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Atlas (topology)

From Wikipedia, the free encyclopedia
Set of charts that describes a manifold
For other uses, seeFiber bundle andAtlas (disambiguation).

Inmathematics, particularlytopology, anatlas is a concept used to describe amanifold. An atlas consists of individualcharts that, roughly speaking, describe individual regions of the manifold. In general, the notion of atlas underlies the formal definition of amanifold and related structures such asvector bundles and otherfiber bundles.

Charts

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"Coordinate patch" redirects here; not to be confused withSurface patch.
"Local coordinate system" redirects here; not to be confused withLocal geodetic coordinate system.
See also:Topological manifold § Coordinate charts

The definition of an atlas depends on the notion of achart. Achart for atopological spaceM is ahomeomorphismφ{\displaystyle \varphi } from anopen subsetU ofM to an open subset of aEuclidean space. The chart is traditionally recorded as the ordered pair(U,φ){\displaystyle (U,\varphi )}.[1]

When a coordinate system is chosen in the Euclidean space, this defines coordinates onU{\displaystyle U}: the coordinates of a pointP{\displaystyle P} ofU{\displaystyle U} are defined as the coordinates ofφ(P).{\displaystyle \varphi (P).} The pair formed by a chart and such a coordinate system is called alocal coordinate system,coordinate chart,coordinate patch,coordinate map, orlocal frame.

Formal definition of atlas

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Anatlas for atopological spaceM{\displaystyle M} is anindexed family{(Uα,φα):αI}{\displaystyle \{(U_{\alpha },\varphi _{\alpha }):\alpha \in I\}} of charts onM{\displaystyle M} whichcoversM{\displaystyle M} (that is,αIUα=M{\textstyle \bigcup _{\alpha \in I}U_{\alpha }=M}). If for some fixedn, theimage of each chart is an open subset ofn-dimensionalEuclidean space, thenM{\displaystyle M} is said to be ann-dimensionalmanifold.

The plural of atlas isatlases, although some authors useatlantes.[2][3]

An atlas(Ui,φi)iI{\displaystyle \left(U_{i},\varphi _{i}\right)_{i\in I}} on ann{\displaystyle n}-dimensional manifoldM{\displaystyle M} is called anadequate atlas if the following conditions hold:[clarification needed]

Everysecond-countable manifold admits an adequate atlas.[4] Moreover, ifV=(Vj)jJ{\displaystyle {\mathcal {V}}=\left(V_{j}\right)_{j\in J}} is an open covering of the second-countable manifoldM{\displaystyle M}, then there is an adequate atlas(Ui,φi)iI{\displaystyle \left(U_{i},\varphi _{i}\right)_{i\in I}} onM{\displaystyle M}, such that(Ui)iI{\displaystyle \left(U_{i}\right)_{i\in I}} is arefinement ofV{\displaystyle {\mathcal {V}}}.[4]

Transition maps

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Two charts on a manifold, and their respectivetransition map

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 theinverse of the other. This composition is not well-defined unless we restrict both charts to theintersection of theirdomains 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(Uα,φα){\displaystyle (U_{\alpha },\varphi _{\alpha })} and(Uβ,φβ){\displaystyle (U_{\beta },\varphi _{\beta })} are two charts for a manifoldM such thatUαUβ{\displaystyle U_{\alpha }\cap U_{\beta }} isnon-empty.Thetransition mapτα,β:φα(UαUβ)φβ(UαUβ){\displaystyle \tau _{\alpha ,\beta }:\varphi _{\alpha }(U_{\alpha }\cap U_{\beta })\to \varphi _{\beta }(U_{\alpha }\cap U_{\beta })} is the map defined byτα,β=φβφα1.{\displaystyle \tau _{\alpha ,\beta }=\varphi _{\beta }\circ \varphi _{\alpha }^{-1}.}

Note that sinceφα{\displaystyle \varphi _{\alpha }} andφβ{\displaystyle \varphi _{\beta }} are both homeomorphisms, the transition mapτα,β{\displaystyle \tau _{\alpha ,\beta }} is also a homeomorphism.

More structure

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

If each transition function is asmooth map, then the atlas is called asmooth atlas, and the manifold itself is calledsmooth. Alternatively, one could require that the transition maps have onlyk continuous derivatives in which case the atlas is said to beCk{\displaystyle C^{k}}.

Very generally, if each transition function belongs to apseudogroupG{\displaystyle {\mathcal {G}}} of homeomorphisms of Euclidean space, then the atlas is called aG{\displaystyle {\mathcal {G}}}-atlas. If the transition maps between charts of an atlas preserve alocal trivialization, then the atlas defines the structure of a fibre bundle.

See also

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References

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  1. ^Jänich, Klaus (2005).Vektoranalysis (in German) (5 ed.). Springer. p. 1.ISBN 3-540-23741-0.
  2. ^Jost, Jürgen (11 November 2013).Riemannian Geometry and Geometric Analysis. Springer Science & Business Media.ISBN 9783662223857. Retrieved16 April 2018 – via Google Books.
  3. ^Giaquinta, Mariano; Hildebrandt, Stefan (9 March 2013).Calculus of Variations II. Springer Science & Business Media.ISBN 9783662062012. Retrieved16 April 2018 – via Google Books.
  4. ^abKosinski, Antoni (2007).Differential manifolds. Mineola, N.Y: Dover Publications.ISBN 978-0-486-46244-8.OCLC 853621933.

External links

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Basic concepts
Main theorems(list)
Maps
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