Product Code Database
Example Keywords: produce -shirt $79
   » Wiki: Homotopy Theory
Tag Wiki 'Homotopy Theory'.
Tag

In , homotopy theory is a systematic study of situations in which maps can come with between them. It originated as a topic in algebraic topology, but nowadays is learned as an independent discipline.


Applications to other fields of mathematics
Besides algebraic topology, the theory has also been used in other areas of mathematics such as:

  • Algebraic geometry (e.g., A1 homotopy 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 weak Hausdorff or a .

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

Often, one works with a —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.

The Cartesian product of two pointed spaces X, Y are not naturally pointed. A substitute is the X \wedge Y which is characterized by the

\operatorname{Map}(X \wedge Y, Z) = \operatorname{Map}(X, \operatorname{Map}(Y, Z)),
that is, a smash product is an analog of a in abstract algebra (see tensor-hom adjunction). Explicitly, X \wedge Y is the quotient of X \times Y by the X \vee Y.


Homotopy
Let I denote the unit interval 0,. A map
h: X \times I \to Y
is called a from the map h_0 to the map h_1, where h_t(x) = h(x, t). Intuitively, we may think of h as a path from the map h_0 to the map h_1. Indeed, a homotopy can be shown to be an equivalence relation. When X, Y are pointed spaces, the maps h_t are required to preserve the basepoint and the homotopy h is called a . A based homotopy is the same as a (based) map X \wedge I_+ \to Y where I_+ is I together with a disjoint basepoint.

Given a pointed space X and an n \ge 0, let \pi_n X = S^n, be the homotopy classes of based maps S^n \to X from a (pointed) n-sphere S^n to X. As it turns out,

  • for n \ge 1, \pi_n X are groups called ; in particular, \pi_1 X is called the fundamental group of X,
  • for n \ge 2, \pi_n X are by the Eckmann–Hilton argument,
  • \pi_0 X can be identified with the set of path-connected components in X.
Every group is the fundamental group of some space.

A map f is called a homotopy equivalence if there is another map g such that f \circ g and g \circ f are both homotopic to the identities. Two spaces are said to be homotopy equivalent if there is a homotopy equivalence between them. A homotopy equivalence class of spaces is then called a . There is a weaker notion: a map f : X \to Y is said to be a weak homotopy equivalence if f_* : \pi_n(X) \to \pi_n(Y) is an isomorphism for each n \ge 0 and each choice of a base point. A homotopy equivalence is a weak homotopy equivalence but the converse need not be true.

Through the adjunction

\operatorname{Map}(X \times I, Y) = \operatorname{Map}(X, \operatorname{Map}(I, Y)), \,\, h \mapsto (x \mapsto h(x, \cdot)),
a homotopy h : X \times I \to Y is sometimes viewed as a map X \to Y^I = \operatorname{Map}(I, Y).


CW complex
A is a space that has a filtration X \supset \cdots \supset X^n \supset X^{n-1} \supset \cdots \supset X^0 whose union is X and such that
  1. X^0 is a discrete space, called the set of 0-cells (vertices) in X.
  2. Each X^n is obtained by attaching several n-disks, n-cells, to X^{n-1} via maps S^{n-1} \to X^{n-1}; i.e., the boundary of an n-disk is identified with the image of S^{n-1} in X^{n-1}.
  3. A subset U is open if and only if U \cap X^n is open for each n.

For example, a sphere S^n has two cells: one 0-cell and one n-cell, since S^n can be obtained by collapsing the boundary S^{n-1} of the n-disk to a point. In general, every manifold has the homotopy type of a CW complex;. NB: "second countable" implies "separable". in fact, implies that a compact manifold has the homotopy type of a finite CW complex.

Remarkably, Whitehead's theorem says that for CW complexes, a weak homotopy equivalence and a homotopy equivalence are the same thing.

Another important result is the approximation theorem. First, the homotopy category of spaces is the category where an object is a space but a morphism is the homotopy class of a map. Then

Explicitly, the above approximation functor can be defined as the composition of the functor S_* followed by the geometric realization functor; see .

The above theorem justifies a common habit of working only with CW complexes. For example, given a space X, one can just define the homology of X to the homology of the CW approximation of X (the cell structure of a CW complex determines the natural homology, the cellular homology and that can be taken to be the homology of the complex.)


Cofibration and fibration
A map f: A \to X is called a if given:

  1. A map h_0 : X \to Z, and
  2. A homotopy g_t : A \to Z
such that h_0 \circ f = g_0, there exists a homotopy h_t : X \to Z that extends h_0 and such that h_t \circ f = g_t. An example is a neighborhood deformation retract; that is, X contains a neighborhood of a closed subspace A and f the inclusion (e.g., a tubular neighborhood of a closed submanifold). In fact, a cofibration can be characterized as a neighborhood deformation retract pair. Another basic example is a (X, A); many often work only with CW complexes and the notion of a cofibration there is then often implicit.

A in the sense of Hurewicz is the dual notion of a cofibration: that is, a map p : X \to B is a fibration if given (1) a map h_0 : Z \to X and (2) a homotopy g_t : Z \to B such that p \circ h_0 = g_0, there exists a homotopy h_t: Z \to X that extends h_0 and such that p \circ h_t = g_t.

While a cofibration is characterized by the existence of a retract, a fibration is characterized by the existence of a section called the as follows. Let p': Np \to B^I be the pull-back of a map p : E \to B along \chi \mapsto \chi(1) : B^I \to B, called the mapping path space of p.Some authors use \chi \mapsto \chi(0). The definition here is from Viewing p' as a homotopy N p\times I \to B (see ), if p is a fibration, then p' gives a homotopy

s: Np \to E^I
such that s(e, \chi)(0) = e, \, (p^I \circ s)(e, \chi) = \chi where p^I : E^I \to B^I is given by p.p in the reference should be p^I. This s is called the path lifting associated to p. Conversely, if there is a path lifting s, then p is a fibration as a required homotopy is obtained via s.

A basic example of a fibration is a as it comes with a unique path lifting. If E is a over a paracompact space, that is, a space with a free and transitive (topological) of a (topological) group, then the projection map p: E \to X is a fibration, because a Hurewicz fibration can be checked locally on a paracompact space.

While a cofibration is injective with closed image, a fibration need not be surjective.

There are also based versions of a cofibration and a fibration (namely, the maps are required to be based).


Lifting property
A pair of maps i : A \to X and p : E \to B is said to satisfy the if for each commutative square diagram
there is a map \lambda that makes the above diagram still commute. (The notion originates in the theory of .)

Let \mathfrak{c} be a class of maps. Then a map p : E \to B is said to satisfy the right lifting property or the RLP if p satisfies the above lifting property for each i in \mathfrak{c}. Similarly, a map i : A \to X is said to satisfy the left lifting property or the LLP if it satisfies the lifting property for each p in \mathfrak{c}.

For example, a Hurewicz fibration is exactly a map p : E \to B that satisfies the RLP for the inclusions i_0 : A \to A \times I. A is a map satisfying the RLP for the inclusions i : S^{n - 1} \to D^n where S^{-1} is the empty set. A Hurewicz fibration is a Serre fibration and the converse holds for CW complexes.

On the other hand, a cofibration is exactly a map satisfying the LLP for evaluation maps p: B^I \to B at 0.


Loop and suspension
On the category of pointed spaces, there are two important functors: the \Omega and the (reduced) suspension functor \Sigma, which are in the . Precisely, they are defined as
  • \Omega X = \operatorname{Map}(S^1, X), and
  • \Sigma X = X \wedge S^1.
Because of the adjoint relation between a smash product and a mapping space, we have:
\operatorname{Map}(\Sigma X, Y) = \operatorname{Map}(X, \Omega Y).

These functors are used to construct and . Namely, if f : X \to Y is a map, the fiber sequence generated by f is the exact sequence

\cdots \to \Omega^2 Ff \to \Omega^2 X \to \Omega^2 Y \to \Omega Ff \to \Omega X \to \Omega Y \to Ff \to X \to Y
where Ff is the of f; i.e., a fiber obtained after replacing f by a (based) fibration. The cofibration sequence generated by f is X \to Y \to C f \to \Sigma X \to \cdots, where Cf is the homotooy cofiber of f constructed like a homotopy fiber (use a quotient instead of a fiber.)

The functors \Omega, \Sigma restrict to the category of CW complexes in the following weak sense: a theorem of Milnor says that if X has the homotopy type of a CW complex, then so does its loop space \Omega X.


Classifying spaces and homotopy operations
Given a topological group G, the classifying space for ("the" up to equivalence) is a space BG such that, for each space X,
X, = {principal G-bundle on X} / ~ , \,\, f \mapsto f^*
where
  • the left-hand side is the set of homotopy classes of maps X \to BG,
  • ~ refers isomorphism of bundles, and
  • = is given by pulling-back the distinguished bundle EG on BG (called universal bundle) along a map X \to BG.
Brown's representability theorem guarantees the existence of classifying spaces.


Spectrum and generalized cohomology
The idea that a classifying space classifies principal bundles can be pushed further. For example, one might try to classify cohomology classes: given an A (such as \mathbb{Z}),
X, = \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 is an example of a generalized cohomology theory.

A basic example of a spectrum is a : S^0 \to S^1 \to S^2 \to \cdots


Ring spectrum and module spectrum

Homotopy colimit and limit

Key theorems
  • Seifert–van Kampen theorem
  • Homotopy excision theorem
  • Freudenthal suspension theorem (a corollary of the excision theorem)
  • Landweber exact functor theorem
  • Dold–Kan correspondence
  • Eckmann–Hilton argument - this shows for instance higher homotopy groups are .
  • Universal coefficient theorem
  • Dold–Thom theorem


Obstruction theory and characteristic class
See also: Characteristic class, , Whitehead torsion


Localization and completion of a space

Specific theories
There are several specific theories
  • simple homotopy theory
  • stable homotopy theory
  • chromatic homotopy theory
  • rational homotopy theory
  • p-adic homotopy theory
  • equivariant homotopy theory
  • simplicial homotopy theory


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.

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 are paths.


Abstract homotopy theory
Abstract homotopy theory is an axiomatic approach to homotopy theory. Such axiomatization is useful for non-traditional applications of homotopy theory. One approach to axiomatization is by Quillen's . A model category is a category with a choice of three classes of maps called weak equivalences, cofibrations and fibrations, subject to the axioms that are reminiscent of facts in algebraic topology. For example, the category of (reasonable) topological spaces has a structure of a model category where a weak equivalence is a weak homotopy equivalence, a cofibration a certain retract and a fibration a Serre fibration. Another example is the category of non-negatively graded chain complexes over a fixed base ring.


Simplicial set
A is an abstract generalization of a simplicial complex and can play a role of a "space" in some sense. Despite the name, it is not a set but is a sequence of sets together with the certain maps (face and degeneracy) between those sets.

For example, given a space X, for each integer n \ge 0, let S_n X be the set of all maps from the n-simplex to X. Then the sequence S_n X of sets is a simplicial set. Each simplicial set K = \{ K_n \}_{n \ge 0} has a naturally associated chain complex and the homology of that chain complex is the homology of K. The singular homology of X is precisely the homology of the simplicial set S_* X. Also, the geometric realization | \cdot | of a simplicial set is a CW complex and the composition X \mapsto |S_* X| is precisely the CW approximation functor.

Another important example is a category or more precisely the nerve of a category, which is a simplicial set. In fact, a simplicial set is the nerve of some category if and only if it satisfies the (a theorem of Grothendieck). Each category is completely determined by its nerve. In this way, a category can be viewed as a special kind of a simplicial set, and this observation is used to generalize a category. Namely, an \infty-category or an \infty-groupoid is defined as particular kinds of simplicial sets.

Since simplicial sets are sort of abstract spaces (if not topological spaces), it is possible to develop the homotopy theory on them, which is called the simplicial homotopy theory.


See also
  • Highly structured ring spectrum
  • Homotopy type theory
  • Shape theory
  • Moduli stack of formal group laws
  • Milnor's theorem on Kan complexes
  • Fibration of simplicial sets


Further reading
  • , lectures by Martin Frankland
  • (1967). 9783540039143, Springer Verlag.


External links
Page 1 of 1
1
Page 1 of 1
1

Account

Social:
Pages:  ..   .. 
Items:  .. 

Navigation

General: Atom Feed Atom Feed  .. 
Help:  ..   .. 
Category:  ..   .. 
Media:  ..   .. 
Posts:  ..   ..   .. 

Statistics

Page:  .. 
Summary:  .. 
1 Tags
10/10 Page Rank
5 Page Refs
1s Time