Obvious changes adapt definitions of sets of real and
complex points, singular points, singular and nonsingular curves and
rigid isotopy to the case of surfaces in
. Exactly as in the
case of curves one formulates the topological classification problem
(cf. 1.1.A above):
However, the isotopy classification problem 1.1.B splits into two problems:
The reason for this splitting is that, contrary to the case of
projective plane, there exists a homeomorphism of
non-isotopic
to the identity. Indeed, 3-dimensional projective space is orientable,
and the mirror reflection of this space in a plane reverses
orientation. Thus the reflection is not isotopic to the identity.
However, there are only two isotopy classes of homeomorphisms of
. It means that the difference between 5.1.B and
5.1.C is not really big. Although the isotopy classification
problem is finer, to resolve it, one should add to a solution of the
ambient topological classification problem an answer to the following
question:
Each of these problems has been solved only for . The
difference between
5.1.B and
5.1.C does not appear: the
solutions of 5.1.B and 5.1.C coincide with each other for
. (Thus Problem 5.1.D has a simple answer for
:
any nonsingular real algebraic surface of degree
is isotopic to
its mirror image.) For
solutions of 5.1.A and
5.1.B also coincide, but for
they are different: there
exist nonsingular surfaces of degree 4 in
which are
homeomorphic, but embedded in
in a such a way that there is no
homeomorphism of
mapping one of them to another. The simplest
example is provided by torus defined by equation
Similar splitting happens with the rigid isotopy classification problem. Certainly, it may be transferred literally:
However, since there exists a projective transformation of
,
which is not isotopic to the identity (e.g., the mirror reflection in a
plane) and a real algebraic surface can be nonisotopic rigidly to its
mirror image, one may consider the following rougher problem:
Again, as in the case of topological isotopy and homeomorphism problem, the difference between these two problems is an amphichirality problem:
Problems 5.1.E, 5.1.F and 5.1.G have been solved
also for . For
the solutions of 5.1.E and
5.1.F coincide with each other and with the solutions of
5.1.A, 5.1.B and 5.1.C. For
all these
problems belong to the traditional analytic geometry. The solutions are
well-known and can be found in traditional textbooks on analytic
geometry. The case
is also elementary. It was studied in the
nineteenth century. The solution is associated with names of Schläfli
and Klein. The case
is really difficult. Although the first
attempts of a serious attack were undertaken in the
nineteenth century, too, and among the attackers we see D. Hilbert and
K. Rohn, the complete solutions of all classification problems listed
above were obtained only in the seventies and eighties. In
higher degrees even the most rough problems, like the Harnack problem
on the maximal number of components of a surface of degree
are
still open.