Cophasing activities at Onera

Slides:



Advertisements
Similar presentations
Gravitational Wave Astronomy Dr. Giles Hammond Institute for Gravitational Research SUPA, University of Glasgow Universität Jena, August 2010.
Advertisements

For the Collaboration GWDAW 2005 Status of inspiral search in C6 and C7 Virgo data Frédérique MARION.
Cascina, January 25th, Coupling of the IMC length noise into the recombined ITF output Raffaele Flaminio EGO and CNRS/IN2P3 Summary - Recombined.
Optics in Astronomy - Interferometry - Oskar von der Lühe Kiepenheuer-Institut für Sonnenphysik Freiburg, Germany.
Error budget for the PRIMA conceptual design review Bob Tubbs, Richard Mathar, Murakawa Koji, Rudolf Le Poole, Jeff Meisner and Eric Bakker Leiden University.
Microspectrophotometry Validation. Reasons for Changing Instruments Reduced reliability. Limited efficiency. Limited availability and cost of replacement.
INTERFEROMETER TO MEASURE DISPERSION Michelson Interferometer response.
Romain G. Petrov Laboratoire LAGRANGE (OCA-UNS-CNRS) Avec S. Lagarde, F. Millour, M. Vannier, S. Rakshit (LAGRANGE), T. Elhalkouj (UCA Marrakech),
George Angeli 11 September, 2001 Current Concepts and Status of GSMT Control Systems.
Géraldine Guerri Post-doc CSL
MOSS Spectroscopy Applications in Plasma Physics John Howard Plasma Research Laboratory Australian National University.
Lagrangian measurements using Doppler techniques: Laser and Ultrasound Nicolas Mordant (Ecole Normale Supérieure de Paris) Romain Volk, Artyom Petrosyan,
Currently: 3 year ( ) NSF-supported UF/IAP collaborative project "Methods and Instruments for High-Precision Characterization of LIGO Optical Components"
PRIMA Astrometry Calibration and Operation Plan PRIMA Astrometry Calibration and Operation Plan VLT-PLA-AOS draft Scope of the Document 
PERFORMANCE OF THE DELPHI REFRACTOMETER IN MONITORING THE RICH RADIATORS A. Filippas 1, E. Fokitis 1, S. Maltezos 1, K. Patrinos 1, and M. Davenport 2.
Investigation of Variations in the Absolute Calibration of the Laser Power Sensors for the LIGO Photon Calibrators Stephanie Erickson (Smith College) Mentor:
Thermally Deformable Mirrors: a new Adaptive Optics scheme for Advanced Gravitational Wave Interferometers Marie Kasprzack Laboratoire de l’Accélérateur.
LumiCal Alignment System Status report Leszek Zawiejski, Tomasz Wojtoń, Arkadiusz Moszczyński Institute of Nuclear Physics PAN, Cracow 25th FCAL Collaboration.
Fringe tracking principles and difficulties F. Delplancke with help from J-B. le Bouquin, S. Ménardi, J. Sahlmann, N. Di Lieto... and many others.
Duke University, Fitzpatrick Institute for Photonics BIOS Lab, Department of Biomedical Engineering Two-wavelength unwrapping for transmission-geometry.
The polarization-based collimated beam combiner and the proposed NOVA fringe tracker (NFT) for the VLTI Jeffrey A. Meisner, Sterrewacht Leiden Walter J.
Blue Dot Team « Multi aperture imaging ». BDT sept MAI techniques High accuracy visibility measurement Differential interferometry Nulling.
Spectral Analysis of atmospheres by nulling interferometry Marc OLLIVIER Institut d’Astrophysique Spatiale - Orsay.
ECE 8443 – Pattern Recognition ECE 8423 – Adaptive Signal Processing Objectives: Introduction SNR Gain Patterns Beam Steering Shading Resources: Wiki:
1 On-sky validation of LIFT on GeMS C. Plantet 1, S. Meimon 1, J.-M. Conan 1, B. Neichel 2, T. Fusco 1 1: ONERA, the French Aerospace Lab, Chatillon, France.
19 February 2009 Cophasing sensor for synthetic aperture optics applications First steps of the development of a cophasing sensor for synthetic aperture.
Blue: Histogram of normalised deviation from “true” value; Red: Gaussian fit to histogram Presented at ESA Hyperspectral Workshop 2010, March 16-19, Frascati,
‘OHANA Towards kilometric infrared arrays Visions for InfraRed Astronomy Paris March 21, 2006 Guy Perrin (+ many others including Pierre)
Andreas Horneffer for the LOPES Collaboration Detecting Radio Pulses from Air Showers with LOPES.
FLAO system test plan in solar tower S. Esposito, G. Brusa, L. Busoni FLAO system external review, Florence, 30/31 March 2009.
An Approach to Stabilizing Large Telescopes for Stellar Interferometry It shakes like a…. [G. Vasisht, 31 March 2006] N. Di Lieto J. Sahlmann, G. Vasisht,
LIGO-G Z Peter Shawhan, for the LIGO Scientific Collaboration APS Meeting April 25, 2006 Search for Gravitational Wave Bursts in Data from the.
 a mathematical procedure developed by a French mathematician by the name of Fourier  converts complex waveforms into a combination of sine waves, which.
Displacement calibration techniques for the LIGO detectors Evan Goetz (University of Michigan)‏ for the LIGO Scientific Collaboration April 2008 APS meeting.
Characterising exoplanetary systems with space-based Bracewell interferometers ARC meeting Denis Defrère Liege, 19 February 2009.
ATLAS The LTAO module for the E-ELT Thierry Fusco ONERA / DOTA On behalf of the ATLAS consortium Advanced Tomography with Laser for AO systems.
CHARA Collaboration Meeting, New York, 15 March 2007 The Precision Astronomical Visible Observations (PAVO) instrument for CHARA Mike Ireland (Michelson.
1 High-order coronagraphic phase diversity: demonstration of COFFEE on SPHERE. B.Paul 1,2, J-F Sauvage 1, L. Mugnier 1, K. Dohlen 2, D. Mouillet 3, T.
The AMBER & MIDI instruments of the VLTI (Observationnal Astronomy II) Lecture by Stéphane Sacuto.
Frequency Scanned Interferometer Demonstration System Tim Blass, Jason Deibel, Sven Nyberg, Keith Riles, Haijun Yang University of Michigan, Ann Arbor.
Koji Arai – LIGO Laboratory / Caltech LIGO-G v2.
1 W. Rooney May 20, 2004 Imaging the Awake Animal MRI Efforts Overview.
Experimental results of tomographic reconstruction on ONERA laboratory WFAO bench A. Costille*, C. Petit*, J.-M. Conan*, T. Fusco*, C. Kulcsár**, H.-F.
Observing Strategies at cm wavelengths Making good decisions Jessica Chapman Synthesis Workshop May 2003.
SNAP Calibration Program Steps to Spectrophotometric Calibration The SNAP (Supernova / Acceleration Probe) mission’s primary science.
CARE / ELAN / EUROTeV Feedback Loop on a large scale quadrupole prototype Laurent Brunetti* Jacques Lottin**
MIDI design, performance, operations, and science Markus Schöller (INS)
Searching for Gravitational Waves from Binary Inspirals with LIGO Duncan Brown University of Wisconsin-Milwaukee for the LIGO Scientific Collaboration.
Olivier ABSIL Université de Liège * Pathways Towards Habitable Planets Barcelona, 14/09/2009.
MONALISA: The precision of absolute distance interferometry measurements Matthew Warden, Paul Coe, David Urner, Armin Reichold Photon 08, Edinburgh.
The Self-Coherent Camera: a focal plane wavefront sensor for EPICS
Gabriele Vajente ILIAS WG1 meeting - Frascati Noise Analysis Tools at Virgo.
1 Locking in Virgo Matteo Barsuglia ILIAS, Cascina, July 7 th 2004.
Charts for TPF-C workshop SNR for Nulling Coronagraph and Post Coron WFS M. Shao 9/28/06.
Ball Aerospace & Technologies Corporation -
Observations with AMBER  General overview  P2VM  OB preparation with P2PP P2PP / OB / templates Available templates for observation procedure Typical.
Electron beams in order to sense nm-size mechanical vibrations? CERN: Marek Gasior: BBQ electronics (Andrea Boccardi: VME electronics) Juergen Pfingstner:
Large Dynamic Range Co-Phasing System Development for Segmented Telescope Mirrors Piston and Tip/Tilt expected errors The initial error after deployment.
教育部顧問室光通訊系統教育改進計畫台科大 師大 淡江 東南 萬能 教育部顧問室光通訊系統教育改進計畫 台科大 師大 淡江 東南 萬能 3. 光調變器之性能量測 (Modulation Measurements) Modulation measurement is essential in characterizing.
ARENA08 Roma June 2008 Francesco Simeone (Francesco Simeone INFN Roma) Beam-forming and matched filter techniques.
LIGO-G D Advanced LIGO Systems & Interferometer Sensing & Control (ISC) Peter Fritschel, LIGO MIT PAC 12 Meeting, 27 June 2002.
Martin Hewitson and the GEO team Measuring gravitational waves with GEO600.
Metrology and integrated optics Geoff Pryde Griffith University.
Calibration and the status of the photon calibrators Evan Goetz University of Michigan with Peter Kalmus (Columbia U.) & Rick Savage (LHO) 17 October 2006.
Optical Coherence Tomography
Adaptive optics Now: Soon: High angular resolution
MICHELSON AND WHITE LIGHT INTERFEROMETRY
Observational Astronomy
Improving LIGO’s stability and sensitivity: commissioning examples
Dispersive Comb-Spectrum Interferometer: Metrological Characterization
Presentation transcript:

Cophasing activities at Onera Kamel Houairi Frédéric Cassaing

Cophasing at Onera I/ Pupil-plane fringe sensing Persee Gravity II/ Focal-plane fringe sensing Phase retrieval/diversity New algorithms under study (F. Cassaing)

PERSEE Context Main objectives Nulling demonstrator for formation-flying missions (Darwin/TPF-I, Pegase, FKSI, …) Main objectives 10-4±10-5 achromatic nulling In the [1.6-3.2] µm spectral band In presence of realistic disturbances For several hours Validate the full operation (star/fringe acquisition, tracking, calibration, unloading of fine correctors)

Consortium and sub-systems ONERA OCA TAS IAS LESIA CNES GEPI Perturbation Source Correction Nulling detector Star Sensor Beam combiner Fringe Sensor Laboratory

Beam combination Wide-band null  Modified Mach-Zehnder P1 P2 P3 P4 Achromatic p shift 4 outputs (ABCD) Spectral separation after combination Common fringe sensor / science instrument Nulling [1.6-3.2] µm Fringe tracking [0.8-1.5] µm A D C B 5

Fringe sensor setup Spatial modulation Central fringe identification Allow high measurement frequency (fringe acquision) D measured by fringe sensor  Real Time null depth monitoring Central fringe identification Dispersion is the simplest way Minimize detector noise  2 spectral channels are enough Simultaneous ABCD in I & J  2 phases, 2 visibilities

Operating modes and free parameter optimization Measurement Estimator Parameters Detection Visibility ls, q Acquisition Goup delay ls Tracking Phase delay ls, p Estimator noises depend on ls Dispersion: I = [0.8-ls]µm -- J = [ls-1.5]µm  Optimal ls ?

Separation wavelength optimization Wide spectral band  Measurement noise = f(d) Estimated OPD measurement noise vs ls (photon noise) Group delay ls = 1 µm, p=0.5, not sensitive d=0 nm d=100 nm d=20 nm d Phase delay d ls = 1 µm, sensitive

Final cophasing (piston/tip/tilt) design - RT computer - 8 monopixel detectors Correction Spectral dispersion

Cophasing design at Onera (autocollimation) - RT computer - 8 monopixel detectors Correction + Perturbation Injection bloc: spectral dispersion One output is used for the light injection

Preliminary cophasing implementation at Onera Backwards light injection Detection Alignment

Calibration Analytical equations of the spatial interferometer Linear system  OPD = f-1(measurement) Need a calibration process Phase shift ≈ p/2 Dark Intensity arm 1 arm 2

New extended coherencing algorithm (experimental results) Estimated OPD is l-periodic  two lambda analysis to extend the unambiguous range Classical algorithms are L periodic Estimation of the synthetic wavelength fringe order by a new (real time) agorithm Mission au VLTI: algorithm sur 5 canaux ? Extension of the OPD estimation range by a factor of 5 To do: Extension for N>2 spectral channels (PRIMA DATA)

Results of the fringe tracking Only laboratory disturbances, sampling = 150Hz Open loop Closed loop OPD PSD Open loop Closed loop Open loop Closed loop Open loop: sopd = 4.5 nm rms Closed loop: sopd = 1.3 nm rms  nanometric residual reached

Gravity 2nd generation VLTI instrument Instrument design: 4 UTs AO correction Fringe tracking Fringe tracking residual OPD < l/10

GRAVITY: 4 beam combination 4 telescopes to combine 3 independent OPDs to control Hyp.: pairwise based combination  6 baselines Several possibilities to combine the beams One OPD measurement 1/3:1 Splitting ratio What is the best combination ? How to choose ? Systematic procedure derived, based on noise propagation minimization

Specification (l/10) reached with loop frequency fs = 400 Hz Gravity FS simulation l/10 Selected Fringe Sensor: S6 Control law: Integrator model based Atmospheric OPD spectrum R0=0.95m @ 2.2µm t0=47ms @ 2.2µm Total variance: 23 µm rms Dispersion: 5 spectral channels (coherencing + science measurements with fringe sensor) Specification (l/10) reached with loop frequency fs = 400 Hz

Onera’s Perspectives for pupil-plane FS Persée : Complete Persee installation and qualification Operate cophasing and nulling systems in parallel New PhD student for advanced control techniques Gravity Refined simulation underway (Phase B) New PhD student fall 2009 (Lesia-Onera)