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In mathematics, an orbit portrait is a combinatorial tool used in
complex dynamics Complex dynamics is the study of dynamical systems defined by iteration of functions on complex number spaces. Complex analytic dynamics is the study of the dynamics of specifically analytic functions. Techniques *General **Montel's theorem ** P ...
for understanding the behavior of one-complex dimensional quadratic maps. In simple words one can say that it is : * a list of external angles for which rays land on points of that orbit * graph showing above list


Definition

Given a quadratic map :f_c : z \to z^2 + c. from the complex plane to itself :f_c : \mathbb \to \mathbb and a repelling or parabolic periodic
orbit In celestial mechanics, an orbit is the curved trajectory of an object such as the trajectory of a planet around a star, or of a natural satellite around a planet, or of an artificial satellite around an object or position in space such as ...
= \ of f, so that f(z_j) = z_ (where subscripts are taken 1 + modulo n), let A_j be the set of
angles The Angles ( ang, Ængle, ; la, Angli) were one of the main Germanic peoples who settled in Great Britain in the post-Roman period. They founded several kingdoms of the Heptarchy in Anglo-Saxon England. Their name is the root of the name ...
whose corresponding
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 ...
s land at z_j. Then the set = () = \ is called the orbit portrait of the periodic orbit . All of the sets A_j must have the same number of elements, which is called the valence of the portrait.


Examples


Parabolic or repelling orbit portrait


valence 2

= \left \{\left( \frac{1}{3},\frac{2}{3} \right) \right \rbrace {\mathcal P} = \left \{ \left( \frac{3}{7} , \frac{4}{7} \right), \left( \frac{6}{7} , \frac{1}{7} \right), \left( \frac{5}{7} , \frac{2}{7} \right) \right \rbrace {\mathcal P} = \left \{ \left( \frac{4}{9} , \frac{5}{9} \right), \left( \frac{8}{9} , \frac{1}{9} \right), \left( \frac{7}{9} , \frac{2}{9} \right) \right \rbrace {\mathcal P} = \left \{ \left( \frac{11}{31} , \frac{12}{31} \right), \left( \frac{22}{31} , \frac{24}{31} \right), \left( \frac{13}{31} , \frac{17}{31} \right), \left( \frac{26}{31} , \frac{3}{31} \right), \left( \frac{21}{31} , \frac{6}{31} \right) \right \rbrace


valence 3

Valence is 3 so rays land on each orbit point. {\mathcal P} = \left \{ \left(\frac{1}{7},\frac{2}{7} ,\frac{4}{7}\right)\right \rbrace For
complex quadratic polynomial A complex quadratic polynomial is a quadratic polynomial whose coefficients and variable are complex numbers. Properties Quadratic polynomials have the following properties, regardless of the form: *It is a unicritical polynomial, i.e. it has on ...
with c= -0.03111+0.79111*i portrait of parabolic period 3 orbit is : {\mathcal P} = \left \{ \left(\frac{74}{511},\frac{81}{511},\frac{137}{511} \right) , \left(\frac{148}{511},\frac{162}{511},\frac{274}{511} \right) , \left(\frac{296}{511},\frac{324}{511},\frac{37}{511} \right) \right \rbrace Rays for above angles land on points of that orbit . Parameter c is a center of period 9 hyperbolic component of Mandelbrot set. For parabolic julia set c = -1.125 + 0.21650635094611*i. It is a root point between period 2 and period 6 components of Mandelbrot set. Orbit portrait of period 2 orbit with valence 3 is : {\mathcal P} = \left \{ \left(\frac{22}{63},\frac{25}{63},\frac{37}{63} \right) , \left(\frac{11}{63},\frac{44}{63},\frac{50}{63} \right) \right \rbrace


valence 4

{\mathcal P} = \left \{ \left(\frac{1}{15},\frac{2}{15} ,\frac{4}{15} ,\frac{8}{15} \right) \right \rbrace


Formal orbit portraits

Every orbit portrait {\mathcal P} has the following properties: *Each A_j is a finite subset of {\mathbb R} / {\mathbb Z} *The doubling map on the circle gives a bijection from A_j to A_{j+1} and preserves cyclic order of the angles. *All of the angles in all of the sets A_1, \ldots, A_n are periodic under the doubling map of the circle, and all of the angles have the same exact period. This period must be a multiple of n, so the period is of the form rn, where r is called the recurrent ray period. *The sets A_j are pairwise unlinked, which is to say that given any pair of them, there are two disjoint intervals of {\mathbb R }/ {\mathbb Z} where each interval contains one of the sets. Any collection \{A_1, \ldots, A_n\} of subsets of the circle which satisfy these four properties above is called a formal orbit portrait. It is a theorem of
John Milnor John Willard Milnor (born February 20, 1931) is an American mathematician known for his work in differential topology, algebraic K-theory and low-dimensional holomorphic dynamical systems. Milnor is a distinguished professor at Stony Brook Univ ...
that every formal orbit portrait is realized by the actual orbit portrait of a periodic orbit of some quadratic one-complex-dimensional map. Orbit portraits contain dynamical information about how external rays and their landing points map in the plane, but formal orbit portraits are no more than combinatorial objects. Milnor's theorem states that, in truth, there is no distinction between the two.


Trivial orbit portraits

Orbit portrait where all of the sets A_j have only a single element are called trivial, except for orbit portrait . An alternative definition is that an orbit portrait is nontrivial if it is maximal, which in this case means that there is no orbit portrait that strictly contains it (i.e. there does not exist an orbit portrait \{A^\prime_1,\ldots,A^\prime_n\} such that A_j \subsetneq A^\prime_j). It is easy to see that every trivial formal orbit portrait is realized as the orbit portrait of some orbit of the map f_0(z) = z^2, since every external ray of this map lands, and they all land at distinct points of the
Julia set In the context of complex dynamics, a branch of mathematics, the Julia set and the Fatou set are two complementary sets (Julia "laces" and Fatou "dusts") defined from a function. Informally, the Fatou set of the function consists of values wi ...
. Trivial orbit portraits are pathological in some respects, and in the sequel we will refer only to nontrivial orbit portraits.


Arcs

In an orbit portrait \{A_1, \ldots, A_n\}, each A_j is a finite subset of the circle \mathbb R / \mathbb Z, so each A_j divides the circle into a number of disjoint intervals, called complementary arcs based at the point z_j. The length of each interval is referred to as its angular width. Each z_j has a unique largest arc based at it, which is called its critical arc. The critical arc always has length greater than \frac 1 2 These arcs have the property that every arc based at z_j, except for the critical arc, maps diffeomorphically to an arc based z_{j+1}, and the critical arc covers every arc based at z_{j+1} once, except for a single arc, which it covers twice. The arc that it covers twice is called the critical value arc for z_{j+1}. This is not necessarily distinct from the critical arc. When c escapes to infinity under iteration of f_c, or when c is in the Julia set, then c has a well-defined external angle. Call this angle \theta_c. \theta_c is in every critical value arc. Also, the two inverse images of c under the doubling map (\frac {\theta_c} 2 and \frac {\theta_c + 1} 2) are both in every critical arc. Among all of the critical value arcs for all of the A_j's, there is a unique smallest critical value arc {\mathcal I}_{\mathcal P}, called the characteristic arc which is strictly contained within every other critical value arc. The characteristic arc is a complete invariant of an orbit portrait, in the sense that two orbit portraits are identical if and only if they have the same characteristic arc.


Sectors

Much as the rays landing on the orbit divide up the circle, they divide up the complex plane. For every point z_j of the orbit, the
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 ...
s landing at z_j divide the plane into v open sets called sectors based at z_j. Sectors are naturally identified the complementary arcs based at the same point. The angular width of a sector is defined as the length of its corresponding complementary arc. Sectors are called critical sectors or critical value sectors when the corresponding arcs are, respectively, critical arcs and critical value arcs. Sectors also have the interesting property that 0 is in the critical sector of every point, and c, the
critical value Critical value may refer to: *In differential topology, a critical value of a differentiable function between differentiable manifolds is the image (value of) ƒ(''x'') in ''N'' of a critical point ''x'' in ''M''. *In statistical hypothesis ...
of f_c, is in the critical value sector.


Parameter wakes

Two parameter rays with angles t_- and t_+ land at the same point of the
Mandelbrot set The Mandelbrot set () is the set of complex numbers c for which the function f_c(z)=z^2+c does not diverge to infinity when iterated from z=0, i.e., for which the sequence f_c(0), f_c(f_c(0)), etc., remains bounded in absolute value. This ...
in parameter space if and only if there exists an orbit portrait \mathcal P with the interval _-, t_+/math> as its characteristic arc. For any orbit portrait \mathcal P let r_{\mathcal P} be the common landing point of the two external angles in parameter space corresponding to the characteristic arc of \mathcal P. These two parameter rays, along with their common landing point, split the parameter space into two open components. Let the component that does not contain the point 0 be called the \mathcal P-wake and denoted as {\mathcal W}_{\mathcal P}. A
quadratic polynomial In mathematics, a quadratic polynomial is a polynomial of degree two in one or more variables. A quadratic function is the polynomial function defined by a quadratic polynomial. Before 20th century, the distinction was unclear between a polynomial ...
f_c(z) = z^2 + c realizes the orbit portrait {\mathcal P} with a repelling orbit exactly when c \in {\mathcal W}_{\mathcal P}. {\mathcal P} is realized with a parabolic orbit only for the single value c= r_{\mathcal P} for about


Primitive and satellite orbit portraits

Other than the zero portrait, there are two types of orbit portraits: primitive and satellite. If v is the valence of an orbit portrait \mathcal P and r is the recurrent ray period, then these two types may be characterized as follows: * Primitive orbit portraits have r = 1 and v = 2. Every ray in the portrait is mapped to itself by f^n. Each A_j is a pair of angles, each in a distinct orbit of the doubling map. In this case, r_{\mathcal P} is the base point of a baby Mandelbrot set in parameter space. * Satellite orbit portraits have r = v \ge 2. In this case, all of the angles make up a single orbit under the doubling map. Additionally, r_{\mathcal P} is the base point of a parabolic bifurcation in parameter space.


Generalizations

Orbit portraits turn out to be useful combinatorial objects in studying the connection between the dynamics and the parameter spaces of other families of maps as well. In particular, they have been used to study the patterns of all periodic dynamical rays landing on a periodic cycle of a unicritical anti-holomorphic polynomial.


See also

*
Lamination Lamination is the technique/process of manufacturing a material in multiple layers, so that the composite material achieves improved strength, stability, sound insulation, appearance, or other properties from the use of the differing materia ...


References

{{Reflist Dynamical systems