High Resolution Ocular Surface OCT to Directly Measure Tear Film Thickness in Human Eyes
|
|
- Patricia Owen
- 5 years ago
- Views:
Transcription
1 High Resolution Ocular Surface OCT to Directly Measure Tear Film Thickness in Human Eyes Rahul Yadav, B.Tech., Kyesung Lee, Ph.D., Jannick Rolland, Ph.D., James Zavislan, Ph.D., James Aquavella, M.D. and Geunyoung Yoon, Ph.D. Advanced Physiological Optics Laboratory Institute of Optics, Flaum Eye Institute,, Rochester, NY
2 Financial Disclosure Grant Support: NIH/NEI 5R01EY014999, NYSTAR/CEIS, RPB, Bausch and Lomb Commercial relationship: Rahul Yadav, None Kyesung Lee, None Jannick Rolland, None James Zavislan, Bausch and Lomb, (Research Funding) James Aquavella, Bausch and Lomb, (Research Funding) Geunyoung Yoon, Bausch and Lomb, (Research Funding)
3 Non-invasive imaging of tear film is important in understanding dry eye 3-5 μm NEI Tear Film Functions Smoothens the corneal surface Protects and cleanses the eye Dry Eye Tear dynamics Tear film thickness profile Tear breakup time Retention time of artificial tears
4 Resolution (mm) Challenges for non-invasive tear imaging OCT 1. Commercial Axial Resolution anterior < 1mm segment FD-OCT systems Theoretical Bioptigen Axial Resolution a RTvue Bandwidth 400nm at 800nm Optopol Copernicus HR Center Wavelength = 800nm 2. Dispersion Bandwidth (nm) 3. Imaging Depth > 1.2mm Spectrometer with high spectral resolution 0.15nm spectral resolution 400nm wavelength range 8mm 1.2mm
5 1. Micrometer axial resolution: Broadband laser supercontinuum source Leukos SM20 0.9mm 400nm
6 2. Dispersion: Free space system Collimator Laser Supercontinuum Scanning Mirror Bandpass Filter Beam splitter Spectrometer Concave Mirror Objective Lens Focusing Lens Linear Grating Sample P = 0.85mW Objective Lens Reference Mirror Line scan CCD Cylindrical Lens Concave Mirror
7 3. Imaging depth : Spectrometer for 400nm bandwidth and spectral resolution 0.15nm Input Modified Czerny Turner Spectrometer Concave Mirror Linear Grating 500G/mm Line Scan CCD 8160 Pixels Cylindrical Lens Concave Mirror
8 Δλ = 0.15nm 3. Imaging depth : Spectrometer performance 980nm 890nm 800nm 710nm 620nm Spectral Resolution 980nm nm 620nm nm Imaging Depth > 1.2mm Lateral Imaging Range > 8mm
9 Signal (db) Measured imaging depth and resolution of ocular surface OCT Measured depth sensitivity Depth sensitivity for 0.15nm spectral resolution mm Axial Distance (mm)
10 6mm Imaging a thin nitrocellulose membrane with tear imaging OCT Membrane thickness : 2mm Refractive Index : 550nm Measured thickness : 2.7mm 35mm
11 0.36mm Tear film imaging on soft contact lens surface with ocular surface OCT Average pre-lens tear thickness 23 µm 1.8 µm OCT scan Pre lens tear film Contact lens Post lens tear film Plastic dome 4mm
12 Tear film thickness profile and its temporal variation on soft contact lens surface Tear thickness (mm) Tear thickness (mm) Lateral distance (mm) Time (s)
13 0.36mm Tear film imaging on cadaver porcine eye with ocular surface OCT 4mm Tear layer Epithelium Stroma
14 Conclusions High resolution anterior segment OCT has been demonstrated for tear imaging Prototype OCT system was used to image tear layer over contact lens and porcine eye indicating its feasibility as an useful instrument in dry eye research
What is Wavefront Aberration? Custom Contact Lenses For Vision Improvement Are They Feasible In A Disposable World?
Custom Contact Lenses For Vision Improvement Are They Feasible In A Disposable World? Ian Cox, BOptom, PhD, FAAO Distinguished Research Fellow Bausch & Lomb, Rochester, NY Acknowledgements Center for Visual
More informationDevelopment of a new multi-wavelength confocal surface profilometer for in-situ automatic optical inspection (AOI)
Development of a new multi-wavelength confocal surface profilometer for in-situ automatic optical inspection (AOI) Liang-Chia Chen 1#, Chao-Nan Chen 1 and Yi-Wei Chang 1 1. Institute of Automation Technology,
More informationExam 4. Name: Class: Date: Multiple Choice Identify the choice that best completes the statement or answers the question.
Name: Class: Date: Exam 4 Multiple Choice Identify the choice that best completes the statement or answers the question. 1. Mirages are a result of which physical phenomena a. interference c. reflection
More informationOptical coherence tomography
Optical coherence tomography Peter E. Andersen Optics and Plasma Research Department Risø National Laboratory E-mail peter.andersen@risoe.dk Outline Part I: Introduction to optical coherence tomography
More informationAxsun OCT Swept Laser and System
Axsun OCT Swept Laser and System Seungbum Woo, Applications Engineer Karen Scammell, Global Sales Director Bill Ahern, Director of Marketing, April. Outline 1. Optical Coherence Tomography (OCT) 2. Axsun
More informationsome aspects of Optical Coherence Tomography
some aspects of Optical Coherence Tomography SSOM Lectures, Engelberg 17.3.2009 Ch. Meier 1 / 34 Contents 1. OCT - basic principles (Time Domain Frequency Domain) 2. Performance and limiting factors 3.
More informationLMT F14. Cut in Three Dimensions. The Rowiak Laser Microtome: 3-D Cutting and Imaging
LMT F14 Cut in Three Dimensions The Rowiak Laser Microtome: 3-D Cutting and Imaging The Next Generation of Microtomes LMT F14 - Non-contact laser microtomy The Rowiak laser microtome LMT F14 is a multi-purpose
More informationSpectraPro 2150 Monochromators and Spectrographs
SpectraPro 215 Monochromators and Spectrographs SpectraPro 215 15 mm imaging spectrographs and monochromators from are the industry standard for researchers who demand the highest quality data. Acton monochromators
More informationBetter Imaging with a Schmidt-Czerny-Turner Spectrograph
Better Imaging with a Schmidt-Czerny-Turner Spectrograph Abstract For years, images have been measured using Czerny-Turner (CT) design dispersive spectrographs. Optical aberrations inherent in the CT design
More informationOptical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember
Günter Toesko - Laserseminar BLZ im Dezember 2009 1 Aberrations An optical aberration is a distortion in the image formed by an optical system compared to the original. It can arise for a number of reasons
More informationHR2000+ Spectrometer. User-Configured for Flexibility. now with. Spectrometers
Spectrometers HR2000+ Spectrometer User-Configured for Flexibility HR2000+ One of our most popular items, the HR2000+ Spectrometer features a high-resolution optical bench, a powerful 2-MHz analog-to-digital
More informationLaser and LED retina hazard assessment with an eye simulator. Arie Amitzi and Menachem Margaliot Soreq NRC Yavne 81800, Israel
Laser and LED retina hazard assessment with an eye simulator Arie Amitzi and Menachem Margaliot Soreq NRC Yavne 81800, Israel Laser radiation hazard assessment Laser and other collimated light sources
More informationSupercontinuum based mid-ir imaging
Supercontinuum based mid-ir imaging Nikola Prtljaga workshop, Munich, 30 June 2017 PAGE 1 workshop, Munich, 30 June 2017 Outline 1. Imaging system (Minerva Lite ) wavelength range: 3-5 µm, 2. Scanning
More informationFigure 7 Dynamic range expansion of Shack- Hartmann sensor using a spatial-light modulator
Figure 4 Advantage of having smaller focal spot on CCD with super-fine pixels: Larger focal point compromises the sensitivity, spatial resolution, and accuracy. Figure 1 Typical microlens array for Shack-Hartmann
More informationTemporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism
VI Temporal coherence characteristics of a superluminescent diode system with an optical feedback mechanism Fang-Wen Sheu and Pei-Ling Luo Department of Applied Physics, National Chiayi University, Chiayi
More informationImproved Spectra with a Schmidt-Czerny-Turner Spectrograph
Improved Spectra with a Schmidt-Czerny-Turner Spectrograph Abstract For years spectra have been measured using traditional Czerny-Turner (CT) design dispersive spectrographs. Optical aberrations inherent
More informationContinuum White Light Generation. WhiteLase: High Power Ultrabroadband
Continuum White Light Generation WhiteLase: High Power Ultrabroadband Light Sources Technology Ultrafast Pulses + Fiber Laser + Non-linear PCF = Spectral broadening from 400nm to 2500nm Ultrafast Fiber
More informationCustomized Correction of Wavefront Aberrations in Abnormal Human Eyes by Using a Phase Plate and a Customized Contact Lens
Journal of the Korean Physical Society, Vol. 49, No. 1, July 2006, pp. 121 125 Customized Correction of Wavefront Aberrations in Abnormal Human Eyes by Using a Phase Plate and a Customized Contact Lens
More informationImaging the Subcellular Structure of Human Coronary Atherosclerosis Using 1-µm Resolution
Imaging the Subcellular Structure of Human Coronary Atherosclerosis Using 1-µm Resolution Optical Coherence Tomography (µoct) Linbo Liu, Joseph A. Gardecki, Seemantini K. Nadkarni, Jimmy D. Toussaint,
More informationGlaucoma Advanced, LAbel-free High resolution Automated OCT Diagnostics GALAHAD
Project Overview Glaucoma Advanced, LAbel-free High resolution Automated OCT Diagnostics GALAHAD Jul-2017 Presentation outline Project key facts Motivation Project objectives Project technology Photonic
More informationEnFocus Your Upgrade Path to High Performance Intrasurgical OCT
Your Upgrade Path to High Performance Intrasurgical OCT is FDA 510(k) Cleared > Ultra HD OCT extends your microscope s potential with intrasurgical OCT BRILLIANT IMAGES, SUB-SURFACE KNOWLEDGE is an intrasurgical
More informationThe Aberration Structure of the Keratoconic Eye
The Aberration Structure of the Keratoconic Eye Geunyoung Yoon, Ph.D. Department of Ophthalmology Center for Visual Science Institute of Optics Department of Biomedical Engineering University of Rochester
More informationMeasurement of Surface Profile and Layer Cross-section with Wide Field of View and High Precision
Hitachi Review Vol. 65 (2016), No. 7 243 Featured Articles Measurement of Surface Profile and Layer Cross-section with Wide Field of View and High Precision VS1000 Series Coherence Scanning Interferometer
More informationCharacteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy
Characteristics of point-focus Simultaneous Spatial and temporal Focusing (SSTF) as a two-photon excited fluorescence microscopy Qiyuan Song (M2) and Aoi Nakamura (B4) Abstracts: We theoretically and experimentally
More informationGuide to SPEX Optical Spectrometer
Guide to SPEX Optical Spectrometer GENERAL DESCRIPTION A spectrometer is a device for analyzing an input light beam into its constituent wavelengths. The SPEX model 1704 spectrometer covers a range from
More informationOptical Characterization and Defect Inspection for 3D Stacked IC Technology
Minapad 2014, May 21 22th, Grenoble; France Optical Characterization and Defect Inspection for 3D Stacked IC Technology J.Ph.Piel, G.Fresquet, S.Perrot, Y.Randle, D.Lebellego, S.Petitgrand, G.Ribette FOGALE
More informationREAL TIME THICKNESS MEASUREMENT OF A MOVING WIRE
REAL TIME THICKNESS MEASUREMENT OF A MOVING WIRE Bini Babu 1, Dr. Ashok Kumar T 2 1 Optoelectronics and communication systems, 2 Associate Professor Model Engineering college, Thrikkakara, Ernakulam, (India)
More informationThe Importance of Wavelengths on Optical Designs
1 The Importance of Wavelengths on Optical Designs Bad Kreuznach, Oct. 2017 2 Introduction A lens typically needs to be corrected for many different parameters as e.g. distortion, astigmatism, spherical
More informationSinusoidal wavelength-scanning common-path interferometer with a beam-scanning system for measurement of film thickness variations
Sinusoidal wavelength-scanning common-path interferometer with a beam-scanning system for measurement of film thickness variations Osami Sasaki, Takafumi Morimatsu, Samuel Choi, and Takamasa Suzuki Faculty
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science
Student Name Date MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science 6.161 Modern Optics Project Laboratory Laboratory Exercise No. 6 Fall 2010 Solid-State
More informationLaser Sources for Frequency-Domain Optical Coherence Tomography FD-OCT
Laser Sources for Frequency-Domain Optical Coherence Tomography FD-OCT Photonic Sensing Workshop SWISSLaser.Net Biel, 17. 9. 2009 Ch. Meier 1/ 20 SWISSLASER.NET Ch. Meier 17.09.09 Content 1. duction 2.
More informationUpper and Lower Tear Menisci on Contact Lenses METHODS
Upper and Lower Tear Menisci on Contact Lenses Jianhua Wang, 1,2 Ian Cox, 3 and William T. Reindel 3 PURPOSE. The purpose of this study was to measure upper and lower tear menisci on contact lenses using
More informationTalbot bands in the theory and practice of optical coherence tomography
Talbot bands in the theory and practice of optical coherence tomography A. Gh. Podoleanu Applied Optics Group, School of Physical Sciences, University of Kent, CT2 7NH, Canterbury, UK Presentation is based
More informationNanoimprint lithography with a focused laser beam for the fabrication of micro-/nano-hybrid patterns
Supplementary Material (ESI) for Lab on a Chip This journal is The Royal Society of Chemistry 20XX Nanoimprint lithography with a focused laser beam for the fabrication of micro-/nano-hybrid patterns Hyungjun
More informationRobert Magnusson, Ph.D.
Robert Magnusson, Ph.D. Texas Instruments Distinguished University Chair in Nanoelectronics Director of the Nanophotonics Device Group Co-founder and Chief Technical Officer of Resonant Sensors Incorporated
More informationData sheet for TDS 10XX system THz Time Domain Spectrometer TDS 10XX
THz Time Domain Spectrometer TDS 10XX TDS10XX 16/02/2018 www.batop.de Page 1 of 11 Table of contents 0. The TDS10XX family... 3 1. Basic TDS system... 3 1.1 Option SHR - Sample Holder Reflection... 4 1.2
More informationExamination Optoelectronic Communication Technology. April 11, Name: Student ID number: OCT1 1: OCT 2: OCT 3: OCT 4: Total: Grade:
Examination Optoelectronic Communication Technology April, 26 Name: Student ID number: OCT : OCT 2: OCT 3: OCT 4: Total: Grade: Declaration of Consent I hereby agree to have my exam results published on
More informationOPTICAL COHERENCE TOMOGRAPHY: OCT supports industrial nondestructive depth analysis
OPTICAL COHERENCE TOMOGRAPHY: OCT supports industrial nondestructive depth analysis PATRICK MERKEN, RAF VANDERSMISSEN, and GUNAY YURTSEVER Abstract Optical coherence tomography (OCT) has evolved to a standard
More informationContents. Acknowledgments. iii. 1 Structure and Function 1. 2 Optics of the Human Eye 3. 3 Visual Disorders and Major Eye Diseases 5
i Contents Acknowledgments iii 1 Structure and Function 1 2 Optics of the Human Eye 3 3 Visual Disorders and Major Eye Diseases 5 4 Introduction to Ophthalmic Diagnosis and Imaging 7 5 Determination of
More information06SurfaceQuality.nb Optics James C. Wyant (2012) 1
06SurfaceQuality.nb Optics 513 - James C. Wyant (2012) 1 Surface Quality SQ-1 a) How is surface profile data obtained using the FECO interferometer? Your explanation should include diagrams with the appropriate
More informationQE65000 Spectrometer. Scientific-Grade Spectroscopy in a Small Footprint. now with. Spectrometers
QE65000 Spectrometer Scientific-Grade Spectroscopy in a Small Footprint QE65000 The QE65000 Spectrometer is the most sensitive spectrometer we ve developed. Its Hamamatsu FFT-CCD detector provides 90%
More informationBragg and fiber gratings. Mikko Saarinen
Bragg and fiber gratings Mikko Saarinen 27.10.2009 Bragg grating - Bragg gratings are periodic perturbations in the propagating medium, usually periodic variation of the refractive index - like diffraction
More informationUniversity of Lübeck, Medical Laser Center Lübeck GmbH Optical Coherence Tomography
University of Lübeck, Medical Laser Center Lübeck GmbH Optical Coherence Tomography 3. The Art of OCT Dr. Gereon Hüttmann / 2009 System perspective (links clickable) Light sources Superluminescent diodes
More informationGRENOUILLE.
GRENOUILLE Measuring ultrashort laser pulses the shortest events ever created has always been a challenge. For many years, it was possible to create ultrashort pulses, but not to measure them. Techniques
More informationLow Coherence Interferometry for the Inline Measurement of Translucent Multilayer Structures
Low Coherence Interferometry for the Inline Measurement of Translucent Multilayer Structures S. Hölters, C. Farkas, R. Fleige, A. Lenenbach, R. Noll, Aachen Abstract In a joint national project with industrial
More informationDiffractive Axicon application note
Diffractive Axicon application note. Introduction 2. General definition 3. General specifications of Diffractive Axicons 4. Typical applications 5. Advantages of the Diffractive Axicon 6. Principle of
More informationGSM OPTICAL MONITORING FOR HIGH PRECISION THIN FILM DEPOSITION
OPTICAL MONITORING FOR HIGH PRECISION THIN FILM DEPOSITION OPTICAL MONITORING TECHNOLOGIES ENABLING OUR NEW WORLD! - ACHIEVING MORE DEMANDING THIN FILM SPECIFICATIONS - DRIVING DOWN UNIT COSTS THE GSM1101
More informationFourier Domain (Spectral) OCT OCT: HISTORY. Could OCT be a Game Maker OCT in Optometric Practice: A THE TECHNOLOGY BEHIND OCT
Could OCT be a Game Maker OCT in Optometric Practice: A Hands On Guide Murray Fingeret, OD Nick Rumney, MSCOptom Fourier Domain (Spectral) OCT New imaging method greatly improves resolution and speed of
More informationSinusoidal wavelength-scanning interferometer using an acousto-optic tunable filter for measurement of thickness and surface profile of a thin film
Sinusoidal wavelength-scanning interferometer using an acousto-optic tunable filter for measurement of thickness and surface profile of a thin film Hisashi Akiyama 1, Osami Sasaki 2, and Takamasa Suzuki
More informationMiniature collimator for POF fiber: large aperture Model 011-TU2
Example testing Report for: M011-TU2 Miniature collimator for POF fiber: large aperture Model 011-TU2 Testing report Move along this direction to adjust lens Model 011_TU2 with glass lens Part Number:
More informationA TUTORIAL By J.M. Lerner and A. Thevenon TABLE OF CONTENTS. Section 1:DIFFRACTION GRATINGS RULED & HOLOGRAPHIC
A TUTORIAL By J.M. Lerner and A. Thevenon TABLE OF CONTENTS Section 1:DIFFRACTION GRATINGS RULED & HOLOGRAPHIC 1.1 Basic Equations 1.2 Angular Dispersion 1.3 Linear Dispersion 1.4 Wavelength and Order
More informationSupplementary Materials
Supplementary Materials In the supplementary materials of this paper we discuss some practical consideration for alignment of optical components to help unexperienced users to achieve a high performance
More informationDesign and Analysis of Resonant Leaky-mode Broadband Reflectors
846 PIERS Proceedings, Cambridge, USA, July 6, 8 Design and Analysis of Resonant Leaky-mode Broadband Reflectors M. Shokooh-Saremi and R. Magnusson Department of Electrical and Computer Engineering, University
More informationBurton's Microbiology for the Health Sciences
Burton's Microbiology for the Health Sciences Chapter 2. Viewing the Microbial World Chapter 2 Outline Introduction Using the metric system to express the sizes of microbes Microscopes Simple microscopes
More informationDIMENSIONAL MEASUREMENT OF MICRO LENS ARRAY WITH 3D PROFILOMETRY
DIMENSIONAL MEASUREMENT OF MICRO LENS ARRAY WITH 3D PROFILOMETRY Prepared by Benjamin Mell 6 Morgan, Ste156, Irvine CA 92618 P: 949.461.9292 F: 949.461.9232 nanovea.com Today's standard for tomorrow's
More informationA High-Concentration Programmable Solar Simulator for Testing Multi-Junction Concentrator Photovoltaics
A High-Concentration Programmable Solar Simulator for Testing ulti-junction Concentrator Photovoltaics Tasshi Dennis 1, Brent Fisher 2, att eitl 2, and John Wilson 2 1 National Institute of Standards and
More informationFiber Optics. Laboratory exercise
Fiber Optics V 1/27/2012 Laboratory exercise The purpose of the present laboratory exercise is to get practical experience in handling optical fiber. In particular we learn how to cleave the fiber and
More informationPREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES
Page 1 of 30 LIGHTMACHINERY TEST REPORT LQT 30.11-1 TITLE: HMI Michelson Interferometer Test Report Serial Number 1 - Wideband FSR INSTRUCTION OWNER HMI Project Manager PREPARED BY: I. Miller DATE: 2004
More information7 CHAPTER 7: REFRACTIVE INDEX MEASUREMENTS WITH COMMON PATH PHASE SENSITIVE FDOCT SETUP
7 CHAPTER 7: REFRACTIVE INDEX MEASUREMENTS WITH COMMON PATH PHASE SENSITIVE FDOCT SETUP Abstract: In this chapter we describe the use of a common path phase sensitive FDOCT set up. The phase measurements
More informationASE Suppression in a Diode-Pumped Nd:YLF Regenerative Amplifier Using a Volume Bragg Grating
ASE Suppression in a Diode-Pumped Nd:YLF Regenerative Amplifier Using a Volume Bragg Grating Spectral density (db) 0 10 20 30 40 Mirror VBG 1053.0 1053.3 1053.6 Wavelength (nm) Frontiers in Optics 2007/Laser
More informationMoving from biomedical to industrial applications: OCT Enables Hi-Res ND Depth Analysis
Moving from biomedical to industrial applications: OCT Enables Hi-Res ND Depth Analysis Patrick Merken a,c, Hervé Copin a, Gunay Yurtsever b, Bob Grietens a a Xenics NV, Leuven, Belgium b UGENT, Ghent,
More informationNoise Analysis of AHR Spectrometer Author: Andrew Xiang
1. Introduction Noise Analysis of AHR Spectrometer Author: Andrew Xiang The noise from Spectrometer can be very confusing. We will categorize different noise and analyze them in this document from spectrometer
More informationPREPARED BY: I. Miller DATE: 2004 May 23 CO-OWNERS REVISED DATE OF ISSUE/CHANGED PAGES
Page 1 of 30 LIGHTMACHINERY TEST REPORT LQT 30.11-2 TITLE: HMI Michelson Interferometer Test Report Serial Number 2 - Narrowband FSR INSTRUCTION OWNER HMI Project Manager PREPARED BY: I. Miller DATE: 2004
More informationTransferring wavefront measurements to ablation profiles. Michael Mrochen PhD Swiss Federal Institut of Technology, Zurich IROC Zurich
Transferring wavefront measurements to ablation profiles Michael Mrochen PhD Swiss Federal Institut of Technology, Zurich IROC Zurich corneal ablation Calculation laser spot positions Centration Calculation
More informationA novel tunable diode laser using volume holographic gratings
A novel tunable diode laser using volume holographic gratings Christophe Moser *, Lawrence Ho and Frank Havermeyer Ondax, Inc. 85 E. Duarte Road, Monrovia, CA 9116, USA ABSTRACT We have developed a self-aligned
More informationConcepts for High Power Laser Diode Systems
Concepts for High Power Laser Diode Systems 1. Introduction High power laser diode systems is a new development within the field of laser diode systems. Pioneer of such laser systems was SDL, Inc. which
More informationALISEO: an Imaging Interferometer for Earth Observation
ALISEO: an Imaging Interferometer for Earth Observation A. Barducci, F. Castagnoli, G. Castellini, D. Guzzi, C. Lastri, P. Marcoionni, I. Pippi CNR IFAC Sesto Fiorentino, ITALY ASSFTS14 Firenze - May 6-8,
More informationX-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope
X-ray generation by femtosecond laser pulses and its application to soft X-ray imaging microscope Kenichi Ikeda 1, Hideyuki Kotaki 1 ' 2 and Kazuhisa Nakajima 1 ' 2 ' 3 1 Graduate University for Advanced
More informationIntegrated into Nanowire Waveguides
Supporting Information Widely Tunable Distributed Bragg Reflectors Integrated into Nanowire Waveguides Anthony Fu, 1,3 Hanwei Gao, 1,3,4 Petar Petrov, 1, Peidong Yang 1,2,3* 1 Department of Chemistry,
More informationThe Optics of Spectroscopy A Tutorial. By J.M. Lerner and A. Thevenon
The Optics of Spectroscopy A Tutorial By J.M. Lerner and A. Thevenon 1 The Optics of Spectroscopy - A TUTORIAL By J.M. Lerner and A. Thevenon Table of Contents Section 1: DIFFRACTION GRATINGS RULED & HOLOGRAPHIC
More informationTunable KiloArc. Tunable Broadband Light Source.
Optical Building Blocks Corporation Tunable KiloArc Tunable Broadband Light Source www.obb1.com Tunable KiloArc Need a CW laser that is tunable from 250 to 1,100 nm? yes Need it to deliver Hundreds of
More informationSupplementary Figure 1. GO thin film thickness characterization. The thickness of the prepared GO thin
Supplementary Figure 1. GO thin film thickness characterization. The thickness of the prepared GO thin film is characterized by using an optical profiler (Bruker ContourGT InMotion). Inset: 3D optical
More informationUltralight Weight Optical Systems using Nano-Layered Synthesized Materials
Ultralight Weight Optical Systems using Nano-Layered Synthesized Materials Natalie Clark, PhD NASA Langley Research Center and James Breckinridge University of Arizona, College of Optical Sciences Overview
More informationConstruction Manual of Merlin spectrometer
Construction Manual of Merlin spectrometer The first generation of our Merlin Spectrometer is based on the ramanpi Spectrometer. The Project was developed open source with a detailed construction documentation.
More informationChapter 17: Wave Optics. What is Light? The Models of Light 1/11/13
Chapter 17: Wave Optics Key Terms Wave model Ray model Diffraction Refraction Fringe spacing Diffraction grating Thin-film interference What is Light? Light is the chameleon of the physical world. Under
More informationAngela Piegari ENEA, Optical Coatings Laboratory, Roma, Italy
Optical Filters for Space Instrumentation Angela Piegari ENEA, Optical Coatings Laboratory, Roma, Italy Trieste, 18 February 2015 Optical coatings for Space Instrumentation Spectrometers, imagers, interferometers,
More informationMaya2000 Pro Spectrometer
now with triggering! Maya2000 Pro Our Maya2000 Pro Spectrometer offers you the perfect solution for applications that demand low light-level, UV-sensitive operation. This back-thinned, 2D FFT-CCD, uncooled
More informationBeam Shaping and Simultaneous Exposure by Diffractive Optical Element in Laser Plastic Welding
Beam Shaping and Simultaneous Exposure by Diffractive Optical Element in Laser Plastic Welding AKL`12 9th May 2012 Dr. Daniel Vogler Page 1 Motivation: Quality and flexibility diffractive spot shaping
More informationOptical Design for OCT
12 Optical Design for OCT Z. Hu and A.M. Rollins This chapter aims to provide insights and tools to design high-quality optical subsystems for OCT. First, we discuss the various optical subsystems common
More informationBeam quality of a new-type MOPO laser system for VUV laser lithography
Beam quality of a new-type MOPO laser system for VUV laser lithography Osamu Wakabayashi a, Tatsuya Ariga a, Takahito Kumazaki a, Koutarou Sasano a, Takayuki Watanabe a, Takayuki Yabu a, Tsukasa Hori a,
More information60 MHz A-line rate ultra-high speed Fourier-domain optical coherence tomography
60 MHz Aline rate ultrahigh speed Fourierdomain optical coherence tomography K. Ohbayashi a,b), D. Choi b), H. HiroOka b), H. Furukawa b), R. Yoshimura b), M. Nakanishi c), and K. Shimizu c) a Graduate
More informationAdvances in laboratory modeling of wave propagation
Advances in laboratory modeling of wave propagation Physical Acoustics Lab Department of Geosciences Boise State University October 19, 2010 Outline Ultrasonic laboratory modeling Bridge between full-size
More informationSimultaneous measurement of two different-color ultrashort pulses on a single shot
Wong et al. Vol. 29, No. 8 / August 2012 / J. Opt. Soc. Am. B 1889 Simultaneous measurement of two different-color ultrashort pulses on a single shot Tsz Chun Wong,* Justin Ratner, and Rick Trebino School
More informationGabor fusion technique in a Talbot bands optical coherence tomography system
Gabor fusion technique in a Talbot bands optical coherence tomography system Petr Bouchal, Adrian Bradu, and Adrian Gh. Podoleanu Applied Optics Group, School of Physical Sciences, University of Kent,
More informationOptical signal processing for fiber Bragg grating based wear sensors
University of Wollongong Research Online Faculty of Informatics - Papers (Archive) Faculty of Engineering and Information Sciences 2005 Optical signal processing for fiber Bragg grating based wear sensors
More informationDirectly Chirped Laser Source for Chirped Pulse Amplification
Directly Chirped Laser Source for Chirped Pulse Amplification Input pulse (single frequency) AWG RF amp Output pulse (chirped) Phase modulator Normalized spectral intensity (db) 64 65 66 67 68 69 1052.4
More informationApplications of Steady-state Multichannel Spectroscopy in the Visible and NIR Spectral Region
Feature Article JY Division I nformation Optical Spectroscopy Applications of Steady-state Multichannel Spectroscopy in the Visible and NIR Spectral Region Raymond Pini, Salvatore Atzeni Abstract Multichannel
More informationImproving the Collection Efficiency of Raman Scattering
PERFORMANCE Unparalleled signal-to-noise ratio with diffraction-limited spectral and imaging resolution Deep-cooled CCD with excelon sensor technology Aberration-free optical design for uniform high resolution
More informationSpectroscopy of Ruby Fluorescence Physics Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 1/12/2018
1 Spectroscopy of Ruby Fluorescence Physics 3600 - Advanced Physics Lab - Summer 2018 Don Heiman, Northeastern University, 1/12/2018 I. INTRODUCTION The laser was invented in May 1960 by Theodor Maiman.
More informationAIR-COUPLED PHOTOCONDUCTIVE ANTENNAS
AIR-COUPLED PHOTOCONDUCTIVE ANTENNAS Report: Air-Coupled Photoconductive Antennas In this paper, we present air-coupled terahertz photoconductive antenna (THz-PCAs) transmitters and receivers made on high-resistive
More informationGrating-waveguide structures and their applications in high-power laser systems
Grating-waveguide structures and their applications in high-power laser systems Marwan Abdou Ahmed*, Martin Rumpel, Tom Dietrich, Stefan Piehler, Benjamin Dannecker, Michael Eckerle, and Thomas Graf Institut
More informationCost-effective optical coherence tomography spectrometer based on a tilted fiber Bragg grating
Cost-effective optical coherence tomography spectrometer based on a tilted fiber Bragg grating Stefan Remund 1a, Anke Bossen a, Xianfeng Chen b, Ling Wang c,d,e, Adedotun Adebayo f, Lin Zhang f, Boris
More informationThe equipment used share any common features regardless of the! being measured. Electronic detection was not always available.
The equipment used share any common features regardless of the! being measured. Each will have a light source sample cell! selector We ll now look at various equipment types. Electronic detection was not
More informationExercise 8: Interference and diffraction
Physics 223 Name: Exercise 8: Interference and diffraction 1. In a two-slit Young s interference experiment, the aperture (the mask with the two slits) to screen distance is 2.0 m, and a red light of wavelength
More informationOCT. Optical Coherence Tomography
OCT Optical Coherence Tomography Optical Coherence Tomography (OCT) is a non-invasive, non-destructive imaging technique that enables high-resolution, cross-sectional imaging of a wide range of highly
More informationSection 1: SPECTRAL PRODUCTS
Section 1: Optical Non-dispersive Wavelength Selection Filter Based Filter Filter Fundamentals Filter at an Incidence Angle Filters and Environmental Conditions Dispersive Instruments Grating and Polychromators
More informationBiophysical Basis of Optical Radiation Exposure Limits. Bruce E. Stuck
Biophysical Basis of Optical Radiation Exposure Limits Bruce E. Stuck ICNIRP Member bstuck@satx.rr.com ICNIRP 8 th International Radiation Workshop Cape Town International Conference Center Cape Town,
More informationDESIGN OF COMPACT PULSED 4 MIRROR LASER WIRE SYSTEM FOR QUICK MEASUREMENT OF ELECTRON BEAM PROFILE
1 DESIGN OF COMPACT PULSED 4 MIRROR LASER WIRE SYSTEM FOR QUICK MEASUREMENT OF ELECTRON BEAM PROFILE PRESENTED BY- ARPIT RAWANKAR THE GRADUATE UNIVERSITY FOR ADVANCED STUDIES, HAYAMA 2 INDEX 1. Concept
More information(51) Int Cl.: G01B 9/02 ( ) G01B 11/24 ( ) G01N 21/47 ( )
(19) (12) EUROPEAN PATENT APPLICATION (11) EP 1 939 581 A1 (43) Date of publication: 02.07.2008 Bulletin 2008/27 (21) Application number: 07405346.3 (51) Int Cl.: G01B 9/02 (2006.01) G01B 11/24 (2006.01)
More informationObservational Astronomy
Observational Astronomy Instruments The telescope- instruments combination forms a tightly coupled system: Telescope = collecting photons and forming an image Instruments = registering and analyzing the
More information