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Deformations and rigidity of lattices in solvable Lie groups

机译:可解李群中晶格的变形和刚度

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Let G be a simply connected, solvable Lie group and Γ be a lattice in G. The deformation space D(Γ,G) is the orbit space associated to the action of Aut(G) on the space X(Γ,G) of all lattice embeddings of Γ into G. Our main result generalizes the classical rigidity theorems of Mal'tsev and Sait? for lattices in nilpotent Lie groups and in solvable Lie groups of real type. We prove that the deformation space of every Zariski-dense lattice Γ in G is finite and Hausdorff, provided that the maximal nilpotent normal subgroup of G is connected. This implies that every lattice in a solvable Lie group virtually embeds as a Zariski-dense lattice with finite deformation space. We give examples of solvable Lie groups G which admit Zariski-dense lattices Γ such that D(Γ,G) is countably infinite, and also examples where the maximal nilpotent normal subgroup of G is connected and simultaneously G has lattices with uncountable deformation space.
机译:令G为简单连接的可解Lie群,Γ为G中的晶格。变形空间D(Γ,G)是与Aut(G)对X的空间X(Γ,G)作用有关的轨道空间。 Γ的所有晶格嵌入。我们的主要结果推广了Mal'tsev和Sait?的经典刚度定理。用于零幂李群和实型可解李群中的格。我们证明,只要连接了G的最大幂等正态子群,G中每个Zariski-密集格Γ的变形空间都是有限的,并且是Hausdorff。这意味着可解李群中的每个晶格实际上都嵌入为具有有限变形空间的Zariski密集晶格。我们给出了允许Zariski-致密晶格Γ使D(Γ,G)无穷大的可解李群G的实例,还给出了G的最大幂等正态子群相连接并且同时G具有不可数变形空间的晶格的实例。

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