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For other senses of the term (such as in geology), see foliation (disambiguation).

In mathematics, a foliation is a geometric device used to study manifolds. Informally speaking, a foliation is a kind of "clothing" worn on a manifold, cut from a stripy fabric. On each sufficiently small piece of the manifold, these stripes give the manifold a local product structure. This product structure does not have to be consistent outside local patches (i. e. well-defined globally): a stripe followed around long enough might return to a different, nearby stripe.

Definition


More formally, a codimension p foliation F of an n-dimensional manifold M is a covering by charts U_i together with maps

\phi_i:U_i \to \R^n

such that on the overlaps U_i \cap U_j the transition functions \varphi_{ij}:\mathbb{R}^n\to\mathbb{R}^n defined by

\varphi_{ij} =\phi_j \phi_i^{-1}

take the form

\varphi_{ij}(x,y) = (\varphi_{ij}^1(x),\varphi_{ij}^2(x,y))

where x denotes the first n-p co-ordinates, and y denotes the last p co-ordinates. That is,

\varphi_{ij}^1:\mathbb{R}^{n-p}\to\mathbb{R}^{n-p}
and
\varphi_{ij}^2:\mathbb{R}^n\to\mathbb{R}^{p}.
In the chart U_i, the stripes x=constant match up with the stripes on other charts U_j. Technically, these stripes are called plaques of the foliation. In each chart, the plaques are n-p dimensional submanifolds. These submanifolds piece together from chart to chart to form maximal connected injectively immersed submanifolds called the leaves of the foliation.

Examples


Flat space

Consider an n-dimensional space, foliated as a product by subspaces consisting of points whose first n-p co-ordinates are constant. This can be covered with a single chart. The statement is essentially that

\mathbb{R}^n=\mathbb{R}^{n-p}\times \mathbb{R}^{p}

with the leaves or plaques \mathbb{R}^{n-p} being enumerated by \mathbb{R}^{p}. The analogy is seen directly in three dimensions, by taking n=3 and p=1: the two-dimensional leaves of a book are enumerated by a (one-dimensional) page number.

Covers

If M \to N is a covering between manifolds, and F is a foliation on N, then it pulls back to a foliation on M. More generally, if the map is merely a branched covering, where the branch locus is transverse to the foliation, then the foliation can be pulled back.

Lie groups

If G is a Lie group, and H is a subgroup obtained by exponentiating a closed subalgebra of the Lie algebra of G, then G is foliated by cosets of H.

Foliations and integrability


There is a close relationship, assuming everything is smooth, with vector fields: given a vector field X on M that is never zero, its integral curves will give a 1-dimensional foliation. (i.e. a codimension n-1 foliation).

This observation generalises to a theorem of Ferdinand Georg Frobenius (the Frobenius theorem), saying that the necessary and sufficient conditions for a distribution (i.e. an n-p dimensional subbundle of the tangent bundle of a manifold) to be tangent to the leaves of a foliation, are that the set of vector fields tangent to the distribution are closed under Lie bracket. One can also phrase this differently, as a question of reduction of the structure group of the tangent bundle from GL(n) to a reducible subgroup.

The conditions in the Frobenius theorem appear as integrability conditions; and the assertion is that if those are fulfilled the reduction can take place because local transition functions with the required block structure exist.

There is a global foliation theory, because topological constraints exist. For example in the surface case, an everywhere non-zero vector field can exist on an orientable compact surface only for the torus. This is a consequence of the Poincaré-Hopf index theorem, which shows the Euler characteristic will have to be 0.

See also


Foliations | Structures on manifolds

叶层结构

 

This article is licensed under the GNU Free Documentation License. It uses material from the "Foliation".

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