Real-Time Measurements, Rogue Events and Photon Economics

Size: px
Start display at page:

Download "Real-Time Measurements, Rogue Events and Photon Economics"

Transcription

1 Real-Time Measurements, Rogue Events and Photon Economics Bahram Jalali UCLA Science Faculty Research Colloquium May 27, 2009 Also presented at the University of Arizona, Tucson, Az. September 17, 2009, and University of Colorado, Boulder, Co. September 21,

2 Outline Examples of rogue events Their unusual statistics Difficulty in studying them Ultrafast phenomenon provides a good testbed and window Technical challenges and scientific tools needed Time-stretch technology Platform for creating real-time ultrafast t instruments t Extreme phenomenon observed in optics (Nature, December 2007) Taming and harvesting the extreme events Connection with socioeconomics Time-stretch imaging and its application to finding rare cancer cells (Nature, April 30, 2009) 2

3 Rogue Events, Outliers, Black Swans Singular, rare, but with massive impact A hallmark of complex systems Occur in social, financial and physical science Past behavior does not predict the future Risk analysis models fail October 2008 crash Do ow Jones Ind dustrial Avera age Stock Market Crashes Year 3

4 Other Examples of Extreme Events Rogue waves on the high seas Suwa-Maru sinks off the cost of Japan under moderate sea conditions (2008) Believed to be fiction until recently Natural disasters Evolution, survival of the fittestt DNA mutation Cancer: Single rogue cell triggers prostate cancer G.S. Bova et al. Nature Medicine, 2009 Rogue waves Communication Spontaneous noise Wave Height Fractal behavior, cantor set PMD errors in optical communication networks Time Size distribution of innovations 4

5 Highly Non-Gaussian Probability Distributions Highly Skewed power-law functions Characterized by a Heavy-tail Events much larger than the mean do occur Probability/Risk is much higher than predicted by Gaussian Classification using Mean and S.D. is inadequate Great impact in both finance and engineering Risk / Error Rate models fail Karl Gauss Extreme Value Distribution Probabili ity x exp Event Magnitude 5

6 Examples of power laws Phenomena * Phenomenon Approx. Exponent Net worth of Americans 1.1 Website hits 1.4 Book sales 1.5 Probab bility Bill Gates Magnitude Exponent Share of top 1% Share of top 20% % 86% % 58% 2 10% 45% Winner Takes All Survival of the Fittest *Nassim Taleb, Black Swans,

7 It s Difficult to Model and Predict Extreme Events Understanding and modeling is hampered by Scarcity of the events Inability to do experiments Examples: oceanic rogue waves or financial markets Ultrafast phenomena provide an opportunity More data in a short time Laboratory experiments under controlled conditions Enough data to develop models and ability to test them 7

8 Extreme Value Events in Ultrafast Science Basic ingredients: noise and nonlinearities are present in: Electronic circuits: micro-seconds to nano-seconds Laser optics: pico-seconds to femto-seconds Many similarities il iti between optics and hydrodynamics d Soliton: wave packet that travels without spreading Turbulence occurs in both media Even gravitational field has an equivalent in optics Common mathematics in the form of NLSE Optical power => fluid density Optical Chirp => fluid velocity Soliton on a bed: group stays together Slowest runner Fastest runner 8

9 Can Ultrafast Phenomena Unveil the Mystery of Extreme Events? Opportunity: Controlled experiments in Table-top testbed Understand the underlying science Learn to engineer and harvest them Challenge: Detecting needle in haystack Requires: fine resolution, non-stop, high throughput Need to understand two classes of instruments: Equivalent time vs. real-time 9

10 Equivalent-time (sampling) Instruments Workhorse of ultrafast research Slows down the event using strobe light effect Works only for repetitive events Strobe light Doesn t really slow down the event, just under-samples it Cannot capture singular, transient events Picosolve TM : 600 Gsample/s equivalent time But only 20 Msample/s real-time! 10

11 Real-time Instruments Fine time resolution, no-stop sampling and long record lengths Holly grail of instrumentation technology What if we can stretch time? Truly slow down events Central theme behind a new class of instruments being developed at UCLA Persistence of Memory, Salvador Dali, 1931 Bahram Jalali & Fredric Coppinger, Data conversion via time manipulation, US Patent # 6,288,

12 Our Portfolio of Real-time Instruments Enabled by Time-stretch Time Stretch Digitizer Ali Motafakker Peter DeVore Brandon Buckley Shalabh Gupta Spectrometer Daniel Solli Jason Chou Camera Keisuke Goda Ata Mahjoubfar Ali Motafakker Kevin Tsia 12

13 Our Approach to Ultrafast Real-time Instrumentation Information to spectrum conversion Spectrum to time conversion Information + Step 1: Femtosecond pulse Group = Velocity Dispersion Map the high speed information onto the spectrum of a femtosecond pulse + = Step 2: Stretched pulse Spectrum is mapped into time Stretch the spectrum into time Digitize the slow waveform (and amplify at the same time) Real-time digitizer Time Stretch allows ultrafast events to be captured in real-time with conventional electronics 13

14 Time Stretch Enhanced Digitizer Work supported by U. Arizona NSF CIAN ERC & DARPA electrical Fast Electrical signal Time optical Time Stretch electrical Stretched electrical signal Electronic Digitizer Dispersion Chirped Pulse Source Optical modulator PD 45-Gbps data captured using 1.5-GHz digitizer Chirped pulses Stretched pulse F. Coppinger, A. Bhushan, B. Jalali, Electronics Letters, 34 (4), Boosts the performance of electronics S. Gupta, A. Motafakker, B. Jalali, Appl. Phys. Lett UCLA Photonics Lab 14

15 Digitizing at 10 Trillion-times per Second in Real-time! 10 Tsample/s Transient Digitizer Sampling Interval = 100 fs 100 fs per conversion step Time stretch extends the performance of electronic digitizers to capture ultrafast events Creates the backend data acquisition needed to capture, store and analyze extreme value events J. Chou, O. Boyraz, D. Solli, and B. Jalali Appl. Phys. Lett. 91, (2007) 15

16 Time-stretch is not a Time Lens Time Lens Time Stretch Time-stretch is a Dispersive Analog Optical Link No need to disperse input signal No need to satisfy the lens equation B. Jalali, et al, Nature Photonics 3, 8-10 (2009) 16

17 Capturing Fast Optical Signals Requirement: fast and non-stop (real-time) Pump-probe Technique Pros: Ultra-fine temporal resolution Long delay Cornerstone of femto-chemistry Cons: Not a real-time technique Only works for repetitive events not applicable to random and rare events Spectrometer Prism CCD Camera Pros: detailed spectral information Cons: Too slow 17

18 A Brief History of Spectroscopy 1666: Newton uses lens and prism to disperse sunlight onto a screen 1812: Fraunhofer develops diffraction grating 1826: Kirchhoff and Bunsen use gratings to show that each element and compound has its own unique spectrum Newton Fraunhofer Kirchoff & Bunsen Fraunhofer demonstrates spectroscopy Speed ~ KHz Modern Optical Spectrum Analyzer 18

19 f Time-stretch also Performs Fourier Transform it i. Z t F e e 2. Z total Dispersive Fourier Transformation ~ 2 / 2 dispersion in seconds/hz 2 d f t ~ i 2 Z t 2 2 z F e 2 d Non - zero only if t 2 z frequency to time mapping 2 t z 2 ( stationary phase approximat ion) Real-time Digitizer Time samples D. Solli, J. Chou, B. Jalali, Nature Photonics, 2008 Absorption or Raman Spectrum Group Velocity Dispersion 19 Time 19

20 Time Stretch Spectrometer Group Velocity Dispersion (GVD) wavelength wavelength Femto-second pulse -470 time 760 Time (ps ) time Time Single-shot Carbon monoxide 8 pico-meter resolution mission Acetylene 20 km fiber CO Trans OSA Wavelength ( nm) Time (ns) P. Kelkar and B. Jalali, Electronics Letters, 1999 J. Chou, D. Solli, B. Jalali, Appl. Phys. Lett, 2008 Spectra acquired at > million times per second Measured without a spectromter Electronic digitizer becomes the spectrometer 20

21 Outline Needle in the haystack problems and significance of rare and extreme events Difficult to study and mystery surrounding them Ultrafast phenomenon provides a testbed Scientific tools needed for the job and the challenge Real-time vs. equivalent time measurements UCLA s time stretch technology Platform for creating real-time ultrafast instruments Observation of extreme value phenomenon in optics Two examples of recent observations Triggering and harvesting extreme events Ultrafast imaging and the problem of finding rare but diseased cells 21

22 Observation of Extreme Events in Optics Amplification of laser pulses in silicon Simple but describes key ingredients Generation of supercontinuum pulses in optical fibers Complex phenomenon with connection to oceanic rogue waves 22

23 Optical Amplification in Silicon First demonstrated at UCLA in 2002 Pump Weak input Silicon Amplified Output 23

24 Extreme Value Statistics during optical amplification in Silicon Input distribution Output distribution Heavy tail Optical pulses follow the Pareto 80/20 law Photon Economics Unlikely connection between photonics and socioeconomics Both processes governed by the survival of the fittest Due to nonlinear response giving strong preference to the fittest 24 David Borlaug and Bahram Jalali, LEOS

25 Making Sense of the Extreme Behavior f ( G) G 1 b / 2 2 b 2 2 Exp I 0 bln( G) 2 Model Measured Heavy tail / power law Heavy tail / power law Results suggest 2 ingredients are necessary 1. Noise / fluctuations in the initial conditions 2. Nonlinear response to the fluctuations 25

26 Optical Rogue Waves D.R. Solli, C. Ropers, P. Koonath B. Jalali, Nature

27 Narrowband input pulse The Experiment Nonlinear fiber Broadband Soliton An nonlinear phenomena Produces white light solitons Resemblance to solitons in water: Common mathematical foundation Both described by the same differential equation Work performed under DARPA PHOBIAC program 27

28 Optical Rogue Waves D.R. Solli, C. Ropers, P. Koonath, B. Jalali, Nature Rare but intense flashes of white light are produced Simulations can reproduce observed statistics What is causing these rare but dramatic events? 28

29 Finding the Culprit The culprit is a particular type of noise at the input Intentionally introducing it seeds a rogue pulse Seed is very weak, 1/10,000 of the input Explains unpredictability of rare events 29 D.R. Solli, C. Ropers, B. Jalali, Phys. Rev. Lett.,

30 Amplitude and Phase Noise Reduction via Stimulated Supercontinuum Generation Amplitude and phase of the output light become dramatically more stable Phase transition from an disordered to an ordered state of optical radiation D.R. Solli, C. Ropers, B. Jalali, Phys. Rev. Lett.,

31 Outline Needle in the haystack problems and significance of rare and extreme events Difficult to study and mystery surrounding them Ultrafast phenomenon provides a testbed Scientific tools needed for the job and the challenge Real-time vs. equivalent time measurements UCLA s time stretch technology Platform for creating real-time ultrafast instruments Examples of extreme value phenomenon observed in optics Understanding, triggering and harvesting the extreme events Ultrafast imaging and the problem of finding rare cells 31

32 Rogue Cells in Cancer 14 year by John Hopkins Medical School Steven Bova, et al., Nature Medicine,

33 Rogue Events in Biology & Medicine Circulating Tumor Cell (CTC) Breast cancer cells Prof. Dino Di Carlo UCLA Biomedical Engineering Precursors to metastasis Accounts for 90% of cancer mortality Detection of CTC s in blood may offer life saving benefits First commercial device named Top Medical Breakthrough of 2009 Morphologically different than normal cells Potentially detectable via imaging 33

34 Detecting CTCs: Needle in a Haystack Problem CTCs are extremely rare ~1 cell in milliliter of blood 1 ml = 5 billion cells Need to look at billions of cells! Speed of today s fastest cameras: < 1000 cells per second possible 2 months to find a single cell Need a much faster instrument: camera 34

35 UCLA s STEAM* Technology World s Fastest Imager K. Goda, K. Tsia, B. Jalali, Nature \..\..\Pictures\STEAM\STEAM Movies\movie1.wmv * Serial Time Encoded Amplified Microscopy (STEAM) 35

36 Taking Pictures with an Oscilloscope! ns 163 Single image frame Time (ns) Time Temporal waveform Waveform Captured by Oscilloscope (oscilloscope) Voltage (mv) Power (mw) Spectrum Measured by Optical Spectrum Analyzer (Spectrometer) Voltage (mv) Time (ns) Wavelength e (nm) K. Goda, K. K. Tsia, and B. Jalali, Nature, 458, (2009) 36

37 Real-time Imaging of Micro-fluidic Transport Spatial resolution: ~1 micron (diffraction limited) Frame interval: 163 ns Shutter speed: 450 ps World s fastest continuous camera Image obtained using single pixel detector 37

38 Time-stamping of Laser Mframes/sec 38

39 STEAM Imager in the news: 15 minutes of fame 39

40 Mechanical-scan-free Laser Microsurgery with Real-time Microscopy K. K. Tsia, K. Goda, and B. Jalali, Optics Letters 34 (2009) 40

41 Laser Microsurgery without mechanical Scanning & with Real-time Imaging Spectral-shower Encoded Confocal Microscopy and Microsurgery (SECOMM) 41 Ablation beam directed to location by tuning the laser wavelength No manual or mechanical motion necessary Micrometer position accuracy Application to Cancer: identification and purging of contaminated (Rogue) cells for Stem Cell Transplant In Collaboration UCLA Medical School 41

42 Summary Extreme, rogue events appear in diverse range of systems and have dramatic Behavior provides a window into complex systems Studying them has been challenging Ultrafast phenomena provides an opportunity Real-time tools based on the time stretch concept are making this possible Insight gained is offering clues about causes them and means to control harvest them New tools hold promise for studying rare events in biological systems Detection of rogue cells in metastatic cancer 42

43 Thanks To my Team: Daniel Solli Keisuke Goda David Borlaug Sasan Fathpour Kevin Tsia Shalabh Gupta Ali Motafakker Jason Chou 43

Time-Stretch Imaging and its Applications to High-throughput Microscopy and Microsurgery

Time-Stretch Imaging and its Applications to High-throughput Microscopy and Microsurgery Research Highlights Time-Stretch Imaging and its Applications to High-throughput Microscopy and Microsurgery Bahram Jalali,2, Keisuke Goda,2, Patrick Soon-Shiong 3, Kevin K. Tsia,4 Photonics Laboratory,

More information

The Temporal Gearbox

The Temporal Gearbox The Temporal Gearbox B. Jalali*, J. C.K. Chan, A. Mahjoubfar, D. Solli, M. H. Asghari University of California, Los Angeles, 420 Westwood Plaza, Los Angeles, 90095, USA ABSTRACT We are inspired by mechanical

More information

Ultrafast web inspection with hybrid dispersion laser scanner

Ultrafast web inspection with hybrid dispersion laser scanner Ultrafast web inspection with hybrid dispersion laser scanner Hongwei Chen, 1,2,3 Chao Wang, 1,4 Akio Yazaki, 1,5 Chanju Kim, 1 Keisuke Goda, 1,6,7,8, * and Bahram Jalali 1,6,7 1 Department of Electrical

More information

Company Pioneer in Ytterbium ultrafast lasers High quality manufacturing Intense and active R&D Located in Bordeaux and Paris US offices in Boston and

Company Pioneer in Ytterbium ultrafast lasers High quality manufacturing Intense and active R&D Located in Bordeaux and Paris US offices in Boston and High power ultrafast lasers Eric Mottay High Brightness Laser sources Burgdorf, November 26, 2009 Company Pioneer in Ytterbium ultrafast lasers High quality manufacturing Intense and active R&D Located

More information

Real time micro/nano particle detection and tracking with. nanosecond resolution

Real time micro/nano particle detection and tracking with. nanosecond resolution Real time micro/nano particle detection and tracking with nanosecond resolution Feng Qian, Qi Song, En-kuang Tien, Ozdal Boyraz Advanced Photonics and Devices Laboratory, EECS Department, University of

More information

Breaking Speed and Sensitivity Limits

Breaking Speed and Sensitivity Limits Breaking Speed and Sensitivity Limits Real-Time Diagnostics with Serial Time-Encoded Amplified Microscopy High-throughput imaging is needed to identify rare diseased cells among a large population of healthy

More information

High-throughput optical coherence tomography at 800 nm

High-throughput optical coherence tomography at 800 nm High-throughput optical coherence tomography at 800 nm Keisuke Goda, 1,2,3,* Ali Fard, 1,2,4 Omer Malik, 1 Gilbert Fu, 1 Alan Quach, 1 and Bahram Jalali 1,2,3,5 1 Department of Electrical Engineering,

More information

Physics 625 Femtosecond laser Project

Physics 625 Femtosecond laser Project Physics 625 Femtosecond laser Project The purpose of this project is for each person to gain experience in designing part of a femtosecond laser system for pump-probe experiments. The system diagram is

More information

Attosecond Optics. Zenghu Chang Kansas State University University of Central Florida

Attosecond Optics. Zenghu Chang Kansas State University University of Central Florida Attosecond Optics Zenghu Chang Kansas State University University of Central Florida CREOL Industrial Affiliates day, April 9, 2010 Why attosecond pulses? Zeptosecond (10-21 s) Attosecond (10-18 s) Femtosecond

More information

Development of Ultrafast CXRS system in Heliotron J. Graduate School of Energy Science Kyoto University LU XIANGXUN 03/15/2016

Development of Ultrafast CXRS system in Heliotron J. Graduate School of Energy Science Kyoto University LU XIANGXUN 03/15/2016 1 Development of Ultrafast CXRS system in Heliotron J Graduate School of Energy Science Kyoto University LU XIANGXUN 03/15/2016 2 Outline 1. Introduction 2. Charge exchange Recombination Spectroscopy (CXRS)

More information

picoemerald Tunable Two-Color ps Light Source Microscopy & Spectroscopy CARS SRS

picoemerald Tunable Two-Color ps Light Source Microscopy & Spectroscopy CARS SRS picoemerald Tunable Two-Color ps Light Source Microscopy & Spectroscopy CARS SRS 1 picoemerald Two Colors in One Box Microscopy and Spectroscopy with a Tunable Two-Color Source CARS and SRS microscopy

More information

HOLOGRAPHIC FEMTOSECOND LASER PROCESSING AND THREE-DIMENSIONAL RECORDING IN BIOLOGICAL TISSUES

HOLOGRAPHIC FEMTOSECOND LASER PROCESSING AND THREE-DIMENSIONAL RECORDING IN BIOLOGICAL TISSUES Progress In Electromagnetics Research Letters, Vol. 2, 115 123, 2008 HOLOGRAPHIC FEMTOSECOND LASER PROCESSING AND THREE-DIMENSIONAL RECORDING IN BIOLOGICAL TISSUES Y. Hayasaki Department of Optical Science

More information

Sensor based adaptive laser micromachining using ultrashort pulse lasers for zero-failure manufacturing

Sensor based adaptive laser micromachining using ultrashort pulse lasers for zero-failure manufacturing Sensor based adaptive laser micromachining using ultrashort pulse lasers for zero-failure manufacturing Fraunhofer Institute for Production Technology, Aachen M. Sc. Guilherme Mallmann Prof. Dr.-Ing. Robert

More information

Laser readiness for all optical EUV FEL

Laser readiness for all optical EUV FEL Laser readiness for all optical EUV FEL Akira Endo EUVA (Extreme Ultraviolet Lithography System Development Association) EUVL Source Workshop 19 October, 2006 Barcelona, Spain Acknowledgments This work

More information

Pump laser requirements for next generation lasers.

Pump laser requirements for next generation lasers. Dr. Lukas Krainer, CEO lukas.krainer@onefive.com Pump laser requirements for next generation lasers. Outline Company introduction Product portfolio Pump lasers field of use Pump lasers for high power cw

More information

Text for the class, Pump-Probe Technique for Picosecond Time-resolved X-ray Diffraction at Cheiron School

Text for the class, Pump-Probe Technique for Picosecond Time-resolved X-ray Diffraction at Cheiron School BL19LXU Yoshihito Tanaka, Oct. 2013 Text for the class, Pump-Probe Technique for Picosecond Time-resolved X-ray Diffraction at Cheiron School Abstract The pulsed time structure of synchrotron radiation

More information

Time-Resolved measurements by FEL spontaneous emission: A proposal for sub-picosecond pumps & probe structural and spectrometric investigations

Time-Resolved measurements by FEL spontaneous emission: A proposal for sub-picosecond pumps & probe structural and spectrometric investigations Time-Resolved measurements by FEL spontaneous emission: A proposal for sub-picosecond pumps & probe structural and spectrometric investigations V. Rossi Albertini, B. Paci & P. Perfetti Istituto di Struttura

More information

Silicon Avalanche Photodiodes in Dynamic Light Scattering

Silicon Avalanche Photodiodes in Dynamic Light Scattering Silicon Avalanche Photodiodes in Dynamic Light Scattering August 2016 Introduction This application note describes the use of the ID100 single photon counting detector for the measurement of light scattered

More information

Chemical Characterization of Diverse Pharmaceutical Samples by Confocal Raman Microscopy

Chemical Characterization of Diverse Pharmaceutical Samples by Confocal Raman Microscopy Whitepaper Chemical Characterization of Diverse Pharmaceutical Samples by Confocal Raman Microscopy WITec GmbH, Lise-Meitner-Str. 6, 89081 Ulm, Germany, www.witec.de Introduction The development and production

More information

Enhanced optical absorptance of metals using interferometric femtosecond ablation

Enhanced optical absorptance of metals using interferometric femtosecond ablation Enhanced optical absorptance of metals using interferometric femtosecond ablation K. Paivasaari, J. J. J. Kaakkunen, M. Kuittinen and T. Jaaskelainen Department of Physics and Mathematics, University of

More information

PICOSECOND TRANSIENT THERMAL IMAGING USING A CCD BASED THERMOREFLECTANCE SYSTEM

PICOSECOND TRANSIENT THERMAL IMAGING USING A CCD BASED THERMOREFLECTANCE SYSTEM Proceedings of the 14th International Heat Transfer Conference IHTC14 August 8-13, 21, Washington, DC, USA IHTC14- PICOSECOND TRANSIENT THERMAL IMAGING USING A CCD BASED THERMOREFLECTANCE SYSTEM James

More information

TITLE: MASSIVELY PARALLEL ROGUE CELL DETECTION USING SERIAL TIME- ENCODED AMPLIFIED MICROSCOPY OF INERTIALLY ORDERED CELLS IN HIGH THROUGHPUT FLOW

TITLE: MASSIVELY PARALLEL ROGUE CELL DETECTION USING SERIAL TIME- ENCODED AMPLIFIED MICROSCOPY OF INERTIALLY ORDERED CELLS IN HIGH THROUGHPUT FLOW AD Award Number: W81XWH-10-1-0518 TITLE: MASSIVELY PARALLEL ROGUE CELL DETECTION USING SERIAL TIME- ENCODED AMPLIFIED MICROSCOPY OF INERTIALLY ORDERED CELLS IN HIGH THROUGHPUT FLOW PRINCIPAL INVESTIGATOR:

More information

Detectors for Future Light Sources. Gerhard Grübel Deutsches Elektronen Synchrotron (DESY) Notke-Str. 85, Hamburg

Detectors for Future Light Sources. Gerhard Grübel Deutsches Elektronen Synchrotron (DESY) Notke-Str. 85, Hamburg Detectors for Future Light Sources Gerhard Grübel Deutsches Elektronen Synchrotron (DESY) Notke-Str. 85, 22607 Hamburg Overview Radiation from X-Ray Free Electron lasers (XFEL, LCLS) Ultrafast detectors

More information

ADVANCED TEMPORAL CONTROL IN HIGH ENERGY ULTRAFAST LASERS DEDICATED TO MICROMACHINING AND BIOMEDICAL APPLICATIONS

ADVANCED TEMPORAL CONTROL IN HIGH ENERGY ULTRAFAST LASERS DEDICATED TO MICROMACHINING AND BIOMEDICAL APPLICATIONS ADVANCED TEMPORAL CONTROL IN HIGH ENERGY ULTRAFAST LASERS DEDICATED TO MICROMACHINING AND BIOMEDICAL APPLICATIONS SPARK LASERS Pascal Dupriez, CEO and Founder EPHJ, Geneve June 13 th, 2018 Pascal.dupriez@spark-lasers.com

More information

NASA Miniature Inspection LADAR

NASA Miniature Inspection LADAR NASA Miniature Inspection LADAR Bradley Sallee SPEC 1 SPEC s Multi-Dimensional Imaging Programs NASA HD6D NRO HD6D AFRL LGSS Army 3D Change AFRL MST Army Imaging SAL DARPA AIRSS DARPA SUAVTL NASA Inspection

More information

Overview. Etalon-Based FSRS Setup APPLICATION NOTE

Overview. Etalon-Based FSRS Setup APPLICATION NOTE 2016 Princeton Instruments, Inc. All rights reserved. Advanced CCD Cameras and Imaging Spectrographs Facilitate Acquisition of Novel Femtosecond Stimulated Raman Spectroscopy Data To Improve SERS Biosensors

More information

High-Power Femtosecond Lasers

High-Power Femtosecond Lasers High-Power Femtosecond Lasers FEATURES 190 fs ps tunable pulse duration Up to 2 mj pulse energy Up to 20 W average power Single pulse 1 MHz tunable repetition rate Includes pulse picker for pulse-on-demand

More information

Tutorial: Instantaneous Measurement of M 2 Beam Propagation Ratio in Real-Time

Tutorial: Instantaneous Measurement of M 2 Beam Propagation Ratio in Real-Time Tutorial: Instantaneous Measurement of M 2 Beam Propagation Ratio in Real-Time By Allen M. Cary, Jeffrey L. Guttman, Razvan Chirita, Derrick W. Peterman, Photon Inc A new instrument design allows the M

More information

A Comparison of the Iterative Fourier Transform Method and. Evolutionary Algorithms for the Design of Diffractive Optical.

A Comparison of the Iterative Fourier Transform Method and. Evolutionary Algorithms for the Design of Diffractive Optical. A Comparison of the Iterative Fourier Transform Method and Evolutionary Algorithms for the Design of Diffractive Optical Elements Philip Birch, Rupert Young, Maria Farsari, David Budgett, John Richardson,

More information

Spectroscopic equipment. Multispectral Imaging

Spectroscopic equipment. Multispectral Imaging Spectroscopic equipment Multispectral Imaging Basic spectroscopic arrangement Source Sample Analyzer Detector Sun Lamps Lasers LEDs Synchrotron Plants Forests Tissue Cells Flames Chemical compounds etc.

More information

Phys 1020, Day 18: Questions? Cameras, Blmfld Reminders: Next Up: digital cameras finish Optics Note Final Project proposals next week!

Phys 1020, Day 18: Questions? Cameras, Blmfld Reminders: Next Up: digital cameras finish Optics Note Final Project proposals next week! Lights. Action. Phys 1020, Day 18: Questions? Cameras, Blmfld 15.1 Reminders: Next Up: digital cameras finish Optics Note Final Project proposals next week! 1 What have we learned in this section: 1) Lasers

More information

Improved Resolution Optical Time Stretch Imaging Based on High Efficiency In-Fiber Diffraction

Improved Resolution Optical Time Stretch Imaging Based on High Efficiency In-Fiber Diffraction www.nature.com/scientificreports Received: 20 September 2017 Accepted: 19 December 2017 Published: xx xx xxxx OPEN Improved Resolution Optical Time Stretch Imaging Based on High Efficiency In-Fiber Diffraction

More information

Photonic Communications Engineering

Photonic Communications Engineering Photonic Communications Engineering Instructor Alan Kost Email - akost@arizona.edu Office OSC 529 Office Hours Walk In or by Appointment 1 Photonic Communications Class Syllabus Engineering Class is divided

More information

Versatile laser Raman Spectrometer. RMP-500 series

Versatile laser Raman Spectrometer. RMP-500 series Versatile laser Raman Spectrometer RMP-500 series About RMP-500 RMP-500 series is a compact and versatile laser Raman spectrometer consisting of a micro Raman probe connected through fiber optics to the

More information

Performance of serial time-encoded amplified microscope

Performance of serial time-encoded amplified microscope Performance of serial time-encoded amplified microscope Kevin K. Tsia 12* Keisuke Goda 1 Dale Capewell 1 and Bahram Jalali 1 1 UCLA Photonics Laboratory University of California Los Angeles CA 90095 USA

More information

The Shannon Hartley theorem provides a tool to quantify the

The Shannon Hartley theorem provides a tool to quantify the MacmsLitetoprire.AlrigREVIEW ARTICLE PUBLISHED ONLINE: 1 JUNE 217 DOI: 1.138/NPHOTON.217.76 Time stretch and its applications Ata Mahjoubfar 1,2, Dmitry V. Churkin 3,4,5, Stéphane Barland 6, Neil Broderick

More information

PGx01 series. High Peak Power. Available models

PGx01 series. High Peak Power. Available models Picosecond Lasers Nanosecond Lasers Nanosecond Tunable Lasers High Energy Lasers Ultrafast Fiber Lasers Other Ekspla Products PGx1 PGx3 PGx11 PT2 Travelling Wave Optical Parametric Generators (TWOPG) are

More information

Recent Advances in Ultrafast Laser Subtractive and Additive Manufacturing

Recent Advances in Ultrafast Laser Subtractive and Additive Manufacturing Industrial Affiliates Symposium March 16-18, 2017 Recent Advances in Ultrafast Laser Subtractive and Additive Manufacturing Xiaoming Yu Assistant Professor Ultrafast Laser Processing Group CREOL, The College

More information

New approach to jitter reduction of an x-ray streak camera in accumulation mode

New approach to jitter reduction of an x-ray streak camera in accumulation mode New approach to jitter reduction of an x-ray streak camera in accumulation mode J. Liu *a, A. G. MacPhee b, C. Liu a, B. Shan c, Z. Chang c and J. Wang a a Advanced Photon Source, Argonne National Laboratory,

More information

The role of light source in coherence scanning interferometry and optical coherence tomography

The role of light source in coherence scanning interferometry and optical coherence tomography The role of light source in coherence scanning interferometry and optical coherence tomography Dr Rong Su Research Fellow Advanced Manufacturing Research Group Manufacturing Metrology Team Precision manufacturing

More information

OPTICAL COHERENCE TOMOGRAPHY:SIGNAL PROCESSING AND ALGORITHM

OPTICAL COHERENCE TOMOGRAPHY:SIGNAL PROCESSING AND ALGORITHM OPTICAL COHERENCE TOMOGRAPHY:SIGNAL PROCESSING AND ALGORITHM OCT Medical imaging modality with 1-10 µ m resolutions and 1-2 mm penetration depths High-resolution, sub-surface non-invasive or minimally

More information

Optics for nonlinear microscopy

Optics for nonlinear microscopy Optics for nonlinear microscopy Nonlinear microscopy Dispersion management Compact housing In-line input/output apertures High throughput Robust mechanical design Latest generations of Dispersive Mirrors

More information

XUV pulse FLASH

XUV pulse FLASH W (GW) XUV pulse duration @ FLASH 50 85µm with bandpass filter 55 60 Kinetic Energy [ev] 65 70 75 80 85 90 95 100 0.5 1 1.5 2 2.5 3 3.5 4 4.5 5 Delay [ps] 80 60 40 20 0 0 50 100 150 200 250 300 t (fs)

More information

Classification of Hyperspectral Breast Images for Cancer Detection. Sander Parawira December 4, 2009

Classification of Hyperspectral Breast Images for Cancer Detection. Sander Parawira December 4, 2009 1 Introduction Classification of Hyperspectral Breast Images for Cancer Detection Sander Parawira December 4, 2009 parawira@stanford.edu In 2009 approximately one out of eight women has breast cancer.

More information

Vision Based Metal Spectral Analysis using

Vision Based Metal Spectral Analysis using 1/27 Vision Based Metal Spectral Analysis using Eranga Ukwatta Department of Electrical and Computer Engineering The University of Western Ontario May 25, 2009 2/27 Outline 1 Overview of Element Spectroscopy

More information

FLEX 2 NEW. Key points. 3D Confocal Raman, 2 lasers, fiber based, AFM combined

FLEX 2 NEW. Key points. 3D Confocal Raman, 2 lasers, fiber based, AFM combined FLEX 2 3D Confocal Raman, 2 lasers, fiber based, AFM combined NEW Key points Compact size 2 lasers, easily switchable 2 confocal operation modes, easily switchable : High Spatial Resolution 35 nm High

More information

Industrial Fiber Beam Delivery for Ultrafast Lasers

Industrial Fiber Beam Delivery for Ultrafast Lasers Photonic Tools GmbH, 2017 Industrial Fiber Beam Delivery for Ultrafast Lasers System Technology and Industrial Application Bastian Kruschke 15.11.2017 Swissphotonics Workshop Specialty Optical Fibers Motivation

More information

Outline. Nuclear Forensics & Laser-Induced Breakdown Spectroscopy. Interferometry & Shadowgraphy. Conclusion & Future Work. Experimental Setup

Outline. Nuclear Forensics & Laser-Induced Breakdown Spectroscopy. Interferometry & Shadowgraphy. Conclusion & Future Work. Experimental Setup Outline Nuclear Forensics Laser-Induced Breakdown Spectroscopy Interferometry Shadowgraphy Experimental Setup Conclusion Future Work 1 Nuclear forensics The analysis of nuclear materials recovered from

More information

Optical properties and characterization

Optical properties and characterization Optical properties and characterization Name Picture Description Site Responsible 1 Laser Nd:YAG MAPLE (Matrix Assisted Pulsed Laser Evaporation) system for biomaterials and polymeric thin film deposition

More information

High-Accuracy LIBS with Nanosecond and Picosecond Time Resolution Enabled by Ultrasensitive emiccd Technology

High-Accuracy LIBS with Nanosecond and Picosecond Time Resolution Enabled by Ultrasensitive emiccd Technology 2015 Princeton Instruments, Inc. All rights reserved. High-Accuracy LIBS with Nanosecond and Picosecond Time Resolution Enabled by Ultrasensitive emiccd Technology The PI-MAX4:1024EMB emiccd camera seamlessly

More information

Optical Ptychography Imaging

Optical Ptychography Imaging Optical Ptychography Imaging Summer Project Annafee Azad Supervisors: Dr Fucai Zhang Prof Ian Robinson Summer 2014 23 October 2014 Optical Ptychography Imaging P a g e 2 Abstract This report details a

More information

Single Photon Counting Module COUNT blue -Series

Single Photon Counting Module COUNT blue -Series Single Photon Counting Module COUNT blue -Series Description Laser Components COUNT blue series of Single Photon Counting Modules has been developed to offer a unique combination of high quantum efficiency,

More information

Simple Spectrograph. grating. slit. camera lens. collimator. primary

Simple Spectrograph. grating. slit. camera lens. collimator. primary Simple Spectrograph slit grating camera lens collimator primary Notes: 1) For ease of sketching, this shows a transmissive system (refracting telescope, transmission grating). Most telescopes use a reflecting

More information

Single Photon Counting Module

Single Photon Counting Module Description Laser Components COUNT series of s has been developed to offer a unique combination of high quantum efficiency, wide dynamic range and ease of use for photon counting applications. Combining

More information

Sample Introduction Systems SOLID LASER ABLATION

Sample Introduction Systems SOLID LASER ABLATION Sample Introduction Systems SOLID LASER ABLATION Laser ablation Benefits: spatial resolution of < 10 um little to no sample preparation required Drawbacks: transient signal reduced precision/accuracy relative

More information

Near Field Observation of a Refractive Index Grating and a Topographical Grating by an Optically Trapped Gold Particle

Near Field Observation of a Refractive Index Grating and a Topographical Grating by an Optically Trapped Gold Particle Near Field Observation of a Refractive Index Grating and a Topographical Grating by an Optically Trapped Gold Particle Hiroo UKITA and Hirotaka UEMI Ritsumeikan University, Kusatsu-shi, Shiga, 2 Japan

More information

Particle Image Velocimetry for Fluid Dynamics Measurements

Particle Image Velocimetry for Fluid Dynamics Measurements Particle Image Velocimetry for Fluid Dynamics Measurements Lyes KADEM, Ph.D; Eng kadem@encs.concordia.ca Laboratory for Cardiovascular Fluid Dynamics MIE Concordia University Presentation - A bit of history

More information

Text for the class, Pump and probe technique for picosecond time-resolved x-ray diffraction at the Cheiron School

Text for the class, Pump and probe technique for picosecond time-resolved x-ray diffraction at the Cheiron School Yoshihito Tanaka, Kiminori Ito Oct. 3-4, 2011 Text for the class, Pump and probe technique for picosecond time-resolved x-ray diffraction at the Cheiron School 1. Introduction 1-1. Purpose The pulsed nature

More information

Quantifying the Dynamic Ocean Surface Using Underwater Radiometric Measurement

Quantifying the Dynamic Ocean Surface Using Underwater Radiometric Measurement DISTRIBUTION STATEMENT A. Approved for public release; distribution is unlimited. Quantifying the Dynamic Ocean Surface Using Underwater Radiometric Measurement Lian Shen Department of Mechanical Engineering

More information

A Direct Simulation-Based Study of Radiance in a Dynamic Ocean

A Direct Simulation-Based Study of Radiance in a Dynamic Ocean A Direct Simulation-Based Study of Radiance in a Dynamic Ocean Lian Shen Department of Civil Engineering Johns Hopkins University Baltimore, MD 21218 phone: (410) 516-5033 fax: (410) 516-7473 email: LianShen@jhu.edu

More information

Scheme ASADOG for stretching or compressing short optical pulses

Scheme ASADOG for stretching or compressing short optical pulses Scheme ASADOG for stretching or compressing short optical pulses Sergiy Kaim 1, George Venus 1, Vadim Smirnov 2, Boris Ya. Zeldovich 1, Leon B. Glebov 1,2 1 CREOL, The College of Optics and Photonics,

More information

Renishaw invia Raman Microscope (April 2006)

Renishaw invia Raman Microscope (April 2006) Renishaw invia Raman Microscope (April 2006) I. Starting the System 1. The main system unit is ON all the time. 2. Switch on the Leica microscope and light source for reflective bright field (BF) imaging.

More information

Chapter 24. Geometric optics. Assignment No. 11, due April 27th before class: Problems 24.4, 24.11, 24.13, 24.15, 24.24

Chapter 24. Geometric optics. Assignment No. 11, due April 27th before class: Problems 24.4, 24.11, 24.13, 24.15, 24.24 Chapter 24 Geometric optics Assignment No. 11, due April 27th before class: Problems 24.4, 24.11, 24.13, 24.15, 24.24 A Brief History of Light 1000 AD It was proposed that light consisted of tiny particles

More information

Lasers and Femtosecond Lasers

Lasers and Femtosecond Lasers 1/26/2004 Lasers and Femtosecond Lasers As you learned in the lecture, a Ti:sapphire laser can operate either as a tunable, continuous-wave (CW) laser, or a pulsed, self-modelocked, laser. A slight alignment

More information

Delayline Detectors. Imaging Detection of Electrons, Ions & Photons with Picosecond Time Resolution. e - I +

Delayline Detectors. Imaging Detection of Electrons, Ions & Photons with Picosecond Time Resolution. e - I + Delayline Detectors Imaging Detection of Electrons, Ions & Photons with Picosecond Time Resolution e - I + Delayline Readout of MCPs - The Technical Approach - Microchannel-Plate (MCP) detectors provide

More information

TRiCAM APPLICATIONS KEY FEATURES. Time Resolved intensified CAMera. TRiCAM 13001A01 31/10/2013

TRiCAM APPLICATIONS KEY FEATURES. Time Resolved intensified CAMera. TRiCAM 13001A01 31/10/2013 TRiCAM Time Resolved intensified CAMera The TRiCAM is a compact Intensified CCD camera for scientific and industrial applications that require 1) lowlight level imaging, 2) ultra-short exposures through

More information

GE Healthcare. Agile Ultrasound. The Next Revolution in Ultrasound Imaging

GE Healthcare. Agile Ultrasound. The Next Revolution in Ultrasound Imaging Agile Ultrasound The Next Revolution in Ultrasound Imaging Abstract Diagnostic use of ultrasound has greatly expanded over the past couple of decades because it offers many advantages as an imaging modality.

More information

WITec Raman Spectroscopy Solutions

WITec Raman Spectroscopy Solutions Confocal Raman Imaging WITec Raman Spectroscopy Solutions -40-20 0 20 CCD cts 500 1000 1500 2000 2500 3000 3000 relative wavenumbers (cm -1 ) www.witec.de WITec UHTS Ultra-High Throughput Spectrometers

More information

Apex High Performance Spectrometer

Apex High Performance Spectrometer Apex High Performance Spectrometer 1 Elite High Performance Spectrometers Challenge Integrated, high end instruments are required to detect low light levels for challenging Fluorescence and Raman applications

More information

POWERSIGHT LASER DOPPLER AND PHASE DOPPLER MEASUREMENT SYSTEMS

POWERSIGHT LASER DOPPLER AND PHASE DOPPLER MEASUREMENT SYSTEMS POWERSIGHT LASER DOPPLER AND PHASE DOPPLER MEASUREMENT SYSTEMS PROVIDING UNMATCHED FLEXIBILITY, SIMPLICITY, AND PATENTED TECHNOLOGY UNDERSTANDING, ACCELERATED THE POWERSIGHT LDV AND PDPA SYSTEMS AN INNOVATIVE

More information

A COMMON SOFTWARE FRAMEWORK FOR FEL DATA ACQUISITION AND EXPERIMENT MANAGEMENT AT FERMI

A COMMON SOFTWARE FRAMEWORK FOR FEL DATA ACQUISITION AND EXPERIMENT MANAGEMENT AT FERMI A COMMON SOFTWARE FRAMEWORK FOR FEL DATA ACQUISITION AND EXPERIMENT MANAGEMENT AT FERMI R. Borghes, V. Chenda, A. Curri, G. Kourousias, M. Lonza, G. Passos, M. Prica, R. Pugliese 1 FERMI overview FERMI

More information

PH880 Topics in Physics

PH880 Topics in Physics PH880 Topics in Physics Modern Optical Imaging (Fall 2010) KAIST PH880 11/10/2010 Overview of week 11 Monday: Digital Holographic Tomography Optical Coherence Tomography Wednesday: PhotoacousticTomography

More information

Compatible with Windows 8/7/XP, and Linux; Universal programming interfaces for easy custom programming.

Compatible with Windows 8/7/XP, and Linux; Universal programming interfaces for easy custom programming. PI-MAX 4: 1024f The PI-MAX4:1024f from Princeton Instruments is the next generation, fully-integrated scientific intensified CCD camera (ICCD) system featuring a 1k x 1k full-frame CCD fiberoptically coupled

More information

Introduction of the Industry's Broadest Tunable Quantum Cascade Lasers. February Block Engineering 1

Introduction of the Industry's Broadest Tunable Quantum Cascade Lasers. February Block Engineering 1 Introduction of the Industry's Broadest Tunable Quantum Cascade Lasers February 2014 2014 Block Engineering 1 Widely-Tunable QCL Products LaserTune Mini-QCL Smallest widely-tunable QCL source Embedded

More information

specular diffuse reflection.

specular diffuse reflection. Lesson 8 Light and Optics The Nature of Light Properties of Light: Reflection Refraction Interference Diffraction Polarization Dispersion and Prisms Total Internal Reflection Huygens s Principle The Nature

More information

Techniques of Noninvasive Optical Tomographic Imaging

Techniques of Noninvasive Optical Tomographic Imaging Techniques of Noninvasive Optical Tomographic Imaging Joseph Rosen*, David Abookasis and Mark Gokhler Ben-Gurion University of the Negev Department of Electrical and Computer Engineering P. O. Box 653,

More information

Efficient Signal Processing Algorithms for Optical Doppler Tomography Literature Survey

Efficient Signal Processing Algorithms for Optical Doppler Tomography Literature Survey Efficient Signal Processing Algorithms for Optical Doppler Tomography Literature Survey University of Texas at Austin Department of Electrical and Computer Engineering Milos Milosevic Wade Schwartzkopf

More information

PI-MAX 4: 1024 EMB. Applications:

PI-MAX 4: 1024 EMB. Applications: The PI-MAX4: 1024 EMB from Princeton Instruments is the ultimate in ICCD technology. This innovative intensified EMCCD camera (emiccd) features back-illuminated 1024 x 1024 frame transfer EMCCD fiberoptically

More information

ULTRAFAST LASERS: TECHNOLOGIES AND GLOBAL MARKETS

ULTRAFAST LASERS: TECHNOLOGIES AND GLOBAL MARKETS ULTRAFAST LASERS: TECHNOLOGIES AND GLOBAL MARKETS PHO017A February 2015 Sinha G. Project Analyst ISBN: 1-62296-036-X BCC Research 49 Walnut Park, Building 2 Wellesley, MA 02481 USA 866-285-7215 (toll-free

More information

Confocal Raman Imaging with WITec Sensitivity - Resolution - Speed. Always - Provable - Routinely

Confocal Raman Imaging with WITec Sensitivity - Resolution - Speed. Always - Provable - Routinely Confocal Raman Imaging with WITec Sensitivity - Resolution - Speed Always - Provable - Routinely WITec GmbH, Ulm, Germany, info@witec.de, www.witec.de A modular microscope series An Example: FLIM optical

More information

Hyperspectral Microscope based on Imaging Fourier transform Spectrometry. Dr. Li Jianping, Claude. Copyright: Claude.

Hyperspectral Microscope based on Imaging Fourier transform Spectrometry. Dr. Li Jianping, Claude. Copyright: Claude. The Claude Research Group Hyperspectral Microscope based on Imaging Fourier transform Spectrometry Dr. Li Jianping, Claude jp.li@siat.ac.cn June 2017 Outline Spectral Imaging Fourier transform Imaging

More information

L. Pina, A. Fojtik, R. Havlikova, A. Jancarek, S.Palinek, M. Vrbova

L. Pina, A. Fojtik, R. Havlikova, A. Jancarek, S.Palinek, M. Vrbova L. Pina, A. Fojtik, R. Havlikova, A. Jancarek, S.Palinek, M. Vrbova Faculty of Nuclear Sciences, Czech Technical University, Brehova 7, 115 19 Prague, Czech Republic CD EXPERIMENTAL ARRANGEMENT SPECTRAL

More information

Cell-based FLIM Energy-Transfer Measurements Using Alba

Cell-based FLIM Energy-Transfer Measurements Using Alba Cell-based FLIM Energy-Transfer Measurements Using Alba ISS, Inc. Introduction This application note describes the use of Alba - Confocal Spectroscopy and Imaging Workstation for the acquisition and analysis

More information

Advanced materials research using the Real-Time 3D Analytical FIB-SEM 'NX9000'

Advanced materials research using the Real-Time 3D Analytical FIB-SEM 'NX9000' SCIENTIFIC INSTRUMENT NEWS 2017 Vol. 9 SEPTEMBER Technical magazine of Electron Microscope and Analytical Instruments. Technical Explanation Advanced materials research using the Real-Time 3D Analytical

More information

ZEISS Launches New High-resolution 3D X-ray Imaging Solutions for Advanced Semiconductor Packaging Failure Analysis

ZEISS Launches New High-resolution 3D X-ray Imaging Solutions for Advanced Semiconductor Packaging Failure Analysis Press Release ZEISS Launches New High-resolution 3D X-ray Imaging Solutions for Advanced Semiconductor Packaging Failure Analysis New submicron and nanoscale XRM systems and new microct system provide

More information

2D-CMOS Detector ELECTRON DETECTOR WITH HIGH SPEED CMOS. Key Features

2D-CMOS Detector ELECTRON DETECTOR WITH HIGH SPEED CMOS. Key Features ELECTRON DETECTOR WITH HIGH SPEED CMOS CAMERA AND Graphics PROCESSING UNIT Key Features MCP Chevron assembly with fast phosphorous screen High speed CMOS camera Parallel true pulse counting by Graphics

More information

Image Reconstruction in Optical Tomography : Utilizing Large Data Sets

Image Reconstruction in Optical Tomography : Utilizing Large Data Sets Image Reconstruction in Optical Tomography : Utilizing Large Data Sets Vadim A. Markel, Ph.D. Department of Radiology John C. Schotland, M.D., Ph.D. Department of Bioengineering http://whale.seas.upenn.edu

More information

Next-Generation High-Efficiency Network Device Technology

Next-Generation High-Efficiency Network Device Technology NEDO Project on Development of Next-Generation High-Efficiency Network Device Technology - Project Status Towards Energy Saving - April 27, 2010 Tohru Asami The University of Tokyo 1 Outline Introduction

More information

Sample Analysis Design

Sample Analysis Design Sample Analysis Design PART III Spectroscopic interferences Matrix effects Matrix Effects Physical physical effects from dissolved or undissolved solids present in solution Chemical Ionization suppression

More information

(Equation 24.1: Index of refraction) We can make sense of what happens in Figure 24.1

(Equation 24.1: Index of refraction) We can make sense of what happens in Figure 24.1 24-1 Refraction To understand what happens when light passes from one medium to another, we again use a model that involves rays and wave fronts, as we did with reflection. Let s begin by creating a short

More information

Model REEF-SS ASF-200

Model REEF-SS ASF-200 1 Femtosecond Single Shot Autocorrelator Model REEF-SS ASF-200 INSTRUCTION MANUAL 4119 Twilight Ridge, San Diego, CA 92130 USA Tel::858.876.3133 Fax::858.630.2376 2 The Single Shot Autocorrelator (SSA)

More information

Technical Basis for optical experimentation Part #4

Technical Basis for optical experimentation Part #4 AerE 545 class notes #11 Technical Basis for optical experimentation Part #4 Hui Hu Department of Aerospace Engineering, Iowa State University Ames, Iowa 50011, U.S.A Light sensing and recording Lenses

More information

GuideStar II Customer Presentation. February 2012

GuideStar II Customer Presentation. February 2012 GuideStar II Customer Presentation February 2012 Outline Product Overview Description Applications and Features Specifications Technical Details Picomotor Mirror Mounts 8784 Cameras Alignment Layout and

More information

Liquid Crystal Displays

Liquid Crystal Displays Liquid Crystal Displays Irma Alejandra Nicholls College of Optical Sciences University of Arizona, Tucson, Arizona U.S.A. 85721 iramirez@email.arizona.edu Abstract This document is a brief discussion of

More information

COMBINING time-domain computation with imagesensing

COMBINING time-domain computation with imagesensing 1648 IEEE TRANSACTIONS ON ELECTRON DEVICES, VOL. 44, NO. 10, OCTOBER 1997 CCD-Based Range-Finding Sensor Ryohei Miyagawa and Takeo Kanade, Fellow, IEEE Abstract Integration-time-based, time-domain computation

More information

Xuechang Ren a *, Canhui Wang, Yanshuang Li, Shaoxin Shen, Shou Liu

Xuechang Ren a *, Canhui Wang, Yanshuang Li, Shaoxin Shen, Shou Liu Available online at www.sciencedirect.com Physics Procedia 22 (2011) 493 497 2011 International Conference on Physics Science and Technology (ICPST 2011) Optical Tweezers Array System Based on 2D Photonic

More information

CARBON FIBER SURFACE MEASUREMENT USING 3D PROFILOMETRY

CARBON FIBER SURFACE MEASUREMENT USING 3D PROFILOMETRY CARBON FIBER SURFACE MEASUREMENT USING 3D PROFILOMETRY Prepared by Craig Leising 6 Morgan, Ste156, Irvine CA 92618 P: 949.461.9292 F: 949.461.9232 nanovea.com Today's standard for tomorrow's materials.

More information

Product Specifications

Product Specifications Product Specifications The ksa RateRat Pro is a turnkey, real-time, in-situ optical reflectance probe designed for deposition monitoring of semi-absorbent thin films. The RateRat Pro measures deposition

More information

Lecture 05. First Example: A Real Lidar

Lecture 05. First Example: A Real Lidar Lecture 05. First Example: A Real Lidar Brief review of lidar basics K Doppler lidar system architecture K lidar signal estimate from lidar equation Comparison of estimate to reality Summary Review of

More information

Nonlinear optics and two photon microscopy. Table of contents. Sam Whiteley and Seth Parker PHYS 173/BGGN 266 July 13, 2014

Nonlinear optics and two photon microscopy. Table of contents. Sam Whiteley and Seth Parker PHYS 173/BGGN 266 July 13, 2014 Nonlinear optics and two photon microscopy Sam Whiteley and Seth Parker PHYS 173/BGGN 266 July 13, 2014 Table of contents 1. Introduction 2. Optical setup 3. Initial images and troubleshooting 4. Determining

More information