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Recall that the Mandelbrot set arises from iterating the complex function z^{2} + c, where c is a set of points in the complex plane. Those values of c for which z, initially zero, remains bounded are in the set, and those which increase forever are not. The (quadratic) Julia set is similar, but now z starts at those points in the complex plane, while c remains at some fixed complex value.

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In the context of complex dynamics, a topic of mathematics, the **Julia set** and the Fatou set are two complementary sets(Julia ‘laces’ and Fatou ‘dusts’) defined from a function. Informally, the Fatou set of the function consists of values with the property that all nearby values behave similarly under repeated iteration of the function, and the Julia set consists of values such that an arbitrarily small perturbation can cause drastic changes in the sequence of iterated function values. Thus the behavior of the function on the Fatou set is ‘regular’, while on the Julia set its behavior is ‘chaotic‘.

According to Paul Bourke:

The Julia set is named after the French mathematician Gaston Julia who investigated their properties circa 1915 and culminated in his famous paper in 1918. While the Julia set is now associated with a simpler polynomial, Julia was interested in the iterative properties of a more general expression, namely z^{4} + z^{3}/(z-1) + z^{2}/(z^{3} + 4 z^{2} + 5) + c.

The Julia set is now associated with those points z = x + iy on the complex plane for which the series z_{n+1} = z_{n}^{2} + c does not tend to infinity. c is a complex constant, one gets a different Julia set for each c. The initial value z_{0} for the series is each point in the image plane. In the broader sense the exact form of the iterated function may be anything, the general form being z_{n+1} = f(z_{n}), interesting sets arise with nonlinear functions f(z). Commonly used functions include the following:

z_{n+1} = c sin(z_{n}) |
z_{n+1} = c exp(z_{n}) |

z_{n+1} = c i cos(z_{n}) |
z_{n+1} = c z_{n} (1 – z_{n}) |

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