LASERS By Swapan Das.

Slides:



Advertisements
Similar presentations
Femtosecond lasers István Robel
Advertisements

Optical sources Lecture 5.
LASER (semiconducting Lasers) LASER 1 EBB 424E Dr Zainovia Lockman.
X-rays & LASERs Section 31-7 Physics 1161: Lecture 24.
LASERS A short introduction on how “lasing” is achieved.
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.
Light Amplification by Stimulated
Lesson 3 Explain the terms monochromatic and coherent. Identify laser light as a source of coherent light. Outline the mechanism for the production of.
What’s so Special about a Laser?
BASICS OF LASERS AND LASER LIGHT
EM Radiation Sources 1. Fundamentals of EM Radiation 2. Light Sources
1.2 Population inversion Absorption and Emission of radiation
After School Optics Lab Quiz. 1. What is the phenomenon that explains how light can be channeled called?
EM Radiation Sources 1. Fundamentals of EM Radiation 2. Light Sources 3. Lasers.
Absorption and emission processes
Optical Pumping Intense light source at h  (e.g. flash lamp) Excites to a metastable state to achieve population inversion With fast flashing, initial.
Light Emission. Today’s Topics Excitation Emission Spectra Incandescence –Absorption Spectra.
Atomic Structure. X-ray Spectrum Continuous spectrum Characteristic spectrum.
Interference Diffraction and Lasers
Laser Principle Eman Ali Ateeq.
Lasers (Light Amplification by Stimulated Emission of Radiation)
PH 0101 UNIT-3 LECT - 2 INTRODUCTION OF LASERS : BASIC PRINCIPLE :
B.SC.II PAPER-B (OPTICS and LASERS) Submitted by Dr. Sarvpreet Kaur Assistant Professor PGGCG-11, Chandigarh.
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.
1 P1X: Optics, Waves and Lasers Lectures, Lasers and their Applications i) to understand what is meant by coherent and incoherent light sources;
Optical Sources. History of Lasers In 1917, Einstein predicted the existence of spontaneous and stimulated emission by which an atom can emit radiation.
 Different from a neon light radiating in any directions, a laser is a beam of coherent light radiating in the same direction with high intensity and.
PHYSICS DEPARTMENT.
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.
The Spectrum of EM Waves According to wavelength or frequency, the EM waves can be distinguished into various types. There is no sharp boundary.
1.Stable radiation source 2.Wavelength selector 3.Transparent sample holder: cells/curvettes made of suitable material (Table 7- 2) 4.Radiation detector.
Chapter 28:Atomic Physics
LASERS AND SPECTROSCOPY . EXCITING MOLECULES  Molecules can be excited using either broadband or monochromatic light. Spectra obtained using monochromatic.
Laser physics and its application Introductory Concept The word LASER is an acronym for Light Amplification by Stimulated Emission of Radiation Lasers,
Interference & Diffraction Light Part 4. Interference Like other forms of wave energy, light waves also combine with each other Interference only occurs.
LASER LASER stands for LIGHT APLIFICATION by STIMULATED EMISSION of RADITIONS First laser was constructed by Maiman Laser action has been obtained with.
Medical Physics Students
LIGHT AMPLIFICATION by STIMULATED ELECTRON RADIATION
Unit 12: Part 2 Quantum Physics. Overview Quantization: Planck’s Hypothesis Quanta of Light: Photons and the Photoelectric Effect Quantum “Particles”:
SHRI DADAJI INSTITUTE OF TECHNOLOGY & SCIENCE A SEMINAR ON LASER COMMUNICATION PRESENTED BY: HITESH SILARPURIYA E.C. FOURTH SEM.
SACE Stage 2 Physics The Structure of The Atom. Emission Spectra Can be observed when a material (gas) glows by heating or an electric current is passed.
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.
Laserlaser. Laser printer Laser pointer Laser: everywhere in your life.
Laser.
Optical Sources.
Light-Matter Interaction
Lasers (Light Amplification by Stimulated Emission of Radiation)
Light Amplification by Stimulated
Properties of Laser There are Severel Properties Of LASER which are defined as follows:- MONOCHROMATICITY COHERENCE DIRECTIONALITY BRIGHTNESS DIVERGENCE.
Lasers & Coherence Grant Jonathan Taylor Holub
Laser and its applications
LASER (semiconducting Lasers)
Well - come.
A short introduction on how “lasing” is achieved
MEDICAL LASER SYSTEMS Assist Prof. Dr. Lutfi Ghulam Awazli
Origin of The Electromagnetic (EM) Waves
Physics 1161: Lecture 24 X-rays & LASERs Section 31-7.
The Structure of the Atom
Cutnell/Johnson Physics 7th edition
Laser and its applications
電磁波或光 但如此相干coherent的光很不容易形成! 不相干的光極易發散!
Physics 1161: Lecture 24 X-rays & LASERs Section 31-7.
Lasers. You know magic and stuff
Unit 2 Particles and Waves Spectra
PRINCIPLE AND WORKING OF A SEMICONDUCTOR LASER
Rayat Shikshan Sanstha’s Veer Wajekar A.S.C. College,Phunde
LASER (semiconducting Lasers)
A Brief Account of LASER & Its Application
Rayat Shikshan Sanstha’s S. M. Joshi College, Hadapsar
Presentation transcript:

LASERS By Swapan Das

Light Amplification by Stimulated Emission of What is LASER???? Light Amplification by Stimulated Emission of Radiation A device that produces a coherent beam of optical radiation by stimulating electronic, ionic, or molecular transitions to higher energy levels. When they return to lower energy levels by stimulated emission, they emit energy.

Basic concepts for a laser Absorption Spontaneous Emission Stimulated Emission Population inversion

Lasers: Basic Principle Absorption and Radiation Processes

photon absorption─ hν = E2 – E1. An electron in an atom can be excited from an energy level E1 to a higher energy level E2 by absorption: photon absorption─ hν = E2 – E1.

Spontaneous Emission The atom decays from level 2 to level 1 through the emission of a photon with the energy hv. It is a completely random process.

Stimulated Emission Atoms in an upper energy level can be triggered or stimulated in phase by an incoming photon of a specific energy.

Stimulated Emission The stimulated photons have unique properties: In phase with the incident photon Same wavelength as the incident photon Travel in same direction as incident photon

Population Inversion A state in which a substance has been energized, or excited to specific energy levels. More atoms or molecules are in a higher excited state. The process of producing a population inversion is called pumping. Examples: →by lamps of appropriate intensity →by electrical discharge

Metastable states An atom or molecule in an excited state remains there for a certain time called the lifetime of that state, before making a transition to a lower state. The lifetime of a state is characteristic of the energy level and varies over a wide range. Most of the states have a short lifetime, of the order of 10-8 s. However, some energy states have very long lifetime of the order of 10-3 s or higher. Energy states with such long life times are called meta-stable states.

Pumping The population inversion can be achieved by exciting the medium with suitable form of energy. This process is called Pumping. There are several methods of pumping a laser and producing population inversion necessary for the occurrence of stimulated emission : (a) Optical pumping (b) Electric Discharge (c) Inelastic atom-atom collision (d) Direct Conversion (e) Chemical reactions

Characteristics of Laser Beam High directionality: Directionality is the characteristic of laser light that causes it to travel in a single direction with a narrow cone of divergence. It is defined in terms of divergence angle. Divergence angle is twice the angle made by the outer edge with the axis of the beam. The angular spread of beam on one side of the axis :

High Intensity The intensity of light is defined as the energy passing per unit area per second through a point normal to the direction of flow. For a spherical source with output power P , intensity at a point distant r from the source is given as: Laser beam is highly intense because it emits light as a narrow beam and intensity remains high even at large distance from the source.

Extraordinary monochromacity If ∆ν is the frequency of a spectral line of frequency ν0then the degree of monochromacity is defined as: ε=∆ν/ν0 Smaller is the value of ε, higher is the monochromacity of light. For laser source ε=10-12 while for ordinary source ε≈10-5

High Coherence Degree of coherence is the measure of phase correlation in the radiation field at different locations and different time. Coherent Incoherent