§ Concrete calculation of hopf fibration
- Take any point
(a, b, c, d) ∈ S3. - This determines a quaternion
a + bi + cj + dk. - Let the rotation determined by a quaternion
q be written as R_q. - Recall that this determines a rotation of 3 space
(b, c, d) and angle 2cos−1(a). - Let P0 be any point on
S2, say (1, 0, 0). - Then, the hopf fibration
h : S3 → S2 sends p ∈ S3 → R_p(P_0) ∈ R3. - Now, see that there are many points in
S3 which have image (1, 0, 0). - For example, one can check that all points
(cos t, sin t, 0, 0). - We can show that for any point
p ∈ S2, the inverse image h^{-1}(p) ∈ S3 will be a unit circle in S^3. - The full fibration will therefore be
S1 → S3 -h→ S2, since each of the fibers of h is a circle ( S1).
§ Rendering
- For a given point on
p ∈ S2, we can render h−1(p)⊆S3as a set of points in R3 via stereographic projection, which furthermore preserves circles (sends circles to circles). - The map sends a point (w,x,y,z) to the point (x/(1−w),y/(1−w),z/(1−w)). The only singularity is at w=1 which we conveniently ignore.
- See that this map sends circles to circles. Suppose we have the locus of points
(w, x, y, z) where w^2 + x^2 + y^2 + z^2 = 1. - Then the length of the sterographic projection vector is
(x^2 + y^2 + z^2)/(1-w)^2, which is 1-w^2/(1-w)^2 ?? SOMETHING IS WRONG! - Recall the intuition for the sterographic projection, wrt
S2 and R3. - For a point
p ∈ S2, draw a line l, from the north pole (0, 0, 1)to the point p. The projection is the point of intersection of l with the xy plane. - Same thing a dimension up.
§ References
- An Elementary Introduction to the Hopf Fibration, by David W Lyons.