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The eight families

Everything in the previous chapters came from one rule, zz2+cz \mapsto z^2 + c. Change the rule and you get a different universe with the same physics: iterate, watch the orbit, colour by its fate. Mandala ships eight families — six that colour by escape, and two that colour by convergence. Equations first; each figure opens the real thing.

The escape-time six

FamilyRule
Mandelbrotzz2+cz \mapsto z^2 + c
Multibrotzz3+cz \mapsto z^3 + c
Tricornzzˉ2+cz \mapsto \bar{z}^2 + c
Burning Shipz(Rez+iImz)2+cz \mapsto \left(\lvert\operatorname{Re} z\rvert + i\,\lvert\operatorname{Im} z\rvert\right)^2 + c
CelticzRe(z2)+iIm(z2)+cz \mapsto \lvert\operatorname{Re}(z^2)\rvert + i\operatorname{Im}(z^2) + c
Phoenixzz2+c+pzprevz \mapsto z^2 + c + p\,z_{\text{prev}}
The full Mandelbrot set in green and yellow on dark blue
The Mandelbrot set. The standard opening view: the cardioid, its bulbs, and the antenna to the west. Interior points are black; the exterior is coloured by escape speed. centre −0.7 · span 3.0 · open this view in Mandala →
The two-lobed degree-3 Multibrot set
Multibrot, degree 3. Raise z to the third power instead and the cardioid grows a second cusp — degree d gives d − 1-fold symmetry. centre 0 · span 2.5 · open this view in Mandala →

Mandelbrot is the original. Multibrot raises the power to z3z^3: the body grows a second cusp and the bulbs arrange themselves with two-fold symmetry — in general, degree dd gives d1d-1 symmetry axes, because the critical points and the map's rotational structure repeat that many times around the origin.

The three-fold symmetric Tricorn set
The Tricorn. Conjugate z before squaring and the set turns three-cornered — the Mandelbar. centre −0.5 · span 3.6 · open this view in Mandala →
A ship-like fractal silhouette in fire colours
The Burning Ship. The hull and rigging of the Burning Ship — the |z| fold turns Mandelbrot curls into masts and flames. c ≈ −1.75 + 0.0175i · span 0.1 · open this view in Mandala →

Tricorn conjugates before squaring — zˉ\bar z flips the imaginary part each step — and the set turns three-cornered. Burning Ship takes absolute values of both coordinates first; that fold in the plane breaks the symmetry of smooth curls and turns them into masts, hulls and flame. It is most dramatic just west of the main body, where a whole armada of smaller ships sails.

The Celtic fractal with knot-like folded structures
The Celtic. Fold just the real part with an absolute value and knotwork appears along the axis. centre −0.85 · span 3.4 · open this view in Mandala →
A symmetric winged fractal in glowing magma colours
The Phoenix. Ushiki’s classic Phoenix attractor — the previous iterate feeds back in, and wings unfold. Phoenix preset: c = 0.5667, p = −0.5 · z-plane span 3.0 · open this view in Mandala →

Celtic folds only the real part of z2z^2, which weaves knotwork along the axis. Phoenix is the strangest of the six: the previous iterate feeds back in with weight pp, giving orbits a one-step memory — the state of the system is really the pair (zn,zn1)(z_n, z_{n-1}). Its classic form — Ushiki's Phoenix, p=0.5p = -0.5 with c=0.5667c = 0.5667 — is viewed in the dynamical plane and spreads wings.

Analytic and non-analytic — a distinction that matters

Mandelbrot and Multibrot are analytic (holomorphic): their rules are polynomials in zz, differentiable in the complex sense. Tricorn, Burning Ship and Celtic are notzˉ\bar z and \lvert\cdot\rvert are folds, not complex-differentiable operations (Phoenix adds the memory term on top). Visually the folds are the point: they create the creases and flames. But the distinction also has hard consequences for the machinery — an analytic map has a well-defined complex derivative to iterate, which powers the shading of the shading chapter and the iteration-skipping tricks of the deep-zoom chapter; the non-analytic families need per-family care to reach the same depths.

The root-finders

Three coloured basins meeting in braided fractal chains
Newton basins of z³ − 1. Newton’s method pulled toward three roots — the basins meet along an infinitely braided boundary. z-plane · span 3.0 · open this view in Mandala →
The Nova fractal parameter plane with minibrot-like shapes
Nova. Newton’s method with a nudge: add c each step and minibrot-like bodies float over the convergence basins. c-plane, centre 0 · span 2.5 · open this view in Mandala →

Newton colours a different question entirely. Apply Newton's root-finding method to p(z)=z31p(z) = z^3 - 1:

zzp(z)p(z)=zz313z2,z \mapsto z - \frac{p(z)}{p'(z)} = z - \frac{z^3-1}{3z^2},

and ask which of the three cube roots of unity each starting point falls into. There is no escape to infinity, and almost every point converges to one of the three roots — but not all of them do: a measure-zero set, the basin boundary (the Newton map's Julia set), never settles. Those basins meet along that boundary so contested that between any two colours the third always intrudes, and the points that never converge are painted black.

Nova perturbs that method with a relaxation factor aa and an added constant:

zzap(z)p(z)+c,z \mapsto z - a\,\frac{p(z)}{p'(z)} + c,

and something remarkable happens: minibrot-like bodies — Mandelbrot's silhouette again — condense over the convergence basins. The same shape haunts entirely different mathematics; that universality is one of the deep facts of the field.

Every escape-time family has both planes (the Julia chapter) — a Burning Ship Julia set is one gesture away — and all six deep-zoom on the full precision ladder (the deep-zoom chapter). The two root-finders are the honest exception: they cap at the double-double tier, around 102710^{-27} — still a trillionfold past where ordinary arithmetic gives up.