! Fiber!Laser!Intracavity!Absorption! Spectroscopy!(FLICAS)!of!CO/CO2! mixture.!!! This experiment will expose you to tools and approaches, common in

Similar documents
Part IV. Fundamentals of Laser Spectroscopy

Laser Detection Techniques

Fundamentals of Spectroscopy for Optical Remote Sensing. Course Outline 2009

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

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

Optical Gain and Multi-Quantum Excitation in Optically Pumped Alkali Atom Rare Gas Mixtures

Quantum Dot Lasers. Jose Mayen ECE 355

Advanced Spectroscopy Laboratory

Spectroscopy in frequency and time domains

A few Experimental methods for optical spectroscopy Classical methods Modern methods. Remember class #1 Generating fast LASER pulses

Wavelength Frequency Measurements

Linear and nonlinear spectroscopy

Diagnósticos em Plasmas

Application of IR Raman Spectroscopy

Module 4 : Third order nonlinear optical processes. Lecture 28 : Inelastic Scattering Processes. Objectives

Because light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency.

Elements of Quantum Optics

doi: /PhysRevLett

Professor Dr. Wolfgang Demtröder

Chemistry Instrumental Analysis Lecture 5. Chem 4631

Atomization. In Flame Emission

Design and Development of a Smartphone Based Visible Spectrophotometer for Analytical Applications

ATOMIC AND LASER SPECTROSCOPY

Vibrational Spectroscopy of Molecules on Surfaces

Optics, Light and Lasers

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

Chemistry 524--Final Exam--Keiderling May 4, :30 -?? pm SES

Modern Techniques in Applied Molecular Spectroscopy

Fundamental Mechanisms, Predictive Modeling, and Novel Aerospace Applications of Plasma Assisted Combustion

Lecture 10. Lidar Effective Cross-Section vs. Convolution

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

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

Distributed feedback semiconductor lasers

Session #1: Theoretical background and computer simulations of molecular vibrations.

Citation for published version (APA): Mollema, A. K. (2008). Laser cooling, trapping and spectroscopy of calcium isotopes s.n.

Lecture 0. NC State University

Investigation of Water Fragments

Chemistry 311: Instrumentation Analysis Topic 2: Atomic Spectroscopy. Chemistry 311: Instrumentation Analysis Topic 2: Atomic Spectroscopy

R O Y G B V. Spin States. Outer Shell Electrons. Molecular Rotations. Inner Shell Electrons. Molecular Vibrations. Nuclear Transitions

Small Signal Gain in DPAL Systems

All-Optical Delay with Large Dynamic Range Using Atomic Dispersion

Lecture 06. Fundamentals of Lidar Remote Sensing (4) Physical Processes in Lidar

Complete the following. Clearly mark your answers. YOU MUST SHOW YOUR WORK TO RECEIVE CREDIT.

Magnetic resonance imaging MRI

Comparison of hollow cathode and Penning discharges for metastable He production

Water in Food 3 rd International Workshop. Water Analysis of Food Products with at-line and on-line FT-NIR Spectroscopy. Dr.

Spectroscopy in Transmission

Characterisation of vibrational modes of adsorbed species

Signal regeneration - optical amplifiers

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

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

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

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

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

Introduction to laser-based combustion diagnostics

INTRODUCTION Atomic fluorescence spectroscopy ( AFS ) depends on the measurement of the emission ( fluorescence ) emitted from gasphase analyte atoms

Two-electron systems

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

What is spectroscopy?

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

QUESTION BANK IN PHYSICS

Hefei

Introduction to XAFS. Grant Bunker Associate Professor, Physics Illinois Institute of Technology. Revised 4/11/97

Roger Ding. Dr. Daniel S. Elliott John Lorenz July 29, 2010

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

In Situ Imaging of Cold Atomic Gases

Chapter 5. Semiconductor Laser

Mid-Infrared Laser based Trace Gas Sensor Technologies: Recent advances and Applications

very high temperature for excitation not necessary generally no plasma/arc/spark AAS

Modern Optical Spectroscopy

Evaluating Labsphere s new UV-2000

Survey on Laser Spectroscopic Techniques for Condensed Matter

= nm. = nm. = nm

Vibrational Spectroscopies. C-874 University of Delaware

Reference literature. (See: CHEM 2470 notes, Module 8 Textbook 6th ed., Chapters )

Spectroscopy tools for PAT applications in the Pharmaceutical Industry

3.1 The Plane Mirror Resonator 3.2 The Spherical Mirror Resonator 3.3 Gaussian modes and resonance frequencies 3.4 The Unstable Resonator

Molecular spectroscopy

Using Calibrated Specular Reflectance Standards for Absolute and Relative Reflectance Measurements

Quantum Electronics Laser Physics PS Theory of the Laser Oscillation

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

Some Topics in Optics

Ultra-Slow Light Propagation in Room Temperature Solids. Robert W. Boyd

Chapter 28 Atomic Physics

3) In CE separation is based on what two properties of the solutes? (3 pts)

Chapter 6 Photoluminescence Spectroscopy

CHAPTER III EXPERIMENTAL SYSTEM

2D Methyl Radical Measurement in a Methane/Air Flame at Atmospheric. Pressure. Abstract

Semiconductor Disk Laser on Microchannel Cooler

Temperature Dependent Optical Band Gap Measurements of III-V films by Low Temperature Photoluminescence Spectroscopy

Bolometry. H. Kroegler Assciazione Euratom-ENEA sulla Fusione, Frascati (Italy)

Spectroscopy. Experimental Optics. Contact: Lisa Kaden Malte Siems

University of Cyprus. Reflectance and Diffuse Spectroscopy

SFs-dimers. Hole Burning in the IR. Predissociation Spectrum of. (948.0 cm-1), see Figure 2a. The shifts and also the relative intensities

Ultraviolet-Visible and Infrared Spectrophotometry

Lab 3-4 : Confocal Microscope Imaging of Single-Emitter Fluorescence and Hanbury-Brown and Twiss Set Up, Photon Antibunching

OPTICAL DIAGNOSTICS TO STUDY SUPERCRITICAL CO 2 PROCESSES. A. Braeuer

Process Analytical Technology Diagnosis, Optimization and Monitoring of Chemical Processes

DIODE LASER SPECTROSCOPY

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

Transcription:

FiberLaserIntracavityAbsorption Spectroscopy(FLICAS)ofCO/CO2 mixture. This experiment will expose you to tools and approaches, common in modern laser spectroscopy. During the following weeks we will cover several important chapters in the field of modern optics and experimental laser spectroscopy: Basic principles of laser operation. Fiber optics. Spectrographs and monochromators. Intracavity Laser Absorption Spectroscopy (ICLAS). Fiber Laser Intracavity Absorption Spectroscopy (FLICAS).

Introduction Laser Diagnostics in Combustion and Environmental Research The availability and high reliability of lasers, laser spectroscopy is assuming an ever-expanding role in the diagnostic probing of combustion and environmental processes. Laser based techniques supply the researcher with the capability for remote, nonintrusive, in-situ, spatially and temporally precise measurements of important chemical parameters. Laser diagnostics are facilitating improved understanding of a wide variety of combustion phenomena that, in turn, will lead to improved efficiency and cleanliness in the energy conversion devices so vital to modern day life. ICLAS: the methodology of the experiment Direct absorption spectroscopy of atoms and molecules in the gas phase, yielding both quantitative absolute concentrations as well as absolute frequency-dependent cross-sections, is a very powerful tool in analytical chemistry and physical chemistry. This absoluteness is the reason why sensitive absorption spectroscopy techniques have gained renewed interest, even in research fields where more sophisticated laser-based diagnostic techniques are commonly applied. Among the various direct absorption techniques, the Intracavity Laser Absorption Spectroscopy (ICLAS) and its fiber-laser based version (FLICAS) have proven to be valuable addition, since they combine a good sensitivity with a relatively simple and straightforward experimental set-up. In a `conventional absorption experiment, one measures the amount of light that is transmitted through a sample. If the light source is monochromatic (e.g. a laser), one can record an absorption spectrum of the sample by recording the transmitted intensity as a function of the frequency. Alternatively, a broad light source can be used when the incident light or the transmitted light is spectrally dispersed. A drawback of direct absorption might be its limited sensitivity. A small attenuation in transmitted light has to be measured on top of a large background. High sensitivity is obtained by using modulation schemes and by increasing the absorption path length. Alternatively, other experimental spectroscopy techniques can be used which are based on the detection of phenomena which are induced by absorption of light, such as pressure changes in photoacoustic spectroscopy, fluorescence in laser-induced fluorescence (LIF), or ions in resonant enhanced multiphoton ionization (REMPI). The great advantage of these techniques is that they are background free. A disadvantage is the

sometimes difficult calibration procedure which is needed to make these techniques absolute (i.e. these techniques are not self-calibrating). ICLAS spectroscopy is a sensitive absorption technique, in which the absorbing species are placed inside the cavity of a broadband laser. Figure 1 illustrates the schematics of the intracavity absorption experiment. The sample is either confined in an absorption cell, or just placed in an open part of the cavity. Fig1: Schematic description of intracavity absorption experiment When the linewidth of the absorber is narrower than homogeneous spectral broadening of the laser gain medium, then even minute absorber quantities lead to spectral holes in the laser output due to the positive feedback mechanism in lasers. Additional inhomogeneous broadening of the gain is beneficial, since the spectral range for absorption measurements with a particular laser is broadened. Experimental procedure During the following weeks you will use the Fiber Laser Intracavity Absorption Spectroscopy (FLICAS) to monitor CO/CO2 mixture. CO/CO2 ratio is an important measure of completeness of combustion and is among the major environmental and performance characteristics of any combustion device. Specifically, you will perform the following tasks: 1. Alignment of the optical layout 2. Measurement of the absorption Spectrum vs. at different pressures of CO/CO2 mixture 3. Measurement of the absorption Spectrum vs. at different temperatures of CO/CO2 mixture 4. Obtain the mixture temperature and quantum-state dependent

Demtröder, Laser Spectroscopy (Vol.1, Vol.2, 4th edition) Baev V. M. et. al, APPLIED PHYSICS B-LASERS AND OPTICS Volume: 69 Issue: 3 Pages: 171-202 DOI: 10.1007/s003400050793 Published: SEP 1999