Chemistry - Foliation

In mathematics, 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.

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 $\varphi_{ij}$ 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. 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 submanifolds called the leaves of the foliation.

Example: $n$ -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.

Example: 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.

Example: 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 $H$ .

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 $G L (n)$ 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.

Foliation

See also