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An illustration of a homotopy between the two bold paths
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.
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.
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 : X → Y are homotopic, and f2,
g2 : Y → Z are homotopic, then their compositions f2 o
f1 and g2 o g1 : X → Z 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 groups 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 to homotopy equivalence, to be described next.
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 : X → Y and
g : Y → X 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
circle S1. Those spaces that are homotopy equivalent to a point are called
contractible.
Clearly, every homeomorphism is a homotopy equivalence, but the
converse is not true: a solid disk is not homeomorphic to a single point.
Homotopy-invariant properties
Homotopy equivalence is important because in algebraic
topology most concepts cannot distinguish homotopy equivalent spaces: if X and Y are homotopy equivalent,
then
Homotopy category and homotopy invariants
More abstractly, one can appeal to category theory concepts. One
can define the homotopy category, whose objects are topological spaces, and whose morphisms are homotopy classes
of continuous maps. Two topological spaces X and Y are isomorphic in this category if and only if they are
homotopy-equivalent.
A homotopy invariant is any function on spaces, (or on mappings), that respects the relation of homotopy
equivalence (resp. homotopy); such invariants are constitutive of homotopy theory. Of course one could
have foundational objection to a function whose domain is the
collection of all topological spaces.
A typical homotopy invariant is the fundamental group of a
space, already mentioned earlier.
In practice homotopy theory is carried out by working with CW complexes, for
technical convenience; or in some other reasonable category.
Relative homotopy
Especially in order to define the fundamental group, one needs
the notion of homotopy relative to a subspace. These are homotopies which keep the elements of the subspace
fixed. Formally: if f and g are continuous maps from X to Y and K is a subset of
X, then we say that f and g are homotopic relative K if there exists a homotopy
H : X × [0,1] → Y between f and g such that
H(k,t) = f(k) for all k∈K and t∈[0,1].
Isotopy
In case the two given continuous functions f and g from the topological space X to the topological
space Y are homeomorphisms, one can ask whether they can be
connected 'through homeomorphisms'. This gives rise to the concept of isotopy, which is a homotopy H in
the notation used before, such that for each fixed t, H(x,t) gives a homeomorphism.
In geometric topology - for example in knot theory - the idea of isotopy
is used to construct equivalence relations. For example, when should two knots be considered the same? We take two knots
K1 and K2 in three-dimensional space. The intuitive idea of deforming one to the
other should correspond to a path of homeomorphisms: an isotopy starting with the identity homeomorphism of three-dimensional
space, and ending at a homeomorphism h such that h moves K1 to K2.
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