Relativistic Quantum Chaos—An Emergent Interdisciplinary Field Ying-Cheng Lai, Hong-Ya Xu, Liang Huang, and Celso Grebogi
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Chaotic Advection, Diffusion, and Reactions in Open Flows Tamás Tél, György Károlyi, Áron Péntek, István Scheuring, Zoltán Toroczkai, Celso Grebogi, and James Kadtke
Chaotic advection, diffusion, and reactions in open flows Tamás Tél, György Károlyi, Áron Péntek, István Scheuring, Zoltán Toroczkai, Celso Grebogi, and James Kadtke Citation: Chaos: An Interdisciplinary Journal of Nonlinear Science 10, 89 (2000); doi: 10.1063/1.166478 View online: http://dx.doi.org/10.1063/1.166478 View Table of Contents: http://scitation.aip.org/content/aip/journal/chaos/10/1?ver=pdfcov Published by the AIP Publishing This article is copyrighted as indicated in the article. Reuse of AIP content is subject to the terms at: http://scitation.aip.org/termsconditions. Downloaded to IP: 128.173.125.76 On: Mon, 24 Mar 2014 14:44:01 CHAOS VOLUME 10, NUMBER 1 MARCH 2000 Chaotic advection, diffusion, and reactions in open flows Tama´sTe´l Institute for Theoretical Physics, Eo¨tvo¨s University, P.O. Box 32, H-1518 Budapest, Hungary Gyo¨rgy Ka´rolyi Department of Civil Engineering Mechanics, Technical University of Budapest, Mu¨egyetem rpk. 3, H-1521 Budapest, Hungary A´ ron Pe´ntek Marine Physical Laboratory, Scripps Institution of Oceanography, University of California at San Diego, La Jolla, California 92093-0238 Istva´n Scheuring Department of Plant Taxonomy and Ecology, Research Group of Ecology and Theoretical Biology, Eo¨tvo¨s University, Ludovika te´r 2, H-1083 Budapest, Hungary Zolta´n Toroczkai Department of Physics, University of Maryland, College Park, Maryland 20742-4111 and Department of Physics, Virginia Polytechnic Institute and State University, Blacksburg, Virginia 24061-0435 Celso Grebogi Institute for Plasma Research, University of Maryland, College Park, Maryland 20742 James Kadtke Marine Physical Laboratory, Scripps Institution of Oceanography, University of California at San Diego, La Jolla, California 92093-0238 ͑Received 30 July 1999; accepted for publication 8 November 1999͒ We review and generalize recent results on advection of particles in open time-periodic hydrodynamical flows. -
Quantum Dots
Quantum Dots www.nano4me.org © 2018 The Pennsylvania State University Quantum Dots 1 Outline • Introduction • Quantum Confinement • QD Synthesis – Colloidal Methods – Epitaxial Growth • Applications – Biological – Light Emitters – Additional Applications www.nano4me.org © 2018 The Pennsylvania State University Quantum Dots 2 Introduction Definition: • Quantum dots (QD) are nanoparticles/structures that exhibit 3 dimensional quantum confinement, which leads to many unique optical and transport properties. Lin-Wang Wang, National Energy Research Scientific Computing Center at Lawrence Berkeley National Laboratory. <http://www.nersc.gov> GaAs Quantum dot containing just 465 atoms. www.nano4me.org © 2018 The Pennsylvania State University Quantum Dots 3 Introduction • Quantum dots are usually regarded as semiconductors by definition. • Similar behavior is observed in some metals. Therefore, in some cases it may be acceptable to speak about metal quantum dots. • Typically, quantum dots are composed of groups II-VI, III-V, and IV-VI materials. • QDs are bandgap tunable by size which means their optical and electrical properties can be engineered to meet specific applications. www.nano4me.org © 2018 The Pennsylvania State University Quantum Dots 4 Quantum Confinement Definition: • Quantum Confinement is the spatial confinement of electron-hole pairs (excitons) in one or more dimensions within a material. – 1D confinement: Quantum Wells – 2D confinement: Quantum Wire – 3D confinement: Quantum Dot • Quantum confinement is more prominent in semiconductors because they have an energy gap in their electronic band structure. • Metals do not have a bandgap, so quantum size effects are less prevalent. Quantum confinement is only observed at dimensions below 2 nm. www.nano4me.org © 2018 The Pennsylvania State University Quantum Dots 5 Quantum Confinement • Recall that when atoms are brought together in a bulk material the number of energy states increases substantially to form nearly continuous bands of states. -
Hyperbolic Metamaterials Based on Quantum-Dot Plasmon-Resonator Nanocomposites
Downloaded from orbit.dtu.dk on: Oct 04, 2021 Hyperbolic metamaterials based on quantum-dot plasmon-resonator nanocomposites. Zhukovsky, Sergei; Ozel, T.; Mutlugun, E.; Gaponik, N.; Eychmuller, A.; Lavrinenko, Andrei; Demir, H. V.; Gaponenko, S. V. Published in: Optics Express Link to article, DOI: 10.1364/OE.22.018290 Publication date: 2014 Document Version Publisher's PDF, also known as Version of record Link back to DTU Orbit Citation (APA): Zhukovsky, S., Ozel, T., Mutlugun, E., Gaponik, N., Eychmuller, A., Lavrinenko, A., Demir, H. V., & Gaponenko, S. V. (2014). Hyperbolic metamaterials based on quantum-dot plasmon-resonator nanocomposites. Optics Express, 22(15), 18290-18298. https://doi.org/10.1364/OE.22.018290 General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. Users may download and print one copy of any publication from the public portal for the purpose of private study or research. You may not further distribute the material or use it for any profit-making activity or commercial gain You may freely distribute the URL identifying the publication in the public portal If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. Hyperbolic metamaterials based on quantum-dot plasmon-resonator nanocomposites 1, 2 2,3 4 S. V. Zhukovsky, ∗ T. Ozel, E. Mutlugun, N. Gaponik, A. -
Quantum Dot and Electron Acceptor Nano-Heterojunction For
www.nature.com/scientificreports OPEN Quantum dot and electron acceptor nano‑heterojunction for photo‑induced capacitive charge‑transfer Onuralp Karatum1, Guncem Ozgun Eren2, Rustamzhon Melikov1, Asim Onal3, Cleva W. Ow‑Yang4,5, Mehmet Sahin6 & Sedat Nizamoglu1,2,3* Capacitive charge transfer at the electrode/electrolyte interface is a biocompatible mechanism for the stimulation of neurons. Although quantum dots showed their potential for photostimulation device architectures, dominant photoelectrochemical charge transfer combined with heavy‑metal content in such architectures hinders their safe use. In this study, we demonstrate heavy‑metal‑free quantum dot‑based nano‑heterojunction devices that generate capacitive photoresponse. For that, we formed a novel form of nano‑heterojunctions using type‑II InP/ZnO/ZnS core/shell/shell quantum dot as the donor and a fullerene derivative of PCBM as the electron acceptor. The reduced electron–hole wavefunction overlap of 0.52 due to type‑II band alignment of the quantum dot and the passivation of the trap states indicated by the high photoluminescence quantum yield of 70% led to the domination of photoinduced capacitive charge transfer at an optimum donor–acceptor ratio. This study paves the way toward safe and efcient nanoengineered quantum dot‑based next‑generation photostimulation devices. Neural interfaces that can supply electrical current to the cells and tissues play a central role in the understanding of the nervous system. Proper design and engineering of such biointerfaces enables the extracellular modulation of the neural activity, which leads to possible treatments of neurological diseases like retinal degeneration, hearing loss, diabetes, Parkinson and Alzheimer1–3. Light-activated interfaces provide a wireless and non-genetic way to modulate neurons with high spatiotemporal resolution, which make them a promising alternative to wired and surgically more invasive electrical stimulation electrodes4,5. -
1.07 Quantum Dots: Theory N Vukmirovic´ and L-W Wang, Lawrence Berkeley National Laboratory, Berkeley, CA, USA
1.07 Quantum Dots: Theory N Vukmirovic´ and L-W Wang, Lawrence Berkeley National Laboratory, Berkeley, CA, USA ª 2011 Elsevier B.V. All rights reserved. 1.07.1 Introduction 189 1.07.2 Single-Particle Methods 190 1.07.2.1 Density Functional Theory 191 1.07.2.2 Empirical Pseudopotential Method 193 1.07.2.3 Tight-Binding Methods 194 1.07.2.4 k ? p Method 195 1.07.2.5 The Effect of Strain 198 1.07.3 Many-Body Approaches 201 1.07.3.1 Time-Dependent DFT 201 1.07.3.2 Configuration Interaction Method 202 1.07.3.3 GW and BSE Approach 203 1.07.3.4 Quantum Monte Carlo Methods 204 1.07.4 Application to Different Physical Effects: Some Examples 205 1.07.4.1 Electron and Hole Wave Functions 205 1.07.4.2 Intraband Optical Processes in Embedded Quantum Dots 206 1.07.4.3 Size Dependence of the Band Gap in Colloidal Quantum Dots 208 1.07.4.4 Excitons 209 1.07.4.5 Auger Effects 210 1.07.4.6 Electron–Phonon Interaction 212 1.07.5 Conclusions 213 References 213 1.07.1 Introduction laterally by electrostatic gates or vertically by etch- ing techniques [1,2]. The properties of this type of Since the early 1980s, remarkable progress in technology quantum dots, sometimes termed as electrostatic has been made, enabling the production of nanometer- quantum dots, can be controlled by changing the sized semiconductor structures. This is the length scale applied potential at gates, the choice of the geometry where the laws of quantum mechanics rule and a range of gates, or external magnetic field. -
Table of Contents (Print, Part 2)
PERIODICALS PHYSICAL REVIEW E 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 75, NUMBER 6 CONTENTS JUNE 2007 PART 2: STATISTICAL AND NONLINEAR PHYSICS, FLUID DYNAMICS, AND RELATED TOPICS RAPID COMMUNICATIONS Chaos and pattern formation Giant acceleration in slow-fast space-periodic Hamiltonian systems (4 pages) ........................... 065201͑R͒ D. V. Makarov and M. Yu. Uleysky Controlling spatiotemporal chaos using multiple delays (4 pages) ..................................... 065202͑R͒ Alexander Ahlborn and Ulrich Parlitz Signatures of fractal clustering of aerosols advected under gravity (4 pages) ............................ 065203͑R͒ Rafael D. Vilela, Tamás Tél, Alessandro P. S. de Moura, and Celso Grebogi Fluid dynamics Clustering of matter in waves and currents (4 pages) ............................................... 065301͑R͒ Marija Vucelja, Gregory Falkovich, and Itzhak Fouxon Experimental study of the bursting of inviscid bubbles (4 pages) ..................................... 065302͑R͒ Frank Müller, Ulrike Kornek, and Ralf Stannarius Surface thermal capacity and its effects on the boundary conditions at fluid-fluid interfaces (4 pages) ....... 065303͑R͒ Kausik S. Das and C. A. Ward Plasma physics Direct evidence of strongly inhomogeneous energy deposition in target heating with laser-produced ion beams (4 pages) .................................................................................. -
Electrodynamic Modeling of Quantum Dot Luminescence in Plasmonic Metamaterials † ‡ † ‡ ‡ § Ming Fang,*, , Zhixiang Huang,*, Thomas Koschny, and Costas M
Article pubs.acs.org/journal/apchd5 Electrodynamic Modeling of Quantum Dot Luminescence in Plasmonic Metamaterials † ‡ † ‡ ‡ § Ming Fang,*, , Zhixiang Huang,*, Thomas Koschny, and Costas M. Soukoulis , † Key Laboratory of Intelligent Computing and Signal Processing, Ministry of Education, Anhui University, Hefei 230001, China ‡ Ames Laboratory and Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, United States § Institute of Electronic Structure and Laser, FORTH, 71110 Heraklion, Crete, Greece ABSTRACT: A self-consistent approach is proposed to simulate a coupled system of quantum dots (QDs) and metallic metamaterials. Using a four-level atomic system, an artificial source is introduced to simulate the spontaneous emission process in the QDs. We numerically show that the metamaterials can lead to multifold enhancement and spectral narrowing of photoluminescence from QDs. These results are consistent with recent experimental studies. The proposed method represents an essential step for developing and understanding a metamaterial system with gain medium inclusions. KEYWORDS: photoluminescence, plasmonics, metamaterials, quantum dots, finite-different time-domain, spontaneous emission he fields of plasmonic metamaterials have made device design based on quantum electrodynamics. In an active − T spectacular experimental progress in recent years.1 3 medium, the electromagnetic field is treated classically, whereas The metal-based metamaterial losses at optical frequencies atoms are treated quantum mechanically. According to the are unavoidable. Therefore, control of conductor losses is a key current understanding, the interaction of electromagnetic fields challenge in the development of metamaterial technologies. with an active medium can be modeled by a classical harmonic These losses hamper the development of optical cloaking oscillator model and the rate equations of atomic population devices and negative index media. -
Data Based Identification and Prediction of Nonlinear and Complex Dynamical Systems
Data Based Identification and Prediction of Nonlinear and Complex Dynamical Systems Wen-Xu Wanga;b, Ying-Cheng Laic;d;e, and Celso Grebogie a School of Systems Science, Beijing Normal University, Beijing, 100875, China b Business School, University of Shanghai for Science and Technology, Shanghai 200093, China c School of Electrical, Computer and Energy Engineering, Arizona State University, Tempe, Arizona 85287, USA d Department of Physics, Arizona State University, Tempe, Arizona 85287, USA e Institute for Complex Systems and Mathematical Biology, King’s College, University of Aberdeen, Aberdeen AB24 3UE, UK Wen-Xu Wang, Ying-Cheng Lai, and Celso Grebogi 1 Abstract The problem of reconstructing nonlinear and complex dynamical systems from measured data or time series is central to many scientific disciplines including physical, biological, computer, and social sciences, as well as engineering and economics. The classic approach to phase-space re- construction through the methodology of delay-coordinate embedding has been practiced for more than three decades, but the paradigm is effective mostly for low-dimensional dynamical systems. Often, the methodology yields only a topological correspondence of the original system. There are situations in various fields of science and engineering where the systems of interest are complex and high dimensional with many interacting components. A complex system typically exhibits a rich variety of collective dynamics, and it is of great interest to be able to detect, classify, under- stand, predict, and control the dynamics using data that are becoming increasingly accessible due to the advances of modern information technology. To accomplish these tasks, especially prediction and control, an accurate reconstruction of the original system is required. -
Quantum Computation with Two-Dimensional Graphene
Quantum computation with two-dimensional graphene quantum dots* Jason Lee(李杰森), Zhi-Bing Li(李志兵), and Dao-Xin Yao (姚道新)†† State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics and Engineering, Sun Yat-sen University, Guangzhou 510275, China Keywords: graphene, quantum dot, quantum computation, Kagome lattice PACS: 73.22.Pr, 73.21.La, 73.22.–f, 74.25.Jb Abstract We study an array of graphene nano sheets that form a two-dimensional S = 1/2 Kagome spin lattice used for quantum computation. The edge states of the graphene nano sheets are used to form quantum dots to confine electrons and perform the computation. We propose two schemes of bang-bang control to combat decoherence and realize gate operations on this array of quantum dots. It is shown that both schemes contain a great amount of information for quantum computation. The corresponding gate operations are also proposed. 1. Introduction There has been increasing interest in grapheme since its discovery. [1−3] It has shown excellent electronic[4,5] and mechanical [6,7] properties and is also a promising candidate for biosensors.[8,9] Before this amazing discovery, Wallace had studied the band structure of graphite and found a linear dispersion around the Dirac point in the Brillouin zone. [10]Much research has been done on this linear dispersion and in particular on the transport properties of graphene. [11−13] Nakada and Fujita studied the edge state and the nano size effect of graphene, and found that the charge can be localized in the zigzag edge[14] to form quantum dots (QDs). -
Strange Attractors That Are Not Chaotic
Physica 13D (1984) 261-268 North-Holland, Amsterdam STRANGE ATTRACTORS THAT ARE NOT CHAOTIC Celso GREBOGI, a Edward OTT, ~b Steven PELIKAN, c and James A. YORKE d Received 7. February 1984 It is shown that in certain types of dynamical systems it is possible to have attractors which are strange but not chaotic. Here we use the word strange to refer to the geometry or shape of the attracting set, while the word chaotic refers to the dynamics of orbits on the attractor (in particular, the exponential divergence of nearby trajectories). We first give examples for which it can be demonstrated that there is a strange nonchaotic attractor. These examples apply to a class of maps which model nonlinear oscillators (continuous time) which are externally driven at two incommensurate frequencies. It is then shown that such attractors are persistent under perturbations which preserve the original system type (i.e., there are two incommensurate external driving frequencies). This suggests that, for systems of the type which we have considered, nonchaotic strange attractors may be expected to occur for a finite interval of parameter values. On the other hand, when small perturbations which do not preserve the system type are numerically introduced the strange nonchaotic attractor is observed to be converted to a periodic or chaotic orbit. Thus we conjecture that, in general, continuous time systems (" flows") which are not externally driven at two incommensurate frequencies should not be expected to have strange nonchaotic attractors except possibly on a set of measure zero in the parameter space. 1. Introduction and definitions ties [1] such as noninteger fractal dimension, Cantor set structure, or nowhere differentiability. -
Crises, Sudden Changes in Chaotic Attractors, and Transient Chaos
Physica 7D (1983) 181-200 North-Holland Publishing Company CRISES, SUDDEN CHANGES IN CHAOTIC ATTRACTORS, AND TRANSIENT CHAOS Celso GREBOGI and Edward OTT Laboratory for Plasma and Fusion Energy Studies, Unit'ersity of Maryland, College Park, Md. 20742, USA and James A. YORKE Institute for Physical Science and Technology and Department of Mathematics, Unit ersi O, of Mao'land, College Park, Md. 20742, USA The occurrence of sudden qualitative changes of chaotic dynamics as a parameter is varied is discussed and illustrated. It is shown that such changes may result from the collision of an unstable periodic orbit and a coexisting chaotic attractor. We call such collisions crises. Phenomena associated with crises include sudden changes in the size of chaotic attractors, sudden appearances of chaotic attractors (a possible route to chaos), and sudden destructions of chaotic attractors and their basins. This paper presents examples illustrating that crisis events are prevalent in many circumstances and systems, and that, just past a crisis, certain characteristic statistical behavior (whose type depends on the type of crisis) occurs. In particular the phenomenon of chaotic transients is investigated. The examples discussed illustrate crises in progressively higher dimension and include the one-dimensional quadratic map, the (two-dimensional) H~non map, systems of ordinary differential equations in three dimensions and a three-dimensional map. In the case of our study of the three-dimensional map a new route to chaos is proposed which is possible only in invertible maps or flows of dimension at least three or four, respectively. Based on the examples presented the following conjecture is proposed: almost all sudden changes in the size of chaotic attractors and almost all sudden destructions or creations of chaotic attractors and their basins are due to crises. -
Sub-Kelvin Transport Spectroscopy of Fullerene Peapod Quantum Dots Pawel Utko, Jesper Nygård, Marc Monthioux, Laure Noé
Sub-Kelvin transport spectroscopy of fullerene peapod quantum dots Pawel Utko, Jesper Nygård, Marc Monthioux, Laure Noé To cite this version: Pawel Utko, Jesper Nygård, Marc Monthioux, Laure Noé. Sub-Kelvin transport spectroscopy of fullerene peapod quantum dots. Applied Physics Letters, American Institute of Physics, 2006, 89 (23), pp.233118. 10.1063/1.2403909. hal-01764467 HAL Id: hal-01764467 https://hal.archives-ouvertes.fr/hal-01764467 Submitted on 12 Apr 2018 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Sub-Kelvin transport spectroscopy of fullerene peapod quantum dots Pawel Utko, Jesper Nygård, Marc Monthioux, and Laure Noé Citation: Appl. Phys. Lett. 89, 233118 (2006); doi: 10.1063/1.2403909 View online: https://doi.org/10.1063/1.2403909 View Table of Contents: http://aip.scitation.org/toc/apl/89/23 Published by the American Institute of Physics Articles you may be interested in Quantum conductance of carbon nanotube peapods Applied Physics Letters 83, 5217 (2003); 10.1063/1.1633680 APPLIED PHYSICS LETTERS 89, 233118 ͑2006͒ Sub-Kelvin transport spectroscopy of fullerene peapod quantum dots ͒ Pawel Utkoa and Jesper Nygård Nano-Science Center, Niels Bohr Institute, University of Copenhagen, Universitetsparken 5, DK-2100 Copenhagen, Denmark Marc Monthioux and Laure Noé Centre d’Elaboration des Matériaux et d’Etudes Structurales (CEMES), UPR A-8011 CNRS, B.P.