Abstract
We pursue the research line proposed in Yang and Zheng (Acta. Math. Sinica (English Series), 34(8):1259–1268, 2018) about the classification of Hermitian manifolds whose s-Gauduchon connection \(\nabla ^s =(1-\frac{s}{2})\nabla ^c + \frac{s}{2}\nabla ^b\) is flat, where \(s\in {\mathbb {R}}\) and \(\nabla ^c\) and \(\nabla ^b\) are the Chern and the Bismut connections, respectively. We focus on Lie groups equipped with a left invariant Hermitian structure. Such spaces provide an important class of Hermitian manifolds in various contexts and are often a valuable vehicle for testing new phenomena in complex and Hermitian geometry. More precisely, we consider a connected 2n-dimensional Lie group G equipped with a left-invariant complex structure J and a left-invariant compatible metric g and we assume that its connection \(\nabla ^s\) is flat. Our main result states that if either n=2 or there exits a \(\nabla ^s\)-parallel left invariant frame on G, then g must be Kähler. This result demonstrates rigidity properties of some complete Hermitian manifolds with \(\nabla ^s\)-flat Hermitian metrics.
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We are grateful to an anonymous referee for providing helpful suggestions to improve the exposition of this paper.
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The research of Bo Yang is partially supported by a grant from Xiamen University (0020-ZK1088).
The research of Fangyang Zheng is partially supported by a Simons Collaboration Grant 355557.
Appendix A: Lie groups with a flat left-invariant Kähler structure
Appendix A: Lie groups with a flat left-invariant Kähler structure
In this section we recall some results on flat left-invariant Lie groups due to Milnor [14] and Barberis-Dotti-Fino [3]. These results lead to Corollary 1.6 stated in Sect. 1.
Theorem A.1
[14, Theorem 1.5 on p. 298] A connected Lie group G with a left invariant Riemannian metric is flat if and only if its Lie algebra \(\mathfrak {g}\) admits an orthogonal decomposition
where \(\mathfrak {h}\) is an abelian Lie subalgebra and \(\mathfrak {i}\) is an abelian ideal. Moreover, \({\text {ad}}(X)\) is skew-adjoint for any \(X \in \mathfrak {h}\).
In the above theorem, the abelian ideal \(\mathfrak {i}\) is \(\mathfrak {i}=\{Y \in \mathfrak {g}\ |\ \nabla _{Y}=0 \}\), where \(\nabla \) is the Levi-Civita connection. It is further observed (Proposition 2.1 in [3]) that \(\mathfrak {i}=\mathfrak {c} \oplus [\mathfrak {g}, \mathfrak {g}]\) where \(\mathfrak {c}\) is the center of \(\mathfrak {g}\) and \([\mathfrak {g}, \mathfrak {g}]\) is of even dimension.
Lie groups with a flat left-invariant Kähler structure were classified in Proposition 2.1 and Corollary 2.2 in [3]. We summarize and slightly rephrase their results as follows.
Theorem A.2
[3, Proposition 2.1, Corollary 2.2, and Proposition 3.1] Let (G, J, g) be connected Lie group with a left invariant complex structure and a flat left invariant Kähler metric. Then the Lie algebra \(\mathfrak {g}\) of G admits an orthogonal decomposition
which satisfies the following properties:
-
(i)
\(\mathfrak {h}\) is a Lie subalgebra, \(\mathfrak {c}\) is the center of \(\mathfrak {g}\), and \([\mathfrak {g}, \mathfrak {g}]\) is J-invariant.
-
(ii)
The adjoint action \({\text {ad}}\) injects \(\mathfrak {h}\) to skew-symmetric transformations on \([\mathfrak {g}, \mathfrak {g}]\) which commutes with J. Furthermore, we have the ‘simultaneous diagonalization’ of the restriction of \({\text {ad}}_{X}=\nabla _X\) on \(\mathfrak {h}\) in the following sense:
There exists an orthonormal basis with \([\mathfrak {g}, \mathfrak {g}]={\text {span}} \{e_1, Je_1, \ldots , e_p, Je_p\}\) and an injective linear map \(q=(q_1, \ldots , q_p): \mathfrak {h} \rightarrow \mathbb {R}^p\) such that for any \(X \in \mathfrak {h}\) and \(1 \le i \le p\), \({\text {ad}}_{X}\) has the block diagonal form:
$$\begin{aligned} ad_X \left[ \begin{array}{cc} e_i \\ Je_i \end{array} \right] = \left[ \begin{array}{cc} 0 &{} q_i(X) \\ -q_i (X) &{} 0 \end{array} \right] \left[ \begin{array}{cc} e_i \\ Je_i \end{array} \right] . \end{aligned}$$ -
(iii)
There are further orthogonal decompositions \(\mathfrak {h}=(\mathfrak {h} \cap J\mathfrak {h}) \oplus \mathfrak {h}_1\) and \(\mathfrak {c}=(\mathfrak {c} \cap J\mathfrak {c}) \oplus \mathfrak {c}_1\), and J restricts to an isomorphism between \(\mathfrak {h}_1\) and \(\mathfrak {c}_1\).
It is straightforward to write down all such Lie algebras in real dimension 4, which is exactly covered in Corollary 1.6.
It might be interesting to compare the kernel space \(\{Y \in \mathfrak {g}\ |\ \nabla _{Y}=0 \}\) in Theorem A.2 with the Lie algebra homomorphism \(p: {\mathfrak {g}} \rightarrow {\mathfrak {u}}(n)\) defined in (29) in Sect. 4. Let \(\nabla =\nabla ^{s}\), then our Theorem 1.3 can be reinterpreted as: for a \(\nabla ^{s}\)-flat Hermitian Lie group (G, J, g) with a left invariant structure, if the kernel space \(\{Y \in \mathfrak {g}\ |\ \nabla _{Y}=0 \}=\mathfrak {g}\), then (G, J, g) is Kähler and isomorphic to a complex vector group. We will study the structure of a \(\nabla ^{s}\)-flat left invariant Hermitian Lie group in the spirit of Theorem A.2 in a future work.
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Vezzoni, L., Yang, B. & Zheng, F. Lie groups with flat Gauduchon connections. Math. Z. 293, 597–608 (2019). https://doi.org/10.1007/s00209-019-02232-w
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DOI: https://doi.org/10.1007/s00209-019-02232-w