Quantum Versus Classical Measures of Complexity on Classical Information

Total Page:16

File Type:pdf, Size:1020Kb

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. • Equation (1) is related to sub- tree similarity discussed later. J. P. Crutchfield and C. R. Shalizi, Physical Review E 59, 275 (1999). Ɛ Machine - Preliminary • In physical processes, measurements are taken as time evolution of the system. • The time series is converted into a sequence of symbols s = s1, s2, . , si, . at time interval τ. ε • Measurement phase space M is segmented or partitioned into cells of size ε. • Each cell can be assigned a label leading to a list of alphabets A = {0, 1, 2, … k -1}. • Then, each si ϵ A. Ɛ-Machine – Reconstruction S = 0, 0, 1, 0, 0, 1, 0, 0, 1, 0, 0, 1, ….. • From symbol sequence -> build a tree structure with nodes and links . Period-3 sequence 0 1 • The links are given symbols according to the symbol sequence with A = {0, 1}. 0 1 0 1 0 0 0 0 1 0 1 0 1 0 0 0 0 1 0 1 0 1 0 0 1 Ɛ-Machine – Reconstruction 0 1 2 3 1 0 1 2 0 1 Level 1 2 0 1 3 0 4 3 Level 2 1 4 3 5 0 0 1 4 3 Level 3 0 3 5 4 0 1 0 5 3 5 0 4 3 1 0 0 4 3 5 5 4 1 0 0 3 5 4 0 0 1 5 0 4 3 1 0 4 1 3 5 0 0 Ɛ-Machine – Reconstruction S = 0, 0, 1, 0, 0, 1, 0, 0, 1, 0, 0, 1, ….. Probabilistic Structure 1 0 ( p = 2/3) 1 ( p = 1/3) Based on Orbit 1 ( p = 1/2) Ensemble 2 3 1 ( p = 1) 0 ( p = 1/2) 0 ( p = 1) 4 5 0 ( p = 1) Combination of both deterministic and random But the Probabilistic Structure computational resources is transient. Ɛ-Machine – Simplest Cases All Head or All “1” Process Purely Random Process s = 1, 1, 1, 1, 1, 1, ….. Fair Coin Process 1 ( p = 1/2) 1 ( p = 1) 0 ( p = 1/2) • These are the extreme cases of Complexity. • They are structurally simple. • We expect their Complexity Measure to be zero. Ɛ-Machine: Complexity from Deterministic Dynamics • The Symbol Sequence is derived from the Logistic Map. • The parameter r is set to the band merging regime r = 3.67859 … • For a finite sequence, a tree length Tlen and a machine length Mlen need to be defined. 3 푇푛 3-level sub-tree of n contains all nodes that can be reached within 3 links The Logistic Map Logistic equation : 푥푛+1 = 푟푥푛 1 − 푥푛 Starts period-doubling; at 푟 = 3 : period-2 Chaotic at 푟 = 3.569946… 0, 푥푖 < 0.5 Partitioning : 푠푖 = 1, 푥푖 ≥ 0.5 Ɛ-Machine: Complexity from Deterministic Dynamics Construction of ε-machine: 1 Transitions Sub-tree Similarity Level 1 2 1 LevelSub 2 -tree 3 2 1 Similarity Level 3 2 2 3 2 1 Ɛ-Machine: Complexity from Deterministic Dynamics Transitions Transient State Ɛ-Machine: Complexity from Deterministic Dynamics s = 1,0,1,1,1,0,1,… • The ε-machine captures the patterns of the process. Ɛ-Machine: Causal State Splitting Reconstruction Total = 9996 P(0|*) A P(1|*) = 3309/9996 = 6687/9996 ≈ 0.33 0 1 ≈ 0.67 P(0|*0) 0 C B 1 P(1|*1) = 1654/3309 = 5032/6687 ≈ 0.5 1 ≈ 0.75 P(1|*0) 0 P(0|*1) =1655/3309 = 1655/6687 C ≈ 0.5 D C ≈ 0.25 A P(1|*11) P(0|*00) P(1|*00) P(0|*01) 0 1 0 ≈ 0.67 ≈ 0.51 ≈ 0.49 = 0 1 P(1|*01) P(1|*10) P(0|*10) 0 1 = 1 ≈ 0.51 P(0|*11) ≈ 0.49 1 0 ≈ 0.33 C D C C D C B P(0|*000) P(1|*111) ≈ 0.49 P(0|*001) P(0|*010) P(0|*011) P(1|*100) P(1|*110) ≈ 0 ≈ 0 ≈ 0.49 ≈ 0.49 ≈ 0.51 ≈ 0.75 0 1 P(0|*101) 0 1 0 1 0 1 0 1 ≈ 0 0 1 0 1 0 1 P(0|*111) P(1|*000) P(1|*001) P(1|*010) P(1|*011) P(0|*100) P(1|*101) P(0|*110) ≈ 0.25 ≈ 0.51 ≈ 1 ≈ 0 ≈ 0.51 ≈ 0.51 ≈ 1 ≈ 0.49 C. R. Shalizi, K. L. Shalizi and J. P. Crutchfield, arXiv preprint cs/0210025. Ɛ-Machine: Causal State Splitting Reconstruction -The Even Process 1 ( p = 0.67) A B 1 ( p = 0.75) 0 ( p = 0.33) 0 ( p = 0.25) C 0 ( p = 0.5) 1 ( p = 0.5) 1 ( p = 1) D Statistical Complexity and Metric Entropy • Statistical Complexity is defined as C p log2 p Bits It serves to measure the computational resources required to reproduce a data stream. • Metric Entropy is defined as 1 m m h ps log2 ps Bits/Symbols m sm It serves to measure the diversity of observed patterns in a data stream. J. P. Crutchfield, Nature Physics 8, 17 (2012). The Logistic Map Linear region in the periodic window Decreasing trend at chaotic region Phase transition, 퐻∗ ≈ 0.28 : “edge of chaos” The Arc-Fractal Systems The Arc-Fractal Systems The Arc-Fractal Systems Out-Out (Levy): Out-In (Heighway): Out-In-Out (Crab): In-Out-In (Arrowhead): The Arc-Fractal Systems Sequence -> each arc is given an index according to its angle of orientation -> Sequence : 11,7,3 Out-In-Out rule, level 3 of construction: 7,3,11,7,11,3,11,7,3,11,3,7,11,7,3,7,11,3,11,7,3,11,3,7,3,11,7 In base-3: 1,0,2,1,2,0,2,1,0,2,0,1,2,1,0,1,2,0,2,1,0,2,0,1,0,2,1 The Arc-Fractal Systems • The fractals generated by the arc-fractal systems can be associated with symbolic sequences1,2. 1H. N. Huynh and L. Y. Chew, Fractals 19, 141 (2011). 2H. N. Huynh, A. Pradana and L. Y. Chew, PLoS ONE 10(2), e0117365 (2015) The Arc-Fractal Systems H. N. Huynh, A. Pradana and L. Y. Chew, PLoS ONE 10(2), e0117365 (2015) Complex Symbolic Sequence and Neuro- behavior Quantum Ɛ-Machine (1) T1,3 General Classical ε-Machine (0) (1) T1,3 (1) T1,2 T2,3 (0) (0) (0) T1,1 T1,2 T2,3 (0) S (1) (0) S (1) S1 T2,2 2 T2,2 T3,3 3 T3,3 Sn T (0) 1,1 T (0) T (0) 2,1 3,2 Causal State of Quantum ε- Machine (1) (1) T T n 1 2,1 T (0) 3,2 (r) 3,1 S j Tj,k r k k1 r0 (1) T3,1 for j 1,2,,n M. Gu, K. Wiesner, E. Rieper and V. Vedral, Nature Communications 3, 762 (2012) Quantum Complexity Quantum Causal State : C p log2 pfor Quantum Complexity : Cq Tr log Bits where the density matrix pi S i S i and pi is the i n 1 (r) probability of the quantum causal state Si . S j Tj,k r k k1 r0 Note that C C Bits q where j 1,2,,n R. Tan, D. R. Terno, J. Thompson, V. Vedral and M. Gu, European Physical Journal Plus 129(9), 1-10 (2014) Quantum versus Classical Complexity The Logistic Map 6 C 5 Cq 4 3 Complexity 2 1 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0 H(16)/16 Ɛ-Machine at Point 1 – Edge of Chaos R 3.569946.... C 5.480236 Cq 5.376835 Ɛ-Machine at Point 2 – Chaotic Region R 3.715 C 3.341681 Cq 3.093695 Ɛ-Machine at Point 3 – Chaotic Region R 3.960 C 1.364846 Cq 0.906989 Quantum Ɛ-Machine -Change of Measurement Basis General Qubit Measurement Basis: (1) T1,2 1 a 0 b 1 * * S2 S1 b 0 a 1 (0) T2,1 1 where and are new orthogonal measurement basis such that: S1 1 2 * 0 a b S2 0 1 1 b* a Quantum Ɛ-Machine -Change of Measurement Basis * S1 b 2 a 2 * S2 a 1 b 1 ( ) 2 T1,2 b S1 Deterministic ε - Machine ( ) 2 T1,2 a S2 Stochastic ε - Machine ( ) 2 T2,1 b ( ) 2 T2,1 a Quantum Ɛ-Machine -Change of Measurement Basis (1) T1,2 q0 (0) (1) T1,1 1 q0 S2 T2,2 1 q1 (0) S1 T1,2 q1 Stochastic ε - Machine S1 1 q0 0 1 q0 1 2 S2 q1 0 1 1 q1 1 2 Quantum Ɛ-Machine -Change of Measurement Basis * * S1 1 q0 a 1 q0 b 2 1 q0 b 1 q0 a 2 * * S2 q1 a 1 1 q1 b 2 q1 b 1 1 q1 a 2 If the quantum ε – machine is prepared in the quantum causal state S1 and measurement yields , the quantum ε – machine now possesses the causal state: * * 1 q0 a S1 q0 b S2 which is a superposition of the quantum resource.
Recommended publications
  • Notices of the American Mathematical Society June/July 2006
    of the American Mathematical Society ... (I) , Ate._~ f.!.o~~Gffi·u.­ .4-e.e..~ ~~~- •i :/?I:(; $~/9/3, Honoring J ~ rt)d ~cLra-4/,:e~ o-n. /'~7 ~ ~<A at a Gift from fL ~ /i: $~ "'7/<J/3. .} -<.<>-a.-<> ~e.Lz?-1~ CL n.y.L;; ro'T>< 0 -<>-<~:4z_ I Kumbakonam li .d. ~ ~~d a. v#a.d--??">ovt<.·c.-6 ~~/f. t:JU- Lo,.,do-,......) ~a page 640 ~!! ?7?.-L ..(; ~7 Ca.-uM /3~~-d~ .Y~~:Li: ~·e.-l a:.--nd '?1.-d- p ~ .di.,r--·c/~ C(c£~r~~u . J~~~aq_ f< -e-.-.ol ~ ~ ~/IX~ ~ /~~ 4)r!'a.. /:~~c~ •.7~ The Millennium Grand Challenge .(/.) a..Lu.O<"'? ...0..0~ e--ne_.o.AA/T..C<.r~- /;;; '7?'E.G .£.rA-CLL~ ~ ·d ~ in Mathematics C>n.A..U-a.A-d ~~. J /"-L .h. ?n.~ ~?(!.,£ ~ ~ &..ct~ /U~ page 652 -~~r a-u..~~r/a.......<>l/.k> 0?-t- ~at o ~~ &~ -~·e.JL d ~~ o(!'/UJD/ J;I'J~~Lcr~~ 0 ??u£~ ifJ>JC.Qol J ~ ~ ~ -0-H·d~-<.() d Ld.orn.J,k, -F-'1-. ~- a-o a.rd· J-c~.<-r:~ rn-u-{-r·~ ~'rrx ~~/ ~-?naae ~~ a...-'XS.otA----o-n.<l C</.J.d:i. ~~~ ~cL.va- 7 ??.L<A) ~ - Ja/d ~~ ./1---J- d-.. ~if~ ~0:- ~oj'~ t1fd~u: - l + ~ _,. :~ _,. .~., -~- .. =- ~ ~ d.u. 7 ~'d . H J&."dIJ';;;::. cL. r ~·.d a..L- 0.-n(U. jz-o-cn-...l- o~- 4; ~ .«:... ~....£.~.:: a/.l~!T cLc.·£o.-4- ~ d.v. /-)-c~ a;- ~'>'T/JH'..,...~ ~ d~~ ~u ~­ ~ a..t-4. l& foLk~ '{j ~~- e4 -7'~ -£T JZ~~c~ d.,_ .&~ o-n ~ -d YjtA:o ·C.LU~ ~or /)-<..,.,r &-.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • Session Chair
    SESSION CHAIR CHEW LOCK YUE School of Physical and Mathematical Sciences, Nanyang Technological University Lock Yue Chew is a theoretical physicist with research interest in the physics of complex systems. The main theme of his research centers on uncovering the organizing principles of complex systems based on the approach of statistical and nonlinear physics. The interdisciplinary research of his group investigates into the self-organization, pattern formation, synchronization, co-operation, competition, phase transition, chaos, and fractal properties of diverse biological, physical, and social complex systems. The elucidation of the emergent properties and underlying mechanisms of these systems, which is typically far from thermodynamic equilibrium, is of interest. Specific research interests include: (1) protein secondary-structure phase transition and the phenomenon of protein aggregation related to the prion and Alzheimer’s disease; (2) quantum entanglement dynamics and its links to quantum chaos; (3) scaling behavior of self-organized criticality in fractal lattices. Recently, he has also embarked active research on the problem of regimes shift in coupled social-ecological systems, statistical physics of urban dynamics, stochastic physics of elementary biological processes, and information theoretical approaches to the characterization of complex systems. He received his B. Eng. (Hons) and M.Sc. in Electrical Engineering from the National University of Singapore and University of Southern California, USA, respectively. He received his PhD in Physics from the National University of Singapore. He is an associate professor in the School of Physical and Mathematical Sciences (Division of Physics and Applied Physics), and an associated member with the Complexity Institute, of Nanyang Technological University. .
    [Show full text]
  • The Effect of Spin Squeezing on the Entanglement Entropy of Kicked Tops
    entropy Article The Effect of Spin Squeezing on the Entanglement Entropy of Kicked Tops Ernest Teng Siang Ong 1,† and Lock Yue Chew 1,2,*,† 1 Division of Physics and Applied Physics, School of Physical and Mathematical Sciences, Nanyang Technological University, 21 Nanyang Link, Singapore 637371, Singapore; [email protected] 2 Complexity Institute, Nanyang Technological University, 18 Nanyang Drive, Singapore 637723, Singapore * Correspondence: [email protected]; Tel.: +65-6316-2968 or +65-6795-7981 † These authors contributed equally to this work. Academic Editors: Gerardo Adesso and Jay Lawrence Received: 20 November 2015; Accepted: 22 March 2016; Published: 2 April 2016 Abstract: In this paper, we investigate the effects of spin squeezing on two-coupled quantum kicked tops, which have been previously shown to exhibit a quantum signature of chaos in terms of entanglement dynamics. Our results show that initial spin squeezing can lead to an enhancement in both the entanglement rate and the asymptotic entanglement for kicked tops when the initial state resides in the regular islands within a mixed classical phase space. On the other hand, we found a reduction in these two quantities if we were to choose the initial state deep inside the chaotic sea. More importantly, we have uncovered that an application of periodic spin squeezing can yield the maximum attainable entanglement entropy, albeit this is achieved at a reduced entanglement rate. Keywords: quantum entanglement; chaos; quantum squeezing 1. Introduction The quantum kicked top is an important model for the fundamental study of quantum chaos [1–4]. It is a paradigm that is fruitful for both analytical and numerical investigations on the influence of classical chaos on various quantum features [5,6].
    [Show full text]
  • Presentation
    Islands of order low-dimensional Islands of order When do deep patterns change? low-dimensional Islands of order Language A Language B Autonomous Networked Stable Transitory low-dimensional Islands of order High-dimensional space low-dimensional Islands of order Tipping points? Shallow Dutch lakes Fertilizer runoff Turbid lake Reduce fertilizer Still turbid ? Nonlinear? Zooplankton Remove fish recover Clear lake Sediment settles But lakes are pretty simple… what about more complex systems? A coupled social-ecological system Centuries to construct…disintegrate without constant labor A Balinese gene for cooperation?If not, how does this work? Phosphate in Indonesian volcanos: In irrigation water: Steep, fissured landscape Requires tunnels & canals to bring nutrient-rich waters to paddies Farmers who share water from the same source form a “subak”- at least 1000 years old Subaks capture irrigation water from rivers and springs Water is used to control rice pests… Insects Rats Disease s Synchronized harvests remove pest habitat Nothing left for pests to eat! Subaks vary in their ability to cooperate Example: Farmers in 4 upper subaks rate their subak’s condition higher than farmers in 4 lower subaks Dictator Game to assess cooperation Offers (gifts) in the Dictator Game Lower Game subaks Offers Worse condition-> give less Subak Condition Offers (gifts) in the Dictator Game Worse condition -> give more Upper subaks Game Offers Subak Condition These dynamics would be averaged out (invisible) under equilibrium assumptions Responses to: How effective are sanctions by my subak? 0 . 3 8 . 2 6 s . n 2 o i t c n a s 4 . 2 2 . 2 SUBAKSLOWER L O W ER SUBAKS UPPERUPPER location labor labor collective in Participation LOWER UPPER LOWER temple rituals of Performance subak 0 0 .
    [Show full text]
  • Journal of Applied Nonlinear Dynamics
    Journal of Applied Nonlinear Dynamics Editors Albert C.J. Luo Miguel A. F. Sanjuan Department of Mechanical and Industrial Engineering Department of Physics Southern Illinois University Edwardsville Universidad Rey Juan Carlos Edwardsville, IL 62026-1805, USA 28933 Mostoles, Madrid, Spain Email: [email protected] Email: [email protected] Associate Editors Hongjun Cao Lock Yue Chew Jorge Duarte Department of Mathematics Division of Physics & Applied Physics ISEL-Engineering Superior Institute of School of Science School of Physical & Mathematical Lisbon Beijing Jiaotong University Sciences Mathematics Department Shang Yuan Cun 3, Haidian District Nanyang Technological University Rua Conselheiro Emídio Navarro Beijing 100044 21 Nanyang Link, SPMS-PAP-04-04 1949-014 Lisboa China Singapore 637371 Portugal Email: [email protected] Email: [email protected] Email: [email protected] Lyudmila Efremova Yurij Holovatch Nikolay V. Kuznetsov Institute of Information Technologies Laboratory for Statistical Physics of Mathematics and Mechanics Faculty Mathematics and Mechanics Complex Systems Saint-Petersburg State University University of Nizhni Novgorod Institute for Condensed Matter Physics Saint-Petersburg, 198504, Russia Gagarin ave., 23a National Acad. Sci. of Ukraine, Lviv Email: [email protected] Nizhni Novgorod, 603950 Ukraine Russia Email: [email protected] Email: [email protected] Edson Denis Leonel Antonio M Lopes J. A. Tenreiro Machado Departamento de Física UISPA-LAETA/INEGI ISEP-Institute of Engineering of Porto UNESP - Univ Estadual Paulista Faculty of Engineering Dept. of Electrical Engineering Av. 24A, 1515 - Rio Claro – SP University of Porto Rua Dr. Antonio Bernardino de Brazil - 13.506-900 Rua Doutor Roberto Frias, s/n, 4200-465 Almeida 431, 4200-072 Porto Portugal Email: [email protected] Porto, Portugal Email: [email protected] Email:[email protected] Vladimir I.
    [Show full text]
  • Kumari Meenu.Pdf (9.124Mb)
    Quantum-Classical Correspondence and Entanglement in Periodically Driven Spin Systems by Meenu Kumari A thesis presented to the University of Waterloo in fulfillment of the thesis requirement for the degree of Doctor of Philosophy in Physics (Quantum Information) Waterloo, Ontario, Canada, 2019 c Meenu Kumari 2019 Examining Committee Membership The following served on the Examining Committee for this thesis. The decision of the Examining Committee is by majority vote. External Examiner: Karl-Peter Marzlin Professor, Dept. of Physics, St. Francis Xavier University Supervisor(s): Shohini Ghose Professor, Dept. of Physics and Computer Sci., Wilfrid Laurier University Robert B. Mann Professor, Dept. of Physics and Astronomy, University of Waterloo Internal Member: Norbert L¨utkenhaus Professor, Dept. of Physics and Astronomy, University of Waterloo Internal-External Member: Achim Kempf Professor, Dept. of Applied Mathematics, University of Waterloo Other Member(s): Eduardo Mart´ın-Mart´ınez Asst. Professor, Dept. of Applied Mathematics, University of Waterloo ii This thesis consists of material all of which I authored or co-authored: see Statement of Contributions included in the thesis. This is a true copy of the thesis, including any required final revisions, as accepted by my examiners. I understand that my thesis may be made electronically available to the public. iii Statement of Contributions This thesis is based on the following publications and forthcoming articles: • Chapters 2 and 3 are based on - M. Kumari and S. Ghose, Quantum-classical correspondence in the vicinity of pe- riodic orbits, Phys. Rev. E 97, 052209 (2018). • Chapter 4 is based on - M. Kumari and S. Ghose, Untangling entanglement and chaos, Phys.
    [Show full text]
  • Physical Review
    PERIODICALS PHYSICAL REVIEW ETM Postmaster send address changes to: For editorial and subscription correspondence, APS Subscription Services please see inside front cover Suite 1NO1 (ISSN: 1539-3755) 2 Huntington Quadrangle Melville, NY 11747-4502 THIRD SERIES, VOLUME 86, NUMBER 2 CONTENTS AUGUST 2012 PART 2: NONLINEAR AND PLASMA PHYSICS, FLUID DYNAMICS, AND RELATED TOPICS RAPID COMMUNICATIONS Interdisciplinary physics Onset of localization in heterogeneous interfacial failure (4 pages) ......................................... 025101(R) Arne Stormo, Knut Skogstrand Gjerden, and Alex Hansen Chaos and pattern formation Probabilistic convergence guarantees for type-II pulse-coupled oscillators (4 pages) .......................... 025201(R) Joel Nishimura and Eric J. Friedman Fluid dynamics Computation of anomalous scaling exponents of turbulence from self-similar instanton dynamics (4 pages) ...... 025301(R) Alexei A. Mailybaev Pressure-driven flow through a single nanopore (5 pages) ................................................. 025302(R) A. E. Velasco, S. G. Friedman, M. Pevarnik, Z. S. Siwy, and P. Taborek Computational physics Allowed and forbidden regimes of entropy balance in lattice Boltzmann collisions (4 pages) ................... 025701(R) Alexander N. Gorban and Dave Packwood ARTICLES Interdisciplinary physics Correlation and network analysis of global financial indices (8 pages) ...................................... 026101 Sunil Kumar and Nivedita Deo Modification of the gravity model and application to the metropolitan Seoul
    [Show full text]
  • Physics – World Scientific Catalogue 2021
    World Scientific Connecting Great Minds PHYSICS 2021 AVAILABLE IN PRINT AND DIGITAL MORE DIGITAL PRODUCTS ON WORLDSCINET HighlightsHighlights Physics Catalogue 2021 page 6 page 6 page 10 page 13 edited by David N Burrows edited by Ofer Lahav edited by David Gross (University of by Alexey P Isaev (Joint Institute for (The Pennsylvania State (University College London, California at Santa Barbara), Alexander Nuclear Research, Dubna, Russia University, USA) UK), Lucy Calder (University Sevrin (Vrije Universiteit Brussel, Belgium & & M V Lomonosov Moscow State College London, UK), et al International Solvay Institutes, Belgium), et al University, Russia), et al page 17 page 18 page 20 page 24 edited by Johnpierre Paglione edited by Bertrand I Halperin by José P Mestre (University of Illinois by Gautier Depambour (University of Maryland, College Park, (Harvard University, USA) & at Urbana-Champaign, USA) & (Université de Paris, France) USA), Nicholas P Butch (National Jainendra K Jain (Penn State Jennifer L Docktor (University of Institute of Standards and Technology, University, USA) Wisconsin-La Crosse, USA) USA), et al page 25 page 26 page 28 page 28 by Leonard A Cole by Vladimir M Kolomietz edited by Lars Brink (Chalmers University of by Alexander Wu Chao (Rutgers University, USA) (Institute for Nuclear Research, Technology, Sweden), Richard C Brower (Boston (SLAC National Accelerator Ukraine) & Shalom Shlomo (Texas University, USA), Carleton DeTar (University of Utah, Laboratory, USA) A&M University, USA) USA), Chung-I Tan (Brown University,
    [Show full text]