NEAT breadboard system analysis and performance models

Size: px
Start display at page:

Download "NEAT breadboard system analysis and performance models"

Transcription

1 NEAT breadboard system analysis François Hénault, Antoine Crouzier, Fabien Malbet, Pierre Kern, Guillermo Martin, Philippe Feautrier, Eric Staedler, Sylvain Lafrasse, Alain Delboulbé, Jean-Michel Le Duigou, Christophe Cara, Alain Léger a Institut de Planétologie et d Astrophysique de Grenoble, Université Joseph Fourier, CNRS B.P. 53, Grenoble France b Centre National d Etudes Spatiales, 18 Avenue Edouard Belin, Toulouse France c Laboratoire AIM, UMR 7158, CEA-IRFU/CNRS-INSU/Université Paris Diderot, CEA Saclay, Bât 709, Gif-sur-Yvette Cedex, France d Institut d Astrophysique Spatiale (IAS), UMR 8617, Université Paris Sud/CNRS-INSU, Bât , Orsay France Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 1

2 NEAT space instrument Detection of Earth-like extra-solar planets around nearby stars Two free-flying vessels, one for the single-mirror telescope, the other for the focal plane array Relative star positions to be measured within 1 micro-arcsec, corresponding to pixels!! IPAG, CNES, CEA and IAS decided to develop a test bench for demonstrating the feasibility of the extremely ambitious performance Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 2

3 Test bench product tree Designed to simulate the most demanding functions of the space instrument NEAT breadboard Pseudo-Stars Simulator (PSS) Optical Bench Pixels Metrology System (PMS) Detection Unit (DU) QTH Lamp Zerodur Block Laser Source CCD detector Optical Condenser Spherical Mirror Laser Coupler and Splitter Detector Straylight Baffle Neutral Densities Mirror Circular Aperture Phase Modulator Cooling System Liquid Core Fiber Pinholes Mask Optical Switch Polarization Maintaining Fibers Translations and Rotations Stage Optical Enclosure Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 3

4 Test bench - Schematic representation QTH lamp Optical condenser Neutral Densities Liquid optical fiber Pixels metrology system (PMS) ϕ(t) Pinholes mask Diaphragm = 5 mm 2 degs. Spherical mirror Translation & rotation stage CCD plane L = 600 mm Detector straylight baffle Zerodur optical bench NEAT Breadboard (under vacuum) Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 4

5 Test bench General view Inside vacuum enclosure : Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 5

6 Pixels metrology system (PMS) Heart of the instrument, generates set of Young s fringes with temporal phase modulation, sweeping each individual pixel Allows to measure their gains g mn and centroid location (δx mn,δy mn ) 6 different horizontal and vertical baselines thanks to an optical switch and 8 polarizing maintaining fibers Laser HeNe 632 nm Splitter 1 to 2 Thermal probes Shutters Phase modulators Vacuum connector Polarisation maintaining fibres Base1(horizontal) CCD camera Fiber coupler Polarization Optical V- Voltage generator maintaining fibers switch grooves Temperature stabilised box Insulated box Base 2 (vertical) Mirror block Pupil Interference fringes Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 6

7 Analytical performance model - Architecture Metrology radiometric and contrast budgets Pixel dimensions δw mn, δh mn M Metrology photon number N ph Detection noises δi Contrast C Phase noises δφ Metrology and calibration error budget Pixel position δx mn, δy mn Subsystems requirements Pseudo-stars simulator Light source power Pinholes size Optical bench Bench stability Wavefront error Baseline stability Metrology system (PMS) Laser power Laser stability: Intensity, wavelength Phase control accuracy Detection unit (DU) Integration times: Pseudo-stars, metrology Noises (daek, readout ) Crosstalk Pseudo-stars radiometric budget PSF width stability δσ O Pixel Response Function (PRF) width stability δσ m Pixel gain δg mn O Star photon number N ph Detection noises δi Photon noise, RON error budget error δu Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 7

8 Subsystems requirements Metrology radiometric and contrast budgets M Metrology photon number N ph Detection noises δi Contrast C Phase noises δφ Metrology and calibration error budget Type of exposures Pixel dimensions δw mn, δh mn DETECTION UNIT Pixel position δx mn, δy mn Pseudo-stars Metromogy Subsystems requirements Integration time s Single frame frequency Hz Pseudo-stars simulator Pixel gain Single frame time 1.67E E-03 s Light source power Pinholes size Number of frames δg mn CCD width 1.92 mm Optical bench Bench stability Number of pixels along X'-axis 80 Wavefront error Pixel width PSF width 24 Baseline stability stability Quantum efficiency δσ O 0.9 Metrology system (PMS) Full well size Laser power Non linearity 1.00E-03 Laser stability: O Intensity, wavelength Spatial crosstalk 1.00E-02 Pseudo-stars Star photon number N ph Phase control accuracy Digitization radiometric budget Detection noises δi 16 error bits Photon noise, RON budget Detection unit (DU) Dark current ( -10 C) 2853 Integration times: Pseudo-stars, metrology Noises (daek, readout ) Crosstalk micron error δu electrons e - / pixel / s Readout noise (1 khz) e - / pixel Digitization noise factor 4.10E E-06 e - Stray reflections factor (Baffle) Pixel Response Function (PRF) 1.00E-09 width stability δσ m Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 8

9 Metrology error budgets Metrology radiometric and contrast budgets Pixel dimensions δw mn, δh mn M Metrology photon number N ph Detection noises δi Contrast C Phase noises δφ Metrology and calibration error budget Pixel position δx mn, δy mn I V mn mn Subsystems M N requirements Ph gmn BXx' mn + BYy' mn (t) = 1 + Vmn cos 2π + ϕ(t) Pseudo-stars M N simulator λ m L Light source power Pinholes πbxwsize mn πbyh mn C sincard sincard λl λl Optical bench Bench stability Wavefront error Phase and intensity Noises PSF width Baseline stability stability Subsystem Metrology system Name (PMS) Value Unit δσ O Type of noise Pixel gain Laser power Pixel gain δg mn Calibration Errors Laser source Wavelength stability 1.00E-05 δλ/λ Phase noise δφ 1.75E E-07 Laser stability: Fibered system Phase control accuracy 1.00E-05 radians Phase noise δφ 9.21E-16 O 5.28E-05 Intensity, wavelength Fibered system Intensity drift 0.00E+00 Pseudo-stars Intensity Star noise photon δi number 0.00E+00 N ph 0.00E+00 Phase control accuracy Fibered system Intensity noise 2.24E-05 Intensity radiometric budget Detection noise δi noises 1.01E-05 δi error 5.88E-05 Fibered system Straylight (parasitic interferograms) 2.24E-05 Intensity noise Photon δi noise, RON 1.01E-05 budget 5.88E-05 Detection unit (DU) Fibered system Baseline stability micron Phase noise δφ 8.73E E-10 Integration times: Optical bench Bench stability (Z-axis) 0.6 micron Phase noise δφ 1.75E E-08 Pseudo-stars, metrology Detection unit Metrology non linearity 0.00E+00 Intensity noise δi 0.00E E+00 Noises (daek, readout ) Detection unit Shot noise 1.10E+05 photons Intensity noise δi 4.09E E-05 Crosstalk Detection unit Readout noise 2.94 e - / pixel Intensity noise δi 7.77E E-06 Detection unit Digitization noise 6.36E+04 e - Intensity noise δi 2.63E E-05 Detection unit Dark current 2853 e - / pixel / s Intensity noise δi 1.26E E-06 Pixel osition error δu (fraction of pixels) Pixel Response Function (PRF) width stability δσ m RMS Sum 1.51E E-04 Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 9

10 Metrology radiometric and contrast budgets NEAT breadboard system analysis Star position error budget PSF half width (1/e) PRF half width (1/e) Radiometric budget M Metrology photon number N ph Shot noise Detection noises δi Readout noise Metrology and Contrast C Digitization noise calibration Phase noises δφdark current error budget Pseudo-stars characteristics Pixel dimensions 4.39E-05 m δw mn, δh mn 1.20E-05 m 6.54E+04 electrons 1.88E+04 electrons 2.16E+04 electrons 3.04E+04 electrons Pixel position δx mn, δy mn Centroïding Subsystems requirements2 O σ Pixel gain error 1.51E-05 m x' m Im = gm N Ph Exp Erf ( w m/2σ ) 2 m Pixel position error 2.46E-09 Pixel m Pseudo-stars σ simulator gain O σ O Straylight (ghost images) 7.67E-05 Light source power Pinholes M size M Non linearity 7.67E-06 δg Pxel width uncertainty 1 nù mn x' = x' m Im Im PSF width stability 1 nm Optical bench m= 1 m= 1 PRF width stability 1 nm Bench stability Wavefront error PSF width Baseline Star stability centroïd and astrometric stability δσ O Metrology system (PMS) Centroid accuracy error Laser Type power of error Laser stability: (fractional pixels) (micro-arcsec) O Star Intensity, intensity wavelength noise 6.29E-06 Pseudo-stars Star 52 photon number N ph Pixel Phase gain control error accuracy 7.18E-06 radiometric budget Detection 59 noises δi Pixel position error 4.80E Photon noise, RON Detection Straylight unit (ghost (DU) images) 2.95E Integration times: Non linearity 2.95E Pseudo-stars, metrology Pxel Noises width (daek, uncertainty readout ) 8.78E PSF Crosstalk width stability 6.42E Pixel Response PRF width stability 1.81E Function (PRF) width stability RMS positoin sum 6.10E δσ m error budget error δu Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 10

11 Numerical performance model Pixel Response Functions (PRF) (Hyper-Gaussian functions) Metrology Pseudo stars Metrology data: dynamic Young s fringes Pseudo stars data: co-moving stars Dark and flat fields 1 Fringe processing 3 Dark and flat calibration Maps of pixel offsets Pre calibrated pseudo star data Metrology fringes Un-noisy 2 Allan deviations 4 Centroiding Centroid positions versus time Noisy Allan deviations of pixel offsets Standard deviation of distance between centroids 5 Procrustes analysis Un-noisy Pseudo-stars images Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 11 Noisy

12 Comparing models with experimental results Both models in global agreement Unexpected critical error items appearing on the test bench : Parasitic interferograms in laser metrology chain New camera baffle under design, concentrating optics at a later stage Pseudo-stars ghost images of electronic origin Modify electronic circuits or use another CCD Error items not so critical as expected : Pseudo-stars photon noise Metrology laser wavelength stability Zerodur and Invar bench thermal stability Other to be investigated : Laser intensity fluctuations Fringes phase fitting accuracy PRF width instability Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 12

13 Breadboard performance status Performance Required (fractions of pixel) Estimated Pixel position error 5.00E E-04 Star position error 5.00E E-05 Digitization noise 16% Dark current 22% Shot noise 48% Pixel position error Star position error Readout noise 14% Readout noise 2% Shot noise 11% Straylight (parasitic interferograms) 27% Dark current 3% Digitization noise 6% Phase control accuracy 24% Intensity noise 27% PRF width stability 14% Star intensity noise 5% Pixel gain error PSF width 6% stability 5% Pxel width uncertainty 7% Non linearity 2% Straylight (ghost images) 23% Pixel position error 38% Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 13

14 Conclusion The NEAT performance models were very helpful to identify the dominant error sources of the breadboard: Most of are well understood (shot noise, detector noise) Some ones deserving further investigations: parasitic interferograms in metrology beam, pseudo-stars ghost images (electronic crosstalk) In way to be eliminated NEAT space instrument will probably be postponed after year 2020, but its test bench will be pursued for high precision characterization of detectors in situ Future developments: New detector arrays funded by CNES Evolutions of the metrology and astrometric performance models: Detector defocus and tilt stability effects More realistic PSF and PRF shape Influence of opto-mechanical on PSF width stability Ghosts and parasitic interferograms issues Conference Modeling, Systems Engineering, and Project Management for Astronomy VI 14

JOVIAL. Jovian Oscillations through radial Velocimetry ImAging observations at several Longitudes

JOVIAL. Jovian Oscillations through radial Velocimetry ImAging observations at several Longitudes JOVIAL Jovian Oscillations through radial Velocimetry ImAging observations at several Longitudes Instrumental Concept JOVIAL instrument is a Doppler Spectro-Imager It heritates SYMPA principle Spectral

More information

International Conference on Space Optics ICSO 2000 Toulouse Labège, France 5 7 December 2000

International Conference on Space Optics ICSO 2000 Toulouse Labège, France 5 7 December 2000 ICSO 000 5 7 December 000 Edited by George Otrio Spatialized interferometer in integrated optics A. Poupinet, L. Pujol, O. Sosnicki, J. Lizet, et al. ICSO 000, edited by George Otrio, Proc. of SPIE Vol.

More information

Department of Mechanical and Aerospace Engineering, Princeton University Department of Astrophysical Sciences, Princeton University ABSTRACT

Department of Mechanical and Aerospace Engineering, Princeton University Department of Astrophysical Sciences, Princeton University ABSTRACT Phase and Amplitude Control Ability using Spatial Light Modulators and Zero Path Length Difference Michelson Interferometer Michael G. Littman, Michael Carr, Jim Leighton, Ezekiel Burke, David Spergel

More information

BEAM HALO OBSERVATION BY CORONAGRAPH

BEAM HALO OBSERVATION BY CORONAGRAPH BEAM HALO OBSERVATION BY CORONAGRAPH T. Mitsuhashi, KEK, TSUKUBA, Japan Abstract We have developed a coronagraph for the observation of the beam halo surrounding a beam. An opaque disk is set in the beam

More information

RAPID: A Revolutionary Fast Low Noise Detector on Pionier

RAPID: A Revolutionary Fast Low Noise Detector on Pionier : A Revolutionary Fast Low Noise Detector on Pionier Sylvain Guieu ESO / IPAG Jean Baptiste Lebouquin Philippe Feautrier Gérard Zins Éric Stadler Pierre Kern Alain Delboulbé Thibault Moulin Sylvain Rochas

More information

Southern African Large Telescope. Prime Focus Imaging Spectrograph. Instrument Acceptance Testing Plan

Southern African Large Telescope. Prime Focus Imaging Spectrograph. Instrument Acceptance Testing Plan Southern African Large Telescope Prime Focus Imaging Spectrograph Instrument Acceptance Testing Plan Eric B. Burgh University of Wisconsin Document Number: SALT-3160AP0003 Revision 2.2 29 April 2004 1

More information

Design of a digital holographic interferometer for the. ZaP Flow Z-Pinch

Design of a digital holographic interferometer for the. ZaP Flow Z-Pinch Design of a digital holographic interferometer for the M. P. Ross, U. Shumlak, R. P. Golingo, B. A. Nelson, S. D. Knecht, M. C. Hughes, R. J. Oberto University of Washington, Seattle, USA Abstract The

More information

Tenerife, Canary Islands, Spain International Conference on Space Optics 7-10 October 2014 THE LAM SPACE ACTIVE OPTICS FACILITY

Tenerife, Canary Islands, Spain International Conference on Space Optics 7-10 October 2014 THE LAM SPACE ACTIVE OPTICS FACILITY THE LAM SPACE ACTIVE OPTICS FACILITY C. Engel 1, M. Ferrari 1, E. Hugot 1, C. Escolle 1,2, A. Bonnefois 2, M. Bernot 3, T. Bret-Dibat 4, M. Carlavan 3, F. Falzon 3, T. Fusco 2, D. Laubier 4, A. Liotard

More information

arxiv: v2 [astro-ph] 7 Aug 2008

arxiv: v2 [astro-ph] 7 Aug 2008 Fresnel interferometric arrays for space-based imaging: testbed results Denis Serre a, Laurent Koechlin a, Paul Deba a a Laboratoire d Astrophysique de Toulouse-Tarbes - Université de Toulouse - CNRS 14

More information

Adaptive Optics for LIGO

Adaptive Optics for LIGO Adaptive Optics for LIGO Justin Mansell Ginzton Laboratory LIGO-G990022-39-M Motivation Wavefront Sensor Outline Characterization Enhancements Modeling Projections Adaptive Optics Results Effects of Thermal

More information

EE119 Introduction to Optical Engineering Fall 2009 Final Exam. Name:

EE119 Introduction to Optical Engineering Fall 2009 Final Exam. Name: EE119 Introduction to Optical Engineering Fall 2009 Final Exam Name: SID: CLOSED BOOK. THREE 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental

More information

Infra Red Interferometers

Infra Red Interferometers Infra Red Interferometers for performance testing of infra-red materials and optical systems Specialist expertise in testing, analysis, design, development and manufacturing for Optical fabrication, Optical

More information

The NAOS visible wave front sensor

The NAOS visible wave front sensor The NAOS visible wave front sensor Philippe Feautrier a, Pierre Kern a, Reinhold Dorn c, Gérard Rousset b, Patrick Rabou a, Sylvain Laurent a, Jean-Louis Lizon c, Eric Stadler a, Yves Magnard a, Olivier

More information

The Henryk Niewodniczański INSTITUTE OF NUCLEAR PHYSICS Polish Academy of Sciences ul. Radzikowskiego 152, Kraków, Poland.

The Henryk Niewodniczański INSTITUTE OF NUCLEAR PHYSICS Polish Academy of Sciences ul. Radzikowskiego 152, Kraków, Poland. The Henryk Niewodniczański INSTITUTE OF NUCLEAR PHYSICS Polish Academy of Sciences ul. Radzikowskiego 152, 31-342 Kraków, Poland. www.ifj.edu.pl/reports/2003.html Kraków, grudzień 2003 Report No 1931/PH

More information

Eric B. Burgh University of Wisconsin. 1. Scope

Eric B. Burgh University of Wisconsin. 1. Scope Southern African Large Telescope Prime Focus Imaging Spectrograph Optical Integration and Testing Plan Document Number: SALT-3160BP0001 Revision 5.0 2007 July 3 Eric B. Burgh University of Wisconsin 1.

More information

Department of Electrical Engineering and Computer Science, Massachusetts Institute of Technology, 77. Table of Contents 1

Department of Electrical Engineering and Computer Science, Massachusetts Institute of Technology, 77. Table of Contents 1 Efficient single photon detection from 500 nm to 5 μm wavelength: Supporting Information F. Marsili 1, F. Bellei 1, F. Najafi 1, A. E. Dane 1, E. A. Dauler 2, R. J. Molnar 2, K. K. Berggren 1* 1 Department

More information

Non-adaptive Wavefront Control

Non-adaptive Wavefront Control OWL Phase A Review - Garching - 2 nd to 4 th Nov 2005 Non-adaptive Wavefront Control (Presented by L. Noethe) 1 Specific problems in ELTs and OWL Concentrate on problems which are specific for ELTs and,

More information

Optimization of coupling between Adaptive Optics and Single Mode Fibers ---

Optimization of coupling between Adaptive Optics and Single Mode Fibers --- Optimization of coupling between Adaptive Optics and Single Mode Fibers --- Non common path aberrations compensation through dithering K. Saab 1, V. Michau 1, C. Petit 1, N. Vedrenne 1, P. Bério 2, M.

More information

NIRCam optical calibration sources

NIRCam optical calibration sources NIRCam optical calibration sources Stephen F. Somerstein, Glen D. Truong Lockheed Martin Advanced Technology Center, D/ABDS, B/201 3251 Hanover St., Palo Alto, CA 94304-1187 ABSTRACT The Near Infrared

More information

Aberrations and adaptive optics for biomedical microscopes

Aberrations and adaptive optics for biomedical microscopes Aberrations and adaptive optics for biomedical microscopes Martin Booth Department of Engineering Science And Centre for Neural Circuits and Behaviour University of Oxford Outline Rays, wave fronts and

More information

GPI INSTRUMENT PAGES

GPI INSTRUMENT PAGES GPI INSTRUMENT PAGES This document presents a snapshot of the GPI Instrument web pages as of the date of the call for letters of intent. Please consult the GPI web pages themselves for up to the minute

More information

Fratricide effect on ELTs

Fratricide effect on ELTs 1st AO4ELT conference, 04005 (2010) DOI:10.1051/ao4elt/201004005 Owned by the authors, published by EDP Sciences, 2010 Fratricide effect on ELTs DamienGratadour 1,a,EricGendron 1,GerardRousset 1,andFrancoisRigaut

More information

EE119 Introduction to Optical Engineering Spring 2003 Final Exam. Name:

EE119 Introduction to Optical Engineering Spring 2003 Final Exam. Name: EE119 Introduction to Optical Engineering Spring 2003 Final Exam Name: SID: CLOSED BOOK. THREE 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental

More information

The performance of the CHEOPS On-Ground calibration system

The performance of the CHEOPS On-Ground calibration system The performance of the CHEOPS On-Ground calibration system B. Chazelas a*, F. P. Wildi a, M. Sarajlic a, M. Sordet a, A. Deline a a University of Geneva, Astonomy dpt., 51 ch. des Maillettes, CH-1290 Sauverny,

More information

Large-Area Interference Lithography Exposure Tool Development

Large-Area Interference Lithography Exposure Tool Development Large-Area Interference Lithography Exposure Tool Development John Burnett 1, Eric Benck 1 and James Jacob 2 1 Physical Measurements Laboratory, NIST, Gaithersburg, MD, USA 2 Actinix, Scotts Valley, CA

More information

Design of the cryo-optical test of the Planck reflectors

Design of the cryo-optical test of the Planck reflectors Design of the cryo-optical test of the Planck reflectors S. Roose, A. Cucchiaro & D. de Chambure* Centre Spatial de Liège, Avenue du Pré-Aily, B-4031 Angleur-Liège, Belgium *ESTEC, Planck project, Keplerlaan

More information

Fine art of computing nulling interferometer maps

Fine art of computing nulling interferometer maps Fine art of computing nulling François Hénault UMR 6525 CNRS H. FIZEAU UNS, OCA Avenue Nicolas Copernic 06130 GRASSE - FRANCE 1 In the frame of arwin/tpf-i space missions: o nulling maps depend on the

More information

Dynamic Phase-Shifting Electronic Speckle Pattern Interferometer

Dynamic Phase-Shifting Electronic Speckle Pattern Interferometer Dynamic Phase-Shifting Electronic Speckle Pattern Interferometer Michael North Morris, James Millerd, Neal Brock, John Hayes and *Babak Saif 4D Technology Corporation, 3280 E. Hemisphere Loop Suite 146,

More information

The Asteroid Finder Focal Plane

The Asteroid Finder Focal Plane The Asteroid Finder Focal Plane H. Michaelis (1), S. Mottola (1), E. Kührt (1), T. Behnke (1), G. Messina (1), M. Solbrig (1), M. Tschentscher (1), N. Schmitz (1), K. Scheibe (2), J. Schubert (3), M. Hartl

More information

Kepler photometric accuracy with degraded attitude control: Simulation of White Paper Attitude

Kepler photometric accuracy with degraded attitude control: Simulation of White Paper Attitude Kepler photometric accuracy with degraded attitude control: Simulation of White Paper Attitude Hans Kjeldsen, Torben Arentoft and Jørgen Christensen-Dalsgaard KASOC, Stellar Astrophysics Centre, Aarhus

More information

AIAA/USU Small Satellite Conference 2007 Paper No. SSC07-VIII-2

AIAA/USU Small Satellite Conference 2007 Paper No. SSC07-VIII-2 Digital Imaging Space Camera (DISC) Design & Testing Mitch Whiteley Andrew Shumway, Presenter Quinn Young Robert Burt Jim Peterson Jed Hancock James Peterson AIAA/USU Small Satellite Conference 2007 Paper

More information

Use of Computer Generated Holograms for Testing Aspheric Optics

Use of Computer Generated Holograms for Testing Aspheric Optics Use of Computer Generated Holograms for Testing Aspheric Optics James H. Burge and James C. Wyant Optical Sciences Center, University of Arizona, Tucson, AZ 85721 http://www.optics.arizona.edu/jcwyant,

More information

Initial Results from the C-Mod Prototype Polarimeter/Interferometer

Initial Results from the C-Mod Prototype Polarimeter/Interferometer Initial Results from the C-Mod Prototype Polarimeter/Interferometer K. R. Smith, J. Irby, R. Leccacorvi, E. Marmar, R. Murray, R. Vieira October 24-28, 2005 APS-DPP Conference 1 Abstract An FIR interferometer-polarimeter

More information

Photon Diagnostics. FLASH User Workshop 08.

Photon Diagnostics. FLASH User Workshop 08. Photon Diagnostics FLASH User Workshop 08 Kai.Tiedtke@desy.de Outline What kind of diagnostic tools do user need to make efficient use of FLASH? intensity (New GMD) beam position intensity profile on the

More information

OPTINO. SpotOptics VERSATILE WAVEFRONT SENSOR O P T I N O

OPTINO. SpotOptics VERSATILE WAVEFRONT SENSOR O P T I N O Spotptics he software people for optics VERSALE WAVEFR SESR Accurate metrology in single and double pass Lenses, mirrors and laser beams Any focal length and diameter Large dynamic range Adaptable for

More information

SPRAY DROPLET SIZE MEASUREMENT

SPRAY DROPLET SIZE MEASUREMENT SPRAY DROPLET SIZE MEASUREMENT In this study, the PDA was used to characterize diesel and different blends of palm biofuel spray. The PDA is state of the art apparatus that needs no calibration. It is

More information

1.6 Beam Wander vs. Image Jitter

1.6 Beam Wander vs. Image Jitter 8 Chapter 1 1.6 Beam Wander vs. Image Jitter It is common at this point to look at beam wander and image jitter and ask what differentiates them. Consider a cooperative optical communication system that

More information

SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals

SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals Published on SOAR (http://www.ctio.noao.edu/soar) Home > SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals SOAR Integral Field Spectrograph (SIFS): Call for Science Verification

More information

Observational Astronomy

Observational 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

erosita mirror calibration:

erosita mirror calibration: erosita mirror calibration: First measurements and future concept PANTER instrument chamber set-up for XMM mirror calibration: 12 m length, 3.5 m diameter: 8m to focal plane instrumentation now: f = 1.6

More information

CHARA AO Calibration Process

CHARA AO Calibration Process CHARA AO Calibration Process Judit Sturmann CHARA AO Project Overview Phase I. Under way WFS on telescopes used as tip-tilt detector Phase II. Not yet funded WFS and large DM in place of M4 on telescopes

More information

J. C. Wyant Fall, 2012 Optics Optical Testing and Testing Instrumentation

J. C. Wyant Fall, 2012 Optics Optical Testing and Testing Instrumentation J. C. Wyant Fall, 2012 Optics 513 - Optical Testing and Testing Instrumentation Introduction 1. Measurement of Paraxial Properties of Optical Systems 1.1 Thin Lenses 1.1.1 Measurements Based on Image Equation

More information

!!! DELIVERABLE!D60.2!

!!! DELIVERABLE!D60.2! www.solarnet-east.eu This project is supported by the European Commission s FP7 Capacities Programme for the period April 2013 - March 2017 under the Grant Agreement number 312495. DELIVERABLED60.2 Image

More information

Instructions for the Experiment

Instructions for the Experiment Instructions for the Experiment Excitonic States in Atomically Thin Semiconductors 1. Introduction Alongside with electrical measurements, optical measurements are an indispensable tool for the study of

More information

MTF and PSF measurements of the CCD detector for the Euclid visible channel

MTF and PSF measurements of the CCD detector for the Euclid visible channel MTF and PSF measurements of the CCD273-84 detector for the Euclid visible channel I. Swindells* a, R. Wheeler a, S. Darby a, S. Bowring a, D. Burt a, R. Bell a, L. Duvet b, D. Walton c, R. Cole c a e2v

More information

Proposed Adaptive Optics system for Vainu Bappu Telescope

Proposed Adaptive Optics system for Vainu Bappu Telescope Proposed Adaptive Optics system for Vainu Bappu Telescope Essential requirements of an adaptive optics system Adaptive Optics is a real time wave front error measurement and correction system The essential

More information

Difrotec Product & Services. Ultra high accuracy interferometry & custom optical solutions

Difrotec Product & Services. Ultra high accuracy interferometry & custom optical solutions Difrotec Product & Services Ultra high accuracy interferometry & custom optical solutions Content 1. Overview 2. Interferometer D7 3. Benefits 4. Measurements 5. Specifications 6. Applications 7. Cases

More information

FIBER EVO. Miniaturized laser module complete with controller and USB power supply all within an incredibly small package

FIBER EVO. Miniaturized laser module complete with controller and USB power supply all within an incredibly small package Miniaturized laser module complete with controller and USB power supply all within an incredibly small package KEY FEATURES: Incredibly small yet fully featured Output powers up to 75 mw Powered by USB:

More information

High resolution cavity-enhanced absorption spectroscopy with a mode comb.

High resolution cavity-enhanced absorption spectroscopy with a mode comb. CRDS User meeting Cork University, sept-2006 High resolution cavity-enhanced absorption spectroscopy with a mode comb. T. Gherman, S. Kassi, J. C. Vial, N. Sadeghi, D. Romanini Laboratoire de Spectrométrie

More information

A Multiwavelength Interferometer for Geodetic Lengths

A Multiwavelength Interferometer for Geodetic Lengths A Multiwavelength Interferometer for Geodetic Lengths K. Meiners-Hagen, P. Köchert, A. Abou-Zeid, Physikalisch-Technische Bundesanstalt, Braunschweig Abstract: Within the EURAMET joint research project

More information

The New IRAM KID Arrays (NIKA) and NIKA-2

The New IRAM KID Arrays (NIKA) and NIKA-2 The New IRAM KID Arrays (NIKA) and NIKA-2 CONFIRMED for NIKA-2: Institut Néel, IPAG, IRAM, LPSC Grenoble University of Cardiff UK IRAM Granada Spain CEA-Irfu, IAS, IEF Saclay and Orsay France TO BE CONFIRMED:

More information

LISA AIV/T. N. Dinu Jaeger ARTEMIS. [joint work with APC and CNES]

LISA AIV/T. N. Dinu Jaeger ARTEMIS. [joint work with APC and CNES] LISA AIV/T N. Dinu Jaeger ARTEMIS [joint work with APC and CNES] Outline General configuration of LISA payload & MOSA Top level MOSA AIV/T flow description Main French MOSA AIV/T activities Proposal for

More information

Fresnel interferometric Arrays as Imaging interferometers

Fresnel interferometric Arrays as Imaging interferometers Fresnel interferometric Arrays as Imaging interferometers L.Koechlin 1, D.Serre 1, P.Deba 1, D.Massonnet 2 1 Observatoire Midi Pyrénées, Université Paul Sabatier,Toulouse, France 2 Centre National d Etudes

More information

3.0 Alignment Equipment and Diagnostic Tools:

3.0 Alignment Equipment and Diagnostic Tools: 3.0 Alignment Equipment and Diagnostic Tools: Alignment equipment The alignment telescope and its use The laser autostigmatic cube (LACI) interferometer A pin -- and how to find the center of curvature

More information

Physics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: Signature:

Physics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: Signature: Physics 431 Final Exam Examples (3:00-5:00 pm 12/16/2009) TIME ALLOTTED: 120 MINUTES Name: PID: Signature: CLOSED BOOK. TWO 8 1/2 X 11 SHEET OF NOTES (double sided is allowed), AND SCIENTIFIC POCKET CALCULATOR

More information

MUSE Image Slicer: Test results on largest slicer ever manufactured

MUSE Image Slicer: Test results on largest slicer ever manufactured MUSE Image Slicer: Test results on largest slicer ever manufactured Florence Laurent a, Edgard Renault a, Johan Kosmalski a, Louisa Adjali a, Didier Boudon a, Roland Bacon a, Patrick Caillier a, Alban

More information

MODULAR ADAPTIVE OPTICS TESTBED FOR THE NPOI

MODULAR ADAPTIVE OPTICS TESTBED FOR THE NPOI MODULAR ADAPTIVE OPTICS TESTBED FOR THE NPOI Jonathan R. Andrews, Ty Martinez, Christopher C. Wilcox, Sergio R. Restaino Naval Research Laboratory, Remote Sensing Division, Code 7216, 4555 Overlook Ave

More information

AgilOptics mirrors increase coupling efficiency into a 4 µm diameter fiber by 750%.

AgilOptics mirrors increase coupling efficiency into a 4 µm diameter fiber by 750%. Application Note AN004: Fiber Coupling Improvement Introduction AgilOptics mirrors increase coupling efficiency into a 4 µm diameter fiber by 750%. Industrial lasers used for cutting, welding, drilling,

More information

FRAUNHOFER AND FRESNEL DIFFRACTION IN ONE DIMENSION

FRAUNHOFER AND FRESNEL DIFFRACTION IN ONE DIMENSION FRAUNHOFER AND FRESNEL DIFFRACTION IN ONE DIMENSION Revised November 15, 2017 INTRODUCTION The simplest and most commonly described examples of diffraction and interference from two-dimensional apertures

More information

UV/Optical/IR Astronomy Part 2: Spectroscopy

UV/Optical/IR Astronomy Part 2: Spectroscopy UV/Optical/IR Astronomy Part 2: Spectroscopy Introduction We now turn to spectroscopy. Much of what you need to know about this is the same as for imaging I ll concentrate on the differences. Slicing the

More information

INTERFEROMETER VI-direct

INTERFEROMETER VI-direct Universal Interferometers for Quality Control Ideal for Production and Quality Control INTERFEROMETER VI-direct Typical Applications Interferometers are an indispensable measurement tool for optical production

More information

The CHEOPS' instrument On-Ground calibration system

The CHEOPS' instrument On-Ground calibration system The CHEOPS' instrument On-Ground calibration system F. P. Wildi a*, B. Chazelas a, A. Deline a, M. Sordet a, M. Sarajlic b a Observatory of Geneva, 51 ch. des Maillettes, CH-1290 Sauverny, Switzerland

More information

METimage Calibration & Performance Verification. Xavier Gnata ICSO 2016

METimage Calibration & Performance Verification. Xavier Gnata ICSO 2016 METimage Calibration & Performance Verification Xavier Gnata ICSO 2016 METimage factsheet Mission Passive imaging radiometer (multi-spectral) 20 spectral channels (443 13.345nm) Global coverage within

More information

The Simbol-X focal plane

The Simbol-X focal plane Mem. S.A.It. Vol. 79, 32 c SAIt 2008 Memorie della The Simbol-X focal plane P. Laurent 1,4, P. Lechner 2, M. Authier 1, U. Briel 3, C. Cara 1, S. Colonges 4, P. Ferrando 1,4, J. Fontignie 1, E. Kendziorra

More information

Lab Report 3: Speckle Interferometry LIN PEI-YING, BAIG JOVERIA

Lab Report 3: Speckle Interferometry LIN PEI-YING, BAIG JOVERIA Lab Report 3: Speckle Interferometry LIN PEI-YING, BAIG JOVERIA Abstract: Speckle interferometry (SI) has become a complete technique over the past couple of years and is widely used in many branches of

More information

TWO TRANSPARENT OPTICAL SENSORS FOR THE POSITIONING OF DETECTORS USING A REFERENCE LASER BEAM

TWO TRANSPARENT OPTICAL SENSORS FOR THE POSITIONING OF DETECTORS USING A REFERENCE LASER BEAM TWO TRANSPARENT OPTICAL SENSORS FOR THE POSITIONING OF DETECTORS USING A REFERENCE LASER BEAM J.-Ch. Barrière, H. Blumenfeld, M. Bourdinaud, O. Cloué, C. Guyot, F. Molinié, P. Ponsot, J.-C. Saudemont,

More information

Optical Components for Laser Applications. Günter Toesko - Laserseminar BLZ im Dezember

Optical 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 information

High-contrast imaging with E-ELT/HARMONI

High-contrast imaging with E-ELT/HARMONI High-contrast imaging with E-ELT/HARMONI A. Carlotti, C. Vérinaud, J.-L. Beuzit, D. Mouillet - IPAG D. Gratadour - LESIA Spectroscopy with HARMONI - 07/2015 - Oxford University 1 Imaging young giant planets

More information

OPAL Optical Profiling of the Atmospheric Limb

OPAL Optical Profiling of the Atmospheric Limb OPAL Optical Profiling of the Atmospheric Limb Alan Marchant Chad Fish Erik Stromberg Charles Swenson Jim Peterson OPAL STEADE Mission Storm Time Energy & Dynamics Explorers NASA Mission of Opportunity

More information

CCD reductions techniques

CCD reductions techniques CCD reductions techniques Origin of noise Noise: whatever phenomena that increase the uncertainty or error of a signal Origin of noises: 1. Poisson fluctuation in counting photons (shot noise) 2. Pixel-pixel

More information

Sensitive measurement of partial coherence using a pinhole array

Sensitive measurement of partial coherence using a pinhole array 1.3 Sensitive measurement of partial coherence using a pinhole array Paul Petruck 1, Rainer Riesenberg 1, Richard Kowarschik 2 1 Institute of Photonic Technology, Albert-Einstein-Strasse 9, 07747 Jena,

More information

EE119 Introduction to Optical Engineering Spring 2002 Final Exam. Name:

EE119 Introduction to Optical Engineering Spring 2002 Final Exam. Name: EE119 Introduction to Optical Engineering Spring 2002 Final Exam Name: SID: CLOSED BOOK. FOUR 8 1/2 X 11 SHEETS OF NOTES, AND SCIENTIFIC POCKET CALCULATOR PERMITTED. TIME ALLOTTED: 180 MINUTES Fundamental

More information

X-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 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 information

LYOT: LYman Orbiting Telescopes

LYOT: LYman Orbiting Telescopes LYOT: LYman Orbiting Telescopes Jean-Claude Vial (PI) et Frédéric Auchère Institut d Astrophysique Spatiale and The LYOT Team Project: Frédéric Rouesnel, Thierry Appourchaux, Michel Berthé, Bernard Cougrand,

More information

Corner Rafts LSST Camera Workshop SLAC Sept 19, 2008

Corner Rafts LSST Camera Workshop SLAC Sept 19, 2008 Corner Rafts LSST Camera Workshop SLAC Sept 19, 2008 Scot Olivier LLNL 1 LSST Conceptual Design Review 2 Corner Raft Session Agenda 1. System Engineering 1. Tolerance analysis 2. Requirements flow-down

More information

Reference and User Manual May, 2015 revision - 3

Reference and User Manual May, 2015 revision - 3 Reference and User Manual May, 2015 revision - 3 Innovations Foresight 2015 - Powered by Alcor System 1 For any improvement and suggestions, please contact customerservice@innovationsforesight.com Some

More information

Stability of a Fiber-Fed Heterodyne Interferometer

Stability of a Fiber-Fed Heterodyne Interferometer Stability of a Fiber-Fed Heterodyne Interferometer Christoph Weichert, Jens Flügge, Paul Köchert, Rainer Köning, Physikalisch Technische Bundesanstalt, Braunschweig, Germany; Rainer Tutsch, Technische

More information

CaSSIS. Colour and Stereo Surface Imaging System. L. Gambicorti & CaSSIS team

CaSSIS. Colour and Stereo Surface Imaging System. L. Gambicorti & CaSSIS team CaSSIS Colour and Stereo Surface Imaging System & CaSSIS team CaSSIS on Exomars TGO l l Introduction CaSSIS: stereo-colour camera Telescope and Optical configuration Best focus on ground CaSSIS integration

More information

Development of a Low-order Adaptive Optics System at Udaipur Solar Observatory

Development of a Low-order Adaptive Optics System at Udaipur Solar Observatory J. Astrophys. Astr. (2008) 29, 353 357 Development of a Low-order Adaptive Optics System at Udaipur Solar Observatory A. R. Bayanna, B. Kumar, R. E. Louis, P. Venkatakrishnan & S. K. Mathew Udaipur Solar

More information

Image Formation and Capture. Acknowledgment: some figures by B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, and A. Theuwissen

Image Formation and Capture. Acknowledgment: some figures by B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, and A. Theuwissen Image Formation and Capture Acknowledgment: some figures by B. Curless, E. Hecht, W.J. Smith, B.K.P. Horn, and A. Theuwissen Image Formation and Capture Real world Optics Sensor Devices Sources of Error

More information

Calibration of AO Systems

Calibration of AO Systems Calibration of AO Systems Application to NAOS-CONICA and future «Planet Finder» systems T. Fusco, A. Blanc, G. Rousset Workshop Pueo Nu, may 2003 Département d Optique Théorique et Appliquée ONERA, Châtillon

More information

A LATERAL SENSOR FOR THE ALIGNMENT OF TWO FORMATION-FLYING SATELLITES

A LATERAL SENSOR FOR THE ALIGNMENT OF TWO FORMATION-FLYING SATELLITES A LATERAL SENSOR FOR THE ALIGNMENT OF TWO FORMATION-FLYING SATELLITES S. Roose (1), Y. Stockman (1), Z. Sodnik (2) (1) Centre Spatial de Liège, Belgium (2) European Space Agency - ESA/ESTEC slide 1 Outline

More information

Design and test of a high-contrast imaging coronagraph based on two. 50-step transmission filters

Design and test of a high-contrast imaging coronagraph based on two. 50-step transmission filters Design and test of a high-contrast imaging coronagraph based on two 50-step transmission filters Jiangpei Dou *a,b, Deqing Ren a,b,c, Yongtian Zhu a,b, Xi Zhang a,b,d, Xue Wang a,b,d a. National Astronomical

More information

Adaptive Optics lectures

Adaptive Optics lectures Adaptive Optics lectures 2. Adaptive optics Invented in 1953 by H.Babcock Andrei Tokovinin 1 Plan General idea (open/closed loop) Wave-front sensing, its limitations Correctors (DMs) Control (spatial and

More information

The predicted performance of the ACS coronagraph

The predicted performance of the ACS coronagraph Instrument Science Report ACS 2000-04 The predicted performance of the ACS coronagraph John Krist March 30, 2000 ABSTRACT The Aberrated Beam Coronagraph (ABC) on the Advanced Camera for Surveys (ACS) has

More information

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Mechanical Engineering Department. 2.71/2.710 Final Exam. May 21, Duration: 3 hours (9 am-12 noon)

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Mechanical Engineering Department. 2.71/2.710 Final Exam. May 21, Duration: 3 hours (9 am-12 noon) MASSACHUSETTS INSTITUTE OF TECHNOLOGY Mechanical Engineering Department 2.71/2.710 Final Exam May 21, 2013 Duration: 3 hours (9 am-12 noon) CLOSED BOOK Total pages: 5 Name: PLEASE RETURN THIS BOOKLET WITH

More information

Wavefront control for highcontrast

Wavefront control for highcontrast Wavefront control for highcontrast imaging Lisa A. Poyneer In the Spirit of Bernard Lyot: The direct detection of planets and circumstellar disks in the 21st century. Berkeley, CA, June 6, 2007 p Gemini

More information

Pixel-remapping waveguide addition to an internally sensed optical phased array

Pixel-remapping waveguide addition to an internally sensed optical phased array Pixel-remapping waveguide addition to an internally sensed optical phased array Paul G. Sibley 1,, Robert L. Ward 1,, Lyle E. Roberts 1,, Samuel P. Francis 1,, Simon Gross 3, Daniel A. Shaddock 1, 1 Space

More information

Puntino. Shack-Hartmann wavefront sensor for optimizing telescopes. The software people for optics

Puntino. Shack-Hartmann wavefront sensor for optimizing telescopes. The software people for optics Puntino Shack-Hartmann wavefront sensor for optimizing telescopes 1 1. Optimize telescope performance with a powerful set of tools A finely tuned telescope is the key to obtaining deep, high-quality astronomical

More information

ECEN. Spectroscopy. Lab 8. copy. constituents HOMEWORK PR. Figure. 1. Layout of. of the

ECEN. Spectroscopy. Lab 8. copy. constituents HOMEWORK PR. Figure. 1. Layout of. of the ECEN 4606 Lab 8 Spectroscopy SUMMARY: ROBLEM 1: Pedrotti 3 12-10. In this lab, you will design, build and test an optical spectrum analyzer and use it for both absorption and emission spectroscopy. The

More information

ZIMPOL-3: a powerful solar polarimeter

ZIMPOL-3: a powerful solar polarimeter ZIMPOL-3: a powerful solar polarimeter San Diego, SPIE, 1. July 2010 Renzo Ramelli, IRSOL, Locarno, Switzerland and the ZIMPOL team The ZIMPOL-3 team Silvano Balemi, SUPSI Michele Bianda, IRSOL Ivan Defilippis,

More information

Focal Plane and non-linear Curvature Wavefront Sensing for High Contrast Coronagraphic Adaptive Optics Imaging

Focal Plane and non-linear Curvature Wavefront Sensing for High Contrast Coronagraphic Adaptive Optics Imaging Focal Plane and non-linear Curvature Wavefront Sensing for High Contrast Coronagraphic Adaptive Optics Imaging Olivier Guyon Subaru Telescope 640 N. A'ohoku Pl. Hilo, HI 96720 USA Abstract Wavefronts can

More information

Spectral Analysis of the LUND/DMI Earthshine Telescope and Filters

Spectral Analysis of the LUND/DMI Earthshine Telescope and Filters Spectral Analysis of the LUND/DMI Earthshine Telescope and Filters 12 August 2011-08-12 Ahmad Darudi & Rodrigo Badínez A1 1. Spectral Analysis of the telescope and Filters This section reports the characterization

More information

VATT Optical Performance During 98 Oct as Measured with an Interferometric Hartmann Wavefront Sensor

VATT Optical Performance During 98 Oct as Measured with an Interferometric Hartmann Wavefront Sensor VATT Optical Performance During 98 Oct as Measured with an Interferometric Hartmann Wavefront Sensor S. C. West, D. Fisher Multiple Mirror Telescope Observatory M. Nelson Vatican Advanced Technology Telescope

More information

MIRI The Mid-Infrared Instrument for the JWST. ESO, Garching 13 th April 2010 Alistair Glasse (MIRI Instrument Scientist)

MIRI The Mid-Infrared Instrument for the JWST. ESO, Garching 13 th April 2010 Alistair Glasse (MIRI Instrument Scientist) MIRI The Mid-Infrared Instrument for the JWST ESO, Garching 13 th April 2010 Alistair Glasse (MIRI Instrument Scientist) 1 Summary MIRI overview, status and vital statistics. Sensitivity, saturation and

More information

DESIGNING AND IMPLEMENTING AN ADAPTIVE OPTICS SYSTEM FOR THE UH HOKU KE`A OBSERVATORY ABSTRACT

DESIGNING AND IMPLEMENTING AN ADAPTIVE OPTICS SYSTEM FOR THE UH HOKU KE`A OBSERVATORY ABSTRACT DESIGNING AND IMPLEMENTING AN ADAPTIVE OPTICS SYSTEM FOR THE UH HOKU KE`A OBSERVATORY University of Hawai`i at Hilo Alex Hedglen ABSTRACT The presented project is to implement a small adaptive optics system

More information

Sub-nanometer Interferometry Aspheric Mirror Fabrication

Sub-nanometer Interferometry Aspheric Mirror Fabrication UCRL-JC- 134763 PREPRINT Sub-nanometer Interferometry Aspheric Mirror Fabrication for G. E. Sommargren D. W. Phillion E. W. Campbell This paper was prepared for submittal to the 9th International Conference

More information

Fringe Parameter Estimation and Fringe Tracking. Mark Colavita 7/8/2003

Fringe Parameter Estimation and Fringe Tracking. Mark Colavita 7/8/2003 Fringe Parameter Estimation and Fringe Tracking Mark Colavita 7/8/2003 Outline Visibility Fringe parameter estimation via fringe scanning Phase estimation & SNR Visibility estimation & SNR Incoherent and

More information

RADIOMETRIC AND PHOTOMETRIC MEASUREMENTS AT THE LNE-INM/CNAM

RADIOMETRIC AND PHOTOMETRIC MEASUREMENTS AT THE LNE-INM/CNAM RADIOMETRIC AND PHOTOMETRIC MEASUREMENTS AT THE LNE-INM/CNAM Jean Bastie, Laura Patricia Gonzalez Galvan. Institut National de Métrologie Conservatoire National des Arts et Métiers 61 rue du Landy 93210

More information

SONG Stellar Observations Network Group. The prototype

SONG Stellar Observations Network Group. The prototype SONG Stellar Observations Network Group The prototype F. Grundahl1, J. Christensen Dalsgaard1, U. G. Jørgensen2, H. Kjeldsen1,S. Frandsen1 and P. Kjærgaard2 1) Danish AsteroSeismology Centre, University

More information