CONVECTIVE INSTABILITY and NOISE-SUSTAINED STRUCTURES IN OPTICS E. Louvergneaux Laboratoire de Physique des Lasers Atomes Molécules University of Lille.

Slides:



Advertisements
Similar presentations
8.1: What is a Vibration?.
Advertisements

Jochen Triesch, UC San Diego, 1 Pattern Formation Goal: See how globally ordered spatial structures can arise from local.
Zero-Phonon Line: transition without creation or destruction of phonons Phonon Wing: at T = 0 K, creation of one or more phonons 7. Optical Spectroscopy.
Sliding of a charge density wave probed by coherent X-Ray Diffraction E. Pinsolle Laboratoire de physique des solides, Orsay.
Ion instability at SuperKEKB H. Fukuma (KEK) and L. F. Wang (SLAC) ECLOUD07, 12th Apr. 2007, Daegu, Korea 1. Introduction 2. Ion trapping 3. Fast ion instability.
Ariadna study : Space-based femtosecond laser filamentation Vytautas Jukna, Arnaud Couairon, Carles Milián Centre de Physique théorique, CNRS École.
Ariadna study : Space-based femtosecond laser filamentation Vytautas Jukna, Arnaud Couairon, Carles Milián Centre de Physique théorique, CNRS École.
WHISTLER TRIGGERING ASSOCIATED WITH A STEP DISCONTINUITY IN THE ELECTRON VELOCITY DISTRIBUTION Martin Lampe and Gurudas Ganguli, Plasma Physics Division,
Modelling Flow Distributed Oscillations In The CDIMA Reaction Jonathan R Bamforth, Serafim Kalliadasis, John H Merkin, Stephen K Scott School of Chemistry,
Lecture 38 Lasers Final Exam next week. LASER L ight A mplification by S timulated E mission of R adiation.
Guillermina Ramirez San Juan
Detection of Emerging Sunspot Regions in the Solar Interior Stathis Ilonidis, Junwei Zhao, and Alexander Kosovichev Stanford University LoHCo Workshop.
DAMPING THE FLAVOR PENDULUM BY BREAKING HOMOGENEITY (Alessandro MIRIZZI, Hamburg U.) NOW 2014 Neutrino oscillation workshop Conca Specchiulla, September.
Higher order laser modes in gravitational wave detectors
Lecture 8 (10/09/2006) Crystallography Part 1: Symmetry Operations
Pattern Formation Induced by Modulation Instability in Nonlinear Optical System Ming-Feng Shih( 石明豐 ) Department of Physics National Taiwan University.
Crystallography Motif: the fundamental part of a symmetric design that, when repeated, creates the whole pattern In 3-D, translation defines operations.
New physics with polar molecules Eugene Demler Harvard University Outline: Measurements of molecular wavefunctions using noise correlations Quantum critical.
G. SEMINARA Dipartimento di Ingegneria Ambientale, Università di Genova, Italy Coworkers: M. Colombini, B. Federici, M. Guala, S. Lanzoni, N. Siviglia,
Interference Diffraction and Lasers
Concepts for Combining Different Sensors for CLIC Final Focus Stabilisation David Urner Armin Reichold.
Recent developments around wave turbulence in nonlinear fiber optics Stéphane Randoux 1, Antonio Picozzi 2, Pierre Suret 1 1: Laboratoire de Physique des.
NOISE-SUSTAINED PATTERNS IN NONLINEAR OPTICS
Controlling the dynamics time scale of a diode laser using filtered optical feedback. A.P.A. FISCHER, Laboratoire de Physique des Lasers, Universite Paris.
Contact Line Instability in Driven Films
TURBO TAKS Week 6 Lesson 1: Body Systems Lesson 2: Heat Transfer Lesson 3: Waves Lesson 4: Physics Equations.
VISCOUS MEANS FLOWS IN NEARLY INVISCID FARADAY WAVES Elena Martín Universidad de Vigo, Spain - Drift instabilities of spatially uniform Faraday waves.
Chapter 10. Laser Oscillation : Gain and Threshold
BROOKHAVEN SCIENCE ASSOCIATES BIW ’ 06 Lepton Beam Emittance Instrumentation Igor Pinayev National Synchrotron Light Source BNL, Upton, NY.
Interaction of radiation with atoms and ions (I) Absorption- Stimulated emission E1E1 E2E2 W 12 =W 21 Spontaneous emission More definitionsCross section.
Collective excitations in a dipolar Bose-Einstein Condensate Laboratoire de Physique des Lasers Université Paris Nord Villetaneuse - France Former PhD.
Introduction to Self-Organization
Frequency analysis of optical imaging system Dinesh Ganotra.
Elastic collisions. Spin exchange. Magnetization is conserved. Inelastic collisions. Magnetization is free. Magnetic properties of a dipolar BEC loaded.
Light-induced instabilities in large magneto-optical traps G. Labeyrie, F. Michaud, G.L. Gattobigio, R. Kaiser Institut Non Linéaire de Nice, Sophia Antipolis,
A Self-consistent Model of Alfvén Wave Phase Mixing G.KIDDIE, I. DE MOORTEL, P.CARGILL & A.HOOD.
LISA R&D activities at APC A status report Hubert Halloin.
Multiple-Cone Formation during the Femtosecond-Laser Pulse Propagation in Silica Kenichi Ishikawa *, Hiroshi Kumagai, and Katsumi Midorikawa Laser Technology.
QUEST - Centre for Quantum Engineering and Space-Time Research Multi-resonant spinor dynamics in a Bose-Einstein condensate Jan Peise B. Lücke, M.Scherer,
The anisotropic excitation spectrum of a chromium Bose-Einstein Condensate Laboratoire de Physique des Lasers Université Sorbonne Paris Cité Villetaneuse.
1 « Control of pattern formation in a single feedback system by photonic bandgap structures » Nicolas Marsal, Germano Montemezzani, Delphine Wolfersberger,
Cavity soliton switching and pattern formation in an optically-pumped vertical-cavity semiconductor amplifier Laboratoire de Photonique et de Nanostructures.
Moti Fridman 1, Alessandro Farsi 2 and Alexander L. Gaeta 2 1 School of Engineering, Bar Ilan University, Ramat Gan, 52900, Israel 2 School of Applied.
On the nature of bend instability Stefano Lanzoni University of Padua, Italy Bianca Federici and Giovanni Seminara University of Genua, Italy.
NUMERICAL SIMULATION OF NONLINEAR EFFECTS IN VOLUME FREE ELECTRON LASER (VFEL) K. Batrakov, S. Sytova Research Institute for Nuclear Problems, Belarusian.
Champaign, June 2015 Samir Kassi, Johannes Burkart Laboratoire Interdisciplinaire de Physique, Université Grenoble 1, UMR CNRS 5588, Grenoble F-38041,
Instability of optical speckle patterns in cold atomic gases ? S.E. Skipetrov CNRS/Grenoble (Part of this.
Light Amplification by Stimulated Emission of Radiation.
Three examples of application of Sussix 1)Data from simulations  sensitivity 2)Data from measurements  frequency resolution.
§3.3 Optical Resonators with Spherical Mirrors We will show the field solutions inside the spherical mirror resonator are Gaussian Beams Z=0 00 z R2R2.
LASCAD  - The Laser Engineering Tool The results of FEA can be used with the ABCD gaussian propagation as well as with the BPM physical optics code. FEA.
Date of download: 7/7/2016 Copyright © ASME. All rights reserved. From: Modal Stability TheoryLecture notes from the FLOW-NORDITA Summer School on Advanced.
Arnau Riera, Grup QIC, Dept. ECM, UB 16 de maig de 2009 Intoduction to topological order and topologial quantum computation.
Aerial view of the Copper River Delta, Alaska
Introduction to Plasma Physics and Plasma-based Acceleration
Low energy scattering and charmonium radiative decay from lattice QCD
An overview of turbulent transport in tokamaks
Research and development
Sven Reiche UCLA ICFA-Workshop - Sardinia 07/02
A. Bramati M. Romanelli E. Giacobino
Many-body Floquet systems & time-crystalline order
Measuring Inches.
Mach-Zehnder atom interferometer with nanogratings
Lasers and effects of magnetic field
Diffraction T. Ishikawa Part 1 Kinematical Theory 1/11/2019 JASS02.
Summary of Lecture 18 导波条件 图解法求波导模式 边界条件 波导中模式耦合的微扰理论
Study of Fast Ions in CESR
Principles of Motor Control and Movement Accuracy
Phase Separation Kinetics of Polymer Dispersed Liquid Crystals (PDLC) on a Chemically Heterogeneous Substrate Polarized optical micrograph of the formation.
In this lesson you are going to learn to how to place a fraction with the numerators other than one on a number line by breaking the whole number one on.
Presentation transcript:

CONVECTIVE INSTABILITY and NOISE-SUSTAINED STRUCTURES IN OPTICS E. Louvergneaux Laboratoire de Physique des Lasers Atomes Molécules University of Lille (France)

Colonia Pattern formation and non locality Pattern formation ≡ spontaneous symmetry breaking (translation) of the ground state System System with transverse non local interaction Pattern formation ≡ spontaneous symmetry breaking (translation) of the ground state + breaking of the reflexion symmetry propagating pattern (drifting pattern)

Colonia Pattern formation and non locality Analysis of pattern formation ≡ determination of wavenumber and growth rate at threshold System System with transverse non local interaction Analysis of pattern formation ≡ determination of wavenumber and growth rate at threshold + analysis of pattern emergence and spreading How the emerging pattern will invade or not the whole space

Colonia Pattern formation and non locality System System with transverse non local interaction Convective patterns / Absolute patterns Noise sustained patterns New types of patterns New features … Well known absolute patterns

Colonia Pattern formation and non locality System System with transverse non local interaction Convective patterns / Absolute patterns Noise sustained patterns New types of patterns New features … Well known absolute patterns

Colonia Pattern formation and non locality in optics System with transverse non local interaction TranslationRotationMagnification See works on LCLV, OPO : M.A. Vorontsov et al P.L. Ramazza et al M. San Miguel et al M. Taki et al

Colonia Pattern formation and non locality in optics Translation Drifting patterns Translational shift in a feedback loop Walk off (anisotropic crystal) System with transverse non local interaction

Colonia The optical system Transverse coordinate x Time t Liquid crystal Laser mirror Liquid crystal Laser mirror With transverse shift Transverse coordinate x Time t Transverse coordinate x Numerics

Colonia Competition between the spreading and the drift (diffraction vs advection) Transverse coordinate x Time t The convective and absolute patterns Absolute pattern Convective pattern Transverse coordinate x (the pattern grows fighting the drift upstream) (the pattern grows but is advected away by the drift) Complex frequency and wavenumber to account for spatial and temporal growth rates Liquid crystal Laser mirror With transverse shift

Colonia The nature of the instabilities Convective instability Absolute instability → Impulse response of the system Initial perturbation Time

Colonia The convective and absolute instabilities Convective instability Absolute instability → Impulse response of the system No pattern at long time Patterned state Final state

Colonia The convective and absolute instabilities Convective instability Absolute instability → Impulse response of the system No pattern at long time Patterned state Final state If noise Noise sustained patterned state

Colonia With noise Transverse coordinate x Noise sustained patternAbsolute pattern Noise sustained pattern The noise sustained patterns Without noise Transverse coordinate x Time t Transverse coordinate x Absolute pattern No pattern noise sustained patterns ≡ convective patterns sustained by noise Numerics