A Lévy flight of light

Size: px
Start display at page:

Download "A Lévy flight of light"

Transcription

1 A Lévy flight of light Diederik Wiersma European Lab. For Non-linear Spectroscopy (LENS) INFM-CNR, Univ. of Florence

2 Micro and nano photonics group European Lab. For Non-linear Spectroscopy (LENS) INFM-CNR, Univ. of Florence Pierre Barthelemy Jacopo Bertolotti Francesca Intonti Rajesh Kumar Lorenzo Pattelli Francesco Riboli Silvia Vignolini Radha Vivekananthan Kevin Vynck Stefano Cavalieri Marcello Colocci Stefano Lepri (CNR) Roberto Livi Roberto Righini Matteo Burresi Paola Costantino Stefano Gottardo Yanjun Liu Sushil Mujumdar Shunsuke Murai Riccardo Sapienza Costanza Toninelli

3 Scattering single scattering phase is maintained multiple scattering interference

4 Interference effects Speckle pattern in transmitted light

5 Schrödinger s equation ) ( ) ( ) ( r E r r V m h Ψ = Ψ + Maxwell s equations ) ( ) ( ) ( r E c r E c r ε ω ε ω = Analogies electrons - photons

6 Transport processes Light transport Electron transport Anderson localization Coherent backscattering (weak localization) Optical Bloch oscillations / Zener tunneling Universal conductance fluctuations Ohm s law

7 Coherent backscattering θ θ A B white paint gysum fog/clouds... coherent backscattering cone A - B close: A - B distant: 0 0 θ θ sum W λ/

8 Coherent backscattering Strongy scattering powders: Phys. Rev. Lett. 74, 4193 (1995) - TiO2 powder - Barium Sulphate

9 Transmission

10 Ohm s law Electrons L Resistance L Photons Resistance L L Diffusive systems linear thickness dependence

11 Interference effects Speckle pattern in transmitted light

12 Vortices in optical speckle Amplitude Phase 10 μm 0 Max 0 2π

13 Phase vortices

14 Vortex repulsion

15 Applications of light diffusion Medical diagnostics, imaging caries in teeth blood flow in tissue / brain functionality optical mammography Diffusing Wave Spectroscopy (DWS) dynamics of e.g. colloidal systems Visibility through fog in air/road traffic Random laser

16 Lévy flights

17 Google search: Levy flights

18 Processes with Lévy statistics Stock market fluctuations Animal foraging Human travel Turbulent flow

19 Stable distributions Linear combination of elements remains in distribution Gaussian is limiting case with finite mean Rest has heavy tail asymptotic behaviour: Pz ( ) 1 1+ z α + 1 0< α < 2 α = 1: Cauchy distribution Infinite variance and (for α 1) also infinite mean

20 Lévy α-stable distributions

21 Lévy walks for light waves

22 Disorder: photonic glass Nature Photonics 2, 429 (2008) With group C. Lopez, Madrid

23 Gaussian random walk Δx Δx from distribution with finite average and variance 2 σ Central limit theorem 2 σ D t Gaussian distribution Diffusion process: x 2 = D t with 1 D = 3 v

24 Lévy walk Δx Δx from stable distribution Generalized central limit theorem Generalized diffusion process: x 2 = D γ t with: γ = 3 α 1 α < 2 for γ =1: Normal diffusion γ >1: Super diffusion

25 How to make materials with non- Gaussian disorder?

26 Lévy walk for light Control step size = n 1 σ σ n cross section density Fractal particle size distibution? does not work due to Rayleigh (Mie) scattering Engineer local particle density!

27 Lévy glass TiO2 nanoparticles + Glass Spheres + Sodium Silicate (liquid glass) Glass and glass: index matched Glass Spheres: introduce the density fluctuations Diameter distribution: Pd ( ) 1 d 2 + α (range between 5 and 650 μm)

28 Lévy glass Glass Spheres determine density fluctuations TiO2 particles Lévy flight from multiple scattering on TiO2 particles Nature 453, 498 (May 22, 2008)

29 Sample design Diameter distribution voids: Pd ( ) 1 d 2 + α Step length distribution: Pz ( ) 1 1+ z α + 1 Super diffusion: x 2 = D γ t with: γ = 3 α 1 α < 2 for

30 How to sample this distribution? Diameter distribution voids: Pd ( ) 1 d 2 + α d between 0 and 100 μm in n steps d between 1 and 100 μm in n steps

31 Logarithmic discrete sampling E-3 P(z) 1E-4 1E-5 Discrete sampling Levy Walk α=1.1 1E-6 1E z

32 Experimental observations

33 Super diffusion Enhanced diffusive transmission Transmission α=2 : Diffusive transport α=0,948: Levy transport Generalised Ohm s law: T 1 = 1 + al α / Thickness (μm)

34 Transmission profiles Diffusive case: small fluctuations Diffusive Levy Probability Density Levy Case: enhanced fluctuations R/R average I/I average

35 Enhanced spreading Diffusive Case: Almost-gaussian profile Lévy Case: Cusped spatial profile Experiments Levy Diffusive Transmission Distance (mm)

36 Dynamic properties 1E7 Ti-Sapphire OPO Levy Diffusive Intensity Delay Line Superdiffusive part BBO crystal Diffusive Tail Photomultiply Time

37 Monte Carlo simulations 30

38 Monte Carlo simulations Free space Lévy flight with step length: Pz ( ) 1 1+ z α + 0< α < 2 1

39 Brownian motion vs. Lévy flight Lévy flight Brownian motion α = steps

40 Monte Carlo simulations Fixed geometry (quenched disorder)

41 Placing spheres in a space

42 Placing spheres in a space

43 Monte Carlo simulations Random walk with quenched disorder

44 Quenched vs annealed disorder 1E Quenched disorder Annealed disorder <x 2 >(a.u.) Time (a.u.)

45 Summary Transport of light in random systems How to realize non-gaussian optical disorder: Levy glass Superdiffusion of light, possibility to study optical Levy flights Open questions: - Unknown properties of Lévy flights (e.g. finite-size effects) - Weak localization (coherent backscattering), strong localization, speckle correlations, etc..

46 Micro and nano photonics group European Lab. For Non-linear Spectroscopy (LENS) INFM-CNR, Univ. of Florence Pierre Barthelemy Jacopo Bertolotti Francesca Intonti Rajesh Kumar Lorenzo Pattelli Francesco Riboli Silvia Vignolini Radha Vivekananthan Kevin Vynck Stefano Cavalieri Marcello Colocci Stefano Lepri (CNR) Roberto Livi Roberto Righini Matteo Burresi Paola Costantino Stefano Gottardo Yanjun Liu Sushil Mujumdar Shunsuke Murai Riccardo Sapienza Costanza Toninelli

Optics of complex micro structures

Optics of complex micro structures Optics of complex micro structures dielectric materials λ L disordered partially ordered ordered random multiple scattering liquid crystals quasi crystals (Fibonacci) photonic crystals Assembly of photonic

More information

Lévy Walks and scaling in quenched disordered media

Lévy Walks and scaling in quenched disordered media Lévy Walks and scaling in quenched disordered media A. Vezzani, - CNR Modena - Parma L. Caniparoli - Sissa Trieste S.Lepri - Firenze CNR - ISC Raffaella Burioni - Parma Sperlonga - September 2010 Work

More information

Anomalous wave transport in one-dimensional systems with. Lévy disorder

Anomalous wave transport in one-dimensional systems with. Lévy disorder Anomalous wave transport in one-dimensional systems with Lévy disorder Xujun Ma,2 and Azriel Z. Genack,2 Department of Physics, Queens College of the City University of New York, Flushing, NY, 367 USA

More information

Use and abuse of the effective-refractive-index concept in turbid colloidal systems

Use and abuse of the effective-refractive-index concept in turbid colloidal systems Use and abuse of the ective-refractive-index concept in turbid colloidal systems Rubén G. Barrera* Instituto de Física, Benemérita Universidad Autónoma de Puebla *Permanent address: Instituto de Física,

More information

Statistical regimes of random laser fluctuations

Statistical regimes of random laser fluctuations Statistical regimes of random laser fluctuations Stefano Lepri Istituto dei Sistemi Complessi ISC-CNR Firenze S. Cavalieri, G.-L. Oppo, D.S. Wiersma Stefano Lepri (ISC-CNR) Random laser fluctuations 1

More information

Random Lasers - Physics & Application

Random Lasers - Physics & Application Random Lasers - Physics & Application HuiCao Depts. of Applied Physics & Physics, Yale University Group members Jonathan Andreasen Yong Ling Bo Liu Heeso Noh Brandon Redding Xiaohua Wu Junying Xu Alexey

More information

FUNDAMENTALS OF POLARIZED LIGHT

FUNDAMENTALS OF POLARIZED LIGHT FUNDAMENTALS OF POLARIZED LIGHT A STATISTICAL OPTICS APPROACH Christian Brosseau University of Brest, France A WILEY-INTERSCIENCE PUBLICATION JOHN WILEY & SONS, INC. New York - Chichester. Weinheim. Brisbane

More information

WAVE INTERFERENCES IN RANDOM LASERS

WAVE INTERFERENCES IN RANDOM LASERS WAVE INTERFERENCES IN RANDOM LASERS Philippe Jacquod U of Arizona P. Stano and Ph. Jacquod, Nature Photonics (2013) What is a laser? Light Amplification by Stimulated Emission of Radiation Three main components

More information

The physics and applications of random lasers

The physics and applications of random lasers The physics and applications of random lasers Recent developments in the field of micro and nanophotonics have shown that it is possible to make use of the intrinsic disorder in photonic materials to create

More information

University of Cyprus. Reflectance and Diffuse Spectroscopy

University of Cyprus. Reflectance and Diffuse Spectroscopy University of Cyprus Biomedical Imaging and Applied Optics Reflectance and Diffuse Spectroscopy Spectroscopy What is it? from the Greek: spectro = color + scope = look at or observe = measuring/recording

More information

Low-coherence heterodyne photon correlation spectroscopy

Low-coherence heterodyne photon correlation spectroscopy Low-coherence heterodyne photon correlation spectroscopy J.H. Johnson, S.L. Siefken, A. Schmidt, R. Corey, and P. Saulnier Department of Physics, Gustavus Adolphus College Saint Peter, MN 56082 ABSTRACT

More information

Single Emitter Detection with Fluorescence and Extinction Spectroscopy

Single Emitter Detection with Fluorescence and Extinction Spectroscopy Single Emitter Detection with Fluorescence and Extinction Spectroscopy Michael Krall Elements of Nanophotonics Associated Seminar Recent Progress in Nanooptics & Photonics May 07, 2009 Outline Single molecule

More information

Strongly Localized Photonic Mode in 2D Periodic Structure Without Bandgap

Strongly Localized Photonic Mode in 2D Periodic Structure Without Bandgap Strongly Localized Photonic Mode in D Periodic Structure Without Bandgap V. M. APALKOV M. E. RAIKH Physics Department, University of Utah The work was supported by: the Army Research Office under Grant

More information

Lecture 06. Fundamentals of Lidar Remote Sensing (4) Physical Processes in Lidar

Lecture 06. Fundamentals of Lidar Remote Sensing (4) Physical Processes in Lidar Lecture 06. Fundamentals of Lidar Remote Sensing (4) Physical Processes in Lidar Light interactions with objects (continued) Resonance fluorescence Laser induced fluorescence Doppler effect (Doppler shift

More information

Nonlinear Optical Waves in Disordered Ferroelectrics

Nonlinear Optical Waves in Disordered Ferroelectrics PhD candidate: Nonlinear Optical Waves in Disordered Ferroelectrics Davide Pierangeli davide.pierangeli@roma1.infn.it Supervisor: Prof. Eugenio DelRe Physics Department, Unversity of Rome La Sapienza,

More information

HYPER-RAYLEIGH SCATTERING AND SURFACE-ENHANCED RAMAN SCATTERING STUDIES OF PLATINUM NANOPARTICLE SUSPENSIONS

HYPER-RAYLEIGH SCATTERING AND SURFACE-ENHANCED RAMAN SCATTERING STUDIES OF PLATINUM NANOPARTICLE SUSPENSIONS www.arpapress.com/volumes/vol19issue1/ijrras_19_1_06.pdf HYPER-RAYLEIGH SCATTERING AND SURFACE-ENHANCED RAMAN SCATTERING STUDIES OF PLATINUM NANOPARTICLE SUSPENSIONS M. Eslamifar Physics Department, BehbahanKhatamAl-Anbia

More information

6. Laser Doppler Anemometry. Introduction to principles and applications

6. Laser Doppler Anemometry. Introduction to principles and applications 6. Laser Doppler Anemometry Introduction to principles and applications Characteristics of LDA Invented by Yeh and Cummins in 1964 Velocity measurements in Fluid Dynamics (gas, liquid) Up to 3 velocity

More information

Workshop on Coherent Phenomena in Disordered Optical Systems May Random Laser - Physics & Application

Workshop on Coherent Phenomena in Disordered Optical Systems May Random Laser - Physics & Application 2583-14 Workshop on Coherent Phenomena in Disordered Optical Systems 26-30 May 2014 Random Laser - Physics & Application Hui CAO Depts. of Applied Physics and Physics Yale University New Haven. U.S.A Random

More information

Lecture notes for /12.586, Modeling Environmental Complexity. D. H. Rothman, MIT September 24, Anomalous diffusion

Lecture notes for /12.586, Modeling Environmental Complexity. D. H. Rothman, MIT September 24, Anomalous diffusion Lecture notes for 12.086/12.586, Modeling Environmental Complexity D. H. Rothman, MIT September 24, 2014 Contents 1 Anomalous diffusion 1 1.1 Beyond the central limit theorem................ 2 1.2 Large

More information

Anno Protocollo: RBFR08UH60_001. BERTOLOTTI Jacopo BRTJCP78B11D612G. (surname) (name) (CF) Dottore di ricerca 11/02/1978

Anno Protocollo: RBFR08UH60_001. BERTOLOTTI Jacopo BRTJCP78B11D612G. (surname) (name) (CF) Dottore di ricerca 11/02/1978 MINISTERO DELL'ISTRUZIONE DELL'UNIVERSITÀ E DELLA RICERCA DIREZIONE GENERALE RICERCA PROGETTO DI RICERCA - MODELLO B BANDO FIRB - PROGRAMMA "FUTURO IN RICERCA" Anno 2008 - Protocollo: RBFR08UH60_001 Linea

More information

ORGANIC MOLECULES in photonics

ORGANIC MOLECULES in photonics ORGANIC MOLECULES in photonics Progress in Photonics, Florence 16.10. 2015 probe surface scattered waves Costanza Toninelli www.lens.unifi.it/quantum- nanophotonics Single Molecules: From Sensing To Quantum

More information

Introduction to Atomic Physics and Quantum Optics

Introduction to Atomic Physics and Quantum Optics Physics 404 and Physics 690-03 Introduction to Atomic Physics and Quantum Optics [images courtesy of Thywissen group, U of T] Prof. Seth Aubin Office: room 255, Small Hall, tel: 1-3545 Lab: room 069, Small

More information

Structural characterization. Part 2

Structural characterization. Part 2 Structural characterization Part Determining partial pair distribution functions X-ray absorption spectroscopy (XAS). Atoms of different elements have absorption edges at different energies. Structure

More information

Lecture 06. Fundamentals of Lidar Remote Sensing (4) Physical Processes in Lidar

Lecture 06. Fundamentals of Lidar Remote Sensing (4) Physical Processes in Lidar Lecture 06. Fundamentals of Lidar Remote Sensing (4) Physical Processes in Lidar Physical processes in lidar (continued) Doppler effect (Doppler shift and broadening) Boltzmann distribution Reflection

More information

Polarization and spatial coherence of electromagnetic waves in disordered media

Polarization and spatial coherence of electromagnetic waves in disordered media Polarization and spatial coherence of electromagnetic waves in disordered media Kevin Vynck Laboratoire Photonique, Numérique et Nanosciences (LP2N) UMR 5298, CNRS IOGS Univ. Bordeaux Institut d'optique

More information

Dynamic Light Scattering Employing One- and Two-Dimensional Detectors and Different Time-Correlation Approaches

Dynamic Light Scattering Employing One- and Two-Dimensional Detectors and Different Time-Correlation Approaches Dynamic Light Scattering Employing One- and Two-Dimensional Detectors and Different Time-Correlation Approaches Ralf Klemt Summer Student Project FS-CXS September 10, 2015 Ralf Klemt Dynamic Light Scattering

More information

Roberto Artuso. Caos e diffusione (normale e anomala)

Roberto Artuso. Caos e diffusione (normale e anomala) Roberto Artuso Caos e diffusione (normale e anomala) Lucia Cavallasca, Giampaolo Cristadoro, Predrag Cvitanović, Per Dahlqvist, Gregor Tanner Damiano Belluzzo, Fausto Borgonovi, Giulio Casati, Shmuel Fishman,

More information

Transient grating measurements of spin diffusion. Joe Orenstein UC Berkeley and Lawrence Berkeley National Lab

Transient grating measurements of spin diffusion. Joe Orenstein UC Berkeley and Lawrence Berkeley National Lab Transient grating measurements of spin diffusion Joe Orenstein UC Berkeley and Lawrence Berkeley National Lab LBNL, UC Berkeley and UCSB collaboration Chris Weber, Nuh Gedik, Joel Moore, JO UC Berkeley

More information

Introduction to Atomic Physics and Quantum Optics

Introduction to Atomic Physics and Quantum Optics Physics 404 and Physics 690-03 Introduction to Atomic Physics and Quantum Optics [images courtesy of Thywissen group, U of T] Instructor Prof. Seth Aubin Office: room 245, Millington Hall, tel: 1-3545

More information

Localization in one-dimensional chains with Lévy-type disorder

Localization in one-dimensional chains with Lévy-type disorder Localization in one-dimensional chains with Lévy-type disorder of this work is to provide a framework to investigate localization in power-law correlated disordered systems and to illustrate how the localization

More information

Introduction to Dynamic Light Scattering with Applications. Onofrio Annunziata Department of Chemistry Texas Christian University Fort Worth, TX, USA

Introduction to Dynamic Light Scattering with Applications. Onofrio Annunziata Department of Chemistry Texas Christian University Fort Worth, TX, USA Introduction to Dynamic Light Scattering with Applications Onofrio Annunziata Department of Chemistry Texas Christian University Fort Worth, TX, USA Outline Introduction to dynamic light scattering Particle

More information

Aging in laponite water suspensions. P. K. Bhattacharyya Institute for Soldier Nanotechnologies Massachusetts Institute of Technology

Aging in laponite water suspensions. P. K. Bhattacharyya Institute for Soldier Nanotechnologies Massachusetts Institute of Technology Aging in laponite water suspensions. P. K. Bhattacharyya Institute for Soldier Nanotechnologies Massachusetts Institute of Technology Outline Laponite Basic background. Laponite in suspension Bonn et al.,

More information

Title. Statistical behaviour of optical vortex fields. F. Stef Roux. CSIR National Laser Centre, South Africa

Title. Statistical behaviour of optical vortex fields. F. Stef Roux. CSIR National Laser Centre, South Africa . p.1/37 Title Statistical behaviour of optical vortex fields F. Stef Roux CSIR National Laser Centre, South Africa Colloquium presented at School of Physics National University of Ireland Galway, Ireland

More information

NANO-flex 180 DLS nanoparticle sizing. Laser. Scattered light from particles. Size & concentration vol%

NANO-flex 180 DLS nanoparticle sizing. Laser. Scattered light from particles. Size & concentration vol% NANO-flex 180 DLS nanoparticle sizing 180 heterodyne back scattering Technical Note Size Analysis Scattered & reflected light Laser in & reflected laser Detector Laser Performance of 180 DLS Scattered

More information

STUDIES ON ZnS - CuS NANOPARTICLE SYSTEM.

STUDIES ON ZnS - CuS NANOPARTICLE SYSTEM. CHAPTER - VI STUDIES ON ZnS - CuS NANOPARTICLE SYSTEM. 6.1 INTRODUCTION ZnS is an important direct band gap semiconductor. It has a band gap energy of 3.6 ev[1], displays a high refractive index (2.37)

More information

Introduction to Dynamic Light Scattering for Particle Size Determination

Introduction to Dynamic Light Scattering for Particle Size Determination www.horiba.com/us/particle Jeffrey Bodycomb, Ph.D. Introduction to Dynamic Light Scattering for Particle Size Determination 2016 HORIBA, Ltd. All rights reserved. 1 Sizing Techniques 0.001 0.01 0.1 1 10

More information

RHEOLASER LAB MICRORHEOLOGY & END USE PROPERTIES ANALYSIS. MICRORHEOLOGY

RHEOLASER LAB MICRORHEOLOGY & END USE PROPERTIES ANALYSIS.  MICRORHEOLOGY RHEOLASER LAB & END USE PROPERTIES ANALYSIS A NEW RHEOLOGY APPROACH TO CHARACTERISE END-USE PROPERTIES THE FIRST READY TO USE & END-USE PROPERTIES ANALYSER Rheolaser Rheolaser is the first Lab ready-to-use

More information

Physical Characterization of Solid-Liquid Slurries at High Weight Fractions Using Optical and Ultrasonic Methods Grant # /28/02

Physical Characterization of Solid-Liquid Slurries at High Weight Fractions Using Optical and Ultrasonic Methods Grant # /28/02 Physical Characterization of Solid-Liquid Slurries at High Weight Fractions Using Optical and Ultrasonic Methods Grant # 81964 5/28/02 Lead Principal Investigators: L.W. Burgess and A.M. Brodsky Center

More information

Nanophysics: Main trends

Nanophysics: Main trends Nano-opto-electronics Nanophysics: Main trends Nanomechanics Main issues Light interaction with small structures Molecules Nanoparticles (semiconductor and metallic) Microparticles Photonic crystals Nanoplasmonics

More information

Quantum Condensed Matter Physics Lecture 9

Quantum Condensed Matter Physics Lecture 9 Quantum Condensed Matter Physics Lecture 9 David Ritchie QCMP Lent/Easter 2018 http://www.sp.phy.cam.ac.uk/drp2/home 9.1 Quantum Condensed Matter Physics 1. Classical and Semi-classical models for electrons

More information

Advanced Vitreous State The Physical Properties of Glass

Advanced Vitreous State The Physical Properties of Glass Advanced Vitreous State The Physical Properties of Glass Active Optical Properties of Glass Lecture 21: Nonlinear Optics in Glass-Applications Denise Krol Department of Applied Science University of California,

More information

Optical Imaging Chapter 5 Light Scattering

Optical Imaging Chapter 5 Light Scattering Optical Imaging Chapter 5 Light Scattering Gabriel Popescu University of Illinois at Urbana-Champaign Beckman Institute Quantitative Light Imaging Laboratory http://light.ece.uiuc.edu Principles of Optical

More information

Lecture 10: Surface Plasmon Excitation. 5 nm

Lecture 10: Surface Plasmon Excitation. 5 nm Excitation Lecture 10: Surface Plasmon Excitation 5 nm Summary The dispersion relation for surface plasmons Useful for describing plasmon excitation & propagation This lecture: p sp Coupling light to surface

More information

Lecture 9: Introduction to Diffraction of Light

Lecture 9: Introduction to Diffraction of Light Lecture 9: Introduction to Diffraction of Light Lecture aims to explain: 1. Diffraction of waves in everyday life and applications 2. Interference of two one dimensional electromagnetic waves 3. Typical

More information

Brewster Angle and Total Internal Reflection

Brewster Angle and Total Internal Reflection Lecture 4: Polarization Outline 1 Polarized Light in the Universe 2 Brewster Angle and Total Internal Reflection 3 Descriptions of Polarized Light 4 Polarizers 5 Retarders Christoph U. Keller, Utrecht

More information

Lecture 5: Polarization. Polarized Light in the Universe. Descriptions of Polarized Light. Polarizers. Retarders. Outline

Lecture 5: Polarization. Polarized Light in the Universe. Descriptions of Polarized Light. Polarizers. Retarders. Outline Lecture 5: Polarization Outline 1 Polarized Light in the Universe 2 Descriptions of Polarized Light 3 Polarizers 4 Retarders Christoph U. Keller, Leiden University, keller@strw.leidenuniv.nl ATI 2016,

More information

Multiphoton microscopy

Multiphoton microscopy Multiphoton microscopy Joonas Holmi ELEC October 6, 2016 Multiphoton microscopy 1. 2. 3. 4. Multiphoton microscopy 2/14 Intro: Multiphoton microscopy Nonlinear optical characterization method Pulsed laser

More information

Investigation of the noise-like structures of the total scattering cross-section of random media

Investigation of the noise-like structures of the total scattering cross-section of random media Investigation of the noise-like structures of the total scattering cross-section of random media Snow H. Tseng, Allen Taflove, Duncan Maitland, Vadim Backman, and Joseph T. Walsh, Jr. Department of Electrical

More information

Atomic and Molecular Spectroscopy

Atomic and Molecular Spectroscopy Atomic and Molecular Spectroscopy Molecular Applied Laser Spectroscopy GASMAS LIDAR Reading instructions: Section 10.2: Laser Remote Sensing and Applications (page 406 425) Section 10.5.4: Scattering Spectroscopy

More information

INTRODUCTION. Definition:-

INTRODUCTION. Definition:- INTRODUCTION Definition:- Light scatteringis a form ofscatteringin whichlightis the form of propagating energy which is scattered. Light scattering can be thought of as the deflection of arayfrom a straight

More information

6. LIGHT SCATTERING 6.1 The first Born approximation

6. LIGHT SCATTERING 6.1 The first Born approximation 6. LIGHT SCATTERING 6.1 The first Born approximation In many situations, light interacts with inhomogeneous systems, in which case the generic light-matter interaction process is referred to as scattering

More information

Optical Spectroscopy of Advanced Materials

Optical Spectroscopy of Advanced Materials Phys 590B Condensed Matter Physics: Experimental Methods Optical Spectroscopy of Advanced Materials Basic optics, nonlinear and ultrafast optics Jigang Wang Department of Physics, Iowa State University

More information

Coherent Backscattering, Photon Localization and Random Laser with Cold Atoms

Coherent Backscattering, Photon Localization and Random Laser with Cold Atoms Coherent Backscattering, Photon Localization and Random Laser with Cold Atoms Robin Kaiser CLXXIII International School of Physics "Enrico Fermi" "Nano optics and atomics: transport of light and matter

More information

Lecture 25: Large Steps and Long Waiting Times

Lecture 25: Large Steps and Long Waiting Times Lecture 25: Large Steps and Long Waiting Times Scribe: Geraint Jones (and Martin Z. Bazant) Department of Economics, MIT Proofreader: Sahand Jamal Rahi Department of Physics, MIT scribed: May 10, 2005,

More information

The DLR Project WETTER & FLIEGEN. Simulated Lidar Signals for Wake-Vortex Detection ahead of the Aircraft

The DLR Project WETTER & FLIEGEN. Simulated Lidar Signals for Wake-Vortex Detection ahead of the Aircraft The DLR Project WETTER & FLIEGEN Final Colloquium, 14.03.2012 Simulated Lidar Signals for Wake-Vortex Detection ahead of the Aircraft Markus Hirschberger, Institute PA, Lidar division 1 Aircraft moves

More information

Contents Preface iii 1 Origins and Manifestations of Speckle 2 Random Phasor Sums 3 First-Order Statistical Properties

Contents Preface iii 1 Origins and Manifestations of Speckle 2 Random Phasor Sums 3 First-Order Statistical Properties Contents Preface iii 1 Origins and Manifestations of Speckle 1 1.1 General Background............................. 1 1.2 Intuitive Explanation of the Cause of Speckle................ 2 1.3 Some Mathematical

More information

Connecting metallic nanoparticles by optical

Connecting metallic nanoparticles by optical Supplementary Information for Connecting metallic nanoparticles by optical printing Julián Gargiulo 1, Santiago Cerrota 1, Emiliano Cortés 1, Ianina L. Violi 1, Fernando D. Stefani* 1,2 1 Centro de Investigaciones

More information

Lecture 11: Introduction to diffraction of light

Lecture 11: Introduction to diffraction of light Lecture 11: Introduction to diffraction of light Diffraction of waves in everyday life and applications Diffraction in everyday life Diffraction in applications Spectroscopy: physics, chemistry, medicine,

More information

Time-resolved Diffusing Wave Spectroscopy to Enable Ultrafast Electro-optic Relaxation Dynamic in Liquid Crystals

Time-resolved Diffusing Wave Spectroscopy to Enable Ultrafast Electro-optic Relaxation Dynamic in Liquid Crystals Time-resolved Diffusing Wave Spectroscopy to Enable Ultrafast Electro-optic Relaxation Dynamic in Liquid Crystals Suman Kalyan Manna 1*, Laurent Dupont 2, Guoqiang Li 3* 1 Department of Cell Biology and

More information

All-optically controllable random laser based on a dye-doped polymer-dispersed liquid crystal with nano-sized droplets

All-optically controllable random laser based on a dye-doped polymer-dispersed liquid crystal with nano-sized droplets All-optically controllable random laser based on a dye-doped polymer-dispersed liquid crystal with nano-sized droplets C.-R. Lee, 1, * S.-H. Lin, 1 C.-H. Guo, 1 S.-H. Chang, 1 T.-S. Mo, 2 and S.-C. Chu

More information

Lecture 3: From Random Walks to Continuum Diffusion

Lecture 3: From Random Walks to Continuum Diffusion Lecture 3: From Random Walks to Continuum Diffusion Martin Z. Bazant Department of Mathematics, MIT February 3, 6 Overview In the previous lecture (by Prof. Yip), we discussed how individual particles

More information

Non contact measurement of viscoelastic properties of biopolymers

Non contact measurement of viscoelastic properties of biopolymers Non contact measurement of viscoelastic properties of biopolymers Christelle Tisserand, Anton Kotzev, Mathias Fleury, Laurent Brunel, Pascal Bru, Gérard Meunier Formulaction, 10 impasse Borde Basse, 31240

More information

Anomalous diffusion in biology: fractional Brownian motion, Lévy flights

Anomalous diffusion in biology: fractional Brownian motion, Lévy flights Anomalous diffusion in biology: fractional Brownian motion, Lévy flights Jan Korbel Faculty of Nuclear Sciences and Physical Engineering, CTU, Prague Minisymposium on fundamental aspects behind cell systems

More information

Lecture 20 Optical Characterization 2

Lecture 20 Optical Characterization 2 Lecture 20 Optical Characterization 2 Schroder: Chapters 2, 7, 10 1/68 Announcements Homework 5/6: Is online now. Due Wednesday May 30th at 10:00am. I will return it the following Wednesday (6 th June).

More information

Registration of CBS Effects from Wedge-shaped Samples Containing Particles of Alumina

Registration of CBS Effects from Wedge-shaped Samples Containing Particles of Alumina VII International Conference on Photonics and Information Optics Volume 2018 Conference Paper Registration of CBS Effects from Wedge-shaped Samples Containing Particles of Alumina Sh. M. ISMAILOV 1,2 and

More information

Brewster Angle and Total Internal Reflection

Brewster Angle and Total Internal Reflection Lecture 5: Polarization Outline 1 Polarized Light in the Universe 2 Brewster Angle and Total Internal Reflection 3 Descriptions of Polarized Light 4 Polarizers 5 Retarders Christoph U. Keller, Leiden University,

More information

Simulation of Quantum Transport in Periodic and Disordered Systems with Ultracold Atoms

Simulation of Quantum Transport in Periodic and Disordered Systems with Ultracold Atoms Simulation of Quantum Transport in Periodic and Disordered Systems with Ultracold Atoms Laurent Sanchez-Palencia Center for Theoretical Physics Ecole Polytechnique, CNRS, Univ. Paris-Saclay F-91128 Palaiseau,

More information

QUANTUM- CLASSICAL ANALOGIES

QUANTUM- CLASSICAL ANALOGIES D. Dragoman M. Dragoman QUANTUM- CLASSICAL ANALOGIES With 78 Figures ^Ü Springer 1 Introduction 1 2 Analogies Between Ballistic Electrons and Electromagnetic Waves 9 2.1 Analog Parameters for Ballistic

More information

Towards quantum metrology with N00N states enabled by ensemble-cavity interaction. Massachusetts Institute of Technology

Towards quantum metrology with N00N states enabled by ensemble-cavity interaction. Massachusetts Institute of Technology Towards quantum metrology with N00N states enabled by ensemble-cavity interaction Hao Zhang Monika Schleier-Smith Robert McConnell Jiazhong Hu Vladan Vuletic Massachusetts Institute of Technology MIT-Harvard

More information

Nanocomposite photonic crystal devices

Nanocomposite photonic crystal devices Nanocomposite photonic crystal devices Xiaoyong Hu, Cuicui Lu, Yulan Fu, Yu Zhu, Yingbo Zhang, Hong Yang, Qihuang Gong Department of Physics, Peking University, Beijing, P. R. China Contents Motivation

More information

Recurrent scattering and memory effect at the Anderson transition

Recurrent scattering and memory effect at the Anderson transition Recurrent scattering and memory effect at the Anderson transition Alexandre Aubry Institut Langevin CNRS UMR 7587, ESPCI ParisTech Paris, France Collaborators: John Page, Laura Cobus (University of Manitoba,

More information

EE 5345 Biomedical Instrumentation Lecture 6: slides

EE 5345 Biomedical Instrumentation Lecture 6: slides EE 5345 Biomedical Instrumentation Lecture 6: slides 129-147 Carlos E. Davila, Electrical Engineering Dept. Southern Methodist University slides can be viewed at: http:// www.seas.smu.edu/~cd/ee5345.html

More information

Optical and Photonic Glasses. Lecture 18. Rayleigh and Mie Scattering, Colloidal Metals and Photo-elastic Properties. Professor Rui Almeida

Optical and Photonic Glasses. Lecture 18. Rayleigh and Mie Scattering, Colloidal Metals and Photo-elastic Properties. Professor Rui Almeida Optical and Photonic Glasses : Rayleigh and Mie Scattering, Colloidal Metals and Photo-elastic Properties Professor Rui Almeida International Materials Institute For New Functionality in Glass Lehigh University

More information

Understanding Nanoplasmonics. Greg Sun University of Massachusetts Boston

Understanding Nanoplasmonics. Greg Sun University of Massachusetts Boston Understanding Nanoplasmonics Greg Sun University of Massachusetts Boston Nanoplasmonics Space 100pm 1nm 10nm 100nm 1μm 10μm 100μm 1ns 100ps 10ps Photonics 1ps 100fs 10fs 1fs Time Surface Plasmons Surface

More information

CHAPTER 6 Quantum Mechanics II

CHAPTER 6 Quantum Mechanics II CHAPTER 6 Quantum Mechanics II 6.1 6.2 6.3 6.4 6.5 6.6 6.7 The Schrödinger Wave Equation Expectation Values Infinite Square-Well Potential Finite Square-Well Potential Three-Dimensional Infinite-Potential

More information

Recent Advances on the Effective Optical Properties of Turbid Colloids. Rubén G. Barrera Instituto de Física, UNAM Mexico

Recent Advances on the Effective Optical Properties of Turbid Colloids. Rubén G. Barrera Instituto de Física, UNAM Mexico Recent Advances on the Effective Optical Properties of Turbid Colloids Rubén G. Barrera Instituto de Física, UNAM Mexico In In collaboration with: Augusto García Edahí Gutierrez Celia Sánchez Pérez Felipe

More information

MCRT L10: Scattering and clarification of astronomy/medical terminology

MCRT L10: Scattering and clarification of astronomy/medical terminology MCRT L10: Scattering and clarification of astronomy/medical terminology What does the scattering? Shape of scattering Sampling from scattering phase functions Co-ordinate frames Refractive index changes

More information

LIGHT CONTROLLED PHOTON TUNNELING. University of Maryland, College Park, MD Phone: , Fax: ,

LIGHT CONTROLLED PHOTON TUNNELING. University of Maryland, College Park, MD Phone: , Fax: , LIGHT CONTROLLED PHOTON TUNNELING Igor I. Smolyaninov 1), Anatoliy V. Zayats 2), and Christopher C. Davis 1) 1) Department of Electrical and Computer Engineering University of Maryland, College Park, MD

More information

Quantum imaging of faint objects

Quantum imaging of faint objects Italian Quantum Information Science Conference 008, Camerino Quantum imaging of faint objects Theory : Lucia Caspani, Enrico Brambilla, Luigi Lugiato, Alessandra Gatti Experiment: Ottavia Jederkiewicz,

More information

X-ray Intensity Fluctuation Spectroscopy. Mark Sutton McGill University

X-ray Intensity Fluctuation Spectroscopy. Mark Sutton McGill University X-ray Intensity Fluctuation Spectroscopy Mark Sutton McGill University McGill University Collaborators J-F. Pelletier K. Laaziri K. Hassani A. Fluerasu E. Dufresne G. Brown M. Grant Yale/MIT S. Mochrie

More information

Quantum simulation with SU(N) fermions: orbital magnetism and synthetic dimensions. Leonardo Fallani

Quantum simulation with SU(N) fermions: orbital magnetism and synthetic dimensions. Leonardo Fallani Quantum simulation with SU(N) fermions: orbital magnetism and synthetic dimensions Frontiers in Quantum Simulation with Cold Atoms, Seattle, April 1 st 2015 Leonardo Fallani Department of Physics and Astronomy

More information

Highly Efficient and Anomalous Charge Transfer in van der Waals Trilayer Semiconductors

Highly Efficient and Anomalous Charge Transfer in van der Waals Trilayer Semiconductors Highly Efficient and Anomalous Charge Transfer in van der Waals Trilayer Semiconductors Frank Ceballos 1, Ming-Gang Ju 2 Samuel D. Lane 1, Xiao Cheng Zeng 2 & Hui Zhao 1 1 Department of Physics and Astronomy,

More information

Lecture 4: Polarisation of light, introduction

Lecture 4: Polarisation of light, introduction Lecture 4: Polarisation of light, introduction Lecture aims to explain: 1. Light as a transverse electro-magnetic wave 2. Importance of polarisation of light 3. Linearly polarised light 4. Natural light

More information

Today: 5 July 2008 ٢

Today: 5 July 2008 ٢ Anderson localization M. Reza Rahimi Tabar IPM 5 July 2008 ١ Today: 5 July 2008 ٢ Short History of Anderson Localization ٣ Publication 1) F. Shahbazi, etal. Phys. Rev. Lett. 94, 165505 (2005) 2) A. Esmailpour,

More information

Lecture 10 Light-Matter Interaction Part 4 Surface Polaritons 2. EECS Winter 2006 Nanophotonics and Nano-scale Fabrication P.C.

Lecture 10 Light-Matter Interaction Part 4 Surface Polaritons 2. EECS Winter 2006 Nanophotonics and Nano-scale Fabrication P.C. Lecture 10 Light-Matter Interaction Part 4 Surface Polaritons 2 EECS 598-002 Winter 2006 Nanophotonics and Nano-scale Fabrication P.C.Ku Schedule for the rest of the semester Introduction to light-matter

More information

University of Lübeck, Medical Laser Center Lübeck GmbH Optical Coherence Tomography

University of Lübeck, Medical Laser Center Lübeck GmbH Optical Coherence Tomography University of Lübeck, Medical Laser Center Lübeck GmbH Optical Coherence Tomography 4. Functional OCT Dr. Gereon Hüttmann / 2009 Doppler OCT (D-OCT) & Polarizationsensitive OCT (PS-OCT) Photonics II, by

More information

Origin of Optical Enhancement by Metal Nanoparticles. Greg Sun University of Massachusetts Boston

Origin of Optical Enhancement by Metal Nanoparticles. Greg Sun University of Massachusetts Boston Origin of Optical Enhancement by Metal Nanoparticles Greg Sun University of Massachusetts Boston Nanoplasmonics Space 100pm 1nm 10nm 100nm 1μm 10μm 100μm Photonics 1ns 100ps 10ps 1ps 100fs 10fs 1fs Time

More information

LC circuit: Energy stored. This lecture reviews some but not all of the material that will be on the final exam that covers in Chapters

LC circuit: Energy stored. This lecture reviews some but not all of the material that will be on the final exam that covers in Chapters Disclaimer: Chapter 29 Alternating-Current Circuits (1) This lecture reviews some but not all of the material that will be on the final exam that covers in Chapters 29-33. LC circuit: Energy stored LC

More information

NETADIS Kick off meeting. Torino,3-6 february Payal Tyagi

NETADIS Kick off meeting. Torino,3-6 february Payal Tyagi NETADIS Kick off meeting Torino,3-6 february 2013 Payal Tyagi Outline My background Project: 1) Theoretical part a) Haus master equation and Hamiltonian b) First steps: - Modelling systems with disordered

More information

Anomalous Lévy diffusion: From the flight of an albatross to optical lattices. Eric Lutz Abteilung für Quantenphysik, Universität Ulm

Anomalous Lévy diffusion: From the flight of an albatross to optical lattices. Eric Lutz Abteilung für Quantenphysik, Universität Ulm Anomalous Lévy diffusion: From the flight of an albatross to optical lattices Eric Lutz Abteilung für Quantenphysik, Universität Ulm Outline 1 Lévy distributions Broad distributions Central limit theorem

More information

X-ray Photon Correlation Spectroscopy (XPCS) at Synchrotron and FEL sources

X-ray Photon Correlation Spectroscopy (XPCS) at Synchrotron and FEL sources X-ray Photon Correlation Spectroscopy (XPCS) at Synchrotron and FEL sources Christian Gutt Department of Physics, University ofsiegen, Germany gutt@physik.uni-siegen.de Outline How to measure dynamics

More information

Effect of nonlinearity on wave scattering and localization. Yuri S. Kivshar

Effect of nonlinearity on wave scattering and localization. Yuri S. Kivshar Effect of nonlinearity on wave scattering and localization Yuri S. Kivshar Nonlinear Physics Centre, Australian National University, Canberra, Australia St. Petersburg University of Information Technologies,

More information

Theory of fractional Lévy diffusion of cold atoms in optical lattices

Theory of fractional Lévy diffusion of cold atoms in optical lattices Theory of fractional Lévy diffusion of cold atoms in optical lattices, Erez Aghion, David Kessler Bar-Ilan Univ. PRL, 108 230602 (2012) PRX, 4 011022 (2014) Fractional Calculus, Leibniz (1695) L Hospital:

More information

Photonic Communications Engineering I

Photonic Communications Engineering I Photonic Communications Engineering I Module 3 - Attenuation in Optical Fibers Alan E. Willner Professor, Dept. of Electrical Engineering - Systems, University of Southern California and Thrust 1 Lead

More information

Name : Roll No. :.... Invigilator s Signature :.. CS/B.Tech (NEW)/SEM-2/PH-201/2013 2013 PHYSICS - I Time Allotted : 3 Hours Full Marks : 70 The figures in the margin indicate full marks. Candidates are

More information

Light Interaction with Small Structures

Light Interaction with Small Structures Light Interaction with Small Structures Molecules Light scattering due to harmonically driven dipole oscillator Nanoparticles Insulators Rayleigh Scattering (blue sky) Semiconductors...Resonance absorption

More information

ME equations. Cylindrical symmetry. Bessel functions 1 kind Bessel functions 2 kind Modifies Bessel functions 1 kind Modifies Bessel functions 2 kind

ME equations. Cylindrical symmetry. Bessel functions 1 kind Bessel functions 2 kind Modifies Bessel functions 1 kind Modifies Bessel functions 2 kind Δϕ=0 ME equations ( 2 ) Δ + k E = 0 Quasi static approximation Dynamic approximation Cylindrical symmetry Metallic nano wires Nano holes in metals Bessel functions 1 kind Bessel functions 2 kind Modifies

More information

Nature of diffraction. Diffraction

Nature of diffraction. Diffraction Nature of diffraction Diffraction From Grimaldi to Maxwell Definition of diffraction diffractio, Francesco Grimaldi (1665) The effect is a general characteristics of wave phenomena occurring whenever a

More information

Time-of-Flight PET using Cherenkov Photons Produced in PbF 2

Time-of-Flight PET using Cherenkov Photons Produced in PbF 2 Photons Produced in PbF 2 R. Dolenec a, S. Korpar b,a, P. Križan c,a, R. Pestotnik a, A. Stanovnik d,a a, Ljubljana, Slovenia b Faculty of Chemistry and Chemical Engineering, University of Maribor, Slovenia

More information

Local time path integrals and their application to Lévy random walks

Local time path integrals and their application to Lévy random walks Local time path integrals and their application to Lévy random walks Václav Zatloukal (www.zatlovac.eu) Faculty of Nuclear Sciences and Physical Engineering Czech Technical University in Prague talk given

More information