External ray

An external ray is a curve that runs from infinity toward a Julia or Mandelbrot set. Although this curve is only rarely a half-line (ray) it is called a ray because it is an image of a ray. External rays are used in complex analysis, particularly in complex dynamics and geometric function theory.

An external ray is a curve that runs from infinity toward a Julia or Mandelbrot set. Although this curve is only rarely a half-line (ray) it is called a ray because it is an image of a ray. External rays are used in complex analysis, particularly in complex dynamics and geometric function theory. ==History== External rays were introduced in Douady and Hubbard's study of the Mandelbrot set. ==Types== Criteria for classification: Plane: parameter or dynamic Map Bifurcation of dynamic rays Stretching Landing ===Bifurcation=== Dynamic rays can be: Bifurcated, branched, broken Smooth, unbranched, unbroken When the filled Julia set is connected, there are no branching external rays. When the Julia set is not connected then some external rays branch. ===Stretching=== Stretching rays were introduced by Branner and Hubbard: "The notion of stretching rays is a generalization of that of external rays for the Mandelbrot set to higher degree polynomials." ===Landing=== Every rational parameter ray of the Mandelbrot set lands at a single parameter. ==Maps== ===Polynomials=== ====Dynamical plane = z-plane ==== External rays are associated to a compact, full, connected subset K\, of the complex plane as : the images of radial rays under the Riemann map of the complement of K\, the gradient lines of the Green's function of K\, field lines of Douady-Hubbard potential an integral curve of the gradient vector field of the Green's function on neighborhood of infinity External rays together with equipotential lines of Douady-Hubbard potential ( level sets) form a new polar coordinate system for exterior ( complement ) of K\, . In other words the external rays define vertical foliation which is orthogonal to horizontal foliation defined by the level sets of potential. =====Uniformization===== Let \Psi_c\, be the conformal isomorphism from the complement (exterior) of the closed unit disk \overline{\mathbb{D}} to the complement of the filled Julia set \ K_c . \Psi_c: \hat{\Complex} \setminus \overline{\mathbb{D}} \to \hat{\Complex} \setminus K_c where \hat{\Complex} denotes the extended complex plane. Let \Phi_c = \Psi_c^{-1}\, denote the Boettcher map. \Phi_c\, is a uniformizing map of the basin of attraction of infinity, because it conjugates f_c on the complement of the filled Julia set K_c to f_0(z)=z^2 on the complement of the unit disk: \begin{align} \Phi_c: \hat{\Complex} \setminus K_c &\to \hat{\Complex} \setminus \overline{\mathbb{D}}\\ z & \mapsto \lim_{n\to \infty} (f_c^n(z))^{2^{-n}} \end{align} and \Phi_c \circ f_c \circ \Phi_c^{-1} = f_0 A value w = \Phi_c(z) is called the Boettcher coordinate for a point z \in \hat{\Complex}\setminus K_c . =====Formal definition of dynamic ray===== The external ray of angle \theta\, noted as \mathcal{R}^K _{\theta} is: the image under \Psi_c\, of straight lines \mathcal{R}_{\theta} = \{\left(r\cdot e^{2\pi i \theta}\right) : \ r > 1 \} \mathcal{R}^K _{\theta} = \Psi_c(\mathcal{R}_{\theta}) set of points of exterior of filled-in Julia set with the same external angle \theta \mathcal{R}^K _{\theta} = \{ z\in \hat{\Complex} \setminus K_c : \arg(\Phi_c(z)) = \theta \} ======Properties====== The external ray for a periodic angle \theta\, satisfies: f(\mathcal{R}^K _{\theta}) = \mathcal{R}^K _{2 \theta} and its landing point \gamma_f(\theta) satisfies: f(\gamma_f(\theta)) = \gamma_f(2\theta) ====Parameter plane = c-plane ==== "Parameter rays are simply the curves that run perpendicular to the equipotential curves of the M-set." =====Uniformization===== as an image of unit circle under \Psi_M\, ]] of complement (exterior) of Mandelbrot set]] Let \Psi_M\, be the mapping from the complement (exterior) of the closed unit disk \overline{\mathbb{D}} to the complement of the Mandelbrot set \ M . \Psi_M:\mathbb{\hat{C}}\setminus \overline{\mathbb{D}}\to\mathbb{\hat{C}}\setminus M and Boettcher map (function) \Phi_M\, , which is uniformizing map of complement of Mandelbrot set, because it conjugates complement of the Mandelbrot set \ M and the complement (exterior) of the closed unit disk \Phi_M: \mathbb{\hat{C}}\setminus M \to \mathbb{\hat{C}}\setminus \overline{\mathbb{D}} it can be normalized so that : \frac{\Phi_M(c)}{c} \to 1 \ as\ c \to \infty \, where : \mathbb{\hat{C}} denotes the extended complex plane Jungreis function \Psi_M\, is the inverse of uniformizing map : \Psi_M = \Phi_{M}^{-1} \, In the case of complex quadratic polynomial one can compute this map using Laurent series about infinity c = \Psi_M (w) = w + \sum_{m=0}^{\infty} b_m w^{-m} = w -\frac{1}{2} + \frac{1}{8w} - \frac{1}{4w^2} + \frac{15}{128w^3} + ...\, where c \in \mathbb{\hat{C}}\setminus M w \in \mathbb{\hat{C}}\setminus \overline{\mathbb{D}} =====Formal definition of parameter ray===== The external ray of angle \theta\, is: the image under \Psi_c\, of straight lines \mathcal{R}_{\theta} = \{\left(r*e^{2\pi i \theta}\right) : \ r > 1 \} \mathcal{R}^M _{\theta} = \Psi_M(\mathcal{R}_{\theta}) set of points of exterior of Mandelbrot set with the same external angle \theta \mathcal{R}^M _{\theta} = \{ c\in \mathbb{\hat{C}}\setminus M : \arg(\Phi_M(c)) = \theta \} \Phi_M(c) \ \overset{\underset{\mathrm{def}}{}}{=} \ \Phi_c(z=c)\, so external angle of point c\, of parameter plane is equal to external angle of point z=c\, of dynamical plane ====External angle==== 2015-03-04 exray binary.gif|collecting bits outwards Binary decomposition.png|Binary decomposition of unrolled circle plane Binary decomposition of dynamic plane for f0(z) = z^2.png|binary decomposition of dynamic plane for f(z) = z^2 Angle is named external angle ( argument ). Principal value of external angles are measured in turns modulo 1 1 turn = 360 degrees = 2 × radians Compare different types of angles : external ( point of set's exterior ) internal ( point of component's interior ) plain ( argument of complex number ) =====Computation of external argument===== argument of Böttcher coordinate as an external argument \arg_M(c) = \arg(\Phi_M(c)) \arg_c(z) = \arg(\Phi_c(z)) kneading sequence as a binary expansion of external argument ===Transcendental maps=== For transcendental maps ( for example exponential ) infinity is not a fixed point but an essential singularity and there is no Boettcher isomorphism. Here dynamic ray is defined as a curve : connecting a point in an escaping set and infinity lying in an escaping set ==Images== ===Dynamic rays=== JuliaRay 1 3.png|Julia set for f_c(z) = z^2 -1 with 2 external ray landing on repelling fixed point alpha JuliaRay3.png|Julia set and 3 external rays landing on fixed point \alpha_c\, Dynamic internal and external rays .svg|Dynamic external rays landing on repelling period 3 cycle and 3 internal rays landing on fixed point \alpha_c\, Julia-p9.png|Julia set with external rays landing on period 3 orbit Parabolic rays landing on fixed point.ogv|Rays landing on parabolic fixed point for periods 2-40 Dynamical plane with branched periodic external ray 0 for map f(z) = z*z + 0.35.png| Branched dynamic ray ===Parameter rays=== Mandelbrot set for complex quadratic polynomial with parameter rays of root points File:Mandelbrot set for complex quadratic polynomial with parameter rays of root points.jpg|External rays for angles of the form : n / ( 2 1 - 1) (0/1; 1/1) landing on the point c= 1/4, which is cusp of main cardioid ( period 1 component) Image:Man2period.jpg|External rays for angles of the form : n / ( 2 2 - 1) (1/3, 2/3) landing on the point c= - 3/4, which is root point of period 2 component Image:Man3period.jpg|External rays for angles of the form : n / ( 2 3 - 1) (1/7,2/7) (3/7,4/7) landing on the point c= -1.75 = -7/4 (5/7,6/7) landing on the root points of period 3 components. Image:Man4period.jpg|External rays for angles of form : n / ( 2 4 - 1) (1/15,2/15) (3/15, 4/15) (6/15, 9/15) landing on the root point c= -5/4 (7/15, 8/15) (11/15,12/15) (13/15, 14/15) landing on the root points of period 4 components. Image:Man5period.jpg| External rays for angles of form : n / ( 2 5 - 1) landing on the root points of period 5 components Image:Mandel ie 1 3.jpg|internal ray of main cardioid of angle 1/3: starts from center of main cardioid c=0, ends in the root point of period 3 component, which is the landing point of parameter (external) rays of angles 1/7 and 2/7 Image:Iray.png|Internal ray for angle 1/3 of main cardioid made by conformal map from unit circle File:Smiley mini Mandelbrot set with external rays.png| Mini Mandelbrot set with period 134 and 2 external rays File:Part of parameter plane with external 5 rays landing on the Mandelbrot set.png File:One arm spiral - part of Mandelbrot set.png File:Mini Mandelbrot set period=68 with external rays.png File:Wakes near the period 3 island in the Mandelbrot set.png|Wakes near the period 3 island File:Wakes along the main antenna in the Mandelbrot set.png|Wakes along the main antenna Parameter space of the complex exponential family f(z)=exp(z)+c. Eight parameter rays landing at this parameter are drawn in black. ==Programs that can draw external rays== Mandel - program by Wolf Jung written in C++ using Qt with source code available under the GNU General Public License Java applets by Evgeny Demidov ( code of mndlbrot::turn function by Wolf Jung has been ported to Java ) with free source code ezfract by Michael Sargent, uses the code by Wolf Jung OTIS by Tomoki KAWAHIRA - Java applet without source code Spider XView program by Yuval Fisher YABMP by Prof. Eugene Zaustinsky for MS-DOS without source code DH_Drawer by Arnaud Chéritat written for Windows 95 without source code Linas Vepstas C programs for Linux console with source code Program Julia by Curtis T. McMullen written in C and Linux commands for C shell console with source code mjwinq program by Matjaz Erat written in delphi/windows without source code ( For the external rays it uses the methods from quad.c in julia.tar by Curtis T McMullen) RatioField by Gert Buschmann, for windows with Pascal source code for Dev-Pascal 1.9.2 (with Free Pascal compiler ) Mandelbrot program by Milan Va, written in Delphi with source code Power MANDELZOOM by Robert Munafo ruff by Claude Heiland-Allen ==See also== external rays of Misiurewicz point Orbit portrait Periodic points of complex quadratic mappings Prouhet-Thue-Morse constant Carathéodory's theorem Field lines of Julia sets ==References== Lennart Carleson and Theodore W. Gamelin, Complex Dynamics, Springer 1993 Adrien Douady and John H. Hubbard, Etude dynamique des polynômes complexes, Prépublications mathémathiques d'Orsay 2/4 (1984 / 1985) John W. Milnor, Periodic Orbits, External Rays and the Mandelbrot Set: An Expository Account; Géométrie complexe et systèmes dynamiques (Orsay, 1995), Astérisque No. 261 (2000), 277–333. (First appeared as a Stony Brook IMS Preprint in 1999, available as arXiV:math.DS/9905169.) John Milnor, Dynamics in One Complex Variable, Third Edition, Princeton University Press, 2006, Wolf Jung : Homeomorphisms on Edges of the Mandelbrot Set. Ph.D. thesis of 2002 ==External links== Hubbard Douady Potential, Field Lines by Inigo Quilez Intertwined Internal Rays in Julia Sets of Rational Maps by Robert L. Devaney Extending External Rays Throughout the Julia Sets of Rational Maps by Robert L. Devaney With Figen Cilingir and Elizabeth D. Russell John Hubbard's presentation, The Beauty and Complexity of the Mandelbrot Set, part 3.1 videos by ImpoliteFruit

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