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.