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Compression body : ウィキペディア英語版
Compression body

In the theory of 3-manifolds, a compression body is a kind of generalized handlebody.
A compression body is either a handlebody or the result of the following construction:
: Let S be a compact, closed surface (not necessarily connected). Attach 1-handles to S \times () along S \times \.
Let C be a compression body. The negative boundary of C, denoted \partial_C, is S \times \. (If C is a handlebody then \partial_- C = \emptyset.) The positive boundary of C, denoted \partial_C, is \partial C minus the negative boundary.
There is a dual construction of compression bodies starting with a surface S and attaching 2-handles to S \times \. In this case \partial_C is S \times \, and \partial_C is \partial C minus the positive boundary.
Compression bodies often arise when manipulating Heegaard splittings.
== References ==

* F.Bonahon, Geometric structures on 3-manifolds, Handbook of Geometric Topology, Daverman and Sher eds. North-Holland (2002).
de:Henkelkörper#Kompressionskörper

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