We prove that a large class of \(2\)-step solvable Lie algebras equipped with a complex structure \(J\) admits a Levi-Malcev type decomposition, adapted to \(J\). As an application, we prove that the Fino–Vezzoni conjecture holds true for \(2\)-step solvable unimodular Lie algebras. Finally, we give a structural characterisation of \(2\)-step, unimodular, completely solvable Lie algebras admitting an SKT metric.
The Levi–Malcev decomposition, see [1], [2], is a milestone in Lie theory. Said decomposition asserts that
any Lie algebra can be written as a semidirect product of a semisimple Lie subalgebra, called Levi subalgebra, and the maximal solvable ideal, called solvable radical. Thus, the Levi–Malcev decomposition elevates semisimple and solvable
Lie algebras as building blocks of any Lie algebra. These two classes have fundamental differences. While semisimple Lie algebras are classified due to the work of Killing and Cartan, the class of solvable Lie algebras is far more vast and chaotic,
resulting into fewer known structural results. On the other hand, whenever a complex structure \(J\) is defined on a Lie algebra, it often fails to be compatible with the associated Levi–Malcev decomposition, i.e. the Levi
subalgebra and the solvable radical are usually not \(J\)-invariant. This naturally raises the question on whether one can find a \(J\)-adapted version of the Levi–Malcev decomposition on a
Lie algebra endowed with a complex structure.
The main goal of the paper is to prove a \(J\)-adapted Levi–Malcev decomposition for a certain class of \(2\)-step solvable Lie algebras endowed with a complex structure.
In order to achieve the desired decomposition, we introduce the notions of solvability, semisimplicity and simplicity for a complex structure \(J\) on a Lie algebra \(\mathfrak{g}\). More
precisely, we will say that \(J\) is solvable or that \(\mathfrak{g}\) is \(J\)-solvable if the following descending series of \(J\)-invariant subalgebras terminates with \(0\): \[\mathfrak{g}^{[0]}(J):=\mathfrak{g}\,, \qquad
\mathfrak{g}^{[j+1]}(J):=[\mathfrak{g}^{[j]}(J),\mathfrak{g}^{[j]}(J)]+J[\mathfrak{g}^{[j]}(J),\mathfrak{g}^{[j]}(J)]\,,\quad j \in \mathbb{N}\,.\] Using this notion, we can define the \(J\)-solvable radical\({\rm Rad} (\mathfrak{g}, J)\) as the maximal \(J\)-solvable ideal of \(\mathfrak{g}\). Thus, we will say that \(J\) is
semisimple, and that \(\mathfrak{g}\) is \(J\)-semisimple, if \({\rm Rad}(\mathfrak{g}, J)=0\), i.e. \(\mathfrak{g}\) admits no non-trivial \(J\)-solvable ideals. Finally, we will say that \(J\) is simple, and that \(\mathfrak{g}\) is \(J\)-simple, if \(\mathfrak{g}\) is not abelian and it does not have any proper \(J\)-invariant
ideal. We remark that an analogue of \(J\)-solvability was already introduced and studied in the hypercomplex setting in [3]–[5].
With these definitions, it is very natural to wonder how far the analogy with the classical notions of solvability, semisimplicity, and simplicity for a Lie algebra can be carried. While some properties fail, other can still be established within our
\(J\)-adapted framework, although very often there are differences that complicate the scenario. For instance, it is not in general true that a \(J\)-semisimple Lie algebra is the direct sum
of \(J\)-simple ideals, see Example 29. However, we prove in Theorem 27 that such a structural result does in fact hold true when the complex structure is abelian. Recall that a complex structure \(J\) on \(\mathfrak{g}\) is called abelian if and only if \[[JX, JY]=[X, Y]\,, \qquad X, Y\in\mathfrak{g}\,.\] Abelian complex structures occur quite frequently, but only on \(2\)-step solvable Lie algebras, see [6]. Said complex structures were extensively studied in the literature, see for instance [7]–[12]. In this setting, \(J\)-semisimplicity is
equivalent to the non-degeneracy of \(B^{1,1}\)–the \((1,1)\)-part of the Killing form–which is reminiscent of Cartan’s criterion for semisimplicity, see Theorem 27.
Among other reasons, this motivates us to focus on \(2\)-step solvable Lie algebras. Within this setting a simple complex structure is necessarily abelian. We classify all \(2\)-step
solvable \(J\)-simple Lie algebras. Up to equivalence, the only examples are the Lie algebras of affine motions over the real and complex numbers: \(\mathfrak{aff}(\mathbb{R})\) and \(\mathfrak{aff}(\mathbb{C})\), see Theorem 31. Each of these is equipped with a unique simple and abelian complex structure. As a consequence, all \(J\)-semisimple Lie algebras with abelian complex structure are direct sums of copies of \(\mathfrak{aff}(\mathbb{R})\) and \(\mathfrak{aff}(\mathbb{C})\). In
particular they admit a \(\mathbb{Z}_2\)-module decomposition into two \(J\)-invariant subspaces which behaves like the Cartan decomposition of semisimple Lie algebras. Furthermore, there
exists a holomorphic involution \(s\) associated to such a decomposition that plays the role of the Cartan involution and thus, by twisting \(B^{1,1}\) with \(s\), we obtain a Hermitian metric \(B^{1,1}_s\), see Corollary 33.
With all this settled, we are able to prove a Levi-type decomposition on any Lie algebra endowed with an abelian complex structure.
Theorem 1. Let \(\mathfrak{g}\) be a Lie algebra endowed with an abelian complex structure \(J\). Then, there exists a unique \(J\)-semisimple subalgebra \(\mathfrak{h}\) of \(\mathfrak{g}\) such that \[\mathfrak{g}=\mathfrak{h}\ltimes {\rm Rad}(\mathfrak{g},
J)\,.\]
Both the existence and uniqueness part of the proof of Theorem 1 are obtained in a step-wise fashion, reducing the problem to simpler situations. The most substantial part
of the existence of the subalgebra \(\mathfrak{h}\) is carried out using a holomorphic version of the Casimir operator, a fundamental tool in the representation theory of semisimple Lie algebras, see Definition 36.
Apart from giving strong information on the structure of Lie algebras with an abelian complex structures, Theorem 1 has a pivotal role in the achievement of the desired
\(J\)-adapted Levi–Malcev decomposition. The key observation is that, for \(2\)-step solvable Lie algebras, the ideal \(\mathfrak{g}'+J\mathfrak{g}'\) always acts holomorphically on \(\mathfrak{g}'_J:=\mathfrak{g}'\cap J\mathfrak{g}'\). In particular, the latter is an ideal in the former. Its
quotient is then naturally equipped with an abelian complex structure and we can take advantage of our previous discoveries to study this case. Unfortunately, the sought-after decomposition cannot be achieved in full generality, see Example 45. However, under a suitable additional mild assumption, this expectation can indeed be fulfilled. Such an assumption is formulated in terms of the mean curvature vector,
defined as follows. Let \(\mathfrak{h}\) be the \(J\)-adapted Levi subalgebra of the quotient \((\mathfrak{g}'+J\mathfrak{g}')/\mathfrak{g}'_J\).
Then the mean curvature vector \(JU\) of \(\mathfrak{h}\) is defined by the implicit relation \[\operatorname{tr}(\operatorname{ad}^{\mathfrak{h}}_X)=B^{1,1}_{s_{\mathfrak{h}}}(JU,X)\,, \qquad X\in \mathfrak{h}\,.\] The terminology is based on [13]. In general, the mean curvature vector has a fundamental role in the study of the homogeneous Ricci flow and its solitons, see [14]–[18], due to its appearance in the formula for the Ricci curvature of a homogeneous metric, see [19]. We will regard \(JU\) as an element of \(\mathfrak{g}\) by identifying it with any representative of its equivalence class in \(\mathfrak{h}\), and we will call it the mean curvature vector of \(\mathfrak{g}\). Note that, since \(2\)-step solvability implies that \(\mathfrak{g}_J'\) is abelian, the action \(\operatorname{ad}_{JU}\vert_{\mathfrak{g}_J'}\) is well-defined.
With these preparations, we are ready to state our main result, which is the announced \(J\)-adapted version of the Levi–Malcev decomposition.
Theorem 2. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra endowed with a complex structure \(J\) and suppose that \(2\notin \mathrm{Spec}(\operatorname{ad}_{JU}\vert_{\mathfrak{g}'_J})\), where \(JU\) is the mean curvature vector of \(\mathfrak{g}\). Then, there exists a
unique \(J\)-semisimple subalgebra \(\mathfrak{h}\) of \(\mathfrak{g}\) such that \[\mathfrak{g}=\mathfrak{h}\ltimes {\rm
Rad}(\mathfrak{g}, J)\,.\]
The condition on the spectrum of \(JU\) is equivalent to the vanishing of certain cohomology, expressed via the adjoint representation induced by the mean curvature vector acting on \(\mathfrak{g}'_J\), see Definition 47 and Lemma 48. We emphasise
that when the complex structure is abelian, such additional assumption is vacuous. Thus, Theorem 2 is in fact a generalisation of Theorem 1. Although, more involved, the proof of Theorem 2 follows a similar strategy to that of Theorem 1. In this case, the most laborious situation is when \(\mathfrak{g}\) acts holomorphically on \(\mathfrak{g}_J'\). To deal with this, after further
reduction to a simpler case, the result is obtained using an operator that is completely determined by the mean curvature vector \(JU\) and the eigenvalues of \(\operatorname{ad}_{JU}|_{\mathfrak{g}_J'}\).
Our main interest in applications of Theorem 2 stems from Hermitian geometry. In particular, the \(J\)-adapted Levi–Malcev decomposition provides a
fruitful structure for identifying obstructions to the existence of certain special Hermitian metrics, as well as incompatibilities among them. For instance, we shall focus on the so-called Fino–Vezzoni conjecture. We recall here the statement:
Fino–Vezzoni Conjecture [20]: Let \((M,J)\) be a compact complex manifold. If \(M\) admits an SKT metric and a balanced metric both compatible with \(J\), then \((M,J)\) admits a Kähler metric.
Recall that a Hermitian metric \(g\) on a complex manifold \((M^n, J)\) is called SKT if its fundamental form \(\omega(\cdot, \cdot):=g(J\cdot, \cdot
)\) satisfies \(dd^c\omega=0\), where \(d^c:=J^{-1}dJ\), see [21], while \(g\) is called balanced if \(d\omega^{n-1}=0\), see [22], [23]. Many examples of SKT and balanced metrics were constructed on Lie algebras, see e.g. [9], [24]–[30]
The Fino-Vezzoni conjecture has attracted a lot of interest in the recent literature and there is plenty of partial confirmation, especially in the context of Lie algebras. Most notably, the aforementioned conjecture has been proved on nilpotent Lie
algebras in [31] and it was addressed and confirmed on certain subclasses of \(2\)-step solvable Lie algebras in [32] and on almost-abelian Lie algebras in [26]. In [32] the authors also show that in the left-invariant setting, unimodularity is a necessary condition. In [33], [34], the Fino–Vezzoni conjecture was proved to hold on semisimple Lie algebras endowed with regular complex structures, while, in [35], the conjecture is proved to be true on Lie algebras admitting a codimension 2 abelian ideal. We mention, in particular, the very recent work [36], where the conjecture is established for all compact quotients of a Lie group equipped with a left-invariant complex structure that is Chern–Ricci flat. More validations of the
aforementioned conjecture can be found in [37]–[41].
While approaching this problem on solvable Lie algebras, it is quite natural to first restrict to the \(2\)-step solvable case. We emphasise that this framework is further particularly well motivated by the classical
result of Hano, which states that left-invariant Kähler structures on unimodular Lie algebras can only be supported by \(2\)-step solvable ones [42].
Interestingly enough, the existence of a compatible SKT metric on a \(2\)-step solvable Lie algebra automatically guarantees that the hypothesis of Theorem 2 is satisfied, see Theorem 57, which thus yields a \(J\)-adapted Levi–Malcev decomposition. This piece of information
enables us to confirm the Fino–Vezzoni conjecture on all \(2\)-step solvable unimodular Lie algebras.
Theorem 3. Let \(\mathfrak{g}\) be a \(2\)-step solvable unimodular Lie algebra endowed with a complex structure \(J\). If there
exist an SKT metric and a balanced metric both compatible with \(J\), then \(J\) is solvable. In particular there exists also a Kähler metric compatible with \(J\).
The theorem is obtained in two main steps. First, we show that the semisimple part of \(\mathfrak{g}\) must vanish, hence we conclude that \(\mathfrak{g}\) is \(J\)-solvable. This step is deduced by means of the characterisation of the existence of balanced metrics in terms of currents, see [23].
Next, we show that a unimodular \(2\)-step solvable Lie algebra is \(J\)-solvable if and only if it is Chern–Ricci flat, see Proposition 59. The theorem then follows from [36].
The connection between \(J\)-solvability and Chern–Ricci flatness is interesting per se and it is exclusive of the \(2\)-step solvable case, see Example 5. On the other hand, Chern–Ricci flatness together with the existence of an SKT metric and some additional mild assumptions, yield information on the spectrum of
the adjoint representation, see Proposition 63. With this in hand, we can prove the following.
Theorem 4. Let \(\mathfrak{g}\) be a \(2\)-step, unimodular, completely solvable Lie algebra admitting an SKT metric. Then, there exists \(p\ge 0\) such that \[\mathfrak{g}=\mathfrak{aff}(\mathbb{R})^p\ltimes \mathfrak{n}_J\,,\] where \(\mathfrak{n}_J\) is the maximal \(J\)-invariant nilpotent ideal of \(\mathfrak{g}\).
The core of the proof of Theorem 4 consists in showing that a \(J\)-solvable, \(2\)-step,
unimodular, completely solvable Lie algebra admitting an SKT metric is in fact nilpotent, see Theorem 67. The result is then a consequence of Theorem 2.
For higher steps of solvability, the situation appears to be much more complicated, and from time to time we shall exhibit counterexamples to properties that hold in the \(2\)-step solvable scenario. Nevertheless, we
shall collect in Subsection 5.3 some interesting results that remain valid in this more general setting.
The paper is organised as follows. In Section 2, after recalling some necessary preliminaries, we define and study basic properties of solvable, semisimple and simple complex structures. The remainder of the section is
devoted to recalling known facts about special Hermitian metrics and the Chern–Ricci form of a Lie algebra. In Section 3 we first characterise \(J\)-semisimple Lie algebras with abelian
complex structure as direct sums of \(J\)-simple Lie algebras, and we give a classification of the latter. We then provide the proof of Theorem 1. In Section 4, we discuss the obstruction appearing in Theorem 2, together with some useful consequences. We then
present the proof of Theorem 2. Finally, Section 5 is devoted to the discussion of the proofs of Theorem 3 and Theorem 4, as well as to other properties of \(J\)-solvable Lie algebras.
Acknowledgements. The authors would like to express their deep gratitude to James Stanfield for numerous and insightful conversations and for his interest in the paper. The authors would like to thank Asia Mainenti for many inspiring
discussions over the preparation of this work. The authors would like also to thank A. Andrada, R. Arroyo, A. Fino, J. Lauret, R. Lafuente and L. Vezzoni for their interest in the present paper. The first named author would like to express his gratitude to
Andrei Moroianu and the Laboratoire de Mathématiques d’Orsay for the warm hospitality and for the pleasant stay during which the paper was concluded.
Notations. We collect here some notations that will be adopted throughout the text.
Let \(\mathfrak{g}\) be a Lie algebra, then we denote by \({\mathfrak{z}}(\mathfrak{g}):=\{ X \in \mathfrak{g}\mid \operatorname{ad}_X=0\}\) the centre of \(\mathfrak{g}\), and by \(\mathfrak{g}':=[\mathfrak{g},\mathfrak{g}]\) the commutator ideal of \(\mathfrak{g}\). Finally, \(\mathfrak{n}(\mathfrak{g})\) denotes the nilradical of \(\mathfrak{g}\), i.e. the maximal nilpotent ideal of \(\mathfrak{g}\). We will simply write \(\mathfrak{n}\) if no confusion is possible.
Let \(\mathfrak{s}\) be a subalgebra of a Lie algebra \(\mathfrak{g}\). We denote by \(C_{\mathfrak{g}}(\mathfrak{s}):=\{X\in\mathfrak{g}\,\, |\,\,
\operatorname{ad}_X\mathfrak{s}=0\}\) the centraliser of \(\mathfrak{s}\) in \(\mathfrak{g}\), and by \(N_{\mathfrak{g}}(\mathfrak{s}):=\{X \in
\mathfrak{g}\, \,|\, \, \operatorname{ad}_X\mathfrak{s}\subseteq \mathfrak{s}\}\) the normaliser of \(\mathfrak{s}\) in \(\mathfrak{g}\).
Let \(\mathfrak{s}\) be a subalgebra of a Lie algebra \(\mathfrak{g}\) equipped with a complex structure \(J\). We will use the notation \(\mathfrak{s}_J:=\mathfrak{s} \cap J\mathfrak{s}\), in particular \(\mathfrak{g}'_J:=\mathfrak{g}'\cap J\mathfrak{g}'\) and \(\mathfrak{n}_J:=\mathfrak{n}
\cap J \mathfrak{n}\).
Let \(\mathfrak{g}_1, \mathfrak{g}_2\) be Lie algebras equipped with a complex structure. If \(\mathfrak{g}_1\) and \(\mathfrak{g}_2\) are
holomorphically isomorphic we write \(\mathfrak{g}_1 \simeq \mathfrak{g}_2\).
\(B_\mathfrak{g}(X,Y):=\operatorname{tr}(\operatorname{ad}_X\operatorname{ad}_Y)\), \(X,Y\in \mathfrak{g}\), is the Cartan–Killing form of the Lie algebra \(\mathfrak{g}\). If no confusion is possible we will simply write \(B\) in place of \(B_\mathfrak{g}\).
If \(T\) is a tensor, \(T^{p,q}\) denotes the \((p,q)\)-part of \(T\) with respect to the complex structure \(J\).
We will write the signature of a symmetric bilinear form with the notation \((n_+,n_-,n_0)\), where \(n_+\) and \(n_-\) denote the number of negative
and positive eigenvalues respectively, counted with multiplicities, while \(n_0\) denotes the nullity.
Before discussing Lie algebras with a complex structure, we begin by recalling some standard definitions and facts concerning Lie algebras.
Definition 1. Let \(\mathfrak{g}\) be a Lie algebra. We say that \(\mathfrak{g}\) is
completely solvable if \({\rm Spec}(\operatorname{ad}_X)\subseteq \mathbb{R}\), for any \(X\in \mathfrak{g}\);
of real type if, for any \(X\in \mathfrak{g}\), \(\operatorname{ad}_X\) is either nilpotent or has at least one eigenvalue with non-zero real part;
of rigid type if \({\rm Spec}(\operatorname{ad}_X)\subseteq \sqrt{-1}\mathbb{R}\), for any \(X\in \mathfrak{g}\).
The following well-known result will be useful in what follows. Its proof can be found in [43].
Lemma 2. Let \(\mathfrak{g}\) be a Lie algebra and \(\mathfrak{k}\) be an ideal of \(\mathfrak{g}\). Then \(\mathfrak{n}(\mathfrak{k})=\mathfrak{n}(\mathfrak{g})\cap \mathfrak{k}.\)
In order to prove Theorem 2, we will need to define the cohomology of a Lie algebra with values in a given representation. We will just define the second degree cohomology, which will
be the most relevant for us. We refer to [43] for further details. Let \(\tau\) be a representation of \(\mathfrak{g}\) on a finite-dimensional vector space \(V\). We consider \[V^1(\mathfrak{g}, \tau):=\mathfrak{g}^*\otimes V\,, \qquad V^2(\mathfrak{g},
\tau):=\Lambda^{2}\mathfrak{g}^*\otimes V\,,\] and, for any \(L\in V^1(\mathfrak{g}, \tau)\) and \(\alpha \in V^2(\mathfrak{g}, \tau)\), we define the differential \[\begin{align}
(d_{\tau}L)(X, Y):=&\, \tau(X) L(Y)-\tau(Y)L(X)-L([X, Y])\,, \quad X,Y\in \mathfrak{g}\,,\\
(d_{\tau}\alpha)(X, Y, Z):=&\, -\sum_{{\rm cyclic}}\alpha(X, [Y, Z])+ \tau(X)\alpha(Y, Z)\,, \quad X, Y,Z \in\mathfrak{g}\,.
\end{align}\] We are now in the position to define the cohomology of \(\mathfrak{g}\) with values in \(\tau\).
Definition 3. Let \(\tau\) be a representation of a Lie algebra \(\mathfrak{g}\) on a finite-dimensional vector space \(V\). Then, the
second degree cohomology of \(\mathfrak{g}\) with values in \(\tau\) is \[H^2(\mathfrak{g}, \tau):=\frac{\ker d_{\tau}\cap V^2(\mathfrak{g},\tau)}{{\rm Im}\,
d_{\tau}\cap V^2(\mathfrak{g},\tau)}\,.\]
Next, let \(\mathfrak{g}\) be a Lie algebra endowed with a complex structure \(J\). Recall that the integrability of \(J\) is encoded by the vanishing of
the Nijenhuis tensor: \[N_J(X,Y):=[X,Y]+J[JX,Y]+J[X,JY]-[JX,JY] \equiv 0\,, \qquad X,Y\in \mathfrak{g}\,.\] Equivalently,\[\label{integrability}
[J, \operatorname{ad}_{JX}]=J[J, \operatorname{ad}_X]\,, \quad X \in \mathfrak{g}\,.\tag{1}\]
We prove here the following basic lemma.
Lemma 4. Let \(\mathfrak{g}\) be a Lie algebra endowed with a complex structure \(J\). Then \[\label{behaviourofJ2step}
[X, JY]+[JX, Y]\in \mathfrak{g}_{J}'\,, \qquad X,Y\in \mathfrak{g}\,.\qquad{(1)}\] Moreover, if \(\mathfrak{g}\) is \(2\)-step solvable, then \(\mathfrak{g}_{J}'\) is a \(J\)-invariant abelian ideal of \(\mathfrak{g}'+J\mathfrak{g}'\) and \[\label{adXg3995J}
J\operatorname{ad}_X=\operatorname{ad}_{JX}\,, \qquad X\in \mathfrak{g}'_J\,.\qquad{(2)}\] Furthermore, \[[\operatorname{ad}_{JY}, J]|_{\mathfrak{g}_{J}'}=0\,, \qquad Y\in
\mathfrak{g}'+J\mathfrak{g}'\,,\] i.e. \(\mathfrak{g}'+J\mathfrak{g}'\) acts holomorphically on \(\mathfrak{g}_J'\).
Proof. The first statement is merely a consequence of the integrability of \(J\). Since \(\mathfrak{g}\) is 2-step solvable, \(\mathfrak{g}_J'\) is clearly abelian. In order to see \(\mathfrak{g}_J'\) is an ideal of \(\mathfrak{g}'+J\mathfrak{g}'\), we observe that, since
\(\mathfrak{g}\) is \(2\)-step solvable, \([\mathfrak{g}_J', \mathfrak{g}']=0\). Hence, it is sufficient to prove \([\mathfrak{g}_J', J \mathfrak{g}']\subseteq \mathfrak{g}_J'\). On the other hand, using again \(2\)-step solvability and integrability of \(J\), for
any \(Y\in \mathfrak{g}'\) and \(X\in\mathfrak{g}_J'\) we have \([X, JY]=-J[JX, JY].\) This proves the remaining claims. ◻
The next example shows that \(\mathfrak{g}'_J\) need not be an ideal of \(\mathfrak{g}'+J\mathfrak{g}'\) when the solvability step is greater than \(2\).
Example 5. Consider the \(3\)-step solvable rigid type Lie algebra \(\mathfrak{g}=\langle e_1,\dots,e_4 \rangle\) with structure equations: \[[e_2,e_3]=-e_1\,, \qquad [e_2,e_4]=-e_3\,, \qquad [e_3,e_4]=e_2\,.\] In the notations of [44] this Lie algebra is \(\mathfrak{s}_{4,7}\). We equip \(\mathfrak{g}\) with the complex structure \[Je_1=e_4\,, \qquad Je_2=e_3\,.\] Note that \(\mathfrak{g}'_J=\langle e_2,e_3 \rangle\) is not an ideal.
In this subsection, we define the types of complex structures mentioned in the introduction and studied throughout the paper. We begin with the notion of abelian complex structures.
Definition 6. Let \(\mathfrak{g}\) be a Lie algebra endowed with a complex structure \(J\). \(J\) is called abelian if \[[JX, JY]=[X, Y]\,,\quad X, Y\in\mathfrak{g}\,.\]
We recall that a Lie algebra equipped with an abelian complex structure is necessarily 2-step solvable [6], furthermore the centre is \(J\)-invariant. Finally, \(\mathfrak{g}_J'\subseteq \mathfrak{z}(\mathfrak{g}'+J\mathfrak{g}')\). Using ?? , we notice that if \(\mathfrak{g}'_J=
0\), then \(J\) is abelian. As we will see in what follows, abelian complex structures will play a key role in our study of complex structures on \(2\)-step solvable Lie algebras.
Let \(\mathfrak{g}\) be a Lie algebra equipped with a complex structure \(J\). We define recursively the following sequences of \(J\)-invariant
subalgebras: for \(j\in \mathbb{N}\), \[\mathfrak{g}^{[0]}(J):=\mathfrak{g}\,, \qquad
\mathfrak{g}^{[j+1]}(J):=[\mathfrak{g}^{[j]}(J),\mathfrak{g}^{[j]}(J)]+J[\mathfrak{g}^{[j]}(J),\mathfrak{g}^{[j]}(J)]\,.\] We call \(\{ \mathfrak{g}^{[j]}(J) \}_{j\in \mathbb{N}}\) the \(J\)-adapted derived series of the Lie algebra \(\mathfrak{g}\). As a first difference from the classical derived series, we note that, in general, \(\mathfrak{g}^{[j]}(J)\) is only an ideal of \(\mathfrak{g}^{[j-1]}(J)\) and not of \(\mathfrak{g}\), as shown by the next example.
Example 7. Let \(\mathfrak{g}=\langle e_1,\dots,e_6 \rangle\) be the Lie algebra defined by \[[e_1,e_2]=e_1\,, \qquad [e_5,e_2]=e_3\,, \qquad [e_6,e_2]=e_4\,,\] with
complex structure \[Je_1=e_2\,, \qquad Je_3=e_4\,, \qquad Je_5=e_6\,.\] In [44] this Lie algebra is called \(\mathfrak{s}_{6,1}\). Note that \(\mathfrak{g}^{[1]}(J)=\mathfrak{g}'+J\mathfrak{g}'=\langle e_1,e_2,e_3,e_4 \rangle\) and \(\mathfrak{g}^{[2]}(J)=\langle
e_1,e_2 \rangle\), which is not an ideal of \(\mathfrak{g}\).
Once the \(J\)-adapted derived series is defined, we can define solvable complex structures as follows.
Definition 8. Let \(\mathfrak{g}\) be a Lie algebra equipped with a complex structure \(J\). We say that \(J\) is solvable if
\(\mathfrak{g}^{[j]}(J)=0\), for some \(j\in \mathbb{N}\). Moreover, we say that it is \(s\)-step solvable, or that \(s\) is the solvability step, if \(\mathfrak{g}^{[s]}(J)=0\) but \(\mathfrak{g}^{[s-1]}(J)\neq 0\). We will also say that a Lie algebra \(\mathfrak{g}\) is \(J\)-solvable if it is equipped with a solvable complex structure \(J\).
Remark 9. In [45] it has been introduced a notion of nilpotency for complex structures. Using the characterisation given in [46] it is easy to see that a nilpotent complex structure is solvable in the sense of Definition 8.
Whenever the complex structure \(J\) is not solvable, the \(J\)-adapted derived series stabilises to a non-zero subalgebra \(\mathfrak{s}\) such that
\(\mathfrak{s}=\mathfrak{s}^{[1]}(J)\). In analogy with perfect Lie algebras, we define the following class of complex structures.
Definition 10. Let \(\mathfrak{g}\) be a Lie algebra with a complex structure \(J\). If \[\mathfrak{g}=
\mathfrak{g}'+J\mathfrak{g}'\,,\] we will say that \(\mathfrak{g}\) is \(J\)-perfect. Equivalently, \(\mathfrak{g}\) is \(J\)-perfect if and only if \(\mathfrak{g}=\mathfrak{g}^{[1]}(J).\)
Obviously \(J\)-perfect Lie algebras cannot be \(J\)-solvable. We also note that such a condition has already been investigated in the literature under different terminology. For instance
in [32], \(J\)-perfect Lie algebras are called of pure type III.
We now prove some basic properties of \(J\)-solvability.
Lemma 11. Let \(\mathfrak{g}\) be a Lie algebra with a complex structure \(J\).
If \(\mathfrak{g}\) is nilpotent then \(J\) is solvable;
If \(J\) is solvable then \(\mathfrak{g}\) is solvable.
Proof. The assertion (2) is clear because the derived series of \(\mathfrak{g}\) is contained in the \(J\)-adapted one. Finally, (1) follows from the results in
[47], according to which a nilpotent Lie algebra is never \(J\)-perfect implying that the \(J\)-adapted derived series must terminate with \(0\). ◻
It is not difficult to show that \(J\)-invariant subalgebras, as well as images of \(J\)-solvable Lie algebras under holomorphic Lie algebra homomorphisms, are again \(J\)-solvable. In particular quotients of \(J\)-solvable Lie algebras by \(J\)-invariant ideals are \(J\)-solvable. Similarly to
the case of solvable Lie algebras, the following holds.
Lemma 12. Let \(\mathfrak{k}\subseteq \mathfrak{g}\) be a \(J\)-solvable ideal such that \(\mathfrak{g}/\mathfrak{k}\) is \(J\)-solvable, then \(\mathfrak{g}\) is \(J\)-solvable. Finally, the intersection and sum of \(J\)-solvable ideals is \(J\)-solvable.
Proof. Denoting with \(\pi\colon \mathfrak{g} \to \mathfrak{g}/\mathfrak{k}\) the canonical projection, we have that \(\pi(\mathfrak{g}^{[j]}(J))=(\mathfrak{g}/\mathfrak{k}
)^{[j]}(J)\) vanishes for some \(j\in \mathbb{N}\). Therefore, \(\mathfrak{g}^{[j]}(J)\subseteq \ker\pi=\mathfrak{k}\) and thus \(\mathfrak{g}^{[l+j]}(J)=(\mathfrak{g}^{[j]}(J))^{[l]}(J)\subseteq \mathfrak{k} ^{[l]}(J)=0\), for some \(l\in \mathbb{N}\). Finally, if \(\mathfrak{k}_1,\mathfrak{k}_2\) are \(J\)-solvable ideals it is obvious that \(\mathfrak{k}_1 \cap \mathfrak{k}_2\) is \(J\)-solvable. From the isomorphism \((\mathfrak{k}_1+\mathfrak{k}_2)/\mathfrak{k}_1\simeq \mathfrak{k}_2/(\mathfrak{k} _1\cap \mathfrak{k}_2)\) we note that \((\mathfrak{k}_1+\mathfrak{k}_2)/\mathfrak{k}_1\) is solvable and thus also \(\mathfrak{k}_1+\mathfrak{k}_2\) is. ◻
Since \(J\)-solvable ideals are closed under the sum the following definition is well-given.
Definition 13. Let \(\mathfrak{g}\) be a Lie algebra equipped with a complex structure \(J\). Define \({\rm Rad}(\mathfrak{g}, J)\) as
the maximal \(J\)-solvable ideal of \(\mathfrak{g}\). This ideal will be called the \(J\)-solvable radical of\(\mathfrak{g}\).
Since we are interested in working on solvable Lie algebras, we will never take into account the usual solvable radical, that is the maximal solvable ideal of a Lie algebra, therefore we shall denote \({\rm
Rad}(\mathfrak{g})\) the \(J\)-solvable radical of \(\mathfrak{g}\) with no ambiguity.
Definition 14. Let \(\mathfrak{g}\) be a Lie algebra equipped with a complex structure \(J\). We say that \(J\) is semisimple if
\(\mathfrak{g}\) admits no non-zero \(J\)-solvable ideals, i.e. \({\rm Rad}(\mathfrak{g})=0\). Furthermore, we will say that \(J\) is simple if \(\mathfrak{g}\) is not abelian and admits no proper \(J\)-invariant ideals. A Lie algebra \(\mathfrak{g}\) equipped with a simple or semisimple complex structure will be called \(J\)-simple or \(J\)-semisimple, respectively.
Let us now establish some basic properties that follow from these definitions.
Lemma 15. Let \(\mathfrak{g}\) be a Lie algebra with a complex structure \(J\). Then
if \(J\) is simple, it is semisimple and \(\mathfrak{g}\) is \(J\)-perfect;
if \(\mathfrak{g}\) is \(2\)-step solvable and \(J\) is simple, then \(J\) is abelian and \(\mathfrak{g}=\mathfrak{g}'\rtimes J \mathfrak{g}'\);
\(\mathfrak{g}/ {\rm Rad}(\mathfrak{g})\) is \(J\)-semisimple.
Proof. To prove (1), we note that if \(J\) is simple it is obviously semisimple. Moreover, \(\mathfrak{g}'+J\mathfrak{g}'\) is a \(J\)-invariant ideal of \(\mathfrak{g}\), hence we either have \(\mathfrak{g}'+J\mathfrak{g}'=0\) or \(\mathfrak{g}'+J\mathfrak{g}'=\mathfrak{g}\). In the first case we would have that \(\mathfrak{g}\) is abelian, which is not possible, deducing that \(\mathfrak{g}\) must be \(J\)-perfect.
As for (2), thanks to (1), and Lemma 4 we know that \(\mathfrak{g}_J'\) is an ideal of \(\mathfrak{g}\). Now, simplicity forces either \(\mathfrak{g}_J'=0\) or \(\mathfrak{g}_J'=\mathfrak{g}\). However, the latter cannot happen since \(\mathfrak{g}\) is solvable. Therefore, \(\mathfrak{g}_J'=0\) implying that \(J\) is abelian and \(\mathfrak{g}=\mathfrak{g}'\rtimes J \mathfrak{g}'\).
Finally, we prove (3). To any \(J\)-solvable ideal \(\mathfrak{k}\) of the quotient \(\mathfrak{g}/ {\rm Rad}(\mathfrak{g})\) corresponds a \(J\)-solvable ideal of \(\mathfrak{g}\). Therefore, the latter ideal must be contained in \({\rm Rad}(\mathfrak{g})\), implying that \(\mathfrak{k}\) is trivial in the quotient. ◻
In view of applications of Theorem 2 to special Hermitian metrics, we recall here some essential notions regarding them. We start by giving the definition of the two kinds of special
metrics we shall be interested in.
Definition 16. Let \((M^n, J)\) be a complex manifold. A Hermitian metric \(g\) is called SKT or pluriclosed if and only if \(dd^c\omega=0\), where \(\omega\) is the associated fundamental form. On the other hand \(g\) is called balanced if and only if \(d\omega^{n-1}=0\).
In order to address the Fino–Vezzoni conjecture, it is useful to have at our disposal characterisations of the existence of balanced and SKT metrics. In particular, we will use the following criterion for the existence of balanced metrics expressed in
terms of currents due to Michelsohn [23].
Theorem 17. Let \((M, J)\) be a compact complex manifold. Then, \((M, J)\) does not admit any balanced metrics if and only if there exists a \(d\)-exact current with non-zero and positive \((1,1)\)-part.
We will exclusively be concerned in the case in which our manifold \(M\) is a quotient of a Lie group by a co-compact lattice endowed with a left-invariant complex structure. In this setting, we can adopt the
symmetrisation technique [48] and infer that the existence of balanced or SKT metrics on \(M\) is equivalent to the existence of
a left-invariant one [30], [49]. This allows to reduce the problem of studying such metrics at the Lie algebra
level. For this reason, unless otherwise stated, we will henceforth work exclusively on Lie algebras. Within this framework, in Theorem 17 compactness can be replaced with
unimodularity. Furthermore, we will only need the following simplified version of one implication. For the readers’ convenience we provide a proof.
Corollary 18. Let \(\mathfrak{g}\) be a unimodular Lie algebra equipped with a complex structure \(J\). If \(\mathfrak{g}\) admits a
\(d\)-exact, non-zero, and semi-positive \((1,1)\)-form, then it does not carry any balanced metrics.
Proof. Let \(\alpha=d\gamma\) be a non-zero and semi-positive \((1,1)\)-form, and assume by contradiction that \(\mathfrak{g}\) admits a
compatible balanced metric, with fundamental form \(\omega\). Then, if \(\dim(\mathfrak{g})=2n\), \[0=d\omega^{n-1}\wedge \gamma =d(\omega^{n-1}\wedge
\gamma)+\omega^{n-1}\wedge d\gamma=\omega^{n-1}\wedge \alpha\,,\] where we used that every \((2n-1)\)-form is closed, thanks to unimodularity. This would imply that \(\alpha=0\),
against our assumption, hence \(\mathfrak{g}\) cannot carry balanced metrics. ◻
Also, for future purposes, it will be useful to write down explicitly the SKT condition. The identity is well-known, see e.g. [50], [51], therefore we omit the proof.
Lemma 19. Let \(\mathfrak{g}\) be a Lie algebra with a complex structure \(J\). A Hermitian metric \(g\) on \(\mathfrak{g}\) is SKT if and only if \[\begin{align}
0&=g([J[X, JX], JY], JY)+g([J[X, JX], Y],Y)+2g([Y,JY],[X, JX])\\
&\quad +g([J[X, Y], X], JY)-g([J[X, Y], Y], JX)-g([J[X, JY], X], Y)\\
&\quad -g([J[X, JY], JY],JX)+g([J[JX, Y], JX], JY)+g([J[JX, Y], Y],X)\\
&\quad -g([J[JX, JY], JX], Y)+g([J[JX, JY], JY], X)+g([J[Y, JY], JX], JX)\\
&\quad +g([J[Y, JY], X], X)-|[X, Y]|^2-|[X, JY]|^2-|[JX, Y]|^2-|[JX, JY]|^2\,,
\end{align}\] for all \(X,Y\in \mathfrak{g}\).
Along our treatment it will become apparent that many structural properties of the Lie algebras taken into account are strictly tied to the curvature of the Chern connection. For this reason, we recall the expression of the first Chern–Ricci
form for Hermitian metrics on a given Lie algebra.
Proposition 20 ([52]). Let \(\mathfrak{g}\) be a Lie algebra with a complex structure \(J\). The Chern–Ricci form \(\rho\) of any left-invariant metric on \(\mathfrak{g}\) can be expressed as \[\rho(X, Y)=-\frac{1}{2}{\rm
tr}(J\operatorname{ad}_{[X, Y]})+\frac{1}{2}{\rm tr}(\operatorname{ad}_{J[X, Y]})\,, \qquad X, Y\in \mathfrak{g}\,.\] In particular, \(\rho\) does not depend on the choice of the metric, and \(\rho=d\sigma\), where \(\sigma\) is the Koszul form* defined as \[\sigma(X):=\frac{1}{2}\mathrm{tr}(J
\operatorname{ad}_X)-\frac{1}{2}\mathrm{tr}(\operatorname{ad}_{JX})\,, \qquad X\in \mathfrak{g}\,.\]*
For future reference, we also denote with \(\eta\) the following form: \[\label{defn95eta}
\eta(X, Y):=-\frac{1}{2}\operatorname{tr}(J\operatorname{ad}_{[X, Y]})\,, \qquad X,Y\in\mathfrak{g}\,.\tag{2}\] It is clear that if \(\mathfrak{g}\) is unimodular then \(\rho=\eta\). We observe that, as for \(\rho\), the form \(\eta\) is again \(d\)-exact. Indeed, \(\eta=d\beta\) with \[\label{eqn95beta}
\beta(X):=\frac{1}{2}{\rm tr}(J\operatorname{ad}_X)\,, \qquad X\in \mathfrak{g}\,.\tag{3}\] It will also be useful for future purposes to have the following alternative expression for \(\eta\).
Lemma 21. Let \(\mathfrak{g}\) be a Lie algebra endowed with a complex structure \(J\). Then, \[\label{form95ricci}
\eta(X, JX)=-\frac{1}{4}{\rm tr}([J,{\rm ad}_{JX}]^2)\,, \qquad X\in \mathfrak{g}\,.\qquad{(3)}\]
Proof. We have \[{\rm tr}(J{\rm ad}_{[X, JX]})=
-{\rm tr}([J, {\rm ad}_{JX}]{\rm ad}_{X})={\rm tr}([J, {\rm ad}_{JX}]J[J,{\rm ad}_{X}])+ {\rm tr}([J, {\rm ad}_{JX}]J{\rm ad}_XJ)\,.\] On the other hand, \[{\rm tr}([J, {\rm ad}_{JX}]J{\rm ad}_XJ)={\rm tr}(-{\rm
ad}_{JX}J{\rm ad}_{X}+ {\rm ad}_{JX}{\rm ad}_{X}J )={\rm tr}(J[{\rm ad}_{JX},{\rm ad}_{X}])=-\operatorname{tr}(J\operatorname{ad}_{[X,JX]})\,,\] which in particular, using 1 , gives \[\eta(X,JX)=-\frac{1}{4}{\rm tr}([J, {\rm ad}_{JX}]J[J,{\rm ad}_{X}])=-\frac{1}{4}{\rm tr}([J, {\rm ad}_{JX}]^2)\,,\] as claimed. ◻
We conclude the section with the following interesting fact.
Lemma 22. Let \(\mathfrak{g}\) be a unimodular Lie algebra endowed with a complex structure \(J\). Then, any balanced Hermitian metric is Chern-scalar flat.
Proof. By Proposition 20 we know that \(\rho=d \sigma\). Now, given a balanced metric \(\omega\), we have \[s^{{\rm Ch}}(\omega)\frac{\omega^n}{n!}=\rho\wedge \frac{\omega^{n-1}}{(n-1)!}=d\sigma\wedge \frac{\omega^{n-1}}{(n-1)!}=0\] using that \(d\omega^{n-1}=0\) and unimodularity. ◻
Given a \(2\)-step solvable Lie algebra \(\mathfrak{g}\), we have seen in Lemma 4 that \(\mathfrak{g}'_J:=\mathfrak{g}'\cap J\mathfrak{g}'\) is always an ideal of \(\mathfrak{g}'+J\mathfrak{g}'\). Hence, we can consider the quotient \((\mathfrak{g}'+J\mathfrak{g}')/\mathfrak{g}_J'\) which yields a Lie algebra with abelian complex structure. With this in mind, we proceed with our investigation by studying abelian complex structures.
The following simple lemma supplies us with a very useful identity that we will use repeatedly.
Lemma 23. Let \(\mathfrak{g}\) be a Lie algebra endowed with an abelian complex structure \(J\). Then \[\label{penis}
\operatorname{ad}_Y\operatorname{ad}_X+\operatorname{ad}_{JX}\operatorname{ad}_{JY}=\operatorname{ad}_{J[JX, Y]}\,, \qquad X, Y \in \mathfrak{g}\,.\qquad{(4)}\]
Proof. By simply using Jacobi identity and abelianity of \(J\), we have that \[\operatorname{ad}_{JX}\operatorname{ad}_{JY}=-\operatorname{ad}_{JX}\operatorname{ad}_YJ=-\operatorname{ad}_{[JX,
Y]}J-\operatorname{ad}_Y\operatorname{ad}_{JX}J=\operatorname{ad}_{J[JX,Y]}-\operatorname{ad}_Y\operatorname{ad}_X\,,\] as claimed. ◻
By means of ?? , we are able to prove the following result, whose importance will become clear quickly.
Proposition 24. Let \(\mathfrak{g}\) be a Lie algebra endowed with an abelian complex structure \(J\). Then,
\(\mathfrak{n}_J\) is a \(J\)-invariant ideal, i.e. \(\mathfrak{n}_J\) is the maximal \(J\)-invariant nilpotent
ideal of \(\mathfrak{g}\);
\(B^{1,1}(JX , Y)=-\eta(X, Y)\), for any \(X, Y\in\mathfrak{g}\), and so it is \(d\)-exact;
for any \(Z\in \mathfrak{n} , X, Y\in\mathfrak{g}\), we have \[B^{1,1}([JZ, X], Y)=B^{1,1}([JZ, Y], X)\,, \qquad B^{1,1}([Z, X], Y)=B^{1,1}(J[Z, JY], X)\,;\]
if \(\mathfrak{g}=\mathfrak{n} +J\mathfrak{n}\), then \(\ker \eta=\ker B\cap J \ker B =\mathfrak{n}_J\);
if \(\mathfrak{g}=\mathfrak{n} +J\mathfrak{n}\) and \(\mathfrak{k}\) is a \(J\)-invariant ideal of \(\mathfrak{g}\), then \(\mathfrak{k} ^{\perp}\) is a \(J\)-invariant ideal, where \((\cdot)^{\perp}\) is the orthogonal
complement with respect to \(B^{1,1}\). Furthermore, \(B_{\mathfrak{k}}^{1,1}=B^{1,1}\vert_{\mathfrak{k}\times \mathfrak{k}}\).
Proof. Most of the proposition hinges on the identity ?? . Up to complexification, we can use Lie’s Theorem and assume that \(\operatorname{ad}_Z\) is upper triangular for all \(Z\in\mathfrak{g}\), after choosing a suitable basis of \(\mathfrak{g}\). Now, take \(X \in\mathfrak{n}_J\). Then \(\operatorname{ad}_X\) and \(\operatorname{ad}_{JX}\) are strictly upper triangular. For any \(Y\in \mathfrak{g}\), this forces \(\operatorname{ad}_Y\operatorname{ad}_X\), \(\operatorname{ad}_{JX}\operatorname{ad}_{JY}\), and hence also \(\operatorname{ad}_{J[JX, Y]}\), to be strictly upper
triangular, and thus nilpotent. Thanks to this \(J[JX, Y]\in \mathfrak{n}\) and consequently \([JX, Y]\in\mathfrak{n}_J\), proving that \(\mathfrak{n}_J\) is
an ideal. The last part of (1) is straightforward.
As for (2), we use ?? again. Indeed, for any \(X,Y\in \mathfrak{g}\), \[B^{1,1}(JX , Y)=\frac{1}{2}{\rm
tr}(\operatorname{ad}_{JX}\operatorname{ad}_Y-\operatorname{ad}_{X}\operatorname{ad}_{JY})=-\frac{1}{2}{\rm tr}(\operatorname{ad}_{J[X, Y]})=\frac{1}{2}{\rm tr}(J\operatorname{ad}_{[X, Y]})=-\eta(X,Y)=-d\beta(X,Y)\,,\] where \(\beta\) is the form defined in 3 , which proves the claim.
To show (3), we exploit the closure of \(\eta\). First of all, we notice that \(B^{1,1}(\mathfrak{n}, J \mathfrak{n})=0\), since \(\mathfrak{n}
\subseteq \ker B\). Now, let \(X, Y\in\mathfrak{g}\) and \(Z\in\mathfrak{n}\), we have \[0=d\eta(JX,JY, Z)=B^{1,1}(J[JX, JY], Z)-B^{1,1}(J[JX, Z],
JY)+B^{1,1}(J[JY, Z], JX)\,.\] Using that \([JX, JY]\in\mathfrak{n}\), we get \[0=-B^{1,1}([JX, Z], Y)+B^{1,1}([JY, Z], X)=B^{1,1}([X, JZ], Y)-B^{1,1}([Y, JZ], X)\,,\] which implies
\[B^{1,1}([JZ, X], Y)=B^{1,1}([JZ, Y], X)\,,\] as claimed. On the other hand, \[B^{1,1}([Z, X], Y)=B^{1,1}([JZ, JX], Y)=B^{1,1}([JZ, Y], JX)=B^{1,1}(J[Z, JY], X)\,,\] concluding the proof
of (3).
As for (4), we observe that \(\ker B\cap J \ker B\subseteq \ker \eta\,.\) Viceversa, fix \(X\in \ker \eta\) and \(Y\in \mathfrak{n}\). By
expanding the relation \(\eta(X, Y)=0\) in terms of \(B\), using part (2), we obtain \(B(X, JY)=0.\) Together with \(\mathfrak{n} \subseteq \ker B\), this implies that \(X\in \ker B\). On the other hand, expanding \(\eta(X, JY)=0\), we get \(B(JX,
JY)=0\,,\) which yields \(JX\in \ker B\). Thus \(X \in \ker B \cap J \ker B\), giving \(\ker B \cap J \ker B =\ker \eta\). Finally, to show that \(\ker \eta = \mathfrak{n}_J\), let \(X\in \ker \eta\) and write \(X=Z+JY\), where \(Y, Z\in \mathfrak{n}\). It follows that \(JY\in \ker B\). Thus, we have \[{\rm tr}(\operatorname{ad}_{JY}^2)=0\,.\] We shall prove that \({\rm tr}(\operatorname{ad}_{JY}^{k+1})=0\) for all \(k\ge 2\). Using ?? , we infer \[\begin{align}
\operatorname{ad}_{JY}^{k+1}=\operatorname{ad}_{JY}^{k-1}\operatorname{ad}_{J[JY, Y]}-\operatorname{ad}_{JY}^{k-1}\operatorname{ad}_Y^2\,.
\end{align}\] Now, \(\operatorname{ad}_Y\) is nilpotent. Hence, as above, \(\operatorname{ad}_{JY}^{k-1}\operatorname{ad}_Y^2\) is nilpotent and therefore \[{\rm tr}(\operatorname{ad}_{JY}^{k+1})={\rm tr}(\operatorname{ad}_{JY}^{k-1}\operatorname{ad}_{J[JY, Y]})\,.\] Applying ?? once again, we obtain \[\operatorname{ad}_{JY}^{k-1}\operatorname{ad}_{J[JY,
Y]}=\operatorname{ad}_{JY}^{k-2}\operatorname{ad}_{J[JY,[JY, Y]]}-\operatorname{ad}_{JY}^{k-2}\operatorname{ad}_{[JY, Y]}\operatorname{ad}_Y\,,\] and thus \[{\rm tr}(\operatorname{ad}_{JY}^{k+1})
={\rm tr}(\operatorname{ad}_{JY}^{k-2}\operatorname{ad}_{J[JY,[JY, Y]]})\,.\] Iterating this process, we eventually obtain \[{\rm tr}(\operatorname{ad}_{JY}^{k+1})={\rm
tr}(\operatorname{ad}_{JY}\operatorname{ad}_{J[JY,[JY, \cdots [JY, Y]]\cdots]})=0\,,\] since \(JY\in \ker B\). This ultimately leads to the fact that \(\operatorname{ad}_{JY}\) is
nilpotent, and hence \(\operatorname{ad}_{X}\) is nilpotent, proving that \(\ker \eta \subseteq \mathfrak{n}\). On the other hand, since clearly \(J \ker \eta =\ker
\eta\), we deduce that \(\ker \eta \subseteq \mathfrak{n}_J\). Conversely, it is well-known that \(\mathfrak{n} \subseteq \ker B\) and so \(\mathfrak{n}_J\subseteq \ker B \cap J \ker B=\ker \eta\).
Finally, we prove (5). Let \(\mathfrak{k}\) be a \(J\)-invariant ideal of \(\mathfrak{g}\). Being \(B^{1,1}\) of
type \((1,1)\) guarantees straightforwardly that \(\mathfrak{k} ^{\perp}\) is \(J\)-invariant. Let \(X\in \mathfrak{k}\),
\(Y\in \mathfrak{k} ^{\perp}\) and \(Z\in \mathfrak{g}\) and write \(Z=Z'+JZ''\) with \(Z',Z''\in
\mathfrak{n}\). Thus, applying part (3), we get \[\begin{align}
B^{1,1}([Z,Y ], X)&=B^{1,1}([Z',Y ], X)+B^{1,1}([JZ'',Y], X)=B^{1,1}(J[Z',JX],Y)+B^{1,1}([JZ'', X],Y)=0\,,
\end{align}\] since \(\mathfrak{k}\) is a \(J\)-invariant ideal. This concludes the first part of (5). The second part is a trivial consequence of the facts that \(B_{\mathfrak{k} }=B_{\mathfrak{g} }|_{\mathfrak{k}\times \mathfrak{k}}\) and that \(J\mathfrak{k} =\mathfrak{k}\). ◻
An important class of Lie algebras admitting abelian complex structures is that of affine Lie algebras, see [8], [11]. In what follows, we will be interested only in those affine Lie algebras constructed from commutative and associative \(\mathbb{R}\)-algebras.
Definition 25. Let \(A\) be a finite-dimensional, commutative and associative \(\mathbb{R}\)-algebra. The affine Lie algebra \(\mathfrak{aff}(A)\) is \(A\oplus A\) with Lie bracket given by \[[(a, b), (a', b')]:=(0, ab'-a'b)\,, \quad a, b, a', b'\in A\,,\] and
complex structure defined by \(J(a, b):=(b, -a)\).
It is straightforward to notice that if \(\mathfrak{g}=\mathfrak{aff}(A)\), for some finite-dimensional, commutative and associative \(\mathbb{R}\)-algebra \(A\), then \(\mathfrak{g}_J'=0\).
We prove the following basic lemma which will be useful later.
Lemma 26. Let \(A\) and \(A'\) be finite-dimensional, commutative and associative \(\mathbb{R}\)-algebras.
Any subalgebra of \(A\) induces a \(J\)-invariant subalgebra of \(\mathfrak{aff}(A)\). Any ideal of \(A\) induces
a \(J\)-invariant ideal of \(\mathfrak{aff}(A).\)
Any \(J\)-perfect subalgebra of \(\mathfrak{aff}(A)\) corresponds to a subalgebra of \(A\). Any \(J\)-perfect
ideal of \(\mathfrak{aff}(A)\) corresponds to an ideal of \(A\).
Assume \(A=S\oplus I\), where \(I\) is an ideal and \(S\) is a subalgebra of \(A\). Then \(\mathfrak{aff}(A)= \mathfrak{aff}(S)\ltimes \mathfrak{aff}(I)\).
Let \(\varphi\colon A \to A'\) be a homomorphism of \(\mathbb{R}\)-algebras. Then there exists \(\mathfrak{aff}( \varphi )\colon \mathfrak{aff}(A)\to
\mathfrak{aff}(A')\) holomorphic Lie algebra homomorphism such that \(\ker \mathfrak{aff}(\varphi)=\mathfrak{aff}(\ker \varphi)\). In particular, if \(\varphi\) is an isomorphism,
then \(\mathfrak{aff}( \varphi)\) is a holomorphic isomorphism.
Let \(I\) be an ideal of \(A\). Then \(\mathfrak{aff}(A/I)\simeq \mathfrak{aff}(A)/\mathfrak{aff}(I).\)
Proof. We start with (1). Let \(S\) be a subalgebra of \(A\) and consider \(\mathfrak{aff}(S)\subseteq \mathfrak{aff}(A)\). Since \(S\) is a subalgebra, we have that, for any \(X=(a, b), Y=(a', b')\in\mathfrak{aff}(S)\) with \(a,b,a',b'\in S\), \[[X,
Y]=(0, ab'-a'b)\in \mathfrak{aff}(S)\,,\] which implies that \(\mathfrak{aff}(S)\) is a subalgebra of \(\mathfrak{aff}(A)\), which is clearly \(J\)-invariant. The statement for ideals follows from the same arguments.
As for (2), we fix a \(J\)-perfect subalgebra \(\mathfrak{s}\) of \(\mathfrak{aff}(A)\). We consider \(S:=p_2\mathfrak{s}'\subseteq A\), where \(p_2\colon \mathfrak{aff}(A)\to A\) is the projection onto the second factor. Now, fix \(a, b\in S\), then there
exist \(X,Y\in \mathfrak{s}'\) such that \(X=(0,a)\) and \(Y=(0,b)\). Then, \[\mathfrak{s}'\ni[JY,X]=(0,ab)\,,\]
which shows that \(ab\in S\). We conclude that \(S\) is a subalgebra of \(A\).
Now, we prove (3). Using (1), \(\mathfrak{aff}(S)\) and \(\mathfrak{aff}(I)\) are, respectively, a \(J\)-invariant subalgebra and a
\(J\)-invariant ideal of \(\mathfrak{aff}(A)\). The claim then follows from the assumption that \(A=S\oplus I\).
To prove (4), we consider \[\mathfrak{aff}( \varphi):=\varphi \oplus \varphi\colon \mathfrak{aff}(A)\to \mathfrak{aff}(A')\,, \quad \mathfrak{aff}(\varphi)(a, b):=(\varphi(a), \varphi(b))\,.\] Using the
definition of the bracket and the complex structure on affine Lie algebras, it is straightforward to check that \(\mathfrak{aff}(\varphi)\) is a holomorphic Lie algebra homomorphism. Now, \(\ker
\mathfrak{aff}( \varphi)=\ker \varphi\oplus \ker \varphi= \mathfrak{aff}(\ker \varphi)\), as claimed.
Finally, by (4), the projection onto the quotient \(\pi\colon A\to A/I\) induces a holomorphic Lie algebra homomorphism \(\mathfrak{aff}( \pi)\colon \mathfrak{aff}(A)\to
\mathfrak{aff}(A/I)\) such that \(\ker \mathfrak{aff}(\pi)=\mathfrak{aff}(\ker \pi)=\mathfrak{aff}(I)\). On the other hand, since \(I\) is an ideal, (1) implies that \(\mathfrak{aff}(I)\) is a \(J\)-invariant ideal of \(\mathfrak{aff}(A)\), hence we may consider the canonical projection onto the quotient \(\pi'\colon \mathfrak{aff}(A)\to \mathfrak{aff}(A)/\mathfrak{aff}(I)\). Since \(\ker \pi'=\ker\mathfrak{aff}( \pi)\) and \(\mathfrak{aff}( \pi)\) is
surjective, we can find a holomorphic isomorphism \(f\colon \mathfrak{aff}(A)/\mathfrak{aff}(I)\to \mathfrak{aff}(A/I)\) such that \(\mathfrak{aff}( \pi)=f\pi'\), which proves the
claim. ◻
We discovered in Proposition 24 that, on Lie algebras of the form \(\mathfrak{g}=\mathfrak{n}+ J\mathfrak{n}\) endowed with an abelian
complex structure, the kernel of \(B^{1,1}\) is an ideal. With this piece of knowledge it becomes possible to characterise non-degeneracy of \(B^{1,1}\) as follows.
Theorem 27. Let \(\mathfrak{g}\) be a Lie algebra with an abelian complex structure \(J\). Then the following are equivalent
\(J\) is semisimple;
\(B^{1,1}\) is non-degenerate and \(\mathfrak{g}=\mathfrak{n}(\mathfrak{g})\oplus J\mathfrak{n}(\mathfrak{g})\) as vector spaces;
\(\mathfrak{g}\) is the direct sum of \(J\)-simple ideals \(\mathfrak{k}_i\).
In particular, if any of the above holds, \(\mathfrak{g}=\mathfrak{g}'\rtimes J\mathfrak{g}'\) and \(J\)-invariant ideals and quotients of \(\mathfrak{g}\) are \(J\)-semisimple.
Proof. Assume that (1) holds. By Proposition 24, part (1), we have \(\mathfrak{n}(\mathfrak{g})_J=0\). Set
\(\mathfrak{k}=\mathfrak{n}(\mathfrak{g})\oplus J \mathfrak{n}(\mathfrak{g})\) and consider \(\mathfrak{k}^{\perp}\), where \((\cdot)^{\perp}\) denotes the
orthogonal complement with respect to \(B^{1,1}\). Clearly, \(\mathfrak{k}^{\perp}\) is \(J\)-invariant. Applying Lemma 2, we obtain \(\mathfrak{k}=\mathfrak{n}(\mathfrak{k})\oplus J\mathfrak{n}(\mathfrak{k})\) and, Proposition 24, part (4), gives \(\mathfrak{k} \cap \mathfrak{k}^{\perp}=\ker B^{1,1}_{\mathfrak{k}}= \mathfrak{n}(\mathfrak{k})_J=0\). Now, since \(d\eta=0\)
and \(\mathfrak{k}\) is an ideal, for any \(X, Y \in\mathfrak{k}^{\perp}\) and \(Z\in\mathfrak{k}\) we have \[\label{detauguale0}
0=d\eta(X, Y, Z)=B^{1,1}(J[X, Y], Z)-B^{1,1}(J[X, Z], Y)+B^{1,1}(J[Y, Z], X)=B^{1,1}(J[X, Y], Z)\,,\tag{4}\] which implies \([X, Y]\in\mathfrak{k}^{\perp}\cap \mathfrak{k} =0\). Hence \(\mathfrak{k}^{\perp}\) is abelian. Instead, choosing \(X\in\mathfrak{k}^{\perp}, Y, Z \in\mathfrak{n}(\mathfrak{g})\) and using Proposition 24, part (3), we deduce \[B^{1,1}([JZ, X], Y)=B^{1,1}([JZ, Y], X)=0\,, \quad B^{1,1}([Z, X], Y)=B^{1,1}(J[Z, JY], X)=0\,,\] since \([JZ, Y], J[Z,
JY]\in\mathfrak{k}\). This allows us to infer that \([\mathfrak{k}^{\perp}, \mathfrak{k} ]\subseteq \mathfrak{k}^{\perp}\cap \mathfrak{k}=0.\) Using 4 again, but now with \(X\in\mathfrak{k} ^{\perp}\), \(Y\in\mathfrak{g}\) and \(Z\in\mathfrak{k}\), we conclude that \(\mathfrak{k}^{\perp}\) is a \(J\)-invariant abelian ideal of \(\mathfrak{g}\). By semisimplicity, this forces \(\mathfrak{k}^{\perp}=0\). In particular, \(\ker
B^{1,1}\subseteq \mathfrak{k}^{\perp}=0\), which implies that \(B^{1,1}\) is non-degenerate. Since \(B^{1,1}_{\mathfrak{k}}\) is also non-degenerate we deduce that \(\mathfrak{g}=\mathfrak{n}(\mathfrak{g})\oplus J\mathfrak{n}(\mathfrak{g})\) and (2) follows.
Assume now that (2) holds. We adapt the proof of [53] to prove (3). If \(\mathfrak{g}\) has no proper \(J\)-invariant ideals, the claim is immediate. Let us assume that \(\mathfrak{g}\) has a proper \(J\)-invariant ideal, hence we can consider the minimal non-zero
\(J\)-invariant ideal \(\mathfrak{k}\). By Lemma 2 and the minimality of \(\mathfrak{k}\), we obtain \(\mathfrak{k}=\mathfrak{n}(\mathfrak{k} )\oplus J \mathfrak{n}(\mathfrak{k} )\). By Proposition 24, part (5), we know that \(\mathfrak{k} ^{\perp}\) is a \(J\)-invariant ideal. Moreover, \(\mathfrak{k}\cap
\mathfrak{k}^{\perp}=\ker B_{\mathfrak{k}}^{1,1}=\mathfrak{n}(\mathfrak{k})_J=0\), thanks to Proposition 24, part (4), and the fact that \(\mathfrak{n}(\mathfrak{g})_J=0\). In particular, \(\mathfrak{g} =\mathfrak{k} \oplus \mathfrak{k}^{\perp}\) as a Lie algebra. Now observe that, if \(\mathfrak{l}
\subseteq \mathfrak{k}\) is a \(J\)-invariant ideal, then \([\mathfrak{l} , \mathfrak{k}^{\perp}]\subseteq \mathfrak{k}\cap \mathfrak{k} ^{\perp}=0\), so \(\mathfrak{l}\) is also a \(J\)-invariant ideal of \(\mathfrak{g}\). By the minimality of \(\mathfrak{k}\), it follows that \(\mathfrak{l}\) is either \(0\) of \(\mathfrak{k}\). Hence, \(\mathfrak{k}\) is \(J\)-simple.
For the same reason, any \(J\)-invariant ideal of \(\mathfrak{k}^{\perp}\) is also a \(J\)-invariant ideal of \(\mathfrak{g}\). Therefore, \(\mathfrak{n}(\mathfrak{k}^{\perp})_J=0\) and \(\mathfrak{k}^{\perp}=\mathfrak{n}( \mathfrak{k}^{\perp})\oplus J\mathfrak{n}(
\mathfrak{k}^{\perp})\). To see the last equality, fix \(X=N+JN'\in \mathfrak{k}^{\perp}\), for some \(N, N'\in\mathfrak{n}(\mathfrak{g})\) and \(Y\in \mathfrak{n}(\mathfrak{k} )\). Since \(B^{1,1}(\mathfrak{n}(\mathfrak{g}), J\mathfrak{n}(\mathfrak{g} ))=0\), we infer \[0=B^{1,1}(X, Y)=B^{1,1}(N, Y)+
B^{1,1}(JN', Y)=B^{1,1}(N, Y)\,.\] Thus, \(N\in (\mathfrak{n}(\mathfrak{k} )\oplus J\mathfrak{n}(\mathfrak{k}))^{\perp}=\mathfrak{k}^{\perp}\). From this, it follows that \(\mathfrak{k}^{\perp}\subseteq \mathfrak{n}(\mathfrak{k}^{\perp})\oplus J\mathfrak{n}(\mathfrak{k}^{\perp})\). Therefore, \(B^{1,1}_{\mathfrak{k} ^{\perp}}\) is non-degenerate, using Proposition
24 part (1) and (4). We can then repeat the procedure on \(\mathfrak{k}^\perp\) and conclude after finitely many steps.
Finally, assume (3), namely \[\mathfrak{g}=\bigoplus_{i=1}^{k}\mathfrak{k}_i\,,\] where \(\mathfrak{k}_i\) is a \(J\)-simple ideal of \(\mathfrak{g}\). Of course, for any \(i=1, \ldots, k\), the projection \(\pi_i\colon \mathfrak{g} \to \mathfrak{k}_i\) is a holomorphic Lie algebra homomorphism.
Hence, if \(\mathfrak{k}\subseteq \mathfrak{g}\) is a \(J\)-invariant ideal of \(\mathfrak{g}\), then \(\pi_i(\mathfrak{k}
)\) is a \(J\)-invariant ideal of \(\mathfrak{k}_i\). Therefore, \(\pi_i(\mathfrak{k} )\) is either \(0\) or \(\mathfrak{k}_i\). If \(\pi_i(\mathfrak{k})=\mathfrak{k}_i\) then \(\mathfrak{k}_i\subseteq \mathfrak{k} .\) Indeed, \[\mathfrak{k}_i'=[\mathfrak{k}_i, \mathfrak{k}_i]_{\mathfrak{k}_i}=[\mathfrak{k}_i, \pi_i(\mathfrak{k} )]_{\mathfrak{k}_i}=[\mathfrak{k}_i, \mathfrak{k} ]\subseteq \mathfrak{k}\,.\] Since \(\mathfrak{k}\) is \(J\)-invariant and \(\mathfrak{k}_i\) is \(J\)-simple, hence \(J\)-perfect,
we also have \(\mathfrak{k}_i=\mathfrak{k}_i'\rtimes J\mathfrak{k}_i'\subseteq \mathfrak{k}\). Consequently, \[\mathfrak{k}=\bigoplus_{\mathfrak{k}_i\subseteq \mathfrak{k}
}\mathfrak{k}_i\,.\] But now, it is clear that \(\mathfrak{k}\) cannot be \(J\)-solvable unless \(\mathfrak{k}=0\).
In addition, \[\mathfrak{g}'=\left[\mathfrak{g}, J\mathfrak{g} \right]=\bigoplus_{i=1}^k[\mathfrak{k}_i, J \mathfrak{k}_i]=\bigoplus_{i=1}^k \mathfrak{k}_i'\,.\] Therefore, \[\mathfrak{g}'\rtimes J \mathfrak{g}'=\bigoplus_{i=1}^k\mathfrak{k}_i'\rtimes J\mathfrak{k}_i'=\mathfrak{g} \,,\] showing that \(\mathfrak{g}\) is \(J\)-perfect. ◻
Proposition 28. Let \(\mathfrak{g}\) be a Lie algebra endowed with a semisimple abelian complex structure \(J\). Then the group \({\rm
Aut}(\mathfrak{g} , J)\) of holomorphic automorphisms of \(\mathfrak{g}\) is discrete. As a consequence, \(\mathfrak{g}\) has no holomorphic vectors.
Proof. It is known that every \(D\in {\rm Der}(\mathfrak{g} )\) satisfies \(D\mathfrak{g}\subseteq \mathfrak{n}\). If \(D\in {\rm Der}(\mathfrak{g} ,
J):=\{D\in {\rm Der}(\mathfrak{g}) \,\, |\, \, DJ =JD\}\), then \(D\mathfrak{g} \subseteq \mathfrak{n} _J=0\), due to semisimplicity of \(\mathfrak{g}\). Hence, \(D=0\), meaning that \({\rm Der}(\mathfrak{g}, J)=\{0\}\). The claim now follows from the well-known fact that \({\rm Der}(\mathfrak{g}, J)={\rm Lie}({\rm
Aut}(\mathfrak{g}, J))\). Finally, if \(X \in \mathfrak{g}\) is a holomorphic vector field, then \(\operatorname{ad}_X\in {\rm Der}(\mathfrak{g}, J)\), which implies \(X\in \mathfrak{z}(\mathfrak{g})\). On the other hand, the centre of \(\mathfrak{g}\) is a \(J\)-invariant abelian ideal, so \(X=0\). ◻
Let \(\mathfrak{g}\) be a \(J\)-perfect and \(J\)-semisimple, 2-step solvable Lie algebra. Then either \(\mathfrak{g}'_J=0\) or \(\mathfrak{g}'_J=\mathfrak{g}\). The second case cannot occur, because \(\mathfrak{g}\) is solvable. Therefore \(\mathfrak{g}\) is a direct sum of \(J\)-simple ideals by Theorem 27. However, the next example shows that if \(\mathfrak{g}\) is not \(J\)-perfect then it might not have such structure. This is in striking contrast with the classical fact that a semisimple Lie algebra is always the direct sum of simple
ideals.
Example 29. Consider the \(2\)-step solvable Lie algebra \(\mathfrak{g}=\langle e_1,e_2,e_3,e_4,e_5,e_6\rangle\) with only non trivial brackets: \[[e_1,e_5]=[e_2,e_6]=[e_3,e_4]=e_4\,, \qquad [e_3,e_5]=e_5\,, \qquad [e_3,e_6]=e_6\,.\] and complex structure given by \[Je_1=e_2\,, \quad Je_3=e_4\,,\quad Je_5=e_6\,.\] As a Lie algebra, \(\mathfrak{g}\) is isomorphic to \(\mathfrak{s}_{6,182}\) in the notation of [44]. It is fairly easy
to see that \(\mathfrak{g}'+J\mathfrak{g}'=\langle e_3,e_4,e_5,e_6 \rangle\) is the only non-trivial \(J\)-invariant ideal of \(\mathfrak{g}\).
However, \(\mathfrak{g}'+J\mathfrak{g}'\) is \(J\)-perfect and therefore cannot be \(J\)-solvable, implying that \(\mathfrak{g}\) is \(J\)-semisimple, even though \(J\) is not abelian.
Also, let us observe that when the solvability step is higher than \(2\) a \(J\)-simple Lie algebra might have degenerate \(B^{1,1}\). Indeed, Example 5 is easily checked to be \(J\)-simple, however \[B^{1,1}=-\left( e^1\otimes e^1 + e^4 \otimes
e^4\right)\,,\] in particular, \(\ker(B^{1,1})=\langle e_2,e_3 \rangle\).
In view of Theorem 27, we now turn our attention to the study of \(J\)-simple \(2\)-step solvable Lie
algebras \(\mathfrak{g}\). We will fully classify them, with two different proofs: the first of a more Lie-theoretic flavour while the second of a more algebraic flavour. Let us introduce the candidates before stating the
theorem itself.
Example 30. The Lie algebra of affine motions of \(\mathbb{R}\) is denoted by \(\mathfrak{aff}(\mathbb{R})\) and it is the unique non-abelian, solvable \(2\)-dimensional Lie algebra: \[[JX, X]=X\,.\] One can easily see that, being \(\mathfrak{aff}(\mathbb{R})\) completely solvable, \(B^{1,1}>0\) and hence \(-\eta\) is an exact Kähler metric on \(\mathfrak{aff}(\mathbb{R})\).
The Lie algebra of affine motions of \(\mathbb{C}\) will be denoted by \(\mathfrak{aff}(\mathbb{C})\) and it is the \(4\)-dimensional Lie algebra defined
by the following structure equations: \[[JX, X]=X, \quad [JX, Y]=[JY, X]=Y, \quad [JY, Y]=-X.\] Thanks to the classification in [54], \(\mathfrak{aff}(\mathbb{C})\) is the unique \(4\)-dimensional non-completely solvable Lie algebra admitting an abelian complex structure. Moreover, one
can easily verify that \(B^{1,1}\) in this case has signature \((2, 2,0)\). We note that \(\mathfrak{aff}(\mathbb{C})\) also carries another, non-equivalent,
abelian complex structure which is solvable, see e.g. [7]. Finally, it is easy to see that \(\mathfrak{aff}(\mathbb{C})\) cannot
carry any SKT metric.
Throughout the paper, whenever we write \(\mathfrak{aff}(\mathbb{R})\) and \(\mathfrak{aff}(\mathbb{C})\) we shall intend them as Lie algebras equipped with the respective abelian complex
structures defined here.
The next theorem gives the full classification of \(J\)-simple \(2\)-step solvable Lie algebras.
Theorem 31. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra endowed with a simple complex structure \(J\). Then, either
\(\mathfrak{g} \simeq \mathfrak{aff}(\mathbb{R})\) or \(\mathfrak{g} \simeq \mathfrak{aff}(\mathbb{C})\).
Proof. Let us begin observing that, since \(\mathfrak{g}\) is \(2\)-step solvable, the family \(\{\operatorname{ad}_{JV}|_{\mathfrak{g}'}\}_{V\in
\mathfrak{g}'}\) consists of commuting operators. Therefore, we can find \(Z\in\mathfrak{g}'\otimes \mathbb{C}\) which is a common eigenvector of \(\{\operatorname{ad}_{JW}|_{\mathfrak{g}'\otimes \mathbb{C}}\}_{W\in\mathfrak{g}' \otimes \mathbb{C}}\), i.e., for any \(W\in \mathfrak{g}' \otimes \mathbb{C}\),
\[\label{common}
[JW,Z ]=\lambda(W)Z\,, \qquad \lambda\in(\mathfrak{g}'\otimes \mathbb{C})^*\,.\tag{5}\] Hence, in particular, we obtain \[\label{commonZ}
[JZ, Z]=\lambda(Z)Z\,.\tag{6}\] Now, we have two possibilities: either \(Z\in\mathfrak{g}'\) or \(Z\) is genuinely complex. Let us assume that \(Z\in\mathfrak{g}'\). This allows us to infer that \[\mathfrak{k}_1 := \langle Z, JZ\rangle\] is a non-zero \(J\)-invariant ideal of \(\mathfrak{g}\). By hypothesis, \(\mathfrak{k}_1 = \mathfrak{g}.\) Moreover, \(\lambda(Z)\ne 0\) otherwise \(\mathfrak{g}\) would
be abelian against simplicity of \(J\). Hence, up to renormalisation, we can suppose that \(\lambda (Z)=1\) which gives straightforwardly that \(\mathfrak{g} \simeq
\mathfrak{aff}(\mathbb{R})\). It remains to understand the case in which \(Z\) is complex. Let us write \(Z=X+\sqrt{-1}Y\), with \(X,
Y\in\mathfrak{g}'\). From 5 , it follows that, for any \(V\in \mathfrak{g}'\), \[\label{affc} [JV,
X]=\lambda_1(V)X-\lambda_2(V)Y\,, \qquad [JV, Y]=\lambda_2(V)X+ \lambda_1(V)Y\,,\tag{7}\] where \(\lambda_1=\mathrm{Re}(\lambda)\) and \(\lambda_2=\operatorname{Im}(\lambda)\).
This, in particular, guarantees that \[\mathfrak{k}_2:= \langle X, Y, JX, JY \rangle\] is a non-zero \(J\)-invariant ideal of \(\mathfrak{g}\) forcing \(\mathfrak{k}_2 =\mathfrak{g}\), by \(J\)-simplicity. Next, we show that \(\mathfrak{g}\simeq \mathfrak{aff}(\mathbb{C}).\) Applying 7 to
\(X\) and \(Y\), we get \[\label{hiddeneqaffC} \begin{align} \relax [JY, Y]=&\,\lambda_2(Y)X+\lambda_1(Y)Y\,, \qquad
[JY, X]=\lambda_1(Y)X- \lambda_2(Y)Y\\ [JX, Y]=&\, \lambda_2(X)X+\lambda_1(X)Y\,, \qquad [JX, X]=\lambda_1(X)X- \lambda_2(X)Y\,. \end{align}\tag{8}\]
Now, since \(J\) is abelian then \([JY, X]=[JX, Y]\), hence \(\lambda_2(X)=\lambda_1(Y)\) and \(\lambda_1(X)=-\lambda_2(Y)\), guaranteeing that \([JY, Y]=-[JX, X].\) Rewriting 6 using these relations shows that \(\lambda(Z)=
2\lambda(X)\). Therefore, \(\lambda(Z)\ne 0\), since otherwise \(\lambda_1(X)=\lambda_2(X)=0\) and \(\mathfrak{g}\) would be abelian, against the fact
that \(J\) is simple. Then, up to renormalisation, we can assume \(\lambda(X)=1\). Thus, we can rewrite 8 as \[[JY, Y]=-X\,, \quad
[JY, X]=Y\,, \quad [JX, Y]=Y\,, \quad [JX, X]=X\,,\] which yields the desired isomorphism. ◻
Remark 32. As anticipated, Theorem 31 can be proved in a more algebraic manner. Thanks to [8], any Lie algebra \(\mathfrak{g} = \mathfrak{g}'\rtimes J\mathfrak{g}'\) endowed with an abelian complex structure is holomorphically isomorphic to \(\mathfrak{aff}( A)\), where \(A\) is a finite-dimensional, associative, commutative \(\mathbb{R}\)-algebra, see Definition 25. In our hypotheses, the algebra \(A\) is given by \(A=(\mathfrak{g}', \cdot)\) with \[X\cdot Y:=[JX,
Y]\,, \qquad X, Y\in \mathfrak{g}'\,.\] Hence, if \(\mathfrak{g}=\mathfrak{g}'\rtimes J \mathfrak{g}'\) is \(J\)-simple, then the algebra \(A\) is simple, using Lemma 26, part (1). Therefore, we can use Artin-Wedderburn Theorem, see [55], and Frobenius’ Theorem, see for instance [56], which imply that the only simple, commutative and
associative \(\mathbb{R}\)-algebras are either \(\mathbb{R}\) or \(\mathbb{C}\), yielding the desired claim.
The next result provides an analogue of the Cartan decomposition of a real semisimple Lie algebra in our context, see [53].
Corollary 33. Let \(\mathfrak{g}\) be a Lie algebra endowed with a semisimple abelian complex structure \(J\). Then, there exist \(p, q\ge
0,\)\(p+q\ge 1\) such that \[\label{sssss}
\mathfrak{g}=\mathfrak{aff}(\mathbb{R})^p\oplus \mathfrak{aff}(\mathbb{C})^q\,.\qquad{(5)}\] In particular
there exists a \(J\)-invariant subalgebra \(\mathfrak{g}_+\) and a \(J\)-invariant subspace \(\mathfrak{g}_-\)
such that \[\mathfrak{g}=\mathfrak{g}_+\oplus \mathfrak{g}_-\,,\quad [\mathfrak{g}_+, \mathfrak{g}_+]\subseteq \mathfrak{g}_+ \,, \quad [\mathfrak{g}_+, \mathfrak{g}_-]\subseteq \mathfrak{g}_-\,, \quad [\mathfrak{g}_-,
\mathfrak{g}_-]\subseteq \mathfrak{g}_+\,.\] As a consequence, there exists an involution \(s \in {\rm Aut}(\mathfrak{g} , J)\) such that \(B_s^{1,1}(X, Y):=B^{1,1}(X, sY)\) defines a
Hermitian metric.
\(\operatorname{ad}_{JX}^{t_s}=\pm \operatorname{ad}_{JX}\), for all \(X\in \mathfrak{g}_{\pm}\cap \mathfrak{g}'\), where \((\cdot)^{t_s}\)
denotes the transpose with respect to \(B^{1,1}_s\).
Proof. By Theorem 27 and Theorem 31 we immediately infer ?? .
To prove (1), we observe that for \(\mathfrak{aff}(\mathbb{R})\) and \(\mathfrak{aff}(\mathbb{C})\) we may choose \[\begin{align}
\qquad \qquad \mathfrak{aff}(\mathbb{R})_+&= \mathfrak{aff}(\mathbb{R}) \,, &\mathfrak{aff}(\mathbb{R})_-&= 0 \,,\qquad \qquad \\
\mathfrak{aff}(\mathbb{C})_+&= \langle X,JX \rangle \,, & \mathfrak{aff}(\mathbb{C})_-&= \langle Y, JY \rangle \,,
\end{align}\] where we retain the notations of Example 30. It is easy to check that these subspaces satisfy the desired Lie bracket relations. Hence, thanks to ?? , it suffices to
choose \[\mathfrak{g}_+:=\mathfrak{aff}(\mathbb{R})^p\oplus \mathfrak{aff}(\mathbb{C})_+^q\,, \qquad \mathfrak{g}_-:=\mathfrak{aff}(\mathbb{C})_-^q\,.\] Furthermore, we define \[s|_{\mathfrak{g}_+}={\rm Id}_{\mathfrak{g}_+}\,, \quad s|_{\mathfrak{g}_-}=-{\rm Id}_{\mathfrak{g}_-}\,.\] Due to the bracket relations above and that \(J\mathfrak{g}_{\pm}=\mathfrak{g}_{\pm}\), we obtain \(s\in {\rm Aut}(\mathfrak{g}, J)\), and clearly \(s^2={\rm Id}\). Next, it is easy to see that \(B^{1,1}_s\) is of type \((1,1)\), since \([s, J]=0\). Moreover, using again that \([s, J]=0\) and \(s\in \mathrm O(B)\), we have, for any \(X, Y\in\mathfrak{g}\), \[\begin{align}
B^{1,1}_s(X, Y)= \frac{1}{2}\left(B(X, sY)+ B(JX, JsY)\right)
=\frac{1}{2}\left(B(Y, sX)+ B(JY, JsX)\right)=B^{1,1}_s(Y, X)\,,
\end{align}\] giving us that \(B_s^{1,1}\) is symmetric. To see positive definiteness, we note that the decomposition of \(\mathfrak{g}\) in \(J\)-simple ideals is orthogonal with respect to \(B_s^{1,1}\). Hence, it is sufficient to prove the claim on each \(J\)-simple ideal. Since \(B_{\mathfrak{aff}(\mathbb{R})}^{1,1}>0\) and \(s_{\mathfrak{aff}(\mathbb{R})}={\rm Id}\), it is enough to prove the statement on \(\mathfrak{aff}(\mathbb{C})\), for which it is easy to see that \[\qquad \, B^{1,1}_{\mathfrak{aff}(\mathbb{C})}|_{\mathfrak{aff}(\mathbb{C})_+\times \mathfrak{aff}(\mathbb{C})_+}>0\,,\quad
B^{1,1}_{\mathfrak{aff}(\mathbb{C})}|_{\mathfrak{aff}(\mathbb{C})_+\times \mathfrak{aff}(\mathbb{C})_-}=0\,, \quad B^{1,1}_{\mathfrak{aff}(\mathbb{C})}|_{\mathfrak{aff}(\mathbb{C})_-\times \mathfrak{aff}(\mathbb{C})_-}<0\,.\] Since \(s|_{\mathfrak{aff}(\mathbb{C})_-}=-{\rm Id}\), the claim follows straightforwardly.
As for (2), we have that, using Proposition 24, part (3), for any \(X\in \mathfrak{g}_{\pm}\cap \mathfrak{g}'\),
\[\begin{align}
B^{1,1}_s(\operatorname{ad}_{JX} Y, Z)=&\,
B^{1,1}(Y, \operatorname{ad}_{JX}sZ)
= B^{1,1}(Y, s\operatorname{ad}_{JsX}Z)=\pm B^{1,1}_s(Y, \operatorname{ad}_{JX}Z)\,,
\end{align}\] concluding the proof. ◻
With this settled, whenever a Lie algebra \(\mathfrak{g}\) is endowed with a semisimple and abelian complex structure \(J\), then, thanks to ?? , we can introduce the following basis of
\(\mathfrak{g}\), which we call standard: \[\label{baseincredibile}
\mathcal{B}:=\{X_1, JX_1, \ldots,X_p, JX_p, X_{p+1}, JX_{p+1}, \ldots, X_{p+q}, JX_{p+q}, Y_{p+1},JY_{p+1}, \ldots, Y_{p+q}, JY_{p+q}\}\,,\tag{9}\] where \(\{X_1, JX_1, \ldots, X_{p+q}, JX_{p+q}\}\) is a basis
of \(\mathfrak{g}_+\) whereas \(\{Y_{p+1},JY_{p+1}, \ldots, Y_{p+q}, JY_{p+q}\}\) is a basis of \(\mathfrak{g}_-\) such that \(\langle X_i, JX_i\rangle\simeq \mathfrak{aff}(\mathbb{R})\) for any \(i=1,\ldots, p\), and \(\langle X_{p+j}, JX_{p+j}, Y_{p+j}, JY_{p+j}\rangle\simeq
\mathfrak{aff}(\mathbb{C})\) for any \(j=1, \ldots, q\).
3.3 Levi–Malcev decomposition for abelian complex structures↩︎
In this subsection we will prove Theorem 1. Before proceeding, we introduce two tools that will be useful in what follows.
Definition 34. Let \(\mathfrak{g}\) be a Lie algebra endowed with a semisimple abelian complex structure \(J\). The mean curvature vector\(JU\) of \((\mathfrak{g}, B^{1,1}_s)\) is defined implicitly by: \[{\rm tr}(\operatorname{ad}_X)=B_s^{1,1}(JU, X)\,, \quad X \in \mathfrak{g}\,.\]
The terminology is standard, see e.g. [13]. In the next result we collect some properties of the mean curvature vector in our setting.
Lemma 35. Let \(\mathfrak{g}\) be a Lie algebra endowed with a semisimple, abelian complex structure \(J\). Then \[JU=2\sum_{i=1}^{\dim_{\mathbb{C}}\mathfrak{g}_+}JX_i\,,\] where \(\{X_1, \ldots, X_{\dim_{\mathbb{C}}\mathfrak{g}_+}\}\) is the basis of \(\mathfrak{g}_+\cap
\mathfrak{g}'\) contained in the standard basis \(\mathcal{B}\). Hence, \([JU, U]=2U\) and, more generally, \[\label{ad95JU2Id}\operatorname{ad}_{JU}|_{\mathfrak{g}'}=2{\rm Id}_{\mathfrak{g}'}\,.\qquad{(6)}\] Finally, if \(\varphi\colon \mathfrak{g}_1\to \mathfrak{g}_2\) is a holomorphic
isomorphism of \(J\)-semisimple Lie algebras with abelian complex structure, then \(\varphi(JU_{\mathfrak{g}_1})=JU_{\mathfrak{g}_2}.\)
Proof. First of all, we define \(JY:=2\sum_{i=1}^{\dim_{\mathbb{C}}\mathfrak{g}_+}JX_i\) and, using the bracket relations of the vectors in the basis \(\mathcal{B}\), we infer
that \(\operatorname{ad}_{JY}|_{\mathfrak{g}'}=2{\rm Id}_{\mathfrak{g}'}\). To prove the first claim, we observe that, for any \(X\in \mathfrak{g}'\), \(B_{s}^{1,1}(JY, X)=0\). Using the fact that \(JY\in\mathfrak{g}_+\) and ?? we deduce \[B_s^{1,1}(JY, JX)=\frac{1}{2} {\rm tr}(\operatorname{ad}_{J[JY, X]})={\rm
tr}(\operatorname{ad}_{JX})\,,\] thereby proving the first three statements.
The last claim is proved by straightforward computations once we observe that \(\varphi s_{\mathfrak{g}_1 }\varphi^{-1}=s_{\mathfrak{g}_2 }\), which follows from \(\varphi((\mathfrak{g}_1)
_{\pm})=(\mathfrak{g}_2)_{\pm}\). This property can be deduced, for instance, using the basis 9 and the fact that \(\varphi\) is a Lie algebra isomorphism. ◻
Next, we introduce an operator which will help us to obtain the desired Levi–Malcev decomposition.
Definition 36. Let \(\mathfrak{g}\) be a Lie algebra endowed with a semisimple abelian complex structure \(J\). The \(J\)-adapted
Casimir operator is defined as \[\Omega^{1,1}_{\mathfrak{g}}:=\frac{1}{2}(\operatorname{ad}_{JU}-J\operatorname{ad}_{U})\in{\rm End}(\mathfrak{g}, J)\,.\]
Remark 37. We now justify the name of \(\Omega_{\mathfrak{g}}^{1,1}.\) To this end, we consider the standard basis \(\mathcal{B}\) defined in 9 and we notice that, for any \(i=1, \ldots, p\) and \(j=1, \ldots, q\), \[B^{1,1}(X_i,X_i)=\frac{1}{2}\,,\quad B^{1,1}(X_{p+j},
X_{p+j})=-B^{1,1}(Y_{p+j}, Y_{p+j})=1\,.\] Hence, the dual basis of \(\mathcal{B}\) with respect to \(B^{1, 1}\), see [53], is given by \[\tilde{\mathcal{B}}:=\{2X_1, 2JX_1, \ldots,2X_{p}, 2JX_p, X_{p+1}, JX_{p+1}, \ldots, X_{p+q}, JX_{p+q}, -Y_{p+1},-JY_{p+1}, \ldots, -Y_{p+q}, -JY_{p+q}\}\,.\] By ?? and
the explicit expressions for the Lie brackets of elements in \(\mathcal{B}\), the Casimir operator \(\Omega_{\mathfrak{g}}\) takes the form \[\begin{align}
\Omega_{\mathfrak{g}}=&\, \sum_{i=1}^pB^{1,1}(X_i, X_i)(\operatorname{ad}^2_{2X_i}+\operatorname{ad}_{2JX_i}^2)+ \sum_{j=1}^{q}B^{1,1}(X_{p+j},
X_{p+j})(\operatorname{ad}_{X_{p+j}}^2+\operatorname{ad}_{JX_{p+j}}^2-\operatorname{ad}_{Y_{p+j}}^2-\operatorname{ad}_{JY_{p+j}}^2)\\
=&\, 2\left(\sum_{i=1}^p\operatorname{ad}_{JX_i}+\sum_{j=1}^q\operatorname{ad}_{JX_{p+j}}\right)=\operatorname{ad}_{JU}\,.
\end{align}\] Hence, \[\Omega_{\mathfrak{g}}^{1,1}=\frac{1}{2}(\Omega_{\mathfrak{g}}-J\Omega_{\mathfrak{g}}J)\,.\]
Moreover, it turns out that \(\Omega^{1,1}_\mathfrak{g}\) coincides with the identity operator on \(\mathfrak{g}\). Indeed, by ?? , we have that \(J\operatorname{ad}_U|_{J\mathfrak{g}' }=-2{\rm Id}_{J\mathfrak{g}'}\). Hence, \(\Omega_{\mathfrak{g}}^{1,1}={\rm Id}_{\mathfrak{g}}\), since \(\mathfrak{g}\) is \(J\)-perfect.
Before presenting the proof of Theorem 1, we give the following definition and prove a general lemma that will be used later.
Definition 38. Let \(\mathfrak{g}\) be a Lie algebra endowed with a complex structure \(J\). We call a \(J\)-invariant subalgebra \(\mathfrak{h}\) of \(\mathfrak{g}\) a \(J\)-adapted Levi subalgebra of \(\mathfrak{g}\) if \[\mathfrak{g}=\mathfrak{h}\ltimes {\rm Rad}(\mathfrak{g})\,.\]
From Lemma 15 it is evident that a \(J\)-adapted Levi subalgebra is necessarily \(J\)-semisimple as it is
holomorphically isomorphic to \(\mathfrak{g}/ {\rm Rad}(\mathfrak{g})\).
Lemma 39. Let \(\mathfrak{g}\) be a Lie algebra endowed with a complex structure \(J\). Let \(\mathfrak{k}_1, \mathfrak{k}_2\subseteq
\mathfrak{g}\) be two \(J\)-invariant ideals such that \(\mathfrak{k}_1\subseteq \mathfrak{k}_2\) such that \(\mathfrak{k}_2'+J\mathfrak{k}_2'\subseteq \mathfrak{k}_1\) and \(\mathfrak{g}'_J \subseteq {\rm Rad}(\mathfrak{k}_2)\). Then \[{\rm
Rad}(\mathfrak{k}_1)={\rm Rad}(\mathfrak{k}_2)\cap \mathfrak{k}_1\,, \qquad \mathfrak{k}_2=\mathfrak{k}_1+ {\rm Rad}(\mathfrak{k}_2)\,.\]
Proof. From the inclusion \(\mathfrak{k}_1\subseteq \mathfrak{k}_2\), we deduce that \({\rm Rad}(\mathfrak{k}_2)\cap\mathfrak{k}_1\) is a \(J\)-solvable ideal of \(\mathfrak{k}_1\). Hence, \({\rm Rad}(\mathfrak{k}_2)\cap \mathfrak{k}_1\subseteq {\rm Rad}(\mathfrak{k}_1)\). On the other hand, \[\frac{\mathfrak{k}_1}{{\rm Rad}(\mathfrak{k}_2)\cap \mathfrak{k}_1}\simeq\frac{\mathfrak{k}_1 + {\rm Rad}(\mathfrak{k}_2)}{{\rm Rad}(\mathfrak{k}_2)}\,,\] which is a \(J\)-invariant ideal of
\(\mathfrak{k}_2/{\rm Rad}(\mathfrak{k}_2)\) and thus \(J\)-semisimple, due to the assumption \(\mathfrak{g}'_J \subseteq {\rm Rad(\mathfrak{k}_2)}\) and
Theorem 27. Therefore, \[0={\rm Rad}\left(\frac{\mathfrak{k}_1}{{\rm Rad}(\mathfrak{k}_2)\cap \mathfrak{k}_1}\right)=\frac{{\rm
Rad}(\mathfrak{k}_1)}{{\rm Rad}(\mathfrak{k}_2)\cap \mathfrak{k}_1},\] concluding that \({\rm Rad}(\mathfrak{k}_1 )={\rm Rad}(\mathfrak{k}_2)\cap \mathfrak{k}_1\). As for the second identity, note that the quotient
\[\frac{\frac{\mathfrak{k}_2}{{\rm Rad}(\mathfrak{k}_2)}}{\frac{\mathfrak{k}_1 + {\rm Rad}(\mathfrak{k}_2)}{{\rm Rad}(\mathfrak{k}_2)}} \simeq \frac{\mathfrak{k}_2}{\mathfrak{k}_1+{\rm Rad}(\mathfrak{k}_2)}\]is \(J\)-semisimple and abelian, since \(\mathfrak{k}_2'+J\mathfrak{k}_2'\subseteq \mathfrak{k}_1\). This can only happen if \(\mathfrak{k}_1 + {\rm
Rad}(\mathfrak{k}_2)=\mathfrak{k}_2\). ◻
Remark 40. We notice that if \(J\) is abelian then \(\mathfrak{g}'_J \subseteq {\rm Rad}(\mathfrak{g})\). Indeed, \(\mathfrak{g}'_J
\subseteq \mathfrak{z}(\mathfrak{g}'+J\mathfrak{g}')\) and \(\mathfrak{z}(\mathfrak{g}'+J\mathfrak{g}')\) is a \(J\)-invariant abelian ideal of \(\mathfrak{g}\), and as such, it is contained in \({\rm Rad}(\mathfrak{g})\).
We can now establish the \(J\)-adapted Levi-Malcev decomposition in the particular case when \(\mathfrak{g}'_J=0\) which is later extended to arbitrary abelian complex structures.
Theorem 41. Let \(\mathfrak{g}=\mathfrak{a}\rtimes J\mathfrak{a}\) be a Lie algebra with an abelian complex structure \(J\) such that \(\mathfrak{a}\) is an abelian ideal and \(\mathfrak{g}_J'=0\). Then there exists a unique \(J\)-invariant subalgebra \(\mathfrak{h}\) such that \[\mathfrak{g}= \mathfrak{h}\ltimes\mathfrak{n}_J\,.\]
Proof. Using [8], we know that \(\mathfrak{g}\simeq \mathfrak{aff}(A)\) for some finite-dimensional, associative and
commutative \(\mathbb{R}\)-algebra \(A\). Using the Wedderburn’s Principal Theorem, see [55],
we can write \[A=J\oplus S\, ,\] where \(J\) is the Jacobson radical and \(S\) is a semisimple subalgebra of \(A\) such
that \(S\simeq A/J\), see [55]. On the other hand, using the finite dimensionality of \(A\) as
an \(\mathbb{R}\)-algebra, we have that \(J=N\), where \(N\) is the nilradical of \(A\), i.e. the maximal ideal consisting
of nilpotent elements. Therefore, \[A=N \oplus S\,.\] Once we have this, we can use Lemma 26, part (3), to infer \[\mathfrak{g}\simeq \mathfrak{aff}(A)=\mathfrak{aff}(N\oplus S)= \mathfrak{aff}(N)\ltimes \mathfrak{aff}(S)\,.\] Since \(S\) is semisimple, \(\mathfrak{aff}(S)\)
is the direct sum of \(J\)-simple ideals by Lemma 26, part (3), and hence \(J\)-semisimple by Theorem
27. On the other hand, using [57], we have that \(\mathfrak{aff}(N)\) is a \(J\)-invariant nilpotent ideal, consequently \(\mathfrak{aff}(N)\subseteq \mathfrak{n}_J\). Since \(\mathfrak{aff}(S)\simeq \mathfrak{aff}(A/N)\) is \(J\)-semisimple, we conclude \(\mathfrak{aff}(N)=\mathfrak{n}_J\).
We now prove the uniqueness part of the statement. Let us assume that there exist two \(J\)-adapted Levi subalgebras \(\mathfrak{h}_1, \mathfrak{h}_2\) of \(\mathfrak{g}\). Using the fact that \(\mathfrak{h}_i\) is \(J\)-perfect and Lemma 26, part (2), we know that there exist a subalgebra \(S_i\subseteq A\) such that \(\mathfrak{h}_i=\mathfrak{aff}(S_i)\), for any \(i=1,2\). Thanks to Lemma 26, part (3), and since \(\mathfrak{aff}(N)=\mathfrak{n}_J\), we deduce that
\(A=S_1\oplus N=S_2\oplus N\). Now, we can apply [55] to conclude that there exists \(n\in N\)
such that \(S_1=(1-n)S_2(1-n)^{-1}\). We obtain \(S_1=S_2\) by commutativity of \(A\). The claim now follows. ◻
With this established, we can now prove Theorem 1.
Theorem 42. Let \(\mathfrak{g}\) be a Lie algebra equipped with an abelian complex structure \(J\). Then there exists a unique \(J\)-invariant subalgebra \(\mathfrak{h}\) such that \[\mathfrak{g}= \mathfrak{h}\ltimes {\rm Rad}(\mathfrak{g})\,.\]
Proof. We prove the existence part of the theorem in a stepwise fashion by successively reducing to simpler cases.
Step 1. We show that we may assume that \(\mathfrak{g}\) has no \(J\)-invariant ideals properly contained in \({\rm Rad}(\mathfrak{g})\).
To prove this we work inductively on \(\dim_\mathbb{C}(\mathfrak{g})\). If \(\mathfrak{g}\) is \(1\)-dimensional, it can only be either \(\mathfrak{aff}(\mathbb{R})\) or \(\mathbb{C}\) and in both cases the theorem is clearly true. Thus, let \(\mathfrak{k} \subset {\rm Rad}(\mathfrak{g})\) be a
\(J\)-invariant ideal in \(\mathfrak{g}\). Since \(\mathrm{Rad}(\mathfrak{g}/\mathfrak{k})={\rm Rad}(\mathfrak{g})/\mathfrak{k}\), by the inductive
assumption we have \(\mathfrak{g}/\mathfrak{k} = \mathfrak{s} \ltimes {\rm Rad}(\mathfrak{g})/\mathfrak{k}\), for some \(J\)-semisimple subalgebra \(\mathfrak{s}\). Consider now the canonical projection onto the quotient \(\pi \colon \mathfrak{g}\to \mathfrak{g}/\mathfrak{k}\), then \(\hat{\mathfrak{s}}:=
\pi^{-1}(\mathfrak{s})\) is a proper \(J\)-invariant subalgebra of \(\mathfrak{g}\) and so, by the inductive assumption again, it can be written as \(\hat{\mathfrak{s}}= \mathfrak{h}\ltimes \mathrm{Rad}(\hat{\mathfrak{s}})\) for a \(J\)-semisimple subalgebra \(\mathfrak{h}\). Since \(\hat{\mathfrak{s}}/\mathfrak{k}=\pi(\pi^{-1}(\mathfrak{s}))= \mathfrak{s}\) is \(J\)-semisimple, it follows that \(\mathrm{Rad}(\hat{\mathfrak{s}})\subseteq
\mathfrak{k}\), but \(\mathfrak{k}\subseteq {\rm Rad}(\mathfrak{g})\) is \(J\)-solvable and thus we must have \(\mathfrak{k}=
\mathrm{Rad}(\hat{\mathfrak{s}})\). It then follows that \(\mathfrak{g}= \mathfrak{h}\ltimes {\rm Rad}(\mathfrak{g})\).
Step 2. We reduce here to the case where \(\mathfrak{g}=\mathfrak{g}'+J\mathfrak{g}'\). Using Lemma 39 with \(\mathfrak{k}_1=\mathfrak{g}'+J\mathfrak{g}'\) and \(\mathfrak{k}_2=\mathfrak{g}\), we have \(\mathfrak{g}=\mathfrak{g}'+J\mathfrak{g}'+{\rm
Rad}(\mathfrak{g})\) and \({\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')={\rm Rad}(\mathfrak{g})\cap (\mathfrak{g}'+J\mathfrak{g}')\). The latter is a \(J\)-invariant ideal
of \(\mathfrak{g}\) contained in \({\rm Rad}(\mathfrak{g})\). Using Step 1, we may assume either \({\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')=0\) or
\({\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')={\rm Rad}(\mathfrak{g})\). In the first case, the Levi–Malcev decomposition follows from \(\mathfrak{g}=(\mathfrak{g}'+J\mathfrak{g}')\oplus{\rm Rad}(\mathfrak{g})\). In the second case we have \({\rm Rad}(\mathfrak{g})\subseteq \mathfrak{g}'+J\mathfrak{g}'\), and
hence \(\mathfrak{g}=\mathfrak{g}'+J\mathfrak{g}'+{\rm Rad}(\mathfrak{g})\subseteq \mathfrak{g}'+J\mathfrak{g}'\), as claimed.
Step 3. We show that it may be assumed that \(\mathfrak{z}(\mathfrak{g})=0\). We suppose \(\mathfrak{z}(\mathfrak{g})\neq 0\) and provide the Levi–Malcev decomposition
for this case. Since \(J\) is abelian, \(\mathfrak{z}(\mathfrak{g})\) is \(J\)-invariant and thus contained in the radical of \(J\). Therefore, again by Step 1, we can suppose \(\mathfrak{z}(\mathfrak{g})= {\rm Rad}(\mathfrak{g})\). In these assumptions, the adjoint representation \(\operatorname{ad}\colon \mathfrak{g}\to \mathrm{End}(\mathfrak{g})\) descends to a well-defined representation of the quotient \[\operatorname{ad}\colon \frac{\mathfrak{g}}{{\rm Rad}(\mathfrak{g})}
\to \mathrm{End}(\mathfrak{g})\,.\] We consider the operator \[\Phi(U):=\frac{1}{2} \left(\operatorname{ad}_{JU}-J\operatorname{ad}_{U}\right) \in \mathrm{End}(\mathfrak{g})\,,\] where \(JU\) is the mean curvature vector of \(\mathfrak{g}/{\rm Rad}(\mathfrak{g})\). It is easy to prove that \(\Phi(U) \in \mathrm{End}(\mathfrak{g}, J)\), namely
\([\Phi(U),J]=0\). Moreover, for every \(X\in \mathfrak{g}/{\rm Rad}(\mathfrak{g})\), we have \[\begin{align}
\relax[\Phi(U), \operatorname{ad}_X]=&\,
\frac{1}{2}(\operatorname{ad}_{JU}\operatorname{ad}_X-J\operatorname{ad}_U\operatorname{ad}_X-\operatorname{ad}_X\operatorname{ad}_{JU}+\operatorname{ad}_XJ\operatorname{ad}_U)\\=&\,\frac{1}{2}(\operatorname{ad}_{JU}\operatorname{ad}_X-\operatorname{ad}_X\operatorname{ad}_{JU}-\operatorname{ad}_{JX}\operatorname{ad}_U+\operatorname{ad}_U\operatorname{ad}_{JX})=\frac{1}{2}(\operatorname{ad}_{[JU,
X]+[U, JX]})=0\,,
\end{align}\] where we used the fact that, since \(\mathfrak{g}\) is \(2\)-step and \(U\in (\mathfrak{g}/{\rm Rad}(\mathfrak{g}))'\), \(\operatorname{ad}_U\operatorname{ad}_X=\operatorname{ad}_U\operatorname{ad}_{JX}=0.\) As a consequence, \(\ker\Phi(U)\) and \(\operatorname{Im}\Phi(U)\) are
\(J\)-invariant ideals of \(\mathfrak{g}\). We now consider the operator \[\Omega^{1,1}_{\mathfrak{g}/ {\rm Rad}(\mathfrak{g})}:=\frac{1}{2}
\left(\operatorname{ad}^{\mathfrak{g}/{\rm Rad}(\mathfrak{g})}_{JU}-J\operatorname{ad}^{\mathfrak{g}/{\rm Rad}(\mathfrak{g})}_{U}\right) \in \mathrm{End}\left(\frac{\mathfrak{g}}{{\rm Rad}(\mathfrak{g})}, J\right)\,,\] defined so that \(\Omega^{1,1}_{\mathfrak{g}/ {\rm Rad}(\mathfrak{g})} \circ \pi = \pi \circ \Phi(U)\), where \(\pi \colon \mathfrak{g}\to \mathfrak{g}/ {\rm Rad}(\mathfrak{g})\) is the canonical projection onto
the quotient. By Remark 37\(\Omega^{1,1}_{\mathfrak{g}/ {\rm Rad}(\mathfrak{g})}=\mathrm{Id}_{\mathfrak{g}/ {\rm Rad}(\mathfrak{g})}\), whence
\(0=\ker \Omega^{1,1}_{\mathfrak{g}/ {\rm Rad}(\mathfrak{g})}=\ker\Phi(U)/{\rm Rad}(\mathfrak{g})\), i.e. \(\ker\Phi(U)={\rm Rad}(\mathfrak{g})\). We then conclude that \(\mathfrak{g}=\operatorname{Im}\Phi(U)\oplus {\rm Rad}(\mathfrak{g})\), completing the proof of this step.
Step 4. Finally, we conclude the existence part of the theorem. Thanks to the previous steps we may assume \(\mathfrak{g}= \mathfrak{g}' + J \mathfrak{g}'\) and \(\mathfrak{z}(\mathfrak{g})=0\). Since \(\mathfrak{z}(\mathfrak{g})=0\), in particular \(\mathfrak{g}'_J=0\), which puts us in the position to apply Theorem
41 to deduce the desired decomposition of \(\mathfrak{g}\).
In order to prove the uniqueness part of the theorem, we proceed by induction on \(\dim_{\mathbb{C}}\mathfrak{g}\). If \(\dim_{\mathbb{C}}\mathfrak{g}=1\), then either \(\mathfrak{g}=\mathbb{C}\) or \(\mathfrak{g}=\mathfrak{aff}(\mathbb{R})\) and the statement is clearly true. Assume the assertion is true for any Lie algebra whose complex dimension is strictly
less than \(\dim_{\mathbb{C}}\mathfrak{g}\). Let \(\mathfrak{h}_1, \mathfrak{h}_2\) be two \(J\)-adapted Levi subalgebras of \(\mathfrak{g}.\) Assume first \(\mathfrak{g}\ne \mathfrak{g}' + J\mathfrak{g}'\). Then, \(\mathfrak{h}_1, \mathfrak{h}_2\subseteq
\mathfrak{g}'+J\mathfrak{g}'\), because they are both \(J\)-perfect. Furthermore, thanks to Lemma 39, we deduce that \(\mathfrak{h}_1, \mathfrak{h}_2\) are \(J\)-adapted Levi subalgebras of \(\mathfrak{g}'+J\mathfrak{g}'\). We then apply the inductive hypothesis and
conclude that they are equal. Then, it remains to treat the case when \(\mathfrak{g}=\mathfrak{g}'+J\mathfrak{g}'\). If \(\mathfrak{z}( \mathfrak{g})=0\), then \(\mathfrak{g}_J'=0\) and we may conclude applying Theorem 41. Hence, we may assume that \(\mathfrak{z}(\mathfrak{g})\ne 0\). We distinguish two cases. Let us assume first that \(\mathfrak{z}(\mathfrak{g})\ne {\rm Rad}(\mathfrak{g})\). Consider the canonical projection onto the
quotient \(\pi\colon\mathfrak{g} \to\mathfrak{g}/\mathfrak{z}(\mathfrak{g})\) and observe that \(\pi(\mathfrak{h}_i)\), \(i=1,2\), are \(J\)-adapted Levi subalgebras of \(\mathfrak{g}/\mathfrak{z}(\mathfrak{g})\). By the inductive hypothesis, \(\pi(\mathfrak{h}_1)=\pi(\mathfrak{h}_2)\). This
allows to infer that \(\mathfrak{h}_1\subseteq \mathfrak{h}_2+\mathfrak{z}(\mathfrak{g}):=\mathfrak{s}\). Of course, \({\rm Rad}(\mathfrak{s} )=\mathfrak{z}(\mathfrak{g})\), hence \(\mathfrak{h}_1, \mathfrak{h}_2\) are \(J\)-adapted Levi subalgebras of \(\mathfrak{s}\) and \(\dim_{\mathbb{C}}\mathfrak{s}<\dim_{\mathbb{C}}\mathfrak{g}\), since \(\mathfrak{z}(\mathfrak{g})\ne {\rm Rad}(\mathfrak{g})\). We conclude that \(\mathfrak{h}_1=\mathfrak{h}_2\) by the inductive hypothesis. It remains to understand the case \(\mathfrak{z}(\mathfrak{g})={\rm Rad}(\mathfrak{g})\). In terms of the decomposition \(\mathfrak{g}=\mathfrak{h}_1\ltimes \mathfrak{z}(\mathfrak{g})\), we consider the projections \(p_{\mathfrak{h}_1}\) and \(p_{\mathfrak{z}(\mathfrak{g})}\) on
\(\mathfrak{h}_1\) and \(\mathfrak{z}(\mathfrak{g})\), respectively. First of all, we observe that, since \(J\mathfrak{h}_1=\mathfrak{h}_1\) and \(J\mathfrak{z}(\mathfrak{g})=\mathfrak{z}(\mathfrak{g})\), \([p_{\mathfrak{h}_1}, J]=[p_{\mathfrak{z}(\mathfrak{g})}, J]=0\). Hence, for any \(Z\in
\mathfrak{h}_2\), we can write \[Z=p_{\mathfrak{h}_1}(Z)+ p_{\mathfrak{z}(\mathfrak{g})}(Z)\,.\] It follows that, for any \(Z_1, Z_2\in \mathfrak{h}_2\), \[p_{\mathfrak{h}_1}([Z_1, Z_2])+ p_{\mathfrak{z}(\mathfrak{g})}([Z_1, Z_2])=[Z_1, Z_2]=[p_{\mathfrak{h}_1}(Z_1), p_{\mathfrak{h}_1}(Z_2)]\,,\] showing that \(p_{\mathfrak{h}_1}\) is a
holomorphic Lie algebra homomorphism and that \(p_{\mathfrak{z}(\mathfrak{g})}|_{\mathfrak{h}_2'}=0\). Since \(\mathfrak{h}_2=\mathfrak{h}_2'\oplus J\mathfrak{h}_2'\) and \([p_{\mathfrak{z}(\mathfrak{g})}, J]=0\) it follows that \(p_{\mathfrak{z}(\mathfrak{g})}|_{\mathfrak{h}_2}=0\). Thus, for any \(Z\in\mathfrak{h}_2\), \(Z=p_{\mathfrak{h}_1}(Z)\in\mathfrak{h}_1\) and so \(\mathfrak{h}_2\subseteq \mathfrak{h}_1\) forcing \(\mathfrak{h}_2=\mathfrak{h}_1\), since they have the same
dimension, thereby completing the proof. ◻
A first consequence of Theorem 42 is the following result.
Corollary 43. Let \(\mathfrak{g}\) be a Lie algebra endowed with an abelian complex structure \(J\). Then the adjoint operators associated with elements of the
standard basis \(\mathcal{B}\) of the \(J\)-adapted Levi subalgebra \(\mathfrak{h}\) defined in 9 , \(\{\operatorname{ad}_{JX_1}, \ldots, \operatorname{ad}_{JX_{p+q}}, \operatorname{ad}_{JY_{p+1}}, \ldots, \operatorname{ad}_{JY_{p+q}}\}\), are simultaneously diagonalisable, with \[{\rm
Spec}(\operatorname{ad}_{JX_i})\subseteq\{0,1\}\,, \quad {\rm Spec}(\operatorname{ad}_{JY_{p+j}})\subseteq\{0, \sqrt{-1}, -\sqrt{-1}\}\,, \quad i=1, \ldots, p+q\,,\quad j=1, \ldots, q\,.\] In particular, for any \(X\in
\mathfrak{h}'\), \(\operatorname{ad}_{JX}\) is diagonalisable.
Proof. First of all, for any \(i=1, \ldots, p+q\) and \(j=1, \ldots, q\), using ?? multiple times, we deduce \[\begin{align}
\operatorname{ad}_{JX_i}^2&=\operatorname{ad}_{J[JX_i, X_i]}=\operatorname{ad}_{JX_i}\,,\\
\operatorname{ad}_{JY_{p+j}}^3&=\operatorname{ad}_{J[JY_{p+j},Y_{p+j}]}\operatorname{ad}_{JY_{p+j}}=-\operatorname{ad}_{JX_{p+j}}\operatorname{ad}_{JY_{p+j}}=-\operatorname{ad}_{J[JX_{p+j}, Y_{p+j}]}=-\operatorname{ad}_{JY_{p+j}}\,,
\end{align}\] which immediately imply that \(\operatorname{ad}_{JX_i}\) and \(\operatorname{ad}_{JY_{p+j}}\) are diagonalisable with \({\rm
Spec}(\operatorname{ad}_{JX_i})\subseteq\{0,1\}\) and \({\rm Spec}(\operatorname{ad}_{JY_{p+j}})\subseteq\{0, \sqrt{-1}, -\sqrt{-1}\}\). Finally, since \(J\) is abelian, \(\{\operatorname{ad}_{JX_1}, \ldots, \operatorname{ad}_{JX_{p+q}}, \operatorname{ad}_{JY_{p+1}}, \ldots, \operatorname{ad}_{JY_{p+q}}\}\) is a family of commuting and diagonalisable endomorphisms of \(\mathfrak{g}\) which are, hence, simultaneously diagonalisable. The last statement is now clear. ◻
As a consequence of Corollary 43, we obtain the following.
Corollary 44. Let \(\mathfrak{g}\) be a Lie algebra endowed with an abelian complex structure \(J\).
If \(\mathfrak{g}'+J\mathfrak{g}'\) is unimodular, then \(\mathfrak{g}\) is \(J\)-solvable.
If \(\mathfrak{g}\) is of real type, then the \(J\)-adapted Levi subalgebra is holomorphically isomorphic to \(\mathfrak{aff}(\mathbb{R})^p\),
\(p\geq 0\).
Proof. Using Corollary 43, we observe that unimodularity of \(\mathfrak{g}'+J\mathfrak{g}'\) would not allow the \(J\)-adapted Levi subalgebra \(\mathfrak{h}\) to be non-zero, proving (1). As for (2), we notice that, again by Corollary 43, if \(\mathfrak{g}\) is of real type then there cannot be any ideal of the \(J\)-adapted Levi subalgebra in the decomposition given by Corollary 33 which is isomorphic to \(\mathfrak{aff}(\mathbb{C})\). ◻
We begin by emphasising that proving a Levi–Malcev decomposition in the general framework of \(2\)-step solvable Lie algebras with complex structure is actually an impossible task, as shown by the following example.
Example 45. Let us consider the almost abelian Lie algebra \(\mathfrak{g}\) defined by: \[[e_1, e_2]=e_2+e_3+e_4\,,\quad [e_1, e_3]=e_3\,,\quad [e_1, e_4]=e_4\,.\] In
the notations of [44], such Lie algebra is isomorphic to \(\mathfrak{s}_{4,3}\) with \(a=b=1\).
We endow \(\mathfrak{g}\) with the complex structure \(Je_1=e_2\) and \(Je_3=e_4\). As it is evident, \(\mathfrak{g}_J'={\rm
Rad}(\mathfrak{g})=\langle e_3,e_4\rangle\) and \(\mathfrak{g}/\mathfrak{g}_J'\simeq \mathfrak{aff }(\mathbb{R})\). It is fairly easy to see that there is no \(J\)-adapted Levi
subalgebra of \(\mathfrak{g}\). Moreover, we also note that \(\mathfrak{g} \ltimes \langle e_5, e_6\rangle\) with \(Je_5=e_6\) and \[[e_1, e_5]=-\frac{3}{2}e_5\,, \quad [e_1, e_6]=-\frac{3}{2}e_6\,,\] is a unimodular, \(2\)-step solvable Lie algebra with no \(J\)-adapted Levi subalgebra.
On the other hand, the previous example gives us an indication of the obstruction to take into account if one wishes to prove a general \(J\)-adapted Levi–Malcev decomposition. We now work towards the formalisation of
such a condition.
Definition 46. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra with a complex structure \(J\). Consider the subspace \(\mathcal{O}(\mathfrak{g}'_J)\) of elements in \(\mathfrak{g}\) that act holomorphically on \(\mathfrak{g}'_J\), i.e. \[\mathcal{O} (\mathfrak{g}_J'):=\{X\in \mathfrak{g} \, |\, [\operatorname{ad}_X, J]|_{\mathfrak{g}_J'}=0\}\,.\] Notice that \(\mathfrak{g}'+J\mathfrak{g}' \subseteq
\mathcal{O}(\mathfrak{g}'_J)\) by Lemma 4, and so \(\mathcal{O}(\mathfrak{g}'_J)\) is an ideal in \(\mathfrak{g}\). By integrability it is also \(J\)-invariant. Furthermore, \(\mathfrak{g}'_J\) is a \(J\)-invariant ideal in
\(\mathcal{O}(\mathfrak{g}'_J)\).
Since \(\mathfrak{g}_J'\) is abelian, we can define the representation \[\tau\colon \frac{\mathcal{O}(\mathfrak{g}'_J)}{\mathfrak{g}_J'}\to {\rm End}(\mathfrak{g}_J')\,, \quad
\tau(X+\mathfrak{g}_J'):=\operatorname{ad}_X|_{\mathfrak{g}_J'}\,.\] On the other hand, using Theorem 42 we can consider the \(J\)-adapted Levi subalgebra \(\mathfrak{h}\) of \(\mathcal{O}(\mathfrak{g}'_J)/\mathfrak{g}'_J\). Within \(\mathfrak{h}\), we take into account the subalgebra \(\mathfrak{h}_{JU}:=\langle U, JU\rangle\), where \(JU\) is the mean curvature vector of \(\mathfrak{h}\), see Definition 34. Then, we define \[\tau_{JU}:=\tau|_{\mathfrak{h}_{JU}}\,,\] which turns out to be a
representation of \(\mathfrak{h}_{JU}\) on \(\mathfrak{g}_J'\). Observe that \(\tau_{JU}(U)=0\), because \(U\in
(\mathcal{O}(\mathfrak{g}'_J)/ \mathfrak{g}_J')'\). The obstruction we are interested in is encoded in the cohomology group arising from the representation \(\tau_{JU}\), see Definition 3. The \(J\)-adapted Levi subalgebra \(\mathfrak{h}\) is unique, hence, the following is
well-defined.
Definition 47. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra with a complex structure \(J\). Then we define the cohomology
group \[H^2(\mathfrak{g}, JU):= H^{2}(\mathfrak{h}_{JU}, \tau_{JU})\,.\]
With a slight abuse of notation, we will often write \(JU\) to denote also a representative in \(\mathcal{O}(\mathfrak{g}'_J)\) of the equivalence class of the mean curvature vector
of \(\mathfrak{h}\).
Our interest in the just defined cohomology group stems from the following characterisation.
Lemma 48. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra with a complex structure \(J\). Then \(H^2(\mathfrak{g}, JU)=0\) if and only if \(2\notin {\rm Spec}(\operatorname{ad}_{JU}|_{\mathfrak{g}_J'})\).
Proof. Of course \(\ker d_{\tau_{JU}}\cap V^2(\mathfrak{h}_{JU}, \tau_{JU})=V^2(\mathfrak{h}_{JU}, \tau_{JU})\), since \(\dim_{\mathbb{R}}\mathfrak{h}_{JU}=2\). On the other
hand, \[(d_{\tau_{JU}}L)(JU, U)=\operatorname{ad}_{JU}L(U)-2L(U)=(\operatorname{ad}_{JU}-2{\rm Id})L(U)\,,\] using the fact that \([JU, U]=2U\) and that \(\tau_{JU}(U)=0\). Now, any \(\alpha \in V^2(\mathfrak{h}_{JU}, \tau_{JU})\) is completely determined by \(\alpha(JU, U)\in \mathfrak{g}_J'\). Hence, the
condition \(H^2(\mathfrak{g}, JU)=0\) is equivalent to the surjectivity of \((\operatorname{ad}_{JU}-2{\rm Id})|_{\mathfrak{g}_J'}\) which, in turn, is equivalent to \(2\notin {\rm Spec}(\operatorname{ad}_{JU}|_{\mathfrak{g}_J'})\). ◻
Before stating and proving a preliminary version of Theorem 2, we show that the vanishing of \(H^2(\mathfrak{g},JU)\) is inherited by suitable \(J\)-invariant subalgebras.
Lemma 49. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra endowed with a complex structure \(J\) such that \(H^{2}(\mathfrak{g}, JU)=0\). Then, for any \(J\)-invariant subalgebra \(\hat{\mathfrak{s}} \subseteq \mathcal{O}(\mathfrak{g}_J')\) satisfying \({\rm Rad}(\hat{\mathfrak{s}})\subseteq {\rm Rad}(\mathcal{O}(\mathfrak{g}_J'))\) and \(\hat{\mathfrak{s}}/{\rm Rad}(\hat{\mathfrak{s}})\simeq \mathcal{O}(\mathfrak{g}_J')/{\rm
Rad}(\mathcal{O}(\mathfrak{g}_J'))\), we have \(H^2(\hat{\mathfrak{s}}, JU_{\hat{\mathfrak{s}}})=0.\)
Proof. Let \(\hat{\mathfrak{s}}\) be a subalgebra as in the statement. It is apparent that \(\hat{\mathfrak{s}}_J'\subseteq \mathfrak{g}_J'\) and, since \(\hat{\mathfrak{s}}\subseteq \mathcal{O}(\mathfrak{g}_J')\), we have \(\hat{\mathfrak{s}}=\mathcal{O}_{\hat{\mathfrak{s}}}(\hat{\mathfrak{s}}_J'):=\{X\in \hat{\mathfrak{s}}\, \, |\, \,
[\operatorname{ad}_X, J]|_{\mathfrak{s}_J'}=0\}\). Furthermore, since \(\hat{\mathfrak{s}}_J'\subseteq \mathfrak{g}_J'\), the inclusion \(\hat{\mathfrak{s}}\to
\mathfrak{g}\) induces a Lie algebra homomorphism \[\varphi\colon \frac{\hat{\mathfrak{s}}}{\hat{\mathfrak{s}}_J'}\to \frac{\mathcal{O}(\mathfrak{g}_J')}{\mathfrak{g}_J'}\,, \quad
\varphi(X+\hat{\mathfrak{s}}_J')=X+\mathfrak{g}_J'\,.\] Now, by Theorem 42, we have that \[\frac{\hat{\mathfrak{s}}}{\hat{\mathfrak{s}}_J'}=\mathfrak{h}_{\hat{\mathfrak{s}}}\ltimes \frac{{\rm Rad}(\hat{\mathfrak{s}})}{\hat{\mathfrak{s}}_J'}\,,\quad
\frac{\mathcal{O}(\mathfrak{g}_J')}{\mathfrak{g}_J'}=\mathfrak{h}_{\mathfrak{g}}\ltimes\frac{{\rm Rad}(\mathcal{O} (\mathfrak{g}_J'))}{\mathfrak{g}_J'}\,.\] Then, since \(\ker(\varphi|_{\mathfrak{h}_{\hat{\mathfrak{s}}}})=\ker \varphi\cap \mathfrak{h}_{\hat{\mathfrak{s}}}=\frac{\mathfrak{g}_J'}{\hat{\mathfrak{s}}_J'}\cap \mathfrak{h}_{\hat{\mathfrak{s}}}=0\), we see that \(\varphi|_{\mathfrak{h}_{\hat{\mathfrak{s}}}}\) is a holomorphic Lie algebra isomorphism onto \({\rm Im}(\varphi|_{{\mathfrak{h}}_{\hat{\mathfrak{s}}}})\). In particular, this implies that \({\rm Im}(\varphi|_{\mathfrak{h}_{\hat{\mathfrak{s}}}})\) is a \(J\)-semisimple Lie subalgebra of \(\mathcal{O}(\mathfrak{g}_J')/\mathfrak{g}_J'\), and
hence \({\rm Im}(\varphi|_{\mathfrak{h}_{\hat{\mathfrak{s}}}})\cap \frac{{\rm Rad}(\mathcal{O} (\mathfrak{g}_J'))}{\mathfrak{g}_J'}=0\). On the other hand, \[\mathfrak{h}_{\hat{\mathfrak{s}}}\simeq \frac{\hat{\mathfrak{s}}}{{\rm Rad}(\hat{\mathfrak{s}})}\simeq \frac{\mathcal{O}(\mathfrak{g}_J')}{{\rm Rad}(\mathcal{O}(\mathfrak{g}_J'))},\] which gives that \({\rm Im}(\varphi|_{\mathfrak{h}_{\hat{\mathfrak{s}}}})\) is a \(J\)-adapted Levi subalgebra of \(\mathcal{O}(\mathfrak{g}_J')/\mathfrak{g}_J'\). Using
Theorem 42, we conclude that \(\mathfrak{h}_{\mathfrak{g}}= {\rm Im}(\varphi|_{\mathfrak{h}_{\hat{\mathfrak{s}}}})\). Then, from the last
statement in Lemma 35 we deduce \[JU_{\hat{\mathfrak{s}}}+ \mathfrak{g}_J'=\varphi(JU_{\hat{\mathfrak{s}}}+
\hat{\mathfrak{s}}_J')=JU_{\mathfrak{g}}+ \mathfrak{g}_J'.\] The claim now follows, since \(\operatorname{ad}_{JU_{\hat{\mathfrak{s}}}}|_{\hat{\mathfrak{s}}_J'}=\operatorname{ad}_{JU_{\mathfrak{g}}}|_{\hat{\mathfrak{s}}_J'}\). ◻
Corollary 50. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra endowed with a complex structure \(J\) such that \(H^2(\mathfrak{g}, JU)=0\). Then \(H^2(\mathfrak{g}'+J\mathfrak{g}', JU_{\mathfrak{g}'+J\mathfrak{g}'})=0.\)
Proof. We have that \(\mathfrak{g}'+J\mathfrak{g}'\) satisfies the hypotheses of Lemma 49, thanks to Corollary 39. The conclusion follows. ◻
The next result proves the desired Levi-Malcev decomposition when the Lie algebra \(\mathfrak{g}\) acts holomorphically on \(\mathfrak{g}_J'\) and the cohomology group defined above
vanishes.
Theorem 51. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra endowed with a complex structure \(J\) such that \(\mathfrak{g}=\mathcal{O}(\mathfrak{g}'_J)\), and suppose that \(H^2(\mathfrak{g}, JU)=0\). Then there exists a \(J\)-semisimple subalgebra \(\mathfrak{h}\) of \(\mathfrak{g}\) such that \[\mathfrak{g}=\mathfrak{h}\ltimes {\rm Rad}(\mathfrak{g})\,.\]
Proof. First of all, we note that in our hypotheses \(\mathfrak{g}_J'\) is a \(J\)-invariant ideal of \(\mathfrak{g}\). With this in mind, we
divide the proof into steps.
Step 1. We show that we may assume \({\rm Rad}(\mathfrak{g})=\mathfrak{g}_J'\ne 0\) and that \(\mathfrak{g}\) has no \(J\)-invariant
ideals properly contained in \({\rm Rad}(\mathfrak{g})\). First, note that we may suppose \(\mathfrak{g}_J'\ne 0\), otherwise we can simply apply Theorem 42 and conclude. To prove that we may reduce ourselves to the case \({\rm Rad}(\mathfrak{g})=\mathfrak{g}_J'\), we work inductively on \(\dim_\mathbb{C}(\mathfrak{g})\). If \(\mathfrak{g}\) is \(1\)-dimensional it can only be either \(\mathfrak{aff}(\mathbb{R})\)
or \(\mathbb{C}\) and in both cases the theorem is clearly true. Let us assume that \(\mathfrak{g}_J'\subset{\rm Rad}(\mathfrak{g})\). Then, since \(\mathfrak{g}/ \mathfrak{g}_J'\) has an abelian complex structure, we can apply Theorem 42 and obtain \[\frac{\mathfrak{g}}{\mathfrak{g}_J'}=\mathfrak{s}\ltimes \frac{{\rm Rad}(\mathfrak{g})}{\mathfrak{g}_J'}\,,\] where \(\mathfrak{s}\) is the \(J\)-adapted Levi subalgebra of \(\mathfrak{g} /\mathfrak{g}_J'\). Now consider \(\hat{\mathfrak{s}}:=\pi^{-1}(\mathfrak{s})\), which is a proper \(J\)-invariant subalgebra of \(\mathfrak{g}\). Since \(\hat{\mathfrak{s}}/\mathfrak{g}_J'=\mathfrak{s}\) is \(J\)-semisimple,
we can infer, using the same strategy as in Step 1 of Theorem 42, that \(\mathfrak{g}_J'= {\rm Rad}(\hat{\mathfrak{s}})\). We may then
apply Lemma 49 to infer that \(H^2(\hat{\mathfrak{s}},JU_{\hat{\mathfrak{s}}})=0\). Hence, by the inductive hypothesis \(\hat{\mathfrak{s}}\) admits a Levi–Malcev decomposition, and therefore so does \(\mathfrak{g}\). Consequently, we can assume \(\mathfrak{g}_J'={\rm
Rad}(\mathfrak{g}).\)
Finally, we prove that \(\mathfrak{g}\) has no \(J\)-invariant ideals properly contained in \({\rm Rad}(\mathfrak{g})\), once again by induction on \(\dim_\mathbb{C}\mathfrak{g}\). If \(\dim_\mathbb{C}\mathfrak{g}=1\), the claim is trivial. Let \(\mathfrak{k} \subset \mathfrak{g}_J'\) be a \(J\)-invariant ideal of \(\mathfrak{g}\). Note that \((\mathfrak{g}/\mathfrak{k})_J'=\frac{\mathfrak{g}_J'}{\mathfrak{k}}\). Furthermore \(\frac{\mathfrak{g}/\mathfrak{k}}{\mathfrak{g}_J'/\mathfrak{k}}\simeq \mathfrak{g}/\mathfrak{g}_J'\) via \(\varphi((X+\mathfrak{k})+
\frac{\mathfrak{g}_J'}{\mathfrak{k}})=X+\mathfrak{g}_J'\). On the other hand, using again Lemma 35, we have \(JU_{\mathfrak{g}/\mathfrak{k}}+ \mathfrak{g}'_J=\varphi((JU_{\mathfrak{g}/\mathfrak{k} }+\mathfrak{k})+\frac{\mathfrak{g}'_J}{\mathfrak{k}})=JU_{\mathfrak{g}}+ \mathfrak{g}_J'.\) Denote by \(\pi^{\mathfrak{k} }\colon \mathfrak{g} \to\mathfrak{g}/\mathfrak{k}\) the quotient map, then \[\operatorname{ad}_{JU_{\mathfrak{g}/\mathfrak{k}}+ \mathfrak{k}}^{\mathfrak{g}/\mathfrak{k}
}|_{\mathfrak{g}_J'/\mathfrak{k}}=\pi^{\mathfrak{k}}\operatorname{ad}_{JU_{\mathfrak{g}/\mathfrak{k}}}^{\mathfrak{g}}|_{\mathfrak{g}_J'}=\pi^{\mathfrak{k}}\operatorname{ad}_{JU_{\mathfrak{g}}}^{\mathfrak{g}}|_{\mathfrak{g}_J'}\,.\]
Hence, since \(2\notin{\rm Spec}(\operatorname{ad}_{JU_{\mathfrak{g}}}^{\mathfrak{g}}|_{\mathfrak{g}_J'})\), the same holds for \(\operatorname{ad}_{JU_{\mathfrak{g}/\mathfrak{k}}+
\mathfrak{k}}^{\mathfrak{g}/\mathfrak{k} }|_{\mathfrak{g}_J'/\mathfrak{k}}\). Furthermore, since \(\mathfrak{g}\) acts holomorphically on \(\mathfrak{g}_J'\), then \(\mathfrak{g}/\mathfrak{k}\) acts holomorphically on \((\mathfrak{g}/\mathfrak{k})_J'\). Therefore, applying the inductive hypothesis we obtain a Levi–Malcev decomposition of \(\mathfrak{g}/ \mathfrak{k}\). The same argument in Step 1 of Theorem 42, together with an argument analogous to that used in the first part of
this proof, guarantees the existence of a \(J\)-adapted Levi subalgebra for \(\mathfrak{g}\).
Step 2. First of all, thanks to Step 1, we may assume \(0\neq \mathfrak{g}'_J={\rm Rad}(\mathfrak{g})\) and \(\mathfrak{g}\) has no \(J\)-invariant ideals properly contained in \({\rm Rad}(\mathfrak{g})\). Moreover, \(\mathfrak{g}/\mathfrak{g}_J'\) is \(J\)-semisimple with an abelian complex structure, hence, it is \(J\)-perfect by Theorem 27. As in Step 2 of
Theorem 42, we can apply Lemma 39 to conclude that \(\mathfrak{g}\)
is \(J\)-perfect. In this setting, we consider \[\Phi\colon \mathfrak{g} \to {\rm End}(\mathfrak{g} )\,,\quad \Phi(X)=\frac{1}{2}(\operatorname{ad}_{JX}-J\operatorname{ad}_X)\,, \quad X
\in\mathfrak{g}\,.\] First of all, using integrability of \(J\), for any \(X\in \mathfrak{g}\), we deduce \[\label{cazzettiinano}
[\Phi(X), J]=0\,, \quad \Phi(JX)=-\Phi(X)J\,.\tag{10}\] By ?? and 10 , we know that \(\mathfrak{g}_J'\subseteq \ker \Phi\) and \(J\ker \Phi=\ker
\Phi\). Furthermore, as in Lemma 4, we observe that \(\mathfrak{g}\) acts holomorphically on \(\ker
\Phi\). Therefore, \([\mathfrak{g}, \ker \Phi]\subseteq \mathfrak{g}_J'\), giving that \(\ker \Phi\) is a \(J\)-solvable ideal of \(\mathfrak{g}\). Thus, \(\mathfrak{g}_J'= \ker \Phi\). In view of this, \(\Phi\) descends to the quotient, i.e. \[\Phi\colon
\frac{\mathfrak{g}}{ \mathfrak{g}_J'}\to {\rm End}(\mathfrak{g}).\] Moreover, we observe that, if \(X\in\mathfrak{g}/\mathfrak{g}_J'\) and \(Y\in\mathfrak{g}_J'\), then
\[\label{giovannibuco}
\Phi(X)\operatorname{ad}_Y=\operatorname{ad}_{\Phi(X)Y}\,.\tag{11}\] Indeed, using \(2\)-step solvability and that \(X\) acts holomorphically on \(\mathfrak{g}_J'=\ker \Phi\), we have \[\begin{align}
\Phi(X)\operatorname{ad}_Y=&\,
\frac{1}{2}(\operatorname{ad}_{JX}\operatorname{ad}_Y-J\operatorname{ad}_X\operatorname{ad}_Y)=
\frac{1}{2}(\operatorname{ad}_{[JX, Y]}-\operatorname{ad}_XJ\operatorname{ad}_Y)=\frac{1}{2}(\operatorname{ad}_{[JX, Y]}-\operatorname{ad}_X\operatorname{ad}_{JY})\\
=&\, \frac{1}{2}\operatorname{ad}_{[JX, Y]-[X, JY]}=\operatorname{ad}_{\Phi(X)Y}\,,
\end{align}\] as claimed. We will only be interested in \(\Phi(U)\), where \(JU\in J(\mathfrak{g} /\mathfrak{g}_J')'\) is the mean curvature vector of \(\mathfrak{g} /\mathfrak{g}_J'\), introduced in Definition 34. We extend the endomorphism \(\Phi(U)\) by \(\mathbb{C}\)-linearity on \(\mathfrak{g}^{\mathbb{C}}:=\mathfrak{g}\otimes \mathbb{C}\). By abuse of notation, this extension will again be denoted \(\Phi(U)\).
Since \(\mathfrak{g}_J'\) is an ideal of \(\mathfrak{g}\), and by 10 , \([\Phi(U), J]=0\), we deduce \[\Phi(U)((\mathfrak{g}_J')^{1,0})\subseteq (\mathfrak{g}_J')^{1,0}\,,\qquad \Phi(U)((\mathfrak{g}_J')^{0,1})\subseteq (\mathfrak{g}_J')^{0,1}\,.\] Consequently, we can find \(\lambda
\in \mathbb{C}\) such that \(\ker \bigl(\left(\Phi(U)-\lambda {\rm Id}\right)|_{(\mathfrak{g}_J')^{1,0}}\bigr)\ne 0\). By simply exploiting \(\mathbb{C}\)-linearity, from 11 , we have \[\left(\Phi(U)-\lambda {\rm Id}\right)\operatorname{ad}^{\mathfrak{g}^{\mathbb{C}}}_Y=\operatorname{ad}^{\mathfrak{g}^{\mathbb{C}}}_{(\Phi(U)-\lambda {\rm Id})Y}\,, \qquad Y \in
(\mathfrak{g}_J')^{1,0}\,.\] Hence, by the above and the fact that \(\mathfrak{g}\) acts holomorphically on \(\mathfrak{g}_J'\), we infer that \(\ker
\bigl(\left(\Phi(U)-\lambda {\rm Id}\right)|_{(\mathfrak{g}_J')^{1,0}}\bigr)\) and \(\ker \bigl(\left(\Phi(U)-\bar \lambda {\rm Id}\right)|_{(\mathfrak{g}_J')^{0,1}}\bigr)\) are \(J\)-invariant ideals of \(\mathfrak{g}^{\mathbb{C}}\) contained in \(\mathfrak{g}_J'\otimes \mathbb{C}\). We then consider \[\mathfrak{k}:=\ker \left(\left(\Phi(U)-\lambda {\rm Id}\right)|_{(\mathfrak{g}_J')^{1,0}}\right)\oplus \ker \left(\left(\Phi(U)-\bar \lambda {\rm Id}\right)|_{(\mathfrak{g}_J')^{0,1}}\right)\subseteq
\mathfrak{g}_J'\otimes \mathbb{C}\] which is a non-zero \(J\)-invariant ideal of \(\mathfrak{g}^{\mathbb{C}}\) which is stable under conjugation. Thus, \(\mathfrak{k}=(\mathfrak{k} \cap \mathfrak{g})\otimes \mathbb{C}\,,\) where \(\mathfrak{k} \cap \mathfrak{g}\subseteq \mathfrak{g}_J'\) is a non-zero \(J\)-invariant ideal of \(\mathfrak{g}.\) As a consequence, using the first step, we may assume \(\mathfrak{k}\cap \mathfrak{g}= \mathfrak{g}_J'\) and, thus,
\(\mathfrak{k}= \mathfrak{g}_J'\otimes \mathbb{C}\). In particular, we conclude that \[\Phi(U)|_{(\mathfrak{g}_J')^{1,0}}=\lambda {\rm Id}_{(\mathfrak{g}_J')^{1,0}}\,,
\quad\Phi(U)|_{(\mathfrak{g}_J')^{0,1}}=\bar \lambda {\rm Id}_{(\mathfrak{g}_J')^{0,1}}\,.\] Denote \(a:={\rm Re}(\lambda)\) and \(b:={\rm Im}(\lambda)\). Then we infer that
\[\label{baumiao}
\Phi(U)|_{\mathfrak{g}_J'}=a{\rm Id}_{\mathfrak{g}_J'}+ b J|_{\mathfrak{g}_J'}\,.\tag{12}\] Now, since \(H^2(\mathfrak{g}, JU)=0\) and by Lemma 48, we deduce that \((a, b)\ne (1,0)\). Therefore, from 12 follows that the map \[\tilde{\Psi}:=\Phi(U)-a{\rm Id}-b J\colon \mathfrak{g}
\to \mathfrak{g}\] descends to a well-defined map on the quotient, namely \[\Psi\colon \frac{\mathfrak{g}}{ \mathfrak{g}_J'}\to \mathfrak{g}\,.\] The first thing to observe is that \(\Psi\) is injective. Indeed, recalling Definition 36 and Remark 37, \[\pi \tilde{\Psi}=\pi\Phi(U)-a\pi-bJ\pi=\Omega_{\mathfrak{g}/ \mathfrak{g}_J'}\pi-a\pi- bJ \pi=((1-a){\rm Id}- bJ)\pi\,.\] Hence, if \(X\in \ker \tilde{\Psi}\), then \((1-a)\pi(X)=bJ\pi(X)\), which is possible if and only if \(\pi(X)=0\), since \((a, b)\ne (1, 0)\), therefore \(X\in
\mathfrak{g}_J'\). On the other hand, \(\operatorname{Im}(\Psi)\cap \mathfrak{g}_J'=0\). Indeed, if \(\Psi(\pi (X))\in\mathfrak{g}_J'\), \(X\in\mathfrak{g}\), then again \[0=\pi \Psi(\pi(X))=\pi \tilde{\Psi}(X)=((1-a)\pi(X)-bJ\pi(X))\] implying that \(\pi(X)=0\), as claimed. Moreover, \({\rm Im}\Psi\) is \(J\)-invariant, since \([\Psi, J]=0\).
It remains to prove that \(\operatorname{Im}\Psi\) is a subalgebra of \(\mathfrak{g}\). To do so, we fix \(X, Y\in
(\mathfrak{g}/\mathfrak{g}_J')'\) and compute \([\Psi(X),\Psi(Y)]\), \([\Psi(JX),\Psi(JY)]\) and \([\Psi(X),\Psi(JY)]\). Let us start by
observing that \[\Psi(X)=\frac{1}{2}[JU,X]-aX-bJX\,, \qquad \Psi(Y)=\frac{1}{2}[JU,Y]-aY-bJY\,.\] Then, using \(2\)-step solvability, Jacobi identity and integrability of \(J\), we get \[\begin{align} [\Psi(X),\Psi(Y)]&=b\left( -\frac{1}{2}[[JU,X],JY]+a[X,JY]-\frac{1}{2}[JX,[JU,Y]]+a[JX,Y]+b[JX,JY]\right)\\ &=b\left(
-\frac{1}{2}[JU,[X,JY]+[JX,Y]]+a[X,JY]+a[JX,Y]+b[JX,JY]\right)\\
&=b\left( \frac{1}{2}[JU,J[JX,JY]]-aJ[JX,JY]+b[JX,JY]\right)=b\Psi(J[JX,JY])=0\,, \end{align}\] since \(J[JX, JY]\in \mathfrak{g}_J'\). On the other hand, using integrability, we have \[\Psi(JX)=\frac{1}{2}J[JU,X]-aJX+bX\,, \qquad \Psi(JY)=\frac{1}{2}J[JU,Y]-aJY+bY\,,\] thus \[\begin{align}
[\Psi(JX),\Psi(JY)]&=\frac{1}{4}[J[JU,X],J[JU,Y]]-\frac{a}{2}[J[JU,X],JY]+\frac{b}{2}[J[JU,X],Y]-\frac{a}{2}[JX,J[JU,Y]]\\&\quad +a^2[JX,JY]-ab[JX,Y]+\frac{b}{2}[X,J[JU,Y]]-ab[X,JY]\,. \end{align}\] We treat the first term as follows. Using
integrability, \(2\)-step solvability and Jacobi identity, we have \[\begin{align}
\relax
[J[JU, X], J[JU, Y]] &=J([J[JU, X], [JU,Y]]+[[JU, X], J[JU, Y]])\\
&=J\left([JU,[J[JU,X],Y]]+ [JU,[X, J[JU, Y]]]\right)\,.
\end{align}\] Also, by integrability \[[J[JU,X],JY]+[JX,J[JU,Y]]=J[J[JU,X],Y]+J[[JU,X],JY]+J[JX,[JU,Y]]+J[X,J[JU,Y]]\,,\] whence \[\begin{align}
[\Psi(JX),\Psi(JY)]&=\frac{1}{2}J\Psi\left([J[JU,X],Y]+[X,J[JU,Y]]\right)\\ &\quad-\frac{a}{2}J[[JU,X],JY]-\frac{a}{2}J[JX,[JU,Y]]+a^2[JX,JY]-ab[JX,Y]-ab[X,JY]\\
&=\frac{1}{2}J\Psi\left([J[JU,X],Y]+[X,J[JU,Y]]\right)-\frac{a}{2}J[JU,[X,JY]]-\frac{a}{2}J[JU,[JX,Y]]\\ &\quad +a^2J[JX,Y]+a^2J[X,JY]-ab[JX,Y]-ab[X,JY]\\ &=\Psi\left(\frac{1}{2}J[J[JU,X],Y]+\frac{1}{2}J[X,J[JU,Y]]-aJ[X,JY]-aJ[JX,Y]\right)=0\,,
\end{align}\] since the argument of \(\Psi\) lies in \(\mathfrak{g}_J'\). Finally, we compute \[\begin{align}
[\Psi(X),\Psi(JY)]&=\frac{1}{4}[[JU,X],J[JU,Y]]-\frac{a}{2}[[JU,X],JY]-\frac{a}{2}[X,J[JU,Y]]+a^2[X,JY]\\ &\quad -\frac{b}{2}[JX,J[JU,Y]]+ab[JX,JY]-b^2[JX,Y]\\
&=\frac{1}{4}[JU,[X,J[JU,Y]]]-\frac{a}{2}[JU,[X,JY]]-\frac{a}{2}[X,J[JU,Y]]+a^2[X,JY]\\ &\quad -\frac{b}{2}J[X,J[JU,Y]]-\frac{b}{2}J[JX,[JU,Y]]+abJ[X,JY]+abJ[JX,Y]-b^2[JX,Y]\\
&=\frac{1}{2}\Psi([X,J[JU,Y]])-a\Psi([X,JY])-bJ\left(\frac{1}{2}[JU,[JX,Y]]-a[JX,Y]-bJ[JX,Y]\right)\\
&=\Psi\left(\frac{1}{2}[X,J[JU,Y]]-a[X,JY]-bJ[JX,Y]\right)\,. \end{align}\] It follows that \([\operatorname{Im}\Psi, \operatorname{Im}\Psi]\subseteq \operatorname{Im}\Psi\), and hence \(\operatorname{Im}\Psi\) is a subalgebra, as desired. ◻
Remark 52. The appearance of the cohomological obstruction in Theorem 51 is somewhat unsurprising. Indeed, a possible proof of the classical Levi–Malcev
decomposition uses the fact that the second cohomology group with values in any representation of a semisimple Lie algebra always vanishes, see [43]. The
difference here is that, in our framework, the vanishing of the relevant cohomology group is not always guaranteed and must therefore be imposed as an additional assumption. For instance, it is easy to check that Example 45 violates the condition \(H^2(\mathfrak{g},JU)=0\).
In order to extend Theorem 51 to the general case we need some preparations. Let \(\mathfrak{g}\) be a \(2\)-step
solvable Lie algebra, we know that \(\mathfrak{g}_J'\) is a \(J\)-invariant ideal in \(\mathfrak{g}'+J\mathfrak{g}'\). We can then make use of
Theorem 42 to infer that there exists a \(J\)-invariant subalgebra \(\mathfrak{h}\) satisfying \[\frac{\mathfrak{g}'+J\mathfrak{g}'}{\mathfrak{g}_J'}=\mathfrak{h} \ltimes \frac{{\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')}{\mathfrak{g}_J'}\,.\] If \(\mathfrak{g}\) is not
\(J\)-solvable, then, as in Corollary 43, we observe that \[\label{adu942612adu}
\operatorname{ad}_{JU}^2=2\operatorname{ad}_{JU}\,.\tag{13}\] In particular, \(\operatorname{ad}_{JU}\) is diagonalisable over \(\frac{{\rm
Rad}(\mathfrak{g}'+J\mathfrak{g}')}{\mathfrak{g}_J'}\) and \[\label{specU}
\mathrm{Spec}\left(\operatorname{ad}_{JU}|_{\frac{{\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')}{\mathfrak{g}_J'}} \right) \subseteq \{0,2\}\,.\tag{14}\] Let \(V_0:=\ker\left(\operatorname{ad}_{JU}|_{\frac{{\rm
Rad}(\mathfrak{g}'+J\mathfrak{g}')}{\mathfrak{g}_J'}}\right)\) and, denoted by \(\pi\colon \mathfrak{g}'+J\mathfrak{g}'\to \frac{\mathfrak{g}'+J\mathfrak{g}'}{\mathfrak{g}_J'}\) the
canonical projection onto the quotient, we define \[\label{defkon}
\mathfrak{q}:=\pi^{-1}(V_0)\cap \mathfrak{g}'=\{ X\in \mathrm{Rad}(\mathfrak{g}'+J\mathfrak{g}')\cap \mathfrak{g}' \mid [JU, X] \in \mathfrak{g}'_J\}\,.\tag{15}\] The next is a technical lemma we will use later.
Lemma 53. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra such that \(H^2(\mathfrak{g}, JU)=0\). Suppose \(S,T\in \mathfrak{g}'\) satisfy \[[JU, S]= aS+bT + Z\,,\qquad
[JU, T]= -bS+aT +Z'\,,\] for some \(a,b\in \mathbb{R}\) with \((a, b)\ne (2, 0)\) and \(Z,Z'\in \mathfrak{g}'_J\). If \(X\in\mathfrak{g}\) is such that \([X,Z],[X,Z']\in \mathfrak{q}\), then \([X,S],[X,T]\in \mathfrak{q}\).
Proof. We start by observing that the hypothesis \(H^2(\mathfrak{g}, JU)=0\) and Corollary 50 put us in the position to apply
Theorem 51 and infer that \[\mathfrak{g}'+J\mathfrak{g}'=\mathfrak{h}\ltimes {\rm Rad}(\mathfrak{g}'+ J \mathfrak{g}')\,, \qquad
\mathfrak{h}\simeq \frac{\mathfrak{g}'+J\mathfrak{g}'}{{\rm Rad}(\mathfrak{g}'+ J\mathfrak{g}')}.\] We first prove that if \([X,Z],[X,Z']\in {\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')\), then
\([X,S],[X,T] \in {\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')\). Surely \([X,S],[X,T]\in \mathfrak{g}'+J\mathfrak{g}'\) and we can decompose \[[X,S]=\sum_{i=1}^{\dim \mathfrak{h}'} \alpha_i Y_i + W_1\,, \qquad
[X,T]=\sum_{i=1}^{\dim \mathfrak{h}'} \beta_i Y_i+ W_2 \,,\] where \(\{Y_1, \ldots, Y_{\dim \mathfrak{h}'}\}\) is a basis of \(\mathfrak{h}'\) and \(W_1, W_2\in {\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')\). Then, since \(S\in\mathfrak{g}'\) and \({\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')\) is
an ideal in \(\mathfrak{g}'+J\mathfrak{g}'\), \(2\)-step solvability and ?? imply \[\begin{align}
0=&\, [[X,JU],S]=[[X,S],JU]+[X,[JU,S]]
=\sum_{i=1}^{\dim \mathfrak{h}'}\left(-2\alpha_i+a\alpha_i+b\beta_i\right)Y_i+W_3\,,\\
0=&\, [[X,JU],T]=[[X,T],JU]+[X,[JU,T]]=\sum_{i=1}^{\dim \mathfrak{h}'} \left(-2\beta_i-b\alpha_i+a\beta_i\right)Y_i+W_4\,,
\end{align}\] where \(W_3, W_4\in {\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')\). Hence, for all \(i=1, \ldots, \dim \mathfrak{h}'\), we obtain the system of equations
\[\label{sefattolastoria}
\begin{cases}
(a-2)\alpha_i+b\beta_i=0\,, \\
(a-2)\beta_i-b\alpha_i=0\,.
\end{cases}\tag{16}\] Assume by contradiction that \([X,S]\notin \mathrm{Rad}(\mathfrak{g}'+J\mathfrak{g}')\), then there exists \(i=1, \ldots, \dim \mathfrak{h}'\)
such that \(\alpha_i\ne 0\). Therefore, from the second equation in 16 we have \(b=(a-2)\frac{\beta_i}{\alpha_i}\), which, plugged in the first equation,
forces \(a=2\) and consequently \(b=0\) which is against our assumptions. We conclude similarly if \([X,T]\notin
\mathrm{Rad}(\mathfrak{g}'+J\mathfrak{g}')\).
Now we prove the lemma. Suppose \([X,Z],[X,Z'] \in \mathfrak{q}\) then, by the first part of the proof, we know that \([X,S],[X, T]\in {\rm
Rad}(\mathfrak{g}'+J\mathfrak{g}')\) and we may write \[[X,S]=P+Z_1\,,\qquad
[X,T]=Q+Z_2\,,\] with \(P,Q\in V\), for some complement \(V\) of \(\mathfrak{g}_J'\) in \({\rm
Rad}(\mathfrak{g}'+J\mathfrak{g}')\), and \(Z_1, Z_2\in\mathfrak{g}_J'\). By repeating the computation done above, we get \[\begin{cases}
[JU,P]= aP+bQ + [X,Z]+Z_3\,,\\
[JU,Q]= -bP+aQ +[X,Z']+Z_4\,,\\
\end{cases}\] for some \(Z_3, Z_4\in\mathfrak{g}_J'\). Applying \(\operatorname{ad}_{JU}\) to these equations and using the assumption that \([X,Z],[X,Z']\in \mathfrak{q}\), we get \[\label{pezzodistoria}
\begin{cases}
[JU, [JU,P]]= a[JU,P]+b[JU,Q] +Z_5\,,\\
[JU, [JU,Q]]= -b[JU,P]+a[JU,Q] +Z_6\,,\\
\end{cases}\tag{17}\] with \(Z_5,Z_6\in \mathfrak{g}'_J\). Now, either \([JU,P],[JU,Q] \in \mathfrak{g}'_J\), meaning \([X,S],[X,T]\in
\mathfrak{q}\), or \(\lambda=a+\sqrt{-1}b\) is an eigenvalue of \(\operatorname{ad}_{JU} \vert_{\frac{{\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')}{\mathfrak{g}'_J}}\) with
eigenvector \([JU,P]-\sqrt{-1}[JU,Q]\). Thus, by 14 we must have \(\lambda\in \{0,2\}\). On the other hand, since \((a,b)\neq
(2,0)\), we necessarily have \(a=b=0\). Using 13 , we conclude from 17 that \([JU,P],[JU,Q] \in \mathfrak{g}'_J\),
as desired. ◻
With this settled, we are now ready to prove the following.
Proposition 54. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra such that \(H^2(\mathfrak{g}, JU)=0\). Then \[\mathfrak{g}'_J \subseteq {\rm Rad}(\mathfrak{g})\,.\]
Proof. First, we aim to prove that \(\mathfrak{q}\) is an ideal, where \(\mathfrak{q}\) is defined in 15 . Notice that, by 2-step solvability we have
\[\operatorname{ad}_{JU}\vert_{(\mathfrak{g}'_J)^{1,0}}=\operatorname{ad}_{JU}\vert_{(\mathfrak{g}'_J)^{1,0}}+\sqrt{-1}\operatorname{ad}_{U}\vert_{(\mathfrak{g}'_J)^{1,0}}=\operatorname{ad}_{JU+\sqrt{-1}U}\vert_{(\mathfrak{g}'_J)^{1,0}}\]
and so, by Lie’s theorem, there exists a basis \(\{W_1,\dots,W_s\}\) of \((\mathfrak{g}'_J)^{1,0}\) with respect to which \(\operatorname{ad}_{JU}\vert_{(\mathfrak{g}'_J)^{1,0}}\) is lower triangular. In particular, the eigenvalues \(\lambda_i\in \mathbb{C}\) of \(\operatorname{ad}_{JU}\vert_{(\mathfrak{g}'_J)^{1,0}}\) satisfy \[[JU, W_k]=\lambda_k W_k+ V_k\,, \qquad V_k\in \bigoplus_{i<k} \langle W_i\rangle \qquad k=1,\dots,s\,.\] Writing \(a_k:=\mathrm{Re}(\lambda_k)\), \(b_k:=\operatorname{Im}(\lambda_k)\), and \(Z_k:=\mathrm{Re}(W_k)\), this is equivalent to \[\begin{cases}
[JU, Z_k]= a_kZ_k+b_kJZ_k+ \tilde{Z}_k\,, & \tilde{Z}_k\in \bigoplus_{i<k} \langle Z_i,JZ_i \rangle\,, \\
[JU,JZ_k]= -b_kZ_k+a_kJZ_k+\tilde{Z}'_k\,, & \tilde{Z}'_k\in \bigoplus_{i<k} \langle Z_i,JZ_i\rangle \,,\\
\end{cases} \qquad k=1,\dots,s\,.\] Note that \(\mathfrak{g}'_J \subseteq \mathfrak{q}\). We first prove that \([\mathfrak{g},\mathfrak{g}'_J]\subseteq \mathfrak{q}\). In
order to do this, we use induction on \(k\), and show that \([\mathfrak{g},Z_k],[\mathfrak{g},JZ_k]\subseteq \mathrm{Rad}(\mathfrak{g}'+J\mathfrak{g}')\). We observe that the
condition \(H^2(\mathfrak{g},JU)=0\) entails that \((a_k,b_k)\neq (2,0)\), for all \(k=1,\dots,s\). For \(k=1\), using Lemma
53 with \(S=Z_1, T=JZ_1, Z=Z'=0\), we see that we have \([\mathfrak{g},Z_1],[\mathfrak{g},JZ_1]\subseteq
\mathfrak{q}\). Now, suppose that \([\mathfrak{g},Z_{i}], [\mathfrak{g},JZ_{i}]\subseteq \mathfrak{q}\), for all \(i=1,\dots,k-1\), and let us prove the claim for \(k\). By the inductive assumption, we can again apply Lemma 53 with \(S=Z_k\), \(T=JZ_k\),
\(Z=\tilde{Z}_k\), and \(Z'=\tilde{Z}'_k\). Hence, we conclude that \([\mathfrak{g},Z_k],[\mathfrak{g},JZ_k]\in \mathfrak{q}\) for all \(k\), meaning that \([\mathfrak{g},\mathfrak{g}'_J]\subseteq \mathfrak{q}\). Knowing this, it now follows immediately from Lemma 53 that \([\mathfrak{g},\mathfrak{q}]\subseteq \mathfrak{q}\).
Let \(\mathfrak{k}\) be the ideal of \(\mathfrak{g}\) generated by \(\mathfrak{g}'_J\), i.e. \[\mathfrak{k}=\mathfrak{g}'_J+[\mathfrak{g},\mathfrak{g}'_J]+[\mathfrak{g},[\mathfrak{g},\mathfrak{g}'_J]]+\dots\] Since \(\mathfrak{q}\) is an ideal, we have \(\mathfrak{k} \subseteq \mathfrak{q}\subseteq \mathrm{Rad}(\mathfrak{g}'+J\mathfrak{g}')\cap \mathfrak{g}'\). Note that, for every \(X\in \mathfrak{g}\), \(Y\in \mathfrak{k}\) we have \([X,JY]+[JX,Y]\in \mathfrak{g}'_J\) and thus \(\mathfrak{k}+ J \mathfrak{k}\) is an ideal of \(\mathfrak{g}\) contained in \(\mathrm{Rad}(\mathfrak{g}'+J\mathfrak{g}')\). In particular, \(\mathfrak{k} + J\mathfrak{k}\) is a \(J\)-solvable ideal of \(\mathfrak{g}\) which contains \(\mathfrak{g}_J'\), implying that \(\mathfrak{g}_J'\subseteq {\rm
Rad}(\mathfrak{g})\). ◻
The above proposition allows us to draw the following corollary, which in particular shows that if \(H^2(\mathfrak{g},JU)=0\), then any semisimple complex structure is abelian.
Corollary 55. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra such that \(H^2(\mathfrak{g}, JU)=0\). Then \[{\rm Rad}(\mathcal{O}(\mathfrak{g}_J'))={\rm Rad}(\mathfrak{g})\cap \mathcal{O}(\mathfrak{g}_J')\,, \qquad \mathfrak{g}=\mathcal{O}(\mathfrak{g}_J')+ {\rm Rad}(\mathfrak{g})\,.\] Moreover, if \(J\) is semisimple, then it is abelian.
Proof. Combining Proposition 54 and Lemma 39 immediately gives the first part. In turn, if
\(J\) is semisimple, this yields \(\mathfrak{g}'_J\subseteq {\rm Rad}(\mathcal{O}(\mathfrak{g}_J'))={\rm Rad}(\mathfrak{g})\cap \mathcal{O}(\mathfrak{g}_J')=0\). ◻
Theorem 56. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra and suppose that \(H^2(\mathfrak{g}, JU)=0\). Then there exists
a unique \(J\)-semisimple subalgebra \(\mathfrak{h}\) of \(\mathfrak{g}\) such that \[\mathfrak{g}=\mathfrak{h}\ltimes {\rm
Rad}(\mathfrak{g})\,.\]
Proof. Thanks to Corollary 55, we know that \({\rm Rad}(\mathcal{O}(\mathfrak{g}'_J)) \subseteq {\rm Rad}(\mathfrak{g})\).
Suppose \({\rm Rad}(\mathcal{O}(\mathfrak{g}'_J))={\rm Rad}(\mathfrak{g})\), which implies \({\rm Rad}(\mathfrak{g})\subseteq \mathcal{O}(\mathfrak{g}'_J)\). Similarly to Step 2 of
Theorem 42 we deduce that \(\mathfrak{g}=\mathcal{O}(\mathfrak{g}'_J)\). We are now in the position to apply Theorem 51 and conclude this case.
Therefore we only need to deal with the case \({\rm Rad}(\mathcal{O}(\mathfrak{g}'_J))\subset {\rm Rad}(\mathfrak{g})\). We know that \(\mathfrak{g}/{\rm
Rad}(\mathcal{O}(\mathfrak{g}'_J))\) has an abelian complex structure. By Theorem 42, there exists a \(J\)-semisimple subalgebra
\(\mathfrak{s}\) such that \[\frac{\mathfrak{g}}{{\rm Rad}(\mathcal{O}(\mathfrak{g}'_J))}=\mathfrak{s}\ltimes \frac{{\rm Rad}(\mathfrak{g})}{{\rm Rad}(\mathcal{O}(\mathfrak{g}'_J))}\,,
\quad \mathfrak{s}\simeq \frac{\mathfrak{g}}{{\rm Rad }(\mathfrak{g})}\,.\] Consider the \(J\)-invariant subalgebra \(\hat{\mathfrak{s}}=\pi^{-1}(\mathfrak{s})\) of \(\mathfrak{g}\), where \(\pi\colon \mathfrak{g} \to \frac{\mathfrak{g}}{{\rm Rad}(\mathcal{O}(\mathfrak{g}'_J))}\) is the canonical projection onto the quotient. As in Step 1 of Theorem 42, we deduce \({\rm Rad}(\hat{\mathfrak{s}})={\rm Rad}(\mathcal{O}(\mathfrak{g}'_J))\). This, together with the fact that \(\mathfrak{s}=\hat{\mathfrak{s}}/{\rm Rad}(\mathcal{O}(\mathfrak{g}'_J))\) is \(J\)-perfect, implies that \(\hat{\mathfrak{s}}\subseteq
\mathcal{O}(\mathfrak{g}'_J)\). Using this last fact and the fact that \(\hat{\mathfrak{s}}\) is a subalgebra, we see that \(\hat{ \mathfrak{s}}\) acts holomorphically on \(\hat{\mathfrak{s}}_J'\). Now, by Corollary 55, we observe that \[\begin{align} \frac{\hat{\mathfrak{s}}}{{\rm
Rad}(\hat{\mathfrak{s}})}\simeq \frac{\mathfrak{g}}{{\rm Rad}(\mathfrak{g})}=\frac{\mathcal{O}(\mathfrak{g}'_J)+{\rm Rad}(\mathfrak{g})}{{\rm Rad}(\mathfrak{g})}\simeq \frac{\mathcal{O}(\mathfrak{g}'_J)}{{\rm Rad}(\mathfrak{g})\cap
\mathcal{O}(\mathfrak{g}'_J)}=\frac{\mathcal{O}(\mathfrak{g}'_J)}{{\rm Rad}(\mathcal{O}(\mathfrak{g}'_J))}
\end{align}\] Thus, we are in the position to apply Lemma 49 to conclude that \(H^2(\hat{\mathfrak{s}},
JU_{\hat{\mathfrak{s}}})=0\). Hence, \(\hat{\mathfrak{s}}\) satisfies the hypotheses of Theorem 51, which allows us to write \(\hat{\mathfrak{s}}=\mathfrak{h}\ltimes {\rm Rad}(\mathcal{O}(\mathfrak{g}'_J)).\) It follows that \(\mathfrak{g}=\mathfrak{h}\ltimes {\rm Rad}(\mathfrak{g})\), which concludes the existence
part of the theorem.
The only thing left to prove is uniqueness of the \(J\)-adapted Levi subalgebra. The argument is by induction on \(\dim_{\mathbb{C}}\mathfrak{g}\) and goes as in the proof of Theorem 42, replacing \(\mathfrak{z}(\mathfrak{g})\) with \(\mathfrak{g}'_J\). The only case that is slightly
different is when \(\mathfrak{g}\) is \(J\)-perfect and \(0\neq \mathfrak{g}'_J={\rm Rad}(\mathfrak{g})\), so we provide some details. Let \(\mathfrak{h}_1,\mathfrak{h}_2\) be \(J\)-adapted Levi subalgebras of \(\mathfrak{g}\). Let \(p_{\mathfrak{h}_1}\) and \(p_{\mathfrak{g}'_J}\) be the holomorphic projections of \(\mathfrak{g}\) onto \(\mathfrak{h}_1\) and \(\mathfrak{g}'_J\), respectively. For any \(Z_1, Z_2\in \mathfrak{h}_2\), we have \[p_{\mathfrak{h}_1}([Z_1, Z_2])+ p_{\mathfrak{g}'_J}([Z_1, Z_2])=[Z_1,
Z_2]=[p_{\mathfrak{h}_1}(Z_1), p_{\mathfrak{h}_1}(Z_2)]+[p_{\mathfrak{h}_1}(Z_1), p_{\mathfrak{g}'_J}(Z_2)]+[p_{\mathfrak{g}'_J}(Z_1), p_{\mathfrak{h}_1}(Z_2)]\,,\] and thus \(p_{\mathfrak{h}_1}\) is a
holomorphic Lie algebra homomorphism and \[\label{boloseipazzo}
p_{\mathfrak{g}'_J}([Z_1, Z_2])=[p_{\mathfrak{h}_1}(Z_1), p_{\mathfrak{g}'_J}(Z_2)]+[p_{\mathfrak{g}'_J}(Z_1), p_{\mathfrak{h}_1}(Z_2)]\,.\tag{18}\] Now, choosing \(Z_1=JU_{\mathfrak{h}_2}\) and
\(Z_2\in \mathfrak{h}_2'\), we get from 18\[2p_{\mathfrak{g}'_J}(Z_2)=[JU_{\mathfrak{h}_1}, p_{\mathfrak{g}'_J}(Z_2)]\,,\] where we used \(2\)-step solvability and the fact that \(p_{\mathfrak{h}_1}(JU_{\mathfrak{h}_2})=JU_{\mathfrak{h}_1}\), thanks to Lemma 35, since \(p_{\mathfrak{h}_1}\vert_{\mathfrak{h}_2}\) is a holomorphic Lie algebra isomorphism. But then \(p_{\mathfrak{g}'_J}(Z_2)\) must vanish, since
otherwise \(2\) would be an eigenvalue for \(\operatorname{ad}_{JU_{\mathfrak{h}_1}}\vert_{\mathfrak{g}'_J}\), which is prohibited by our assumptions. As \(\mathfrak{h}_2\) is \(J\)-perfect we infer \(p_{\mathfrak{g}'_J}|_{\mathfrak{h}_2}=0\) and thus \(\mathfrak{h}_2=\mathfrak{h}_1\), as desired. ◻
We now show that whenever there is an SKT metric compatible with the complex structure the obstruction to the existence of the Levi–Malcev decomposition vanishes.
Theorem 57. Let \(\mathfrak{g}\) be a \(2\)-step solvable SKT Lie algebra. Then \(H^2(\mathfrak{g},JU)=0\). As a consequence, \[\mathfrak{g}=\mathfrak{aff}(\mathbb{R})^p\ltimes {\rm Rad}(\mathfrak{g})\,,\] for some \(p\ge 0\).
Proof. We know that \(\mathcal{O}(\mathfrak{g}_J')\) is a \(J\)-invariant ideal of \(\mathfrak{g}\) which inherits an SKT metric. Since \(\mathfrak{g}_J'\) is a \(J\)-invariant ideal of \(\mathcal{O}(\mathfrak{g}'_J)\), we can use Theorem 42 to infer that \[\frac{\mathcal{O}(\mathfrak{g}'_J)}{\mathfrak{g}_J'}=\mathfrak{h}\ltimes \frac{{\rm Rad}(\mathcal{O}(\mathfrak{g}'_J))}{\mathfrak{g}_J'}\,, \quad
\mathfrak{h}\simeq \frac{\mathcal{O} (\mathfrak{g}_J')}{{\rm Rad}(\mathcal{O}(\mathfrak{g}_J'))}\,.\] We consider the subalgebra \(\mathfrak{h}_U=\langle U, JU \rangle\) of \(\mathfrak{h}\) and its preimage \(\pi^{-1}(\mathfrak{h}_U)\) via the canonical projection onto the quotient \(\pi\colon \mathcal{O}(\mathfrak{g}'_J) \to
\mathcal{O}(\mathfrak{g}'_J)/ \mathfrak{g}_J'\). Observe that \(\pi^{-1}(\mathfrak{h}_U)\) is an almost-abelian \(J\)-invariant subalgebra of \(\mathfrak{g}\). Indeed, \(\mathfrak{a}:=\pi^{-1}(\langle U\rangle)=\pi^{-1}(\mathfrak{h}_U')\) is an abelian ideal of \(\pi^{-1}(\mathfrak{h}_U)\), since
\(U\in (\mathcal{O}(\mathfrak{g}'_J)/\mathfrak{g}_J')'=\mathcal{O}(\mathfrak{g}'_J)'/\mathfrak{g}_J'\) and \(\mathfrak{g}\) is \(2\)-step solvable. Since \(\mathcal{O}(\mathfrak{g}'_J)\) is SKT, \(\pi^{-1}(\mathfrak{h}_U)\) admits an SKT metric \(g\).
We consider an orthogonal complement \(\langle U', JU'\rangle\) of \(\mathfrak{g}_J'\) in \(\pi^{-1}(\mathfrak{h}_U)\) with respect to \(g\). Clearly \(U'=bU+X\), for some \(X\in\mathfrak{g} _J'\) and \(b\in \mathbb{R}\). Therefore, we have \([JU',U' ]=2bU'+ v,\) for some \(v\in\mathfrak{g}_J'\), and thus \(\operatorname{ad}_{JU'}|_{\mathfrak{g}_J'}=b\operatorname{ad}_{JU}|_{\mathfrak{g}_J'}\). We can further suppose, up to scaling, that \(|U'|_g=1\). Now, we are in the position to
apply [58] or [59] with \(a=2b\), to
infer that the real parts of the eigenvalues of \(\operatorname{ad}_{JU}|_{\mathfrak{g}_J'}\) are either \(0\) or \(-1\). This concludes the proof of the
first part.
We can now apply Theorem 56 to obtain \[\mathfrak{g}=\mathfrak{h}\ltimes {\rm Rad}(\mathfrak{g})\,,\] where \(\mathfrak{h}\) is a \(J\)-semisimple subalgebra. Using Corollary 33, we have that \(\mathfrak{h}\) is a direct sum of \(p\) copies of \(\mathfrak{aff}(\mathbb{R})\) and \(q\) copies of \(\mathfrak{aff}(\mathbb{C})\). On the other hand, \(\mathfrak{h}\) is again SKT and hence \(q=0\), since \(\mathfrak{aff}(\mathbb{C})\) does not admit any SKT metric. ◻
In this subsection, we explore the relation between \(J\)-solvability of a Lie algebra and the vanishing of the form \(\eta\), defined in 2 . For starters, we
relate \(\eta\) to the \(J\)-solvable radical in a class of Lie algebras that includes \(J\)-perfect ones. This will be useful in what follows.
Proposition 58. Let \(\mathfrak{g}= \mathfrak{a}+ J \mathfrak{a}\) be a solvable Lie algebra such that \(\mathfrak{a}\) is an abelian ideal and \(\mathfrak{g}_J'\subseteq \mathfrak{a}_J\). Then, \(\mathfrak{g}'\subseteq \mathfrak{a}\), \(\mathfrak{a}_J\) is an ideal in \(\mathfrak{g}\) and \[\eta=\pi^*\eta_{\mathfrak{g}/\mathfrak{a}_J}\,,\] where \(\pi\colon \mathfrak{g} \to \mathfrak{g}/\mathfrak{a}_J\) is the canonical
projection onto the quotient. Moreover, \(\ker \eta={\rm Rad}(\mathfrak{g})\).
Proof. Firstly, we prove that \(\mathfrak{g}'\subseteq \mathfrak{a}\). Since \(\mathfrak{a}\) is an ideal, it is sufficient to prove that \([J\mathfrak{a},J\mathfrak{a}]\subseteq \mathfrak{a}\). Fix \(X, Y\in\mathfrak{a}\), exploiting integrability, we have \[\mathfrak{g}'\ni [JX, JY]=J([JX, Y]+[X,
JY])\in J \mathfrak{g}'\,,\] concluding that \([JX, JY]\in\mathfrak{g}_J'\subseteq \mathfrak{a}_J\). Similarly to the proof of Lemma 4 we deduce that \(\mathfrak{a}_J\) is an ideal. In addition, using that \(\mathfrak{a}_J\) is abelian, for every \(X\in
\mathfrak{a}_J\) and \(Y\in \mathfrak{g}\) we have \(\operatorname{Im}(J\operatorname{ad}_{[X, Y]})\subseteq \mathfrak{a}_J\) and \(J\operatorname{ad}_{[X,
Y]}|_{\mathfrak{a}_J}=0\). Consequently \[\eta(X, Y)=-\frac{1}{2}{\rm tr}(J\operatorname{ad}_{[X,Y]})=0\,, \qquad X\in \mathfrak{a}_J\,,\,\,Y \in\mathfrak{g}\,,\] showing that \(\mathfrak{a}_J \subseteq \ker \eta\). Consider a Hermitian metric \(g\) and fix \(Y\in (\mathfrak{a}_J)^{\perp}\cap \mathfrak{a}\), where the orthogonal is with
respect to \(g\). Since \(\mathfrak{a}\) is an abelian ideal, \([Y, JY]\in\mathfrak{a}\) and we have that \(\operatorname{ad}_{[Y,
JY]}\vert_{\mathfrak{a}_J}=0\). Thus \[\begin{align}
\eta(Y, JY)&=-\frac{1}{2} \operatorname{tr}(J\operatorname{ad}_{[Y,JY]} \vert_{\mathfrak{a}_J})- \frac{1}{2}\operatorname{tr}(J
\operatorname{ad}_{[Y,JY]}\vert_{(\mathfrak{a}_J)^\perp})=-\frac{1}{2}\operatorname{tr}(J\operatorname{ad}_{[Y,JY]^{\perp}}\vert_{ (\mathfrak{a}_J)^{\perp}})\,,
\end{align}\] where \([Y,JY]^{\perp}\) is the orthogonal projection on \((\mathfrak{a}_J)^{\perp}\). Thus, we obtain that \[\eta(Y, JY)
=-\frac{1}{2}{\rm tr}^{\mathfrak{g}/\mathfrak{a}_J}(J\operatorname{ad}_{[\pi(Y), J\pi(Y)]})\,.\] The claim that \(\eta=\pi^*\eta_{\mathfrak{g}/\mathfrak{a}_J}\) follows from the above equation and from the inclusion
\(\mathfrak{a}_J\subseteq \ker \eta\).
Furthermore, we note that \(\ker \eta=\pi^{-1}(\ker\eta_{\mathfrak{g}/\mathfrak{a}_J})=\pi^{-1}(\mathfrak{n}_J)\), where \(\mathfrak{n}_J\) is the maximal nilpotent \(J\)-invariant ideal of \(\mathfrak{g}/\mathfrak{a}_J\). Using that \(\pi\) is a holomorphic Lie algebra homomorphism, we get that \(\ker \eta\) is a \(J\)-invariant ideal of \(\mathfrak{g}\). Finally, by Lemma 12\(\ker\eta\) is also \(J\)-solvable. Thus, \(\ker \eta\subseteq {\rm Rad}(\mathfrak{g})\).
Next, we claim that \(\mathfrak{n}_J={\rm Rad}(\mathfrak{g}/ \mathfrak{a}_J)\). Indeed, since \(\mathfrak{g}_J'\subseteq \mathfrak{a}_J\), we have that \(\mathfrak{g}/\mathfrak{a}_J\) has an abelian complex structure \(J\). Moreover, clearly, \(\mathfrak{g}/\mathfrak{a}_J=\mathfrak{a}/\mathfrak{a}_J\oplus J
\mathfrak{a}/\mathfrak{a}_J.\) In addition, since \(\mathfrak{g}'\subseteq \mathfrak{a}\), we obtain \((\mathfrak{g}/\mathfrak{a}_J)'_J=(\mathfrak{g}'/\mathfrak{a}_J)\cap
J(\mathfrak{g}'/\mathfrak{a}_J)\subseteq (\mathfrak{a}/\mathfrak{a}_J)\cap J(\mathfrak{a}/\mathfrak{a}_J)=0\). Then, using Theorem 41, we conclude the proof of the
claim. In particular, since \[\frac{\mathfrak{g}}{\ker \eta}\simeq \frac{\mathfrak{g}/\mathfrak{a}_J}{\pi^{-1}(\mathfrak{n}_J)/\mathfrak{a}_J}\simeq \frac{\mathfrak{g}/\mathfrak{a}_J}{\mathfrak{n}_J}\,,\]this gives that
\(\mathfrak{g}/ \ker \eta\) is \(J\)-semisimple and hence \({\rm Rad}(\mathfrak{g})=\ker \eta\), which concludes the proof. ◻
Proposition 58 allows us to relate \(J\)-solvability with the vanishing of \(\eta\), as follows.
Proposition 59. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra endowed with a complex structure \(J\). Then \(\eta=0\) if and only if \(\mathfrak{g}\) is \(J\)-solvable. In particular, \(\frac{\mathfrak{g}'+J\mathfrak{g}'
}{\mathfrak{g}_J'}\) is nilpotent.
Proof. It is easy to see that \(\eta|_{\mathfrak{\mathfrak{g}}'+J\mathfrak{g}' }=\eta_{\mathfrak{g}'+J\mathfrak{g}' }\,\). We observe that, since \(\mathfrak{g}\)
is a \(2\)-step solvable Lie algebra, \(\mathfrak{g}'\) is an abelian ideal of \(\mathfrak{g}'+J\mathfrak{g}'\). We are in the position to apply
Proposition 58 to \(\mathfrak{g}'+J\mathfrak{g}'\), and obtain, assuming \(\eta=0\), that \(\mathfrak{g}'+J\mathfrak{g}'={\rm Rad}(\mathfrak{g}'+J\mathfrak{g}')\), which clearly gives that \(\mathfrak{g}\) is \(J\)-solvable.
Viceversa, let us suppose that \(J\) is solvable. In particular, by Proposition 58, \(\mathfrak{g}'+J\mathfrak{g}'\) is \(J\)-solvable and equal to \(\ker \eta_{\mathfrak{\mathfrak{g}}'+J\mathfrak{g}'}=\pi^{-1}(\mathfrak{n}_J)\),
where \(\pi\colon \mathfrak{g}'+J\mathfrak{g}' \to (\mathfrak{g}'+J\mathfrak{g}')/\mathfrak{g}_J'\) is the canonical projection onto the quotient and \(\mathfrak{n}_J\)
is the maximal \(J\)-invariant nilpotent ideal of \((\mathfrak{g}'+J\mathfrak{g}')/\mathfrak{g}_J'\). Thus, \((
\mathfrak{g}'+J\mathfrak{g}')/\mathfrak{g}_J'=\mathfrak{n}_J\) is nilpotent. We will use this piece of information to conclude that \(\eta=0\). We know that \(\eta=0\) is
equivalent to require that \(\beta|_{\mathfrak{g}'}=0\), where \(\beta\) is the potential \(1\)-form of \(\eta\), see 3 . Since \(\mathfrak{g}_J'\) is an abelian ideal in \(\mathfrak{g}'+J\mathfrak{g}'\) by Lemma 4, we observe that \(\mathfrak{g}'_J \subseteq \ker \beta\). Now, let \(X\in\mathfrak{g}'\), we have \[\beta(X)=\frac{1}{2}{\rm tr}(J\operatorname{ad}_X|_{\mathfrak{g}'+J\mathfrak{g}'})=\frac{1}{2}{\rm tr}^{\mathfrak{n}_J}(J\operatorname{ad}_{\pi(X)})+\frac{1}{2}{\rm
tr}(J\operatorname{ad}_X|_{\mathfrak{g}'_J})=\pi^*\beta_{\mathfrak{n}_J}(X)\,,\] where we used that \(\operatorname{ad}_X|_{\mathfrak{g}_J'}=0\), because \(X\in
\mathfrak{g}'\). Now, thanks to [60], we know that \(\beta_{\mathfrak{n}_J}=0\), since \(\mathfrak{n}_J\) is nilpotent. This concludes the proof. ◻
Theorem 60. Let \(\mathfrak{g}\) be a \(2\)-step solvable unimodular Lie algebra endowed with a complex structure \(J\). If there
exist both an SKT metric and a balanced metric compatible with \(J\), then \(J\) is solvable. In particular, there also exists a Kähler metric compatible with \(J\).
Proof. Applying Theorem 57 we immediately know that \(\mathfrak{g}=\mathfrak{aff}(\mathbb{R})^p\ltimes {\rm Rad}(\mathfrak{g}),\) for
some \(p\ge 0\). Suppose by contradiction that \(p\neq 0\) and consider the holomorphic quotient map \(\pi \colon \mathfrak{g}\to \mathfrak{g}/{\rm
Rad}(\mathfrak{g})\simeq \mathfrak{aff}(\mathbb{R})^p\). We know that \(\mathfrak{aff}(\mathbb{R})^p\) is endowed with an exact Kähler form \(-\eta\). Therefore, \(-\pi^*\eta\) gives rise to a non-zero, semi-positive \((1,1)\)-form which is exact. We can now use Corollary 18 to
conclude \(p=0\) and thus \(\mathfrak{g}\) must be \(J\)-solvable. In particular, Proposition 59 tells us that \(\rho=0\). In this scenario we can then infer that there exists a Kähler metric invoking [36]. ◻
From Proposition 58 we can characterise the signature of the form \(\eta\) on any \(J\)-perfect \(2\)-step solvable Lie algebra.
Corollary 61. Let \(\mathfrak{g}\) be a \(J\)-perfect \(2\)-step solvable Lie algebra and let \(\mathfrak{g}/\ker \eta\simeq \mathfrak{aff}(\mathbb{R})^p\oplus \mathfrak{aff}(\mathbb{C})^q\). Then, the signature of \(\eta\) is \((2p+2q,2q, 2k)\) where \(k=\dim_{\mathbb{C}}\ker \eta.\) In particular, \(\eta \le 0\) if and only if \(\mathfrak{g}/\ker \eta\) is the direct sum of \(p\) copies of \(\mathfrak{ aff}(\mathbb{R}).\)
Proof. By Proposition 58 and Theorem 41, we know that \(\eta=\pi^*\eta_{\mathfrak{g}/\mathfrak{g}'_J}\) and \(\mathfrak{g}/\mathfrak{g}'_J=\mathfrak{h}\ltimes \mathfrak{n}_J\), where \(\mathfrak{n}_J=\ker
\eta_{\mathfrak{g}/\mathfrak{g}'_J}\) and \(\mathfrak{h}\simeq \mathfrak{g}/\ker \eta\). Since \(\eta_{\mathfrak{g}/\mathfrak{g}'_J}\) makes the \(J\)-simple ideals of \(\mathfrak{h}\) orthogonal, the conclusion follows from Corollary 43. ◻
Example 5 is a \(J\)-perfect \(3\)-step solvable Lie algebra and it is straightforward to
check that \(\rho=\eta=0\). Hence, one implication of Proposition 59 is no longer true for higher solvability steps.
By means of Proposition 59, we can also prove the converse of Corollary 44, part
(1).
Corollary 62. Let \(\mathfrak{g}\) be a Lie algebra endowed with a solvable abelian complex structure \(J\). Then \(\mathfrak{g}'+J\mathfrak{g}'\) is unimodular.
Proof. Using Proposition 59, we have that \(\eta=0\), which is equivalent to \(\beta|_{\mathfrak{g}'}=0\). The claim then follows from the abelianity of \(J\) and the observation that, for any \(X\in\mathfrak{g}'\), \(\beta(X)=-\frac{1}{2}{\rm tr}(\operatorname{ad}_{JX})=0.\) ◻
The aim of this subsection is to present the proof of Theorem 4. We first prove the following proposition.
Proposition 63. Let \(\mathfrak{g}\) be a unimodular, solvable Lie algebra endowed with a complex structure such that there exists a \(J\)-invariant abelian ideal
\(\mathfrak{a}\) satisfying \(\mathfrak{g}_J'\subseteq \mathfrak{a} \subseteq C(\mathfrak{g}')\). Assume that \(\mathfrak{g}\) admits an SKT metric
\(g\), then \(\rho \le 0\). If \(\rho=0\), \(\operatorname{ad}_X|_{\mathfrak{a}}\in \mathfrak{su}(\mathfrak{a}, g )\), for
any \(X\in\mathfrak{g}\). In these last hypotheses, if \(\mathfrak{g}\) is completely solvable, then \(\mathfrak{a}\subseteq \mathfrak{z}(\mathfrak{g}).\) In
particular, if \(\mathfrak{g}\) is \(2\)-step, then \(\mathfrak{g}'+J\mathfrak{g}'\) is \(2\)-step
nilpotent.
Proof. Using the same argument as in the proof of Proposition 58, we infer that \(\mathfrak{a}\subseteq \ker \rho.\) Now, we
decompose \(\mathfrak{g}=\mathfrak{a}^{\perp}\oplus \mathfrak{a}\), where the orthogonal complement is taken with respect to \(g\). As a consequence, for the claim to be true it suffices to
prove that \(\rho(X, JX)\le 0\), for all \(X\in\mathfrak{a}^{\perp}\). For any such \(X\), since \(\mathfrak{a} \subseteq
C(\mathfrak{g}')\) and \(\mathfrak{a}\) is an ideal, we have \[\begin{align}
\rho(X, JX)=&\, -\frac{1}{2}{\rm tr}(J\operatorname{ad}_{[X, JX]}|_{\mathfrak{a}^{\perp}})-\frac{1}{2}{\rm tr}(J\operatorname{ad}_{[X, JX]}|_{\mathfrak{a}})
= -\frac{1}{2}{\rm tr}(J\operatorname{ad}_{[X, JX]}|_{\mathfrak{a}^{\perp}})\\
=&\, -\frac{1}{2}{\rm tr}(J\operatorname{ad}_{[X, JX]^{\perp}}|_{\mathfrak{a}^{\perp}})=-\frac{1}{2}{\rm tr}^{\mathfrak{g}/\mathfrak{a}}(J\operatorname{ad}_{\pi([X, JX])})\,,
\end{align}\] where \(\pi \colon \mathfrak{g}\to \mathfrak{g}/\mathfrak{a}\) is the canonical projection onto the quotient and \([X, JX]^{\perp}\) is the orthogonal projection of
\([X, JX]\) onto \(\mathfrak{a}^{\perp}\). Exploiting the fact that \(\mathfrak{g}/\mathfrak{a}\) has an abelian complex structure, since \(\mathfrak{g}_J'\subseteq \mathfrak{a}\), we infer \[\begin{align}
\rho(X, JX)=&\, -\frac{1}{2}{\rm tr}^{\mathfrak{g}/\mathfrak{a}}(J\operatorname{ad}_{\pi([X, JX])})=\frac{1}{2}{\rm tr}^{\mathfrak{g}/\mathfrak{a}}(\operatorname{ad}_{\pi(J[X, JX])})
=\frac{1}{2}{\rm tr}(\operatorname{ad}_{J[X, JX]}|_{\mathfrak{a}^{\perp}})=-\frac{1}{2}{\rm tr}(\operatorname{ad}_{J[X, JX]}|_{\mathfrak{a}})\,,
\end{align}\] where we used once again that \(\mathfrak{a}\) is an abelian ideal of \(\mathfrak{g}\) and unimodularity. Now, we apply Lemma 19 choosing \(Y\in \mathfrak{a}\), and obtain \[\begin{align}
0=&\,g([J[X, JX], JY], JY)+g([J[X, JX], Y],Y) +g([J[X, Y], X], JY)-g([J[X, JY], X], Y)\\
&\, +g([J[JX, Y], JX], JY) -g([J[JX, JY], JX], Y) -|[X, Y]|^2-|[X, JY]|^2\\
&\, - |[JX, Y]|^2-|[JX, JY]|^2\,.
\end{align}\] Summing over an orthonormal basis of \(\mathfrak{a}\) with respect to \(g\), we have \[\begin{align}
{\rm tr}(\operatorname{ad}_{J[X, JX]}|_{\mathfrak{a}})=- {\rm tr}((J\operatorname{ad}_X)^2|_{\mathfrak{a}})-{\rm tr}((J{\operatorname{ad}_{JX}})^2|_{\mathfrak{a}})+|\operatorname{ad}_X|_{\mathfrak{a}}|^2+|\operatorname{ad}_{JX}|_{\mathfrak{a}}|^2\,.
\end{align}\] On the other hand, by integrability of \(J\), we obtain \[\begin{align}
0&=\mathrm{tr}(J\operatorname{ad}_{[X,JX]}|_{\mathfrak{a}})
=\mathrm{tr}(J\operatorname{ad}_X\operatorname{ad}_{JX}|_{\mathfrak{a}})-\mathrm{tr}(J\operatorname{ad}_{JX}\operatorname{ad}_X|_{\mathfrak{a}})\\
&=-\mathrm{tr}(J\operatorname{ad}_X\operatorname{ad}_{X}J|_{\mathfrak{a}})+\mathrm{tr}(J\operatorname{ad}_XJ\operatorname{ad}_{X}|_{\mathfrak{a}})-\mathrm{tr}(J\operatorname{ad}_XJ\operatorname{ad}_{JX}J|_{\mathfrak{a}})-\mathrm{tr}(J\operatorname{ad}_{JX}\operatorname{ad}_X|_{\mathfrak{a}})
\\
&=\mathrm{tr}\left((\operatorname{ad}_X)^2|_{\mathfrak{a}}\right)+\mathrm{tr}\left((J\operatorname{ad}_X)^2|_{\mathfrak{a}}\right)\,.
\end{align}\] Hence, using the above equation, we get \[\begin{align}
\rho(X, JX)=-\frac{1}{2}{\rm tr}(\operatorname{ad}_{J[X, JX]}|_{\mathfrak{a}})=&\, -\frac{1}{2}\left( {\rm tr}((\operatorname{ad}_X)^2|_{\mathfrak{a}})+{\rm
tr}(({\operatorname{ad}_{JX}})^2|_{\mathfrak{a}})+|\operatorname{ad}_X|_{\mathfrak{a}}|^2+|\operatorname{ad}_{JX}|_{\mathfrak{a}}|^2\right)\\
=&\, -2(|{\rm Sym}(\operatorname{ad}_X|_{\mathfrak{a}})|^2+|{\rm Sym}(\operatorname{ad}_{JX}|_{\mathfrak{a}})|^2)\le 0\,.
\end{align}\] If \(\rho=0\), then clearly \(\operatorname{ad}_X|_{\mathfrak{a}}\in \mathfrak{so}(\mathfrak{a}, g)\). The only thing remained to check is that \([\operatorname{ad}_X, J]|_{\mathfrak{a}}=0\), for any \(X\in\mathfrak{a}^{\perp}\). Recalling the proof of Lemma 21,
we have \[\frac{1}{2}{\rm tr}([\operatorname{ad}_X|_{\mathfrak{a}}, J|_{\mathfrak{a}}]^2 )=\frac{1}{2}{\rm tr}([\operatorname{ad}_X, J]^2 |_{\mathfrak{a}})={\rm tr}(J\operatorname{ad}_{[X, JX]}|_{\mathfrak{a}})=0\,.\] On
the other hand, since \(\operatorname{ad}_{X}|_{\mathfrak{a}}, J\in\mathfrak{so}(\mathfrak{a}, g)\), then \([\operatorname{ad}_X, J]|_{\mathfrak{a}}\in \mathfrak{so}(\mathfrak{a}, g)\).
Hence, \({\rm tr}([\operatorname{ad}_X, J]^2|_{\mathfrak{a}})=0\) if and only if \([\operatorname{ad}_X, J]|_{\mathfrak{a}}=0\). Finally, if we assume that \(\mathfrak{g}\) is completely solvable, then \(\operatorname{ad}_X|_{\mathfrak{a}}=0\), for any \(X\in\mathfrak{g}\), forcing \(\mathfrak{g}_J'\subseteq\mathfrak{a}\subseteq \mathfrak{z}(\mathfrak{g}).\) Now, if \(\mathfrak{g}\) is \(2\)-step with \(\rho=0\), then \(J\) is solvable and \((\mathfrak{g}'+J\mathfrak{g}')/\mathfrak{g}_J'\) is nilpotent, by Proposition 59. This, together with the fact that \(\mathfrak{g}_J'\) is central, gives that \(\mathfrak{g}'+J \mathfrak{g}'\) is
nilpotent and hence \(2\)-step since it is SKT, see [50]. ◻
Remark 64. Let \(\mathfrak{g}\) be a \(2\)-step solvable Lie algebra. We consider \(N_{\mathfrak{g}}:=N_{\mathfrak{g}}(\mathfrak{g}_J')\), the normaliser of \(\mathfrak{g}_J'\) in \(\mathfrak{g}\), and note that \(N_{\mathfrak{g} }\) is an ideal of \(\mathfrak{g}\), since \(\mathfrak{g}'+J \mathfrak{g}' \subseteq N_{\mathfrak{g}}\) by Lemma 4. Moreover, \(N_{\mathfrak{g}}\) is \(J\)-invariant. Indeed, using ?? , for any \(X\in
N_{\mathfrak{g}}\) and \(Y\in \mathfrak{g}_J'\), we have that \([JX, Y]
\in \mathfrak{g}_J'\) implying that \(JX\in N_{\mathfrak{g}}\). Thus, if \(\mathfrak{g}\) is a unimodular, SKT, 2-step solvable Lie algebra, then, \(N_{\mathfrak{g}}\) has the same properties and contains \(\mathfrak{g}_J'\) as an ideal. Most importantly, we note that \(N_{\mathfrak{g}}\) satisfies the
hypotheses of Proposition 63 with \(\mathfrak{a}=\mathfrak{g}_J'\).
The next lemma collects some interesting facts on solvable abelian complex structures.
Lemma 65. Let \(\mathfrak{g}\) be a Lie algebra endowed with a solvable and abelian complex structure \(J\). Then, the Killing form \(B\) is of type \((2,0)+(0,2)\) and \(\ker B\) is a \(J\)-invariant ideal. Moreover, the nilradical \(\mathfrak{n}\) of \(\mathfrak{g}\) is \(J\)-invariant. In particular, \(\mathfrak{g}'+J\mathfrak{g}'\) is
nilpotent.
Proof. By Corollary 62, we know that \(\mathfrak{g}'+J\mathfrak{g}'\) is unimodular. Using this fact and Proposition 24, part (2), we deduce that \(B^{1,1}=0\), thereby proving the first statement. It follows that \(\ker
B\) is \(J\)-invariant ideal, since \(\mathfrak{n} \subseteq \ker B\). Let us now fix \(X\in \mathfrak{n}\) and we prove that \({\rm tr}(\operatorname{ad}_{JX}^k)=0\), for any \(k\ge 2\).
For \(k=2\), we have that \[0=B(X, X)=-B(JX, JX)=-{\rm tr}(\operatorname{ad}_{JX}^2)\,.\] Now, let us suppose that \(k\ge 3\). The strategy is the same
as in the proof of Proposition 24, part (4). Using ?? and Lie’s Theorem, we can conclude, iterating \(k-1\) times the argument, that
\[{\rm tr}(\operatorname{ad}_{JX}^k)={\rm tr}(\operatorname{ad}_{JX}^{k-2}\operatorname{ad}_{J[JX, X]})={\rm tr}(\operatorname{ad}_{J[JX, [JX, \ldots, [JX, X]]\ldots]})=0\,,\] by unimodularity of \(\mathfrak{g}'+J\mathfrak{g}'\). Hence, \({\rm tr}(\operatorname{ad}_{JX}^k)=0\), for any \(k\ge 2\), which implies \(JX\in
\mathfrak{n}\), and thus forces \(\mathfrak{n}\) to be \(J\)-invariant. ◻
As consequence of the previous lemma we deduce the following.
Corollary 66. Let \((\mathfrak{g}, J)\) be a Lie algebra endowed with an abelian complex structure \(J\).
If \(\mathfrak{g}\) is completely solvable and \(J\) is solvable, then \(\mathfrak{g}\) is nilpotent.
If \(\mathfrak{g}\) is of rigid type, then it is nilpotent.
Proof. We prove (1). The proof of (2) is similar once one observes that Lie algebras of rigid type are always unimodular, hence \(J\)-solvable by Corollary 44, part (1). Applying Lemma 65, we know that the Killing form is of type \((2,0)+(0,2)\). On the other hand, by complete solvability, we have \[0\le {\rm tr}(\operatorname{ad}_X^2)=B(X, X)=-B(JX, JX)=-{\rm tr}(\operatorname{ad}_{JX}^2)\le 0\,,\] and hence \({\rm tr}(\operatorname{ad}^2_X)=0\), for any \(X\in\mathfrak{g}\). Using again complete solvability, \({\rm tr}(\operatorname{ad}_X^2)=0\) implies that \(\operatorname{ad}_X\) is nilpotent, for any \(X\in\mathfrak{g}\), concluding the proof. ◻
Theorem 67. Let \(\mathfrak{g}\) be a unimodular, SKT, \(2\)-step completely solvable Lie algebra endowed with a solvable complex structure. Then \(\mathfrak{g}\) is nilpotent. Consequently, any unimodular, SKT, \(2\)-step completely solvable Lie algebra \(\mathfrak{g}\) satisfies \[\mathfrak{g}=\mathfrak{aff}(\mathbb{R})^p\ltimes \mathfrak{n}_J\,\] for some \(p\ge 0\).
Proof. As for the first claim, by Remark 64, the normaliser \(N_{\mathfrak{g}}\) of \(\mathfrak{g}_J'\) in \(\mathfrak{g}\) satisfies the hypotheses of Proposition 63. Furthermore \(N_{\mathfrak{g}}\) is \(J\)-solvable and completely solvable. Applying the last part of Proposition 63, we have
that \(\mathfrak{g}_J'\subseteq \mathfrak{z}(N_{\mathfrak{g}})\cap (\mathfrak{g}'+J \mathfrak{g}')\subseteq \mathfrak{z}(\mathfrak{g}'+J \mathfrak{g}')\). Since \(J\) is
solvable, we know that \((\mathfrak{g}'+J\mathfrak{g}')/ \mathfrak{g}_J'\) is nilpotent and \(\mathfrak{g}_J'\subseteq \mathfrak{z}(\mathfrak{g}'+J \mathfrak{g}')\),
implying that \(\mathfrak{g}'+J \mathfrak{g}'\) is nilpotent and SKT. Using [51], we obtain that \(\mathfrak{z}(\mathfrak{g}'+J \mathfrak{g}')\) is \(J\)-invariant. Hence, we are in the position to apply Proposition 63 with \(\mathfrak{a}=\mathfrak{z}(\mathfrak{g}'+J \mathfrak{g}' )\), which allows us to infer that \(\mathfrak{g}_J'\subseteq\mathfrak{z}(\mathfrak{g}'+J\mathfrak{g}')\subseteq \mathfrak{z}(\mathfrak{g})\). Therefore, taking the quotient by \(\mathfrak{g}_J'\), we obtain a
completely solvable Lie algebra with a solvable abelian complex structure. Now, we can use Corollary 66, part (1), to conclude that \(\mathfrak{g}/\mathfrak{g}_J'\) is nilpotent, which establishes the claim, using that \(\mathfrak{g}_J'\subseteq \mathfrak{z}(\mathfrak{g}).\)
The second claim is now a straightforward consequence of Theorem 57, together with the first part of the proof applied to \({\rm
Rad}(\mathfrak{g})\). ◻
We conclude this subsection inspecting the SKT condition on Lie algebras of real type.
Lemma 68. Le \(\mathfrak{g}\) be an SKT unimodular, \(2\)-step solvable Lie algebra of real type endowed with a solvable complex structure \(J\). Then, \(\mathfrak{g}'+J\mathfrak{g}'\) is \(2\)-step nilpotent.
Proof. We will again make use of Remark 64. We know that \(N_{\mathfrak{g}}\) is a \(J\)-invariant ideal of \(\mathfrak{g}\) that contains \(\mathfrak{g}'+J \mathfrak{g}'\). In addition, \(\mathfrak{g}'_J\) is an ideal of \(N_{\mathfrak{g}}\) that satisfies the hypotheses of Proposition 63. This
allows us to infer that \(\mathfrak{g}'+J\mathfrak{g}'\) acts skew-symmetrically on \(\mathfrak{g}_J'\). On the other hand, being \(J\) solvable,
we know that \(\frac{\mathfrak{g}'+J\mathfrak{g}'}{\mathfrak{g}_J'}\) is nilpotent. Now, using the fact that \(\mathfrak{g}\) is of real type, we can infer that \(\mathfrak{g}'+J\mathfrak{g}'\) is nilpotent and \(\mathfrak{g}_J'\subseteq \mathfrak{z}(\mathfrak{g} '+J \mathfrak{g}')\). Finally, applying [50], we conclude that \(\mathfrak{g}'+J \mathfrak{g}'\) is \(2\)-step nilpotent. ◻
In this subsection we collect some results in full generality, dropping the hypothesis of \(2\)-step solvability. For completely solvable Lie algebras an implication of Proposition 59 can be extended to any solvability step. In order to prove this, we need the following result, which is nothing but an extension of [60].
Proposition 69. Let \(\mathfrak{g}\) be a solvable Lie algebra endowed with a complex structure \(J\). Then
If \(\mathfrak{g}\) is completely solvable, then \(\rho=0\) if and only if \(\sigma=0\).
If \(\mathfrak{g}\) is of rigid type, then any complex structure on \(\mathfrak{g}\) is Chern–Ricci flat.
Proof. Fix an element \(X\in \mathfrak{g}\) and consider the adjoint representation \[\operatorname{ad}_X-\sqrt{-1}\operatorname{ad}_{JX}=\operatorname{ad}_{X^{1,0}}=\begin{pmatrix}
A_X & *\\ 0 & *
\end{pmatrix}\,,\] where the matrix is written with respect to the decomposition \(\mathfrak{g}_\mathbb{C}=\mathfrak{g}^{1,0}\oplus \mathfrak{g}^{0,1}\). By Lie’s Theorem we may pick a basis \(\{Z_1,\dots,Z_{n}\}\) of \(\mathfrak{g}^{1,0}\) with respect to which the block \(A_X\) is upper triangular. Set \(Z_j=\frac{1}{\sqrt{2}}(e_{2j-1}-\sqrt{-1}e_{2j})\) so that \(e_{2j}=Je_{2j-1}\). Choose a Hermitian metric \(g\) on \(\mathfrak{g}\) having \(\{e_1,\dots,e_{2n}\}\) as an orthonormal basis and extend it bilinearly to \(\mathfrak{g}_\mathbb{C}\) so that \(\{Z_1,\dots,Z_{n}\}\) is a unitary basis. We then compute \[\begin{align}
\mathrm{tr}(A_X)&=\sum_{j=1}^{n}g(A_XZ_j,\bar Z_j)=\frac{1}{2}\sum_{j=1}^{n}g\left([X-\sqrt{-1}JX,e_{2j-1}-\sqrt{-1}e_{2j}], e_{2j-1}+\sqrt{-1}e_{2j}\right)\\
&=\frac{1}{2}\left( \mathrm{tr}(\operatorname{ad}_X)-\mathrm{tr}(J\operatorname{ad}_{JX}) - \sqrt{-1}\, \mathrm{tr}(\operatorname{ad}_{JX})-\sqrt{-1}\,\mathrm{tr}(J\operatorname{ad}_X) \right)\,.
\end{align}\] Choosing \(X\in J\mathfrak{n}\) we have that \(\operatorname{ad}_{JX}\) is nilpotent, hence the eigenvalues of \(\operatorname{ad}_{X^{1,0}}\) are those of \(\operatorname{ad}_X\).
In particular, if \(\mathfrak{g}\) is of rigid type, then \(\mathrm{tr}(A_X)\) is purely imaginary, and it follows that \(\mathrm{tr}(J\operatorname{ad}_{JX})=0\), for all \(X\in J\mathfrak{n}\), because \(\mathfrak{g}\) is unimodular. From this we immediately deduce \[\rho(X,Y)=-\frac{1}{2}\mathrm{tr}(J\operatorname{ad}_{[X,Y]})+\frac{1}{2}\mathrm{tr}(\operatorname{ad}_{J[X,Y]})=0\,, \qquad X,Y\in \mathfrak{g}\,,\] which proves (2).
Assume instead that \(\mathfrak{g}\) is completely solvable. Then \(\mathrm{tr}(A_X)\) is real and so \(\mathrm{tr}(J\operatorname{ad}_X)=0\), for all
\(X\in J\mathfrak{n}\). This implies that \(\sigma\) vanishes on \(J\mathfrak{g}'\). On the other hand \(\rho=d\sigma=-\sigma
\vert_{\mathfrak{g}'}\) therefore Chern–Ricci flatness implies that \(\sigma\) vanishes on \(\mathfrak{g}'+J\mathfrak{g}'\). Now, we have \(0=\sigma\vert_{\mathfrak{g}'+J\mathfrak{g}'}=\sigma_{\mathfrak{g}'+J\mathfrak{g}'}\) hence there exists a closed, nowhere vanishing \((k,0)\)-form \(\Psi\) on \(\mathfrak{g}'+J\mathfrak{g}'\), where \(k=\dim_\mathbb{C}(\mathfrak{g}'+J\mathfrak{g}')\), see [61]. Pick an orthogonal complement \(\mathfrak{k}\) of \(\mathfrak{g}'+J\mathfrak{g}'\) in \(\mathfrak{g}\) and a basis \(z_1,\dots,z_{n-k}\) of \(\mathfrak{k}^{1,0}\). Let \(\varphi^1,\dots,\varphi^{n-k}\) be the dual
\((1,0)\)-forms. Since \(\mathfrak{g}' \subseteq \mathfrak{k}^\perp\) the form \(\varphi^1\wedge \dots \wedge \varphi^{n-k}\wedge \Psi\) is closed and
nowhere vanishing on \(\mathfrak{g}\) which then implies \(\sigma=0\), again by [61]. ◻
A first consequence of part (1) of the above Proposition concerns holomorphic volume forms on completely solvable solvmanifold.
Corollary 70. Let \(M=G/\Gamma\) be a completely solvable solvmanifold equipped with a left-invariant complex structure \(J\). Then any holomorphic trivialisation of
the canonical bundle of \(M\) must be left-invariant.
Proof. If the canonical bundle of \(M\) is holomorphically trivial clearly \(\rho=0\). By Proposition 69 we deduce \(\sigma=0\) which implies, together with [61], that there exists a
left-invariant holomorphic volume form on \(G\), which then descends to \(M\), concluding the proof. ◻
Another interesting consequence of Corollary 69 is the following.
Corollary 71. Let \(\mathfrak{g}\) be a unimodular completely solvable Lie algebra equipped with a solvable complex structure \(J\). Then \(\rho=0\).
Proof. We prove the corollary by induction on the solvability step \(s\) of \(J\). If \(s=2\) then the result follows from Proposition 59. Let us assume that the result is true for \(s-1\) and let us prove it for \(s\). If \(\mathfrak{g}\) is \(s\)-step \(J\)-solvable the ideal \(\mathfrak{g}' + J \mathfrak{g}'\) is \((s-1)\)-step \(J\)-solvable, thus, by the inductive assumption, \(\rho_{\mathfrak{g}'+J\mathfrak{g}'}=0\). But then, from Proposition 69 we infer that \(\sigma_{\mathfrak{g}'+J\mathfrak{g}'}=0\). In particular \(\rho=\sigma
\vert_{\mathfrak{g}'}=0\). ◻
The purpose of the next example is to show that the converse of Corollary 71 does not hold, unless the solvability step is at most \(2\).
Example 72. Let \(\mathfrak{g}\) be the \(6\)-dimensional Lie algebra with structure equations: \[[e_2, e_4]=-e_1\,,\quad [e_3, e_5]=-e_1\,,
\quad [e_2,e_6]=-e_2\,,\quad [e_3, e_6]=-e_3\,, \quad [e_4, e_6]=e_4\,,\quad [e_5, e_6]=e_5\,.\] The equations above define a \(3\)-step completely solvable Lie algebra which in [27] is denoted by \(\mathfrak{s}_{6.162}^{1}\). We endow \(\mathfrak{g}\) with the following complex structure: \[Je_1=e_6\,, \quad Je_2=e_3\,, \quad Je_4=e_5\,.\] It turns out that \(J\) is simple and \(\rho=0\), showing that the converse of Corollary 71 is not true in higher steps of solvability, even assuming complete solvability.
We can extend the first statement of Theorem 67 to higher steps of solvability with a suitable assumption.
Proposition 73. Let \(\mathfrak{g}\) be a unimodular, SKT, completely solvable Lie algebra with solvable complex structure \(J\) such that \(\mathfrak{g}_J'\) is abelian. Then, \(\mathfrak{g}\) is \(2\)-step nilpotent.
Proof. We will prove the statement using induction on the step of solvability of \(J\). Let \(J\) be a \(s\)-step solvable complex structure. If
\(s=1\), then \(\mathfrak{g}'+J\mathfrak{g}'\) is abelian, hence \(\mathfrak{g}\) is \(2\)-step solvable. We can use
Theorem 67 to conclude. Let us assume that the statement is true for complex structures which are \((s-1)\)-step solvable and
assume that \(J\) is \(s\)-step solvable. We can then consider \(\mathfrak{k}:=\mathfrak{g}'+J\mathfrak{g}'\) which is unimodular, SKT and completely
solvable so that \(\mathfrak{k}_J'\subseteq \mathfrak{g}_J'\), hence abelian. Clearly, the complex structure on \(\mathfrak{k}\) is \((s-1)\)-step
solvable. Hence, by the inductive hypothesis, \(\mathfrak{k}\) is \(2\)-step nilpotent. Now, thanks to [51] and [50], we know respectively that \(\mathfrak{z}(\mathfrak{k})\) is a \(J\)-invariant abelian ideal of \(\mathfrak{g}\) and that \(\mathfrak{g}_J'\subseteq \mathfrak{z}(\mathfrak{k})\). Since \(J\) is solvable, we can now apply Corollary 71 and infer that \(\rho =0\). On the other hand, \(\mathfrak{z}(\mathfrak{k})\) can be chosen as the abelian \(J\)-invariant ideal of \(\mathfrak{g}\) in Proposition 63, which implies that \(\mathfrak{g}\) acts skew-symmetrically on \(\mathfrak{z}(\mathfrak{k}).\) We are in the position to use
complete solvability and infer that \(\mathfrak{g}_J'\subseteq \mathfrak{z}(\mathfrak{k})\subseteq \mathfrak{z}(\mathfrak{g}).\) In order to conclude, we just need to observe that \(\mathfrak{g}/ \mathfrak{z}(\mathfrak{g})\) is a completely solvable Lie algebra with a solvable abelian complex structure. By Corollary 66, we conclude that \(\mathfrak{g}/\mathfrak{z}(\mathfrak{g})\) is nilpotent and hence \(\mathfrak{g}\) is nilpotent as well, as claimed. ◻
We finally extend to Theorem 3 under the assumption of complete solvability and a condition on \(\mathfrak{g}_J'.\)
Proposition 74. Let \(\mathfrak{g}\) be a unimodular, completely solvable Lie algebra endowed with a complex structure \(J\) such that \(\mathfrak{g}_J'\subseteq {\rm Rad}(\mathfrak{g})\). If \(\mathfrak{g}\) admits a balanced metric, then \(J\) is solvable. Furthermore, if an SKT metric also
exists, then \(\mathfrak{g}\) is Kähler.
Proof. Assume that \(J\) is not solvable. Then \(\mathfrak{h}:=\mathfrak{g}/ {\rm Rad}(\mathfrak{g})\) is a completely solvable Lie algebra with abelian semisimple complex
structure \(J\). Using Proposition 24, part \((2)\), we have that \(-\eta_{\mathfrak{h}}\) is \(d\)-exact and non-negative, thanks to the fact that \(\mathfrak{g}\) is completely solvable. Let \(\pi\colon \mathfrak{g} \to \mathfrak{h}\) be the canonical projection onto \(\mathfrak{h}\). Thus, \(-\pi^*\eta_\mathfrak{h}\) is a \(d\)-exact non-negative \((1,1)\)-form, hence it must vanish by Corollary 18. This is equivalent to \(\eta_\mathfrak{h}=0\), and therefore \(B_{\mathfrak{h}}^{1,1}=0\), contradicting the \(J\)-semisimplicity of \(\mathfrak{h}\),
by Theorem 27. Using Corollary 71, we conclude that \(\rho=0\). The final claim follows from [36]. ◻
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