# 2. Strange & Complex

## 2.2 Julia Sets

Julia sets rendered with Object Mandelbrot & Julia's Dream.

Let's return for a while to our original map

ƒ: x → x^{2} + c.

The graph of this function is a parabola when "x" and "c" are real numbers. The orbits of well-behaved seeds are bounded for parameter values in the interval [−2, ¼]. These orbits can settle on to attracting fixed points, be periodic, or ergodic. A small set of fixed points, the repelling fixed points, do not generate orbits in the traditional sense. They neither roam nor run off to infinity and one need not wait for them to exhibit "characteristic" behavior. They are permanently and immutably fixed and nearby points avoid them. They lie on the frontier between those seeds with bounded orbits and those with unbounded orbits. Such is the behavior in general for all points and all parameter values — or is it?

The discussion so far has been constrained by a prejudice for real numbers. What happens when we admit that i^{2} = −1 has a solution? How does our function behave when "z" and "c" are complex numbers? The answer, of course, is the same but the results are much more interesting than such a flip statement implies.

The map…

ƒ: z → z^{2} + c

is equivalent to the two-dimensional map…

ƒ: (x, y) → (x^{2} − y^{2} + a, 2xy + b)

where z = x + iy = (x, y) is a point to be iterated and c =

Actually, it's easier to discuss these transformations if we represent the complex numbers as points on a complex sphere. The origin would be one pole and infinity another pole with the unit sphere being the equator. Imagine placing a light bulb at the infinity pole. Points on the sphere would leave shadows in unique positions on the plane. The complex plane is thus a projection of the complex sphere. While this is easier to deal with because we have a single point called infinity, it is not easier to diagram. Let's give it a shot.

This family of mappings is said to be conformal; that is, it leaves angles unchanged. Despite all this stretching, twisting, and shifting there is always a set of points that transforms into itself. Such sets are called the Julia sets after the French mathematician Gaston Julia who first conceived of them in the 1910s. The special case of c =

Sets on the real axis are reflection symmetric while those with complex parameter values show rotational symmetry. With the exception of the parameter value c =