Differential structure

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In mathematics, an n-dimensional differential structure (or differentiable structure) on a set M makes it into an n-dimensional differential manifold, which is a topological manifold with some additional structure that allows us to do differential calculus on the manifold. If M is already a topological manifold, we require that the new topology is identical to the existing one.

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Definition

For a natural number n and some k which may be a non-negative integer or infinity, an n-dimensional Ck differential structure is defined using a Ck-atlas, which is a set of bijections called charts between a set of subsets of M (whose union is the whole of M), and a set of open subsets of an n-dimensional vector space:

<math>\varphi_{i}:W_{i}\subset M\rightarrow U_{i}\subset\mathbb{R}^{n}.</math>

which are Ck-compatible (in the sense defined below):

Each such map provides a way in which certain subsets of the manifold may be viewed as being like open subsets of <math>\mathbb{R}^{n}</math> but the usefulness of this notion depends on to what extent these notions agree when the domains of two such maps overlap.

Consider two charts:

<math>\varphi_{i}:W_{i}\rightarrow U_{i}</math>,
<math>\varphi_{j}:W_{j}\rightarrow U_{j}</math>.

The intersection of the ranges of these two functions is:

<math>W_{ij}=W_{i}\cap W_{j}\;</math>

and is mapped to two images

<math>U_{ij}=\varphi_{i}\left(W_{ij}\right)</math>,
<math>U_{ji}=\varphi_{j}\left(W_{ij}\right)</math>

by the two chart maps.

The transition map between the two charts is the map between the two images of this intersection under the two chart maps.

<math>\varphi_{ij}:U_{ij}\rightarrow U_{ji}</math>
<math>\varphi_{ij}(x)=\varphi_{j}\left(\varphi_{i}^{-1}\left(x\right)\right).</math>

Two charts <math>\varphi_{i},\,\varphi_{j}</math> are Ck-compatible if

<math>U_{ij},\, U_{ji}</math>

are open, and the transition maps

<math>\varphi_{ij},\,\varphi_{ji}</math>

have continuous derivatives of order k. If k = 0, we only require that the transition maps are continuous, consequently a C0-atlas is simply another way to define a topological manifold. If k = ∞, derivatives of all orders must be continuous. A family of Ck-compatible charts covering the whole manifold is a Ck-atlas defining a Ck differential manifold. Two atlases are Ck-equivalent if the union of their sets of charts forms a Ck-atlas. In particular, a Ck-atlas that is C0-compatible with a C0-atlas that defines a topological manifold is said to determine a Ck differential structure on the topological manifold. The Ck equivalence classes of such atlases are the distinct Ck differential structures of the manifold.

Existence and uniqueness theorems

On any manifold with a Ck structure for k>0, there is a unique Ck-compatible C-structure, a theorem due to Whitney. On the other hand, there exist topological manifolds which admit no differential structures, see Donaldson's theorem (confer Hilbert's fifth problem).

When people count differential structures on a manifold, they usually count them modulo orientation-preserving homeomorphisms. There is only one differential structure of any manifold of dimension smaller than 4. For all manifolds of dimension greater than 4 there is a finite number of differential structures on any compact manifold. There is only one differential structure on <math> \mathbb{R}^{n}</math> except when <math>n = 4</math>, in which case there are uncountably many.

Differential structures on spheres of dimensions from 1 to 18

The following table lists the numbers of differential structures (modulo orientation-preserving homeomorphism) on the <math>n</math>-sphere for dimensions <math>n</math> up to dimension 18. Spheres with differential structures different from the usual one are known as exotic spheres.

Dimension 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18
Structures 1 1 1 ∞? 1 1 28 2 8 6 992 1 3 2 16256 2 16 16

It is not currently known how many differential structures there are on the 4-sphere, beyond that there is at least one. There may be one, a finite number, or an infinite number. The claim that there is just one is known as the smooth Poincaré conjecture.

See also