Symmetric rational maps
Quadratic rational maps fc(z) = (z2 + c) / (1 + cz2) form the family of symmetric maps, since they commute with the inversion z ↦ 1/z. The videos illustrate applications of the Thurston algorithm to construct these maps from polynomials. The visualization of mating is based on the Buff–Chéritat approach to slow mating.Mating and anti-mating
Definitions of mating and anti-mating are given here.Two symmetric maps are related by f1/c(z) = fc(1/z) = 1/fc(z), and we have fc(z) ∼ P ∐ P, if and only if f1/c(z) ∼ P ∏ P.
Mixung is a generalization of self-anti-matings, see arXiv:2209.08012.
The self-matings of the Rabbit and of the Kokopelli: play — show.
The classical example of a shared mating, Airplane ∐ Rabbit is conjugate to Rabbit ∐ Airplane by a rotation. They are conjugate to a symmetric map fc(z), which is not a self-mating: play — show.
Deformation of M to the loci of self-matings and and self-anti-matings: play — show.
Locus of the 1/3-limb mated and anti-mated with itself: play — show.
The 1/4-vein mated and anti-mated with itself: play — show.
Lattès maps
When a mating gives a Lattès map of type (2, 2, 2, 2), the Thurston pullback diverges in general; the point configurations spiral toward a center manifold. This is illustrated with a zoom of the video around a postcritical point. See the joint paper [B6] with Arnaud Chéritat and the poster from the conference celebrating Jack Milnor.1/12 ∐ 5/12 (divergent, non-self, f not symmetric): play — show.
See the path of point configurations: play — show.
1/4 ∐ 1/4 (convergent, self-mating, f symmetric): play — show.
See the path of point configurations: play — show.
53/60 ∐ 29/60 (divergent, non-self, f symmetric, the same): play — show.
See the path of point configurations: play — show.
3/14 ∐ 3/14 (divergent, self-mating, f symmetric): play — show.
See the path of point configurations: play — show.
1/6 ∐ 1/6 (divergent, self-mating, f symmetric): play — show.
See the path of point configurations: play — show.
Chebyshev maps
For a Chebyshev map ya(z) = (-z2 + a + 2) / (z2 + a), we have ∞ ↦ -1 ↦ 1, and 1 is fixed. The Petersen transformation sends fc(z) and f1/c(z) to the same Chebyshev map, and especially P ∐ P and P ∏ P to P ∐ T with T(z) = z2 - 2.other possibilities, here veins through period 3, when equal
veins ...: play — show.
veins ...: play — show.