Laser Physics OXFORD UNIVERSITY PRESS SIMON HOOKER COLIN WEBB. and. Department of Physics, University of Oxford

Size: px
Start display at page:

Download "Laser Physics OXFORD UNIVERSITY PRESS SIMON HOOKER COLIN WEBB. and. Department of Physics, University of Oxford"

Transcription

1 Laser Physics SIMON HOOKER and COLIN WEBB Department of Physics, University of Oxford OXFORD UNIVERSITY PRESS

2 Contents 1 Introduction 1.1 The laser 1.2 Electromagnetic radiation in a closed cavity The density of modes 1.3 Planck's law The energy density of blackbody radiation 2 The interaction of radiation and matter 2.1 The Einstein treatment Relations between the Einstein coefficients 2.2 Conditions for optical gain Conditions for steady-state inversion Necessary, but not sufficient condition 2.3 The semi-classical treatment ^ Outline Selection rules for electric dipole transitions 2.4 Atomic population kinetics^ Rate equations Semi-classical equations Validity of the rate-equation approach 3 Broadening mechanisms and lineshapes 3.1 Homogeneous broadening mechanisms Natural broadening Pressure broadening Phonon broadening 3.2 Inhomogeneous broadening mechanisms Doppler broadening Broadening in amorphous solids 3.3 The interaction of radiation and matter in the presence spectral broadening Homogeneously broadened transitions Inhomogeneously broadened atoms ^ 3.4 The formation of spectral lines: The Voigt profile^

3 viii contents 3.5 Other broadening effects Self-absorption 4 Light amplification by the stimulated emission of radiation 4.1 The optical gain cross-section Condition for optical gain Frequency dependence of the gain cross-section The gain coefficient Gain narrowing 4.2 Narrowband radiation Amplification of narrowband radiation Form of rate equations 4.3 Gain cross-section for inhomogeneous broadening* 4.4 Orders of magnitude 4.5 Absorption The absorption cross-section Self-absorption Radiation trapping 5 Gain saturation Saturation in a steady-state amplifier Homogeneous broadening Inhomogeneous broadening 1 ' Saturation in a homogeneously broadened pulsed amplifier* Design of laser amplifiers The laser oscillator Introduction Amplified spontaneous emission (ASE) lasers Optical cavities General considerations Low-loss (or 'stable') optical cavities High-loss (or 'unstable') optical cavities* Beam quality* The M 2 beam-propagation factor The approach to laser oscillation The 'cold' cavity The laser threshold condition Laser oscillation above threshold Condition for steady-state laser oscillation Homogeneously broadened systems 113

4 contents ix Inhomogeneously broadened systems^ 6.7 Output power Low-gain lasers High-gain lasers: the Rigrod analysis^ Output power in other cases 7 Solid-state lasers 7.1 General considerations Energy levels of ions doped in solid hosts ^ Radiative transitions* Non-radiative transitions* Line broadening* Three- and four-level systems Host materials Techniques for optical pumping 7.2 Nd 3+ :YAG and other trivalent rare-earth systems Energy-level structure Transition linewidth Nd:YAG laser Other crystalline hosts Nd:glass laser Erbium lasers Praseodymium ions 7.3 Ruby and other trivalent iron-group systems Energy-level structure* The ruby laser Alexandrite laser CnLiSAF and CnLiCAF Ti:sapphire 8 Dynamic cavity effects 8.1 Laser spiking and relaxation oscillations Rate-equation analysis Analysis of relaxation oscillations Numerical analysis of laser spiking 8.2 Q-switching Techniques for Q-switching Rate-equation analysis of Q-switching Comparison with numerical simulations 8.3 Modelocking General ideas Simple treatment of modelocking Active modelocking techniques Passive modelocking techniques

5 x contents 8.4 Other forms of pulsed output Semiconductor lasers Basic features of a typical semiconductor diode laser Review of semiconductor physics Band structure Density of states and the Fermi energy (T = OK) The Fermi-Dirac distribution {T ^ 0 K) Doped semiconductors Radiative transitions in semiconductors Gain at a p-i-n junction Gain in diode lasers Carrier and photon confinement: the double heterostructure Laser materials Quantum-well lasers 1 " Laser threshold Diode laser beam properties Beam shape Transverse modes of edge-emitting lasers Longitudinal modes of diode lasers Single longitudinal mode diode lasers Diode laser linewidth Tunable diode laser cavities^ Diode laser output power 1 " VCSEL lasers 1 " Strained-layer lasers Quantum cascade lasers 1^ Fibre lasers Optical fibres The importance of optical-fibre technology Optical-fibre properties: Ray optics Optical-fibre properties: Wave optics Dispersion in optical fibres Fabrication of optical fibres Fibre-optic components Wavelength bands for fibre-optic telecommunications Erbium-doped fibre amplifiers Energy levels and pumping schemes Gain spectra EDFA design and layout Fabrication of erbium-doped fibre amplifiers Fibre Raman amplifiers Introduction 285

6 contents xi Raman scattering Fibre Raman amplifiers Long-haul optical transmission systems High-power fibre lasers The revolution in fibre-laser performance Cladding-pumped fibre-laser design Materials and mechanisms of cladding-pumped fibre-laser systems High-power fibre lasers: Linewidth considerations High-power pulsed fibre lasers Large mode area (LMA) fibres Q-switched fibre lasers Oscillator-amplifier pulsed fibre lasers Applications of high-power fibre lasers Atomic gas lasers Discharge physics interlude Low-pressure and high-pressure discharges Low-pressure glow discharge Temperatures The steady-state positive column Ionization rates Excitation rates Second-kind or superelastic collisions Excited-state populations in low-pressure discharges The helium-neon laser Introduction Energy levels, transitions and excitation mechanisms Laser construction and operating parameters Output-power limitations of the He-Ne laser Applications of He-Ne lasers The argon-ion laser Introduction Energy levels, transitions and excitation mechanisms Laser construction and operating parameters Argon-ion laser: Power limitations Krypton-ion lasers Applications of ion lasers Infra-red molecular gas lasers Efficiency considerations Energy levels of atoms and molecules Quantum ratio 333

7 12.2 Partial population inversion between vibrational energy levels of molecules Physics of the C0 2 laser Levels and lifetimes The effect of adding N Effect of adding He CO2 laser parameters Low-pressure c.w. CO2 lasers High-pressure pulsed CO2 lasers Other types of C0 2 laser Gas-dynamic C0 2 lasers Waveguide C0 2 lasers Applications of CO2 lasers Ultraviolet molecular gas lasers The UV and VUV spectral regions Energy levels of diatomic molecules Separation of the overall wave function Vibrational eigenfunctions Electronic transitions in diatomic molecules: The Franck-Condon principle Absorption transitions The'Franck-Condon loop' The VUV hydrogen laser The UV nitrogen laser Excimer molecules Rare-gas excimer lasers Rare-gas halide excimer lasers Spectroscopy of the rare-gas halides Rare-gas halide laser design Pulse-length limitations of discharge-excited RGH lasers Cavity design and beam properties of RHG lasers Performance and applications of RGH excimer laser Dye lasers Introduction Dye molecules Energy levels and spectra of dye molecules in solution Energy-level scheme Singlet-singlet absorption Singlet-singlet emission spectra Triplet-triplet absorption Rate-equation models of dye laser kinetics 387

8 contents xiii 14.5 Pulsed dye lasers Flashlamp-pumped systems Dye lasers pumped by pulsed lasers Continuous-wave dye lasers Population kinetics Continuous waves dye laser design Solid-state dye lasers Applications of dye lasers Non-linear frequency conversion Introduction Linear optics of crystals Classes of anisotropic crystals Vectors Field directions for o- and e-rays in a uniaxial crystal Basics of non-linear optics Maxwell's equations for non-linear media Second-harmonic generation in anisotropic crystals The requirement for phase matching Phase-matching techniques Birefringent phase matching in uniaxial crystals Critical and non-critical phase matching Poynting vector walk-off in birefringent phase matching Other factors affecting SHG conversion efficiency Phase-matched SHG in biaxial crystals Birefringent materials for SHG Quasi-phase matching techniques SHG: practical aspects Three-wave mixing and third-harmonic generation (THG) Three-wave mixing processes in general Third-harmonic generation (THG) Optical parametric oscillators (OPOs) Parametric interactions Optical parametric oscillators (OPOs) Practical parametric devices Precision frequency control of lasers^ Frequency pulling Single longitudinal mode operation Short cavity Intra-cavity etalons Ring resonators Other techniques 440

9 xiv contents 16.3 Output linewidfh The Schawlow-Townes limit Practical limitations Intensity noise Frequency locking Locking to atomic or molecular transitions Locking to an external cavity Frequency combs Ultrafast lasers Propagation of ultrafast laser pulses in dispersive media The time-bandwidth product General considerations Propagation through a dispersive system Propagation of Gaussian pulses Non-linear effects: self-phase modulation and the B-integral Dispersion control Geometric dispersion control Chirped mirrors Pulse shaping Sources of ultrafast optical pulses Modelocked lasers Oscillators Chirped-pulse amplification (CPA) Measurement of ultrafast pulses Autocorrelators Methods for exact reconstruction of the pulse Short-wavelength lasers Definition of wavelength ranges Difficulties in achieving optical gain at short wavelengths Pump-power scaling General properties of short-wavelength lasers Travelling-wave pumping Threshold and saturation behaviour in an ASE laser Spectral width of the output Coherence properties of ASE lasers Laser-generated plasmas^ Inverse bremsstrahlung heating Generation of highly ionized plasmas from laser-solid interactions Optical field ionization Collisionally excited lasers 517

10 contents xv Ne-likeions t Ni-likeions t Methods of pumping Collisionally excited OFI lasers Recombination lasers H-like carbon OFI recombination lasers Other sources High-harmonic generation Free-electron lasers Appendix A: The semi-classical theory of the interaction of radiation and matter 548 A.l The amplitude equations 548 A. 1.1 Derivation of the amplitude equations 548 A. 1.2 Solution of the amplitude equations 550 A.2 Calculation of the Einstein B coefficient 551 A.2.1 Polarized atoms and radiation 551 A.2.2 Unpolarized atoms and/or radiation 553 A.2.3 Treatment of degeneracy 554 A.3 Relations between the Einstein coefficients 555 A.4 Validity of rate equations 555 Appendix B: The spectral Einstein coefficients 557 Appendix C: Kleinman's conjecture 560 Bibliography 563 Index 579

Lasers and Electro-optics

Lasers and Electro-optics Lasers and Electro-optics Second Edition CHRISTOPHER C. DAVIS University of Maryland III ^0 CAMBRIDGE UNIVERSITY PRESS Preface to the Second Edition page xv 1 Electromagnetic waves, light, and lasers 1

More information

ATOMIC AND LASER SPECTROSCOPY

ATOMIC AND LASER SPECTROSCOPY ALAN CORNEY ATOMIC AND LASER SPECTROSCOPY CLARENDON PRESS OXFORD 1977 Contents 1. INTRODUCTION 1.1. Planck's radiation law. 1 1.2. The photoelectric effect 4 1.3. Early atomic spectroscopy 5 1.4. The postulates

More information

LIST OF TOPICS BASIC LASER PHYSICS. Preface xiii Units and Notation xv List of Symbols xvii

LIST OF TOPICS BASIC LASER PHYSICS. Preface xiii Units and Notation xv List of Symbols xvii ate LIST OF TOPICS Preface xiii Units and Notation xv List of Symbols xvii BASIC LASER PHYSICS Chapter 1 An Introduction to Lasers 1.1 What Is a Laser? 2 1.2 Atomic Energy Levels and Spontaneous Emission

More information

Diode Lasers and Photonic Integrated Circuits

Diode Lasers and Photonic Integrated Circuits Diode Lasers and Photonic Integrated Circuits L. A. COLDREN S. W. CORZINE University of California Santa Barbara, California A WILEY-INTERSCIENCE PUBLICATION JOHN WILEY & SONS, INC. NEW YORK / CHICHESTER

More information

Engineering Medical Optics BME136/251 Winter 2017

Engineering Medical Optics BME136/251 Winter 2017 Engineering Medical Optics BME136/251 Winter 2017 Monday/Wednesday 2:00-3:20 p.m. Beckman Laser Institute Library, MSTB 214 (lab) Teaching Assistants (Office hours: Every Tuesday at 2pm outside of the

More information

Modern optics Lasers

Modern optics Lasers Chapter 13 Phys 322 Lecture 36 Modern optics Lasers Reminder: Please complete the online course evaluation Last lecture: Review discussion (no quiz) LASER = Light Amplification by Stimulated Emission of

More information

Distributed feedback semiconductor lasers

Distributed feedback semiconductor lasers Distributed feedback semiconductor lasers John Carroll, James Whiteaway & Dick Plumb The Institution of Electrical Engineers SPIE Optical Engineering Press 1 Preface Acknowledgments Principal abbreviations

More information

Quantum Electronics Laser Physics. Chapter 5. The Laser Amplifier

Quantum Electronics Laser Physics. Chapter 5. The Laser Amplifier Quantum Electronics Laser Physics Chapter 5. The Laser Amplifier 1 The laser amplifier 5.1 Amplifier Gain 5.2 Amplifier Bandwidth 5.3 Amplifier Phase-Shift 5.4 Amplifier Power source and rate equations

More information

Fundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009

Fundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009 Fundamentals of Spectroscopy for Optical Remote Sensing Course Outline 2009 Part I. Fundamentals of Quantum Mechanics Chapter 1. Concepts of Quantum and Experimental Facts 1.1. Blackbody Radiation and

More information

Chemistry Instrumental Analysis Lecture 5. Chem 4631

Chemistry Instrumental Analysis Lecture 5. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 5 Light Amplification by Stimulated Emission of Radiation High Intensities Narrow Bandwidths Coherent Outputs Applications CD/DVD Readers Fiber Optics Spectroscopy

More information

Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p.

Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p. Preface p. xiii Fiber Gratings p. 1 Basic Concepts p. 1 Bragg Diffraction p. 2 Photosensitivity p. 3 Fabrication Techniques p. 4 Single-Beam Internal Technique p. 4 Dual-Beam Holographic Technique p. 5

More information

Optics, Optoelectronics and Photonics

Optics, Optoelectronics and Photonics Optics, Optoelectronics and Photonics Engineering Principles and Applications Alan Billings Emeritus Professor, University of Western Australia New York London Toronto Sydney Tokyo Singapore v Contents

More information

Optics, Light and Lasers

Optics, Light and Lasers Dieter Meschede Optics, Light and Lasers The Practical Approach to Modern Aspects of Photonics and Laser Physics Second, Revised and Enlarged Edition BICENTENNIAL.... n 4 '':- t' 1 8 0 7 $W1LEY 2007 tri

More information

Elements of Quantum Optics

Elements of Quantum Optics Pierre Meystre Murray Sargent III Elements of Quantum Optics Fourth Edition With 124 Figures fya Springer Contents 1 Classical Electromagnetic Fields 1 1.1 Maxwell's Equations in a Vacuum 2 1.2 Maxwell's

More information

Signal regeneration - optical amplifiers

Signal regeneration - optical amplifiers Signal regeneration - optical amplifiers In any atom or solid, the state of the electrons can change by: 1) Stimulated absorption - in the presence of a light wave, a photon is absorbed, the electron is

More information

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful Main Requirements of the Laser Optical Resonator Cavity Laser Gain Medium of 2, 3 or 4 level types in the Cavity Sufficient means of Excitation (called pumping) eg. light, current, chemical reaction Population

More information

Figure 1 Relaxation processes within an excited state or the ground state.

Figure 1 Relaxation processes within an excited state or the ground state. Excited State Processes and Application to Lasers The technology of the laser (Light Amplified by Stimulated Emission of Radiation) was developed in the early 1960s. The technology is based on an understanding

More information

What Makes a Laser Light Amplification by Stimulated Emission of Radiation Main Requirements of the Laser Laser Gain Medium (provides the light

What Makes a Laser Light Amplification by Stimulated Emission of Radiation Main Requirements of the Laser Laser Gain Medium (provides the light What Makes a Laser Light Amplification by Stimulated Emission of Radiation Main Requirements of the Laser Laser Gain Medium (provides the light amplification) Optical Resonator Cavity (greatly increase

More information

PROBLEMS IN LASER PHYSICS

PROBLEMS IN LASER PHYSICS PROBLEMS IN LASER PHYSICS PROBLEMS IN LASER PHYSICS G. Cerullo, s. Longhi, M. Nisoli, s. Stagira, and o. Svelto Politecnico di Milano Milano, ltaly SPRINGER SCIENCE+BUSINESS MEDIA, LLC Library of Congress

More information

Instructor: Welcome to. Phys 774: Principles of Spectroscopy. Fall How can we produce EM waves? Spectrum of Electromagnetic Radiation and Light

Instructor: Welcome to. Phys 774: Principles of Spectroscopy. Fall How can we produce EM waves? Spectrum of Electromagnetic Radiation and Light Welcome to Phys 774: Principles of Spectroscopy Fall 2007 Instructor: Andrei Sirenko Associate Professor at the Dept. of Physics, NJIT http://web.njit.edu/~sirenko 476 Tiernan Office hours: After the classes

More information

Stimulated Emission. Electrons can absorb photons from medium. Accelerated electrons emit light to return their ground state

Stimulated Emission. Electrons can absorb photons from medium. Accelerated electrons emit light to return their ground state Lecture 15 Stimulated Emission Devices- Lasers Stimulated emission and light amplification Einstein coefficients Optical fiber amplifiers Gas laser and He-Ne Laser The output spectrum of a gas laser Laser

More information

Stimulated Emission Devices: LASERS

Stimulated Emission Devices: LASERS Stimulated Emission Devices: LASERS 1. Stimulated Emission and Photon Amplification E 2 E 2 E 2 hυ hυ hυ In hυ Out hυ E 1 E 1 E 1 (a) Absorption (b) Spontaneous emission (c) Stimulated emission The Principle

More information

Chapter9. Amplification of light. Lasers Part 2

Chapter9. Amplification of light. Lasers Part 2 Chapter9. Amplification of light. Lasers Part 06... Changhee Lee School of Electrical and Computer Engineering Seoul National Univ. chlee7@snu.ac.kr /9 9. Stimulated emission and thermal radiation The

More information

Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy

Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy Model Answer (Paper code: AR-7112) M. Sc. (Physics) IV Semester Paper I: Laser Physics and Spectroscopy Section I Q1. Answer (i) (b) (ii) (d) (iii) (c) (iv) (c) (v) (a) (vi) (b) (vii) (b) (viii) (a) (ix)

More information

Lasers... the optical cavity

Lasers... the optical cavity Lasers... the optical cavity history principle, intuitive aspects, characteristics 2 levels systems Ti: Helium Al2O3 - Neon model-locked laser laser VCSEL bragg mirrors cleaved facets 13 ptical and/or

More information

Chapter-4 Stimulated emission devices LASERS

Chapter-4 Stimulated emission devices LASERS Semiconductor Laser Diodes Chapter-4 Stimulated emission devices LASERS The Road Ahead Lasers Basic Principles Applications Gas Lasers Semiconductor Lasers Semiconductor Lasers in Optical Networks Improvement

More information

Materialwissenschaft und Nanotechnologie. Introduction to Lasers

Materialwissenschaft und Nanotechnologie. Introduction to Lasers Materialwissenschaft und Nanotechnologie Introduction to Lasers Dr. Andrés Lasagni Lehrstuhl für Funktionswerkstoffe Sommersemester 007 1-Introduction to LASER Contents: Light sources LASER definition

More information

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful

Laser Types Two main types depending on time operation Continuous Wave (CW) Pulsed operation Pulsed is easier, CW more useful What Makes a Laser Light Amplification by Stimulated Emission of Radiation Main Requirements of the Laser Laser Gain Medium (provides the light amplification) Optical Resonator Cavity (greatly increase

More information

Wolfgang Demtroder. Laser Spectroscopy. Basic Concepts and Instrumentation. Second Enlarged Edition With 644 Figures and 91 Problems.

Wolfgang Demtroder. Laser Spectroscopy. Basic Concepts and Instrumentation. Second Enlarged Edition With 644 Figures and 91 Problems. Wolfgang Demtroder Laser Spectroscopy Basic Concepts and Instrumentation Second Enlarged Edition With 644 Figures and 91 Problems Springer Contents 1. Introduction 1 2. Absorption and Emission of Light

More information

CONTENTS. vii. CHAPTER 2 Operators 15

CONTENTS. vii. CHAPTER 2 Operators 15 CHAPTER 1 Why Quantum Mechanics? 1 1.1 Newtonian Mechanics and Classical Electromagnetism 1 (a) Newtonian Mechanics 1 (b) Electromagnetism 2 1.2 Black Body Radiation 3 1.3 The Heat Capacity of Solids and

More information

X-Rays From Laser Plasmas

X-Rays From Laser Plasmas X-Rays From Laser Plasmas Generation and Applications I. C. E. TURCU CLRC Rutherford Appleton Laboratory, UK and J. B. DANCE JOHN WILEY & SONS Chichester New York Weinheim Brisbane Singapore Toronto Contents

More information

Introduction Fundamentals of laser Types of lasers Semiconductor lasers

Introduction Fundamentals of laser Types of lasers Semiconductor lasers Introduction Fundamentals of laser Types of lasers Semiconductor lasers Is it Light Amplification and Stimulated Emission Radiation? No. So what if I know an acronym? What exactly is Light Amplification

More information

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626

OPTI510R: Photonics. Khanh Kieu College of Optical Sciences, University of Arizona Meinel building R.626 OPTI510R: Photonics Khanh Kieu College of Optical Sciences, University of Arizona kkieu@optics.arizona.edu Meinel building R.626 Announcements HW #5 due today April 11 th class will be at 2PM instead of

More information

F.G. Major. The Quantum Beat. The Physical Principles of Atomic Clocks. With 230 Illustrations. Springer

F.G. Major. The Quantum Beat. The Physical Principles of Atomic Clocks. With 230 Illustrations. Springer F.G. Major The Quantum Beat The Physical Principles of Atomic Clocks With 230 Illustrations Springer Contents Preface Chapter 1. Celestial and Mechanical Clocks 1 1.1 Cyclic Events in Nature 1 1.2 The

More information

Phys 2310 Fri. Dec. 12, 2014 Today s Topics. Begin Chapter 13: Lasers Reading for Next Time

Phys 2310 Fri. Dec. 12, 2014 Today s Topics. Begin Chapter 13: Lasers Reading for Next Time Phys 2310 Fri. Dec. 12, 2014 Today s Topics Begin Chapter 13: Lasers Reading for Next Time 1 Reading this Week By Fri.: Ch. 13 (13.1, 13.3) Lasers, Holography 2 Homework this Week No Homework this chapter.

More information

Paper B2: Radiation and Matter - Basic Laser Physics

Paper B2: Radiation and Matter - Basic Laser Physics Paper B2: Radiation and Matter - Basic Laser Physics Dr Simon Hooker Michaelmas Term 2006 ii Contents 1 The Interaction of Radiation and Matter 1 1.1 Introduction.............................. 1 1.2 Radiation...............................

More information

Principles of Lasers FIFTH EDITION

Principles of Lasers FIFTH EDITION Principles of Lasers FIFTH EDITION Principles of Lasers FIFTH EDITION Orazio Svelto Polytechnic Institute of Milan and National Research Council Milan, Italy Translated from Italian and edited by David

More information

Introduction to Semiconductor Integrated Optics

Introduction to Semiconductor Integrated Optics Introduction to Semiconductor Integrated Optics Hans P. Zappe Artech House Boston London Contents acknowledgments reface itroduction Chapter 1 Basic Electromagnetics 1 1.1 General Relationships 1 1.1.1

More information

Contents. Part I Fundamentals of Lasers 1 Introduction... 3

Contents. Part I Fundamentals of Lasers 1 Introduction... 3 Contents Part I Fundamentals of Lasers 1 Introduction... 3 2 Basic Optics... 9 2.1 Introduction...... 9 2.2 TheWaveEquation... 9 2.3 Linearly Polarized Waves.... 13 2.4 Circularly and Elliptically Polarized

More information

Unit-2 LASER. Syllabus: Properties of lasers, types of lasers, derivation of Einstein A & B Coefficients, Working He-Ne and Ruby lasers.

Unit-2 LASER. Syllabus: Properties of lasers, types of lasers, derivation of Einstein A & B Coefficients, Working He-Ne and Ruby lasers. Unit-2 LASER Syllabus: Properties of lasers, types of lasers, derivation of Einstein A & B Coefficients, Working He-Ne and Ruby lasers. Page 1 LASER: The word LASER is acronym for light amplification by

More information

Quantum Dot Lasers. Jose Mayen ECE 355

Quantum Dot Lasers. Jose Mayen ECE 355 Quantum Dot Lasers Jose Mayen ECE 355 Overview of Presentation Quantum Dots Operation Principles Fabrication of Q-dot lasers Advantages over other lasers Characteristics of Q-dot laser Types of Q-dot lasers

More information

(b) Spontaneous emission. Absorption, spontaneous (random photon) emission and stimulated emission.

(b) Spontaneous emission. Absorption, spontaneous (random photon) emission and stimulated emission. Lecture 10 Stimulated Emission Devices Lasers Stimulated emission and light amplification Einstein coefficients Optical fiber amplifiers Gas laser and He-Ne Laser The output spectrum of a gas laser Laser

More information

LASERS. Amplifiers: Broad-band communications (avoid down-conversion)

LASERS. Amplifiers: Broad-band communications (avoid down-conversion) L- LASERS Representative applications: Amplifiers: Broad-band communications (avoid down-conversion) Oscillators: Blasting: Energy States: Hydrogen atom Frequency/distance reference, local oscillators,

More information

THETOPPERSWAY.COM. Laser System. Principle of Lasers. Spontaneous Emission and Stimulated Emission. Page 1

THETOPPERSWAY.COM. Laser System. Principle of Lasers. Spontaneous Emission and Stimulated Emission. Page 1 LASER is the abbreviation of Light Amplification by the Stimulated Emission of Radiation. It is a device that creates a narrow and low-divergent beam of coherent light, while most other light sources emit

More information

L.A.S.E.R. LIGHT AMPLIFICATION. EMISSION of RADIATION

L.A.S.E.R. LIGHT AMPLIFICATION. EMISSION of RADIATION Lasers L.A.S.E.R. LIGHT AMPLIFICATION by STIMULATED EMISSION of RADIATION History of Lasers and Related Discoveries 1917 Stimulated emission proposed by Einstein 1947 Holography (Gabor, Physics Nobel Prize

More information

Phys 2310 Mon. Dec. 4, 2017 Today s Topics. Begin supplementary material: Lasers Reading for Next Time

Phys 2310 Mon. Dec. 4, 2017 Today s Topics. Begin supplementary material: Lasers Reading for Next Time Phys 2310 Mon. Dec. 4, 2017 Today s Topics Begin supplementary material: Lasers Reading for Next Time 1 By Wed.: Reading this Week Lasers, Holography 2 Homework this Week No Homework this chapter. Finish

More information

Lasers & Holography. Ulrich Heintz Brown University. 4/5/2016 Ulrich Heintz - PHYS 1560 Lecture 10 1

Lasers & Holography. Ulrich Heintz Brown University. 4/5/2016 Ulrich Heintz - PHYS 1560 Lecture 10 1 Lasers & Holography Ulrich Heintz Brown University 4/5/2016 Ulrich Heintz - PHYS 1560 Lecture 10 1 Lecture schedule Date Topic Thu, Jan 28 Introductory meeting Tue, Feb 2 Safety training Thu, Feb 4 Lab

More information

EE 472 Solutions to some chapter 4 problems

EE 472 Solutions to some chapter 4 problems EE 472 Solutions to some chapter 4 problems 4.4. Erbium doped fiber amplifier An EDFA is pumped at 1480 nm. N1 and N2 are the concentrations of Er 3+ at the levels E 1 and E 2 respectively as shown in

More information

Abstract... I. Acknowledgements... III. Table of Content... V. List of Tables... VIII. List of Figures... IX

Abstract... I. Acknowledgements... III. Table of Content... V. List of Tables... VIII. List of Figures... IX Abstract... I Acknowledgements... III Table of Content... V List of Tables... VIII List of Figures... IX Chapter One IR-VUV Photoionization Spectroscopy 1.1 Introduction... 1 1.2 Vacuum-Ultraviolet-Ionization

More information

OPTICAL GAIN AND LASERS

OPTICAL GAIN AND LASERS OPTICAL GAIN AND LASERS 01-02-1 BY DAVID ROCKWELL DIRECTOR, RESEARCH & DEVELOPMENT fsona COMMUNICATIONS MARCH 6, 2001 OUTLINE 01-02-2 I. DEFINITIONS, BASIC CONCEPTS II. III. IV. OPTICAL GAIN AND ABSORPTION

More information

Emission Spectra of the typical DH laser

Emission Spectra of the typical DH laser Emission Spectra of the typical DH laser Emission spectra of a perfect laser above the threshold, the laser may approach near-perfect monochromatic emission with a spectra width in the order of 1 to 10

More information

A Guide to Experiments in Quantum Optics

A Guide to Experiments in Quantum Optics Hans-A. Bachor and Timothy C. Ralph A Guide to Experiments in Quantum Optics Second, Revised and Enlarged Edition WILEY- VCH WILEY-VCH Verlag CmbH Co. KGaA Contents Preface 1 Introduction 1.1 Historical

More information

Ho:YLF pumped HBr laser

Ho:YLF pumped HBr laser Ho:YLF pumped HBr laser L R Botha, 1,2,* C Bollig, 1 M J D Esser, 1 R N Campbell 4, C Jacobs 1,3 and D R Preussler 1 1 National Laser Centre, CSIR, Pretoria, South Africa 2 Laser Research Institute, Department

More information

Stimulated Emission. ! Electrons can absorb photons from medium. ! Accelerated electrons emit light to return their ground state

Stimulated Emission. ! Electrons can absorb photons from medium. ! Accelerated electrons emit light to return their ground state Lecture 15 Stimulated Emission Devices- Lasers! Stimulated emission and light amplification! Einstein coefficients! Optical fiber amplifiers! Gas laser and He-Ne Laser! The output spectrum of a gas laser!

More information

In a metal, how does the probability distribution of an electron look like at absolute zero?

In a metal, how does the probability distribution of an electron look like at absolute zero? 1 Lecture 6 Laser 2 In a metal, how does the probability distribution of an electron look like at absolute zero? 3 (Atom) Energy Levels For atoms, I draw a lower horizontal to indicate its lowest energy

More information

Laserphysik. Prof. Yong Lei & Dr. Yang Xu. Fachgebiet Angewandte Nanophysik, Institut für Physik

Laserphysik. Prof. Yong Lei & Dr. Yang Xu. Fachgebiet Angewandte Nanophysik, Institut für Physik Laserphysik Prof. Yong Lei & Dr. Yang Xu Fachgebiet Angewandte Nanophysik, Institut für Physik Contact: yong.lei@tu-ilmenau.de; yang.xu@tu-ilmenau.de Office: Heisenbergbau V 202, Unterpörlitzer Straße

More information

Liquid Crystals IAM-CHOON 1(1100 .,4 WILEY 2007 WILEY-INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION. 'i; Second Edition. n z

Liquid Crystals IAM-CHOON 1(1100 .,4 WILEY 2007 WILEY-INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION. 'i; Second Edition. n z Liquid Crystals Second Edition IAM-CHOON 1(1100.,4 z 'i; BICENTCNNIAL 1 8 0 7 WILEY 2007 DICENTENNIAL n z z r WILEY-INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION Contents Preface xiii Chapter 1.

More information

MOLECULAR SPECTROSCOPY

MOLECULAR SPECTROSCOPY MOLECULAR SPECTROSCOPY First Edition Jeanne L. McHale University of Idaho PRENTICE HALL, Upper Saddle River, New Jersey 07458 CONTENTS PREFACE xiii 1 INTRODUCTION AND REVIEW 1 1.1 Historical Perspective

More information

F. Elohim Becerra Chavez

F. Elohim Becerra Chavez F. Elohim Becerra Chavez Email:fbecerra@unm.edu Office: P&A 19 Phone: 505 277-2673 Lectures: Monday and Wednesday, 5:30-6:45 pm P&A Room 184. Textbook: Many good ones (see webpage) Lectures follow order

More information

Modern Optical Spectroscopy

Modern Optical Spectroscopy Modern Optical Spectroscopy With Exercises and Examples from Biophysics and Biochemistry von William W Parson 1. Auflage Springer-Verlag Berlin Heidelberg 2006 Verlag C.H. Beck im Internet: www.beck.de

More information

Optical Characterization of Solids

Optical Characterization of Solids D. Dragoman M. Dragoman Optical Characterization of Solids With 184 Figures Springer 1. Elementary Excitations in Solids 1 1.1 Energy Band Structure in Crystalline Materials 2 1.2 k p Method 11 1.3 Numerical

More information

PRINCIPLES OF PHYSICAL OPTICS

PRINCIPLES OF PHYSICAL OPTICS PRINCIPLES OF PHYSICAL OPTICS C. A. Bennett University of North Carolina At Asheville WILEY- INTERSCIENCE A JOHN WILEY & SONS, INC., PUBLICATION CONTENTS Preface 1 The Physics of Waves 1 1.1 Introduction

More information

Optoelectronics ELEC-E3210

Optoelectronics ELEC-E3210 Optoelectronics ELEC-E3210 Lecture 3 Spring 2017 Semiconductor lasers I Outline 1 Introduction 2 The Fabry-Pérot laser 3 Transparency and threshold current 4 Heterostructure laser 5 Power output and linewidth

More information

Lasers E 6 E 4 E 3 E 2 E 1

Lasers E 6 E 4 E 3 E 2 E 1 Lasers Laser is an acronym for light amplification by stimulated emission of radiation. Here the process of stimulated emission is used to amplify light radiation. Spontaneous emission: When energy is

More information

Introduction to Laser Material Processing. ME 677: Laser Material Processing Instructor: Ramesh Singh 1

Introduction to Laser Material Processing. ME 677: Laser Material Processing Instructor: Ramesh Singh 1 Introduction to Laser Material Processing 1 Outline Brief History Design of Laser cavity Stability Types of Lasers 2 Laser History 1917 - Albert Einstein: Theoretical prediction of stimulated emission

More information

Chapter 5. Semiconductor Laser

Chapter 5. Semiconductor Laser Chapter 5 Semiconductor Laser 5.0 Introduction Laser is an acronym for light amplification by stimulated emission of radiation. Albert Einstein in 1917 showed that the process of stimulated emission must

More information

Steady state operation : g = 1

Steady state operation : g = 1 Laser = active medium + cavity L active medium R1 R2 47 47 Net gain per round trip L active medium R1 R2 losses gain (intrinsic) g Intensity after one round trip = = R1$ R2$ exp6 2^b-ah $ l@ I0 Steady

More information

Ar and Kr ion lasers

Ar and Kr ion lasers Types of Lasers Ar and Kr ion lasers Nd:YAG and Nd:YLF lasers CO 2 lasers Excimer lasers Dye lasers Transition metal lasers Optical parametric amplification Ar and Kr ion lasers Noble gas ions are created

More information

Figure 5.1: Theodore Maiman constructed the first operational laser. Wikipedia). 5.1 Emission and absorption of electromagnetic radiation

Figure 5.1: Theodore Maiman constructed the first operational laser. Wikipedia). 5.1 Emission and absorption of electromagnetic radiation 5 Laser The word laser is an acronym for light amplification by stimulated emission of radiation. The first laser was demonstrated by Theodore Maiman in 1960. Figure 5.1: Theodore Maiman constructed the

More information

Lecture 10. Lidar Effective Cross-Section vs. Convolution

Lecture 10. Lidar Effective Cross-Section vs. Convolution Lecture 10. Lidar Effective Cross-Section vs. Convolution q Introduction q Convolution in Lineshape Determination -- Voigt Lineshape (Lorentzian Gaussian) q Effective Cross Section for Single Isotope --

More information

SOLID STATE PHYSICS. Second Edition. John Wiley & Sons. J. R. Hook H. E. Hall. Department of Physics, University of Manchester

SOLID STATE PHYSICS. Second Edition. John Wiley & Sons. J. R. Hook H. E. Hall. Department of Physics, University of Manchester SOLID STATE PHYSICS Second Edition J. R. Hook H. E. Hall Department of Physics, University of Manchester John Wiley & Sons CHICHESTER NEW YORK BRISBANE TORONTO SINGAPORE Contents Flow diagram Inside front

More information

SOFT X-RAYS AND EXTREME ULTRAVIOLET RADIATION

SOFT X-RAYS AND EXTREME ULTRAVIOLET RADIATION SOFT X-RAYS AND EXTREME ULTRAVIOLET RADIATION Principles and Applications DAVID ATTWOOD UNIVERSITY OF CALIFORNIA, BERKELEY AND LAWRENCE BERKELEY NATIONAL LABORATORY CAMBRIDGE UNIVERSITY PRESS Contents

More information

External (differential) quantum efficiency Number of additional photons emitted / number of additional electrons injected

External (differential) quantum efficiency Number of additional photons emitted / number of additional electrons injected Semiconductor Lasers Comparison with LEDs The light emitted by a laser is generally more directional, more intense and has a narrower frequency distribution than light from an LED. The external efficiency

More information

P. W. Atkins and R. S. Friedman. Molecular Quantum Mechanics THIRD EDITION

P. W. Atkins and R. S. Friedman. Molecular Quantum Mechanics THIRD EDITION P. W. Atkins and R. S. Friedman Molecular Quantum Mechanics THIRD EDITION Oxford New York Tokyo OXFORD UNIVERSITY PRESS 1997 Introduction and orientation 1 Black-body radiation 1 Heat capacities 2 The

More information

Chapter 7: Optical Properties of Solids. Interaction of light with atoms. Insert Fig Allowed and forbidden electronic transitions

Chapter 7: Optical Properties of Solids. Interaction of light with atoms. Insert Fig Allowed and forbidden electronic transitions Chapter 7: Optical Properties of Solids Interaction of light with atoms Insert Fig. 8.1 Allowed and forbidden electronic transitions 1 Insert Fig. 8.3 or equivalent Ti 3+ absorption: e g t 2g 2 Ruby Laser

More information

PRINCIPLES OF NONLINEAR OPTICAL SPECTROSCOPY

PRINCIPLES OF NONLINEAR OPTICAL SPECTROSCOPY PRINCIPLES OF NONLINEAR OPTICAL SPECTROSCOPY Shaul Mukamel University of Rochester Rochester, New York New York Oxford OXFORD UNIVERSITY PRESS 1995 Contents 1. Introduction 3 Linear versus Nonlinear Spectroscopy

More information

Spectroscopy of. Semiconductors. Luminescence OXFORD IVAN PELANT. Academy ofsciences of the Czech Republic, Prague JAN VALENTA

Spectroscopy of. Semiconductors. Luminescence OXFORD IVAN PELANT. Academy ofsciences of the Czech Republic, Prague JAN VALENTA Luminescence Spectroscopy of Semiconductors IVAN PELANT Institute ofphysics, v.v.i. Academy ofsciences of the Czech Republic, Prague JAN VALENTA Department of Chemical Physics and Optics Charles University,

More information

Interested in exploring science or math teaching as a career?

Interested in exploring science or math teaching as a career? Interested in exploring science or math teaching as a career? Start with Step 1: EDUC 2020 (1 credit) Real experience teaching real kids! No commitment to continue with education courses Registration priority

More information

MODERN OPTICS. P47 Optics: Unit 9

MODERN OPTICS. P47 Optics: Unit 9 MODERN OPTICS P47 Optics: Unit 9 Course Outline Unit 1: Electromagnetic Waves Unit 2: Interaction with Matter Unit 3: Geometric Optics Unit 4: Superposition of Waves Unit 5: Polarization Unit 6: Interference

More information

Quantum Electronics Laser Physics PS Theory of the Laser Oscillation

Quantum Electronics Laser Physics PS Theory of the Laser Oscillation Quantum Electronics Laser Physics PS407 6. Theory of the Laser Oscillation 1 I. Laser oscillator: Overview Laser is an optical oscillator. Resonant optical amplifier whose output is fed back into its input

More information

All-Optical Delay with Large Dynamic Range Using Atomic Dispersion

All-Optical Delay with Large Dynamic Range Using Atomic Dispersion All-Optical Delay with Large Dynamic Range Using Atomic Dispersion M. R. Vanner, R. J. McLean, P. Hannaford and A. M. Akulshin Centre for Atom Optics and Ultrafast Spectroscopy February 2008 Motivation

More information

Photon Physics. Week 4 26/02/2013

Photon Physics. Week 4 26/02/2013 Photon Physics Week 4 6//13 1 Classical atom-field interaction Lorentz oscillator: Classical electron oscillator with frequency ω and damping constant γ Eqn of motion: Final result: Classical atom-field

More information

Molecular spectroscopy

Molecular spectroscopy Molecular spectroscopy Origin of spectral lines = absorption, emission and scattering of a photon when the energy of a molecule changes: rad( ) M M * rad( ' ) ' v' 0 0 absorption( ) emission ( ) scattering

More information

MEFT / Quantum Optics and Lasers. Suggested problems Set 4 Gonçalo Figueira, spring 2015

MEFT / Quantum Optics and Lasers. Suggested problems Set 4 Gonçalo Figueira, spring 2015 MEFT / Quantum Optics and Lasers Suggested problems Set 4 Gonçalo Figueira, spring 05 Note: some problems are taken or adapted from Fundamentals of Photonics, in which case the corresponding number is

More information

Laser-Based Measurements for Time and Frequency

Laser-Based Measurements for Time and Frequency Laser-Based Measurements for Time and Frequency Domain Applications A Handbook Pasquale Maddaloni Marco Bellini Paolo De Natale CRC Press Taylor Si Francis Croup Boca Raton London New York CRC Press is

More information

F. Elohim Becerra Chavez

F. Elohim Becerra Chavez F. Elohim Becerra Chavez Email:fbecerra@unm.edu Office: P&A 19 Phone: 505 277-2673 Lectures: Tuesday and Thursday, 9:30-10:45 P&A Room 184. Textbook: Laser Electronics (3rd Edition) by Joseph T. Verdeyen.

More information

-I (PH 6151) UNIT-V PHOTONICS AND FIBRE OPTICS

-I (PH 6151) UNIT-V PHOTONICS AND FIBRE OPTICS Engineering Physics -I (PH 6151) UNIT-V PHOTONICS AND FIBRE OPTICS Syllabus: Lasers Spontaneous and stimulated emission Population Inversion -Einstein s co-efficient (Derivation)- types of lasers-nd-yag,co

More information

Tentative Schedule: Date, Place & Time Topics Sep.4 (Mo) No classes Labor Day Holiday Exam 1 Exam 2 Over Chapters 4-6

Tentative Schedule: Date, Place & Time Topics Sep.4 (Mo) No classes Labor Day Holiday Exam 1 Exam 2 Over Chapters 4-6 Tentative Schedule: Date, Place & Time Topics 1 Aug. 8 (Mo) 394; 5:00-6:15 Introduction, Spontaneous and Stimulated Transitions (Ch. 1) Lecture Notes Aug. 30 (We) 394; 5:00-6:15 Spontaneous and Stimulated

More information

The Generation of Ultrashort Laser Pulses

The Generation of Ultrashort Laser Pulses The Generation of Ultrashort Laser Pulses The importance of bandwidth More than just a light bulb Two, three, and four levels rate equations Gain and saturation But first: the progress has been amazing!

More information

Semiconductor Lasers EECE 484. Winter Dr. Lukas Chrostowski

Semiconductor Lasers EECE 484. Winter Dr. Lukas Chrostowski Semiconductor Lasers EECE 484 Winter 2013 Dr. Lukas Chrostowski 1 484 - Course Information Web Page: http://siepic.ubc.ca/eece484 (password DBR, check for updates) + Piazza, https://piazza.com/ubc.ca/winterterm22013/eece484

More information

Other Devices from p-n junctions

Other Devices from p-n junctions Memory (5/7 -- Glenn Alers) Other Devices from p-n junctions Electron to Photon conversion devices LEDs and SSL (5/5) Lasers (5/5) Solid State Lighting (5/5) Photon to electron conversion devices Photodectors

More information

CHAPTER 13 Molecular Spectroscopy 2: Electronic Transitions

CHAPTER 13 Molecular Spectroscopy 2: Electronic Transitions CHAPTER 13 Molecular Spectroscopy 2: Electronic Transitions I. General Features of Electronic spectroscopy. A. Visible and ultraviolet photons excite electronic state transitions. ε photon = 120 to 1200

More information

Surface Plasmon Amplification by Stimulated Emission of Radiation. By: Jonathan Massey-Allard Graham Zell Justin Lau

Surface Plasmon Amplification by Stimulated Emission of Radiation. By: Jonathan Massey-Allard Graham Zell Justin Lau Surface Plasmon Amplification by Stimulated Emission of Radiation By: Jonathan Massey-Allard Graham Zell Justin Lau Surface Plasmons (SPs) Quanta of electron oscillations in a plasma. o Electron gas in

More information

What do we study and do?

What do we study and do? What do we study and do? Light comes from electrons transitioning from higher energy to lower energy levels. Wave-particle nature of light Wave nature: refraction, diffraction, interference (labs) Particle

More information

QUESTION BANK IN PHYSICS

QUESTION BANK IN PHYSICS QUESTION BANK IN PHYSICS LASERS. Name some properties, which make laser light different from ordinary light. () {JUN 5. The output power of a given laser is mw and the emitted wavelength is 630nm. Calculate

More information

Principles of Lasers. Cheng Wang. Phone: Office: SEM 318

Principles of Lasers. Cheng Wang. Phone: Office: SEM 318 Principles of Lasers Cheng Wang Phone: 20685263 Office: SEM 318 wangcheng1@shanghaitech.edu.cn The course 2 4 credits, 64 credit hours, 16 weeks, 32 lectures 70% exame, 30% project including lab Reference:

More information

Metal Vapour Lasers Use vapoured metal as a gain medium Developed by W. Silfvast (1966) Two types: Ionized Metal vapour (He-Cd) Neutral Metal vapour

Metal Vapour Lasers Use vapoured metal as a gain medium Developed by W. Silfvast (1966) Two types: Ionized Metal vapour (He-Cd) Neutral Metal vapour Metal Vapour Lasers Use vapoured metal as a gain medium Developed by W. Silfvast (1966) Two types: Ionized Metal vapour (He-Cd) Neutral Metal vapour (Cu) All operate by vaporizing metal in container Helium

More information

Unit I LASER Engineering Physics

Unit I LASER Engineering Physics Introduction LASER stands for light Amplification by Stimulated Emission of Radiation. The theoretical basis for the development of laser was provided by Albert Einstein in 1917. In 1960, the first laser

More information

Ms. Monika Srivastava Doctoral Scholar, AMR Group of Dr. Anurag Srivastava ABV-IIITM, Gwalior

Ms. Monika Srivastava Doctoral Scholar, AMR Group of Dr. Anurag Srivastava ABV-IIITM, Gwalior By Ms. Monika Srivastava Doctoral Scholar, AMR Group of Dr. Anurag Srivastava ABV-IIITM, Gwalior Unit 2 Laser acronym Laser Vs ordinary light Characteristics of lasers Different processes involved in lasers

More information

Light Emission. Today s Topics. Excitation/De-Excitation 10/26/2008. Excitation Emission Spectra Incandescence

Light Emission. Today s Topics. Excitation/De-Excitation 10/26/2008. Excitation Emission Spectra Incandescence Light Emission Excitation Emission Spectra Incandescence Absorption Spectra Today s Topics Excitation/De-Excitation Electron raised to higher energy level Electron emits photon when it drops back down

More information