Intro

Pariod doubling cascade in the Mandelbrot set ( 1/2 family) showed by the exponential mapping
escape route 1/2
period doubling
Self-similarity in the Mandelbrot set shown by zooming on a round feature while panning in negative-X direction. The display center pans from (-1,0) to (-1.31,0) while the view magnifies from .5 x.5 to .12 x.12.

Periods of the period doubling cascade:^[1]

 $1*2^{n}$

Angled internal address:

 $\mathbf {MF} _{1/2}{\xleftarrow {1/2}}....{\xleftarrow {1/2}}\ 16\quad {\xleftarrow {1/2}}\ 8\quad {\xleftarrow {1/2}}\ 4\quad {\xleftarrow {1/2}}\ 2\quad {\xleftarrow {1/2}}\ 1$

where:

$\mathbf {MF} _{1/2}$ is the Myrberg-Feigenbaum point c = −1.401155 with external angles = (0.412454... , 0,58755...)

It is a part of Sharkovsky ordering

External angles (combinatorial algorithms)

External angle of the parameter rays landin on the root points of hyperbolic components from the 1/2 family

Binary

The period also corresponds to the number of digits that make up the binary periodic fraction.

angles ( binary periodic fractions) of hyperbolic components from the period doubling cascade 1*2^n
period = 1 	 0.(0)	                                                                 0.(1)
period = 2 	 0.(01)	                                                                 0.(10)
period = 4 	 0.(0110)	                                                         0.(1001)
period = 8 	 0.(01101001)	                                                         0.(10010110)
period = 16 	 0.(0110100110010110)	                                                 0.(1001011001101001)
period = 32 	 0.(01101001100101101001011001101001)	                                 0.(10010110011010010110100110010110)
period = 64 	 0.(0110100110010110100101100110100110010110011010010110100110010110)	 0.(1001011001101001011010011001011001101001100101101001011001101001)
period = 128 	 0.(01101001100101101001011001101001100101100110100101101001100101101001011001101001011010011001011001101001100101101001011001101001)	 
                 0.(10010110011010010110100110010110011010011001011010010110011010010110100110010110100101100110100110010110011010010110100110010110)
period = 256 	 
0.(0110100110010110100101100110100110010110011010010110100110010110100101100110100101101001100101100110100110010110100101100110100110010110011010010110100110010110011010011001011010010110011010010110100110010110100101100110100110010110011010010110100110010110)	 
0.(1001011001101001011010011001011001101001100101101001011001101001011010011001011010010110011010011001011001101001011010011001011001101001100101101001011001101001100101100110100101101001100101101001011001101001011010011001011001101001100101101001011001101001)

Note that :

all angles are periodic binary fractions
length of binary periodic part = period

String Concatenation

MSS-harmonics ^[2] ( Metropolis, Stein and Stein^[3] ):

$H_{MSS}(s_{1},s_{2})=(s_{1}s_{2},s_{2}s_{1})$

in the form of binary fraction:

input : $0.(s_{1})$ and $0.(s_{2})$
output : $0.(s_{1}s_{2})$ and $0.(s_{2}s_{1})$

I can be computed with c code :

/*
Operating with external arguments in the Mandelbrot set antenna
by G Pastor, M Romera, G Alvarez and F Montoya, December 16, 2004

-------------- asprintf --------------------------------------
Using asprintf instead of sprintf or snprintf by james
http://www.stev.org/post/2012/02/10/Using-saprintf-instead-of-sprintf-or-snprintf.aspx

http://ubuntuforums.org/showthread.php?t=279801

gcc c.c -D_GNU_SOURCE -Wall // without #define _GNU_SOURCE

gcc h.c -Wall
cppcheck h.c

----------- run ----------------------

./a.out
./a.out > h.txt

----------------
*/

#define _GNU_SOURCE // asprintf
#include <stdio.h>
#include <stdlib.h>
#include <string.h> // strlen
 
int main() {
    	// output = angles of p*2^n component
    	char *sOut1  = ""; // in plaint text format
    	char *sOut2  = ""; // in plaint text format
    
    	// input = angles of period p=1 component
    	char *sIn1 = "0"; 
    	char *sIn2 = "1"; 
	
	int n = 0;    
	int nMax = 10;
	int p =1;  
	
  	printf(" angles ( binary periodic fractions) of hyperbolic components from the period doubling cascade %d*2^n\n ", p);
	printf(" period = %d \t 0.(%s)\t 0.(%s)\n", p, sIn1, sIn2);
    	
	
  
   	for (n=1; n<nMax; n  ){

   		p *= 2; // period doubling cascade
   		// MSS-harmonic h(sIn1. sIn2) = (sOut1, sOut2) = (sIn1 sIn2, sIn2   sIn1  ) here   means concat the strings 
   		asprintf(&sOut1, "%s%s", sIn1, sIn2);
   		asprintf(&sOut2, "%s%s", sIn2, sIn1);
   		
       		//
		printf(" period = %d \t 0.(%s)\t 0.(%s)\n", p, sOut1, sOut2);
		// 
		sIn1 = sOut1;
		sIn2 = sOut2;
		
		}
    	

    	//
    	free(sOut1);
    	free(sOut2); 
   
    	return 0;
}

hyperbolic components ( numerical algorithms)

Root points

$n$	Period = $2 n$	Root point ( $c n$ )
0	1	0.25
1	2	−0.75
2	4	−1.25
3	8	−1.3680989
4	16	−1.3940462
5	32	−1.3996312
6	64	−1.4008287
7	128	−1.4010853
8	256	−1.4011402
9	512	−1.401151982029
10	1024	−1.401154502237
$\infty$		−1.4011551890…

Centers

Data by lkmitch:

Period 262144

x = -1.4011551890902510331817705605834440363471931682724714412452613678632418220750013209654238789188079407613058592287511922521315976742525764917468403339396930937 30785180509439998407177461884732043 f(x) = 0.0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 00000000000000000000000000000001994 Approx Feigenbaum constant = 4.6692016090744525662279815203708867539460996466796182702147591041742162322183312521153913774503310728833354374225852275733454310057268638843688036767882792034 77482728794667534497622208785380761

Period 524288

-1.4011551890916651883071968100816546650318029614591678115404876967937578305271204258535401015561476261168939337667710591343229259782689769629427546629533666727 86737113473009338909783794873017929 0.0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 00000000000000000000000000008829391 4.6692016090968787947051350378647836776226665257418367260642987723027044088401013356743953120638886994058416817724607788627924785757422345903201225592627931049 69373245311653832559840230430927275

Period 1048576

-1.4011551890919680570294789310328705961503197610898601690317026045601400345356095836255726490446857492092529857212919383793658357679431376624985583329486967143 41390220891894934332628723842939248 -0.0000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000000 00000000000000000000000000022112864 4.6692016091016816811869601608458017299280888932440761709767910764158204329663666795299227205144754947240340906747557847995318754327409221893703408072446351537 83290121618647654581771235818384323

c code from mandelbrot-numerics

m-feigenbaum program from mandelbrot-numerics library

m-feigenbaum
period = 4 	     		 nucleus = -1.310702641336833008e 00 	size = 1.179602276312223114e-01
period = 8 		    	 nucleus = -1.381547484432061657e 00 	size = 2.590331788620404280e-02
period = 16 			 nucleus = -1.396945359704560685e 00 	size = 5.574904503817590395e-03
period = 32 			 nucleus = -1.400253081214783091e 00 	size = 1.195288587163239984e-03
period = 64 			 nucleus = -1.400961962944842210e 00 	size = 2.560528805309172169e-04
period = 128 			 nucleus = -1.401113804939776664e 00 	size = 5.484142131458955168e-05
period = 256 			 nucleus = -1.401146325826946537e 00 	size = 1.174547734653405196e-05
period = 512 			 nucleus = -1.401153290849925570e 00 	size = 2.515527294624666474e-06
period = 1024 			 nucleus = -1.401154782546613964e 00 	size = 5.387491809938387059e-07
period = 2048 			 nucleus = -1.401155102022462628e 00 	size = 1.153835913118543914e-07
period = 4096 			 nucleus = -1.401155170444413400e 00 	size = 2.471163334462234791e-08
period = 8192 			 nucleus = -1.401155185098302614e 00 	size = 5.292465190668938379e-09
period = 16384 			 nucleus = -1.401155188236713700e 00 	size = 1.133481216591179550e-09
period = 32768 			 nucleus = -1.401155188908850047e 00 	size = 2.427895317585669274e-10
period = 65536 			 nucleus = -1.401155189052770256e 00 	size = 5.204848444681121846e-11
period = 131072 		 nucleus = -1.401155189083645558e 00 	size = 1.116488091172383448e-11
period = 262144 		 nucleus = -1.401155189090176112e 00 	size = 2.401481531760724511e-12
period = 524288 		 nucleus = -1.401155189091663589e 00 	size = 6.463020532652650290e-13
period = 1048576 		 nucleus = -1.401155189092033737e 00 	size = 3.635753686080000682e-14
period = 2097152 		 nucleus = -1.401155189093066022e 00 	size = 9.366255511607845319e-19
period = 4194304 		 nucleus = -1.401155189093066022e 00 	size = 2.943937947459073103e-26
period = 8388608 		 nucleus = -1.401155189093066022e 00 	size = 5.438985544182134629e-40
period = 16777216 		 nucleus = -1.401155189093066022e 00 	size = 5.967915741322236566e-68
period = 33554432 		 nucleus = -1.401155189093066022e 00 	size = 8.736600707368986815e-124
period = 67108864 		 nucleus = -1.401155189093066022e 00 	size = 1.222084981000085251e-235
period = 134217728 		 nucleus = -1.401155189093066022e 00 	size = 0.000000000000000000e 00
period = 268435456 		 nucleus = -1.401155189093066022e 00 	size = 0.000000000000000000e 00

It seems that double precision is not enough

c code from Mandel

Centers of hyperbolic components are easier to compute then root points ( bifurcation points).

Period =          1 	center =  0.000000000000000000
Period =          2 	center = -1.000000000000000000
Period =          4 	center = -1.310702641336832884
Period =          8 	center = -1.381547484432061470
Period =         16 	center = -1.396945359704560642
Period =         32 	center = -1.400253081214782798
Period =         64 	center = -1.400961962944841041
Period =        128 	center = -1.401113804939776124
Period =        256 	center = -1.401146325826946179
Period =        512 	center = -1.401153290849923882
Period =       1024 	center = -1.401154782546617839 
Period =       2048 	center = -1.401155102022463976
Period =       4096 	center = -1.401155170444411267
Period =       8192 	center = -1.401155185098297292
Period =      16384 	center = -1.401155188236710937
Period =      32768 	center = -1.401155188908863045
Period =      65536 	center = -1.401155189052817413
Period =     131072 	center = -1.401155189083648072
Period =     262144 	center = -1.401155189090251057
Period =     524288 	center = -1.401155189091665208
Period =    1048576 	center = -1.401155189091968106
Period =    2097152 	center = -1.401155189092033014
Period =    4194304 	center = -1.401155189092046745
Period =    8388608 	center = -1.401155189092049779
Period =   16777216 	center = -1.401155189092050532
Period =   33554432 	center = -1.401155189092051127
Period =   67108864 	center = -1.401155189092050572
Period =  134217728 	center = -1.401155189092050593
Period =  268435456 	center = -1.401155189092050599

It is computed with cpp program using the code from Mandel

 
/*

This is not official program by W Jung,
but it usess his code ( I hope in a good way)
   These functions are part of Mandel  by Wolf Jung (C) 
   which is free software; you can
   redistribute and / or modify them under the terms of the GNU General
   Public License as published by the Free Software Foundation; either
   version 3, or (at your option) any later version. In short: there is
   no warranty of any kind; you must redistribute the source code as well.
   
   http://www.mndynamics.com/indexp.html
   
   to compile :
   g   f.cpp -Wall -lm
   ./a.out
   
  
*/

#include <iostream> // std::cout
#include <cmath>     // sqrt
#include <limits>
#include <cfloat>
  
typedef  unsigned int  uint;
typedef  long double  mdouble; // mdynamo.h

// from the file qmnshell.cpp  by Wolf Jung (C) 2007-2018
mdouble cFb = -1.40115518909205060052L; 
mdouble dFb = 4.66920160910299067185L;

mdouble bailout = 16.0L; // mdynamoi.h

// c = A B*i
mdouble A= 0.0L;  
mdouble B = 0.0L;

/* 
   function from mndlbrot.cpp  by Wolf Jung (C) 2007-2017 ...
   part of Mandel 5.14, which is free software; you can
   redistribute and / or modify them under the terms of the GNU General
   Public License as published by the Free Software Foundation; either
   version 3, or (at your option) any later version. In short: there is
   no warranty of any kind; you must redistribute the source code as well.
   
   http://www.mndynamics.com/indexp.html
   ----------------------------------------------
   
   it is used to find :
   * periodic or preperiodic points on dynamic plane 
   * on parameter plane 
   ** centers
   ** Misiurewicz points
   
   using Newton method
  
   
*/
int find(int sg, uint preper, uint per, mdouble &x, mdouble &y) 
{  mdouble a = A, b = B, fx, fy, px, py, w;
  uint i, j;
   
  for (i = 0; i < 30; i  )
    { if (sg > 0) // parameter plane
	{ a = x; b = y; } 
         
      if (!preper) // preperiod==0
	{  if (sg > 0) // parameter plane
	    { fx = 0; 
	      fy = 0; 
	      px = 0; 
	      py = 0; }
	       
	  else // dynamic plane
	    { fx = -x; 
	      fy = -y; 
	      px = -1; 
	      py = 0; }
	}
	
      else // preperiod > 0
	{ fx = x; 
	  fy = y; 
	  px = 1.0; 
	  py = 0;
	  
	  for (j = 1; j < preper; j  )
	    {  if (px*px   py*py > 1e100) return 1;
	      w = 2*(fx*px - fy*py); 
	      py = 2*(fx*py   fy*px);
	      px = w; 
	      if (sg > 0) px  ; // parameter plane
	      w = fx*fx - fy*fy   a; 
	      fy = 2*fx*fy   b; 
	      fx = w;
	    }
	}
	
      mdouble Fx = fx, Fy = fy, Px = px, Py = py;
      
      for (j = 0; j < per; j  )
	{  if (px*px   py*py > 1e100) return 2;
	  w = 2*(fx*px - fy*py); 
	  py = 2*(fx*py   fy*px);
	  px = w; 
	  if (sg > 0) px  ; // parameter plane
	  w = fx*fx - fy*fy   a; 
	  fy = 2*fx*fy   b; 
	  fx = w;
	}
      fx  = Fx; 
      fy  = Fy; 
      px  = Px; 
      py  = Py;
      w = px*px   py*py; 
      if (w < 1e-100) return -1;
      x -= (fx*px   fy*py)/w; 
      y  = (fx*py - fy*px)/w;
    }
  return 0;
}

int main()
{

  
	int plane = 1; // positive is parameter plane, negative is dynamic plane = signtype
  	uint preper = 0; // " the usual convention is to use the preperiod of the critical value. This has the advantage, that the angles of the critical value have the same preperiod under doubling as the point, and the same angles are found in the parameter plane." ( Wolf Jung )
  	uint per ; // period
  	mdouble x ;
  	mdouble y = 0.0L;
  	int n;
  
  	// Starting with a center of period  n
  	per = 1;
	x = 0.0L;
	
	// find an approximation for the center of period  2n 
	for (n=1; n<30; n  ){
     
     		 printf("Period = u \tcenter = %.18Lf\n", per, x);
        
        	// next center
      		per *= 2; // period doubling 
        	// approximate  of next value using Feigenbaum rescaling ( in the 1/2-limb )
        	x = cFb   (x - cFb)/dFb; 
        	// more precise value of x useing Newton method  
        	find(plane, preper, per, x, y); 
      
   }

  return 0;
}

Escape route 1/2

escape route 1/2

This process in which an orbit of period- $2^{n}$  successively lose stability to an orbit of period- $2^{n 1}$ , ending at a limiting value at which all periodic solutions are unstable is known as the period doubling route to chaos. (Mark Nelson)^[4]

References

Universal aspects of the period-doubling route to chaos | experiments, ODEs, and maps by Ross Dynamics Lab

[1] wikipedia: Period-doubling_bifurcation

[2] OPERATING WITH EXTERNAL ARGUMENTS IN THE MANDELBROT SET ANTENNA by G. Pastor, M. Romera, G. Alvarez, and F. Montoya

[3] On Finite Limit Sets for Transformations on the Unit interval by N. METROPOLIS, M. L. STEIN, AND P. R. STEIN

[4] M Nelson teaching. materials : part4.pdf

[5] External rays and the real slice of the Mandelbrot set by Saeed Zakeri ( paper in pdf from arxiv)

[6] ON BIACCESSIBLE POINTS OF THE MANDELBROT SET by SAEED ZAKERI

[7] wikipedia: Feigenbaum_constants

[1]

[2]

[3]

[4]

[5]

[6]

[7]

Fractals/Iterations in the complex plane/1over2 family