Laser Excitation Dynamics of Argon Metastables Generated in Atmospheric Pressure Flows by Microwave Frequency Microplasma Arrays (II)
|
|
- Elvin Conrad Watts
- 6 years ago
- Views:
Transcription
1 Physical Sciences Inc. Laser Excitation Dynamics of Argon Metastables Generated in Atmospheric Pressure Flows by Microwave Frequency Microplasma Arrays (II) W.T. Rawlins, K.L. Galbally-Kinney, S.J. Davis Physical Sciences Inc., Andover, MA A.R. Hoskinson, J.A. Hopwood ECE Department, Tufts University, Medford, MA High Energy/Average Power Lasers and Intense Beam Applications IX SPIE Photonics West 2016 San Francisco, CA 15 February 2016 Paper VG Physical Sciences Inc. 20 New England Business Center Andover, MA 01810
2 Three-level systems CW Optically Pumped Microplasma Rare-Gas Laser Alkali-Atom Laser np 6 (n+1)s 1 2 Pump Laser 1 G Collisional Transfer Laser Transition Micro-discharge 3 VG Rare-Gas Metastable Laser np 5 (n+1)s 1 Diode-pumped rare-gas metastable laser: analogue to DPAL M.C. Heaven and coworkers, Opt. Lett. 37, 2157 (2012), 38, 5458 (2013) Excellent beam quality for conversion of high-power diode beams ZERO CHEMISTRY, PARTICULATES, OPTICAL DEGRADATION!!! Many selectable wavelengths (visible to mid-ir) Microplasma laser demonstrated CW at 1 atm Optically efficient (>50%), low discharge power, scalable Compact, high gain: power available ~25 kw/liter (per Ar* cycle)
3 Optical Pumping Scheme for Ar(1s 5 ) Metastables Physical Sciences Inc. VG Ar 4s and 4p Energy Levels Paschen (at left) and Racah Notation Possible Laser Transitions: Pump 1s 5 2p 9, nm Lase 2p 10 1s 5, nm (illustrated) Pump 1s 5 2p 7, nm Lase 2p 7 1s 4, nm or 2p 8 1s 4, nm or 2p 9 1s 5, nm or 2p 10 1s 5, nm Lower states: 1s 5, 1s 3 are metastable 1s 4, 1s 2 are radiatively trapped
4 1s 5-2p nm Diode Laser (Probe) Lens Observations of Ar* Gain, LIF, and Laser Power Extraction Detector Window NIR Spectrometer NIR Camera Lens Grating Single-Board Resonator Array VG Wave Plate WM Polarizing BS Cube Flip Mirror Window Window Pump Laser Probe Laser 1s 5-2p nm Beam Dump PD L-0506a TDL Scans 912 nm [Ar(1s 5 )] o = 2.8 x cm -3
5 Optically Pumped Argon Microplasma Laser Atmospheric Pressure Ar/He Micro-Discharge M1 TEMoo mode Ti:S Beam VG Microplasma µm Beam Splitter 300 µm 1.9 cm CW laser output at nm 22 mw with 15% output coupler 40 mw absorbed at nm Optical efficiency ~ 55% Output Beam M2 L-0548 Observed stable output for greater than 30 minutes Excellent beam quality Optics Express 23, 4804 (2015)
6 Interesting Kinetics: Collisional Coupling of Ar(4s,4p) Spin-Orbit States in He Collisional energy transfer 2p 9 2p 8, 2p 10 ; 1s 4 1s 5 Controls optical gain achieved for given initial [Ar(1s 5 )] o from discharge Kinetics measurements: 1s 4 1s 5 coupling is slow in He at 300 K J. Han and M.C. Heaven, Opt. Lett. 39, 6451 (2014) Observe G o ~ 1 cm -1 for [Ar(1s 5 )] o ~ 4 x cm -3 VG level steady-state model: optical gain data indicate rapid collisional state coupling at discharge temperature k C [M] 3 2p 9 (g 3 = 7) IB 13 IB 31 k Q [M] 2 2p 10 (g 2 = 3) A 31 I B 12 I B 21 A 21 A s 4 (g 4 = 3) 1 k 41 [M] 1s 5 (g 1 = 5) L-0766 Need more data on energy transfer kinetics at elevated temperatures! (M. Heaven et al., in progress)
7 Keys to Scaling Microplasma OPRgL Physical Sciences Inc. Volume scaling Multiple overlapping micro-discharges Initial experiments with dual-discharge Pressure effects Reduced pressure larger microplasma Effects on Ar*, gain, line width Array design Gap width, substrate, number of resonator strips, drive frequency Kinetics of Ar* production, collisional lifetime Discharge production/loss, post-discharge survival Ar* energy pooling, three-body excimer formation Quenching by contaminants Diode laser pump Requires high power, line-narrowed diode Optical efficiency, beam quality Models, preliminary data 50-60%, M 2 ~ 1.3 VG
8 Optical Gain and [Ar*] Scaling: 2% Ar/He, 1 atm New Substrate Material and Gap VG Duroid Substrate, 100 mm discharge gap, ~950 MHz Saturated gain and [Ar*] ~ same as with 25 mm gap Empirical ratio: [Ar*]/G o at saturation Metric for collisional coupling efficiency = (4 ± 1) x cm -2 (25 mm gap) = 4.2 x cm -2 (100 mm gap)
9 Scaling of [Ar*], Gain with Discharge Power: 1 atm 100 mm Gap, Duroid Substrate Ar(1s 5 ) Number Density Optical Gain 2p 10 1s 5 VG [Ar*] scales as {power} 1/2 Note E/N also scales as {power} 1/2 Scaling may be limited by energy pooling at high [Ar*] Ar* + Ar* Ar + + Ar + e - Three-body excimer formation may also limit Ar* lifetime Ar* + Ar + He Ar 2 * + He
10 Pressure Scaling: Gain and Ar(1s 5 ) Number Density 100 mm Discharge Gap, Duroid Substrate VG Ar(1s 5 ) Number Density Gain Curves: 302 and 770 Torr High Ar* production Torr Observe positive gain for P 85 Torr Duroid substrate degrades with use: contaminant outgassing! Switch to AlN substrate
11 Post-Discharge Collisional Lifetime of Ar* Energy Pooling and Excimer Formation VG Ar* + Ar* Ar + + Ar + e - k = 5 x (T/300) 0.5 = 7.1 x cm 3 /s at 600 K Ar* + Ar + He Ar 2 * + He k III = 1 x cm 6 /s for M=Ar He, T dependence =?? For 2% Ar/He, 1 atm, 600 K: k III [Ar][He] = 3 x 10 4 s -1 Rate constants are very poorly known: no actual measurements Three-body excimer formation may be the dominant loss process in post-discharge flow Superelastic quenching by electrons probably dominates in active discharge: e - + Ar* Ar + e ev
12 Effects of Vacuum Contaminants: N 2, H 2 O Physical Sciences Inc. VG Ar* + N 2 : k = 2.8 x cm 3 /s 90 ppmv N 2 at 1 atm, 600 K 3 x 10 4 s -1 Ar* + H 2 O: k = 4 x cm 3 /s 6 ppmv H 2 O at 1 atm, 600 K 3 x 10 4 s -1 Even modest leaks and outgassing can destroy Ar*
13 Height (mm) Physical Sciences Inc. Two Resonant Modes Even Mode Initial Volume Scaling: Overlapping Dual Discharges Odd Mode Side View, 2p 10 Emission Even Mode, 252 Torr Plasma Side Fluorescence (Zoom) Coupled Board VG Ar/He Flow Input Board Width (mm) Ar(1s 5 ) Probe Measurements, nm: 1 mm board separation 200 0
14 Pressure Dependence of Ar(1s 5 ) Production Single and Dual Arrays VG Single Array 100 mm Discharge Gap Dual Array, Even Mode 25 mm Discharge Gaps Similar production for single and dual arrays Not much change with pressure Torr Ar* concentration fills in space between arrays Increases overall gain volume
15 Dual Discharge: Line Widths and Temperatures (Preliminary) Ar(1s 5 2p 10 Absorption Line Widths VG Rotational Temperatures: CH(A 2 D X 2 P) Emission, 1 atm Lindholm-Foley analysis indicates factor-of-2 increase in T from 200 to 775 Torr T 600 K in discharge at 1 atm: faster energy transfer kinetics Need definitive data on pressure broadening coefficients vs T for Ar-He, Ar-Ar: 1s 5-2p 10, 1s 5-2p 9 transitions!
16 Micro-Discharge-Flow: [Ar(1s 5 )] at 775 Torr Flow Velocity ~ 4910 cm/s Ar(2p 10 ) Emission VG Upper discharge length: 0.5 mm Lower discharge length: 0.3 mm
17 Micro-Discharge-Flow: [Ar(1s 5 )] at 208 Torr Flow Velocity ~ 5460 cm/s Ar(2p 10 ) Emission VG Upper discharge length: 1.3 mm Lower discharge length: 0.9 mm
18 [Ar(1s 5 )] Dual-Discharge Flow Times (Approximate) 775 and 208 Torr VG Upper Discharge: 10 ms Lower Discharge: 6 ms Upper Discharge: 24 ms Lower Discharge: 16 ms Data indicate Ar(1s 5 ) post-discharge lifetimes in the range ms Consistent with possible loss rate due to Ar* + Ar + He reaction But -- it could also be trace N 2, H 2 O background in vacuum system!
19 Summary: Microplasma OPRgL Physical Sciences Inc. VG Scaling the gain volume Multi-array flow-through design appears to work (use <1 mm spacing) Aided by expansion of discharge at reduced pressure ( Torr) Ar(1s 5 ) collisional lifetime: determines recycling of Ar* atoms Short post-discharge lifetime: ~10s of ms at 1 atm Sensitive to quenching by ordinary vacuum contaminants Architecture: pump within or at the edge of the active discharge region Scaling Ar(1s 5 ) production preliminary results (power) 1/2 Independent of micro-discharge gap width Roughly constant for P > 200 Torr Absorption line widths (1s 5-2p 10 ): ~20 MHz/Torr at 1 atm, ~600 K [Ar(1s 5 )]/G o appears to be robust scaling and conceptual metric Correlates to collisional state coupling via simple steady-state model High energy content: I sat G o 25 kw/liter at 1 atm
20 Acknowledgements Physical Sciences Inc. VG Michael Heaven, Emory University Glen Perram, Air Force Institute of Technology High Energy Laser Joint Technology Office (MRI - Emory University) Air Force Research Laboratory/AFMC (Dr. Steve Adams) Air Force Office of Scientific Research
21 OPRgL Projected Scaling Characteristics (Preliminary Estimates) VG Overall scaling and functionality and SWaP similar to DPAL Three OPRgL scaling models, consistent with each other Russians: Demyanov et al., J. Phys. D: Appl. Phys. 46, (2013) Chinese: Yang et al., Optics Express 23, (2015) USA: G. Perram (AFIT) and G. Hager, 2015 Efficiency: 55% (o-o) x 75% (e-o pump diode) = ~40% overall Beam Quality: expect M 2 ~ 1.3 Micro-discharge power required: ~6 kw at 2.45 GHz for 100 kw Operating wavelengths: ~40 wavelengths, nm 500 W/cm 3 b << 0.1
Short overview of TEUFEL-project
Short overview of TEUFEL-project ELAN-meeting may 2004 Frascati (I) Contents Overview of TEUFEL project at Twente Photo cathode research Recent experience Outlook Overview FEL Drive laser Photo cathode
More informationPUMPED Nd:YAG LASER. Last Revision: August 21, 2007
PUMPED Nd:YAG LASER Last Revision: August 21, 2007 QUESTION TO BE INVESTIGATED: How can an efficient atomic transition laser be constructed and characterized? INTRODUCTION: This lab exercise will allow
More information- thus, the total number of atoms per second that absorb a photon is
Stimulated Emission of Radiation - stimulated emission is referring to the emission of radiation (a photon) from one quantum system at its transition frequency induced by the presence of other photons
More informationSpectroscopy. Biogeochemical Methods OCN 633. Rebecca Briggs
Spectroscopy Biogeochemical Methods OCN 633 Rebecca Briggs Definitions of Spectrometry Defined by the method used to prepare the sample 1. Optical spectrometry Elements are converted to gaseous atoms or
More informationDefense & Security Symposium 2004, Kigre Er:glass Publication #144. Eye-Safe Erbium Glass Laser Transmitter Study Q-Switched with Cobalt Spinel
Eye-Safe Erbium Glass Laser Transmitter Study Q-Switched with Cobalt Spinel Ruikun Wu, TaoLue Chen, J.D. Myers, M.J. Myers, Chris R. Hardy, John K. Driver Kigre, Inc. 1 Marshland Road, Hilton Head Island,
More informationExperiment #5: Qualitative Absorption Spectroscopy
Experiment #5: Qualitative Absorption Spectroscopy One of the most important areas in the field of analytical chemistry is that of spectroscopy. In general terms, spectroscopy deals with the interactions
More informationHelium-Neon Laser. Figure 1: Diagram of optical and electrical components used in the HeNe laser experiment.
Helium-Neon Laser Experiment objectives: assemble and align a 3-mW HeNe laser from readily available optical components, record photographically the transverse mode structure of the laser output beam,
More informationLasers Design and Laser Systems
Lasers Design and Laser Systems Tel: 04-8563674 Nir Dahan Tel: 04-8292151 nirdahan@tx.technion.ac.il Thank You 1 Example isn't another way to teach, it is the only way to teach. -- Albert Einstein Course
More information13C NMR Spectroscopy
13 C NMR Spectroscopy Introduction Nuclear magnetic resonance spectroscopy (NMR) is the most powerful tool available for structural determination. A nucleus with an odd number of protons, an odd number
More informationQuasi-Continuous Wave (CW) UV Laser Xcyte Series
COMMERCIAL LASERS Quasi-Continuous Wave (CW) UV Laser Xcyte Series Key Features 355 nm outputs available Quasi-CW UV output Field-proven Direct-Coupled Pump (DCP ) TEM00 mode quality Light-regulated output
More informationTime out states and transitions
Time out states and transitions Spectroscopy transitions between energy states of a molecule excited by absorption or emission of a photon hn = DE = E i - E f Energy levels due to interactions between
More informationTi:Sapphire Lasers. Tyler Bowman. April 23, 2015
Ti:Sapphire Lasers Tyler Bowman April 23, 2015 Introduction Ti:Sapphire lasers are a solid state laser group based on using titanium-doped sapphire (Ti:Al 2O 3) plates as a gain medium. These lasers are
More informationTechnology Developments Towars Silicon Photonics Integration
Technology Developments Towars Silicon Photonics Integration Marco Romagnoli Advanced Technologies for Integrated Photonics, CNIT Venezia - November 23 th, 2012 Medium short reach interconnection Example:
More informationRaman spectroscopy Lecture
Raman spectroscopy Lecture Licentiate course in measurement science and technology Spring 2008 10.04.2008 Antti Kivioja Contents - Introduction - What is Raman spectroscopy? - The theory of Raman spectroscopy
More informationExperiment 5. Lasers and laser mode structure
Northeastern University, PHYS5318 Spring 2014, 1 1. Introduction Experiment 5. Lasers and laser mode structure The laser is a very important optical tool that has found widespread use in science and industry,
More informationMethods of plasma generation and plasma sources
Methods of plasma generation and plasma sources PlasTEP trainings course and Summer school 2011 Warsaw/Szczecin Indrek Jõgi, University of Tartu Partfinanced by the European Union (European Regional Development
More informationDevelopment of MEMS micromirrors for intracavity laser control
Development of MEMS micromirrors for intracavity laser control Walter Lubeigt Centre for Microsystems and Photonics, EEE Department, University of Strathclyde,204 George Street, Glasgow G1 1XW,UK Motivation
More informationQuantum- dot based nonlinear source of THz radia5on
Quantum- dot based nonlinear source of THz radia5on A. Andronico a, J. Claudon b, M. Munsch b, I. Favero a, S. Ducci a, J. M. Gérard b, and G. Leo a a Univ Paris Diderot, MPQ Lab, CNRS- UMR 7162, Paris,
More informationKatharina Lückerath (AG Dr. Martin Zörnig) adapted from Dr. Jörg Hildmann BD Biosciences,Customer Service
Introduction into Flow Cytometry Katharina Lückerath (AG Dr. Martin Zörnig) adapted from Dr. Jörg Hildmann BD Biosciences,Customer Service How does a FACS look like? FACSCalibur FACScan What is Flow Cytometry?
More informationArgon ion laser-induced fluorescence with diode lasers
Argon ion laser-induced fluorescence with diode lasers G. D. Severn, a) D. A. Edrich, and R. McWilliams Department of Physics & Astronomy, University of California, Irvine, Irvine, California 92627 Received
More informationPump-probe experiments with ultra-short temporal resolution
Pump-probe experiments with ultra-short temporal resolution PhD candidate: Ferrante Carino Advisor:Tullio Scopigno Università di Roma ƒla Sapienza 22 February 2012 1 Pump-probe experiments: generalities
More informationMCAL Spectrophotometry. Spectrophotometry
MCAL Spectrophotometry Instruments include: Cary 50 UV-vis Spectrophotometer Eclipse Spectrofluorometer HPLC Diode Array and Fluorescence ICP-OES with CCD detection Spectrophotometry The instruments all
More informationRAY TRACING UNIFIED FIELD TRACING
RAY TRACING Start to investigate the performance of your optical system using 3D ray distributions, dot diagrams of ray positions and directions, and optical path length. GEOMETRIC FIELD TRACING Switch
More informationPhysics 30 Worksheet # 14: Michelson Experiment
Physics 30 Worksheet # 14: Michelson Experiment 1. The speed of light found by a Michelson experiment was found to be 2.90 x 10 8 m/s. If the two hills were 20.0 km apart, what was the frequency of the
More informationMolecular Spectroscopy
Molecular Spectroscopy UV-Vis Spectroscopy Absorption Characteristics of Some Common Chromophores UV-Vis Spectroscopy Absorption Characteristics of Aromatic Compounds UV-Vis Spectroscopy Effect of extended
More informationLocal Heating Attacks on Flash Memory Devices. Dr Sergei Skorobogatov
Local Heating Attacks on Flash Memory Devices Dr Sergei Skorobogatov http://www.cl.cam.ac.uk/~sps32 email: sps32@cam.ac.uk Introduction Semi-invasive attacks were introduced in 2002 ( Optical fault induction
More informationDIODE PUMPED CRYSTALASER
DIODE PUMPED CRYSTALASER Ultra-compact CW & Pulsed Turnkey Systems UV Visible to IR High Reliability High Stability High Efficiency TEMoo & SLM Low Noise Low Cost ULTRA-COMPACT DIODE-PUMPED CRYSTAL LASER
More informationStatus of the FERMI@Elettra Free Electron Laser
Status of the FERMI@Elettra Free Electron Laser E. Allaria on behalf of the FERMI team Work partially supported by the Italian Ministry of University and Research under grants FIRB-RBAP045JF2 and FIRB-RBAP06AWK3
More informationAlignement of a ring cavity laser
Alignement of a ring cavity laser 1 Introduction This manual describes a procedure to align the cavity of our Ti:Sapphire ring laser and its injection with an Argon-Ion pump laser beam. The setup is shown
More informationSpatial and temporal coherence of polariton condensates
Spatial and temporal coherence of polariton condensates R. Spano Dpt. Fisica de Materiales, Universidad Autónoma Madrid. SPAIN XIV JORNADA DE JÓVENES CIENTÍFICOS DEL INSTITUTO DE CIENCIA DE MATERIALES
More informationHow To Understand The Measurement Process
April 24, 2015 Exam #3: Solution Key online now! Graded exams by Monday! Final Exam Monday, May 4 th, 10:30 a.m. Room: Perkins 107 1 A Classical Perspective A classical view will help us understand the
More informationSpecifying Plasma Deposited Hard Coated Optical Thin Film Filters. Alluxa Engineering Staff
Specifying Plasma Deposited Hard Coated Optical Thin Film Filters. Alluxa Engineering Staff December 2012 Specifying Advanced Plasma Deposited Hard Coated Optical Bandpass and Dichroic Filters. Introduction
More informationChemistry 102 Summary June 24 th. Properties of Light
Chemistry 102 Summary June 24 th Properties of Light - Energy travels through space in the form of electromagnetic radiation (EMR). - Examples of types of EMR: radio waves, x-rays, microwaves, visible
More informationBroadband THz Generation from Photoconductive Antenna
Progress In Electromagnetics Research Symposium 2005, Hangzhou, China, August 22-26 331 Broadband THz Generation from Photoconductive Antenna Qing Chang 1, Dongxiao Yang 1,2, and Liang Wang 1 1 Zhejiang
More informationRaman Spectroscopy Basics
Raman Spectroscopy Basics Introduction Raman spectroscopy is a spectroscopic technique based on inelastic scattering of monochromatic light, usually from a laser source. Inelastic scattering means that
More informationAMPLIFIED HIGH SPEED FIBER PHOTODETECTOR USER S GUIDE
AMPLIFIED HIGH SPEED FIBER PHOTODETECTOR USER S GUIDE Thank you for purchasing your Amplified High Speed Fiber Photodetector. This user s guide will help answer any questions you may have regarding the
More informationNANO SILICON DOTS EMBEDDED SIO 2 /SIO 2 MULTILAYERS FOR PV HIGH EFFICIENCY APPLICATION
NANO SILICON DOTS EMBEDDED SIO 2 /SIO 2 MULTILAYERS FOR PV HIGH EFFICIENCY APPLICATION Olivier Palais, Damien Barakel, David Maestre, Fabrice Gourbilleau and Marcel Pasquinelli 1 Outline Photovoltaic today
More informationNederland België / Belgique
Cronus Brochure 2 Introduction Cronus: The first spectrometer and colorimeter in one The Cronus is world s first spectrocolorimeter combining a high en VIS spectrometer with a high speed XYZ colorimeter.
More informationA More Efficient Way to De-shelve 137 Ba +
A More Efficient Way to De-shelve 137 Ba + Abstract: Andrea Katz Trinity University UW REU 2010 In order to increase the efficiency and reliability of de-shelving barium ions, an infrared laser beam was
More informationElemental Analyses by ICP-AES
Elemental Analyses by ICP-AES Henry Gong, Senior Analytical Chemist September 10, 2008 ICP-AES inductively coupled plasma atomic emission spectrophotometry Electrons of an atom absorb energy and jump to
More informationLaserLight Networks Inc.
INTRODUCTION Figure 1 Hornet Take Off LaserLight Networks predecessor (LIGHTEC) was awarded a Phase 2 SBIR from the Naval Air Warfare Center Aircraft Division in NJ (NAWCAD/Lk) to design and develop hardware
More informationATOMIC SPECTRA. Apparatus: Optical spectrometer, spectral tubes, power supply, incandescent lamp, bottles of dyed water, elevating jack or block.
1 ATOMIC SPECTRA Objective: To measure the wavelengths of visible light emitted by atomic hydrogen and verify the measured wavelengths against those predicted by quantum theory. To identify an unknown
More informationHow To Understand Light And Color
PRACTICE EXAM IV P202 SPRING 2004 1. In two separate double slit experiments, an interference pattern is observed on a screen. In the first experiment, violet light (λ = 754 nm) is used and a second-order
More informationReliability Test Station. David Cheney Electrical & Computing Engineering
Reliability Test Station David Cheney Electrical & Computing Engineering Overview Turnkey vs. In-house Electrical Stress Protocols System Specifications & Features UF Semiconductor Reliability System Development
More informationHow To Read A Fiber Optic Sensor
2572-17 Winter College on Optics: Fundamentals of Photonics - Theory, Devices and Applications 10-21 February 2014 Optical Fiber Sensors Basic Principles Scuola Superiore Sant'Anna Pisa Italy Optical Fiber
More informationReal-world applications of intense light matter interaction beyond the scope of classical micromachining.
Dr. Lukas Krainer lk@onefive.com CEO Real-world applications of intense light matter interaction beyond the scope of classical micromachining. 1 Management & Company Company Based in Zürich, Switzerland
More informationPIPELINE LEAKAGE DETECTION USING FIBER-OPTIC DISTRIBUTED STRAIN AND TEMPERATURE SENSORS WHITE PAPER
PIPELINE LEAKAGE DETECTION USING FIBER-OPTIC DISTRIBUTED STRAIN AND TEMPERATURE SENSORS WHITE PAPER Lufan Zou and Taha Landolsi OZ Optics Limited, 219 Westbrook Road, Ottawa, ON, Canada, K0A 1L0 E-mail:
More informationROFIN FL SERIES. High Brightness Fiber Lasers Precise, Fast and Reliable.
LASER MACRO ROFIN FL SERIES High Brightness Fiber Lasers Precise, Fast and Reliable. T H E P O W E R O F L I G H T ROFIN FL SERIES THE PRODUCT Ideal Beam Quality for Every Application The high brightness
More informationIntegrated optics Er-Yb amplifier with potassium ion-exchanged glass waveguides
Integrated optics Er-Yb amplifier with potassium ion-exchanged glass waveguides P. Meshkinfam 1, P. Fournier', M.A. Fardad 2, M. P. Andrews 2, and S. I. Najafl' 1 Photonics Research Group, Ecole Polytechnique,
More informationPHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS
PHOTOELECTRIC EFFECT AND DUAL NATURE OF MATTER AND RADIATIONS 1. Photons 2. Photoelectric Effect 3. Experimental Set-up to study Photoelectric Effect 4. Effect of Intensity, Frequency, Potential on P.E.
More informationExtended spectral coverage of BWO combined with frequency multipliers
Extended spectral coverage of BWO combined with frequency multipliers Walter C. Hurlbut, Vladimir G. Kozlov, Microtech Instruments, Inc. (United States) Abstract: Solid state frequency multipliers extend
More informationMillijoules high master-slave pulse ratio 532 nm picosecond laser
Millijoules high master-slave pulse ratio 532 nm picosecond laser Zhao You Fan Zhongwei 1, Bai Zhenao 12, Zhang Guoxin 2, Lian Fuqiang 12, Zhao You 3, Shen Ming 3 1 Academy of Opto-Electronics, Chinese
More informationDIODE LASER BASED PHOTOACOUSTIC SYSTEM FOR ATMOSPHERIC WATER VAPOR MEASUREMENTS
SUMMARY OF PHD THESIS DIODE LASER BASED PHOTOACOUSTIC SYSTEM FOR ATMOSPHERIC WATER VAPOR MEASUREMENTS MIKLÓS SZAKÁLL Consultants: Dr. Gábor Szabó professor, member of the Hungarian Academy of Science Dr.
More informationTOF FUNDAMENTALS TUTORIAL
TOF FUNDAMENTALS TUTORIAL Presented By: JORDAN TOF PRODUCTS, INC. 990 Golden Gate Terrace Grass Valley, CA 95945 530-272-4580 / 530-272-2955 [fax] www.rmjordan.com [web] info@rmjordan.com [e-mail] This
More informationHigh-Performance Wavelength-Locked Diode Lasers
Copyright 29 Society of Photo-Optical Instrumentation Engineers. This paper was published in the proceedings of the SPIE Photonics West 29, Vol. 7198-38 (29), High-Power Diode Laser Technology and High-Performance
More informationLight as a Wave. The Nature of Light. EM Radiation Spectrum. EM Radiation Spectrum. Electromagnetic Radiation
The Nature of Light Light and other forms of radiation carry information to us from distance astronomical objects Visible light is a subset of a huge spectrum of electromagnetic radiation Maxwell pioneered
More informationE190Q Lecture 5 Autonomous Robot Navigation
E190Q Lecture 5 Autonomous Robot Navigation Instructor: Chris Clark Semester: Spring 2014 1 Figures courtesy of Siegwart & Nourbakhsh Control Structures Planning Based Control Prior Knowledge Operator
More informationFIBRE OPTICS & LASERS
FIBRE OPTICS & LASERS PHOTONICS FOR ENGINEERS EDUCATIONAL KITS PHOTONICS EXPERIMENTS FOR ENGINEERS FIBRE OPTICS & LASERS Since lasers and optic systems are a major upcoming drive of nowadays important
More informationThe CVD diamond booklet
available at: www.diamond-materials.com/download Content 1. General properties of diamond... 2 2. Optical Properties... 4 Optical transparency...4 Absorption coefficient at 10.6 µm...5 Refractive index:
More informationL-LAS-TB-CL serie. laser light curtains for inline measuring tasks
L-LAS-TB-CL serie laser light curtains for inline measuring tasks Maximum distance 2.000 mm Measurement range 6 up to 98 mm Resolution up to 4 µm up to 1,5 khz scan rate 0-10 V or 4-20 ma analogue output
More informationPreview of Period 3: Electromagnetic Waves Radiant Energy II
Preview of Period 3: Electromagnetic Waves Radiant Energy II 3.1 Radiant Energy from the Sun How is light reflected and transmitted? What is polarized light? 3.2 Energy Transfer with Radiant Energy How
More informationRadiant Dyes Laser Accessories GmbH
New NarrowScan New Resonator Design Improved Sine Drive Unit Autotracking Frequency doubling, tripling and mixing Wavelength Separation Unit Frequency Stabilization Temperature Stabilization Wavelength
More informationHow To Analyze Plasma With An Inductively Coupled Plasma Mass Spectrometer
What is ICP-MS? and more importantly, what can it do? Inductively Coupled Plasma Mass Spectrometry or ICP-MS is an analytical technique used for elemental determinations. The technique was commercially
More informationSpectraTec II. Polarized Multi-Laser Source BLUE SKY RESEARCH WAVELENGTHS. The SpectraTec II
BLUE SKY RESEARCH The SpectraTec II, two wavelength laser module is a highly integrated system comprised of two lasers, individual driving and temperature control electronics, wavelength combining, and
More informationLimiting factors in fiber optic transmissions
Limiting factors in fiber optic transmissions Sergiusz Patela, Dr Sc Room I/48, Th. 13:00-16:20, Fri. 9:20-10:50 sergiusz.patela@pwr.wroc.pl eportal.pwr.wroc.pl Copying and processing permitted for noncommercial
More informationZecotek S Light Projection Network Marketing
White Paper Zecotek Visible Fiber Laser Platform Enabling the future of laser technology Zecotek Photonics Inc. (TSX- V: ZMS; Frankfurt: W1I) www.zecotek.com is a Canadian photonics technology company
More informationDepartment of Physics and Astronomy Vanderbilt University Nashville, Tennessee- 37203. Nuclear Pumped Laser II. Final Report
Department of Physics and Astronomy Vanderbilt University Nashville, Tennessee- 37203 Nuclear Pumped Laser II Final Report August 1975 - August 1977 NASA Grant Number NSG 1232 by Russell J. DeYoung Ja
More informationDevelopment of Optical Wave Microphone Measuring Sound Waves with No Diaphragm
Progress In Electromagnetics Research Symposium Proceedings, Taipei, March 5 8, 3 359 Development of Optical Wave Microphone Measuring Sound Waves with No Diaphragm Yoshito Sonoda, Takashi Samatsu, and
More informationConcept 2. A. Description of light-matter interaction B. Quantitatities in spectroscopy
Concept 2 A. Description of light-matter interaction B. Quantitatities in spectroscopy Dipole approximation Rabi oscillations Einstein kinetics in two-level system B. Absorption: quantitative description
More informationUnderstanding Laser Beam Parameters Leads to Better System Performance and Can Save Money
Understanding Laser Beam Parameters Leads to Better System Performance and Can Save Money Lasers became the first choice of energy source for a steadily increasing number of applications in science, medicine
More informationMCQ - ENERGY and CLIMATE
1 MCQ - ENERGY and CLIMATE 1. The volume of a given mass of water at a temperature of T 1 is V 1. The volume increases to V 2 at temperature T 2. The coefficient of volume expansion of water may be calculated
More informationChapter 5. Second Edition ( 2001 McGraw-Hill) 5.6 Doped GaAs. Solution
Chapter 5 5.6 Doped GaAs Consider the GaAs crystal at 300 K. a. Calculate the intrinsic conductivity and resistivity. Second Edition ( 2001 McGraw-Hill) b. In a sample containing only 10 15 cm -3 ionized
More informationStatus of the HOM Damped Cavity for the Willy Wien Ring
Status of the HOM Damped Cavity for the Willy Wien Ring Ernst Weihreter / BESSY Short Review of HOM Damped Cavity Prototype Modifications for the Willy Wien Ring Cavity Results of Low Power Measurements
More informationLBS-300 Beam Sampler for C-mount Cameras. YAG Focal Spot Analysis Adapter. User Notes
LBS-300 Beam Sampler for C-mount Cameras P/N SP90183, SP90184, SP90185 and SP90186 YAG Focal Spot Analysis Adapter P/N SP90187, SP90188, SP90189, SP90190, SP90191 User Notes Ophir-Spiricon Inc. 60 West
More informationPower Laser Trends. Dr. Ch. Harder July 2, 2009 harder@swisslaser.net
Power Laser Trends Dr. Ch. Harder July 2, 2009 harder@swisslaser.net Power Laser Trends Distinguish between Non-Diode and Diode Laser Market Non-Diode laser market All lasers except direct diodes, i.e.
More informationIt has long been a goal to achieve higher spatial resolution in optical imaging and
Nano-optical Imaging using Scattering Scanning Near-field Optical Microscopy Fehmi Yasin, Advisor: Dr. Markus Raschke, Post-doc: Dr. Gregory Andreev, Graduate Student: Benjamin Pollard Department of Physics,
More informationVolumes. Goal: Drive optical to high volumes and low costs
First Electrically Pumped Hybrid Silicon Laser Sept 18 th 2006 The information in this presentation is under embargo until 9/18/06 10:00 AM PST 1 Agenda Dr. Mario Paniccia Director, Photonics Technology
More informationLaser-induced surface phonons and their excitation of nanostructures
CHINESE JOURNAL OF PHYSICS VOL. 49, NO. 1 FEBRUARY 2011 Laser-induced surface phonons and their excitation of nanostructures Markus Schmotz, 1, Dominik Gollmer, 1 Florian Habel, 1 Stephen Riedel, 1 and
More informationCopyright 1999 2010 by Mark Brandt, Ph.D. 12
Introduction to Absorbance Spectroscopy A single beam spectrophotometer is comprised of a light source, a monochromator, a sample holder, and a detector. An ideal instrument has a light source that emits
More informationINFRARED MONITORING OF 110 GHz GYROTRON WINDOWS AT DIII D
GA A23981 INFRARED MONITORING OF 110 GHz GYROTRON WINDOWS AT DIII D by Y. GORELOV, J. LOHR, R.W. CALLIS, and D. PONCE MAY 2002 DISCLAIMER This report was prepared as an account of work sponsored by an
More information2 Absorbing Solar Energy
2 Absorbing Solar Energy 2.1 Air Mass and the Solar Spectrum Now that we have introduced the solar cell, it is time to introduce the source of the energy the sun. The sun has many properties that could
More informationUltrafast Optical Characterization of Novel Mid-Infrared Nanoscale Structures
NSF ERC MIRTHE Summer Symposium, Princeton University, June 15-16, 2015 Ultrafast Optical Characterization of Novel Mid-Infrared Nanoscale Structures Dr. Anthony M. Johnson, Director* Center for Advanced
More informationEnergy band diagrams. Single atom. Crystal. Excited electrons cannot move. Excited electrons can move (free electrons)
Energy band diagrams In the atoms, the larger the radius, the higher the electron potential energy Hence, electron position can be described either by radius or by its potential energy In the semiconductor
More informationQGA Quantitative Gas Analyser
QGA Quantitative Gas Analyser A compact bench-top system for real-time gas and vapour analysis Detailed product information / introduction catalysis studies environmental gas analysis fermentation off-gas
More informationHow To Use A Kodak Kodacom 2.5D (Kodak) With A Power Supply (Power Supply) And Power Supply
Reflective Optical Sensor with Transistor Output Description The CNY7 has a compact construction where the emitting light source and the detector are arranged in the same direction to sense the presence
More informationEncoders for Linear Motors in the Electronics Industry
Technical Information Encoders for Linear Motors in the Electronics Industry The semiconductor industry and automation technology increasingly require more precise and faster machines in order to satisfy
More informationRealization of a UV fisheye hyperspectral camera
Realization of a UV fisheye hyperspectral camera Valentina Caricato, Andrea Egidi, Marco Pisani and Massimo Zucco, INRIM Outline Purpose of the instrument Required specs Hyperspectral technique Optical
More informationMolecular Spectroscopy:
: How are some molecular parameters determined? Bond lengths Bond energies What are the practical applications of spectroscopic knowledge? Can molecules (or components thereof) be identified based on differences
More informationThe photoionization detector (PID) utilizes ultraviolet
Chapter 6 Photoionization Detectors The photoionization detector (PID) utilizes ultraviolet light to ionize gas molecules, and is commonly employed in the detection of volatile organic compounds (VOCs).
More informationAS COMPETITION PAPER 2008
AS COMPETITION PAPER 28 Name School Town & County Total Mark/5 Time Allowed: One hour Attempt as many questions as you can. Write your answers on this question paper. Marks allocated for each question
More informationSynthetic Sensing: Proximity / Distance Sensors
Synthetic Sensing: Proximity / Distance Sensors MediaRobotics Lab, February 2010 Proximity detection is dependent on the object of interest. One size does not fit all For non-contact distance measurement,
More information3 - Atomic Absorption Spectroscopy
3 - Atomic Absorption Spectroscopy Introduction Atomic-absorption (AA) spectroscopy uses the absorption of light to measure the concentration of gas-phase atoms. Since samples are usually liquids or solids,
More informationRecording the Instrument Response Function of a Multiphoton FLIM System
Recording the Instrument Response Function of a Multiphoton FLIM System Abstract. FLIM data analysis in presence of SHG signals or extremely fast decay components requires the correct instrument response
More informationTowards large dynamic range beam diagnostics and beam dynamics studies. Pavel Evtushenko
Towards large dynamic range beam diagnostics and beam dynamics studies Pavel Evtushenko Motivation Linacs with average current 1-2 ma and energy 1-2.5 GeV are envisioned as drivers for next generation
More information8.1 Radio Emission from Solar System objects
8.1 Radio Emission from Solar System objects 8.1.1 Moon and Terrestrial planets At visible wavelengths all the emission seen from these objects is due to light reflected from the sun. However at radio
More informationMetastability Exchange Optical Pumping of Helium-3 at High Pressures and 1.5 T: Comparison of two Optical Pumping Transitions
Metastability Exchange Optical Pumping of Helium-3 at High Pressures and 1.5 T: Comparison of two Optical Pumping Transitions Marie Abboud, Alice Sinatra, Geneviève Tastevin, Pierre-Jean Nacher, Xavier
More informationCoating Technology: Evaporation Vs Sputtering
Satisloh Italy S.r.l. Coating Technology: Evaporation Vs Sputtering Gianni Monaco, PhD R&D project manager, Satisloh Italy 04.04.2016 V1 The aim of this document is to provide basic technical information
More informationEngineering Sciences 151. Electromagnetic Communication Laboratory Assignment 3 Fall Term 1998-99
Engineering Sciences 151 Electromagnetic Communication Laboratory Assignment 3 Fall Term 1998-99 WAVE PROPAGATION II: HIGH FREQUENCY SLOTTED LINE AND REFLECTOMETER MEASUREMENTS OBJECTIVES: To build greater
More informationA Guide to Acousto-Optic Modulators
A Guide to Acousto-Optic Modulators D. J. McCarron December 7, 2007 1 Introduction Acousto-optic modulators (AOMs) are useful devices which allow the frequency, intensity and direction of a laser beam
More informationLab 9: The Acousto-Optic Effect
Lab 9: The Acousto-Optic Effect Incoming Laser Beam Travelling Acoustic Wave (longitudinal wave) O A 1st order diffracted laser beam A 1 Introduction qb d O 2qb rarefractions compressions Refer to Appendix
More information