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Algebraic topology Homotopy theory


In topology, two continuous functions from one topological space to another are called homotopic if one can be "continuously deformed" into the other, such a deformation being called a homotopy between the two functions. An outstanding use of homotopy is the definition of homotopy groups and cohomotopy groups, important invariants in algebraic topology.

1 Formal definitions

Formally, a homotopy between two continuous functions f and g from a topological space X to a topological space Y is defined to be a continuous function H : X × [0,1] → Y from the product of the space X with the unit interval [0,1] to Y such that, for all points x in X, H(x,0)=f(x) and H(x,1)=g(x).

If we think of the second parameter of H as "time", then H describes a "continuous deformation" of f into g: at time 0 we have the function f, at time 1 we have the function g.

2 Properties

Being homotopic is an equivalence relation on the set of all continuous functions from X to Y. This homotopy relation is compatible with function composition in the following sense: if f1, g1 : XY are homotopic, and f2, g2 : YZ are homotopic, then their compositions f2 o f1 and g2 o g1 : XZ are homotopic as well.

If f and g from X to Y are homotopic, then the group homomorphisms induced by f and g on the level of homology groups are the same: Hn(f) = Hn(g) : Hn(X) → Hn(Y) for all n. If, in addition, X and Y are path-connected, then the group homomorphisms induced by f and g on the level of homotopy groupIn mathematics, homotopy groups are used in algebraic topology to classify topological spaces. The many different ways to (continuously) map an n dimensional sphere into a given space are collected into equivalence classes, called homotopy classes. Two mas are also the same: πn(f) = πn(g) : πn(X) → πn(Y).

These latter statements are the reason that algebraic topology generally can distinguish spaces only up toIn mathematics, the jargon term up to xxxx" is used to describe a situation in which members of an equivalence class can be regarded as a single entity for some purpose. xxxx" describes a property or process which transforms an element into one from the s homotopy equivalence, to be described next.

3 Homotopy equivalence of spaces

Given two spaces X and Y, we say they are homotopy equivalent or of the same homotopy type if there exist continuous maps f : XY and g : YX such that g o f is homotopic to the identity map idX and f o g is homotopic to idY.

The maps f and g are called homotopy equivalences in this case.

Intuitively, two spaces X and Y are homotopy equivalent if they can be transformed into one another by bending, shrinking and expanding operations. For example, a solid disk or solid ball is homotopy equivalent to a point, and R2 - {(0,0)} is homotopy equivalent to the unit circleIllustration of a unit circle. t is an angle measure. In mathematics, a unit circle is a circle with unit radius, i. a circle whose radius is 1. Frequently, especially in trigonometry, "the" unit circle is the circle of radius 1 centered at the origin (0, S1. Those spaces that are homotopy equivalent to a point are called contractible.

Clearly, every homeomorphismThis word should not be confused with homomorphism. In topology, two geometrical objects (or "spaces") are called homeomorphic if, roughly speaking, the first can be deformed into the second by stretching and bending; cutting is also allowed, but only if is a homotopy equivalence, but the converse is not true: a solid disk is not homeomorphic to a single point.



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