Definitions
Contents
AddressEdit
InternalEdit
Internal addresses describe the combinatorial structure of the Mandelbrot set.^{[1]}
Internal address :
 is not constant within hyperbolic component. Example : internal address of 1 is 1>2 and internal address of 0.9999 is 1^{[2]}
 of hyperbolic component is defined as a internal address of it's center
angledEdit
Angled internal address is an extension of internal address
AngleEdit
Types of angleEdit
external angle  internal angle  plain angle  

parameter plane  
dynamic plane 
where :
 is a multiplier map
 is a Boettcher function
externalEdit
The external angle is a angle of point of set's exterior. It is the same on all points on the external ray
internalEdit
The internal angle is an angle of point of component's interior
 it is a rational number and proper fraction measured in turns
 it is the same for all point on the internal ray
 in a contact point ( root point ) it agrees with the rotation number
 root point has internal angle 0
plainEdit
The plain angle is an agle of complex point = it's argument ^{[3]}
UnitsEdit
 turns
 degrees
 radians
Number typesEdit
Angle ( for example external angle in turns ) can be used in different number types
Examples :
the external arguments of the rays landing at z = −0.15255 + 1.03294i are :^{[4]}
where :
CoordinateEdit
 Fatou coordinate for every repelling and attracting petal ( linearization of function near parabolic fixed point )
 Boettcher
 Koenigs
CurvesEdit
Types:
 topology: closed versus open
 other properities:
 invariant
 critical
closedEdit
Closed curves are curves whose ends are joined. Closed curves do not have end points.
 Simple Closed Curve : A connected curve that does not cross itself and ends at the same point where it begins. It divides the plane into exactly two regions ( Jordan curve theorem ). Examples of simple closed curves are ellipse, circle and polygons.^{[5]}
 complex Closed Curve ( not simple = nonsimple ) It divides the plane into more than two regions. Example : Lemniscates.
"nonselfintersecting continuous closed curve in plane" = "image of a continuous injective function from the circle to the plane"
CircleEdit
Inner circleEdit
Unit circleEdit
Unit circle is a boundary of unit disk^{[6]}
where coordinates of point of unit circle in exponential form are :
Critical curvesEdit
Diagrams of critical polynomials are called critical curves.^{[7]}
These curves create skeleton of bifurcation diagram.^{[8]} (the dark lines^{[9]})
Escape linesEdit
"If the escape radius is equal to 2 the contour lines have a contact point (c= 2) and cannot be considered as equipotential lines" ^{[10]}
InvariantEdit
curve is invariant for the map f ( evolution function ) if images of every point from the curve stay on that curve
IsocurvesEdit
Equipotential linesEdit
Equipotential lines = Isocurves of complex potential
"If the escape radius is greater than 2 the contour lines are equipotential lines" ^{[11]}
Jordan curveEdit
Jordan curve = a simple closed curve that divides the plane into an "interior" region bounded by the curve and an "exterior" region containing all of the nearby and far away exterior points^{[12]}
LaminationEdit
Lamination of the unit disk is a closed collection of chords in the unit disc, which can intersect only in an endpoint of each on the boundary circle^{[13]}^{[14]}
It is a model of Mandelbrot or Julia set.
A lamination, L, is a union of leaves and the unit circle which satisfies :^{[15]}
 leaves do not cross (although they may share endpoints) and
 L is a closed set.
LeafEdit
Chords = leaves = arcs
A leaf on the unit disc is a path connecting two points on the unit circle. ^{[16]}
Open curveEdit
Curve which is not closed. Examples : line, ray.
RayEdit
Rays are :
 invariant curves
 dynamic or parameter
 external or internal
External rayEdit
Internal rayEdit
Internal rays are :
 dynamic ( on dynamic plane , inside filled Julia set )
 parameter ( on parameter plane , inside Mandelbrot set )
SpiderEdit
A spider S is a collection of disjoint simple curves called legs ^{[17]}( extended rays = external + internal ray) in the complex plane connecting each of the postcritical points to infnity ^{[18]}
See :
VeinEdit
"A vein in the Mandelbrot set is a continuous, injective arc inside in the Mandelbrot set"
"The principal vein is the vein joining to the main cardioid" (Entropy, dimension and combinatorial moduli for onedimensional dynamical systems. A dissertation by Giulio Tiozzo )
DiscretizationEdit
discretization^{[19]} and its reverse ^{[20]}
DynamicsEdit
 symbolic^{[21]}
 complex
 Arithmetic
 combinatorial
equationEdit
differentialEdit
differential equations
 exact analytic solutions.
 approximated solution
 use perturbation theory to approximate the solutions
FunctionEdit
DerivativeEdit
Derivative of Iterated function (map)
Derivative with respect to cEdit
On parameter plane :
 is a variable
 is constant
This derivative can be found by iteration starting with
and then
This can be verified by using the chain rule for the derivative.
 Maxima CAS function :
dcfn(p, z, c) := if p=0 then 1 else 2*fn(p1,z,c)*dcfn(p1, z, c)+1;
Example values :
Derivative with respect to zEdit
is first derivative with respect to c.
This derivative can be found by iteration starting with
and then :
GermEdit
Germ ^{[22]} of the function f in the neighborhood of point z is a set of the functions g which are indistinguishable in that neighborhood
See :
mapEdit
 differences between map and the function ^{[23]}
 Iterated function = map^{[24]}
 an evolution function^{[25]} of the discrete nonlinear dynamical system^{[26]}
is called map :
typesEdit
 The map f is hyperbolic if every critical orbit converges to a periodic orbit.^{[27]}
Complex quadratic mapEdit
FormsEdit
c form : Edit
quadratic map^{[28]}
 math notation :
 Maxima CAS function :
f(z,c):=z*z+c;
(%i1) z:zx+zy*%i; (%o1) %i*zy+zx (%i2) c:cx+cy*%i; (%o2) %i*cy+cx (%i3) f:z^2+c; (%o3) (%i*zy+zx)^2+%i*cy+cx (%i4) realpart(f); (%o4) zy^2+zx^2+cx (%i5) imagpart(f); (%o5) 2*zx*zy+cy
Iterated quadratic map
 math notation
...
or with subscripts :
 Maxima CAS function :
fn(p, z, c) := if p=0 then z elseif p=1 then f(z,c) else f(fn(p1, z, c),c);
zp:fn(p, z, c);
lambda form : Edit
More description Maxima CAS code ( here m not lambda is used ) :
(%i2) z:zx+zy*%i; (%o2) %i*zy+zx (%i3) m:mx+my*%i; (%o3) %i*my+mx (%i4) f:m*z+z^2; (%o4) (%i*zy+zx)^2+(%i*my+mx)*(%i*zy+zx) (%i5) realpart(f); (%o5) zy^2my*zy+zx^2+mx*zx (%i6) imagpart(f); (%o6) 2*zx*zy+mx*zy+my*zx
Switching between formsEdit
Start from :
 internal angle
 internal radius r
Multiplier of fixed point :
When one wants change from lambda to c :^{[29]}
or from c to lambda :
Example values :
r  c  fixed point alfa  fixed point  

1/1  1.0  0.25  0.5  1.0  0 
1/2  1.0  0.75  0.5  1.0  0 
1/3  1.0  0.64951905283833*i0.125  0.43301270189222*i0.25  0.86602540378444*i0.5  0 
1/4  1.0  0.5*i+0.25  0.5*i  i  0 
1/5  1.0  0.32858194507446*i+0.35676274578121  0.47552825814758*i+0.15450849718747  0.95105651629515*i+0.30901699437495  0 
1/6  1.0  0.21650635094611*i+0.375  0.43301270189222*i+0.25  0.86602540378444*i+0.5  0 
1/7  1.0  0.14718376318856*i+0.36737513441845  0.39091574123401*i+0.31174490092937  0.78183148246803*i+0.62348980185873  0 
1/8  1.0  0.10355339059327*i+0.35355339059327  0.35355339059327*i+0.35355339059327  0.70710678118655*i+0.70710678118655  0 
1/9  1.0  0.075191866590218*i+0.33961017714276  0.32139380484327*i+0.38302222155949  0.64278760968654*i+0.76604444311898  0 
1/10  1.0  0.056128497072448*i+0.32725424859374  0.29389262614624*i+0.40450849718747  0.58778525229247*i+0.80901699437495 
One can easily compute parameter c as a point c inside main cardioid of Mandelbrot set :
of period 1 hyperbolic component ( main cardioid) for given internal angle ( rotation number) t using this c / cpp code by Wolf Jung^{[30]}
double InternalAngleInTurns;
double InternalRadius;
double t = InternalAngleInTurns *2*M_PI; // from turns to radians
double R2 = InternalRadius * InternalRadius;
double Cx, Cy; /* C = Cx+Cy*i */
// main cardioid
Cx = (cos(t)*InternalRadius)/2(cos(2*t)*R2)/4;
Cy = (sin(t)*InternalRadius)/2(sin(2*t)*R2)/4;
or this Maxima CAS code :
/* conformal map from circle to cardioid ( boundary of period 1 component of Mandelbrot set */ F(w):=w/2w*w/4; /* circle D={w:abs(w)=1 } where w=l(t,r) t is angle in turns ; 1 turn = 360 degree = 2*Pi radians r is a radius */ ToCircle(t,r):=r*%e^(%i*t*2*%pi); GiveC(angle,radius):= ( [w], /* point of unit circle w:l(internalAngle,internalRadius); */ w:ToCircle(angle,radius), /* point of circle */ float(rectform(F(w))) /* point on boundary of period 1 component of Mandelbrot set */ )$ compile(all)$ /*  global constants & var */ Numerator :1; DenominatorMax :10; InternalRadius:1; /*  main  */ for Denominator:1 thru DenominatorMax step 1 do ( InternalAngle: Numerator/Denominator, c: GiveC(InternalAngle,InternalRadius), display(Denominator), display(c), /* compute fixed point */ alfa:float(rectform((1sqrt(14*c))/2)), /* alfa fixed point */ display(alfa) )$
Circle mapEdit
Circle map ^{[31]}
 irrational rotation^{[32]}
Doubling mapEdit
definition ^{[33]}
C function ( using GMP library) :
// rop = (2*op ) mod 1
void mpq_doubling(mpq_t rop, const mpq_t op)
{
mpz_t n; // numerator
mpz_t d; // denominator
mpz_inits(n, d, NULL);
//
mpq_get_num (n, op); //
mpq_get_den (d, op);
// n = (n * 2 ) % d
mpz_mul_ui(n, n, 2);
mpz_mod( n, n, d);
// output
mpq_set_num(rop, n);
mpq_set_den(rop, d);
mpz_clears(n, d, NULL);
}
 Maxima CAS function using numerator and denominator as an input
doubling_map(n,d):=mod(2*n,d)/d $
or using rational number as an input
DoublingMap(r):= block([d,n], n:ratnumer(r), d:ratdenom(r), mod(2*n,d)/d)$
 Common Lisp function
(defun doublingmap (ratioangle)
" period doubling map = The dyadic transformation (also known as the dyadic map,
bit shift map, 2x mod 1 map, Bernoulli map, doubling map or sawtooth map "
(let* ((n (numerator ratioangle))
(d (denominator ratioangle)))
(setq n (mod (* n 2) d)) ; (2 * n) modulo d
(/ n d))) ; result = n/d
 Haskell function^{[34]}
 by Claude HeilandAllen
 type Q = Rational
double :: Q > Q
double p
 q >= 1 = q  1
 otherwise = q
where q = 2 * p
 C++
// mndcombi.cpp by Wolf Jung (C) 2010.
// http://mndynamics.com/indexp.html
// n is a numerator
// d is a denominator
// f = n/d is a rational fraction ( angle in turns )
// twice is doubling map = (2*f) mod 1
// n and d are changed ( Arguments passed to function by reference)
void twice(unsigned long long int &n, unsigned long long int &d)
{ if (n >= d) return;
if (!(d & 1)) { d >>= 1; if (n >= d) n = d; return; }
unsigned long long int large = 1LL;
large <<= 63; //avoid overflow:
if (n < large) { n <<= 1; if (n >= d) n = d; return; }
n = large;
n <<= 1;
large = (d  large);
n += large;
}
Inverse function of doubling mapEdit
Every angle α ∈ R/Z measured in turns has :
 one image = 2α mod 1 under doubling map
 "two preimages under the doubling map: α/2 and (α + 1)/2." ^{[35]}. Inverse of doubling map is multivalued function.
In Maxima CAS :
InvDoublingMap(r):= [r/2, (r+1)/2];
Note that difference between these 2 preimages
is half a turn = 180 degrees = Pi radians.
First return mapEdit
definition ^{[36]}
"In contrast to a phase portrait, the return map is a discrete description of the underlying dynamics. .... A return map (plot) is generated by plotting one return value of the time series against the previous one "^{[37]}
"If x is a periodic point of period p for f and U is a neighborhood of x, the composition maps U to another neighborhood V of x. This locally defined map is the return map for x." ( W P Thurston : On the geometry and dynamics of Iterated rational maps)
"The first return map S → S is the map defined by sending each x0 ∈ S to the point of S where the orbit of x0 under the system first returns to S." ^{[38]}
"way to obtain a discrete time system from a continuous time system, called the method of Poincar´e sections Poincar´e sections take us from : continuous time dynamical systems on (n + 1)dimensional spaces to discrete time dynamical systems on ndimensional spaces"^{[39]}
Multiplier mapEdit
Multiplier map gives an explicit uniformization of hyperbolic component by the unit disk :
Multiplier map is a conformal isomorphism.^{[40]}
Rotation mapEdit
typesEdit
PolynomialEdit
CriticalEdit
Critical polynomial :
so
These polynomials are used for finding :
 centers of period n Mandelbrot set components. Centers are roots of nth critical polynomials ( points where critical curve Qn croses x axis )
 Misiurewicz points
postcritically finiteEdit
a postcritically finite polynomial = all critical points have finite orbit
ResurgentEdit
"resurgent functions display at each of their singular points a behaviour closely related to their behaviour at the origin. Loosely speaking, these functions resurrect, or surge up  in a slightly different guise, as it were  at their singularities"
J. Écalle, 1980^{[41]}
glitchesEdit
glitches = Incorrect parts of renders^{[42]} using perturbation techique
InvariantsEdit
sth is invariant with respect to the transformation = non modified, steady
Topological methods for the analysis of dynamical systems
Invariants type
 metric invariants
 dynamical invariants,
 topological invariants.
dynamicalEdit
Dynamical invariants = invariants of the dynamical system
 periodic points
 fixed point
 invariant curve
 periodic ray
 external
 internal
 periodic ray
Dynamical Invariants Derived from Recurrence Plots^{[43]}
IntervalEdit
a partition of an interval into subintervals
 Markov paritition^{[44]}
IterationEdit
ItineraryEdit
S(x) is an itinerary of point x under the map f is a rightinfinite sequence of zeros and ones ^{[45]}
where
Examples :
For a unimodal map with a critical point and invariant interval I :
one can split interval into 2 subintervals :
then compute s according to it's relation with critical point :
Itinerary can be converted^{[46]} to point
MagnitudeEdit
magnitude of the point ( complex number in 2D case) = it's distance from the origin
MultiplierEdit
Multiplier of periodic zpoint : ^{[47]}
Math notation :
Maxima CAS function for computing multiplier of periodic cycle :
m(p):=diff(fn(p,z,c),z,1);
where p is a period. It takes period as an input, not z point.
period  

1  
2  
3 
It is used to :
 compute stability index of periodic orbit ( periodic point) = ( where r is a n internal radius
 multiplier map
NumberEdit
Rotation numberEdit
The rotation number^{[48]}^{[49]}^{[50]} of the disk ( component) attached to the main cardioid of the Mandelbrot set is a proper, positive rational number p/q in lowest terms where :
 q is a period of attached disk ( child period ) = the period of the attractive cycles of the Julia sets in the attached disk
 p descibes fc action on the cycle : fc turns clockwise around z0 jumping, in each iteration, p points of the cycle ^{[51]}
Features :
 in a contact point ( root point ) it agrees with the internal angle
 the rotation numbers are ordered clockwise along the boundary of the componant
 " For parameters c in the p/qlimb, the filled Julia set Kc has q components at the fixed point αc . These are permuted cyclically by the quadratic polynomial fc(z), going p steps counterclockwise " Wolf Jung
Winding numberEdit
def^{[52]}
OrbitEdit
Orbit is a sequence of points = trajectory
BackwardEdit
CriticalEdit
Forward orbit^{[53]} of a critical point^{[54]}^{[55]} is called a critical orbit. Critical orbits are very important because every attracting periodic orbit^{[56]} attracts a critical point, so studying the critical orbits helps us understand the dynamics in the Fatou set.^{[57]}^{[58]} ^{[59]}
This orbit falls into an attracting periodic cycle.
Code :
"https://github.com/conanite/rainbow/blob/master/src/arc/rainbow/spiral.arc
This software is copyright (c) Conan Dalton 2008. Permission to use it is granted under the Perl Foundations's Artistic License 2.0.
This software includes software that is copyright (c) Paul Graham and Robert Morris, distributed under the Perl Foundations's Artistic License 2.0.
This software uses javacc which is copyright (c) its authors
"
(def plot (plt c)
(with (z 0+0i
n 0
repeats 0)
(while (and (small z) (< n 10000) (< repeats 1000))
(assign n (+ n 1)
z (+ c (* z z))
repeats (if (apply plt (complexparts z))
(+ repeats 1)
0)))))
Here are images:
 images of critical orbitsat commons
 by Mike Croucher^{[60]}
 Chris King ^{[61]}
 list : critical orbits
 images by Conan written in Rainbow
ForwardEdit
Homoclinic / heteroclinicEdit
InverseEdit
Inverse = Backward
ParameterEdit
Parameter
 point of parameter plane : " is renormalizable if restriction of some of its iterate gives a polinomiallike map of the same or lower degree. " ^{[62]}
 parameter of the function
PeriodEdit
The smallest positive integer value p for which this equality
holds is the period^{[63]} of the orbit.^{[64]}
is a point of periodic orbit ( limit cycle ) .
More is here
PerturbationEdit
 Perturbation technque for fast rendering the deep zoom images of the Mandelbrot set^{[65]}
 perturbation of parabolic point ^{[66]}
 use perturbation theory to approximate the solutions of the differential equations
PlaneEdit
Planes ^{[67]}
Douady’s principle : “sow in dynamical plane and reap in parameter space”.
Dynamic planeEdit
 zplane for fc(z)= z^2 + c
 zplane for fm(z)= z^2 + m*z
Parameter planeEdit
See :^{[68]}
Types of the parameter plane :
 cplane ( standard plane )
 exponential plane ( map) ^{[69]}^{[70]}
 flatten' the cardiod ( unroll ) ^{[71]}^{[72]} = "A region along the cardioid is continuously blown up and stretched out, so that the respective segment of the cardioid becomes a line segment. .." ( Figure 4.22 on pages 204205 of The Science Of Fractal Images)^{[73]}
 transformations ^{[74]}
PointsEdit
BandmergingEdit
the bandmerging points are Misiurewicz points^{[75]}
BiaccessibleEdit
If there exist two distinct external rays landing at point we say that it is a biaccessible point. ^{[76]}
CenterEdit
Nucleus or center of hyperbolic componentEdit
A center of a hyperbolic component H is a parameter ( or point of parameter plane ) such that the corresponding periodic orbit has multiplier= 0." ^{[77]}
Synonyms :
 Nucleus of a MuAtom ^{[78]}
Center of Siegel DiscEdit
Center of Siegel disc is a irrationally indifferent periodic point.
Mane's theorem :
"... appart from its center, a Siegel disk cannot contain any periodic point, critical point, nor any iterated preimage of a critical or periodic point. On the other hand it can contain an iterated image of a critical point." ^{[79]}
CriticalEdit
A critical point^{[80]} of is a point in the dynamical plane such that the derivative vanishes:
Since
implies
we see that the only (finite) critical point of is the point .
is an initial point for Mandelbrot set iteration.^{[81]}
CutEdit
Cut point k of set S is a point for which set Sk is dissconected ( consist of 2 or more sets).^{[82]} This name is used in a topology.
Examples :
 root points of Mandelbrot set
 Misiurewicz points of boundary of Mandelbrot set
 cut points of Julia sets ( in case of Siegel disc critical point is a cut point )
These points are landing points of 2 or more external rays.
Point which is a landing point of 2 external rays is called biaccesible
Cut ray is a ray which converges to landing point of another ray. ^{[83]} Cut rays can be used to construct puzzles.
Cut angle is an angle of cut ray.
fixedEdit
Periodic point when period = 1
FeigenbaumEdit
The Feigenbaum Point^{[84]} is a :
 point c of parameter plane
 is the limit of the period doubling cascade of bifurcations
 an infinitely renormalizable parameter of bounded type
 boundary point between chaotic ( 2 < c < MF ) and periodic region ( MF< c < 1/4)^{[85]}
Generalized Feigenbaum points are :
 the limit of the periodq cascade of bifurcations
 landing points of parameter ray or rays with irrational angles
Examples :
 .1528+1.0397i)
The Mandelbrot set is conjectured to be self similar around generalized Feigenbaum points^{[86]} when the magnification increases by 4.6692 (the Feigenbaum Constant) and period is doubled each time^{[87]}

n Period = 2^n Bifurcation parameter = c_{n} Ratio 1 2 0.75 N/A 2 4 1.25 N/A 3 8 1.3680989 4.2337 4 16 1.3940462 4.5515 5 32 1.3996312 4.6458 6 64 1.4008287 4.6639 7 128 1.4010853 4.6682 8 256 1.4011402 4.6689 9 512 1.401151982029 10 1024 1.401154502237 infinity 1.4011551890 ...
Bifurcation parameter is a root point of period = 2^n component. This series converges to the Feigenbaum point c = −1.401155
The ratio in the last column converges to the first Feigenbaum constant.
" a "Feigenbaum point" (an infinitely renormalizable parameter of bounded type, such as the famous Feigenbaum value which is the limit of the period2 cascade of bifurcations), then Milnor's hairiness conjecture, proved by Lyubich, states that rescalings of the Mandelbrot set converge to the entire complex plane. So there is certainly a lot of thickness near such a point, although again this may not be what you are looking for. It may also prove computationally intensive to produce accurate pictures near such points, because the usual algorithms will end up doing the maximum number of iterations for almost all points in the picture." Lasse RempeGillen^{[88]}
infinityEdit
The point at infinity ^{[89]}" is a superattracting fixed point, but more importantly its immediate basin of attraction  that is, the component of the basin containing the fixed point itself  is completely invariant (invariant under forward and backwards iteration). This is the case for all polynomials (of degree at least two), and is one of the reasons that studying polynomials is easier than studying general rational maps (where e.g. the Julia set  where the dynamics is chaotic  may in fact be the whole Riemann sphere). The basin of infinity supports foliations into "external rays" and "equipotentials", and this allows one to study the Julia set. This idea was introduced by Douady and Hubbard, and is the basis of the famous "Yoccoz puzzle"." Lasse RempeGillen^{[90]}
MisiurewiczEdit
Misiurewicz point^{[91]} = " parameters where the critical orbit is preperiodic.
Examples are:
 bandmerging points of chaotic bands (the separator of the chaotic bands Bi−1 and Bi )^{[92]}
 the branch points
 tips in the Mandelbrot set ( tips of the midgets ) ^{[93]}
Characteristic Misiurewicz pointof the chaotic band of the Mandelbrot set is :^{[94]}
 the most prominent and visible Misiurewicz point of a chaotic band
 have the same period as the band
 have the same period as the gene of the band
MyrbergFeigenbaumEdit
MF = the MyrbergFeigenbaum point is the different name for the Feigenbaum Point.
Parabolic pointEdit
parabolic points : this occurs when two singular points coallesce in a double singular point (parabolic point)^{[95]}
PeriodicEdit
Point z has period p under f if :
PinchingEdit
"Pinching points are found as the common landing points of external rays, with exactly one ray landing between two consecutive branches. They are used to cut M or K into welldefined components, and to build topological models for these sets in a combinatorial way. " ( definition from Wolf Jung program Mandel )
See for examples :
 period 2 = Mandel, demo 2 page 3.
 period 3 = Mandel, demo 2 page 5 ^{[96]}
postcriticalEdit
A postcritical point is a point
where is a critical point. ^{[97]}
precriticalEdit
precritical points, i.e., the preimages of 0
rootEdit
The root point :
 has a rotational number 0
 it is a biaccesible point ( landing point of 2 external rays )
singularEdit
the singular points of a dynamical system
In complex analysis there are four classes of singularities:
 Isolated singularities: Suppose the function f is not defined at a, although it does have values defined on U \ {a}.
 The point a is a removable singularity of f if there exists a holomorphic function g defined on all of U such that f(z) = g(z) for all z in U \ {a}. The function g is a continuous replacement for the function f.
 The point a is a pole or nonessential singularity of f if there exists a holomorphic function g defined on U with g(a) nonzero, and a natural number n such that f(z) = g(z) / (z − a)^{n} for all z in U \ {a}. The least such number n is called the order of the pole. The derivative at a nonessential singularity itself has a nonessential singularity, with n increased by 1 (except if n is 0 so that the singularity is removable).
 The point a is an essential singularity of f if it is neither a removable singularity nor a pole. The point a is an essential singularity if and only if the Laurent series has infinitely many powers of negative degree.
 Branch points are generally the result of a multivalued function, such as or being defined within a certain limited domain so that the function can be made singlevalued within the domain. The cut is a line or curve excluded from the domain to introduce a technical separation between discontinuous values of the function. When the cut is genuinely required, the function will have distinctly different values on each side of the branch cut. The shape of the branch cut is a matter of choice, however, it must connect two different branch points (like and for ) which are fixed in place.
PortraitEdit
orbit portraitEdit
typesEdit
There are two types of orbit portraits: primitive and satellite. ^{[98]}If is the valence of an orbit portrait and is the recurrent ray period, then these two types may be characterized as follows:
 Primitive orbit portraits have and . Every ray in the portrait is mapped to itself by . Each is a pair of angles, each in a distinct orbit of the doubling map. In this case, is the base point of a baby Mandelbrot set in parameter space.
 Satellite ( nonprimitive ) orbit portraits have . In this case, all of the angles make up a single orbit under the doubling map. Additionally, is the base point of a parabolic bifurcation in parameter space.
Processes and phenomenonaEdit
Contraction and dilatationEdit
 the contraction z → z/2
 the dilatation z → 2z.
Implosion and explosionEdit
Implosion is :
 the process of sudden change of quality fuatures of the object, like collapsing (or being squeezed in)
 the opposite of explosion
Example : parabolic implosion in complex dynamics, when filled Julia for complex quadratic polynomial set looses all its interior ( when c goes from 0 along internal ray 0 thru parabolic point c=1/4 and along extrnal ray 0 = when c goes from interior , crosses the bounday to the exterior of Mandelbrot set)^{[99]}
Explosion is a :
 is a sudden change of quality fuatures of the object in an extreme manner,
 the opposite of implosion
Example : in exponential dynamics when λ> 1/e , the Julia set of is the entire plane.^{[100]}
TuningEdit
RadiusEdit
Conformal radiusEdit
Conformal radius of Siegel Disk ^{[102]}^{[103]}
Escape radius ( ER)Edit
Escape radius ( ER ) or bailout value is a radius of circle target set used in bailout test
Minimal Escape Radius should be grater or equal to 2 :
Better estimation is :^{[104]}^{[105]}
Inner radiusEdit
Inner radius of Siegel Disc
 radius of inner circle, where inner circle with center at fixed point is the biggest circle inside Siegel Disc.
 minimal distance between center of Siel Disc and critical orbit
Internal radiusEdit
Internal radius is a:
 absolute value of multiplier
SequencesEdit
A sequence is an ordered list of objects (or events).^{[106]}
A series is the sum of the terms of a sequence of numbers.^{[107]} Some times these names are not used as in above definitions.
OrbitEdit
Orbit can be:
SetEdit
ContinuumEdit
definition^{[108]}
ComponentEdit
Components of parameter planeEdit
muatom , ball, bud, bulb, decoration, lake and lakelet.^{[109]}
IslandsEdit
Names :
 mini Mandelbrot set
 'baby'Mandelbrot set
 island mumolecules = embedded copy of the Mandelbrot Set^{[110]}
 Bug
 Island
 Mandelbrotie
 Midget
List of islands :
 http://mrob.com/pub/mudata/largestislands.txt
 http://mrob.com/pub/muency/largestislands.html
 http://www.math.cornell.edu/~rperez/Documents/maximals.pdf
 http://fraktal.republika.pl/mset_external_ray_mini.html
Primary and satelliteEdit
"Hyperbolic components come in two kinds, primitive and satellite, depending on the local properties of their roots." ^{[111]}
Child (Descendant ) and the parentEdit
def ^{[112]}
Hyperbolic component of Mandelbrot setEdit
Domain is an open connected subset of a complex plane.
"A hyperbolic component H of Mandelbrot set is a maximal domain (of parameter plane) on which has an attracting periodic orbit.
A center of a H is a parameter ( or point of parameter plane ) such that the corresponding periodic orbit has multiplier= 0." ^{[113]}
A hyperbolic component is narrow if it contains no component of equal or lesser period in its wake ^{[114]}
features of hyperbolic component
 period
 islandhood ( shape = cardiod or circle )
 angled internal address
 lower and upper external angle of rays landing on it's root
 center (
 root
 orientation
 size
LimbEdit
p/q limb is a part of Mandelbrot set contained inside p/q wake
WakeEdit
Wake is the region of parameter plane enclosed by two external rays landing on the same root point on the boundary of main cardioid ( period 1 hyperbolic component).
Angles of the external rays that land on the root point one can find by :
 Combinatorial algorithm = Devaney's method
 book program by Claude HeilandAllen
 wake function from program Mandel by Wolf Jung
Components of dynamical planeEdit
In case of Siegel disc critical orbit is a boundary of component containing Siegel Disc.
DomainEdit
Domain in mathematical analysis it is an open connected set
Jordan domainEdit
"A Jordan domain^{[115]} J is the the homeomorphic image of a closed disk in E2. The image of the boundary circle is a Jordan curve, which by the Jordan Curve Theorem separates the plane into two open domains, one bounded, the other not, such that the curve is the boundary of each." ^{[116]}
FlowerEdit
Planar setEdit
a nonseparating planar set is a set whose complement in the plane is connected.^{[117]}
SepalEdit
Target setEdit
Elliptic caseEdit
For the elliptic dynamics, when there is a Siegel disc, the target set is an inner circle
Hyperbolic caseEdit
Infinity is allways hyperbolic attractor for forward iteration of polynomials. Target set here is an exterior of any shape containing all point of Julia set ( and it's interior). There are also other hyperbolic attractors.
In case of forward iteration target set is an arbitrary set on dynamical plane containing infinity and not containing points of filled Julia set.
For escape time algorithms target set determines the shape of level sets and curves. It does not do it for other methods.
Exterior of circleEdit
This is typical target set. It is exterior of circle with center at origin and radius =ER :
Radius is named escape radius ( ER ) or bailout value.
Circle of radius=ER centered at the origin is :
Exterior of squareEdit
Here target set is exterior of square of side length centered at origin
Parabolic case : petalEdit
In the parabolic case target set shoul be iside petal
TrapEdit
Trap is an another name of the target set. It is a set which captures any orbit tending to point inside the trap ( fixed / periodic point ).
TestEdit
Bailout test or escaping testEdit
It is used to check if point z on dynamical plane is escaping to infinity or not.^{[118]} It allows to find 2 sets :
 escaping points ( it should be also the whole basing of attraction to infinity)^{[119]}
 not escaping points ( it should be the complement of basing of attraction to infinity)
In practice for given IterationMax and Escape Radius :
 some pixels from set of not escaping points may contain points that escape after more iterations then IterationMax ( increase IterMax )
 some pixels from escaping set may contain points from thin filaments not choosed by maping from integer to world ( use DEM )
If is in the target set then is escaping to infinity ( bailouts ) after n forward iterations ( steps).^{[120]}
The output of test can be :
 boolean ( yes/no)
 integer : integer number (value of the last iteration)
Attraction testEdit
TreeEdit
Hubbard treeEdit
"Hubbard trees are finite planar trees, equipped with selfmaps, which classify postcritically finite polynomials as holomorphic dynamical systems on the complex plane." ^{[121]}
ReferencesEdit
 ↑ Rational Maps with Clustering and the Mating of Polynomials by Thomas Joseph Sharland
 ↑ Topics from OneDimensional Dynamics by Karen M. Brucks,Henk Bruin. page 265 exercise 14.2.12
 ↑ argument of complex number
 ↑ A Method to Solve the Limitations in Drawing External Rays of the Mandelbrot Set M. Romera, G. Pastor, A. B. Orue, A. Martin, M.F. Danca, and F. Montoya
 ↑ What is a Curve ?
 ↑ Unit circle in wikipedia
 ↑ The Road to Chaos is Filled with Polynomial Curves by Richard D. Neidinger and R. John Annen III. American Mathematical Monthly, Vol. 103, No. 8, October 1996, pp. 640653
 ↑ Hao, Bailin (1989). Elementary Symbolic Dynamics and Chaos in Dissipative Systems. World Scientific. ISBN 9971506823. http://power.itp.ac.cn/~hao/.
 ↑ M. Romera, G. Pastor and F. Montoya, "Misiurewicz points in onedimensional quadratic maps", Physica A, 232 (1996), 517535. Preprint
 ↑ Escape lines versus equipotential lines in the Mnadelbrot set by M. Romera, Pastor G , D. de la Guía, Montoya
 ↑ Escape lines versus equipotential lines in the Mnadelbrot set by M. Romera, Pastor G , D. de la Guía, Montoya
 ↑ wikipedia : Jordan curve theorem
 ↑ Modeling Julia Sets with Laminations: An Alternative Definition by Debra Mimbs
 ↑ Laminations of the unit disk with irrational rotation gaps by John C. Mayer
 ↑ Rational maps represented by both rabbit and aeroplane matings Thesis submitted in accordance with the requirements of the University of Liverpool for the degree of Doctor in Philosophy by Freddie R. Exall July 2010
 ↑ Rational maps represented by both rabbit and aeroplane matings Thesis submitted in accordance with the requirements of the University of Liverpool for the degree of Doctor in Philosophy by Freddie R. Exall July 2010
 ↑ Iterated Monodromy Groups of Quadratic Polynomials, I Laurent Bartholdi, Volodymyr V. Nekrashevych
 ↑ GROWTH OF GROUPS DEFINED BY AUTOMATA : ASHLEY S. DOUGHERTY, LYDIA R. KINDELIN, AARON M. REAVES, ANDREW J. WALKER, AND NATHANIEL F. ZAKAHI
 ↑ wikipedia : discretization
 ↑ mathinsight : from_discrete_to_continuous_dynamical_systems
 ↑ Symbolic Dynamics of Quadratic Polynomials by H. Bruin and D. Schleicher
 ↑ Germ in wikipedia
 ↑ math.stackexchange question : isthereanydifferencebetweenmappingandfunction
 ↑ Iterated function (map) in wikipedia
 ↑ evolution function
 ↑ the discrete nonlinear dynamical system
 ↑ Hyperbolic Components by John Milnor
 ↑ Complex quadratic map in wikipedia
 ↑ Michael Yampolsky, Saeed Zakeri : Mating Siegel quadratic polynomials.
 ↑ Mandel: software for real and complex dynamics by Wolf Jung
 ↑ threecoolfactsaboutrotationsofthecircle by David Richeson
 ↑ irrationalrotationsofthecircleandbenfordslaw by David Richeson
 ↑ wikipedia : Dyadic transformation
 ↑ lavaurs' algorithm in Haskell with SVG output by Claude HeilandAllen
 ↑ SYMBOLIC DYNAMICS AND SELFSIMILAR GROUPS by VOLODYMYR NEKRASHEVYCH
 ↑ Poincaré map
 ↑ General principles of chaotic dynamics by P.B. Persson , C.D. Wagner
 ↑ Continuous time and discrete time dynamical systems by Shaun Bullett
 ↑ Continuous time and discrete time dynamical systems by Shaun Bullett
 ↑ Conformal Geometry and Dynamics of Quadratic Polynomials Mikhail Lyubich
 ↑ A Beginners’ Guide to Resurgence and Transseries in Quantum Theories Gerald Dunne
 ↑ dinkydauset at deviantar :PerturbationfortheMandelbrotset450766847
 ↑ N. Marwan, M. C. Romano, M. Thiel, J. Kurths: Recurrence Plots for the Analysis of Complex Systems, Physics Reports, 438(56), 237329, 2007.
 ↑ math.stackexchange question : definitionofmarkovpartition
 ↑ Structure of Inverse Limit Spaces of Tent Maps with Nonrecurrent Critical Points by Brian Raines and Sonja Stimac
 ↑ Bifurcation structures in maps of Henon type by Kai T Hansen and Predrag Cvitanovic
 ↑ Multiplier at wikipedia
 ↑ wikipedia : Rotation number
 ↑ scholarpedia : Rotation_theory
 ↑ The Fractal Geometry of the Mandelbrot Set II. How to Count and How to Add Robert L. Devaney
 ↑ Complex systems simulation Curso 20122013 by Antonio Giraldo and María Asunción Sastre
 ↑ https://plus.maths.org/content/windingnumberstopographyandtopologyii
 ↑ wikipedia : orbit (dynamics)
 ↑ Wikipedia : Complex quadratic polynomial  Critical point
 ↑ MandelOrbits  A visual realtime trace of Mandelbrot iterations by Ivan Freyman
 ↑ wikipedia : Periodic points of complex quadratic mappings
 ↑ M. Romera, G. Pastor, and F. Montoya : Multifurcations in nonhyperbolic fixed points of the Mandelbrot map. Fractalia 6, No. 21, 1012 (1997)
 ↑ Burns A M : Plotting the Escape: An Animation of Parabolic Bifurcations in the Mandelbrot Set. Mathematics Magazine, Vol. 75, No. 2 (Apr., 2002), pp. 104116
 ↑ Khan Academy : Mandelbrot Spirals 2
 ↑ Complex Power Towers (Or ‘mucking around with Mathematica’) by Mike Croucher
 ↑ /DarkHeart by Chris King
 ↑ Ouadraticlike maps and Renormalization by Nuria Fagella
 ↑ Peiod From the Mandelbrot Set Glossary and Encyclopedia, by Robert Munafo, (c) 19872015.
 ↑ scholarpedia : Periodic Orbit for a Map
 ↑ Perturbation for the Mandelbrot set by DinkydauSet, Apr 28, 2014, 3:46:13 PM
 ↑ PARABOLIC IMPLOSION A MINICOURSE ARNAUD CHERITAT
 ↑ wikipedia : Complex_quadratic_polynomial  Planes
 ↑ Alternate Parameter Planes by David E. Joyce
 ↑ muency : exponential map by R Munafo
 ↑ Exponential mapping and OpenMP by Claude HeilandAllen
 ↑ Linas Vepstas : Self Similar?
 ↑ the flattened cardioid of a Mandelbrot by Tom Rathborne
 ↑ Stretching cusps by Claude HeilandAllen
 ↑ Twisted Mandelbrot Sets by Eric C. Hill
 ↑ doubling bifurcations on complex plane by E Demidov
 ↑ On biaccessible points in the Julia set of the family z(a+z^{d}) by Mitsuhiko Imada
 ↑ Surgery in Complex Dynamics by Carsten Lunde Petersen, online paper
 ↑ Nucleus  From the Mandelbrot Set Glossary and Encyclopedia, by Robert Munafo, (c) 19872015.
 ↑ Siegel disks by Xavier Buff and Arnaud Ch ́ritat e Univ. Toulouse Roma, April 2009
 ↑ wikipedia : Critical point (mathematics)
 ↑ Java program by Dieter Röß showing result of changing initial point of Mandelbrot iterations
 ↑ Cut point in wikipedia
 ↑ On local connectivity for the Julia set of rational maps : Newton’s famous example By P. Roesch
 ↑ muency : feigenbaum point
 ↑ On Periodic and Chaotic Regions in the Mandelbrot Set by G. Pastor , M. Romera, G. Álvarez, D. Arroyo and F. Montoya
 ↑ fractalfaq : section 6
 ↑ Period doubling and Feigenbaum's scaling be E Demidov
 ↑ mathoverflow question : isthereawaytofindregionsofdepthinthemandelbrotsetotherthansimply?rq=1
 ↑ [w:Point at infinityPoint at infinity in wikipedia]
 ↑ Mathoverflow question : Attractive Basins and Loops in Julia Sets
 ↑ wikipedia : Misiurewicz point
 ↑ Symbolic sequences of onedimensional quadratic map points by G Pastor, Miguel Romera, Fausto Montoya Vitini
 ↑ mathoverflow question : Is there a way to find regions of depth in the Mandelbrot set other than simply poking around?
 ↑ G. Pastor, M. Romera, G. Álvarez, D. Arroyo and F. Montoya, "On periodic and chaotic regions in the Mandelbrot set", Chaos, Solitons & Fractals, 32 (2007) 1525
 ↑ The bifurcation diagram of cubic polynomial vector fields on CP1 by Christiane Rousseau
 ↑ http://www.mndynamics.com/indexp.html%7C program Mandel by Wolf Jung , demo 2 page 3
 ↑ GROWTH OF GROUPS DEFINED BY AUTOMATA : ASHLEY S. DOUGHERTY, LYDIA R. KINDELIN, AARON M. REAVES, ANDREW J. WALKER, AND NATHANIEL F. ZAKAHI
 ↑ wikipedia : Orbit portrait
 ↑ Airplane primitive parabolic implosion by Wolf Jung
 ↑ CANTOR BOUQUETS, EXPLOSIONS, AND KNASTER CONTINUA: DYNAMICS OF COMPLEX EXPONENTIALS by Robert L. Devaney Publicacions Matematiques, Vol 43 (1999), 27–54.
 ↑ Tuning From the Mandelbrot Set Glossary and Encyclopedia, by Robert Munafo, (c) 19872014.
 ↑ wikipedia : Conformal radius
 ↑ scholarpedia : Quadratic Siegel disks
 ↑ Julia Sets of Complex Polynomials and Their Implementation on the Computer by Christoph Martin Stroh
 ↑ fractalforums: bounding circle of julia sets by knighty
 ↑ wikipedia : Sequence
 ↑ wikipedia : series
 ↑ wikipedia : Continuum in set theory
 ↑ Muatom From the Mandelbrot Set Glossary and Encyclopedia, by Robert Munafo, (c) 19872013.
 ↑ Island MuMolecule by Robert P. Munafo, 2012 Aug 18.
 ↑ Internal addresses in the Mandelbrot set and Galois groups of polynomials by Dierk Schleicher, page 31
 ↑ Child From the Mandelbrot Set Glossary and Encyclopedia, by Robert Munafo, (c) 19872013.
 ↑ Surgery in Complex Dynamics by Carsten Lunde Petersen, online paper
 ↑ Internal addresses in the Mandelbrot set and irreducibility of polynomials by Dierk Schleicher
 ↑ wikipedia : Carathéodory's theorem (conformal mapping)
 ↑ The intrinsic geometry of a Jordan domain by Richard L. Bishop
 ↑ A. Blokh, X. Buff, A. Cheritat, L. Oversteegen The solar Julia sets of basic quadratic Cremer polynomials, Ergodic Theory and Dynamical Systems , 30 (2010), #1, 5165
 ↑ Fractus doc by Richard Rosenman
 ↑ wikipedia : Escaping set
 ↑ fractint doc : bailout
 ↑ Dessins d’enfants and Hubbard trees by Kevin M. Pilgrim