Almost inner derivations of Lie algebras II
Dietrich Burde, Karel Dekimpe, Bert Verbeke

TL;DR
This paper extends the algebraic understanding of almost inner derivations in Lie algebras, explicitly determining these derivations for various classes including free nilpotent, almost abelian, and certain filiform nilpotent Lie algebras over characteristic zero fields.
Contribution
It provides explicit descriptions of almost inner derivations for several classes of Lie algebras and introduces a family of characteristically nilpotent filiform Lie algebras with all derivations almost inner.
Findings
Determined almost inner derivations for free nilpotent Lie algebras.
Identified all derivations as almost inner for a family of filiform nilpotent Lie algebras.
Compared almost inner derivations over different base fields.
Abstract
We continue the algebraic study of almost inner derivations of Lie algebras over a field of characteristic zero and determine these derivations for free nilpotent Lie algebras, for almost abelian Lie algebras, for Lie algebras whose solvable radical is abelian and for several classes of filiform nilpotent Lie algebras. We find a family of -dimensional characteristically nilpotent filiform Lie algebras , for all , all of whose derivations are almost inner. Finally we compare the almost inner derivations of Lie algebras considered over two different fields for a finite-dimensional field extension.
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Almost inner derivations of Lie algebras II
Dietrich Burde
,
Karel Dekimpe
and
Bert Verbeke
Fakultät für Mathematik
Universität Wien
Oskar-Morgenstern-Platz 1
1090 Wien
Austria
Katholieke Universiteit Leuven Kulak
E. Sabbelaan 53 bus 7657
8500 Kortrijk
Belgium
Abstract.
We continue the algebraic study of almost inner derivations of Lie algebras over a field of characteristic zero and determine these derivations for free nilpotent Lie algebras, for almost abelian Lie algebras, for Lie algebras whose solvable radical is abelian and for several classes of filiform nilpotent Lie algebras. We find a family of -dimensional characteristically nilpotent filiform Lie algebras , for all , all of whose derivations are almost inner. Finally we compare the almost inner derivations of Lie algebras considered over two different fields for a finite-dimensional field extension.
Key words and phrases:
Almost inner derivations
2010 Mathematics Subject Classification:
17B40
1. Introduction
Almost inner automorphisms of Lie groups and almost inner derivations of Lie algebras have been introduced by Gordon and Wilson [4] in the study of isospectral deformations of compact solvmanifolds. They constructed isospectral but non-isometric compact Riemannian manifolds of the form , with a simply connected exponential solvable Lie group , and a discrete cocompact subgroup of . This construction relies on almost inner automorphisms and almost inner derivations. Larsen [7] studied algebraic groups for which every two almost conjugated homomorphisms are globally conjugated. This is closely related to the question whether or not a compact group can be the common covering space of a pair of non-isometric isospectral manifolds.
The concept of “almost inner” automorphisms and derivations, almost homomorphisms, or almost conjugate subgroups arises in many areas of algebra and geometry. However, a systematic algebraic study was not done so far. So we started an investigation of almost inner derivations of Lie algebras in [1]. The aim of this paper is to continue this study and prove further results on almost inner derivations for certain classes of Lie algebras.
We recall the following definitions. Let be a finite-dimensional Lie algebra over a field and its derivation Lie algebra. A derivation is said to be almost inner, if for all . The space of all almost inner derivations of is denoted by . The subspace becomes a Lie subalgebra of by the Lie bracket . We denote the Lie subalgebra of inner derivations by . An almost inner derivation is called central almost inner if there exists an such that maps to the center . We denote the subalgebra of central almost inner derivations of by .
The paper is structured as follows. In the second section we show that every almost inner derivation of a free nilpotent Lie algebra over a field of characteristic zero is inner. Similarly, in the third section, we show that every almost inner derivation of an almost abelian Lie algebra is inner. In the fourth section we compute the almost inner derivations for certain classes of filiform nilpotent Lie algebras, e.g., for the Witt algebras and for a family , , which is closely related to . We show that the Witt algebra has linearly independent outer derivations, where of them are almost inner. For we show that every derivation is almost inner. This comes as a surprise and it is the first known family of nilpotent Lie algebras, where all derivations are almost inner. In the fifth section we show that every almost inner derivation is inner for Lie algebras whose solvable radical is abelian over an algebraically closed field of characteristic zero. Here we use results about “distinguished” elements in semisimple Lie algebras, whose centralizers consist entirely of nilpotent elements.
The last two sections contain results about almost inner derivations of Lie algebras considered over two different fields . In particular we show that if a Lie algebra viewed over admits a non-trivial almost inner derivation, then so does also the Lie algebra viewed over the smaller field . However, the converse does not hold in general. We can construct new almost inner derivations using field extensions.
2. Free nilpotent Lie Algebras
In this section we will prove that a free nilpotent Lie algebra over a field of characteristic zero does not admit any non-trivial almost inner derivations. We will use the following lemma, which can be shown by induction on .
Lemma 2.1**.**
Let be a non-negative integer and be a vector space over a field of characteristic zero. Consider a sequence in . Suppose that there exist such that
[TABLE]
for all . Then there exist vectors such that
[TABLE]
Consider the free Lie algebra on two generators and . Define as the vector space spanned by the generators and and , for , as the subspace of generated by all Lie brackets of length in the generators and . Denote further for the subspace of generated by all Lie brackets in the generators where the first generator appears times and the second one appears times. It is clear that
[TABLE]
Moreover, it holds that
[TABLE]
We are interested in the equation
[TABLE]
in the variables and , which was studied in [8]. Let
[TABLE]
be the solution space of the equation. Note that is a vector space. For each , we define . Consider now the maps
[TABLE]
Denote and . We assert that is an isomorphism for all . It is obvious that the map is linear. Surjectivity follows by construction. Suppose that is not injective, then there is a solution , which means that . Therefore, and we have a contradiction. Analogously, also is an isomorphism. Hence, for all , there is a vector space isomorphism such that for all . Note that under this isomorphism for all . Denote further by and , the terms of the lower central series.
Theorem 2.2**.**
Let be a field of characteristic zero and let be the free –step nilpotent Lie algebra over on generators. Then we have .
Proof.
We prove this theorem by induction on the nilpotency class . The case is clear and the cases and were already treated in [1]. So let and assume that the theorem holds for . Consider now with generators . Let be an almost inner derivation of . We will prove that is in fact inner. It is clear that induces an almost inner derivation on
[TABLE]
By the induction hypothesis, this is an inner derivation. Hence, by changing up to an inner derivation, we may assume that , which means that . Hence, there exists such that . By replacing by , we can assume that is an almost inner derivation of with . Further, for all , we have , with . It suffices to prove that for all . We first look at . For each , there exists a such that
[TABLE]
because is almost inner. We can assume without loss of generality that is a linear combination of Lie brackets of length in the generators (and does not contain a component using Lie brackets of length ). By linearity, we also have that
[TABLE]
The two observations above imply that the equation
[TABLE]
holds for all . We consider as an equation in the free Lie algebra on generators. For , define . It is clear that is also a free generating set for the free Lie algebra .
It follows from [8, section 5] that for all , where denotes the Lie algebra generated by and . This means that can be written as , where is a linear combination of Lie brackets where and appear respectively times. We can assume without loss of generality that we work in , the free Lie algebra on two generators and (and so , using the notations introduced above this theorem). To prove that , it suffices by equation (1) to show that . Suppose on the contrary that . Define
[TABLE]
then and there exists an such that . It follows from equation (2) that , which implies that
[TABLE]
with . Note that this consists in fact of several equations (one per bi-degree with ).
We will now prove by induction on that for all and all , there exist , with such that
[TABLE]
Basis step : we first consider the component of equation (3) with in total appearances of , i.e. the bi-degree –part. This gives
[TABLE]
Hence, , which means that is a constant and belongs to . Therefore, we have that .
Induction step: we assume that the assertion holds for a given . Hence, there exist with such that
[TABLE]
From the component of equation (3) with appearances of , it follows that
[TABLE]
Hence,
[TABLE]
which can be written as the sum of and terms of lower degree. Since , also holds. Note that all belong to . Hence, it follows from Lemma 2.1 that there exist with such that
[TABLE]
which concludes the proof of our claim on the form of the .
The above assertion implies that for all , the equation holds, where and .
We now look at the term of equation (3) with exactly one factor of . We then have
[TABLE]
and thus
[TABLE]
This implies that
[TABLE]
Hence, we can write [math] as a sum of and some terms of lower degree. This equation has to hold for all , which implies that . Since we work in a field of characteristic zero, this gives a contradiction, because . Hence, . It now follows from equation (1) that . By a similar reasoning, we find that for all . This finishes the proof. ∎
3. Almost abelian Lie algebras
The aim of this section is to show the following result.
Theorem 3.1**.**
Let be a finite-dimensional Lie algebra over a field containing an abelian ideal of codimension one. Then .
Proof.
As has a codimension one abelian ideal, it holds that for some Lie algebra morphism . We use to denote a basis vector of . With respect to a suitable basis of , we may assume that is in rational canonical form. This means that there is a basis (, ) of such that
[TABLE]
is a blocked diagonal matrix where each block is a companion matrix
[TABLE]
of a polynomial , where is irreducible. Since is irreducible, it holds that either and hence or .
Now, let . There exists an element such that . By replacing with , we may assume that .
For any vector , there exists a scalar , for which it holds that
[TABLE]
Our aim is to show now that if both , then
[TABLE]
Since we assume that , it holds that
[TABLE]
Moreover by considering several cases we can see that and are linearly independent when :
Case 1, : then belongs to the span of , while belongs to the span of , which shows that these vectors are linearly independent.
Case 2, : we may assume that .
In case we have that and which are clearly linearly independent.
In case we have that with (if , then also and ). Hence we obtain again that and are linearly independent.
We find that
[TABLE]
while on the other hand we also have
[TABLE]
Since and must coincide and using the fact that and are linearly independent, we finally find that
[TABLE]
Now, let be the fixed value such that when , then we have that
[TABLE]
It follows that coincides with on all basis vectors and hence . ∎
This result cannot be extended to Lie algebras of the form .
Example 3.2**.**
Let and consider the Lie algebra over with basis and non-vanishing Lie brackets
[TABLE]
Then we have . Let be defined by . Then is a derivation. Define the map by
[TABLE]
Then we have that for all , showing that . It is easy to see that . Hence we have .
This result can also not be generalized to Lie algebras of the form where is a free nilpotent Lie algebra on generators and of class .
Example 3.3**.**
Let be the free 2-step nilpotent Lie algebra on 3 generators, then has a basis with non-trivial brackets
[TABLE]
Now, add one more generator and one extra non trivial bracket
[TABLE]
to obtain a 7-dimensional Lie algebra . Define by
[TABLE]
Again, it is obvious that is a derivation of . Define by
[TABLE]
Then for all , showing that . It is easy to see that , and so also in this case we have that .
4. Filiform nilpotent Lie algebras
In this section we determine the almost inner derivations for the classes of filiform nilpotent Lie algebras discussed in [5, Chapter 4] and for a family of characteristically nilpotent, filiform Lie algebras for introduced in [2]. We always assume that is an adapted basis, which satisfies for all .
Definition 4.1**.**
The Lie algebra for is defined by the Lie brackets
[TABLE]
The Lie algebra for even is defined by the Lie brackets
[TABLE]
The Lie algebra for is defined by the Lie brackets
[TABLE]
The Witt Lie algebra for is defined by the Lie brackets
[TABLE]
The Witt algebra also has a basis with for , which is not adapted. The derivation algebras of have been determined in [5]. Since the algebras are filiform nilpotent, we have for all classes. The dimensions of are given as follows:
[TABLE]
We have shown that in [1, Proposition ] and that
[TABLE]
in [1, Proposition ]. Here denotes the linear map which maps to and to [math] for . As a matrix, it has an entry at position and zero entries otherwise. Let . Define linear maps in by
[TABLE]
A computation shows that these linear maps are derivations of . We have the following result, see [5].
Proposition 4.2**.**
Let even. Then is a basis of .
Note that there is a mistake in the formulation and proof in [5], since the map is not taken into account although it is a derivation. It corresponds with the map of the proof, which is not zero as is claimed there. It is easy to see then that every almost inner derivation of is inner.
Proposition 4.3**.**
Let even. Then .
Proof.
Take an arbitrary , then there exist values (with ) such that
[TABLE]
Suppose that . For we have
[TABLE]
Since , we must have that .
Moreover, , but , which means that (for all ). Hence, the only almost inner derivation in is . ∎
For the Witt algebra define linear maps by
[TABLE]
We have the following result, see [5].
Proposition 4.4**.**
Let . Then is a basis of .
From this we obtain the following result.
Proposition 4.5**.**
Let . Then .
Proof.
The derivation is not almost inner, because . We need to show that are almost inner for all . Then the claim follows by Proposition 4.4. Let us write , for the coefficients appearing in the Lie brackets of . Let . Define a map by
[TABLE]
Here in since . We claim that for all , so that is almost inner. Indeed, for we have . For we also have .
For we define a map by
[TABLE]
This is well-defined for the since . We claim that for all , so that is almost inner for all . Indeed, for we have
[TABLE]
For and we have
[TABLE]
Finally, for we have
[TABLE]
For we define a map by
[TABLE]
with
[TABLE]
This is well-defined since . It is straightforward to see that for all , so that is almost inner for all . This finishes the proof. ∎
Remark 4.6*.*
For we have and for we have .
In [2] we have introduced a family of filiform nilpotent Lie algebras for . They are closely related to the Witt algebras . The Lie brackets are defined as follows:
[TABLE]
with parameters for , which are zero except for
[TABLE]
and
[TABLE]
For convenience consider the case separately. For it is easy to see that the Lie brackets of are given by
[TABLE]
where the coefficients
[TABLE]
are the same as for . This follows from the Pfaff-Saalschütz formula, see [2]. It is also easy to see that for all . Define linear maps exactly like in the case of . Note that with is not a derivation of , because
[TABLE]
so that
[TABLE]
are different for all .
Proposition 4.7**.**
Let . Then is a basis of . In particular, all derivations of are nilpotent.
Proof.
For the proof goes exactly like the proof for the Witt algebra , except that only are derivations, but not . For the claim can be verified explicitly. ∎
We obtain the remarkable result that all derivations of for are almost inner. In particular, are almost inner, but not inner.
Proposition 4.8**.**
We have for all .
Proof.
Indeed, the derivations are almost inner. For this follows in the same way as in the proof of Proposition 4.5, using the functions . These depend only on the structure constants , and all computations are also valid here. For the result can be verified directly. ∎
5. Lie algebras whose solvable radical is abelian
The aim of this section is to show that for any Lie algebra whose solvable radical is abelian, over an algebraically closed field of characteristic zero. Fix such a Lie algebra and let denote the solvable radical of , which is abelian. Then we have , where is a semisimple Lie algebra. Let and . Denote by the -module structure of . Then the Lie bracket in is given by
[TABLE]
In the sequel we will use
[TABLE]
to denote the space of -endomorphisms of . For any we define
[TABLE]
Lemma 5.1**.**
We have .
Proof.
Let and . On the one hand, we have that
[TABLE]
while on the other hand
[TABLE]
Since , it holds that (6) coincides with (7), which shows that . ∎
Proposition 5.2**.**
Let . Then as vector spaces we have that
[TABLE]
Proof.
It is easy to see that , so we have to show that . Now, consider any . The derivation induces a derivation on , which is an inner derivation, since is semisimple. So, after changing up to an inner derivation, we may assume that induces the zero map on . It follows that there exists a linear map such that for all . As is a derivation we have that
[TABLE]
And so
[TABLE]
which gives
[TABLE]
This means that is a 1–cocycle. As is semisimple, we have that and so there exists an element such that for all . Now
[TABLE]
This means that after changing again with an inner derivation we will assume that and hence there is a linear map such that
[TABLE]
Now, using the fact that is a derivation, we must have that
[TABLE]
which implies that
[TABLE]
This shows that after changing up to an inner derivation we have that which finishes the proof. ∎
We are now ready to prove the main result of this section.
Theorem 5.3**.**
Let be a Lie algebra over an algebraically closed field of characteristic zero whose solvable radical is abelian. Then .
Proof.
As before, we can write , with abelian and semisimple. We have shown that . In order to prove the result, we have to show that if a derivation is not the zero map, then is not an almost inner derivation. So consider a nonzero , then for some nonzero . Let be the image of . Then is a nonzero –submodule of . The Lie algebra contains a nilpotent element such that consists entirely of nilpotent elements, see for example [9, section ]. In particular is also nilpotent as a Lie algebra. Consider the map , where . Then is a representation of Lie algebras and since is semisimple maps nilpotent elements to nilpotent elements. It follows that consists of nilpotent endomorphisms and in particular, it follows that is strictly contained in . Let and pick an with . Note that since is semisimple, we can find a complementary –submodule of in such that decomposes as a direct sum of –modules. In particular, we also find that .
We claim that , which shows that is not an almost inner derivation. Indeed, assume that
[TABLE]
Then we have that
[TABLE]
This shows that and so . However, this now implies that which is a contradiction with the fact that we have chosen such that . ∎
6. Change of base field
Consider a field extension of . Let be a Lie algebra over and denote by the corresponding Lie algebra over . This is an extension of scalars. We will assume that has characteristic zero and that the field extension is of finite degree . The primitive element theorem ensures that for some . Then is a vector space basis of over . It follows that
[TABLE]
holds as vector spaces over . The typical example is and , where and . We can also consider as a Lie algebra over . We will denote this Lie algebra with . Note that, as sets, we have . Finally, is again a Lie algebra over .
Let us for the moment consider the special situation when . In that case we have that for some with . Hence, we can write . Now let be a Lie algebra over of dimension with basis and structure constants , so . Then has the same structure constants and the same basis. Further, has basis . Denote for all , then the structure constants are
[TABLE]
The Lie algebra has the same basis and structure constants as .
Lemma 6.1**.**
For we have .
Proof.
The Lie algebra has basis and structure constants as above. We take for a basis with
[TABLE]
Let be the linear map with and for all . Then is an isomorphism of vector spaces. Moreover, is a Lie algebra morphism. Indeed, take arbitrarily, then we have that
[TABLE]
Furthermore, also
[TABLE]
is satisfied. Finally, we find that
[TABLE]
∎
Remark 6.2*.*
Let be a Galois extension and a Lie algebra over with underlying Lie algebra . A more general result about the structure of can be found in [3].
Now, we return again to the general situation where . Suppose that , then we can consider where is the -linear map such that . This means that . Conversely, if and , then .
Remark 6.3*.*
These two “procedures” are inverses of each other. Indeed, for , we have that . Moreover, for with we have .
Lemma 6.4**.**
We have .
Proof.
We already mentioned that any derivation can be viewed as a derivation . From this, the conclusion is clear. We now show the other inclusion. Let . We can write
[TABLE]
where is a derivation for all . Take
[TABLE]
then we find that . Since also holds, this implies that . ∎
Hence, there is a nice correspondence between the derivations of and .
Lemma 6.5**.**
Let . If , then also .
Proof.
Let be a basis of over and be a derivation. Assume that , then there exists a map such that holds for all . We can write
[TABLE]
where for all . Now take an arbitrary . Then we obtain
[TABLE]
Since , it follows from equation (8) that for all ,
[TABLE]
and for all . Hence, this means that . ∎
Note that the converse of this result does not hold in general since there exist examples for which , but , see Example 7.4.
Proposition 6.6**.**
If , then also .
Proof.
Denote as before for a basis of over . Let , , then there exists a map such that for all . Furthermore, there are maps (for all ) such that
[TABLE]
Now define for each the map
[TABLE]
We claim that each is a derivation (and thus an almost inner derivation).
Let , then
[TABLE]
On the other hand, we have
[TABLE]
Since is a derivation the above equations imply that , hence for all .
Moreover, we claim that there exists at least one for which . Suppose on the contrary that for all . Then there exist such that for all . Denote . This means that
[TABLE]
for all . Now consider , then . Since two derivations of are equal when they agree on , this implies that is inner. This contradiction shows that for at least one , we have . ∎
This proposition means that if the Lie algebra over the bigger field admits a non-trivial almost inner derivation, then also the Lie algebra over the smaller field . The converse does not hold in general, see again Example 7.4.
7. Constructing new almost inner derivations
We keep using the same notations as in the previous section. In this section, we will show how to find new almost inner derivations of the Lie algebra , determined by . Remember that as a set, but now viewed as a Lie algebra over .
Define the set
[TABLE]
We will show how to construct, starting from a fixed element a collection of almost inner derivations of which are not inner, even when itself is an inner derivation of .
So fix some . Since is one-dimensional, is of codimension . Hence, for some . We also fix a choice of and let . Any element of can be written as , where and . Denote again for a basis of over , then any element can be uniquely written as with for all . We use the notation to denote the -th coordinate of with respect to the basis . We now have that . Since , there exists a map such that
[TABLE]
Associated to we introduce new -linear maps of , namely
[TABLE]
where . Note that . We remark here that the maps do depend on the choice of , so in what follows we always assume that for a given , a fixed outside of has been chosen. We can now multiply the above maps with powers of to get a total of -linear maps , with .
Lemma 7.1**.**
For any we have for all .
Proof.
First note that . Indeed, let . Because by definition, we have that and
[TABLE]
This last equation implies that and hence, is a derivation. Since is almost inner, it is determined by a map . Define
[TABLE]
For , we have that
[TABLE]
When , it follows that
[TABLE]
This shows that for all . Moreover, for each , the map is an almost inner derivation, determined by the map . ∎
In this way, each gives rise to almost inner derivations of , where .
Proposition 7.2**.**
Suppose that and define , the –vector space spanned by the maps . Then and
[TABLE]
Hence we have or .
Proof.
We will first show that the maps are –linearly independent. So assume that and that
[TABLE]
Applying the above to for some gives . As , it follows that and since is a basis of over , it follows that all coefficients , showing that the maps are –linearly independent.
Now assume that . Let and assume that for some . Note that is also -linear, since can also be seen as an inner derivation of . As above we have
[TABLE]
for every . On the other hand, since is also –linear, it must hold that and therefore we get the equality
[TABLE]
It follows that for all we have that and we let be this common value. Hence , where . So for some and therefore if and only if and if this is the case, the above shows that which finishes the proof, since as sets . ∎
In many cases, the above proposition allows us to construct Lie algebras over a non algebraically closed field with many almost inner derivations which are not inner. As an example of this we have the following result.
Corollary 7.3**.**
Let be a field extension of a field , with . Using the notation from above, assume that is a -step nilpotent Lie algebra for with , then .
Proof.
Let be an element with . Such a exists, since we assume that is –step nilpotent. Moreover . It follows that . By Proposition 7.2 we know that is an -dimensional subspace of intersecting in a -dimensional space, which proves the corollary. ∎
Note that the above corollary can for example be applied when is a filiform Lie algebra. We finish this paper with an example where and , i.e., with . Then we can take with .
Example 7.4**.**
Consider the real Heisenberg Lie algebra , then is the complex Heisenberg Lie algebra and both of these algebras can be described via a basis , where the non-zero Lie brackets are given by . Then we have
[TABLE]
It follows from Lemma 6.1 that
[TABLE]
*Let and be inner derivations of , then both .
The Lie algebra has a basis and non-zero brackets*
[TABLE]
We can now consider the –linear maps as defined above and these satisfy:
[TABLE]
We have and it is easy to see that , so that we obtain
[TABLE]
The maps do, like any other derivation, extend to derivations of , but these will no longer be almost inner derivations.
8. Acknowledgements
The first author was supported in part by the Austrian Science Fund (FWF), grant P28079 and grant I3248. The second and third author are supported by a long term structural funding, the Methusalem grant of the Flemish Government. The third author gratefully acknowledges financial support during his research stay at the Erwin Schrödinger International Institute for Mathematics and Physics in Vienna.
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