Fractals/Iterations in the complex plane/parabolic

"Most programs for computing Julia sets work well when the underlying dynamics is hyperbolic but experience an exponential slowdown in the parabolic case." ( Mark Braverman )

In other words it means that one can need days for making a good picture of parabolic Julia set with standard / naive algorithms.

There are 2 problems here :
 * slow (= lazy) local dynamics ( in the neighbourhood of a parabolic fixed point )
 * some parts are very thin ( hard to find using standard plane scanning)

=Planes=

Dynamic plane
Dynamic plane = complex z-plane $$ \mathbb{C}  = J_f \cup F_f $$ :
 * Julia set $$ J_f \subset \mathbb{C}  $$ is a common boundary : $$J_f\, = \partial A_f(p) =\partial  A_{f}(\infty)$$
 * Fatou set $$ F_f \subset \mathbb{C}  $$
 * exterior of Julia set = basin of attraction to infinity : $$A_{f}(\infty) \ \overset{\underset{\mathrm{def}}{}}{=} \  \{ z \in  \mathbb{C}  : f^{(k)} (z)  \to  \infty\  as\  k \to \infty \}. $$
 * interior of Julia set = basin of attraction of finite, parabolic fixed point p : $$A_f(p) \ \overset{\underset{\mathrm{def}}{}}{=} \  \{ z \in  \mathbb{C}  : f^{(k)} (z)  \to  p\  as\  k \to \infty \}. $$
 * immediate basin = sum of componets which have parabolic fixed point p on it's boundary  ; the immediate parabolic basin of p is the union of periodic connected components of the parabolic basin.
 * attracting Lea-Fatou flower = sum of n attracting petals = sum of 2*n attracting sepals
 * petal = part of the flower. Each petal contains part of 2 sepals,
 * sepals ( Let 1 be an invariant curve in the first quadrant and L 1 the region enclosed by 1 ∪ {0}, called a sepal. )

$$ \mathbb{C} \supset F(f) \supset A_{f}(p) $$

See also :
 * Filled Julia set $$ K_f $$

=Key words=
 * parabolic chessboard or checkerboard
 * parabolic implosion
 * Fatou coordinate
 * Hawaiian earring
 * in wikipedia = "The plane figure formed by a sequence of circles that are all tangent to each other at the same point and such that the sequence of radii converges to zero." ( Barile, Margherita in MathWorld)
 * commons:Category:Hawaiian earrings
 * Gevrey symptotic expansions
 * the Écalle-Voronin invariants of (7.1) at the origin which have Gevrey- 1/2 asymptotic expansions
 * germ
 * germ of the function : Taylor expansion of the function
 * multiplicity
 * Julia-Lavaurs sets
 * The Leau-Fatou flower theorem: repelling or attracting flower. Flower consist of petals
 * Parabolic Linearization theorem
 * The horn map
 * Blaschke product
 * Inou and Shishikura's near parabolic renormalization
 * complex polynomial vector field
 * numbers
 * "a positive integer ν, the parabolic degeneracy with the following property: there are νq attracting petals and νq repelling petals, which alternate cyclically around the fixed point."
 * combinatorial rotation number
 * a Poincaré linearizer of function f at parabolic fixed point
 * " the parabolic pencil. This is the family of circles which all have one common point, and thus are all tangent to each other, either internally or externally. "

Ecalle cilinder
Ecalle cylinders or Ecalle-Voronin cylinders ( by Jean Ecalle )

"... the quotient of a petal P under the equivalence relation identifying z and f (z) if both z and f (z) belong to P. This quotient manifold is called the Ecalle cilinder, and it is conformally isomorphic to the infinite cylinder C/Z"

eggbeater dynamics
Physical model : the behaviour of cake when one uses eggbeater.

The mathematical model : a 2D vector field with 2 centers ( second-order degenerate points )

The field is spinning about the centers, but does not appear to be diverging.

Maybe better description of parabolic dynamics will be Hawaiian earrings

parabolic germ
Germ :
 * z+z^2
 * z+z^3
 * z+z^{k+1}
 * z+a_{k+1}z^{k+1}
 * z+a_{k+1}z^{k+1}
 * "a germ $$f(x)= a_{1}x+a_{2}x^2 + \ldots $$ with $$\vert a_{1} \vert \neq 0,1$$ is holomorphically conjugated to its linear part $$g(x)=a_{1}z$$" ( Sylvain Bonnot )

germ of vector field

The horn map
" the horn map h = Φ ◦ Ψ, where Φ is a shorthand for Φattr and Ψ for Ψrep (extended Fatou coordinate and parameterizations)."

Petal


"The petals ... are interesting not only because they give a rather good intuitive idea of the dynamics that arise near a parabolic point, but also because that the dynamic of f0 on a petal can be linearized, i.e., it is conjugated to the shift map T of C defined by T(w) := w + 1." ( Laurea Triennale )

There is no unified definition of petals.

Petal of a flower can be :
 * attracting / repelling
 * small/alfa/big/ ( small attracting petals do not ovelap with repelling petals, but big do)

Each petal is invariant under f^period. In other words it is mapped to itself by f^period.

Attracting petal P is a :
 * Each petal is invariant under $$f^n $$. In other words it is mapped to itself by $$f^n $$: $$f^n(\overline{P} ) \subset P \cup \left\{ p \right\} $$
 * domain (topological disc ) containing :
 * parabolic periodic point p in its boundary $$\overline{P} \ni \left\{ p \right\} $$ ( precisely in its root, which is a coomon points of all attracting and repelling petals = center of the Lea-Fatou flower)
 * critical point or it's n=period images on the other side ( only small ?? )
 * trap which captures any orbit tending to parabolic point
 * set contained inside component of filled-in Julia set. The attracting petals of parabolic fixed point are contained in it's basin of attraction
 * " ... is maximal with respect to this property. This preferred petal P max always has one or more critical points on its boundary."
 * "an attracting petal is the interior of an analytic curve which lies entirely in the Fatou set, has the right tangency property at the fixed point, and is mapped into its interior by the correct power of the map" Scott Sutherland
 * "... an attracting petal is a set of points in a sufficient small disk around the periodic point whose forward orbits always remain in the disk under powers of return map. " ( W P Thurston : On the geometry and dynamics of Iterated rational maps)

Petals $$P_j$$ are symmetric with respect to the d-1 directions :

$$ arg(z) = \frac{2 \Pi l}{d - 1}  $$

where :
 * d is (to do)
 * l is from 0 to d-2

Petals can have different size.

If $$\lambda^n = 1 $$ then Julia set should approach parabolic periodic point in n directions, between n petals.

" Using the language of holomorphic dynamics, people would say that you are studying the dynamics of a polynomial near the parabolic fixed point $$z=0$$. By a simple linear change of variables, the study of any such parabolic fixed point can be reduced to the study of $$z \mapsto z+z^{2}+O(z^3)$$. Then you can apply another change $$w=-\frac{1}{z}$$. Thus you are reduced to the study of $$f(w)=w+1+O(1/w)$$. If the real part $Re(w)$ is large enough you will obtain $$f^{n}(w)=w+n+O(\log n)$$. This will give you what you want (when going back to the z-variable).

The domain $$Re(w)>R$$ (for large $$R$$) looks like some kind of cardioid (in your particular case) when you visualize it in the z-variable (it's poetically called an attracting petal). " Sylvain Bonnot

0/1 or 1/1
First attracting petal is a circle with:
 * center on the x axis
 * radius = ( cabs(zf) + cabs(z))/2

Other ( bigger ) attracting petals are preimages of first petal which include first petal

where:
 * z is the last point of critical orbit
 * zf is a fixed point

1/2
circular attracting petal:
 * center is between fixed point and critical point
 * radius smaller then half of the distance between fixed and critical point

1/3
Method by Scott Sutherland:
 * choose the connected component containing the critical point
 * find an analytic curve which lies entirely in the Fatou set, has the right tangency property at the fixed point, and is mapped into its interior by the correct power of the map
 * the other two are just the image of this curve under the first and second iterates.

Number of petals


For quadratic polynomials :

Multiplicity = ParentPeriod + ChildPeriod

NumberOfPetals = multiplicity - ParentPeriod

It is because in parabolic case fixed point coincidence with periodic cycle. Length of cycle ( child period) is equal to number of petals

For other polynomial maps :

For f(z)= -z+z^(p+1) parabolic flower has :
 * 2p petals for p odd
 * p petals for p even

... ( to do )

Sepal
Definitions:
 * A sepal is the intersection of an attracting and repelling petal.A parabolic Pommerenke-Levin-Yoccoz inequality. by Xavier Buf and Adam L. Epstein There does not seem to be an official definition of sepal.
 * "Let l be an invariant curve in the first quadrant and L1 the region enclosed by l ∪ {0}, called a sepal."
 * interior of component with parabolic fixed point on it's boundary

Flower
Sum of all petals creates a flower with center at parabolic periodic point.

Cauliflower
Cauliflower or broccoli :
 * empty ( its interior is empty ) for c outside Mandelbrot set. Julia set is a totally disconnected (
 * filled cauliflower for c=1/4 on boundary of the Mandelbrot set. Julia set is a Jordan curve ( quasi circle).

Pleae note that :
 * size of image differs because of different z-planes.
 * different algorithms are used so colours are hard to compare

Bifurcation of the Cauliflower
How Julia set changes along real axis ( going from c=0 thru c=1/4 and further ) :

Perturbation of a function $$f(z)$$ by complex $$\epsilon$$ :

$$g(z) = f(z) + \epsilon $$

When one add epsilon > 0 ( move along real axis toward + infinity ) there is a bifurcation of parabolic fixed point :
 * attracting fixed point ( epsilon<0 )
 * one parabolic fixed point ( epsilon = 0 )
 * one parabolic fixed point splits up into two conjugate repelling fixed points ( epsilon > 0 )

"If we slightly perturb with epsilon<0 then the parabolic fixed point splits up into two real fixed points on the real axis (one attracting, one repelling). "

See :
 * demo 2 page 9 in program Mandel by Wolf Jung

parabolic implosion
Video on YouTube

Vector field

 * 2D vector field and its

singularity
singularity types :
 * center type : "In this case, one can find a neighborhood of the singular point where all integral curves are closed, inside one another, and contain the singular point in their interior"
 * non-center type : neighborhood of singularity is made of several curvilinear sectors :

" A curvilinear sector is defined as the region bounded by a circle C with arbitrary small radius and two streamlines S and S! both converging towards singularity. One then considers the streamlines passing through the open sector g in order to distinguish between three possible types of curvilinear sectors."

=Local dynamics=

Local dynamics :
 * in the exterior of Julia set
 * on the Julia set
 * near parabolic fixed point ( inside Julia set )

Near parabolic fixed point
Why analyze f^p not f ?

Forward orbit of f near parabolic fixed point is composite. It consist of 2 motions :
 * around fixed point
 * toward / away from fixed point

=How to compute parabolic c values = Description

For internal angle n/p parabolic period p cycle consist of one z-point with multiplicity p and multiplier = 1.0. This point z is equal to fixed point $$z_{alfa}$$

Period 1
One can easily compute boundary point c

$$ c = c_x + c_y*i $$

of period 1 hyperbolic component ( main cardioid) for given internal angle ( rotation number) t using this cpp code by Wolf Jung

or this Maxima CAS code : /* conformal map from circle to cardioid ( boundary of period 1 component of Mandelbrot set */ F(w):=w/2-w*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((1-sqrt(1-4*c))/2)), /* alfa fixed point */ display(alfa) )$

Periods 1-6
/*

batch file for Maxima CAS computing bifurcation points for period 1-6

Formulae for cycles in the Mandelbrot set II Stephenson, John; Ridgway, Douglas T. Physica A, Volume 190, Issue 1-2, p. 104-116.

kill(all); remvalue(all);

start:elapsed_run_time ;

/* functions --*/

/* exponential for of complex number with angle in turns */ /* "exponential form prevents allroots from working", code by Robert P. Munafo */

GivePoint(Radius,t):=rectform(ev(Radius*%e^(%i*t*2*%pi), numer))$ /* gives point of unit circle for angle t in turns */

GiveCirclePoint(t):=rectform(ev(%e^(%i*t*2*%pi), numer))$ /* gives point of unit circle for angle t in turns Radius = 1 */

/* gives a list of iMax points of unit circle */ GiveCirclePoints(iMax):=block( [circle_angles,CirclePoints], CirclePoints:[], circle_angles:makelist(i/iMax,i,0,iMax), for t in circle_angles do CirclePoints:cons(GivePoint(1,t),CirclePoints), return(CirclePoints) /* multipliers */ )$

/* http://commons.wikimedia.org/wiki/File:Mandelbrot_set_Components.jpg Boundary equation b_n(c,P)=0 defines relations between hyperbolic components and unit circle for given period n , allows computation of exact coordinates of hyperbolic componenets.

b_n(w,c), is boundary polynomial ( implicit function of 2 variables ).



GiveBoundaryEq(P,n):= block( if n=1 then return(c + P^2 - P), if n=2 then return(- c + P - 1), if n=3 then return(c^3 + 2*c^2 - (P-1)*c + (P-1)^2), if n=4 then return( c^6 + 3*c^5 + (P+3)* c^4 + (P+3)* c^3 - (P+2)*(P-1)*c^2 - (P-1)^3), if n=5 then return(c^15 + 8*c^14 + 28*c^13 + (P + 60)*c^12 + (7*P + 94)*c^11 + (3*P^2 + 20*P + 116)*c^10 + (11*P^2 + 33*P + 114)*c^9 + (6*P^2 + 40*P + 94)*c^8 + (2*P^3 - 20*P^2 + 37*P + 69)*c^7 + (3*P - 11)*(3*P^2 - 3*P - 4)*c^6 + (P - 1)*(3*P^3 + 20*P^2 - 33*P - 26)*c^5 + (3*P^2 + 27*P + 14)*(P - 1)^2*c^4 - (6*P + 5)*(P - 1)^3*c^3 + (P + 2)*(P - 1)^4*c^2 - c*(P - 1)^5 + (P - 1)^6), if n=6 then return( c^27+ 13*c^26+ 78*c^25+ (293 - P)*c^24+ (792 - 10*P)*c^23+ (1672 - 41*P)*c^22+ (2892 - 84*P - 4*P^2)*c^21+ (4219 - 60*P - 30*P^2)*c^20+ (5313 + 155*P - 80*P^2)*c^19+ (5892 + 642*P - 57*P^2 + 4*P^3)*c^18+ (5843 + 1347*P + 195*P^2 + 22*P^3)*c^17+ (5258 + 2036*P + 734*P^2 + 22*P^3)*c^16+ (4346 + 2455*P + 1441*P^2 - 112*P^3 + 6*P^4)*c^15 + (3310 + 2522*P + 1941*P^2 - 441*P^3 + 20*P^4)*c^14 + (2331 + 2272*P + 1881*P^2 - 853*P^3 - 15*P^4)*c^13 + (1525 + 1842*P + 1344*P^2 - 1157*P^3 - 124*P^4 - 6*P^5)*c^12 + (927 + 1385*P + 570*P^2 - 1143*P^3 - 189*P^4 - 14*P^5)*c^11 + (536 + 923*P - 126*P^2 - 774*P^3 - 186*P^4 + 11*P^5)*c^10 + (298 + 834*P + 367*P^2 + 45*P^3 - 4*P^4 + 4*P^5)*(1-P)*c^9 + (155 + 445*P - 148*P^2 - 109*P^3 + 103*P^4 + 2*P^5)*(1-P)*c^8 + 2*(38 + 142*P - 37*P^2 - 62*P^3 + 17*P^4)*(1-P)^2*c^7 + (35 + 166*P + 18*P^2 - 75*P^3 - 4*P^4)*((1-P)^3)*c^6 + (17 + 94*P + 62*P^2 + 2*P^3)*((1-P)^4)*c^5 + (7 + 34*P + 8*P^2)*((1-P)^5)*c^4 + (3 + 10*P + P^2)*((1-P)^6)*c^3 + (1 + P)*((1-P)^7)*c^2 + -c*((1-P)^8) + (1-P)^9) )$

/* gives a list of points c on boundaries on all components for give period */ GiveBoundaryPoints(period,Circle_Points):=block( [Boundary,P,eq,roots], Boundary:[], for m in Circle_Points do (/* map from reference plane to parameter plane */ P:m/2^period, eq:GiveBoundaryEq(P,period), /* Boundary equation b_n(c,P)=0  */ roots:bfallroots(%i*eq), roots:map(rhs,roots), for root in roots do Boundary:cons(root,Boundary)), return(Boundary) )$

/* divide llist of roots to 3 sublists = 3 components */ /* boundaries of period 3 components period:3$ Boundary3Left:[]$ Boundary3Up:[]$ Boundary3Down:[]$

Radius:1;

for m in CirclePoints do ( P:m/2^period,  eq:GiveBoundaryEq(P,period),  roots:bfallroots(%i*eq),  roots:map(rhs,roots),  for root in roots do      ( if realpart(root)<-1 then Boundary3Left:cons(root,Boundary3Left), if (realpart(root)>-1 and imagpart(root)>0.5) then Boundary3Up:cons(root,Boundary3Up), if (realpart(root)>-1 and imagpart(root)<0.5) then Boundary3Down:cons(root,Boundary3Down) )

)$ - */

/* gives a list of parabolic points for given : period and internal angle */ GiveParabolicPoints(period,t):=block ( [m,ParabolicPoints,P,eq,roots], m: GiveCirclePoint(t), /* root of unit circle, Radius=1, angle t=0 */ ParabolicPoints:[], /* map from reference plane to parameter plane */ P:m/2^period, eq:GiveBoundaryEq(P,period), /* Boundary equation b_n(c,P)=0  */ roots:bfallroots(%i*eq), roots:map(rhs,roots), for root in roots do ParabolicPoints:cons(float(root),ParabolicPoints), return(ParabolicPoints)

)$

compile(all)$

/* - constant values --*/

fpprec:16;

/* unit circle on a w-plane -*/ a:GiveParabolicPoints(6,1/3); a$

=How to draw parabolic Julia set=

All points of interior of filled Julia set tend to one periodic orbit ( or fixed point ). This point is in Julia set and is weakly attracting. One can analyse only behevior near parabolic fixed point. It can be done using critical orbits.

There are two cases here : easy and hard.

If the Julia set near parabolic fixed point is like n-th arm star ( not twisted) then one can simply check argument of of zn, relative to the fixed point. See for example z+z^5. This is an easy case.

In the hard case Julia set is twisted around fixed.

Escape time
Description

Long iteration method
Long iteration method

Dynamic rays
One can use periodic dynamic rays landing on parabolic fixed point to find narrow parts of exterior.

Let's check how many backward iterations needs point on periodic ray with external radius = 4 to reach distance 0.003 from parabolic fixed point :

One can use only argument of point z of external rays and its distance to alfa fixed point. ( see code from image) It works for periods up to 15 ( maybe more ... )

Estimation from interior
Julia set is a boundary of filled-in Julia set Kc.


 * find points of interior of Kc
 * find boundary of interior of Kc using edge detection

If components of interior are lying very close to each other then find components using : color = LastIteration % period

For parabolic components between parent and child component : periodOfChild = denominator*periodOfParent color = iLastIteration % periodOfChild

where denominator is a denominator of internal angle of parent comonent of Mandelbrot set.

Angle
"if the iterate zn of tends to a fixed parabolic point, then the initial seed z0 is classified according to the argument of zn−z0, the classification being provided by the flower theorem " ( Mark McClure )

Attraction time
Interior of filled Julia set consist of components. All comonents are preperiodic, some of them are periodic ( immediate basin of attraction).

In other words :
 * one iteration moves z to another component ( and whole component to another component)
 * all point of components have the same attraction time ( number of iteration needed to reach target set around attractor)

It is possible to use it to color components. Because in parabolic case attractor is weak ( weakly attracting) it needs a lot of iterations for some points to reach it.

Here are some example values : iWidth = 1001 // width of image in pixels PixelWidth = 0.003996 AR = 0.003996 // Radius around attractor denominator = 1 ; Cx  = 0.250000000000000; Cy  = 0.000000000000000 ax  = 0.500000000000000; ay  = 0.000000000000000 denominator = 2 ; Cx  = -0.750000000000000; Cy  = 0.000000000000000 ax  = -0.500000000000000; ay  = 0.000000000000000 denominator = 3 ; Cx  = -0.125000000000000; Cy  = 0.649519052838329 ax  = -0.250000000000000; ay  = 0.433012701892219 denominator = 4 ; Cx  = 0.250000000000000; Cy  = 0.500000000000000 ax  = 0.000000000000000; ay  = 0.500000000000000 denominator = 5 ; Cx  = 0.356762745781211; Cy  = 0.328581945074458 ax  = 0.154508497187474; ay  = 0.475528258147577 denominator = 6 ; Cx  = 0.375000000000000; Cy  = 0.216506350946110 ax  = 0.250000000000000; ay  = 0.433012701892219 denominator = 1 ;   i =               243.000000 denominator = 2 ;   i =            31 171.000000 denominator = 3 ;   i =         3 400 099.000000 denominator = 4 ;   i =       333 293 206.000000 denominator = 5 ;   i =    29 519 565 177.000000 denominator = 6 ;   i = 2 384 557 783 634.000000

where :

C = Cx + Cy*i a = ax + ay*i // fixed point alpha i // number of iterations after which critical point z=0.0 reaches disc around fixed point alpha with radius AR denominator of internal angle ( in turns ) internal angle = 1/denominator

Note that attraction time i is proportional to denominator. Now you see what means weakly attracting.

One can :
 * use brutal force method ( Attracting radius < pixelSize; iteration Max big enough to let all points from interior reach target set; long time or fast computer )
 * find better method (:-)) if time is to long for you

Estimation from interior and exterior
Julia set is a common boundary of filled-in Julia set and basin of attraction of infinity.


 * find points of interior/components of Kc
 * find escaping points
 * find boundary points using Sobel filter

It works for denominator up to 4.

Inverse iteration of repelling points
Inverse iteration of alfa fixed point. It works good only for cuting point ( where external rays land). Other points still are not hitten.

Bof61

 * Using bof61 for coloring interior
 * example

=Gallery=

External examples:
 * A parabolic point with 377 petalsparabolic renormalization of z^3+c by YANG Fei
 * A quad. Julia sets with 987 and 89 petals by A Cheritat

For other polynomial maps see here

=See also =
 * Image : Nonstandard Parabolic by Cheritat
 * Julia set of parabolic case in Maxima CAS
 * The parabolic Mandelbrot set Pascale ROESCH (joint work with C. L. PETERSEN
 * PARABOLIC IMPLOSION A MINI-COURSE by ArnaudCheritat
 * Workshop on parabolic implosion 2010
 * The renormalization for parabolic fixed points... Mitsushiro Shishikura and Hiroyuki Inou
 * Dynamics of holomorphic maps: Resurgence of Fatou coordinates, and Poly-time computability of Julia sets by Artem Dudko, arxiv.org : Dudko_A
 * Minicourse "Analytic classification of germs of generic families unfolding a parabolic point by Christiane Rousseau
 * Perspectives on Parabolic Points in Holomorphic Dynamics - The Banff International Research Station for Mathematical Innovation and Discovery (BIRS)
 * Richard Oudkerk : The Parabolic Implosion for f_0(z) = z + z^{nu+1} + O(z^{nu+2})
 * Perspectives on Parabolic Points in Holomorphic Dynamics Videos from BIRS Workshop 15w5082
 * Generic Perturbation of Parabolic Points Having More Than One Attracting Petal by Arnaud Chéritat

=References=