Lecture 38 Lasers Final Exam next week. LASER L ight A mplification by S timulated E mission of R adiation.

Slides:



Advertisements
Similar presentations
Lasers 2.71/2.710 Optics (Laser lecture) 12/12/01-1.
Advertisements

Femtosecond lasers István Robel
Prof. Dr. Salah I. Hassab Elnaby
Chapter 30 Light Emission
LASER (semiconducting Lasers) LASER 1 EBB 424E Dr Zainovia Lockman.
Components of ultrafast laser system
May Chuck DiMarzio, Northeastern University ECE-1466 Modern Optics Course Notes Part 9 Prof. Charles A. DiMarzio Northeastern University.
PHYS 252 Lasers1 Lasers What is stimulated emission? Well, there are two types of light emission that can occur with atoms! The kind that we have been.
EE 230: Optical Fiber Communication Lecture 9 From the movie Warriors of the Net Light Sources.
Introduction to Lasers 자연과학부 나종훈. 목 차 LASER 의 시초 Atomic Structure Transitions between Laser states Population Inversion Pulsed Operation Power and Energy.
General Properties of Light Light as a wave Speed Wave properties: wavelength, frequency, period, speed, amplitude, intensity Electromagnetic wave.
Spectrophotometer Light Sources: Lasers. L.A.S.E.R. Acronym for: light amplification by stimulated emission of radiation Basic principle of lasing: population.
ight mplification of ight mplification of ight mplification of timulated ight mplification of timulated.
Light Amplification by Stimulated
Quantum Well Lasers Christopher P. Heagney Jason Yoo.
8. Optical Modulation. Modulation Techniques Direct modulation of laser diode –Vary the current supply to the laser diode –Directly modulates the output.
How Lasers Work. Lasers show up in an amazing range of products and technologies. You will find them in everything from CD players to dental drills to.
Ruby Laser Crystal structure of sapphire: -Al2O3 (aluminum oxide). The shaded atoms make up a unit cell of the structure. The aluminum atom inside the.
Laser (Light Amplification by Stimulated Emission of Radiation)
BASICS OF LASERS AND LASER LIGHT
EE 230: Optical Fiber Communication Lecture 7 From the movie Warriors of the Net Optical Amplifiers-the Basics.
1.3 Cavity modes Axial modes λ = 2d / n ν = nc / 2d n = 2d / λ
EM Radiation Sources 1. Fundamentals of EM Radiation 2. Light Sources
Dye lasers The gain medium in a dye lasers is a solution made with an organic dye molecule. The solution is intensely coloured owing to the very strong.
Some quantum properties of light Blackbody radiation to lasers.
Spectroscopy 2: Electronic Transitions CHAPTER 14.
1.2 Population inversion Absorption and Emission of radiation
Absorption and emission processes
Lasers. Spontaneous Emission  Atomic electrons can be excited by external radiation. EM wavesEM waves Electrons in a fieldElectrons in a field  Atoms.
Ultrafast Spectroscopy
The Amazing World of Lasers Alexey Belyanin Department of Physics, TAMU Laser Definition and History Laser Radiation Laser System –Active Medium and Pump.
1.4 Pulsed operation Normal pulsed mode In a normal-mode pulsed laser, pumping is usually via a short pulse that produces a short-lived population inversion.
LASERs Light Amplification by Stimulated Emission of Radiation.
Interference Diffraction and Lasers
Lasers, Yeah They Look Cool, But How Do They Work? Brought To You Buy: STEVE KESSLER & DANNY GOEPFERT.
Laser Principle Eman Ali Ateeq.
2010: A Laser Odyssey Short presentation about lasers by the Université Laval OSA and SPIE Student Chapters.
By Alex Ellis.
NOISE IN OPTICAL SYSTEMS F. X. Kärtner High-Frequency and Quantum Electronics Laboratory University of Karlsruhe.
An Introduction. The first step on the road to laser was the publication of paper by Albert Einstein in 1916 –describing how atoms could interact with.
ECE 455: Optical Electronics Lecture #9: Inhomogeneous Broadening, the Laser Equation, and Threshold Gain Substitute Lecturer: Tom Spinka Tuesday, Sept.
B.SC.II PAPER-B (OPTICS and LASERS)
PHYSICS DEPARTMENT.
4-Level Laser Scheme. He-Ne Laser Tunable Dye Lasers.
Lecture 6. Polarization splitter based Filters Acoustooptic Tunable Filters.
PROPERTIES OF LASER BEAMS  Laser beam is generated in a specific wave length by the interaction of electromagnetic wave with the active medium.  To represent.
Low-Power Lasers Jennifer L. Doherty-Restrepo, MS, ATC, LAT Entry-Level Master Athletic Training Education Program PET 4995: Therapeutic Modalities.
LASERS. LASER is an acronym for light amplification by Stimulated Emission of radiation. When radiation interacts with matter we have three processes.
1LASER is a short form of a) Light amplification by stimulated absorption radiation b) Light amplification by stimulated emission of radiation c) Light.
Optics Focus Confocal theory.
LIGHT AMPLIFICATION by STIMULATED ELECTRON RADIATION
Optical sources Types of optical sources
SHRI DADAJI INSTITUTE OF TECHNOLOGY & SCIENCE A SEMINAR ON LASER COMMUNICATION PRESENTED BY: HITESH SILARPURIYA E.C. FOURTH SEM.
Lasers. Question: In movies, laser beams are always shown as bright pencils of light streaking through the air or space. If you were to look from the.
 LIGHT  AMPLIFICATION BY  STIMULATED  EMISSION OF  RADIATION.
Lasers The final project Lukáš Jörka 3.C. Introduction The aim of my final project: o Analyse lasers from different viewpoints o Create an overall view.
Many-electron atoms CHAPTER 8 Many-electron atoms What distinguished Mendeleev was not only genius, but a passion for the elements. They became his personal.
Laserlaser. Laser printer Laser pointer Laser: everywhere in your life.
Laser transient induced by a pumping step t Ip Case of HeNe :  and  c same order of magnitude n0n0 Laser intensity  n th nn.
Laser.
Light-Matter Interaction
Light Amplification by Stimulated
Properties of Laser There are Severel Properties Of LASER which are defined as follows:- MONOCHROMATICITY COHERENCE DIRECTIONALITY BRIGHTNESS DIVERGENCE.
Lasers.
8.2.2 Fiber Optic Communications
LASER (semiconducting Lasers)
Principle of Mode Locking
Kansas Light Source Laser System J. R. Macdonald Laboratory
Lasers. You know magic and stuff
PRINCIPLE AND WORKING OF A SEMICONDUCTOR LASER
Presentation transcript:

Lecture 38 Lasers Final Exam next week

LASER L ight A mplification by S timulated E mission of R adiation

Electronic Energy Levels Energy e-e- e-e- Fluorescence or ‘Spontaneous Emission’ e-e- e-e-

Stimulated Emission Energy e-e- e-e- The stimulated emission has the same frequency and phase as the incoming photon

3 level system e-e- ‘Short’ lifetime ‘long’ lifetime

Stimulated Emission Light Amplifier Pump (does not need to be light) Gain medium can be gas, liquid, or solid All light is in phase and has the same frequency

Laser Cavity Once the amount of gain is equal to the cavity losses, ‘lasing’ happens Losses can include output coupler, reflectivity, other optics in cavity

Cavity modes The mirrors force the amplitude of the wave to zero. Only integral number of half wavelengths can exist. Every wave exits in phase

Allowed frequencies It is a combination to the energy spread and the cavity modes

Laser pulse generation PC “Q-switching”, ns pulses “Mode-locking”, fs pulses Cavity length ~1.5m Gain medium Q= 2  *Energy stored Energy Lost per cycle

Transverse modes

Transverse Modes The 00 mode is the smallest….

Types of lasers Gas: HeNe Solid-state: Semi-conductor Diode, Crystals (sapphire), nano-particles Liquid: Dyes, Chemical laser: CO 2, Excimer