Homotopy theory explained

In mathematics, homotopy theory is a systematic study of situations in which maps can come with homotopies between them. It originated as a topic in algebraic topology, but nowadays is learned as an independent discipline. Besides algebraic topology, the theory has also been used in other areas of mathematics such as algebraic geometry (e.g., A1 homotopy theory) and category theory (specifically the study of higher categories).

Concepts

Spaces and maps

In homotopy theory and algebraic topology, the word "space" denotes a topological space. In order to avoid pathologies, one rarely works with arbitrary spaces; instead, one requires spaces to meet extra constraints, such as being compactly generated, or Hausdorff, or a CW complex.

In the same vein as above, a "map" is a continuous function, possibly with some extra constraints.

Often, one works with a pointed space—that is, a space with a "distinguished point", called a basepoint. A pointed map is then a map which preserves basepoints; that is, it sends the basepoint of the domain to that of the codomain. In contrast, a free map is one which needn't preserve basepoints.

Homotopy

See main article: Homotopy. Let I denote the unit interval. A family of maps indexed by I,

ht:X\toY

is called a homotopy from

h0

to

h1

if

h:I x X\toY,(t,x)\mapstoht(x)

is a map (e.g., it must be a continuous function). When X, Y are pointed spaces, the

ht

are required to preserve the basepoints. A homotopy can be shown to be an equivalence relation. Given a pointed space X and an integer

n\ge1

, let

\pin(X)=[Sn,X]*

be the homotopy classes of based maps

Sn\toX

from a (pointed) n-sphere

Sn

to X. As it turns out,

\pin(X)

are groups; in particular,

\pi1(X)

is called the fundamental group of X.

If one prefers to work with a space instead of a pointed space, there is the notion of a fundamental groupoid (and higher variants): by definition, the fundamental groupoid of a space X is the category where the objects are the points of X and the morphisms are paths.

Cofibration and fibration

A map

f:A\toX

is called a cofibration if given (1) a map

h0:X\toZ

and (2) a homotopy

gt:A\toZ

, there exists a homotopy

ht:X\toZ

that extends

h0

and such that

ht\circf=gt

. In some loose sense, it is an analog of the defining diagram of an injective module in abstract algebra. The most basic example is a CW pair

(X,A)

; since many work only with CW complexes, the notion of a cofibration is often implicit.

A fibration in the sense of Serre is the dual notion of a cofibration: that is, a map

p:X\toB

is a fibration if given (1) a map

Z\toX

and (2) a homotopy

gt:Z\toB

, there exists a homotopy

ht:Z\toX

such that

h0

is the given one and

p\circht=gt

. A basic example is a covering map (in fact, a fibration is a generalization of a covering map). If

E

is a principal G-bundle, that is, a space with a free and transitive (topological) group action of a (topological) group, then the projection map

p:E\toX

is an example of a fibration.

Classifying spaces and homotopy operations

Given a topological group G, the classifying space for principal G-bundles ("the" up to equivalence) is a space

BG

such that, for each space X,

[X,BG]=

/ ~

,[f]\mapstof*EG

where

X\toBG

,

EG

on

BG

(called universal bundle) along a map

X\toBG

.Brown's representability theorem guarantees the existence of classifying spaces.

Spectrum and generalized cohomology

See main article: Spectrum (algebraic topology).

The idea that a classifying space classifies principal bundles can be pushed further. For example, one might try to classify cohomology classes: given an abelian group A (such as

Z

),

[X,K(A,n)]=\operatorname{H}n(X;A)

where

K(A,n)

is the Eilenberg–MacLane space. The above equation leads to the notion of a generalized cohomology theory; i.e., a contravariant functor from the category of spaces to the category of abelian groups that satisfies the axioms generalizing ordinary cohomology theory. As it turns out, such a functor may not be representable by a space but it can always be represented by a sequence of (pointed) spaces with structure maps called a spectrum. In other words, to give a generalized cohomology theory is to give a spectrum.

A basic example of a spectrum is a sphere spectrum:

S0\toS1\toS2\to

Key theorems

Obstruction theory and characteristic class

See also: Characteristic class, Postnikov tower, Whitehead torsion

Localization and completion of a space

See main article: Localization of a topological space.

Specific theories

There are several specific theories

Homotopy hypothesis

See main article: Homotopy hypothesis.

One of the basic questions in the foundations of homotopy theory is the nature of a space. The homotopy hypothesis asks whether a space is something fundamentally algebraic.

Abstract homotopy theory

Concepts

Model categories

See main article: Model category.

Simplicial homotopy theory

See also

References

Further reading

External links

Web site: homotopy theory . ncatlab.org.