# Homotopy group

A generalization of the fundamental group, proposed by W. Hurewicz [1] in the context of problems on the classification of continuous mappings. Homotopy groups are defined for any . For the homotopy group is identical with the fundamental group. The definition of homotopy groups is not constructive and for this reason their computation is a difficult task, general methods for which were developed only in the 1950s. Their importance is due to the fact that all problems in homotopy theory can be reduced (cf. Homotopy type), to a greater or lesser extent, to the computation of certain homotopy groups.

Let

be the dimensional unit cube, let be its face , and let be the union of its remaining faces. For any pointed pair (cf. Pointed object) the symbol (or simply ) denotes the pointed set of all homotopy classes (cf. Homotopy) of mappings

The distinguished (zero) element of this set is the constant mapping that maps the whole cube into . Any continuous mapping

induces a morphism

of pointed sets. For any the sets and the morphisms constitute a functor from the category of pointed pairs into the category of pointed sets. This functor is homotopy invariant, i.e. if and are homotopic (as mappings of pointed pairs). Furthermore, it is normalized in the sense that if , then .

For it is possible to introduce into the set an operation of addition, with respect to which it becomes a group (if even an Abelian group). By definition, if and , then , where is the mapping

defined by the formula

(1) |

The resulting group is said to be the -th homotopy group (or the -dimensional homotopy group) of the pointed pair ; one also speaks of the homotopy group of the pair at or of the homotopy group of the space with respect to the subspace at . The mappings are homomorphisms of these groups. Thus, if it may be assumed that the function takes values in the category of groups (if even in the category of Abelian groups).

For the group is denoted by , or simply by , and is called the absolute homotopy group of the pointed space (or of the space at ). Its elements are the homotopy classes of mappings , where is the boundary of the cube . For such mappings formula (1) is meaningful for as well, and so is a group. This group coincides with the classical fundamental group. The group operation in is usually called multiplication. This group is, generally speaking, non-Abelian, while the group is Abelian. For any the groups and the corresponding homomorphisms form a functor from the category of pointed spaces into the category of groups (if into the category of Abelian groups). This functor is the composition of the imbedding functor and the functor described above.

The functor is extended to include the case , where is the pointed set of path-components (cf. Path-connected space) of ; the zero of this set is the component containing . The set is not defined for . In order to simplify the formulations, the sets and are usually also called homotopy groups, even though they are not groups in general.

For each element the mapping represents a mapping , and thus defines a certain element of the homotopy group . This element depends only on and is denoted by the symbol . The resulting mapping is a morphism of pointed sets (if a homomorphism of groups) and is called a boundary homomorphism or a boundary operator. The boundary homomorphism, together with the homomorphisms and induced by the imbeddings and , makes it possible to write down a sequence of groups and homomorphisms, infinite from the left:

This is an exact sequence; it is called the exact homotopy sequence of the pair and is usually denoted by . If for all , then the homomorphism is an isomorphism (also for all ).

The boundary homomorphism is natural, that is, it is a morphism of the functor into the functor (more exactly, into the functor where ). This makes it possible to define as a functor that takes values in the category of exact sequences of pointed sets which, except for the last six sets, are Abelian groups and, except for the last three sets, are groups.

Let be an arbitrary fibration in the sense of Serre and let , , , and . The mapping defines a mapping of pointed pairs. For any the induced homomorphism is an isomorphism. In particular, this is true for . In the latter case the formula unambiguously defines a homomorphism where is the fibre of over . This homomorphisms is called the homotopy transgression. It occurs in the exact sequence

This sequence is called the homotopy sequence of the fibration . Putting a fibration into correspondence with its homotopy sequence yields a functor on the category of all (pointed) fibrations.

In the particular case when is the standard Serre fibration of paths over a space , for any one has the isomorphism , where is the loop space of . This isomorphism is called the Hurewicz isomorphism.

The above properties actually unambiguously define the homotopy groups , i.e. may be taken as axioms which describe these groups. In fact, let be an arbitrary sequence of homotopy-invariant normalized functors, defined on the category of pointed spaces, taking values in the category of pointed sets, and having the following property: For any fibration in the sense of Serre , any subset and any point , the induced homomorphism is an isomorphism. Such a sequence is called a homotopy system if for any there is defined a morphism of the functor into the functor (if , into ) that is an isomorphism for any pointed pair for which for all . Any homotopy system is isomorphic to the homotopy system constructed above, which consists of homotopy groups. Furthermore, if , a group structure can be uniquely introduced into the pointed sets (and also into the sets ) so that all morphisms are homomorphism (this structure accordingly corresponds to that described by formula (1)). On the other hand, the sets if and carry only the inverse group operation. All this means that the above properties unambiguously define the homotopy groups (up to the order of multiplication in non-commutative groups).

For any mapping and any path connecting two points and , the formula , defines a homotopy of . By the homotopy extension axiom (cf. Cofibration) this homotopy can be extended to a homotopy for which . The final mapping of this homotopy maps into , i.e. represents a mapping . The corresponding element of the homotopy group depends only on the class of and the homotopy class of , and is denoted by the symbol (if , by the symbol ). The family is thus defined as a local family on the space , i.e. on the fundamental groupoid of this space. In particular, for any point the group operates on . If these operators act as inner automorphisms: , and if they make the group into a -module. For any continuous mapping the induced homomorphisms are operator homomorphisms (homomorphisms of modules): .

In a similar way, the groups , , constitute a local family of homotopy groups on the subspace . In particular, the group operates on the homotopy group so that if the group is a -module. The group is said to be a crossed -module (cf. Crossed modules), where is the boundary homomorphism.

The group acts as a group of operators not only on the groups but also on the groups , and also, by virtue of the natural homomorphism , on the groups . With respect to these actions of all homomorphisms of the exact sequence are operator homomorphisms, so that can be regarded as a group of operators on the sequence . This is equivalent to saying that the sequences , , constitute a local family of exact sequences of the subspace .

If the complement is represented as a union of disjoint open -dimensional cells, then the -module is a free module (if , a free crossed module) and has a system of free generators — a basis in bijective (not necessarily natural) correspondence with the cells of (Whitehead's theorem).

The mappings are in bijective correspondence with the mappings , where is an -dimensional sphere and is some point on it. For this reason the elements of can be regarded as the homotopy classes of mappings . This is also true if . The above identification depends on the selection of some relative homeomorphism . It is common to select and fix the sphere and the homeomorphism once and for all. In the original definition of Hurewicz, which is not frequently used nowadays, was not fixed, while was given up to a homotopy. Such a specification of is equivalent to specifying an orientation on . Thus, according to Hurewicz, the elements of are pointed homotopy classes of mappings of an oriented -dimensional sphere into . The set of non-pointed homotopy classes of mappings is in bijective correspondence with the orbits of the action of on (cf. Orbit). If (or, more generally, if acts trivially on ), then is said to be homotopically -simple. In this case is independent of (so that the notation is fully justified). This group is naturally identified with the set , which, as a consequence, has a group structure. A space that is homotopically -simple for all is said to be Abelian.

Let be the orientation class of the sphere and let , . This defines a homomorphism , the so-called Hurewicz homomorphism. Its kernel contains all elements of the form , , (if , all elements of the form , i.e. it contains the commutator of ). Poincaré's classical theorem states that for the kernel of coincides with the commutator , so that the group is isomorphic to the Abelianization of the fundamental group . Hurewicz's theorem, which is a generalization of Poincaré's theorem to the case , states that if for , then the homomorphism is an isomorphism (and the homomorphism is an epimorphism).

In a similar way, the elements of can be regarded as (pointed) homotopy classes of mappings , where is an (oriented) -dimensional ball and is its boundary. If the pair is homotopically -simple (i.e. if acts trivially on ), then the requirement of pointedness may be dropped in this definition. The formula

where is the orientation class of the pair and defines the Hurewicz homomorphism

If and for , this homomorphism is an isomorphism (Hurewicz's theorem for relative groups).

Two principal methods are known for the computation of the homotopy groups of specific spaces: the method of killing spaces (cf. Killing space) and the method of homotopy resolutions (cf. Homotopy type; Postnikov system). The first method is based on the isomorphism , which follows from Hurewicz's theorem and the definition of the killing space . This isomorphism reduces the computation of to the problem of computing the homology groups . The space fibres over the space with fibre , and the homology groups of the space are known. Therefore one may try to find the lower homology groups of killing spaces by induction. The problem of computing the homology groups of a fibre space from the homology groups of its base and fibre is still not completely solved in its general formulation (and, obviously, a general satisfactory solution does not exist). However, extensive information on the homology groups of the spaces can be extracted from the corresponding Serre spectral sequence. In many cases this information is sufficient for the computation of , at least for some . An essential technical simplification of the problem is obtained on the basis of the Serre's theory of classes of Abelian groups and the -approximation derived from it. With this theory it is possible to compute entirely in the cohomology and only for the coefficient groups . The geometric principles on which this technique is based were first clarified by J.F. Adams and D. Sullivan on the basis of the concept of localization of topological spaces at a given prime number .

The second (also inductive) method of computing homotopy groups consists of a stepwise construction of the homotopy resolution of the space . Suppose the -th term of this resolution is known (e.g. if , then ). The next term must be the fibre space over with fibre ; moreover, the group must be isomorphic to the known group . This gives (on the basis of the corresponding spectral sequence) definite information on the group , which, in many cases, makes it possible to compute it completely. For example, for by this method all groups , , can be found. In its modern form, this method is also based on the concept of localization.

The method of homology resolutions was extended (cf. [4]) to an algorithm that is applicable to any simply-connected finite -complex and that gives all its homotopy groups. However, for practical use this algorithm is too complicated.

Since the homotopy theory is completely equivalent to the homotopy theory of simplicial sets, the definition of a homotopy group may be transferred to any (complete) simplicial set. The "combinatorial" definition obtained (due to D. Kan) can easily be extended to an algorithm. However, this algorithm is also too complicated for practical use.

From any of the above methods it is easy to establish that the homotopy groups of a simply-connected space having finitely-generated homology groups, are also finitely generated. The analogous statement for non-simply connected spaces (i.e. its homology groups should be finitely generated as -modules) is, in general, not true.

Let be the (reduced) suspension functor, and let be the loop functor. Since these functors are adjoint, the identity mapping defines an imbedding , for any . Since , this imbedding defines a homomorphism

which is known as the suspension homomorphism. It coincides with the homomorphism obtained by assigning to an arbitrary (pointed) mapping its suspension . This homomorphism occurs in an exact sequence:

This sequence is called the suspension sequence of the space . The homomorphism in it is a generalization of the classical Hopf invariant.

If is a countable CW-complex with one vertex, the space may be replaced by the infinite reduced product of the complex . This shows that if for , then is an isomorphism for all and an epimorphism if . This theorem is known as Freudenthal's suspension theorem (H. Freudenthal first published the proof for the case , although the theorem was known much earlier.)

Freudenthal's theorem shows that for the group is independent of . It is called the -th stable homotopy group of the sphere (cf. also Stable homotopy group). Similar stabilization phenomena occur for the homotopy groups of the orthogonal groups, of the Thom spaces (cf. Thom space) and in many other cases. The general study of these phenomena is most conveniently done within the framework of the so-called theory of spectra. In this theory stable homotopy groups arise as the homotopy groups of spectra. These groups have an essentially simpler structure than the homotopy groups of a space and their study (and computation) is an easier task. For example, for the computation of these groups one has a special device: the Adams spectral sequence.

Homotopy groups have been generalized in various directions. For example, an attempt was made to replace the spheres by other spaces. Here one may note toroidal homotopy groups, obtained by interpreting the Whitehead product as a commutator. It was also shown that the set of homotopy classes of mappings admits a group operation which is natural with respect to if and only if is a co--space. Homotopy groups with coefficients were obtained by replacing the spheres by the Moore spaces (cf. Moore space). This definition of homotopy groups with coefficients was not very successful. A more satisfactory definition (compatible with the general Eckmann–Hilton duality principle) was obtained by replacing the Moore -spaces by co--spaces. However, these homotopy groups were not defined for all (e.g. for the additive group of real numbers, these groups are not defined).

The question of the construction of homotopy groups in categories other than the category of pointed pairs has been studied in detail. First of all one has to mention the homotopy groups of a triad (cf. Triads, see, e.g., [3]), which were very useful in the study of the homomorphism . A very general construction of homotopy groups was proposed in connection with studies on duality. On the basis of the concept of a standard construction (see [6]) the construction of homotopy groups was transferred to arbitrary categories. A fundamental role in this construction is played by the homotopy groups of simplicial sets mentioned earlier.

#### References

[1] | N.E. Steenrod, "The topology of fibre bundles" , Princeton Univ. Press (1951) |

[2] | V.G. Boltyanskii, "The homotopy theory of continuous mapping and vector fields" , Moscow (1955) (In Russian) |

[3] | S.-T. Hu, "Homotopy theory" , Acad. Press (1959) |

[4] | E.H. Brown, "Finite computability of Postnikov complexes" Ann. of Math. (2) , 65 (1957) pp. 1–20 |

[5] | D. Kan, "A combinatorial definition of homotopy groups" Ann. of Math. (2) , 67 (1958) pp. 282–313 |

[6] | J. Stallings, "A finitely presented group whose 3-dimensional integral homology is not finitely generated" Amer. J. Math. , 85 (1963) pp. 541–543 |

[7a] | B. Eckmann, P. Hilton, "Groupes d'homotopie et dualité. Groupes absolus" C.R. Acad. Sci. , 246 (1958) pp. 2444–2447 |

[7b] | B. Eckmann, P. Hilton, "Groupes d'homotopie et dualité. Suites exactes" C.R. Acad. Sci. , 246 (1958) pp. 2555–2558 |

[7c] | B. Eckmann, P. Hilton, "Groupes d'homotopie et dualité. Coefficients" C.R. Acad. Sci. , 246 (1958) pp. 2991–2993 |

[7d] | B. Eckmann, P. Hilton, "Transgression homotopique et cohomologique" C.R. Acad. Sci. , 247 (1958) pp. 620–623 |

[7e] | B. Eckmann, P. Hilton, "Décomposition homologique d'une polyèdre simplement connexe" C.R. Acad. Sci. , 248 (1959) pp. 2054–2056 |

[8] | D. Sullivan, "Geometric topology" , M.I.T. (1971) (Notes) |

#### Comments

Although W. Hurewicz

was the first to study the higher homotopy groups in detail, the definition was in fact suggested a few years earlier by E. Čech [a2]. The action of the fundamental group on the higher homotopy groups was first studied by S. Eilenberg [a3]. A good general reference for homotopy groups is [a4].

The stable homotopy groups form a generalized homology theory, i.e. a theory which satisfies all the Eilenberg–Steenrod axioms except possibly the dimension axiom. This theory is in fact defined by the spectrum of spheres , cf. Spectrum of spaces. The corresponding generalized cohomology theory (cf. Generalized cohomology theories) defined by this spectrum consists of the cohomotopy group. Cf., e.g., [a4] and [a11] for more details. Powerful tools for computing the stable homotopy groups of the spheres (besides the (classical) Adams spectral sequence) involve the Adams–Novikov spectral sequence, the so-called chromatic spectral sequence and complex cobordism, cf. [a12].

#### References

[a1a] | W. Hurewicz, "Beiträge zur Topologie der Deformationen I-II" Proc. Ned. Akad. Weten. Ser. A , 38 (1935) pp. 112–119; 521–528 |

[a1b] | W. Hurewicz, "Beiträge zur Topologie der Deformationen III-IV" Proc. Ned. Akad. Weten. Ser. A , 39 (1936) pp. 117–126; 215–224 |

[a2] | E. Čech, "Höherdimensionale Homotopiegruppen" , Verh. Intern. Mathematikerkongress Zürich, 1932 , O. Füssli (1932) pp. 203 |

[a3] | S. Eilenberg, "On the relation between the fundamental group of a space and the higher homotopy groups" Fund. Math. , 32 (1939) pp. 167–175 |

[a4] | G.W. Whitehead, "Elements of homotopy theory" , Springer (1978) pp. 23; 415–455 |

[a5] | B. Gray, "Homotopy theory. An introduction to algebraic topology" , Acad. Press (1975) pp. §12 |

[a6] | P.J. Hilton, "An introduction to homotopy theory" , Cambridge Univ. Press (1953) |

[a7] | E.H. Spanier, "Algebraic topology" , McGraw-Hill (1960) |

[a8] | D. Sullivan, "Genetics of homotopy theory and the Adams conjecture" Ann. of Math. , 100 (1974) pp. 1–79 |

[a9] | D.G. Quillen, "Homotopical algebra" , Springer (1967) |

[a10] | B. Eckmann, "Homotopie et dualité" , Coll. Topol. Algébrique Louvain, 1956 , Masson (1957) pp. 41–53 |

[a11] | R.M. Switzer, "Algebraic topology - homotopy and homology" , Springer (1975) |

[a12] | D.C. Ravenel, "Complex cobordism and stable homotopy groups of spheres" , Acad. Press (1986) |

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Homotopy group.

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