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Field · Emerged 1918 – 1985

Complex Dynamics

What happens when a simple formula on the complex numbers is applied over and over again?

4 chapters4 min read5 turning points1 open problem

Branched from
Dynamical Systems + Complex Analysis
Branched into
Not yet surveyed past here
Figures
Gaston Julia, Pierre Fatou, Robert Brooks, J. Peter Matelski, Benoit Mandelbrot, Adrien Douady, John Hubbard, Dennis Sullivan, Mitsuhiro Shishikura

In brief

Complex dynamics studies what happens when a function of a complex number, as simple as z↦z2+cz \mapsto z^2 + c, is applied repeatedly. Some starting points stay bounded forever and others escape to infinity. The boundary between them, the Julia set, is usually a fractal of infinite intricacy. The Mandelbrot set catalogues, for every cc at once, which kind of Julia set appears.

Pierre Fatou and Gaston Julia founded the subject around 1918 using the tools of complex analysis, without being able to see what they described. It was largely dormant until computers drew the pictures in the late 1970s. Douady, Hubbard, Sullivan and others then turned the pictures into theorems, and the Mandelbrot set became one of the best-known images in mathematics. Whether it is locally connected is still unknown.

Key ideas

IterationEnters 1918 – 1920

Applying the same function again and again: z0z_0, f(z0)f(z_0), f(f(z0))f(f(z_0)), and so on. The sequence of results is the orbit of z0z_0.

Julia set and Fatou setEnters 1918 – 1920

The Fatou set is where iteration behaves tamely, so nearby points stay nearby. The Julia set is the rest, where it is chaotic. For polynomials, the Julia set is the boundary of the set of points whose orbits stay bounded.

Mandelbrot setEnters 1982

The set of values cc for which the orbit of 0 under z↦z2+cz \mapsto z^2 + c stays bounded. It is exactly the set of cc whose Julia set is connected.

FractalEnters 1978 – 1980

A shape with detail at every scale, often with a fractional dimension. Mandelbrot coined the word in 1975, and Julia sets are among the richest examples.

Chapter I

Iteration Without Pictures

In 1918 the Paris Academy of Sciences offered its Grand Prix for work on iterating functions. The winner was Gaston Julia, aged twenty-five, who had lost his nose to a wound in the First World War and wore a leather patch for the rest of his life. Pierre Fatou had reached many of the same results independently, and the two quarrelled bitterly over priority. Between them they used the new theory of normal families from complex analysis to split the plane into a region where iteration is tame and a region where it is chaotic.

They could only imagine what these regions looked like. Calculating even one detailed picture by hand was out of the question. After a burst of activity, the subject lay mostly dormant for sixty years.

Chapter II

The Pictures Arrive

By the late 1970s computers could test millions of points. Robert Brooks and Peter Matelski printed a crude image in 1978 of the set of parameters cc for which z2+cz^2 + c keeps 0 bounded. Benoit Mandelbrot, at IBM, drew it in detail and saw that it was extraordinary. Zooming in reveals spirals, filaments and tiny copies of the whole set, without end. Mandelbrot had coined the word "fractal" in 1975 for shapes with detail at every scale, and this became its emblem.

Then the pictures became theorems. Adrien Douady and John Hubbard proved in 1982 that the set is connected, although the pictures seemed to show separate islands, and named it after Mandelbrot. In 1985 Dennis Sullivan settled a question left open by Fatou, using methods borrowed from hyperbolic geometry.

Chapter III

A Closer Look: Bounded or Escaping?

Take the rule z↦z2+cz \mapsto z^2 + c, start from z=0z = 0 and watch what happens for a few values of cc:

ccOrbit of 0Fate
000,0,0,…0, 0, 0, \ldotsfixed, bounded
−1-1−1,0,−1,0,…-1, 0, -1, 0, \ldotscycle of length 2, bounded
iii, −1+i, −i, −1+i, −i,…i,\ -1+i,\ -i,\ -1+i,\ -i, \ldotseventually a 2-cycle, bounded
−2-2−2,2,2,2,…-2, 2, 2, 2, \ldotsfixed from then on, bounded
111,2,5,26,677,…1, 2, 5, 26, 677, \ldotsescapes to infinity

For c=ic = i, squaring −1+i-1 + i gives (−1)2+2(−1)(i)+i2=−2i(-1)^2 + 2(-1)(i) + i^2 = -2i, and adding ii gives −i-i. Squaring −i-i gives −1-1, and adding ii gives −1+i-1 + i again. The orbit is trapped.

The Mandelbrot set is the set of all cc whose orbit stays bounded, so 00, −1-1, ii and −2-2 are in it and 11 is not. There is a simple test: once an orbit gets farther than 2 from the origin, it must escape. That is how computers draw the set, colouring each cc by how many steps its orbit takes to pass distance 2.

The boundary is where it gets hard. The real number c=0.25c = 0.25 is in the set: its orbit creeps up towards 0.50.5 and never passes it. But c=0.26c = 0.26, only a hundredth larger, escapes after 30 steps, and c=0.251c = 0.251 after 97. The closer cc is to the boundary, the longer it takes to decide. For points exactly on the boundary, no finite computation can settle the question. That is why the set's finest structure is still not fully understood.

Chapter IV

Still Unmapped

In 1998 Mitsuhiro Shishikura proved that the boundary of the Mandelbrot set is as complicated as a boundary in the plane can be, with dimension 2. The central conjecture of the field, that the set is locally connected, would give a complete description of it, and with it of all quadratic dynamical systems. Jean-Christophe Yoccoz proved it at most points, and his work contributed to his Fields Medal in 1994. The remaining points, deep inside nested copies of the set, are still out of reach. The same zooming, or renormalisation, that produces those copies also explains the universal constants of chaos theory.

Applications

Where it is used

  • Numerical computation

    Where Newton's method goes

    Newton's method for finding roots is an iteration, and Cayley asked in 1879 which starting points lead to which root. Complex dynamics answers it: the basins are separated by fractal Julia sets. The theory also gives explicit starting points that are guaranteed to find every root of a polynomial.

    › Sources (1)
    • Hubbard, J., Schleicher, D. & Sutherland, S. (2001). How to find all roots of complex polynomials by Newton's method. Inventiones Mathematicae 146(1): 1–33.
  • Computer graphics

    Fractal landscapes

    Fractal geometry gave graphics a way to generate mountains, coastlines and clouds from a few rules. Loren Carpenter's fractal terrain in 1980 led to the first computer-generated planet sequence in a feature film, in Star Trek II (1982).

    › Sources (1)
    • Fournier, A., Fussell, D. & Carpenter, L. (1982). Computer rendering of stochastic models. Communications of the ACM 25(6): 371–384.
  • Universality↗ Physics · Phase Transitions

    Why Feigenbaum's constant is universal

    Physicists explained the universality of period doubling with a renormalisation argument, a zoom that turns a system into a smaller copy of itself. Mathematicians working in complex dynamics, notably Sullivan, McMullen and Lyubich, turned that argument into a proof, explaining numbers measured in fluids and circuits.

    › Sources (1)
    • Lyubich, M. (1999). Feigenbaum–Coullet–Tresser universality and Milnor's hairiness conjecture. Annals of Mathematics 149(2): 319–420.

Open problems

Where the map runs out

Open

Is the Mandelbrot set locally connected? (MLC)

Open as of 2026; proved at many parameter values, beginning with Yoccoz's work around 1990 and most recently at the Feigenbaum points (Dudko and Lyubich).

Douady and Hubbard conjectured that the Mandelbrot set is locally connected: near each of its points, the nearby parts are connected to each other, with no infinitely fine comb-like structure. If true, their theory gives a complete combinatorial description of the whole set.

Why it is hard

Local connectivity has to be proved at every point of the boundary, and different points need different techniques. Jean-Christophe Yoccoz proved it at all points except those lying in infinitely many nested smaller copies of the set, where renormalisation methods are needed and are only partly understood.

What resolving it unlocks

MLC implies the density of hyperbolicity for quadratic polynomials: every cc can be moved, by an arbitrarily small change, to a parameter with stable, predictable dynamics. It would complete the description of the simplest non-trivial family of dynamical systems.

› Sources (2)
  • Douady, A. & Hubbard, J. H. (1984–1985). Étude dynamique des polynômes complexes I–II. Publications Mathématiques d'Orsay.
  • Milnor, J. (2006). Dynamics in One Complex Variable (3rd ed.). Princeton University Press.

Further reading

  1. Peitgen, H.-O. & Richter, P. H. (1986). The Beauty of Fractals. Springer.

    The book of pictures that popularised Julia and Mandelbrot sets, with the mathematics behind them.

  2. Mandelbrot, B. B. (1982). The Fractal Geometry of Nature. W. H. Freeman.

    Mandelbrot's manifesto for fractals, wide-ranging and idiosyncratic.

  3. Milnor, J. (2006). Dynamics in One Complex Variable (3rd ed.). Princeton University Press.

    The standard graduate text, clearly written.