Appendix A Viewing the Real Projective Plane in R3;The Cross-Cap and the Steiner Roman Surface
It turns out that there are several ways of viewing the real projective plane in R3 as a surface with self-intersection. Recall that, as a topological space, the projective plane, RP2, is the quotient of the 2-sphere, S 2,(inR3) by the equivalence relation that identifies antipodal points. In Hilbert and CohnÐVossen [2](andalsodoCarmo [1]) an interesting map, H , from R3 to R4 is defined by
.x; y; z/ 7! .xy; yz;xz;x2 y2/:
This map has the remarkable property that when restricted to S 2,wehave H .x; y; z/ D H .x0;y0; z0/ iff .x0;y0; z0/ D .x; y; z/ or .x0;y0; z0/ D . x; y; z/. In other words, the inverse image of every point in H .S 2/ consists of two antipodal points. Thus, the map H induces an injective map from the projective plane onto H .S 2/, which is obviously continuous, and since the projective plane is compact, it is a homeomorphism. Therefore, the map H allows us to realize concretely the projective plane in R4 by choosing any parametrization of the sphere, S 2,and applying the map H to it. Actually, it turns out to be more convenient to use the map A defined such that
.x; y; z/ 7! .2xy; 2yz;2xz;x2 y2/; because it yields nicer parametrizations. For example, using the stereographic representation of S 2 where 2u x.u; v/ D ; u2 C v2 C 1 2v y.u; v/ D ; u2 C v2 C 1 u2 C v2 1 z.u; v/ D ; u2 C v2 C 1
J. Gallier and D. Xu, A Guide to the Classification Theorem for Compact Surfaces, 105 Geometry and Computing 9, DOI 10.1007/978-3-642-34364-3, © Springer-Verlag Berlin Heidelberg 2013 106 A Viewing the Real Projective Plane in R3; The Cross-Cap and the Steiner Roman . . .
Fig. A.1 Jakob Steiner, 1796Ð1863
we obtain the following four fractions parametrizing the projective plane in R4:
8uv x.u; v/ D ; .u2 C v2 C 1/2 4v.u2 C v2 1/ y.u; v/ D ; .u2 C v2 C 1/2 4u.u2 C v2 1/ z.u; v/ D ; .u2 C v2 C 1/2 4.u2 v2/ t.u; v/ D : .u2 C v2 C 1/2
Of course, we don’t know how to visualize this surface in R4, but we can visualize its four projections in R3, using parallel projections with respect to the four axes, which amounts to dropping one of the four coordinates. The resulting surfaces turn out to be very interesting. Only two distinct surfaces are obtained, both very well known to topologists. Indeed, the surface obtained by dropping y or z is known the cross-cap surface, and the surface obtained by dropping x or t is known as the Steiner roman surface. These surfaces can be easily displayed. We begin with the Steiner surface named after Jakob Steiner (Fig. A.1). 1. The Steiner roman surface. This is the surface obtained by dropping t. Going back to the map A and renaming x;y;z as ˛; ˇ; ,if
x D 2˛ˇ; y D 2ˇ ; z D 2˛ ; t D ˛2 ˇ2; it is easily seen that A Viewing the Real Projective Plane in R3; The Cross-Cap and the Steiner Roman . . . 107
xy D 2zˇ2; yz D 2x 2; xz D 2y˛2:
If .˛;ˇ; /is on the sphere, we have ˛2 Cˇ2 C 2 D 1, and thus we get the following implicit equation for the Steiner roman surface:
x2y2 C y2z2 C x2z2 D 2xyz:
It is easily verified that the following parametrization works:
2v x.u; v/ D ; u2 C v2 C 1 2u y.u; v/ D ; u2 C v2 C 1 2uv z.u; v/ D : u2 C v2 C 1
Thus, amazingly, the Steiner roman surface (Fig. A.2) can be specified by fractions of quadratic polynomials! It can be shown that every quadric surface can be defined as a rational surface of degree 2, but other surfaces can also be defined, as shown by the Steiner roman surface. It can be shown that the Steiner roman surface is contained inside the tetrahedron defined by the planes