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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 the sum of a derivation and a map from the centroid of
, 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 is called a derivation if
for all
. As usual, we denote the set of all derivations of L by
. Obviously,
is a Lie subalgebra of the general linear algebra
. 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
be a linear map. If there exist linear maps
such that
for all
, then f is called a generalized derivation. In case there exists a linear map
such that
for all
, then f is said to be a quasiderivation. By
we shall denote the set of all generalized derivations of L and by
the set of all quasiderivations of L. Obviously,
and
are Lie subalgebras of
such that
Yet another Lie subalgebra of is the centroid of L, which is defined as
For each map we have
for all
. Thus,
and so
In several cases this is a strict inclusion. However, for some Lie algebras we have
(1.1)
(1.1)
or even
(1.2)
(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 (or shortly
) is also a Lie algebra over F, which is called a current Lie algebra. Recall that the Lie product on
is defined as a bilinear map such that
for any simple tensors
.
The aim of this paper is to consider the following two questions.
Does
satisfy (1.1), if L satisfies (1.1)?
Does
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
and the derived algebra
are ideals of L. If
, we say that L is centerless. For any subset S of L the set
is called the annihilator of S in L. If I is an ideal of L then
is also an ideal of L. Thus,
is an ideal of L and
Note that for any centerless Lie algebra L the sum 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
. Clearly, all prime Lie algebras are centerless. A Lie algebra is said to be perfect if
. Let us state our main result on the form of quasiderivations of a current Lie algebra
.
Theorem 2.1.
Let be a current Lie algebra over a field F, where L is centerless and
. Suppose that L is either perfect or prime. If
, then
.
Another aim of this paper is to obtain a similar result for generalized derivations. Recall that the notion of a quasicentroid of a Lie algebra L was defined in [Citation6] as
Obviously, and
(2.1)
(2.1)
(see [Citation6, Proposition 3.3]). Note that each commuting linear map
(i.e.
for all
) belongs to
. Moreover, if
then
coincides with the set of all commuting linear maps of L.
Let L be a centerless Lie algebra over a field F with . Suppose that L is either perfect or prime. Then
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
. Thus,
and hence (2.1) implies
. Since
it follows that
and so
as well. Hence, Theorem 2.1 implies the following corollary.
Corollary 2.2.
Let be a current Lie algebra over a field F, where L is centerless and
. Suppose that L is either perfect or prime. Then
implies
.
If 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 be a current Lie algebra over a field F with
. Suppose that L is centerless and A is finite dimensional.
If
, then
.
If
, then
.
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 of A. Hence every element in
can be written uniquely in the form
where
and
.
Let be a linear map. For any element
there exist unique elements
, such that
(3.1)
(3.1)
where
for all but finitely many
. For each
the map
defined by
is obviously linear. Let
be a linear map such that
(3.2)
(3.2)
for each simple tensor
. Obviously,
is well-defined since for each
we have
for only finitely many elements
. Note that
for all
.
The following proposition shows that certain properties of a linear map f are inherited to the map .
Proposition 3.1.
Let be a current Lie algebra over a field F. For any basis
of A the following assertions hold true:
If
, then
.
If
, then
.
Proof.
First, suppose that . Then there exist linear maps
such that
(3.3)
(3.3)
for all
. Pick any basis
of A. Then according to (3.2) the linear maps
are given by
(3.4)
(3.4)
for any simple tensor
. In order to prove that
, let us show that
(3.5)
(3.5)
for all
. Setting simple tensors
in (3.3) and using
, we get
According to (3.2) this identity can be rewritten as
and consequently
for all
. Thus, for any
we have
(3.6)
(3.6)
for all
. Using (3.6) we obtain
for all simple tensors
. Since
, and
are linear maps it follows that (3.5) holds true. Thus,
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 be a current Lie algebra over a field F and let
be a basis of A. Suppose that
is a family of linear maps such that for any
we have
for only finitely many elements
. Let a linear map
be defined as in (3.2).
If
for all
, then
.
If
for all
, then
.
Proof.
(i) Suppose that for all
. Thus, for each
for all
. For any simple tensors
we have
Since is linear it follows that
.
(ii) Let’s assume that for all
. Thus, for each
for all . For any simple tensors
we have
Since is linear it follows that
. □
Lemma 3.3.
Let be a current Lie algebra over a field F and let
be a basis of A. Suppose that L is perfect or L is prime. Furthermore, assume that
. If
, then
.
Proof.
Let us pick an arbitrary quasi-derivation . Then there exists a linear map
such that
(3.7)
(3.7)
for all
. Recall that there exist families of linear maps
and
such that
for all
, where for each
we have
for only finitely many elements
and
for only finitely many elements
(see (3.1)). Similarly as in the proof of Proposition 3.1 we see that for any
we get
(3.8)
(3.8)
for all
. Hence, each fi
is a quasi-derivation of L. Consequently, our assumption implies
for all
. Thus, for each
there exist maps
and
such that
. Hence, (3.8) can be rewritten as
(3.9)
(3.9)
for all
and
.
First, suppose that L is perfect. Since it follows from (3.9) that
for all
and
. Hence, for each
we have
for all but finitely many elements
and consequently
for all but finitely many elements
.
Next, suppose that L is prime. According to (3.9) we see that for each pair we have
for all but finitely many elements
. Without loss of generality, we may assume that L is nonzero. Since L is prime it follows that
. Hence, there exist elements
such that
. Since L is torsion free
-module (see [Citation5, Theorem 1.1]) and since
for all but finitely many elements
it follows that
for all but finitely many elements
. Consequently, for each
also
for all but finitely many elements
.
Let be linear maps such that
(3.10)
(3.10)
for each simple tensor
. Obviously,
and
are well-defined, since in case L is perfect or prime, both sums in (3.10) are finite. Namely, for any
in both cases
for all but finitely many elements
and
for all but finitely many elements
. Now, Lemma 3.2 implies that
and
. We can now conclude that
for each simple tensor
. Since
, and
are linear maps it follows
. □
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 and
are well-defined. Thus, using similar arguments as in the proof of Lemma 3.3 we obtain the following proposition.
Proposition 3.4.
Let be a current Lie algebra over a field F and let
be a basis of A. Suppose that
.
If
and
, then
.
If
and
, then
.
Recall that a map is commuting if
for all
. 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 . If a quasi-derivation
is commuting, then
.
Now, we can prove our main results, Theorems 2.1 and 2.3.
Proof of Theorem 2.1.
Suppose that . Pick any basis
of A. Let
be an arbitrary quasi-derivation. According to Proposition 3.1 the map
is a quasi-derivation of
. Moreover, Lemma 3.3 implies that
. Let
. Obviously,
and
for all
. Since F is a quasi-derivation there exists a linear map
such that
(3.11)
(3.11)
for all
. For each simple tensor
there exist unique elements
, such that
where
for only finitely many
. For each
and each
we define a map
by
, which is obviously linear. First, we shall show that
for any
and any
. Let us fix an arbitrary
. Setting simple tensors
and
in (3.11) and using
we obtain
for all
. Hence,
for all
. Consequently,
for all
and all
. Thus, for each
and each
the map
is commuting. According to our assumption L is perfect and centerless or L is prime. In both cases it follows that
. Hence, [Citation4, Corollary 3.3] yields that
for all
. Next, we claim that
. Namely, setting simple tensors
in
in (3.11) we get
(3.12)
(3.12)
On the other hand, since and
, we obtain
for all
and
. Since
it follows
for all
and
. Hence,
(3.13)
(3.13)
for all
. Consequently, (3.12) can be rewritten as
for all
. Since F is linear it follows that
We can now conclude that
where
and
. Thus,
and so the proof is complete. □
Proof of Theorem 2.3.
In order to prove (i) let us assume that . Pick any basis
of A. Here,
, since A is finite dimensional. Let
. Then there exist linear maps
such that
(3.14)
(3.14)
for all
. Proposition 3.1 implies
. Moreover,
(3.15)
(3.15)
for all
(see the proof of Proposition 3.1). According to Proposition 3.4 we know that
. Let us define the following maps:
, and
. Obviously, F, G, and H are linear maps. Using (3.14) and (3.15) we get
(3.16)
(3.16)
for all
Moreover,
for all
. For each simple tensor
there exist unique elements
, such that
(3.17)
(3.17)
For each and each
we define maps
by
, and
. It is easy to see that
are linear maps. Our aim is to prove that F is a derivation. First, let us prove that
for all
and
. Since
it follows from (3.16) that
(3.18)
(3.18)
for all
and
. Fix an arbitrary element
. Using (3.17) we can rewrite (3.18) as
for all
. Hence,
(3.19)
(3.19)
for all
. Consequently,
for all
. Thus,
is a commuting linear map for each
and each
. By interchanging the roles of x and y in (3.19) and using
we get
and so
for all
. This means that
and hence Lemma 3.5 yields that
for each
and each
. Next, we shall prove that F = G. Namely, since
we see that (3.16) yields
for all
and
. Fix an arbitrary
. Using (3.17) we can rewrite the last identity as
for all
. Consequently, for each
we have
for all
. Since
it follows
and hence
for all
and
. Thus,
belongs to the center of L for all
and
. Since L is centerless it now follows that
for all
and all
. Accordingly, (3.17) implies
for each simple tensor
. 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
, where
and
, it follows that
. 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
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