W&M ScholarWorks Arts & Sciences Articles Arts and Sciences 2003 Geometry and topology of Escape II, Homotopic lobe dynamics K. A. Mitchell J. P. Handley J. B. Delos Stephen Knudson Follow this and additional works at: https://scholarworks.wm.edu/aspubs Part of the Physics Commons Geometry and topology of escape. II. Homotopic lobe dynamics Cite as: Chaos 13, 892 (2003); https://doi.org/10.1063/1.1598312 Submitted: 01 October 2002 . Accepted: 17 June 2003 . Published Online: 15 August 2003 K. A. Mitchell, J. P. Handley, J. B. Delos, and S. K. Knudson ARTICLES YOU MAY BE INTERESTED IN Geometry and topology of escape. I. Epistrophes Chaos: An Interdisciplinary Journal of Nonlinear Science 13, 880 (2003); https:// doi.org/10.1063/1.1598311 Isotope effect on bifurcating reaction path: Valley–ridge inflection point in totally symmetric coordinate The Journal of Chemical Physics 113, 477 (2000); https://doi.org/10.1063/1.481826 The separation of the reaction coordinate in transition state theory: Regularity and dimensionality reduction resulting from local symmetry The Journal of Chemical Physics 150, 164310 (2019); https://doi.org/10.1063/1.5092859 Chaos 13, 892 (2003); https://doi.org/10.1063/1.1598312 13, 892 © 2003 American Institute of Physics. CHAOS VOLUME 13, NUMBER 3 SEPTEMBER 2003 Geometry and topology of escape. II. Homotopic lobe dynamics K. A. Mitchell,a) J. P. Handley, and J. B. Delosb) Department of Physics, College of William and Mary, Williamsburg, Virginia 23187-8795 S. K. Knudson Department of Chemistry, College of William and Mary, Williamsburg, Virginia 23187-8795 ͑Received 1 October 2002; accepted 17 June 2003; published 15 August 2003͒ We continue our study of the fractal structure of escape-time plots for chaotic maps. In the preceding paper, we showed that the escape-time plot contains regular sequences of successive escape segments, called epistrophes, which converge geometrically upon each end point of every escape segment. In the present paper, we use topological techniques to: ͑1͒ show that there exists a minimal required set of escape segments within the escape-time plot; ͑2͒ develop an algorithm which computes this minimal set; ͑3͒ show that the minimal set eventually displays a recursive structure governed by an ‘‘Epistrophe Start Rule:’’ a new epistrophe is spawned ⌬ϭDϩ1 iterates after the segment to which it converges, where D is the minimum delay time of the complex. © 2003 American Institute of Physics. ͓DOI: 10.1063/1.1598312͔ Topological methods and symbolic dynamics have long map required for a point to escape the complex, plotted as a been valuable tools for describing orbits of dynamical function along the line of initial conditions ͑Fig. 2͒. For cha- systems. For example, if a particle in the plane scatters otic systems, such escape-time plots have a complicated set from three fixed disks, labeled A, B, and C, its orbit can of singularities and structure at all levels of resolution.2–16 be characterized by a sequence of symbols, such as These fractal escape-time plots play a central role in a variety ...ABA*BCBCA..., giving the sequence of collisions of classical decay and scattering problems; we have been with the disks. The asterisk gives the location of the par- particularly motivated by the ionization of atoms, especially ticle at the present time; as time goes by the asterisk hydrogen in parallel electric and magnetic fields. takes one step to the right. In this paper, we describe a The escape-time plot of a discrete map is divided into new kind of symbolic dynamics, in which the symbol se- ‘‘escape segments,’’ intervals over which the escape time is quence describes the structure of a curve in the plane. constant. In Paper I, we proved that there exist certain im- The relevant curve is not the trajectory of a particle, but portant sequences of consecutive escape segments, which we rather an ensemble of initial points in phase space—the called epistrophes, at all levels of resolution. The epistrophes line of initial conditions. This line winds around ‘‘holes’’ are characterized by the Epistrophe Theorem, whose core in the plane in a manner described by the symbol se- results are: ͑1͒ each end point of an escape segment spawns quence. The dynamical map applied to the line induces a a new epistrophe which converges upon it; ͑2͒ in the limit !ϱ map on the symbol sequence, which is more complicated ni , every epistrophe converges geometrically, with rate than a simple shift. We use this symbolic dynamics to equal to the Liapunov factor ␣ of the X point; ͑3͒ the derive properties of the epistrophes introduced in the asymptotic tails of any two epistrophes differ by a simple preceding paper. In particular, we use it to obtain a scaling. ‘‘minimal set of escape segments’’ and an ‘‘epistrophe The focus of Paper I was the asymptotic behavior of start rule.’’ epistrophes. In the present paper, we address how epistro- phes begin. We use the topological structure of the ho- moclinic tangle and the line of initial conditions to show that I. INTRODUCTION there is a certain minimal set of escape segments. For this minimal set, we prove the Epistrophe Start Rule ͑Theorem 1 As in the preceding paper ͑Paper I͒, we study maps of 1͒, which says that after a sufficiently large time, each epis- the phase plane, having an unstable fixed point ͑an X point͒ trophe begins some number of iterates ⌬ after the segment and an associated homoclinic tangle of stable and unstable that spawned it ͑i.e., the segment upon which the epistrophe manifolds ͑Fig. 1͒. The stable and unstable manifolds inter- converges͒. The number ⌬ is the same for all epistrophes of sect transversely, bounding a region of phase space ͑called a given map and is dependent on the topological structure of the ‘‘complex’’͒ from which a trajectory may or may not the tangle; explicitly, ⌬ϭDϩ1, where D is the minimum escape. We consider an initial distribution of points along a delay time of the complex, that is, the minimum number of curve passing through the complex ͑the line of initial condi- iterates a scattering trajectory spends inside the complex. tions͒. The escape-time plot is the number of iterates of the The bulk of our effort is devoted to developing an algebraic algorithm for constructing the minimal set of escape seg- a͒Electronic mail: [email protected] ments for a general line of initial conditions. This algorithm b͒Electronic mail: [email protected] allows us to compute the initial structure of the escape-time 1054-1500/2003/13(3)/892/11/$20.00892 © 2003 American Institute of Physics Chaos, Vol. 13, No. 3, 2003 Geometry and topology of escape. II 893 of symbolic dynamics which we call ‘‘homotopic lobe dy- namics.’’ From the symbol sequence, one can readily read off the structure of the minimal set of escape segments. Lines with different symbol sequences may have different minimal sets; however, at long enough times, these minimal sets al- ways obey the Epistrophe Start Rule. Some escape segments, such as that marked with an as- terisk in Fig. 2, are not within the minimal set guaranteed by the topology. These segments are ‘‘surprises’’ which, within the present topological analysis, we cannot predict. Since they break the regular structure and since they often have no obvious connection with any of the epistrophes, we call them ‘‘strophes’’ as in Sec. III B of Paper I. Strophes interfere with the self-similar structure of the fractal and typically do not go away in the asymptotic limit, resulting in what we called FIG. 1. A phase space portrait is shown for our saddle-center map, which ‘‘epistrophic self-similarity’’ in Sec. III C of Paper I. Despite L possesses a homoclinic tangle. The line of initial conditions 0 coincides the presence of these strophes, the minimal set often seems with qϭ1.72. to accurately describe the early and intermediate time struc- ture of the escape-time plot. Patterns similar to our Epistrophe Start Rule have been plot for iterates before the Epistrophe Start Rule sets in. The seen in other work. In the numerical study of Tiyapan and algorithm is then used to prove the Epistrophe Start Rule Jaffe´,14 epistrophes and the Epistrophe Start Rule are evident itself. in the structure of the initial angle-final action plot ͑analo- A critical aspect of this paper is our use of homotopy gous to the escape-time plot͒. Similarly, Jung and theory. We develop the necessary formalism in Sec. III, and co-workers9–11 used symbolic dynamics to construct a tree- prior knowledge of homotopy theory is not required. Homo- diagram that gives a comparable description of a scattering topy theory provides an algebraic framework for describing system. In each case, the authors consider a specific line of the topological structure of curves in the phase plane. As we initial conditions that is far outside of the complex and is shall explain, the phase plane has a set of ‘‘holes’’ into which topologically simple. Easton,17 followed by Rom-Kedar and the line of initial conditions cannot pass. A symbol sequence others,18–20 showed that recursive patterns also apply to ho- can be used to describe how the line circumvents these holes. moclinic intersections between the stable and unstable mani- As the dynamics maps the line forward, there is an induced folds. Thus, it may not be surprising that comparable patterns dynamics on the symbol sequence, representing a new kind should apply to the intersections between the stable manifold and an arbitrary line of initial conditions, at least at suffi- ciently large iterate. But at what iterate does this pattern set in, and what is the minimal set before it sets in? Algorithm 1 answers both these questions, as well as giving a simple proof of the Epistrophe Start Rule.