So far we have been discussing topological spaces under the assumption
that two spaces may be identified if their topological type is the
same, namely, when they are homeomorphic. The topological type of a
space however is a very strong invariant of the space in the sense
that for many applications two spaces may be thought of as the same
although they are not homeomorphic. For these applications it is many
times useful to think about two spaces as identical if one can
continuously deformed into the other. For example, any Euclidean space
can be deformed continuously into a single point. However the circle
or any sphere or the torus cannot be deformed to a point. It is also
not hard to see that the circle cannot be deformed into a 2-sphere and
generally an n-sphere cannot be deformed into a k-sphere is n
k. This motivates the idea of homotopy and homotopy type. A brief
description follows.
Suppose
f, g : X
Y are two maps. We say that f and g are
homotopic if in some precise sense f can be deformed continuously
into g. It is not hard to see even from this intuitive definition
that this relation on maps from X to Y is an equivalence
relation. Two spaces X and Y are said to be homotopy equivalent if
there are maps
f : X
Y and
g : Y
X such that fog is
homotopic to the identity of Y and gof is homotopic to the
identity of X. Once more, it is not hard to see that homotopy
equivalence is indeed an equivalence relation on topological
spaces. The homotopy type of a space X is the class of X under
this equivalence relation. The study of homotopy types and related
features of topological spaces forms a rich, well developed
mathematical discipline called homotopy theory. In this section we
describe some of the fundamental concepts of homotopy theory with an
eye towards geometric applications.