Riemannian Foliations
Riemannian Foliations
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DOI:
10.1007/978-1-4684-8670-4
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发表时间:
1988
期刊:
影响因子:
--
通讯作者:
P. Molino;G. Cairns
中科院分区:
文献类型:
--
作者:
P. Molino;G. Cairns
Foliation theory has its origins in the global analysis of solutions of ordinary differential equations: on an n-dimensional manifold M, an [autonomous] differential equation is defined by a vector field X; if this vector field has no singularities, then its trajectories form a par tition of M into curves, ie a foliation of codimension n-1. More generally, a foliation F of codimension q on M corresponds to a partition of M into immersed submanifolds [the leaves] of dimension,--------,--.---p= n-q. The first global image that comes to mind is 1--------;------that of a stack of" plaques". 1---------;------Viewed laterally [transver 1--------1-----sally], the leaves of such a 1--------1-----. stacking are the points of a 1--------1-------. quotient manifold W of di L.....-'_ mension q.-----~) WM Actually, this image corresponds to an elementary type of folia tion, that one says is" simple". For an arbitrary foliation, it is only l-u L ally [on a" simpIe" open set U] that the foliation appears as a stack of plaques and admits a local quotient manifold. Globally, a leaf L may--return and cut a simple open set U in several plaques, sometimes even an infinite number of plaques.