Mandelbrot set
The Mandelbrot set (/ˈmændəlbroʊt, brɒt/)^{[1]}^{[2]} is a twodimensional set with a relatively simple definition that exhibits great complexity, especially as it is magnified. It is popular for its aesthetic appeal and fractal structures. The set is defined in the complex plane as the complex numbers for which the function does not diverge to infinity when iterated starting at , i.e., for which the sequence , , etc., remains bounded in absolute value.
This set was first defined and drawn by Robert W. Brooks and Peter Matelski in 1978, as part of a study of Kleinian groups.^{[3]} Afterwards, in 1980, Benoit Mandelbrot obtained highquality visualizations of the set while working at IBM's Thomas J. Watson Research Center in Yorktown Heights, New York.
Images of the Mandelbrot set exhibit an infinitely complicated boundary that reveals progressively everfiner recursive detail at increasing magnifications; mathematically, the boundary of the Mandelbrot set is a fractal curve. The "style" of this recursive detail depends on the region of the set boundary being examined. Mandelbrot set images may be created by sampling the complex numbers and testing, for each sample point , whether the sequence goes to infinity. Treating the real and imaginary parts of as image coordinates on the complex plane, pixels may then be colored according to how soon the sequence crosses an arbitrarily chosen threshold (the threshold must be at least 2, as 2 is the complex number with the largest magnitude within the set, but otherwise the threshold is arbitrary). If is held constant and the initial value of is varied instead, the corresponding Julia set for the point is obtained.
The Mandelbrot set has become popular outside mathematics both for its aesthetic appeal and as an example of a complex structure arising from the application of simple rules. It is one of the bestknown examples of mathematical visualization, mathematical beauty, and motif.
History[edit]
The Mandelbrot set has its origin in complex dynamics, a field first investigated by the French mathematicians Pierre Fatou and Gaston Julia at the beginning of the 20th century. The fractal was first defined and drawn in 1978 by Robert W. Brooks and Peter Matelski as part of a study of Kleinian groups.^{[3]} On 1 March 1980, at IBM's Thomas J. Watson Research Center in Yorktown Heights, New York, Benoit Mandelbrot first visualized the set.^{[4]}
Mandelbrot studied the parameter space of quadratic polynomials in an article that appeared in 1980.^{[5]} The mathematical study of the Mandelbrot set really began with work by the mathematicians Adrien Douady and John H. Hubbard (1985),^{[6]} who established many of its fundamental properties and named the set in honor of Mandelbrot for his influential work in fractal geometry.
The mathematicians HeinzOtto Peitgen and Peter Richter became well known for promoting the set with photographs, books (1986),^{[7]} and an internationally touring exhibit of the German GoetheInstitut (1985).^{[8]}^{[9]}
The cover article of the August 1985 Scientific American introduced the algorithm for computing the Mandelbrot set. The cover was created by Peitgen, Richter and Saupe at the University of Bremen.^{[10]} The Mandelbrot set became prominent in the mid1980s as a computergraphics demo, when personal computers became powerful enough to plot and display the set in high resolution.^{[11]}
The work of Douady and Hubbard occurred during an increase in interest in complex dynamics and abstract mathematics,^{[12]} and the study of the Mandelbrot set has been a centerpiece of this field ever since.^{[citation needed]}
Formal definition[edit]
This section needs additional citations for verification. (September 2023) 
The Mandelbrot set is the set of values of c in the complex plane for which the orbit of the critical point under iteration of the quadratic map
remains bounded.^{[13]} Thus, a complex number c is a member of the Mandelbrot set if, when starting with and applying the iteration repeatedly, the absolute value of remains bounded for all .
For example, for c = 1, the sequence is 0, 1, 2, 5, 26, ..., which tends to infinity, so 1 is not an element of the Mandelbrot set. On the other hand, for , the sequence is 0, −1, 0, −1, 0, ..., which is bounded, so −1 does belong to the set.
The Mandelbrot set can also be defined as the connectedness locus of the family of quadratic polynomials , the subset of the space of parameters for which the Julia set of the corresponding polynomial forms a connected set. In the same way, the boundary of the Mandelbrot set can be defined as the bifurcation locus of this quadratic family, the subset of parameters near which the dynamic behavior of the polynomial (when it is iterated repeatedly) changes drastically.
Basic properties[edit]
The Mandelbrot set is a compact set, since it is closed and contained in the closed disk of radius 2 around the origin. A point belongs to the Mandelbrot set if and only if for all . In other words, the absolute value of must remain at or below 2 for to be in the Mandelbrot set, , and if that absolute value exceeds 2, the sequence will escape to infinity. Since , it follows that , establishing that will always be in the closed disk of radius 2 around the origin.^{[citation needed]}
The intersection of with the real axis is the interval . The parameters along this interval can be put in onetoone correspondence with those of the real logistic family,
The correspondence is given by
This gives a correspondence between the entire parameter space of the logistic family and that of the Mandelbrot set.^{[citation needed]}
Douady and Hubbard showed that the Mandelbrot set is connected. They constructed an explicit conformal isomorphism between the complement of the Mandelbrot set and the complement of the closed unit disk. Mandelbrot had originally conjectured that the Mandelbrot set is disconnected. This conjecture was based on computer pictures generated by programs that are unable to detect the thin filaments connecting different parts of . Upon further experiments, he revised his conjecture, deciding that should be connected. A topological proof of the connectedness was discovered in 2001 by Jeremy Kahn.^{[14]}
The dynamical formula for the uniformisation of the complement of the Mandelbrot set, arising from Douady and Hubbard's proof of the connectedness of , gives rise to external rays of the Mandelbrot set. These rays can be used to study the Mandelbrot set in combinatorial terms and form the backbone of the Yoccoz parapuzzle.^{[15]}
The boundary of the Mandelbrot set is the bifurcation locus of the family of quadratic polynomials. In other words, the boundary of the Mandelbrot set is the set of all parameters for which the dynamics of the quadratic map exhibits sensitive dependence on i.e. changes abruptly under arbitrarily small changes of It can be constructed as the limit set of a sequence of plane algebraic curves, the Mandelbrot curves, of the general type known as polynomial lemniscates. The Mandelbrot curves are defined by setting , and then interpreting the set of points in the complex plane as a curve in the real Cartesian plane of degree in x and y.^{[16]} Each curve is the mapping of an initial circle of radius 2 under . These algebraic curves appear in images of the Mandelbrot set computed using the "escape time algorithm" mentioned below.
Other properties[edit]
Main cardioid and period bulbs[edit]
The main cardioid is the period 1 continent. It is the region of parameters for which the map
has an attracting fixed point. It consists of all parameters of the form
for some in the open unit disk.
To the left of the main cardioid, attached to it at the point , a circular bulb, the period2 bulb is visible. The bulb consists of for which has an attracting cycle of period 2. It is the filled circle of radius 1/4 centered around −1.
More generally, for every positive integer , there are circular bulbs tangent to the main cardioid called periodq bulbs (where denotes the Euler phi function), which consist of parameters for which has an attracting cycle of period . More specifically, for each primitive th root of unity (where ), there is one periodq bulb called the bulb, which is tangent to the main cardioid at the parameter
and which contains parameters with cycles having combinatorial rotation number . More precisely, the periodic Fatou components containing the attracting cycle all touch at a common point (commonly called the fixed point). If we label these components in counterclockwise orientation, then maps the component to the component .
The change of behavior occurring at is known as a bifurcation: the attracting fixed point "collides" with a repelling periodq cycle. As we pass through the bifurcation parameter into the bulb, the attracting fixed point turns into a repelling fixed point (the fixed point), and the periodq cycle becomes attracting.
Hyperbolic components[edit]
Bulbs that are interior components of the Mandelbrot set in which the maps have an attracting periodic cycle are called hyperbolic components.^{[citation needed]}
It is conjectured that these are the only interior regions of and that they are dense in . This problem, known as density of hyperbolicity, is one of the most important open problems in complex dynamics.^{[17]} Hypothetical nonhyperbolic components of the Mandelbrot set are often referred to as "queer" or ghost components.^{[18]}^{[19]} For real quadratic polynomials, this question was proved in the 1990s independently by Lyubich and by Graczyk and Świątek. (Note that hyperbolic components intersecting the real axis correspond exactly to periodic windows in the Feigenbaum diagram. So this result states that such windows exist near every parameter in the diagram.)
Not every hyperbolic component can be reached by a sequence of direct bifurcations from the main cardioid of the Mandelbrot set. Such a component can be reached by a sequence of direct bifurcations from the main cardioid of a little Mandelbrot copy (see below).
Each of the hyperbolic components has a center, which is a point c such that the inner Fatou domain for has a superattracting cycle—that is, that the attraction is infinite. This means that the cycle contains the critical point 0, so that 0 is iterated back to itself after some iterations. Therefore, for some n. If we call this polynomial (letting it depend on c instead of z), we have that and that the degree of is . Therefore, constructing the centers of the hyperbolic components is possible by successively solving the equations .^{[citation needed]} The number of new centers produced in each step is given by Sloane's OEIS: A000740.
Local connectivity[edit]
It is conjectured that the Mandelbrot set is locally connected. This conjecture is known as MLC (for Mandelbrot locally connected). By the work of Adrien Douady and John H. Hubbard, this conjecture would result in a simple abstract "pinched disk" model of the Mandelbrot set. In particular, it would imply the important hyperbolicity conjecture mentioned above.^{[citation needed]}
The work of JeanChristophe Yoccoz established local connectivity of the Mandelbrot set at all finitely renormalizable parameters; that is, roughly speaking those contained only in finitely many small Mandelbrot copies.^{[20]} Since then, local connectivity has been proved at many other points of , but the full conjecture is still open.
Selfsimilarity[edit]
The Mandelbrot set is selfsimilar under magnification in the neighborhoods of the Misiurewicz points. It is also conjectured to be selfsimilar around generalized Feigenbaum points (e.g., −1.401155 or −0.1528 + 1.0397i), in the sense of converging to a limit set.^{[21]}^{[22]} The Mandelbrot set in general is quasiselfsimilar, as small slightly different versions of itself can be found at arbitrarily small scales. These copies of the Mandelbrot set are all slightly different, mostly because of the thin threads connecting them to the main body of the set.^{[citation needed]}
Further results[edit]
The Hausdorff dimension of the boundary of the Mandelbrot set equals 2 as determined by a result of Mitsuhiro Shishikura.^{[23]} The fact that this is greater by a whole integer than its topological dimension, which is 1, reflects the extreme fractal nature of the Mandelbrot set boundary. Roughly speaking, Shishikura's result states that the Mandelbrot set boundary is so "wiggly" that it locally fills space as efficiently as a twodimensional planar region. Curves with Hausdorff dimension 2, despite being (topologically) 1dimensional, are oftentimes capable of having nonzero area (more formally, a nonzero planar Lebesgue measure). Whether this is the case for the Mandelbrot set boundary is an unsolved problem.^{[citation needed]}
It has been shown that the generalized Mandelbrot set in higherdimensional hypercomplex number spaces (i.e. when the power of the iterated variable tends to infinity) is convergent to the unit (1)sphere.^{[24]}
In the Blum–Shub–Smale model of real computation, the Mandelbrot set is not computable, but its complement is computably enumerable. Many simple objects (e.g., the graph of exponentiation) are also not computable in the BSS model. At present, it is unknown whether the Mandelbrot set is computable in models of real computation based on computable analysis, which correspond more closely to the intuitive notion of "plotting the set by a computer". Hertling has shown that the Mandelbrot set is computable in this model if the hyperbolicity conjecture is true.^{[citation needed]}
Relationship with Julia sets[edit]
As a consequence of the definition of the Mandelbrot set, there is a close correspondence between the geometry of the Mandelbrot set at a given point and the structure of the corresponding Julia set. For instance, a value of c belongs to the Mandelbrot set if and only if the corresponding Julia set is connected. Thus, the Mandelbrot set may be seen as a map of the connected Julia sets.^{[citation needed]}
This principle is exploited in virtually all deep results on the Mandelbrot set. For example, Shishikura proved that, for a dense set of parameters in the boundary of the Mandelbrot set, the Julia set has Hausdorff dimension two, and then transfers this information to the parameter plane.^{[23]} Similarly, Yoccoz first proved the local connectivity of Julia sets, before establishing it for the Mandelbrot set at the corresponding parameters.^{[20]}
Geometry[edit]
For every rational number , where p and q are relatively prime, a hyperbolic component of period q bifurcates from the main cardioid at a point on the edge of the cardioid corresponding to an internal angle of .^{[25]} The part of the Mandelbrot set connected to the main cardioid at this bifurcation point is called the p/qlimb. Computer experiments suggest that the diameter of the limb tends to zero like . The best current estimate known is the Yoccozinequality, which states that the size tends to zero like .^{[citation needed]}
A periodq limb will have "antennae" at the top of its limb. The period of a given bulb is determined by counting these antennas. The numerator of the rotation number, p, is found by numbering each antenna counterclockwise from the limb from 1 to and finding which antenna is the shortest.^{[25]}
Pi in the Mandelbrot set[edit]
In an attempt to demonstrate that the thickness of the p/qlimb is zero, David Boll carried out a computer experiment in 1991, where he computed the number of iterations required for the series to diverge for ( being the location thereof). As the series does not diverge for the exact value of , the number of iterations required increases with a small . It turns out that multiplying the value of with the number of iterations required yields an approximation of that becomes better for smaller . For example, for = 0.0000001, the number of iterations is 31415928 and the product is 3.1415928.^{[26]} In 2001, Aaron Klebanoff proved Boll's discovery.^{[27]}
Fibonacci sequence in the Mandelbrot set[edit]
It can be shown that the Fibonacci sequence is located within the Mandelbrot set and that a relation exists between the main cardioid and the Farey diagram.^{[28]} Upon mapping the main cardioid to a disk, the amount of antennae that extends from the next largest hyperbolic component, and that is located between the two previously selected components, follows suit with the Fibonacci sequence. The amount of antennae also correlates with the Farey diagram and the denominator amounts within the corresponding fractional values, of which relate to the distance around the disk. Both portions of these fractional values themselves can be summed together after to produce the location of the next hyperbolic component within the sequence. Thus, the Fibonacci sequence of 1, 2, 3, 5, 8, 13, and 21 can be found within the Mandelbrot set.
Image gallery of a zoom sequence[edit]
The boundary of the Mandelbrot set shows more intricate detail the closer one looks or magnifies the image. The following is an example of an image sequence zooming to a selected c value.
The magnification of the last image relative to the first one is about 10^{10} to 1. Relating to an ordinary computer monitor, it represents a section of a Mandelbrot set with a diameter of 4 million kilometers.

Start. Mandelbrot set with continuously colored environment.

Gap between the "head" and the "body", also called the "seahorse valley"

Doublespirals on the left, "seahorses" on the right

"Seahorse" upside down
The seahorse "body" is composed by 25 "spokes" consisting of two groups of 12 "spokes" each and one "spoke" connecting to the main cardioid. These two groups can be attributed by some metamorphosis to the two "fingers" of the "upper hand" of the Mandelbrot set; therefore, the number of "spokes" increases from one "seahorse" to the next by 2; the "hub" is a Misiurewicz point. Between the "upper part of the body" and the "tail", there is a distorted copy of the Mandelbrot set, called a "satellite".

The central endpoint of the "seahorse tail" is also a Misiurewicz point.

Part of the "tail" – there is only one path consisting of the thin structures that lead through the whole "tail". This zigzag path passes the "hubs" of the large objects with 25 "spokes" at the inner and outer border of the "tail"; thus the Mandelbrot set is a simply connected set, which means there are no islands and no loop roads around a hole.

Satellite. The two "seahorse tails" are the beginning of a series of concentric crowns with the satellite in the center.

Each of these crowns consists of similar "seahorse tails"; their number increases with powers of 2, a typical phenomenon in the environment of satellites. The unique path to the spiral center passes the satellite from the groove of the cardioid to the top of the "antenna" on the "head".

"Antenna" of the satellite. There are several satellites of second order.

The "seahorse valley" of the satellite. All the structures from the start reappear.

Doublespirals and "seahorses" – unlike the second image from the start, they have appendices consisting of structures like "seahorse tails"; this demonstrates the typical linking of n + 1 different structures in the environment of satellites of the order n, here for the simplest case n = 1.

Doublespirals with satellites of second order – analogously to the "seahorses", the doublespirals may be interpreted as a metamorphosis of the "antenna".

In the outer part of the appendices, islands of structures may be recognized; they have a shape like Julia sets J_{c}; the largest of them may be found in the center of the "doublehook" on the right side.

Part of the "doublehook".

Islands.

A detail of one island.

Detail of the spiral.
The islands in the thirdtolast step seem to consist of infinitely many parts, as is the case for the corresponding Julia set . They are connected by tiny structures, so that the whole represents a simply connected set. The tiny structures meet each other at a satellite in the center that is too small to be recognized at this magnification. The value of for the corresponding is not the image center but, relative to the main body of the Mandelbrot set, has the same position as the center of this image relative to the satellite shown in the 6th step.
Inner structure[edit]
While the Mandelbrot set is typically rendered showing outside boundary detail, structure within the bounded set can also be revealed. For example, while calculating whether or not a given c value is bound or unbound, while it remains bound, the maximum value that this number reaches can be compared to the c value at that location. If the sum of squares method is used, the calculated number would be max:(real^2 + imaginary^2)  c:(real^2 + imaginary^2). The magnitude of this calculation can be rendered as a value on a gradient.
This produces results like the following, gradients with distinct edges and contours as the boundaries are approached. The animations serve to highlight the gradient boundaries.

Animated gradient structure inside the Mandelbrot set

Animated gradient structure inside the Mandelbrot set, detail

Rendering of progressive iterations from 285 to approximately 200,000 with corresponding bounded gradients animated

Thumbnail for gradient in progressive iterations
Generalizations[edit]
Multibrot sets[edit]
Multibrot sets are bounded sets found in the complex plane for members of the general monic univariate polynomial family of recursions
 .^{[citation needed]}
For an integer d, these sets are connectedness loci for the Julia sets built from the same formula. The full cubic connectedness locus has also been studied; here one considers the twoparameter recursion , whose two critical points are the complex square roots of the parameter k. A parameter is in the cubic connectedness locus if both critical points are stable.^{[29]} For general families of holomorphic functions, the boundary of the Mandelbrot set generalizes to the bifurcation locus.^{[citation needed]}
The Multibrot set is obtained by varying the value of the exponent d. The article has a video that shows the development from d = 0 to 7, at which point there are 6 i.e. lobes around the perimeter. In general, when d is a positive integer, the central region in each of these sets is always an epicycloid of cusps. A similar development with negative integral exponents results in clefts on the inside of a ring, where the main central region of the set is a hypocycloid of cusps.^{[citation needed]}
Higher dimensions[edit]
There is no perfect extension of the Mandelbrot set into 3D, because there is no 3D analogue of the complex numbers for it to iterate on. There is an extension of the complex numbers into 4 dimensions, the quaternions, that creates a perfect extension of the Mandelbrot set and the Julia sets into 4 dimensions.^{[30]} These can then be either crosssectioned or projected into a 3D structure. The quaternion (4dimensional) Mandelbrot set is simply a solid of revolution of the 2dimensional Mandelbrot set (in the jk plane), and is therefore uninteresting to look at.^{[30]} Taking a 3dimensional cross section at results in a solid of revolution of the 2dimensional Mandelbrot set around the real axis.^{[citation needed]}
Other nonanalytic mappings[edit]
Of particular interest is the tricorn fractal, the connectedness locus of the antiholomorphic family
 .
The tricorn (also sometimes called the Mandelbar) was encountered by Milnor in his study of parameter slices of real cubic polynomials. It is not locally connected. This property is inherited by the connectedness locus of real cubic polynomials.
Another nonanalytic generalization is the Burning Ship fractal, which is obtained by iterating the following:
 .
Computer drawings[edit]
There exist a multitude of various algorithms for plotting the Mandelbrot set via a computing device. Here, the most widely used and simplest algorithm will be demonstrated, namely, the naïve "escape time algorithm". In the escape time algorithm, a repeating calculation is performed for each x, y point in the plot area and based on the behavior of that calculation, a color is chosen for that pixel.
The x and y locations of each point are used as starting values in a repeating, or iterating calculation (described in detail below). The result of each iteration is used as the starting values for the next. The values are checked during each iteration to see whether they have reached a critical "escape" condition, or "bailout". If that condition is reached, the calculation is stopped, the pixel is drawn, and the next x, y point is examined.
The color of each point represents how quickly the values reached the escape point. Often black is used to show values that fail to escape before the iteration limit, and gradually brighter colors are used for points that escape. This gives a visual representation of how many cycles were required before reaching the escape condition.
To render such an image, the region of the complex plane we are considering is subdivided into a certain number of pixels. To color any such pixel, let be the midpoint of that pixel. Iterate the critical point 0 under , checking at each step whether the orbit point has a radius larger than 2. When this is the case, does not belong to the Mandelbrot set, and color the pixel according to the number of iterations used to find out. Otherwise, keep iterating up to a fixed number of steps, after which we decide that our parameter is "probably" in the Mandelbrot set, or at least very close to it, and color the pixel black.
In pseudocode, this algorithm would look as follows. The algorithm does not use complex numbers and manually simulates complexnumber operations using two real numbers, for those who do not have a complex data type. The program may be simplified if the programming language includes complexdatatype operations.
for each pixel (Px, Py) on the screen do x0 := scaled x coordinate of pixel (scaled to lie in the Mandelbrot X scale (2.00, 0.47)) y0 := scaled y coordinate of pixel (scaled to lie in the Mandelbrot Y scale (1.12, 1.12)) x := 0.0 y := 0.0 iteration := 0 max_iteration := 1000 while (x*x + y*y ≤ 2*2 AND iteration < max_iteration) do xtemp := x*x  y*y + x0 y := 2*x*y + y0 x := xtemp iteration := iteration + 1
color := palette[iteration] plot(Px, Py, color)
Here, relating the pseudocode to , and :
and so, as can be seen in the pseudocode in the computation of x and y:
 and .
To get colorful images of the set, the assignment of a color to each value of the number of executed iterations can be made using one of a variety of functions (linear, exponential, etc.).
References in popular culture[edit]
The Mandelbrot set is widely considered the most popular fractal,^{[31]}^{[32]} and has been referenced several times in popular culture.
 The Jonathan Coulton song "Mandelbrot Set" is a tribute to both the fractal itself and to the man it is named after, Benoit Mandelbrot.^{[33]}
 Multiple track titles on the 1999 debut album by the Blue Man Group, Audio, refer to the Mandelbrot set. These are "Opening Mandelbrot", "Mandelgroove", and "Klein Mandelbrot".^{[34]}
 The second book of the Mode series by Piers Anthony, Fractal Mode, describes a world that is a perfect 3D model of the set.^{[35]}
 The Arthur C. Clarke novel The Ghost from the Grand Banks features an artificial lake made to replicate the shape of the Mandelbrot set.^{[36]}
 Benoit Mandelbrot and the eponymous set were the subjects of the Google Doodle on 20 November 2020 (the late Benoit Mandelbrot's 96th birthday).^{[37]}
 The American rock band Heart has an image of a Mandelbrot set on the cover of their 2004 album, Jupiters Darling.
 The British black metal band Anaal Nathrakh uses an image resembling the Mandelbrot set on their Eschaton album cover art.
 The television series Dirk Gently's Holistic Detective Agency (2016) prominently features the Mandelbrot set in connection with the visions of the character Amanda. In the second season, her jacket has a large image of the fractal on the back.^{[38]}
 In Ian Stewart's 2001 book Flatterland, there is a character called the Mandelblot, who helps explain fractals to the characters and reader.^{[39]}
 The unfinished Alan Moore 1990 comic book series Big Numbers used Mandelbrot's work on fractal geometry and chaos theory to underpin the structure of that work. Moore at one point was going to the name the comic book series The Mandelbrot Set.^{[40]}
 In the manga The Summer Hikaru Died, Yoshiki hallucinates the Mandelbrot set when he reaches into the body of the false Hikaru.
See also[edit]
References[edit]
 ^ "Mandelbrot set". Lexico UK English Dictionary. Oxford University Press. Archived from the original on 31 January 2022.
 ^ "Mandelbrot set". MerriamWebster.com Dictionary. Retrieved 30 January 2022.
 ^ ^{a} ^{b} Robert Brooks and Peter Matelski, The dynamics of 2generator subgroups of PSL(2,C), in Irwin Kra (1 May 1981). Irwin Kra (ed.). Riemann Surfaces and Related Topics: Proceedings of the 1978 Stony Brook Conference (PDF). Bernard Maskit. Princeton University Press. ISBN 0691082677. Archived from the original (PDF) on 28 July 2019. Retrieved 1 July 2019.
 ^ R.P. Taylor & J.C. Sprott (2008). "Biophilic Fractals and the Visual Journey of Organic Screensavers" (PDF). Nonlinear Dynamics, Psychology, and Life Sciences. Society for Chaos Theory in Psychology & Life Sciences. 12 (1): 117–129. PMID 18157930. Retrieved 1 January 2009.
 ^ Mandelbrot, Benoit (1980). "Fractal aspects of the iteration of for complex ". Annals of the New York Academy of Sciences. 357 (1): 249–259. doi:10.1111/j.17496632.1980.tb29690.x. S2CID 85237669.
 ^ Adrien Douady and John H. Hubbard, Etude dynamique des polynômes complexes, Prépublications mathémathiques d'Orsay 2/4 (1984 / 1985)
 ^ Peitgen, HeinzOtto; Richter Peter (1986). The Beauty of Fractals. Heidelberg: SpringerVerlag. ISBN 0387158510.
 ^ Frontiers of Chaos, Exhibition of the GoetheInstitut by H.O. Peitgen, P. Richter, H. Jürgens, M. Prüfer, D.Saupe. Since 1985 shown in over 40 countries.
 ^ Gleick, James (1987). Chaos: Making a New Science. London: Cardinal. p. 229.
 ^ "Exploring The Mandelbrot Set". Scientific American. 253 (2): 4. August 1985. JSTOR 24967754 – via JSTOR.
 ^ Pountain, Dick (September 1986). "Turbocharging Mandelbrot". Byte. Retrieved 11 November 2015.
 ^ Rees, Mary (January 2016). "One hundred years of complex dynamics". Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences. 472 (2185). doi:10.1098/rspa.2015.0453. PMC 4786033. PMID 26997888.
 ^ "Mandelbrot Set Explorer: Mathematical Glossary". Retrieved 7 October 2007.
 ^ Kahn, Jeremy (8 August 2001). "The Mandelbrot Set is Connected: a Topological Proof" (PDF).
 ^ The Mandelbrot set, theme and variations. Tan, Lei. Cambridge University Press, 2000. ISBN 9780521774765. Section 2.1, "Yoccoz parapuzzles", p. 121
 ^ Weisstein, Eric W. "Mandelbrot Set Lemniscate". Wolfram Mathworld. Retrieved 17 July 2023.
 ^ Anna Miriam Benini (2017). "A survey on MLC, Rigidity and related topics". arXiv:1709.09869 [math.DS].
 ^ Douady, Adrien; Hubbard, John H. Exploring the Mandelbrot set. The Orsay Notes. p. 12.
 ^ Jung, Wolf (2002). Homeomorphisms on Edges of the Mandelbrot Set (Doctoral thesis). RWTH Aachen University. urn:nbn:de:hbz:82opus3719.
 ^ ^{a} ^{b} Hubbard, J. H. (1993). "Local connectivity of Julia sets and bifurcation loci: three theorems of J.C. Yoccoz" (PDF). Topological methods in modern mathematics (Stony Brook, NY, 1991). Houston, TX: Publish or Perish. pp. 467–511. MR 1215974.. Hubbard cites as his source a 1989 unpublished manuscript of Yoccoz.
 ^ Lei (1990). "Similarity between the Mandelbrot set and Julia Sets". Communications in Mathematical Physics. 134 (3): 587–617. Bibcode:1990CMaPh.134..587L. doi:10.1007/bf02098448. S2CID 122439436.
 ^ J. Milnor (1989). "SelfSimilarity and Hairiness in the Mandelbrot Set". In M. C. Tangora (ed.). Computers in Geometry and Topology. New York: Taylor & Francis. pp. 211–257. ISBN 9780824780319.)
 ^ ^{a} ^{b} Shishikura, Mitsuhiro (1998). "The Hausdorff dimension of the boundary of the Mandelbrot set and Julia sets". Annals of Mathematics. Second Series. 147 (2): 225–267. arXiv:math.DS/9201282. doi:10.2307/121009. JSTOR 121009. MR 1626737. S2CID 14847943..
 ^ Katunin, Andrzej; Fedio, Kamil (2015). "On a Visualization of the Convergence of the Boundary of Generalized Mandelbrot Set to (n1)Sphere" (PDF). Journal of Applied Mathematics and Computational Mechanics. 14 (1): 63–69. doi:10.17512/jamcm.2015.1.06. Retrieved 18 May 2022.
 ^ ^{a} ^{b} "Number Sequences in the Mandelbrot Set". youtube.com. The Mathemagicians' Guild. 4 June 2020. Archived from the original on 30 October 2021.
 ^ Flake, Gary William (1998). The Computational Beauty of Nature. MIT Press. p. 125. ISBN 9780262561273.
 ^ Klebanoff, Aaron D. (2001). "π in the Mandelbrot Set". Fractals. 9 (4): 393–402. doi:10.1142/S0218348X01000828.
 ^ "Fractal Foundation Online Course  Chapter 11  FIBONACCI FRACTALS". fractalfoundation.org. Retrieved 19 July 2023.
 ^ Rudy Rucker's discussion of the CCM: CS.sjsu.edu
 ^ ^{a} ^{b} Barrallo, Javier (2010). "Expanding the Mandelbrot Set into Higher Dimensions" (PDF). BridgesMathArt. Retrieved 15 September 2021.
 ^ Mandelbaum, Ryan F. (2018). "This Trippy Music Video Is Made of 3D Fractals." Retrieved 17 January 2019
 ^ Moeller, Olga de. (2018)."what are Fractals?" Retrieved 17 January 2019.
 ^ "Mandelbrot Set". JoCopeda. Retrieved 15 January 2015.
 ^ "Blue Man Group  Audio Album Reviews, Songs & More". Allmusic.com. Retrieved 4 July 2023.
 ^ Piers Anthony (1992). Fractal Mode. HarperCollins. ISBN 9780246139023.
 ^ Arthur C. Clarke (29 September 2011). The Ghost From The Grand Banks. Orion. ISBN 9780575121799.
 ^ Sheridan, Wade (20 November 2020). "Google honors mathematician Benoit Mandelbrot with new Doodle". United Press International. Retrieved 30 December 2020.
 ^ "Hannah Marks "Amanda Brotzman" customized black leather jacket from Dirk Gently's Holistic Detective Agency". www.icollector.com.
 ^ Trout, Jody (April 2002). "Book Review: 'Flatterland: Like Flatland, Only More So" (PDF). Notices of the AMS. 49 (4): 462–465.
 ^ "The Great Alan Moore Reread: Big Numbers by Tim Callahan". Tor.com. 21 May 2012.
Further reading[edit]
 Milnor, John W. (2006). Dynamics in One Complex Variable. Annals of Mathematics Studies. Vol. 160 (Third ed.). Princeton University Press. ISBN 0691124884.
(First appeared in 1990 as a Stony Brook IMS Preprint, available as arXiV:math.DS/9201272 )  LesmoirGordon, Nigel (2004). The Colours of Infinity: The Beauty, The Power and the Sense of Fractals. Clear Press. ISBN 1904555055.
(includes a DVD featuring Arthur C. Clarke and David Gilmour)  Peitgen, HeinzOtto; Jürgens, Hartmut; Saupe, Dietmar (2004) [1992]. Chaos and Fractals: New Frontiers of Science. New York: Springer. ISBN 0387202293.
External links[edit]
 Chaos and Fractals at Curlie
 Video: Mandelbrot fractal zoom to 6.066 e228
 Relatively simple explanation of the mathematical process, by Dr Holly Krieger, MIT
 Mandelbrot Viewer: Browser based Mandelbrot set renderer including a gallery with examples.
 Various algorithms for calculating the Mandelbrot set (on Rosetta Code)
 Fractal calculator written in Lua by Deyan Dobromiroiv, Sofia, Bulgaria