C. Cacciari INAF - Osservatorio Astronomico, Bologna The primary objective of Gaia is the Galaxy: to observe the physical characteristics, kinematics and.

Slides:



Advertisements
Similar presentations
MEASURING DISTANCES IN ASTRONOMY Basic Principles: Geometric methods Standard candles Standard rulers [the last two methods relate quantities that are.
Advertisements

Infrared Space Astrometry mission for the Galactic Bulge
P.Tisserand Rencontres du Vietnam Final results on galactic dark matter from the EROS-2 microlensing survey ~ images processed - 55 million.
WHY STUDY ASTROPHYSICS?  To gain an understanding of our universe and our role in it Learn about how the universe operates --> modern science  Observations.
How to simulate the Gaia products Francesca Figueras Universidad de Barcelona (Spain)
Distance Ladder. Pre-class Problem You stand are looking at “famous local landmark” from two positions on either side of the “other famous local place”.
Chapitre 3- Astrometry PHY6795O – Chapitres Choisis en Astrophysique Naines Brunes et Exoplanètes.
Carlos Allende Prieto Mullard Space Science Laboratory University College London The ESA mission Gaia.
Gaia A Stereoscopic Census of our Galaxy November 2003
Compilation of stellar fundamental parameters from literature : high quality observations + primary methods Calibration stars for astrophysical parametrization.
30 March 2006Birmingham workshop1 The Gaia Mission A stereoscopic census of our Galaxy.
Distances. Parallax Near objects appear to move more than far objects against a distant horizon. Trigonometric parallax is used to measure distance to.
PLAnetary Transits and Oscillations of stars Thierry Appourchaux for the PLATO Consortium
February 14, 2006 Astronomy Chapter 18: Celestial Distances A Galaxy 150 Million Light Years From Earth.
9B The Milky Way Our Galactic Home. 9B 9B Goals Structure of our Galaxy. Its size and shape. How do stars and things move through it? Mass and Dark Matter.
Properties of Stars. Distance Luminosity (intrinsic brightness) Temperature (at the surface) Radius Mass.
The Milky Way Center, Shape Globular cluster system
The Milky Way Galaxy. The Milky Way We see a band of faint light running around the entire sky. Galileo discovered it was composed of many stars. With.
Distance Determination of the Hubble Constant H o by the use of Parallax and Cepheid Variable Stars presented by Michael McElwain and G. Richard Murphy.
The Gaia mission Data reduction activities in the UK Floor van Leeuwen, IoA.
The GAIA photometry The GAIA mission, the next ESA Cornerstone 6 (launch ), will create a precise three dimensional map of about one billion.
The impact of Gaia on the future of astrophysics Coryn A.L. Bailer-Jones Max-Planck-Institut für Astronomie, Heidelberg.
BASIC PROPERTIES of STARS - 2 Distances to the stars Stellar motions Stellar motions Sections 3.1 & 3.2, poorly Sections 3.1 & 3.2, poorly covered in the.
Measuring the Stars How big are stars? How far away are they?
1B11 Foundations of Astronomy Cosmic distance scale Liz Puchnarewicz
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.
Properties of Stars.
AST 443/PHY 517 : Observational Techniques November 6, 2007 ASTROMETRY By: Jackie Faherty.
Gaia A Stereoscopic Census of our Galaxy November 2010
Surveys and Catalogs Summary: What is a survey? What surveys can do? Survey keywords (completeness, area, mag.limit, …) Type of surveys Survey among the.
High Precision Astrometry and Parallax from Spatial Scanning Part 2 Adam Riess and Stefano Casertano.
The Nature of the Stars Chapter 19. Parallax.
CU5-DU13: Ground-based support observations for Gaia absolute photometric calibration BOLOGNA: C. Cacciari, G. Altavilla, M. Bellazzini, A. Bragaglia,
THIS PRESENTAION HAS BEEN RATED BY THE CLASSIFICATION AND RATING ADMINISTRATION TG-13 TEACHERS’ GUIDANCE STRONGLY ADVISED Some Material May Be Unintelligible.
Luminosity and Colour of Stars Michael Balogh Stellar Evolution (PHYS 375)
Extrasolar planets. Detection methods 1.Pulsar Timing Pulsars are rapidly rotating neutron stars, with extremely regular periods Anomalies in these periods.
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.
Cosmology and extragalactic astronomy Mat Page Mullard Space Science Lab, UCL 5. The cosmic distance ladder.
Il ruolo della spettroscopia a grande campo per Gaia B. Bucciarelli - INAF/Osservatorio Astronomico di Torino S. Randich - INAF /Osservatorio Astrofisico.
Chapter 10 Measuring the Stars. Star Cluster NGC ,000 light-years away.
Announcements HW #1 will be returned on Wednesday Problem #7 – I wrote the distance incorrectly, should have been x1019 km. But don’t change your.
Object classification and physical parametrization with GAIA and other large surveys Coryn A.L. Bailer-Jones Max-Planck-Institut für Astronomie, Heidelberg.
Measuring the Stars What properties of stars might you want to determine?
Measuring the Stars How big are stars? How far away are they? How bright are they? How hot? How old, and how long do they live? What is their chemical.
FIRST LIGHT A selection of future facilities relevant to the formation and evolution of galaxies Wavelength Sensitivity Spatial resolution.
FoV: 0.7 deg x 0.7 deg, pixel (10 µm x 30 µm): 0.059”(AL) x 0.177”(AC) 106 CCD 4500x1966 px (TDI) ~4.4 sec 0.93m 0.42m Skymapper.
The Gaia Challenge Coryn A.L. Bailer-Jones Max-Planck-Institut für Astronomie, Heidelberg acknowledgements: ESA, the Gaia scientific community and industrial.
 Distance is the most important & most difficult quantity to measure in Astronomy  Method of Trigonometric Parallaxes  Direct geometric method of finding.
Properties of Stars. "There are countless suns and countless earths all rotating around their suns in exactly the same way as the seven planets of our.
Gaia A Stereoscopic Census of our Galaxy June 2009
Gaia Data Processing Coryn A.L. Bailer-Jones Max-Planck-Institut für Astronomie, Heidelberg on behalf of the Data Processing and Analysis Consortium (DPAC)
The Gaia Galactic Survey Mission Coryn Bailer-Jones Max Planck Institute for Astronomy, Heidelberg 2 nd Heidelberg Astronomy Summer School September 2007.
From last class Proper motion: movement of stars in the sky. Typical 0.1”/yr. Barnard's star 10”/yr. Distance is hard to measure. Parallaxes only work.
Gaia A Stereoscopic Census of our Galaxy December 2013
Measuring the Stars How big are stars? How far away? How luminous?
The Family of Stars.
Modern cosmology 1: The Hubble Constant
CASE-FOMBS Follow-up of One Million Bright Stars
Gaia A Stereoscopic Census of our Galaxy cosmos. esa
Institute of Cosmos Sciences - University of Barcelona
Astronomical distances.
Resolving the black hole - nuclear cluster - spheroid connection
Gaia impact on asteroidal occultations
Gaia impact on asteroidal occultations
9. Distances in open space
The Milky Way Our Galactic Home.
Gaia Tomaž Zwitter Gaia: > 1.1 billion objects (V ≤ 20.9),
Galactic and Extragalatic Astronomy AA 472/672
Celestial Distances A Galaxy 150 Million Light Years From Earth
Presentation transcript:

C. Cacciari INAF - Osservatorio Astronomico, Bologna The primary objective of Gaia is the Galaxy: to observe the physical characteristics, kinematics and distribution of stars over a large fraction of its volume, with the goal of achieving a full understanding of the MW dynamics and structure, and consequently its formation and history. (Concept and Technology Study Report, ESA-SCI(2000)4

Gaia in a nutshell  all sky (i.e. ~ 40,000 deg 2 ) survey complete to V lim = 20  ~ one billion sources  high (μas) accuracy astrometry (parallaxes, positions, proper motions)  optical spectrophotometry (luminosities, astrophysical parameters)  spectroscopy (radial velocities, rotation, chemistry) to V = 16

Satellite and System Figures courtesy EADS-Astrium ESA-only mission (Airbus DS contractor) Lifetime: 5 yr (+ 1yr possible extension) Launched on 19 December 2013 from Kourou (French Guiana) Launcher: Soyuz–Fregat L2 (gravitational equilibrium 1.5 million km from Earth away from Sun ) Figure courtesy A. Buzzoni Lissajous orbit around L2

Satellite and System Figures courtesy EADS-Astrium

Payload and Telescope Two SiC primary mirrors 1.45  0.50 m 2 at 106.5° SiC toroidal structure (optical bench) Basic angle monitoring system Combined focal plane (CCDs) Rotation axis (6 h) Superposition of two Fields of View (FoV) FoV 1.7° x 0.6°

Sky Scanning Principle Spin axis: 45 o to Sun Scan rate: 60 arcsec/s Spin period: 6 hr FoV-1: t 0 t 0 + 6hr FoV-2: t m t m + 6hr repeated days later 29 revolutions of spin axis around solar direction in 5 yr :

Transit maps Ecliptic coordinates Galactic coordinates End of mission (5 yr) sky-average number of transits: ~ 70 (max  200 at  = 45   10  )

Scanning the entire sky

MOVIE

The instruments Slitless spectroscopy on Ca triplet (847–870 nm) Resolution 11,500 R ~ 80 – 20 R ~ 90 – 70

Focal Plane CCD X time = 4.4 s Total field: - active area: 0.75 deg 2 - CCDs: each CCD: 4500x1966 px (TDI) - pixel size = 10 µm x 30 µm = 59 mas x 177 mas Astrometric Field CCDs – Total FOV ~ 40x40 arcmin ~ 4.4 ‘ ~ 4.4 ' Blue Photometer CCDs Sky Mapper CCDs cm Red Photometer CCDs Radial-Velocity Spectrometer CCDs Basic Angle Monitor Wave Front Sensor Basic Angle Monitor Wave Front Sensor Sky mapper: - detects all objects to 20 mag - rejects cosmic-ray events - FoV discrimination Astrometry: - total detection noise: 6 e - Photometry: - spectro-photometer - blue and red CCDs Spectroscopy: - high-resolution spectra - red CCDs 42.35cm along-scan

Gaia spectro-photometric system Figure courtesy A. Brown Internal calibration External calibration ● same principle as for classical spectrophotometry ● much more complicated instrument model ● ~ 200 calibrators needed to model instrument response ● mmag internal accuracy, a few % external accuracy

BP/RP first results Star HIP K5, V=6.64 ● BP and RP low resolution internally calibrated spectral energy distributions ● single transit ESA/Gaia/DPAC/Airbus

Radial-Velocity Measurement Concept Field of view RVS spectrograph CCD detectors Courtesy David Katz Spectra of the star HIP Top: Gaia-RVS on FoV 0, CCD row 4 strip 15 Bottom: Narval on 2-m Bernard Lyot Telescope (Pic du Midi), convolved to the nominal resolving power of the RVS: R=11500

Parallax – Parsec Arcsecond = 1/60 arcmin = 1/3600 deg = 1/ radian = 1/1,296,000 circle 1˝ ≈ the angle subtended by a US dime coin (17.9 mm diameter) at a distance of 4 km parallax (˝) = 1/distance (pc) Parsec (pc): distance at which the average Earth-Sun distance (1 AU= km) is seen under a parallactic angle (parallax) of 1˝ 1pc = 3.26ly

Astrometry: a historical perspective 150 BC degree 1 arcminute 1 arcsecond 1 milli-arcsecond 1 micro- arcsecond Hipparchos Tycho Brahe Flamsteed Bessel Hipparcos Gaia ?? Year meridian circles Large-angle astrometry Small-angle astrometry Figure: Lennart Lindegren 1/60 1/1000 1/100

Astrometry: data reduction principles Sky scans (highest accuracy along scan) Scan width: 0.7° 1. Object matching in successive scans 2. Attitude and calibrations are updated 3. Objects positions etc. are solved 4. Higher terms are solved 5. More scans are added 6. System is iterated (Global Iterative Solution) Figure courtesy Michael Perryman

From Hipparcos to Gaia Hipparcos (1997)Gaia ( ) Magnitude limit Completeness Bright limit Number of objects Effective distance (Mv=-3) Quasars Galaxies Accuracy Broad band photometry Spectrophotometry Spectroscopy (CaT) Observing programme ~ kpc None 1 ~ mas 2 (B and V) None Pre-selected targets 20 ~ 20 ~ Mpc ~ ~ ~ 5-14 μas at V  μas at V= μas at V=20 3 (to V=20) + 1 (to V=16) 2 bands (B/R) 1-15 km/s to V=16 Complete and unbiased

Astrometric accuracy: the Hyades d= 46 pc = 151 ly Figure courtesy ESA

One billion stars in 5D (6D … 9D) will provide: in the Galaxy … distances, velocity distributions and astrophysical parameters (APs) of all stellar populations in the MW to unprecedented accuracy allowing to:  map the spatial and dynamical structure of bulge, disk(s) and halo(s)  derive formation and chemical history (e.g. accretion and/or interaction events) of the MW & star formation history throughout  obtain the trigonometric calibration of primary distance indicators (RR Lyraes, Cepheids)  accurate and robust definition of the cosmic distance scale and beyond the Galaxy …  QSO detection and definition of rest frame  structure and stellar population studies in nearby (LG) galaxies

Stellar populations of the MW: The Hertzprung-Russell diagram BRIGHT intrinsic luminosities need distances FAINT HOT Temperatures from colours (spectrophotometry) COLD MOVIE

Trigonometric parallaxes: RR Lyr HST (Benedict et al. 2002; 2011) : RR Lyr π = 3.77 ± 0.13 mas (~265 pc)  mod = 7.13 ± 3.4% mag at [Fe/H] = -1.39, V=7.8, Av=0.13 mag,  V 0 =7.67 mag M V = 0.54  0.07 mag, M K =  0.07 mag Hipparcos (van Leeuwen 2007) : RR Lyr ( =7.8): the only RRL star with good Hipparcos parallax π = 3.46 ± 0.64 mas (~289 pc)  mod = 7.30 ± 18% mag Multiwavelength photometry & models (Catelan & Cortes 2008) : V=7.76, Av=0.048 mag, V 0 =7.71  0.06 mag, mod = 7.11 mag (weighted mean of all π)  M V = 0.60  0.13 mag evolved  overluminous by ~ 0.06  0.01 mag Non-evolved star of that metallicity should then have M V ~ 0.66 mag RR Lyr is not a `good’ candle … Δmod = 0.17 mag ΔV, ΔA V, evol

Gaia: MW field RR Lyraes GEOS database photometry: = – 0.15 = – 0.30  V mid IS = – 0.08 Mv = 0.52 for all (~ [Fe/H]=-1.5 dex) = (V max + V min )/2 Zero reddening  Individual end-of-mission   /  estimates ~ 5  (~ 340 RRL) to  1   1.5 kpc ~ 15  (~ 1000 RRL) to  5   4 kpc ~ 26  (~ 1750 RRL) to  10   5.7 kpc ~ 43  (~ 2900 RRL) to  20   8 kpc ~ 60  (~ 4000 RRL) to  30   10 kpc Expected from Gaia ~ bulge ~ halo (Eyer & Cuypers, 2000)

The distance scale: MW Cepheids Only ~ 800 Galactic Cepeheids are known – most are located in the Solar neighbourhood 400 Galactic Cepheids from David Dunlap DB distance and magnitude  Gaia predicted accuracy for parallax d < 0.5 kpc D < 1 kpc d < 2 kpc Presently, ~ 250 Cepheids with parallax & photometry (10 with HST parallax) only ~ 100 with σ π ≤ 1 mas (Hipparcos) Figure courtesy A. Brown Most (~ 3/4) Galactic Cepheids will have Gaia individual parallaxes to < 3%

The distance scale: MC Cepheids The bulk of the distribution for fundamental LMC pulsators lies at Period = 3 – 5 days Mv ~ -3  V ~ 15.8 – 16  individual distances to ~ 150%  mean of 400 to ~ 7-8 % Cepheids with P ≥ 10 d Mv ≤ ~  V ~ 14.5 individual distances to ~ 80% Ultra-long period (> 100 d) Cepheids Mv ≤ ~ - 7  V ~ 12 4 in LMC, 3 in SMC (Bird et al. 2009)  individual distances to ~ 45% (LMC) - 55% (SMC) 600 Cepheids in the LMC (OGLE, Udalski et al. 1999)  direct (trigonometric) calibration of the cosmological distance scale ~ 2000/1000 Cepheids are known (and observable by Gaia) in the LMC/SMC

Gravitational light bending This is the dominating relativistic effect in Gaia astrometric measurements Accurate measures of γ of Parametrized Post-Newtonian (PPN) formulation of gravitational theories is of key importance in fundamental physics Gaia will measure  to ~ 5x10 -7 ( present)

Data processing & distribution  Data Processing and Analysis Consortium (DPAC): more than 500 people from 20 European countries and ESA  Final catalogue ~ 2020–22  Intermediate data releases  Science alerts (e.g. SNe) data released immediately  No proprietary data rights

Thank you !

Parallax – Parsec Arcsecond = 1/60 arcmin = 1/3600 deg = 1/ radian = 1/1,296,000 circle 1˝ ≈ the angle subtended by a US dime coin (17.9 mm diameter) at a distance of 4 km parallax (˝) = 1/distance (pc) Parsec (pc): distance at which the average Earth-Sun distance (1 AU= km) is seen under a parallactic angle (parallax) of 1˝ 1pc = 3.26ly

GAIA science products: census of … Stellar pops in the Galaxy (based on the Besançon Galaxy model - Robin et al. 2003, 2004)  Disk: 9.0 x 10 8  Thick disk: 4.3 x 10 8  Spheroid: 2.1 x 10 7  Bulge: 1.7 x 10 8 Special objects in the Galaxy  Solar System bodies (~ 10 5 )  extra-solar planets (~ 10 4 )  binaries & rare stellar types (fast evolutionary phases)  WDs (~ 2 x 10 5 ), BDs (~ 5 x 10 4 ) Outside the Galaxy  brightest stars in nearby (LG) galaxies  supernovae and burst sources (~2x10 4 )  galaxies (~ 10 7 )  QSOs (~ 10 6 )  gravitational lensing events: < 10 2 photometric; a few 10 2 astrometric Fundamental Physics   to ~ 5x10 -7 ( present)

One billion stars in 5D (6D … 9D) will provide: in the Galaxy …  detailed structure, dynamics, formation and chemical history of the Milky Way, e.g. accretion/interaction events, star formation history etc.  a rigorous framework for stellar structure and evolution modelling  dating of all spectral types and Galactic populations  microlensing distribution and rate  map dark matter distribution … and beyond  definitive and robust definition (zero-point) of the cosmic distance scale (local calibrators, SNe)  QSO detection and definition of rest frame  structure and stellar population studies in nearby (LG) galaxies

Summary – Conclusions  Gaia will provide the distances, velocity distributions and APs of all stellar populations in the MW to unprecedented accuracy allowing to:  map the spatial and dynamical structure of bulge, disk(s) and halo(s)  derive formation and chemical history (e.g. accretion and/or interaction events) of the MW & star formation history throughout  obtain the trigonometric calibration of primary distance indicators  accurate and robust definition of the cosmic distance scale  Future surveys (especially the spectroscopic ones): none will provide all-sky coverage, but synergy will be extremely fruitful

Sky-averaged end-of-mission parallax standard error, in units of μas, as a function of Johnson V magnitude for 2 reference stellar types Estimates include a 20% margin for unmodelled errors (e.g. radiation damage effect on CCDs not fully taken into account) Astrometric performance (J. De Bruijne, ESA) σ ω ≤ 300 μas V lim = σ pos = 0.74 σ ω σ μ = 0.53 σ ω 6 < V < 12: bright-star regime (calibration errors, CCD saturation) V › 12: photon-noise regime

Photometry Measurement Concept Figures courtesy Anthony Brown RP spectrum of M dwarf (V = 17.3 mag) Red box: data sent to ground White contour: sky-background level Colour coding: signal intensity

Spectro-photometry (V < 20-22) Integrated:  white-light (G-band, nm) from the Astrometric Field  BP-band & RP-band  BP- RP colour Dispersed:  Blue (BP, nm) & Red (RP, nm) low resolution spectra Main sequence stars from O5 to M6: G=15, A V =0.0 (Straizys et al. 2006) dispersion 4-32 nm/px dispersion 7-15 nm/px

Photometric bandpasses: G, BP, RP & RVS Figure courtesy ESA

Radial-Velocity Measurement Concept RVS spectra of F3 giant (V = 15 mag) S/N = 7 (single measurement) S/N = 130 (summed over mission) Field of view RVS spectrograph CCD detectors Figures courtesy David Katz

RVS first results ESA/Gaia/DPAC/CNES/Yves Viala and Francoise Crifo RVS spectra ● calibrated in wavelength and flux ● on the three along scan CCDs for a single transit The internal apparent Grvs magnitude, computed from the flux of the spectra, is about 5.5 The star is HIP and is a K5 giant

Parallax – Parsec Arcsecond = 1/60 arcmin = 1/3600 deg = 1/ radian = 1/1,296,000 circle 1˝ ≈ the angle subtended by a US dime coin (17.9 mm diameter) at a distance of 4 km parallax (˝) = 1/distance (pc) Parsec (pc): distance at which the average Earth-Sun distance (1 AU= km) is seen under a parallactic angle (parallax) of 1˝ 1pc = 3.26ly