SAIt 2008M. Gai - INAF-OATo1 GAME: Gamma Astrometric Measurement Experiment Space-time curvature parameter  Light deflection close to the Sun Apparent.

Slides:



Advertisements
Similar presentations
EUCLID : From Dark Energy to Earth mass planets and beyond Jean-Philippe Beaulieu Institut dAstrophysique de Paris Dave Bennett University of Notre Dame.
Advertisements

March , Birmingham GR tests and micro-arcsecond light bending parameters by global and differential Gaia mesurements Maria Teresa Crosta Astronomical.
General Astrophysics with TPF-C David Spergel Princeton.
UCL, 7-8 April 2010 EPRAT Workshop The Gaia Astrometric Survey A. Sozzetti A. Sozzetti INAF – Osservatorio Astronomico di Torino.
C. Beichman, Dimitra Touli, Gautam Vasisht, Roger Smith Tom Greene
Detection and Photometric Monitoring of QSOs and AGN with COROT J. Surdej, J.Poels, J.-F. Claeskens, E. Gosset Institut d’Astrophysique et de Géophysique,
Deriving the true mass of an unresolved BD companion by AO aided astrometry Eva Meyer MPIA, Heidelberg Supervisor: Martin Kürster New Technologies for.
Topic 11.3 Diffraction.
NEAT: Very high precision astrometry to detect nearby planetary systems down to one Earth mass F. Malbet, A. Crouzier, M. Shao, A. Léger and the NEAT collaboration.
Binary stellar systems are interesting to study for many reasons. For example, most stars are members of binary systems, and so studies of binary systems.
Early Universe Gamma Ray Burst Detection Scientific Rationale The first generation of stars were very important for the conditions of the early.
Chapitre 3- Astrometry PHY6795O – Chapitres Choisis en Astrophysique Naines Brunes et Exoplanètes.
Outline of the Lectures Lecture 1: The Einstein Equivalence Principle Lecture 2: Post-Newtonian Limit of GR Lecture 3: The Parametrized Post-Newtonian.
 (rad) = d/D = d/1AU = 0.53(2  /360  ) = , hence d = AU = x x 10 8 km = x 10 6 km or R sun = 6.96 x 10 5 km Can we apply.
Science Team Management Claire Max Sept 14, 2006 NGAO Team Meeting.
General Relativity Physics Honours 2006 A/Prof. Geraint F. Lewis Rm 557, A29 Lecture Notes 5.
The Search for Earth-sized Planets Around Other Stars The Kepler Mission (2009)
Extrasolar planet detection: Methods and limits Ge/Ay133.
Robo-AO First Science Workshop May 20, The Demo Period Robo-AO Science Workshop Agenda.
Circumstellar disk imaging with WFIRST: not just for wide field surveys any more... Tom Greene (NASA ARC) & WFIRST Coronagraph Team AAS / WFIRST Session.
Optical Interferometry for Fundamental Physics
PLAnetary Transits and Oscillations of stars Thierry Appourchaux for the PLATO Consortium
High Redshift Galaxies: Encircled energy performance budget and IFU spectroscopy Claire Max Sept 14, 2006 NGAO Team Meeting.
Detection of Terrestrial Extra-Solar Planets via Gravitational Microlensing David Bennett University of Notre Dame.
What stellar properties can be learnt from planetary transits Adriana Válio Roque da Silva CRAAM/Mackenzie.
JOVIAN and SOLAR RADIO DEFLECTION EXPERIMENTS Ed Fomalont National Radio Astronomy Observatory Charlottesville, VA USA Sergei Kopeikin University of Missouri.
Blue Dot Team « Multi aperture imaging ». BDT sept MAI techniques High accuracy visibility measurement Differential interferometry Nulling.
Jian-Yang Li, University of Maryland Marc Kuchner, NASA Goddard Space Flight Center Ron Allen, Space Telescope Science Institute Scott Sheppard, Carnegie.
December 14, 2001MISU Page 1 DARWIN D etecting & A nalysing R emote W orlds through I nterferometric N ulling a vessel.
ISNS Phenomena of Nature 1. Imaging –use a camera to take pictures (images) –Photometry  measure total amount of light from an object 2.Spectroscopy.
Exploring Space CHAPTER the BIG idea People develop and use technology to explore and study space. Some space objects are visible to the human eye. Telescopes.
The Hard X-ray Modulation Telescope Mission
Maria Teresa Crosta and Francois Mignard Small field relativistic experiment with Gaia: detection of the quadrupolar light deflection.
Recent determination of Gamma with Cassini M.T. Crosta, F. Mignard CNRS-O.C.A. 5th RRFWG, June, Estec.
M. Gai - GAMELa Thuile, Rencontres de Moriond XLVI, Gravitation Astrometric Measurement Experiment M. Gai - INAF-Osservatorio Astronomico di Torino.
Optical principles of diffraction focussing, Preparing the way to space borne Fresnel imagers NiceSeptember 23-25, Laurent Koechlin Laboratoire.
6/11/2012 Building on NEAT concept - M. Gai - INAF-OATo 1 Building on NEAT concept M. Gai – INAF-OATo (a) Extension of science case (b) Payload implementation.
The Origins Billion Star Survey K. Johnston, B. Dorland, R. Gaume, R. Olling,, (U.S. Naval Observatory), K. Seidelmann (University of Virginia), S. Seager.
AST 443/PHY 517 : Observational Techniques November 6, 2007 ASTROMETRY By: Jackie Faherty.
Jenam 2010 Exoplanet Targets for Upcoming Cosmic Visions Space Missions James Frith September 8 th 2010 University of Hertfordshire.
Characterising exoplanetary systems with space-based Bracewell interferometers ARC meeting Denis Defrère Liege, 19 February 2009.
Fundamental Principles of General Relativity  general principle: laws of physics must be the same for all observers (accelerated or not)  general covariance:
1 System wide optimization for dark energy science: DESC-LSST collaborations Tony Tyson LSST Dark Energy Science Collaboration meeting June 12-13, 2012.
Explorations of the Outer Solar System B. Scott Gaudi Harvard-Smithsonian Center for Astrophysics.
DARWIN The InfraRed Space Interferometer. Status of exo-planet search Stars (Solar type) observed: Planets detected: ~ 86 Radial velocity measurement.
Astronomy 340 Fall December 2005 Class #27.
Weak Lensing from Space with SNAP Alexandre Refregier (IoA) Richard Ellis (Caltech) David Bacon (IoA) Richard Massey (IoA) Gary Bernstein (Michigan) Tim.
A STEP Expected Yield of Planets … Survey strategy The CoRoTlux Code Understanding transit survey results Fressin, Guillot, Morello, Pont.
Science of the Solar System with GAIA D. Hestroffer 1,2, V. Zappalà 2, D. Carollo 2, M. Gai 2, F. Mignard 3, P. Tanga 2 1/ IMCCE, Paris Observatory, France.
Astrometry: The Second Oldest Profession A Random Walk Through Astrometry George H. Kaplan Astronomical Applications Department Astrometry Department U.S.
1 Optical observations of asteroids – and the same for space debris… Dr. D. Koschny European Space Agency Chair of Astronautics, TU Munich Stardust school.
SNAP Calibration Program Steps to Spectrophotometric Calibration The SNAP (Supernova / Acceleration Probe) mission’s primary science.
VST ATLAS: Requirements, Operations and Products Tom Shanks, Nigel Metcalfe, Jamie McMillan (Durham Univ.) +CASU.
Early science on exoplanets with Gaia A. Mora 1, L.M. Sarro 2, S. Els 3, R. Kohley 1 1 ESA-ESAC Gaia SOC. Madrid. Spain 2 UNED. Artificial Intelligence.
Binary stellar systems are interesting to study for many reasons. For example, most stars are members of binary systems, and so studies of binary systems.
Measuring Radii and Temperatures of Stars Definitions (again…) Direct measurement of radii – Speckle – Interferometry – Occultations – Eclipsing binaries.
System Performance Metrics and Current Performance Status George Angeli.
Binary stellar systems are interesting to study for many reasons
Lecture 13 Light: the Cosmic Messenger Telescopes and Observational Astronomy.
Charts for TPF-C workshop SNR for Nulling Coronagraph and Post Coron WFS M. Shao 9/28/06.
MPI Semiconductor Laboratory, The XEUS Instrument Working Group, PNSensor The X-ray Evolving-Universe Spectroscopy (XEUS) mission is under study by the.
Astronomy 3040 Astrobiology Spring_2016 Day-7. Homework -1 Due Monday, Feb. 8 Chapter 2: 1, 3, 16 23, 24, 26 29, 30, , 54, 56 The appendices will.
ISUAL Design Concept S. Mende. SDR 7 Jun NCKU UCB Tohoku ISUAL Design Concept S. Mende Sprite Example Sprite Image obtained by Berkeley/NCKU 1999.
X-ray Interferometer Mirror Module ISAL Study Pre-work Overview.
Terrestrial Planet Finder - Coronagraph
Science of the Solar System with GAIA
High Resolution Spectroscopy of the IGM: How High
Direct imaging discovery of a Jovian exoplanet within a triple-star system by Kevin Wagner, Dániel Apai, Markus Kasper, Kaitlin Kratter, Melissa McClure,
Observational Astronomy
CHEOPS - CHaracterizing ExOPlanet Satellite
Presentation transcript:

SAIt 2008M. Gai - INAF-OATo1 GAME: Gamma Astrometric Measurement Experiment Space-time curvature parameter  Light deflection close to the Sun Apparent star position variation Small mission class M. Gai INAF-Osservatorio Astronomico di Torino

SAIt 2008M. Gai - INAF-OATo2 Scientific rationale The GAME concept Implementation highlights Status and next steps Outline of talk:

SAIt 2008M. Gai - INAF-OATo3 Goals: Fundamental physics and cosmology Scientific rationale of GAME Review of basic framework: The classical tests on General Relativity Spacetime curvature in General Relativity   in Parametrised Post-Newtonian (PPN) formulation Current experimental findings on  Potential cosmological implications of  Science bonus

SAIt 2008M. Gai - INAF-OATo4 A space mission in the visible range to achieve long permanent artificial eclipses no atmospheric disturbances, low noise Method: repeated measurement of star angular separation The GAME concept

SAIt 2008M. Gai - INAF-OATo5 Observation sequence Fully differential measurement Precision on image location Systematic error control: beam combiner Fizeau-like interferometer solution PSF of the phased array Elementary astrometric performance Photon limited mission performance Key GAME concepts

SAIt 2008M. Gai - INAF-OATo6 Implementation highlights Payload layout Telescope configuration Detector Baffling Metrology Mission profile

SAIt 2008M. Gai - INAF-OATo7 Status and next steps Proposal submitted to FP7 IDEAS call (Feb. 2008) Next presentations: SPIE, COSPAR Preparation of proposals for next calls: ASI, MIUR, … Realistic simulations of observations and baffling Lab tests on telescope + BC feasibility / criticalities Lab test on metrology and baffling performance System level tests on sky of representative GAME mock-up Dissemination among scientific community to build support to the GAME concept

SAIt 2008M. Gai - INAF-OATo8 The current GAME team INAF-OATo: M. Gai, M.G. Lattanzi,S. Ligori, L. Corcione, M.T. Crosta, A. Vecchiato, G. Massone, D. Loreggia, D. Gardiol, A. Sozzetti, D. Bonino, D. Busonero INRIM: M. Bisi, F. Bertinetto, F. Alasia, P. Cordiale Industry: Thales Alenia Space; Altec Collaborations: A. Tartaglia (PoliTo); S. Capozziello (Univ. NA)

SAIt 2008M. Gai - INAF-OATo9 GAME OVER [PRESENTATION]

SAIt 2008M. Gai - INAF-OATo10 1. Perihelion precession of planetary orbit  Mercury 2. Light deflection by massive objects  Sun Eddington’s parameter  3. Gravitational redshift / blueshift of light “Modern” tests: Gravitational lensing; Equivalence principle; Time delay of electromagnetic waves (Shapiro effect); Frame dragging tests (Lense-Thirring effect); Gravitational waves; Cosmological tests (cosmic background) Classical tests of general relativity [Einstein, 1916]

SAIt 2008M. Gai - INAF-OATo11 Light deflection around massive objects 1".74 at Solar limb  8.4  rad Apparent variation of star position depending on light bending due to the gravitational field of the Sun  spacetime curvature

SAIt 2008M. Gai - INAF-OATo12 Repeated through XX century Precision achieved: ~10% Limiting factors: Need for natural eclipses Atmospheric turbulence ValueYearAuthors 1.66 ± TMET 1.98 ± Schmeidler 2.17 ± Schmeidler 1.70 ± van Biesbroeck 2.01 ± van Biesbroeck 2.73 ± Mikhailov 2.24 ± Freundlich & al ± Dodwell & al ± Dyson & al. Dyson - Eddington - Davidson experiment (1919): First test of General Relativity by light deflection nearby the Sun Short exposures, high background Large astrometric noise [A. Vecchiato et al., MGM ]

SAIt 2008M. Gai - INAF-OATo13 Cassini Radio link delay timing,  / ~1e-14 (similarly for Viking, VLBI: Shapiro delay effect, i.e. “temporal” component) Alternative experiment results Hipparcos Different observing conditions: global astrometry, estimate of full-sky level deflection on survey sample Precision achieved: 1e-4 ~ 2e-5 Earth Sun Cassini [B. Bertotti et al. Nature 2003]

SAIt 2008M. Gai - INAF-OATo14 Cosmology: Dark Matter, Dark Energy

SAIt 2008M. Gai - INAF-OATo15 [Capozziello & Francaviglia Gen. Relativ Gravit 40, 2008 and references therein]

SAIt 2008M. Gai - INAF-OATo16 f(R) gravitation fits experimental data

SAIt 2008M. Gai - INAF-OATo17 f(R) gravitation within Solar System Local measurements  cosmological constraints

SAIt 2008M. Gai - INAF-OATo18 Additional science topics Light deflection effects due to oblate and moving planets Monopole and quadrupole terms of asymmetric mass distribution Close encounters between Jupiter and selected quasars and stars Speed of gravity; link between dynamical reference system and ICRF Upper limits on masses of massive planets and brown dwarfs Nearby (d < pc), bright (4 < V < 9) stars, orbital radii 3-7 AU Time resolved photometry on transiting exo-planet systems Constraints on additional companions: mass, period, eccentricity Observation in / through inner part of Solar System NEO orbits and asteroid dynamics (a few close encounters) Circumsolar environment transient phenomena Mercury’s orbit  perihelion precession determination

SAIt 2008M. Gai - INAF-OATo19 Observation sequence Measurements epochs: E1, E2 to modulate deflection on fields F1, F2 (Sun action on/off) Deflection  measurement Calibration fields,   0

SAIt 2008M. Gai - INAF-OATo20 Star separation variation: deflection + instrument [base angle] Calibration fields affected mainly by instrument variations Fully differential measurement Basic equations referred to stars in Fields 1, 2, 3, 4; Epochs 1, 2 Base Angle: hardware separation between observing directions

SAIt 2008M. Gai - INAF-OATo21 Precision on image location  : Standard deviation of image location : Effective wavelength of observation Signal to Noise Ratio  photons, RON, background N: Number of photons collected  : Instrumental factor of degradation (geometry, sampling, …) X: Root Mean Square size of the aperture  can be a small fraction of pixel/image size Diffraction Statistics [MG et al., PASP 110, 1998]

SAIt 2008M. Gai - INAF-OATo22 Image displacement  BC mirror tilt only: 1  as x 1 m = 5 pm Base angle materialised in one component / degree of freedom Systematic error control: beam combiner [MG et al., Meas. Sci. Tech 10, 1999] HIPPARCOS-like split mirror

SAIt 2008M. Gai - INAF-OATo23 Basic technical requirements Sufficient angular resolution and photometric SNR  increase telescope size [collect more photons and concentrate them more effectively] Sufficient rejection of high Solar (background + diffracted) flux  reduce telescope size; increase baffling [shield line of sight from sources at narrow angle] Conflicting requirements!

SAIt 2008M. Gai - INAF-OATo24 A solution: Fizeau-like interferometer Pupil masking: set of elementary apertures cut on telescope pupil F1 F2 Top / bottom: pointed to different lines of sight, separated by Base Angle BA 7-aperture Phased Array Elementary aperture: 4  12 cm Aperture spacing: 4 cm External diameter: 0.57 m Internal diameter: 0.30 m Geometry to be optimised vs. astrometry / background

SAIt 2008M. Gai - INAF-OATo25 PSF of the phased array Monochromatic, = 650 nm Image size: ~4 arcsec Central peak: ~200 mas FWHM [MG & Cancelliere, MNRAS 377, 2007]

SAIt 2008M. Gai - INAF-OATo26 Bright case: 100 s exposures, close to Sun Background: 15.5 mag per square arcsec Faint case: 500 s exposures, away from Sun Background: 19.5 mag per square arcsec Elementary astrometric performance Band: _0 = 650 nm,  = 120 nm

SAIt 2008M. Gai - INAF-OATo27 Photon limited mission performance Precision on one 15 mag star: < 1 mas 1 million stars required to achieve 1  as cumulative  1e-6 equivalent precision on  Observing time required: days [on average Galactic plane stellar density from GSCII] Observation in Galactic center direction: higher density 1e-7 equivalent precision on  (3 + 3 month) [Vecchiato et al., IAUS 248, 2007]

SAIt 2008M. Gai - INAF-OATo28 PM: Pupil Mask FM1: Folding Mirror 1 FM2: Folding mirror 2 (Beam Combiner) TM1: Telescope Primary TM2: Telescope Secondary CCD: Detector Camera Volume of payload: ~1.5  1.5  1 m Mass budget: 120 kg + baffling structure Payload layout

SAIt 2008M. Gai - INAF-OATo29 Telescope configuration Ritchey-Chrétien, 5 mirrors, EFL = 20.6 m, visibility > 95% over 7  7 arcmin field; distortion < 1e-4 [Loreggia et al., IAUS 248, 2007]

SAIt 2008M. Gai - INAF-OATo30 [MG et al., A&A 367, 2001] E2V CCD42-80 Back illuminated, high performance CCD sensor Format: 2k  4k, 13.5  m pixels Two devices required for 7  7 arcmin field, sampling ~5 pixels/peak A possible CCD detector

SAIt 2008M. Gai - INAF-OATo31 Baffling Pupil masking on subsequent folding mirrors Observed field (solid) transmitted by facing surfaces, forbidden directions (dashed) shielded by pupil masks AND side baffles

SAIt 2008M. Gai - INAF-OATo32 Base Angle Metrology Metrology: considered to complement on-sky calibration

SAIt 2008M. Gai - INAF-OATo33 Stowed in launcher fairing Operating configuration – Side view Operating configuration – Top view Telemetry requirements OK with Kiruna and Fucino ground stations Mission profile Polar orbit, 1500 km elevation  no eclipse Spacecraft: ~Simbol-X Lifetime: 2(+2) years

SAIt 2008M. Gai - INAF-OATo34 GSCII star counts along ecliptic plane Astrometric performance depends on actual number, brightness and spectral type of observed targets

SAIt 2008M. Gai - INAF-OATo35 and GAIA (1-10 mas) Measurement range of GAME (0.1 – 1 arcsec) Observations are set in region of high amplitude deflection

SAIt 2008M. Gai - INAF-OATo36 GAME concept validation on-sky Observations close to full Moon: realistic performance on diffused background; set-up of pointing strategy

SAIt 2008M. Gai - INAF-OATo37 Baffling concept validation in lab Validation of rejection performance predictions

SAIt 2008M. Gai - INAF-OATo38 E2V CCD42-80 Quantum Efficiency Spectral band optimised on detector response AND sunlight rejection performance