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Notices of the American Mathematical Society June/July 2006
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STRONG REGULARITY 3 Ergodic Theorem Produces Lyapunov Exponents (W.R.T
STRONG REGULARITY by Pierre Berger and Jean-Christophe Yoccoz 1. Uniformly hyperbolic dynamical systems The theory of uniformly hyperbolic dynamical systems was constructed in the 1960’s under the dual leadership of Smale in the USA and Anosov and Sinai in the Soviet Union. It is nowadays almost complete. It encompasses various examples [Sma67]: expanding maps, horseshoes, solenoid maps, Plykin attractors, Anosov maps and DA, all of which are basic pieces. We recall standard definitions. Let f be a C1-diffeomorphism f of a finite dimen- sional manifold M. A compact f-invariant subset Λ ⊂ M is uniformly hyperbolic if the restriction to Λ of the tangent bundle TM splits into two continuous invariant subbundles TM|Λ= Es ⊕ Eu, Es being uniformly contracted and Eu being uniformly expanded. Then for every z ∈ Λ, the sets W s(z)= {z′ ∈ M : lim d(f n(z),f n(z′))=0}, n→+∞ W u(z)= {z′ ∈ M : lim d(f n(z),f n(z′))=0} n→−∞ are called the stable and unstable manifolds of z. They are immersed manifolds tangent at z to respectively Es(z) and Eu(z). s arXiv:1901.09430v1 [math.DS] 27 Jan 2019 The ǫ-local stable manifold Wǫ (z) of z is the connected component of z in the intersection of W s(z) with a ǫ-neighborhood of z. The ǫ-local unstable manifold u Wǫ (z) is defined likewise. Definition 1.1. — A basic set is a compact, f-invariant, uniformly hyperbolic set Λ which is transitive and locally maximal: there exists a neighborhood N of Λ such that n Λ= ∩n∈Zf (N). -
Quantum-Inspired Identification of Complex Cellular Automata
Quantum-inspired identification of complex cellular automata Matthew Ho,1, 2, ∗ Andri Pradana,1, y Thomas J. Elliott,3, 2, 1, z Lock Yue Chew,1, 2, x and Mile Gu1, 2, 4, { 1School of Physical and Mathematical Sciences, Nanyang Technological University, Singapore 637371, Singapore 2Complexity Institute, Nanyang Technological University, Singapore 637335, Singapore 3Department of Mathematics, Imperial College London, London SW7 2AZ, United Kingdom 4Centre for Quantum Technologies. National University of Singapore, 3 Science Drive 2, Singapore 117543, Singapore (Dated: March 29, 2021) Elementary cellular automata (ECA) present iconic examples of complex systems. Though de- scribed only by one-dimensional strings of binary cells evolving according to nearest-neighbour update rules, certain ECA rules manifest complex dynamics capable of universal computation. Yet, the classification of precisely which rules exhibit complex behaviour remains a significant challenge. Here we approach this question using tools from quantum stochastic modelling, where quantum statistical memory { the memory required to model a stochastic process using a class of quantum machines { can be used to quantify the structure of a stochastic process. By viewing ECA rules as transformations of stochastic patterns, we ask: Does an ECA generate structure as quantified by the quantum statistical memory, and if so, how quickly? We illustrate how the growth of this measure over time correctly distinguishes simple ECA from complex counterparts. Moreover, it provides a more refined means for quantitatively identifying complex ECAs { providing a spectrum on which we can rank the complexity of ECA by the rate in which they generate structure. t-1 We all have some intuition of complexity. -
DOUBLE STANDARD MAPS 1. Introduction It Is a Usual
DOUBLE STANDARD MAPS MICHALMISIUREWICZ AND ANA RODRIGUES Abstract. We investigate the family of double standard maps of the circle onto itself, given by fa,b(x) = 2x + a + (b/π) sin(2πx) (mod 1), where the parameters a, b are real and 0 ≤ b ≤ 1. Similarly to the well known family of (Arnold) standard maps of the circle, Aa,b(x) = x + a + (b/(2π)) sin(2πx) (mod 1), any such map has at most one attracting periodic orbit and the set of parameters (a, b) for which such orbit exists is divided into tongues. However, unlike the classical Arnold tongues, that begin at the level b = 0, for double standard maps the tongues begin at higher levels, depending on the tongue. Moreover, the order of the tongues is different. For the standard maps it is governed by the continued fraction expansions of rational numbers; for the double standard maps it is governed by their binary expansions. We investigate closer two families of tongues with different behavior. 1. Introduction It is a usual procedure that in order to understand the behavior of a system in higher dimension one investigates first a one-dimensional system that is somewhat similar. The classical example is the H´enonmap and similar systems, where a serious progress occurred only after unimodal interval maps have been thoroughly understood. Another example of this type was investigation by V. Arnold of the family of standard maps of the circle, given by the formula b (1.1) A (x) = x + a + sin(2πx) (mod 1) a,b 2π (when we write “mod 1,” we mean that both the arguments and the values are taken modulo 1). -
An Entire Transcendental Family with a Persistent Siegel Disk
An entire transcendental family with a persistent Siegel disk Rub´en Berenguel, N´uria Fagella March 12, 2009 Abstract We study the class of entire transcendental maps of finite order with one critical point and one asymptotic value, which has exactly one finite pre-image, and having a persistent Siegel disk. After normalization ∗ this is a one parameter family fa with a ∈ C which includes the semi- standard map λzez at a = 1, approaches the exponential map when a → 0 and a quadratic polynomial when a → ∞. We investigate the stable components of the parameter plane (capture components and semi-hyperbolic components) and also some topological properties of the Siegel disk in terms of the parameter. 1 Introduction Given a holomorphic endomorphism f : S → S on a Riemann surface S we consider the dynamical system generated by the iterates of f, denoted by n) n f = f◦ ··· ◦f. The orbit of an initial condition z0 ∈ S is the sequence + n O (z0)= {f (z0)}n N and we are interested in classifying the initial condi- ∈ tions in the phase space or dynamical plane S, according to the asymptotic behaviour of their orbits when n tends to infinity. There is a dynamically natural partition of the phase space S into the Fatou set F (f) (open) where the iterates of f form a normal family and the Julia set J (f)= S\F (f) which is its complement (closed). If S = C = C ∪∞ then f is a rational map. If S = C and f does not extend to the point at infinity, then f is an entire transcendental map, b that is, infinity is an essential singularity. -
Quantum Versus Classical Measures of Complexity on Classical Information
Quantum versus Classical Measures of Complexity on Classical Information Lock Yue Chew, PhD Division of Physics and Applied Physics School of Physical & Mathematical Sciences & Complexity Institute Nanyang Technological University Astronomical Scale Macroscopic Scale Mesoscopic Scale What is Complexity? • Complexity is related to “Pattern” and “Organization”. Nature inherently organizes; Pattern is the fabric of Life. James P. Crutchfield • There are two extreme forms of Pattern: generated by a Clock and a Coin Flip. • The former encapsulates the notion of Determinism, while the latter Randomness. • Complexity is said to lie between these extremes. J. P. Crutchfield and K. Young, Physical Review Letters 63, 105 (1989). Can Complexity be Measured? • To measure Complexity means to measure a system’s structural organization. How can that be done? • Conventional Measures: • Difficulty in Description (in bits) – Entropy; Kolmogorov-Chaitin Complexity; Fractal Dimension. • Difficulty in Creation (in time, energy etc.) – Computational Complexity; Logical Depth; Thermodynamic Depth. • Degree of organization – Mutual Information; Topological ϵ- machine; Sophistication. S. Lloyd, “Measures of Complexity: a Non-Exhaustive List”. Topological Ɛ-Machine 1. Optimal Predictor of the System’s Process 2. Minimal Representation – Ockham’s Razor 3. It is Unique. 4. It gives rise to a new measure of Complexity known as Statistical Complexity to account for the degree of organization. 5. The Statistical Complexity has an essential kind of Representational Independence. J. P. Crutchfield, Nature 8, 17 (2012). Concept of Ɛ-Machine Symbolic Sequences: ….. S-2S-1S0S1 ….. Futures : Past : • Within each partition, we have Partitioning the set 푺 of all histories into causal states 푆푖. where 푠 and 푠′ are two different individual histories in the same partition. -
Elliptic Bubbles in Moser's 4D Quadratic Map: the Quadfurcation
Elliptic Bubbles in Moser's 4DQuadratic Map: the Quadfurcation ∗ Arnd B¨ackery and James D. Meissz Abstract. Moser derived a normal form for the family of four-dimensional, quadratic, symplectic maps in 1994. This six-parameter family generalizes H´enon'subiquitous 2d map and provides a local approximation for the dynamics of more general 4D maps. We show that the bounded dynamics of Moser's family is organized by a codimension-three bifurcation that creates four fixed points|a bifurcation analogous to a doubled, saddle-center|which we call a quadfurcation. In some sectors of parameter space a quadfurcation creates four fixed points from none, and in others it is the collision of a pair of fixed points that re-emerge as two or possibly four. In the simplest case the dynamics is similar to the cross product of a pair of H´enonmaps, but more typically the stability of the created fixed points does not have this simple form. Up to two of the fixed points can be doubly-elliptic and be surrounded by bubbles of invariant two-tori; these dominate the set of bounded orbits. The quadfurcation can also create one or two complex-unstable (Krein) fixed points. Special cases of the quadfurcation correspond to a pair of weakly coupled H´enonmaps near their saddle-center bifurcations. Key words. H´enonmap, symplectic maps, saddle-center bifurcation, Krein bifurcation, invariant tori AMS subject classifications. 37J10 37J20 37J25 70K43 1. Introduction. Multi-dimensional Hamiltonian systems model dynamics on scales rang- ing from zettameters, for the dynamics of stars in galaxies [1, 2], to nanometers, in atoms and molecules [3, 4]. -
A Partial Justification of Greene's Criterion For
A PARTIAL JUSTIFICATION OF GREENE'S CRITERION FOR CONFORMALLY SYMPLECTIC SYSTEMS RENATO C. CALLEJA, ALESSANDRA CELLETTI, CORRADO FALCOLINI, AND RAFAEL DE LA LLAVE Abstract. Greene's criterion for twist mappings asserts the existence of smooth in- variant circles with preassigned rotation number if and only if the periodic trajectories with frequency approaching that of the quasi-periodic orbit are linearly stable. We formulate an extension of this criterion for conformally symplectic systems in any dimension and prove one direction of the implication, namely that if there is a smooth invariant attractor, we can predict the eigenvalues of the periodic orbits whose frequencies approximate that of the tori. The proof of this result is very different from the proof in the area preserving case, since in the conformally symplectic case the existence of periodic orbits requires adjusting parameters. Also, as shown in [13], in the conformally symplectic case there are no Birkhoff invariants giving obstructions to linearization near an invariant torus. As a byproduct of the techniques developed here, we obtain quantitative information on the existence of periodic orbits in the neighborhood of quasi-periodic tori and we provide upper and lower bounds on the width of the Arnold tongues in n-degrees of freedom conformally symplectic systems. Contents 1. Introduction 2 1.1. The Greene's criterion 2 1.2. Greene's criterion for conformally symplectic systems 3 1.3. Organization of the paper 6 2. Local behavior near rotational Lagrangian tori in conformally symplectic systems 6 2.1. Conformally symplectic systems 6 2.2. Local behavior in a neighborhood of a KAM torus 7 3. -
IPS Meeting 2015 4 - 6 March
IPS Meeting 2015 4 - 6 March Institute of Physics Singapore Conference Program (post-printed version, status: March 3, 2015, 17:00SGT) The IPS Meeting 2015 thanks its sponsors for their generous support Institutional Sponsors: SINGAPORE UNIVERSITY OF TECHNOLOGY AND DESIGN Established in collaboration with MIT 1 Foreword Dear fellow Physicists, this year we are back again to the School of Physical and Mathematical Sciences on the campus of Nanyang Technological University for our annual gathering of physicists active in research. For some of our colleagues, who come from their new campus of the Singapore University of Technology and Design (SUTD), this is probably as far as it gets - at least in Singapore. Some time ago, when the IPS council got together, we realized that the UNESCO had declared 2015 as the international year of light. As physicists, this is something many of us use in their daily work, so here was the theme for this year’s meeting. We felt that a focus session on precision measurements and Spectroscopy does fit very well this theme - and a lot of work is done on this topic in Singapore as well! This emphasis is also highlighted by plenary talks discussing exciting new developments in various realizations of precision measurements. It turned out that even one of our colleagues who works – among other topics – on black holes got noted widely for his work describing light paths around these objects - something that made it into a major Hollywood movie. So convinced Edward Teo to open the meeting with a plenary talk, explaining to us the exotic physics hidden in the movie. -
Bifurcations, Mode Locking, and Chaos in a Dissipative System
The Bogdanov Map: Bifurcations, Mode Locking, and Chaos in a Dissipative System David K. Arrowsmith, School of Mathematical Sciences Queen Mary and Westfield College University of London Mile End Road London E1 4NS, UK Julyan H. E. Cartwright, Departament de F´ısica Universitat de les Illes Balears 07071 Palma de Mallorca, Spain Alexis N. Lansbury, Department of Physics Brunel, The University of West London Uxbridge, Middlesex UB8 3PH, UK &ColinM.Place.∗ Int. J. Bifurcation and Chaos, 3,803–842,1993 We investigate the bifurcations and basins of attraction in the Bog- danov map, a planar quadratic map which is conjugate to the Henon´ area-preserving map in its conservative limit. It undergoesaHopf bifurcation as dissipation is added, and exhibits the panoply of mode locking, Arnold tongues, and chaos as an invariant circle grows out, finally to be destroyed in the homoclinic tangency of the manifolds of aremotesaddlepoint.TheBogdanovmapistheEulermapofatwo- dimensional system of ordinary differential equations firstconsidered by Bogdanov and Arnold in their study of the versal unfolding of the double-zero-eigenvalue singularity, and equivalently of avectorfield invariant under rotation of the plane by an angle 2π.Itisauseful system in which to observe the effect of dissipative perturbations on Hamiltonian structure. In addition, we argue that the Bogdanov map provides a good approximation to the dynamics of the Poincaremaps´ of periodically forced oscillators. ∗Formerly: Department of Mathematics, Westfield College, University of London, UK. 1 1. Introduction Tisnowwellknownthatthestudyofsystemsofordinarydifferential equations, which commonly arise in dynamical systems investigated in I many fields of science, can be aided by utilizing the surface-of-section technique of Poincaremaps.The´ Poincar´e or return map of a system of or- dinary differential equations reduces the dimension of the problem, replac- ing an n-dimensional set of ordinary differential equations with an (n 1)- dimensional set of difference equations. -
Table of Contents (Online, Part 2)
TM PERIODICALS PHYSICALREVIEWA Postmaster send address changes to: For editorial and subscription correspondence, please see inside front cover APS Subscription Services (ISSN: 2469-9926) P.O. Box 41 Annapolis Junction, MD 20701 THIRD SERIES, VOLUME 95, NUMBER 6 CONTENTS JUNE 2017 PARTS A AND B The Table of Contents is a total listing of Parts A and B. Part A consists of pages 060101(R)–062709, and Part B pages 063401–069908(E). PART A RAPID COMMUNICATIONS Fundamental concepts Peres experiment using photons: No test for hypercomplex (quaternionic) quantum theories (3 pages) .......... 060101(R) Stephen L. Adler Approximating local observables on projected entangled pair states (5 pages)................................ 060102(R) M. Schwarz, O. Buerschaper, and J. Eisert Atomic and molecular structure and dynamics One-loop electron self-energy for the bound-electron g factor (4 pages)..................................... 060501(R) V. A. Yerokhin and Z. Harman Atomic and molecular collisions and interactions Center-of-mass-momentum-dependent interaction between ultracold atoms (5 pages) ......................... 060701(R) Jianwen Jie and Peng Zhang Molecular-frame electron-scattering experiment on the dipole-forbidden 2σg → 1πg transition of N2 (5 pages) ..................................................................................... 060702(R) Noboru Watanabe, So Yamada, and Masahiko Takahashi Atomic and molecular processes in external fields, including interactions with strong fields and short pulses Simulation of field-induced molecular dissociation in atom-probe tomography: Identification of a neutral emission channel (6 pages) ................................................................................... 061401(R) David Zanuttini, Ivan Blum, Lorenzo Rigutti, François Vurpillot, Julie Douady, Emmanuelle Jacquet, Pierre-Matthieu Anglade, and Benoit Gervais X-ray versus Auger emission following Xe 1s photoionization (6 pages) .................................... 061402(R) M. N. -
5Th Workshop on Quantum Chaos and Localisation Phenomena
5th Workshop on Quantum Chaos and Localisation Phenomena May 20–22, 2011, Warsaw, Poland organised by Institute of Physics Polish Academy of Sciences, Center for Theoretical Physics Polish Academy of Sciences, and Pro Physica Foundation PROGRAMME Organising Committee Szymon Bauch ([email protected]) Sunday, May 22 Oleh Hul ([email protected]) INVITED TALKS Marek Kuś ([email protected]) 9:00–9:35 Uzy Smilansky (Rehovot, Israel) Michał Ławniczak ([email protected]) Stationary scattering from a nonlinear network Leszek Sirko – chairman ([email protected]) 9:35–10:10 Yan V. Fyodorov (Nottingham, UK) Level curvature distribution at the spectral edge of random Hermitian matrices 10:10–10:45 Pavel Kurasov (Stockholm, Sweden) Magnetic Schrödinger operators on graphs: spectra, Objectives inverse problems and applications 10:45–11:20 Karol Życzkowski (Warsaw, Poland) To assess achievements and to formulate directions of new research Level spacing distribution revisited on quantum chaos and localisation 11:20–11:50 coffee break To bring together prominent experimental and theoretical physicists 11:50–12:25 Andreas Buchleitner (Freiburg, Germany) who share a common interest in quantum chaos and localisation Transport, disorder, and entanglement phenomena 12:25–13:00 Jan Kˇríž (Hradec Králové, Czech Republic) Chaos in the brain 13:00–13:35 Agn`es Maurel (Paris, France) Experimental study of waves propagation using Fourier Transform Profilometry Scope 13:35–14:30 lunch break CONTRIBUTED TALKS Presentations will focus on the following topics: 14:30–14:50 Filip Studniˇcka (Hradec Králové, Czech Republic) Quantum chaos and nonlinear classical systems Analysis of biomedical signals using differential geometry invariants Quantum and microwave billiards 14:50–15:10 Michał Ławniczak (Warsaw, Poland) Quantum and microwave graphs Investigation of Wigner reaction matrix, cross- and velocity Atoms in strong electromagnetic fields – experiment and theory correlators for microwave networks Chaos vs.