RECENT DEVELOPMENT IN SUM FREQUENCY GENERATION SPECTROSCOPY SYSTEMS

Slides:



Advertisements
Similar presentations
Photoinjector Lasers for Ultra-Bright Electron Sources
Advertisements

LASER BASED SENSOR FOR DETECTION OF TRACE GASES IN THE ENVIRONMENT M. A. Gondal, I. A. Bakhtiari and Z. H. Yamani Laser Research Laboratory & Physics.
Raman Spectroscopy A) Introduction IR Raman
OL 750 Diffuse Spectral Reflectance Measurement System
Sub-Doppler Resolution Spectroscopy of the fundamental band of HCl with an Optical Frequency Comb ○ K. Iwakuni, M. Abe, and H. Sasada Department of Physics,
Ultrafast XUV Coherent Diffractive Imaging Xunyou GE, CEA Saclay Director : Hamed Merdji.
Presented By: Gaurav C Josan Department - EE NON-LINEAR OPTICS NON LINEAR OPTICS.
Excitation processes during strong- field ionization and dissociatation of molecules Grad students: Li Fang, Brad Moser Funding : NSF-AMO November 29,
Ultrafast Spectroscopy
Ch 6: Optical Sources Variety of sources Variety of sources LS considerations: LS considerations: Wavelength Wavelength  Output power Output power Modulation.
Microwave Spectroscopy I
Stimulated Raman scattering If high enough powered radiation is incident on the molecule, stimulated Anti-Stokes radiation can be generated. The occurrence.
Introduction to Infrared Spectrometry Chap 16. Quantum Mechanical Treatment of Vibrations Required to include quantized nature of E From solving the wave.
Are you getting the concept? Calculate D a, D l, R d and s g for 1 st order diffraction under optimal conditions for the indicated 0.5 m grating with 100.
ARC 11/02/10 Recent Advances in Surface Plasmon Resonance: From Biosensor to Space/astronomical Interest Hololab and CSL S. Habraken, C. Lenaerts, and.
Neodymium:YAG Laser Nd3+ in yttrium-aluminum-garnet (Y3Al5O12)
Lecture 3 INFRARED SPECTROMETRY
Surface Enhanced Raman Spectroscopy (SERS) Jeanne Bonner PHYS 275 November 26, 2007.
Common types of spectroscopy
High-speed ultrasensitive measurements of trace atmospheric species 250 spectra in 0.7 s David A. Long A. J. Fleisher, D. F. Plusquellic, J. T. Hodges.
 PART Requirements for Spectroscopic Techniques for Polymers 1. High resolution 2. High sensitivity (>1%) 3. High selectivity between molecular.
30. Nov I.Will, G. Klemz, Max Born Institute: Optical sampling system Optical sampling system for detailed measurement of the longitudinal pulse.
What is spectroscopy? It is the study of how matter interacts with electromagnetic radiation (gamma rays down to radio waves) Matter can interact with.
DMP Product Portfolio Femtosecond Lasers Trestles Ti:Sapphire lasers …… fs; nm, mW Mavericks Cr:Forsterite lasers
PicoTRAIN IC Only oscillator (no MOPA design)  more simplicity and reliability Dimensions: 480*200*101.6mm3 ongoing volume production High stability.
A 5 fs high average power OPCPA laser system for attosecond pulse production Philip Bates, Yunxin Tang, Emma Springate and Ian Ross Central Laser Facility,
Spectroscopic Line Shapes Of Broad Band Sum Frequency Generation Himali Jayathilake Igor Stiopkin, Champika Weeraman, Achani Yatawara and Alexander Benderskii.
Infrared Spectroscopy Chapters Chapter 7- I.
4 TH IOS, SZCZYRK 2010 PL0471 A. Waz, P. Kaczmarek, A. Antończak, J. Sotor, G. Soboń, M. Walczakowski, K. M. Abramski Laser & Fibre Electronics Group,
Observation of Excited Biexciton States in CuCl Quantum Dots : Control of the Quantum Dot Energy by a Photon Itoh Lab. Hiroaki SAWADA Michio IKEZAWA and.
Optical Characterization methods Rayleigh scattering Raman scattering transmission photoluminescence excitation photons At a glance  Transmission: “untouched”
Nanonics MultiView 2000™ Product Presentation. MultiView 2000 ™ Complete System MultiView 2000™ Product Presentation.
The Nobel Prize in Physics 1930 "for his work on the scattering of light and for the discovery of the effect named after him" Sir Chandrasekhara Venkata.
Automated 2D IR Spectroscopy using a high repetition rate laser system
FEMTOSECOND LASER FABRICATION OF MICRO/NANO-STRUCTURES FOR CHEMICAL SENSING AND DETECTION Student: Yukun Han MAE Department Faculty Advisors: Dr. Hai-Lung.
WDM Fiber Vibrometry Krzysztof M. Abramski.
Optronic Laboratories Inc. OL Series 750 Automated Spectroradiometric Measurement System Optronic Laboratories Inc. OL Series 750 Automated Spectroradiometric.
4-Level Laser Scheme. He-Ne Laser Tunable Dye Lasers.
Fluorescence Spectroscopy
Dr Gihan Gawish King Saud University Riyadh Saudi Arabia 1.
Spectrophotometry.
Micro-mirror Supervisor: Prof. Kämper Team member: Chun Wa George Young Issis Contreras Ramanathan Swaminathan Spandan Shroff Micromechatronics.
OL 750 Measurement Systems OL 750 Measurement Systems Optronic Laboratories, Inc.
LIGO-G09xxxxx-v1 Form F v1 Development of a Low Noise External Cavity Diode Laser in the Littrow Configuration Chloe Ling LIGO SURF 2013 Mentors:
Oscillator stability & ASE Reduction
Laser System Upgrade Overview
Ultrafast Terahertz Kerr Effect Spectroscopy: Detection of Intramolecular Vibrational Coherences Marco Allodi, Ian Finneran, Geoffrey Blake California.
MultiView 1000™ Product Presentation Nanonics MultiView 1000™
SPECTRAL PRODUCTS INTRODUCTION 111 Highland Drive, Putnam, CT 06260, USA (East Office) 2659A Pan American Freeway NE, Albuquerque, NM 87107, USA (West.
1 Dual Etalon Frequency Comb Spectrometer David W. Chandler and Kevin E. Strecker Sandia National Laboratories – Biological and Energy Sciences Division.
Ultra-stable, high-power laser systems Patrick Kwee on behalf of AEI Hannover and LZH Advanced detectors session, 26. March 2011 Albert-Einstein-Institut.
The dye is a large molecule with a large number of closely spaced vibrational states – essentially a continuum of states. The pump pulse populates the.
DECam Spectrophotometric Calibration DECam calibration workshop, TAMU April 20 th, 2009 Jean-Philippe Rheault, Texas A&M University.
RAMAN EFFECT.
The Electromagnetic Spectrum High Harmonic Generation
Status of the SPARC laser and “dazzler” experiments
H1 Squeezing Experiment: the path to an Advanced Squeezer
Components of Optical Instruments
Mingyun Li & Kevin Lehmann Department of Chemistry and Physics
by: Mrs. Aboli N. Moharil Assistant Professor, EXTC dept.
Integrated Semiconductor Modelocked Lasers
Single and dual wavelength Er:Yb double clad fiber lasers
Principle of Mode Locking
OL 750 Measurement Systems
Fibre Lasers for SILIcon testing
High harmonic generation in a large-volume capillary for seeding of free-electron lasers Siew Jean Goh.
Fiber Laser Part 1.
LCLS Injector Laser System Paul R. Bolton, SLAC April 24, 2002
Injector Drive Laser Technical Status
OL 750 Spectroradiometer & Linear Spectral Transmission Measurements
Presentation transcript:

RECENT DEVELOPMENT IN SUM FREQUENCY GENERATION SPECTROSCOPY SYSTEMS Michael Patterson, Lucian Hand Altos Photonics, Bozeman, MT Zenonas Kuprionis EKSPLA UAB, Vilnius, Lithuania

Outline 50 Hz SFG spectrometer Double resonance SFG SFG imaging microscope USB-CAN data acquisition system

50 Hz Sum Frequency Generation Spectrometer PL2241 series – new generation of picosecond lasers Features: Robust, reliable diode pumped oscillator Folded, more stable regenerative amplifier Frequencies up to 250 Hz Wide range of output energies Disadvantages of our standard SFG spectrometer: Long spectra acquisition time Complicated maintenance New 50 Hz system: Up to five time faster data acquisition More easy maintenance PL2241/50 + PG501 Compromise of high repetition rate and high enough output energy Efficient pump source for SFG set-up

50 Hz Sum Frequency Generation Spectrometer: Spectra samples

Double resonance SFG option Doubly resonant SFG spectrum selectively enhances the vibrational modes through their electron-vibration coupling Features Two parametrical generators pumped by single powerful laser Wide tunability of VIS wavelength 210 – 680 nm Triple monochromator for tunable VIS rejection Automatic compensation of tunable VIS delay Special design for high UV throughput Doubly resonant enhancement of Rhodamine SFG spectra

SFG imaging microscope (joint project with Steven Baldelli group, HU) ICCD Tube lens Notch filters Objective Diffraction grating Sample 1064 nm beam IR beam 1064 nm Filter 532 nm Filter Design Far field imaging Detection via an intermediate image on the surface of a blazed grating Upgradeable option of standard EKSPLA SFG spectrometer An image of ODT covered etched gold sample. The first lines are spaced, in order left -right  20, 5, 2, and 8 micrometers. Image taken at ωIR=2875 cm-1 and acquired for 5000 laser shots.

Information transfer USB-CAN bus What is “Controller Area Network” ? CAN is a serial bus system especially suited for networking “intelligent” devices as well as sensors and actuators within a system or sub-system What can Ekspla offer for this type of system? Si, Ge, GaAs ... photodiode-based photodetectors PMT-based photodetectors Motion controller Laser diode power supply HV power supply TEC cooler controller

Take advantage of our 10 years experience in SFG We offer: Highly qualified consultations and assistance Picosecond lasers with outstanding stability Picosecond OPG/OPA/DFG Laser accessories and components Photonics components, beam delivery optics