Applications of lasers M. Rudan

Similar documents
Light Emission.

Optical Systems Program of Studies Version 1.0 April 2012

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

What do we study and do?

LASERS. Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology Sathyamangalam

Light is an electromagnetic wave (EM)

Optics, Light and Lasers

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

Lasers and Electro-optics

INTRODUCTION TO MICROWAVE REMOTE SENSING. Dr. A. Bhattacharya

Light as a Transverse Wave.

ELECTROMAGNETICALLY INDUCED TRANSPARENCY IN RUBIDIUM 85. Amrozia Shaheen

Laboratory 3: Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown, and Twiss Setup for Photon Antibunching

Frequency: the number of complete waves that pass a point in a given time. It has the symbol f. 1) SI Units: Hertz (Hz) Wavelength: The length from

The Electromagnetic Properties of Materials

UNIVERSITY OF SOUTHAMPTON

How does your eye form an Refraction

LASER. Challenging MCQ questions by The Physics Cafe. Compiled and selected by The Physics Cafe

DIFFRACTION GRATING. OBJECTIVE: To use the diffraction grating in the formation of spectra and in the measurement of wavelengths.

Absorption and scattering

Waves & Oscillations

Higher Physics. Particles and Waves

Confocal Microscopy Imaging of Single Emitter Fluorescence and Hanbury Brown and Twiss Photon Antibunching Setup

Michelson Interferometer

Lecture 9: Introduction to Diffraction of Light

Lab 11: Must what goes in be the same as what comes out? Spectroscopy & Fluorescence in Chlorophyll.

WAVE OPTICS GENERAL. Fig.1a The electromagnetic spectrum

Chapter 5 Light and Matter: Reading Messages from the Cosmos

7. Telescopes: Portals of Discovery Pearson Education Inc., publishing as Addison Wesley

Massachusetts Institute of Technology Physics 8.03 Practice Final Exam 3

Physics 201. Professor P. Q. Hung. 311B, Physics Building. Physics 201 p. 1/3

Preview from Notesale.co.uk Page 1 of 38

Lecture 20 Optical Characterization 2

Speed of Light Measurement with a Simple Way

2. Discrete means unique, that other states don t overlap it. 3. Electrons in the outer electron shells have greater potential energy.

Lecture 11: Introduction to diffraction of light

Lecture Fall, 2005 Astronomy 110 1

Advanced Spectroscopy Laboratory

A system of two lenses is achromatic when the separation between them is

Chapter 26: Properties of Light

Light. Mike Maloney Physics, SHS

Vibrational Spectroscopies. C-874 University of Delaware

ELECTROMAGNETIC WAVES ELECTROMAGNETIC SPECTRUM

Laser Detection Techniques

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

Precision Interferometry with a Bose-Einstein Condensate. Cass Sackett. Research Talk 17 October 2008

Light and Matter: Reading Messages from the Cosmos Pearson Education, Inc.

UNIT I -(ELECTROMAGNETISM AND MAGNETIC PROPERTIES OF MATERIALS)

Lecture 7. Outline. ASTR 111 Section 002. Discuss Quiz 5 Light. Light travels through empty space at a speed of 300,000 km/s

Lecture 12. Measurements in Astronomy. Using Light. ASTR 111 Section 002. In astronomy, we need to make remote and indirect measurements

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

Preface to the Second Edition. Preface to the First Edition

Chapter 5 Light and Matter: Reading Messages from the Cosmos. 5.1 Light in Everyday Life. How do we experience light?

National 3 Waves and Radiation

Light.notebook May 03, 2016

Interference, Diffraction and Fourier Theory. ATI 2014 Lecture 02! Keller and Kenworthy

A) n L < 1.0 B) n L > 1.1 C) n L > 1.3 D) n L < 1.1 E) n L < 1.3

Chapter 7. Interference of Light

X-Rays From Laser Plasmas

PRINCIPLES OF PHYSICAL OPTICS

Re-radiation: Scattering. Electric fields are not blocked by matter: how can E decrease?

Page 2. Q1.Electrons and protons in two beams are travelling at the same speed. The beams are diffracted by objects of the same size.

Answers to questions on exam in laser-based combustion diagnostics on March 10, 2006

Newton s Laws of Motion

Higher -o-o-o- Past Paper questions o-o-o- 3.4 Spectra

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

Electricity & Optics

BANNARI AMMAN INSTITUTE OF TECHNOLOGY SATHYAMANGALAM DEPARTMENT OF PHYSICAL SCIENCES. UNIT II Applied Optics

Which of the following classes of electromagnetic waves will not ionise neutral atoms?

PH 222-3A Spring 2010

1. In Young s double slit experiment, when the illumination is white light, the higherorder fringes are in color.

Chapter 5 Telescopes

Optical and Photonic Glasses. Lecture 37. Non-Linear Optical Glasses I - Fundamentals. Professor Rui Almeida

Chapter 5: Light and Matter: Reading Messages from the Cosmos

1) Introduction 2) Photo electric effect 3) Dual nature of matter 4) Bohr s atom model 5) LASERS

Carbon Dating The decay of radioactive nuclei can be used to measure the age of artifacts, fossils, and rocks. The half-life of C 14 is 5730 years.

Optics in a Fish Tank Demonstrations for the Classroom

EA Notes (Scen 101), Tillery Chapter 7. Light

Skoog Chapter 6 Introduction to Spectrometric Methods

Prentice Hall: Conceptual Physics 2002 Correlated to: Tennessee Science Curriculum Standards: Physics (Grades 9-12)

and the radiation from source 2 has the form. The vector r points from the origin to the point P. What will the net electric field be at point P?

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

General Physics II PHYS 102 Final Exam Spring st May 2011

progressive electromagnetic wave

Chapter 10. Interference of Light

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

Experiment 9. Emission Spectra. measure the emission spectrum of a source of light using the digital spectrometer.

Stimulated Emission Devices: LASERS

Purdue University PHYS 221 EXAM II 11/6/03 (with solutions) All questions are worth 5 points unless otherwise stated.

Interested in exploring science or math teaching as a career?

Discussion Review Test #2. Units 12-19: (1) (2) (3) (4) (5) (6)

Electromagnetic Waves

Chemistry Instrumental Analysis Lecture 5. Chem 4631

Light and Matter: Reading Messages from the Cosmos. White light is made up of many different colors. Interactions of Light with Matter

Experiment 3 1. The Michelson Interferometer and the He- Ne Laser Physics 2150 Experiment No. 3 University of Colorado

Chapter 18. Fundamentals of Spectrophotometry. Properties of Light

Grade 8 Science: Unit 3-Optics Chapter 4: Properties of Light

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

2001 Spectrometers. Instrument Machinery. Movies from this presentation can be access at

List of Publications Yury Kronn, Ph. D.

Transcription:

ELECTROMAGNETIC SPECTRUM LASER (Zanichelli, 1999), p. 17.

HETEROSTRUCTURE LASER LASER (Zanichelli, 1999), p. 103.

FUNDAMENTAL SCIENCE (I) The laser emission is monochromatic and has a high brightness. These properties may be exploited, e.g., to investigate phenomena related to the interaction of radiation with matter. Second-harmonic generation. If a material does not exhibit a transition at the laser frequency, the most important phenomenon is polarization. In the linear case, P = c E with P the polarization vector, E the electric field, and c the dielectric susceptivity. In the high-field, scalar case it is P = c 1 E + c 2 E 2 + c 3 E 3

FUNDAMENTAL SCIENCE (II) For isotropic materials the even terms are missing because it must be P (E) = P( E). For non-isotropic materials, assuming that E has the form E = E 0 sin ( ωt ), the second-order summand contributes the term P 2 = (1/2) c 2 E 2 0 [ 1 - cos ( 2ωt ) ] to the series, which contains the second harmonic. The emitted second harmonic has the same direction as the incoming radiation.

APPLIED SCIENCE - BRIGHTNESS (I) The small diameter of the laser beam, absence of contamination, and fine control of the released energy, can be exploited for treating materials. This concept is applicable to different fields, e.g., Microelectronics technology: precision etching, annealing. Mechanical technology: shaping of hard crystals in watch industry, precise formation of holes in hard metals, balancing of rotating masses by evaporation of small amounts of material (vibration measurement performed during rotation), soldering of refractory materials, cleaning of surfaces (e.g., by shallow UV absorption).

SURFACE CLEANING LASER (Zanichelli, 1999), p. 179. In many materials, the absorption of UV radiation happens in a very shallow layer. The surface dirt absorbs the UV radiation and vaporizes.

APPLIED SCIENCE - BRIGHTNESS (II) Biology: excitation of living cells, killing of cells to monitor the behavior of the neighboring cells. Medicine: the laser beam may be used as a scalpel. If the emission is in the blue region (e.g., Ar + laser), there is a strong absorption by the blood cells, which helps the blood to coagulate. The laser is also used to fix the retina by thermal effect. The laser beam crosses harmlessly the transparent parts of the eye. In all medicine application, the functioning of the laser is in the pulse mode.

FIXING OF THE RETINA LASER (Zanichelli, 1999), p. 35. This type of operation exploits the transparency of the external layer and of the interior of the eye. The retina interacts with radiation and is heated up.

APPLIED SCIENCE - COHERENCE (I) Laser gyroscope: it is based on the Doppler effect. Long-distance interferometry: precision mechanical tools (e.g., equipments for electron-beam lithography), geological survey (shift of earth platforms, low-frequency vibrations? terrestrial tides ), radar detection (e.g., missiles), extra-terrestrial survey (measurement of the earth-moon distance), long-term deformations and buildings (e.g., hysteresis of dams may lead to destruction), analysis of the internal strain in mechanical structures or buildings.

LASER GYROSCOPE LASER (Zanichelli, 1999), p. 61. LASER (Zanichelli, 1999), p. 60. When the equipment rotates, the Doppler effect produces interferences that are detected at the mirrors.

LASER INTERFEROMETRY (I) LASER (Zanichelli, 1999), p. 57.

LASER INTERFEROMETRY (II) LASER (Zanichelli, 1999), p. 47. Remote control of machinery

LASER INTERFEROMETRY (III) LASER (Zanichelli, 1999), p. X. Measuring changes in the atmospheric composition due to pollution.

LASER INTERFEROMETRY (IV) LASER (Zanichelli, 1999), p. 2. LASER (Zanichelli, 1999), p. 5. Measuring the Earth-Moon distance. Pulse duration < 1 ns, error < 2.5 cm.

APPLIED SCIENCE - COHERENCE (II) Telecommunications: very large band (the optical range provides an available band that is about 10 4 times larger than the microwave band). The diffraction divergence of an optical beam is about 10 4 times smaller (same reason). The difficulty arising from the strong attenuation due to the atmosphere is solved by using the optical fibers. Modulation is achieved, e.g., by solid-state lasers. Holography: both the intensity and phase information are stored in a film. Optical data processing: based on the far-field properties.

HOLOGRAPHY (I) LASER (Zanichelli, 1999), p. 62. Picture using a stenopeic pinhole. The effect of the pinhole is letting each point in the film be illuminated by a single point of the original object. The film detects the intensity of each color component.

HOLOGRAPHY (II) Picture using holography. The film detects the intensity, however, the latter is due to the interference between the radiation reflected by the object and the reference beam. The light source is monochromatic. After the interference pattern is stored in the film, illumination by the reference beam interacts with the interference pattern. This produces the three-dimensional image of the original object. From the mathematical point of view, the procedure is equivalent to replacing the data of a PDE with a set of boundary conditions, such that the solution inside a given volume is left unchanged. LASER (Zanichelli, 1999), p. 64.