Everything about Homotopy Group totally explained
In
mathematics,
homotopy groups are used in
algebraic topology to classify
topological spaces. The base point preserving maps from an
n-dimensional
sphere (with base point) into a given space (with base point) are collected into
equivalence classes, called
homotopy classes. Two mappings are
homotopic if one can be continuously deformed into the other. These homotopy classes form a
group, called the
n-th homotopy group, π
n(
X), of the given space
X with base point. Topological spaces with differing homotopy groups are never equivalent (
homeomorphic), but the converse isn't true. The first homotopy group is also called the
fundamental group.
The notion of homotopy of paths was introduced by
Camille Jordan.
Introduction
In modern mathematics it's common to study a
category by
associating to every object of this category a simpler object which still retains a sufficient amount of information about the object in question. Homotopy groups are a certain way of associating groups to topological spaces. A
group is a set which allows adding of elements in a suitable sense. For examples, the
integers Z form a group. Another example are the finite groups
Z/sZ.
The provided link between topology and groups allows the application of
group theory to get insights in
topology. For example, if two topological objects have different homotopy groups, they can't have the same topological structure, a fact which may be difficult to prove without resorting to non-topological means. For example, the
torus seems to be visibly different from the
sphere, the former having a "hole", the latter one not having one. However, as continuity, the basic notion of topology, only deals with the local structure, it can be difficult to formally pin down this intuition. The homotopy groups, however, carry information about the global structure.
As for the example: one can show that the first homotopy group of the torus
T » π
1(
T)=
Z2,
because the
universal cover of the torus is the
complex plane
C, mapping to the torus
T ≅
C /
Z2. On the other hand the sphere
S2 satisfies
» π
1(
S2)=0,
because every loop can be contracted to a constant map (see
homotopy groups of spheres for this and more complicated examples of homotopy groups).
Hence the torus isn't
homeomorphic to the sphere.
Definition
In the
n-sphere Sn we choose a base point
a. For a space
X with base point
b, we define π
n(
X) to be the set of homotopy classes of maps
» f :
Sn →
X
that map the base point
a to the base point
b. In particular, the equivalence classes are given by homotopies that are constant on the basepoint of the sphere. Equivalently, we can define π
n(X) to be the group of homotopy classes of maps
g : [0,1]
n →
X from the
n-cube to
X that take the boundary of the
n-cube to
b.
For
n ≥ 1, the homotopy classes form a
group. To define the group operation, recall that in the
fundamental group, the product
f *
g of two loops
f and
g is defined by setting (
f *
g)(
t) =
f(2
t) if
t is in [0,1/2] and (
f *
g)(
t) =
g(2
t-1) if
t is in [1/2,1]. The idea of composition in the fundamental group is that of following the first path and the second in succession, or, equivalently, setting their two domains together. The concept of composition that we want for the
n-th homotopy group is the same, except that now the domains that we stick together are cubes, and we must glue them along a face. We therefore define the sum of maps
f,
g : [0,1]
n →
X by the formula (
f +
g)(
t1,
t2, ...
tn) =
f(2
t1,
t2, ...
tn) for
t1 in [0,1/2] and (
f +
g)(
t1,
t2, ...
tn) =
g(2
t1-1,
t2, ...
tn) for
t1 in [1/2,1]. For the corresponding definition in terms of spheres, define the sum
f +
g of maps
f, g :
Sn →
X to be
composed with
h, where
is the map from
Sn to the
wedge sum of two
n-spheres that collapses the equator and
h is the map from the wedge sum of two
n-spheres to
X that's defined to be
f on the first sphere and
g on the second.
If
n ≥ 2, then π
n is
abelian. (For a proof of this, note that in two dimensions or greater, two homotopies can be "rotated" around each other.)
It is tempting to try to simplify the definition of homotopy groups by omitting the base points, but this doesn't usually work for spaces that are not simply connected, even for path connected spaces. The set of homotopy classes of maps from a sphere to a path connected space isn't the homotopy group, but is essentially the set of orbits of the fundamental group on the homotopy group, and in general has no natural group structure.
A way out of these difficulties has been found by defining higher homotopy
groupoids of filtered spaces and of
n-cubes of spaces. These are related to relative homotopy groups and to
n-adic homotopy groups respectively. A higher homotopy van Kampen theorem then enables one to derive some new information on homotopy groups and even on homotopy types. For more background and references, see
"Higher dimensional group theory"
and the references below.
Long exact sequence of a fibration
Let
p:
E →
B be a basepoint-preserving
Serre fibration with fiber
F, that is, a map possessing the
homotopy lifting property with respect to
CW complexes. Then there's a long
exact sequence of homotopy groups
» ... → π
n(
F) → π
n(
E) → π
n(
B) → π
n−1(
F) →... → π
0(
E) → π
0(
B) → 0
Here the maps involving π
0 are not group
homomorphisms because the π
0 are not groups, but they're exact in the sense that the image equals the kernel.
Example: the
Hopf fibration. Let
B equal
S2 and
E equal
S3. Let
p be the
Hopf fibration, which has fiber
S1. From the long exact sequence
» ⋯ → π
n(
S1) → π
n(
S3) → π
n(
S2) → π
n−1(
S1) → ⋯
and the fact that π
n(
S1) = 0 for
n ≥ 2, we find that π
n(
S3) = π
n(
S2) for
n ≥ 3. In particular, π
3(
S2) = π
3(
S3) =
Z.
In the case of a cover space, when the fiber is discrete, we've that π
n(E) is isomorphic to π
n(B) for all n greater than 1, that π
n(E) embeds injectively into π
n(B) for all positive
n, and that the subgroup of π
1(B) that corresponds to the embedding of π
1(E) has cosets in bijection with the elements of the fiber.
Methods of calculation
Calculation of homotopy groups is in general much more difficult than some of the other homotopy
invariants learned in algebraic topology. Unlike the
Seifert-van Kampen theorem for the fundamental group and the
Excision theorem for
singular homology and
cohomology, there's no simple way to calculate the homotopy groups of a space by breaking it up into smaller spaces. However methods developed in the 1980s involving a van Kampen type theorem for higher homotopy groupoids have allowed new calculations on homotopy types and so on homotopy groups. See for a sample result the 2008
paper by Ellis and Mikhailov
listed below.
For some spaces, such as
tori, all higher homotopy groups (that is, second and higher homotopy groups) are trivial. These are the so-called
aspherical spaces. However, despite intense research in calculating the homotopy groups of spheres, even in two dimensions a complete list isn't known. To calculate even the fourth homotopy group of
S2 one needs much more advanced techniques than the definitions might suggest. In particular the
Serre spectral sequence was constructed for just this purpose.
Certain Homotopy groups of
n-connected spaces can be calculated by comparison with
homology groups via the
Hurewicz theorem.
Relative homotopy groups
There are also relative homotopy groups π
n(
X,
A) for a pair (
X,
A). The elements of such a group are homotopy classes of based maps
Dn → X which take carry the boundary
Sn-1 into A. Two maps
f, g are called homotopic
relative to A if they're homotopic by a basepoint-preserving homotopy
F :
Dn × [0,1] →
X such that, for each
p in
Sn-1 and
t in [0,1], the element
F(
p,t) is in
A. The ordinary homotopy groups are the special case in which
A is the base point.
There is a long exact sequence of relative homotopy groups.
Related notions
The homotopy groups are a cornerstone of the
homotopy theory, which in turn stimulated the development
model categories. It is possible to define abstract homotopy groups for
simplicial sets.
Further Information
Get more info on 'Homotopy Group'.
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