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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==
 
The definition of an atlas depends on the notion of a ''chart''. 
A '''chart''' for a [[topological space]] ''M'' is a [[homeomorphism]] <math>\varphi</math> from an [[open set|open subset]] ''U'' of ''M'' to an open subset of [[Euclidean space]]. The chart is traditionally recorded as the ordered pair <math> (U, \varphi)</math>.
 
==Formal definition of atlas==
 
An '''atlas''' for a [[topological space]] ''M'' is a collection <math> \{(U_{\alpha}, \varphi_{\alpha})\}</math> of charts on ''M'' such that
<math> \bigcup U_{\alpha} = M</math>. 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]].
 
==Transition maps==
 
{{ Annotated image | caption=Two charts on a manifold
| image=Two coordinate charts on a manifold.svg
| image-width = 250
| annotations =
{{Annotation|45|70|<math>M</math>}}
{{Annotation|67|54|<math>U_\alpha</math>}}
{{Annotation|187|66|<math>U_\beta</math>}}
{{Annotation|42|100|<math>\varphi_\alpha</math>}}
{{Annotation|183|117|<math>\varphi_\beta</math>}}
{{Annotation|87|109|<math>\tau_{\alpha,\beta}</math>}}
{{Annotation|90|145|<math>\tau_{\beta,\alpha}</math>}}
{{Annotation|55|183|<math>\mathbf R^n</math>}}
{{Annotation|145|183|<math>\mathbf R^n</math>}}
}}
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 <math>(U_{\alpha}, \varphi_{\alpha})</math> and <math>(U_{\beta}, \varphi_{\beta})</math> are two charts for a manifold ''M'' such that <math>U_{\alpha} \cap U_{\beta}</math> is non-empty.
The '''transition map''' <math> \tau_{\alpha,\beta}: \varphi_{\alpha}(U_{\alpha} \cap U_{\beta}) \to \varphi_{\beta}(U_{\alpha} \cap U_{\beta})</math> is the map defined by
 
: <math>\tau_{\alpha,\beta} = \varphi_{\beta} \circ \varphi_{\alpha}^{-1}.</math>
 
Note that since <math>\varphi_{\alpha}</math> and <math>\varphi_{\beta}</math> are both homeomorphisms, the transition map <math> \tau_{\alpha, \beta}</math> is also a homeomorphism.
 
==More structure==
 
One often desires more structure on a manifold than simply the topological structure. For example, if one would like an unambiguous notion of [[differentiation (mathematics)|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 manifold|differentiable]]. Given a differentiable manifold, one can unambiguously define the notion of [[tangent vectors]] and then [[directional derivative]]s.
 
If each transition function
is a [[smooth map]], then the atlas is called a
[[smooth structure|smooth atlas]], and the manifold itself is called [[Differentiable manifold#Definition|smooth]].
Alternatively, one could require that the transition maps
have only ''k'' continuous derivatives in which case the atlas is
said to be <math> C^k </math>.
 
Very generally, if each transition function
belongs to a [[pseudo-group]] <math> {\mathcal G} </math>
of [[homeomorphism]]s of [[Euclidean space]],
then the atlas is called a  <math> {\mathcal G}</math>-atlas.
 
==References==
{{reflist}}
{{refbegin}}
*{{cite book | first = John M. | last = Lee | year = 2006 | title = Introduction to Smooth Manifolds | publisher = Springer-Verlag | isbn = 978-0-387-95448-6}}
*{{cite book | first = Mark R. | last = Sepanski | year = 2007 | title = Compact Lie Groups | publisher = Springer-Verlag | isbn = 978-0-387-30263-8}}
{{refend}}
 
==External links==
*[http://mathworld.wolfram.com/Atlas.html Atlas] by Rowland, Todd
 
[[Category:Differential topology]]

Revision as of 05:41, 1 February 2014

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

The definition of an atlas depends on the notion of a chart. A chart for a topological space M is a homeomorphism from an open subset U of M to an open subset of Euclidean space. The chart is traditionally recorded as the ordered pair .

Formal definition of atlas

An atlas for a topological space M is a collection of charts on M such that . 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.

Transition maps

Template:Annotated image 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 and are two charts for a manifold M such that is non-empty. The transition map is the map defined by

Note that since and are both homeomorphisms, the transition map is also a homeomorphism.

More structure

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 .

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

References

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Template:Refend

External links