (3.1) f(x1)=iIfi(x)bi,(3.1) where fi(x)=0 for all but finitely many iI. For each iI the map fi:LL defined by fi:xfi(x) is obviously linear. Let fB:LALA be a linear map such that (3.2) fB(xa)=iIfi(x)abi(3.2) for each simple tensor xaLA. Obviously, fB is well-defined since for each xL we have fi(x)0 for only finitely many elements iI. Note that f(x1)=fB(x1) for all xL.

The following proposition shows that certain properties of a linear map f are inherited to the map fB.

Proposition 3.1.

Let LA be a current Lie algebra over a field F. For any basis B of A the following assertions hold true:

  1. If fGenDer(LA), then fBGenDer(LA).

  2. If fQDer(LA), then fBQDer(LA).

Proof.

First, suppose that fGenDer(LA). Then there exist linear maps g,h:LALA such that (3.3) [f(x),y]+[x,g(y)]=h([x,y])(3.3) for all x,yLA. Pick any basis B={bi|iI} of A. Then according to (3.2) the linear maps gB,hB:LALA are given by (3.4) gB(xa)=iIgi(x)abiandhB(xa)=iIhi(x)abi(3.4) for any simple tensor xaLA. In order to prove that fBGenDer(LA), let us show that (3.5) [fB(x),y]+[x,gB(y)]=hB([x,y])(3.5) for all x,yLA. Setting simple tensors x1,y1 in (3.3) and using [x1,y1]=[x,y]1, we get h([x,y]1)=[f(x1),y1]+[x1,g(y1)].

According to (3.2) this identity can be rewritten as iIhi([x,y])bi=[iIfi(x)bi,y1]+[x1,iIgi(y)bi]=iI[fi(x),y]bi+iI[x,gi(y)]bi and consequently iI([fi(x),y]+[x,gi(y)]hi([x,y]))bi=0. for all x,yL. Thus, for any iI we have (3.6) [fi(x),y]+[x,gi(y)]=hi([x,y])(3.6) for all x,yL. Using (3.6) we obtain hB([xa,yb])=hB([x,y]ab)=iIhi([x,y])abbi=iI([fi(x),y]+[x,gi(y)])abbi=iI[fi(x),y]abbi+iI[x,gi(y)]abbi=iI[fi(x)abi,yb]+iI[xa,gi(y)bbi]=[iIfi(x)abi,yb]+[xa,iIgi(y)bbi]=[fB(xa),yb]+[xa,gB(yb)]. for all simple tensors xa,ybLA. Since fB, gB, and hB are linear maps it follows that (3.5) holds true. Thus, fBGenDer(LA) and so the proof of (i) is complete.

Note that (ii) can be proved analogously by setting f = g in the arguments above. □

Lemma 3.2.

Let LA be a current Lie algebra over a field F and let B={bi|iI} be a basis of A. Suppose that {fi:LL|iI} is a family of linear maps such that for any xL we have fi(x)0 for only finitely many elements iI. Let a linear map fB:LALA be defined as in (3.2).

  1. If fiDer(L) for all iI, then fBDer(LA).

  2. If fiCent(L) for all iI, then fBCent(LA).

Proof.

(i) Suppose that fiDer(L) for all iI. Thus, for each iI [fi(x),y]+[x,fi(y)]=fi([x,y]) for all x,yL. For any simple tensors xa,ybLA we have fB([xa,yb])=fB([x,y]ab)=iIfi([x,y])abbi=iI([fi(x),y]+[x,fi(y)])abbi=iI[fi(x),y]abbi+iI[x,fi(y)]abbi=iI[fi(x)abi,yb]+iI[xa,fi(y)bbi]=[iIfi(x)abi,yb]+[xa,iIfi(y)bbi]=[fB(xa),yb]+[xa,fB(yb)].

Since fB is linear it follows that fBDer(LA).

(ii) Let’s assume that fiCent(L) for all iI. Thus, for each iI [fi(x),y]=fi([x,y])

for all x,yL. For any simple tensors xa,ybLA we have fB([xa,yb])=fB([x,y]ab)=iIfi([x,y])abbi=iI[fi(x),y]abbi=iI[fi(x)abi,yb]=[iIfi(x)abi,yb]=[fB(xa),yb].

Since fB is linear it follows that fBCent(LA). □

Lemma 3.3.

Let LA be a current Lie algebra over a field F and let B={bi|iI} be a basis of A. Suppose that L is perfect or L is prime. Furthermore, assume that QDer(L)=Der(L)Cent(L). If fQDer(LA), then fBDer(LA)Cent(LA).

Proof.

Let us pick an arbitrary quasi-derivation fQDer(LA). Then there exists a linear map h:LALA such that (3.7) [f(x),y]+[x,f(y)]=h([x,y])(3.7) for all x,yLA. Recall that there exist families of linear maps {fi:LL|iI} and {hi:L L|iI} such that f(x1)=iIfi(x)bi  and  h(x1)=iIhi(x)bi for all xL, where for each xL we have fi(x)0 for only finitely many elements iI and hi(x)0 for only finitely many elements iI (see (3.1)). Similarly as in the proof of Proposition 3.1 we see that for any iI we get (3.8) [fi(x),y]+[x,fi(y)]=hi([x,y])(3.8) for all x,yL. Hence, each fi is a quasi-derivation of L. Consequently, our assumption implies fiDer(L)Cent(L) for all iI. Thus, for each iI there exist maps diDer(L) and γiCent(L) such that fi=di+γi. Hence, (3.8) can be rewritten as (3.9) hi([x,y])=[di(x)+γi(x),y]+[x,di(y)+γi(y)]=[di(x),y]+[x,di(y)]+[γi(x),y]+[x,γi(y)]=di([x,y])+γi([x,y])+γi([x,y])=fi([x,y])+γi([x,y])(3.9) for all x,yL and iI.

First, suppose that L is perfect. Since [L,L]=L it follows from (3.9) that γi(x)=hi(x)fi(x) for all xL and iI. Hence, for each xL we have γi(x)=0 for all but finitely many elements iI and consequently di(x)=fi(x)γi(x)=0 for all but finitely many elements iI.

Next, suppose that L is prime. According to (3.9) we see that for each pair x,yL we have γi([x,y])=0 for all but finitely many elements iI. Without loss of generality, we may assume that L is nonzero. Since L is prime it follows that [L,L]{0}. Hence, there exist elements x0,y0L such that [x0,y0]0. Since L is torsion free Cent(L)-module (see [Citation5, Theorem 1.1]) and since γi([x0,y0])=0 for all but finitely many elements iI it follows that γi=0 for all but finitely many elements iI. Consequently, for each xL also di(x)=fi(x)γi(x)=0 for all but finitely many elements iI.

Let dB,γB:LALA be linear maps such that (3.10) dB(xa)=iIdi(x)abiandγB(xa)=iIγi(x)abi(3.10) for each simple tensor xaLA. Obviously, dB and γB are well-defined, since in case L is perfect or prime, both sums in (3.10) are finite. Namely, for any xL in both cases di(x)=0 for all but finitely many elements iI and γi(x)=0 for all but finitely many elements iI. Now, Lemma 3.2 implies that dBDer(LA) and γBCent(LA). We can now conclude that fB(xa)=iIfi(x)abi=iI(di(x)+γi(x))abi=iIdi(x)abi+iIγi(x)abi=dB(xa)+γB(xa) for each simple tensor xaLA. Since fB, dB, and γB are linear maps it follows fB=dB+γBDer(LA)Cent(LA). □

If we assume that A is a finite dimensional algebra in Lemma 3.3, then we can drop the assumption of L being perfect or prime. Namely, in this case both sums in (3.10) are finite and so the maps dB and γB are well-defined. Thus, using similar arguments as in the proof of Lemma 3.3 we obtain the following proposition.

Proposition 3.4.

Let LA be a current Lie algebra over a field F and let B be a basis of A. Suppose that dimFA<.

  1. If fGenDer(LA) and GenDer(L)=Der(L)Cent(L), then fBDer(LA)Cent(LA).

  2. If fQDer(LA) and QDer(L)=Der(L)Cent(L), then fBDer(LA)Cent(LA).

Recall that a map f:LL is commuting if [f(x),x]=0 for all xL. The following lemma, which will be used in the proof of Theorem 2.3, follows directly from [Citation6, Proposition 5.26].

Lemma 3.5.

Let L be a centerless Lie algebra over a field F with char(F)2. If a quasi-derivation fQDer(L) is commuting, then fCent(L).

Now, we can prove our main results, Theorems 2.1 and 2.3.

Proof of Theorem 2.1.

Suppose that QDer(L)=Der(L)Cent(L). Pick any basis B={bi|iI} of A. Let fQDer(LA) be an arbitrary quasi-derivation. According to Proposition 3.1 the map fB is a quasi-derivation of LA. Moreover, Lemma 3.3 implies that fBDer(LA)Cent(LA). Let F=ffB. Obviously, FQDer(LA) and F(x1)=f(x1)fB(x1)=0 for all xL. Since F is a quasi-derivation there exists a linear map H:LALA such that (3.11) [F(x),y]+[x,F(y)]=H([x,y])(3.11) for all x,yLA. For each simple tensor xaLA there exist unique elements Fi(xa)L, iI, such that F(xa)=iIFi(xa)bi, where Fi(xa)0 for only finitely many iI. For each aA and each iI we define a map Fa,i:LL by Fa,i:xFi(xa), which is obviously linear. First, we shall show that Fa,iCent(L) for any aA and any iI. Let us fix an arbitrary aA. Setting simple tensors xa and x1 in (3.11) and using F(x1)=0 we obtain [F(xa),x1]=H([xa,x1])=H([x,x]a)=0 for all xL. Hence, 0=[F(xa),x1]=[iIFi(xa)bi,x1]=iI[Fa,i(x),x]bi for all xL. Consequently, [Fa,i(x),x]=0 for all xL and all iI. Thus, for each aA and each iI the map Fa,i is commuting. According to our assumption L is perfect and centerless or L is prime. In both cases it follows that ZL([L,L])={0}. Hence, [Citation4, Corollary 3.3] yields that Fa,iCent(L) for all iI, aA. Next, we claim that FDer(LA). Namely, setting simple tensors xa in yb in (3.11) we get (3.12) H([xa,yb])=[F(xa),yb]+[xa,F(yb)].(3.12)

On the other hand, since [xa,yb]=[xab,y1] and F(y1)=0, we obtain H([xa,yb])=[F(xab),y1]=[iIFab,i(x)bi,y1] for all x,yL and a,bA. Since Fab,iCent(L) it follows H([xa,yb])=iI[Fab,i(x),y]bi=iIFab,i([x,y])bi=F([x,y]ab) for all x,yL and a,bA. Hence, (3.13) H([xa,yb])=F([xa,yb])(3.13) for all xa,ybLA. Consequently, (3.12) can be rewritten as F([xa,yb])=[F(xa),yb]+[xa,F(yb)] for all xa,ybLA. Since F is linear it follows that FDer(LA). We can now conclude that f=fB+F, where fBDer(LA)Cent(LA) and FDer(LA). Thus, fDer(LA)Cent(LA) and so the proof is complete. □

Proof of Theorem 2.3.

In order to prove (i) let us assume that GenDer(L)=Der(L)Cent(L). Pick any basis B={bi|iI} of A. Here, I={1,2,,n}, since A is finite dimensional. Let fGenDer(LA). Then there exist linear maps g,h:LALA such that (3.14) [f(x),y]+[x,g(y)]=h([x,y])(3.14) for all x,yLA. Proposition 3.1 implies fBGenDer(LA). Moreover, (3.15) [fB(x),y]+[x,gB(y)]=hB([x,y])(3.15) for all x,yLA (see the proof of Proposition 3.1). According to Proposition 3.4 we know that fBDer(LA)Cent(LA). Let us define the following maps: F=ffB, G=ggB, and H=hhB. Obviously, F, G, and H are linear maps. Using (3.14) and (3.15) we get (3.16) [F(x),y]+[x,G(y)]=H([x,y])(3.16) for all x,yLA. Moreover, F(x1)=0=G(x1) for all xL. For each simple tensor xaLA there exist unique elements Fi(xa),Gi(xa),Hi(xa)L, iI, such that (3.17) F(xa)=iIFi(xa)bi,G(xa)=iIGi(xa)bi,H(xa)=iIHi(xa)bi.(3.17)

For each aA and each iI we define maps Fa,i,Ga,i,Ha,i:LL by Fa,i:xFi(xa), Ga,i:xGi(xa), and Ha,i:xHi(xa). It is easy to see that Fa,i,Ga,i,Ha,i are linear maps. Our aim is to prove that F is a derivation. First, let us prove that Fa,iCent(L) for all aA and iI. Since G(y1)=0 it follows from (3.16) that (3.18) [F(xa),y1]=H([xa,y1])=H([x,y]a)(3.18) for all x,yL and aA. Fix an arbitrary element aA. Using (3.17) we can rewrite (3.18) as 0=[F(xa),y1]H([x,y]a)=[iIFi(xa)bi,y1]iIHi([x,y]a)bi=iI([Fi,a(x),y]Hi,a([x,y]))bi for all x,yL. Hence, (3.19) [Fa,i(x),y]=Ha,i([x,y])(3.19) for all x,yL. Consequently, [Fa,i(x),x]=0 for all xL. Thus, Fa,i is a commuting linear map for each aA and each iI. By interchanging the roles of x and y in (3.19) and using [x,y]=[y,x] we get [x,Fa,i(y)]=Ha,i([x,y]) and so [Fa,i(x),y]+[x,Fa,i(y)]=2Ha,i([x,y]) for all x,yL. This means that Fa,iQDer(L) and hence Lemma 3.5 yields that Fi,aCent(L) for each aA and each iI. Next, we shall prove that F = G. Namely, since G(y1)=0=F(x1) we see that (3.16) yields [F(xa),y1]=H([xa,y1])=H([x1,ya])=[x1,G(ya)] for all x,yL and aA. Fix an arbitrary aA. Using (3.17) we can rewrite the last identity as 0=[iIFa,i(x)bi,y1][x1,iIGa,i(y)bi]=iI[Fa,i(x),y]biiI[x,Ga,i(y)]bi=iI([Fa,i(x),y][x,Ga,i(y)])bi for all x,yL. Consequently, for each iI we have [Fa,i(x),y]=[x,Ga,i(y)] for all x,yL. Since Fa,iCent(L) it follows [x,Ga,i(y)]=[Fa,i(x),y]=Fa,i([x,y])=[x,Fa,i(y)] and hence [x,Ga,i(y)Fa,i(y)]=0 for all x,yL and iI. Thus, Ga,i(y)Fa,i(y) belongs to the center of L for all yL and iI. Since L is centerless it now follows that Ga,i=Fa,i for all iI and all aA. Accordingly, (3.17) implies F(xa)=G(xa) for each simple tensor xaLA. However, since F and G are linear it follows F = G. By using the same arguments as in the proof of Theorem 2.1 we can now show that F is a derivation. Thus, since f=fB+F, where fBDer(LA)Cent(LA) and FDer(LA), it follows that fDer(LA)Cent(LA). The proof of (i) is now complete.

Note that (ii) can be proved analogously by setting f = g in the arguments above. □

Remark.

According to Theorem 2.3 one might conjecture that Theorem 2.1 holds true even without the assumption that a Lie algebra L is either perfect or prime. Unfortunately, we were not able to prove nor disprove this conjecture.

References