Atlas (topology)

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For other uses of "atlas", see Atlas (disambiguation).

In mathematics, particularly topology, one describes a manifold using an atlas. An atlas consists of individual charts that, roughly speaking, describe individual regions of the manifold. If the manifold is the surface of the Earth, then an atlas has its more common meaning. In general, the notion of atlas underlies the formal definition of a manifold.

Charts[edit]

The definition of an atlas depends on the notion of a chart. A chart for a topological space M (also called a coordinate chart or coordinate map) is a homeomorphism \varphi from an open subset U of M to an open subset of Euclidean space. The chart is traditionally recorded as the ordered pair  (U, \varphi).

Formal definition of atlas[edit]

An atlas for a topological space M is a collection  \{(U_{\alpha}, \varphi_{\alpha})\} of charts on M such that  \bigcup U_{\alpha} = M. If the codomain of each chart is the n-dimensional Euclidean space and the atlas is connected, then M is said to be an n-dimensional manifold.

Maximal atlas[edit]

The atlas containing all possible charts consistent with a given atlas is called the maximal atlas (i.e. an equivalence class containing that given atlas (under the already defined equivalence relation given in the previous paragraph)). Unlike an ordinary atlas, the maximal atlas of a given manifold is unique. Though it is useful for definitions, it is an abstract object and not used directly (e.g. in calculations).

Transition maps[edit]

M
U_\alpha
U_\beta
\varphi_\alpha
\varphi_\beta
\tau_{\alpha,\beta}
\tau_{\beta,\alpha}
\mathbf R^n
\mathbf R^n
Two charts on a manifold

A transition map provides a way of comparing two charts of an atlas. To make this comparison, we consider the composition of one chart with the inverse of the other. This composition is not well-defined unless we restrict both charts to the intersection of their domains of definition. (For example, if we have a chart of Europe and a chart of Russia, then we can compare these two charts on their overlap, namely the European part of Russia.)

To be more precise, suppose that (U_{\alpha}, \varphi_{\alpha}) and (U_{\beta}, \varphi_{\beta}) are two charts for a manifold M such that U_{\alpha} \cap U_{\beta} is non-empty. The transition map  \tau_{\alpha,\beta}: \varphi_{\alpha}(U_{\alpha} \cap U_{\beta}) \to \varphi_{\beta}(U_{\alpha} \cap U_{\beta}) is the map defined by

\tau_{\alpha,\beta} = \varphi_{\beta} \circ \varphi_{\alpha}^{-1}.

Note that since \varphi_{\alpha} and \varphi_{\beta} are both homeomorphisms, the transition map  \tau_{\alpha, \beta} is also a homeomorphism.

More structure[edit]

One often desires more structure on a manifold than simply the topological structure. For example, if one would like an unambiguous notion of differentiation of functions on a manifold, then it is necessary to construct an atlas whose transition functions are differentiable. Such a manifold is called differentiable. Given a differentiable manifold, one can unambiguously define the notion of tangent vectors and then directional derivatives.

If each transition function is a smooth map, then the atlas is called a smooth atlas, and the manifold itself is called smooth. Alternatively, one could require that the transition maps have only k continuous derivatives in which case the atlas is said to be  C^k .

Very generally, if each transition function belongs to a pseudo-group  {\mathcal G} of homeomorphisms of Euclidean space, then the atlas is called a  {\mathcal G}-atlas.

References[edit]

External links[edit]