Nonlinear Optics Tobias J. Kippenberg

Slides:



Advertisements
Similar presentations
Nonlinear Optical Microscopy. X Y Non-linear? Actual response can be written as y = c 1 x+ c 3 x 3 (this is called a cubic distortion) Assuming the input.
Advertisements

Key CLARITY technologies II – Four-Wave Mixing wavelength conversion National and Kapodistrian University of Athens Department of Informatics and Telecommunications.
Multi-wave Mixing In this lecture a selection of phenomena based on the mixing of two or more waves to produce a new wave with a different frequency, direction.
Multiwave stimulated Raman scattering with quasi-phase matching Victor G. Bespalov Russian Research Center "S. I. Vavilov State Optical Institute" Nikolai.
Fundamentals of Photonics
Chapter 1 Electromagnetic Fields
Interaction of Electromagnetic Radiation with Matter
S Digital Communication Systems Fiber-optic Communications - Supplementary.
Observation of the relativistic cross-phase modulation in a high intensity laser plasma interaction Shouyuan Chen, Matt Rever, Ping Zhang, Wolfgang Theobald,
Quasi-phase matching SRS generation. Nikolai S. Makarov, State Institute of Fine Mechanics and Optics, Victor G. Bespalov, Russian Research Center "S.
The Sum Over States model, although exact, requires a detailed knowledge of many parameters which are not generally available. Experience has shown that.
Resonances and optical constants of dielectrics: basic light-matter interaction.
Optical Engineering for the 21st Century: Microscopic Simulation of Quantum Cascade Lasers M.F. Pereira Theory of Semiconductor Materials and Optics Materials.
Fundamentals of Photonics 1 NONLINEAR OPTICS- III.
Optical Field Mixing. Oscillating Polarisation Optical polarisation Fundamental polarisation SH Polarisation Constant (dc) polarisation.
EE 230: Optical Fiber Communication Lecture 6 From the movie Warriors of the Net Nonlinear Processes in Optical Fibers.
2. Nonlinear Systems. Part I 1.Nonlinear Mechanics 2.Competition Phenomena 3.Nonlinear Electrical Phenomena 4.Chemical and Other Oscillators.
Polarization-Insensitive Cross Correlation Using Two-Photon Absorption in a Silicon Photodiode Pape Sylla.
2.3. Nonlinear Electrical Phenomena
CHEM 515 Spectroscopy Lecture # 1.
Lattice Vibrations – Phonons in Solids Alex Mathew University of Rochester.
Fiber-Optic Communications James N. Downing. Chapter 2 Principles of Optics.
WHY ???? Ultrashort laser pulses. (Very) High field physics Highest peak power, requires highest concentration of energy E L I Create … shorter pulses.
2. Centre de PhysiqueThéorique 1. DAM; Bruyères-le-Châtel DCSA 1. : M. Casanova 1., 2. : Thomas Fouquet 2. : S. Hüller, D. Pesme HEDP Summer School UC.
MSEG 667 Nanophotonics: Materials and Devices 8: Nonlinear Optics
LESSON 4 METO 621. The extinction law Consider a small element of an absorbing medium, ds, within the total medium s.
All-Fiber Optical Parametric Oscillator (FOPO) Chengao Wang.
Nonlinear Optics: Phenomena, Materials and Devices -Honors senior undergraduate and graduate level course. -Approximately lecture hours + 3 seminars.
Nonlinear Optics Lab. Hanyang Univ. Chapter 3. Classical Theory of Absorption 3.1 Introduction Visible color of an object : Selective absorption, Scattering,
Motion of a mass at the end of a spring Differential equation for simple harmonic oscillation Amplitude, period, frequency and angular frequency Energetics.
Chapter 12. Multimode and Transient Oscillation
Ashida lab M1 toyota M. Cai, O.Painter, K. J. Vahala, Opt. Lett. 25, 1430 (2000). Fiber-coupled microsphere laser.
Chapter 8. Second-Harmonic Generation and Parametric Oscillation
Picosecond fiber laser for thin film micro-processing
Chapter 10. Laser Oscillation : Gain and Threshold
1 Chapter 3 Electromagnetic Theory, Photons and Light September 5,8 Electromagnetic waves 3.1 Basic laws of electromagnetic theory Lights are electromagnetic.
Adiabatic approximation
IPC Friedrich-Schiller-Universität Jena 1 ASP_MP_S2j Biophotonics Prof. Dr. Rainer Heintzmann Institut für Physikalische Chemie Friedrich-Schiller-Universität.
Linear optical properties of dielectrics
LECTURE-VI CONTENTS  NON LINEAR OPTICAL MATERIALS AND ITS APPLICATIONS.
IPC Friedrich-Schiller-Universität Jena 1 ASP_MP_S2j Biophotonics Prof. Dr. Rainer Heintzmann Institut für Physikalische Chemie Friedrich-Schiller-Universität.
Nonlinear Optics Lab. Hanyang Univ. Chapter 4. The Intensity-Dependent Refractive Index - Third order nonlinear effect - Mathematical description of the.
8. Propagation in Nonlinear Media Microscopic Description of Nonlinearity Anharmonic Oscillator. Use Lorentz model (electrons on a spring)
Introduction to materials physics #4
Introduction to materials physics #3
Observation of Raman Self-Focusing in an Alkali Vapor Cell Nicholas Proite, Brett Unks, Tyler Green, and Professor Deniz Yavuz.
10 Nonlinear Optics.
Announcements 1/18/12 Prayer. The electric field E, electrion polarization P, and electric susceptibility , are related through which equation? a. a.
Oscillations and Resonances PHYS 5306 Instructor : Charles Myles Lee, EunMo.
Lez. 6 - Fisica At. Mol. Spec Carlo Altucci Consorzio Nazionale Interuniversitario di Struttura della Materia – CNISM Dipartimento di Scienze.
5. Electromagnetic Optics. 5.1 ELECTROMAGNETIC THEORY OF LIGHT for the 6 components Maxwell Eq. onde Maxwell.
§8.4 SHG Inside the Laser Resonator
1 8 Chapter Survey Hagen- Rubens Model Continuum theory: limited to frequencies for which the atomistic structure of solids does not play a.
Topic report 2012 March 15 Raman gain & stimulated emission gain
The Interaction of Light and Matter: a and n
Chapter 1 Electromagnetic Fields
PHY 752 Solid State Physics
Nonlinear Optics Tobias J. Kippenberg
Multiwave quasi-phase matching stimulated Raman scattering with dispersion of Raman gain Nikolai S. Makarov Saint-Petersburg State Institute of Fine Mechanics.
Slow Light Photon Physics Anke Kuijk
Coherent Nonlinear Optics
Physics 111 Practice Problem Solutions 14 Oscillations SJ 8th Ed
Chapter 3 Electromagnetic Theory, Photons and Light
Squeezed Input Interferometer
LECTURE-VI CONTENTS NON LINEAR OPTICAL MATERIALS AND ITS APPLICATIONS.
Notes Over 7.4 Finding an Inverse Relation
The nature of light-matter interaction:
Fiber Laser Part 1.
9 Nonlinear Optics.
Presentation transcript:

Nonlinear Optics Tobias J. Kippenberg tjk@mpq.mpg.de T. Kippenberg (2006) Nonlinear Optics Tobias J. Kippenberg tjk@mpq.mpg.de T.W. Hänsch Division Lecture 17

Platzek Model of Raman scattering Damped Harmonic Oscillator Force due to an electric field Response to the E field Lecture 17

T. Kippenberg (2006) Raman susceptibility Lecture 17

Stokes Anti-Stokes Coupling Lecture 17

3rd Order Nonlinear Processes 1 2 3 Linear Susceptibility (refractive index, absorption) Second order nonlinearity (e.g. solids without inversion symmetry) Third order nonlinearity Lecture 17

Parametric Amplification in a X(3) Medium Lecture 16

Parametric Gain with XPM Equations of motion (for two pump fields F1, F2): Pump: Lecture 17

Coupled 3rd Order Equations Equations of motion for Stokes and Anti-Stokes: Lecture 17

Parametric Gain Lecture 17