Gaia – Revue des Exigences préliminaires 1 Testing dark matter with Gaia O. Bienaymé O. Bienaymé Strasbourg Observatory.

Slides:



Advertisements
Similar presentations
General Astrophysics with TPF-C David Spergel Princeton.
Advertisements

Measuring Our Rotation Measuring rotation in our galaxy is hard because we are inside it. One method for measuring circular rate of rotation at our radius:
Infrared Space Astrometry mission for the Galactic Bulge
MOND Modified Newtonian Dynamics A Humble Introduction Johannes Kepler Isaac Newton Markus Nielbock.
Galaxy Formation and Evolution Open Problems Alessandro Spagna Osservatorio Astronomico di Torino Torino, 18 Febbraio 2002.
Charles Hakes Fort Lewis College1. Charles Hakes Fort Lewis College2.
TeV Particle Astrophysics, Venice, August 29, 2007J. Siegal-Gaskins1 Signatures of ΛCDM substructure in tidal debris Jennifer Siegal-Gaskins in collaboration.
Chania, Crete, August 2004 “The environment of galaxies” Pierre-Alain Duc Recycling in the galaxy environment F. Bournaud J. Braine U. Lisenfeld P. Amram.
Galactic archaeology Rodrigo Ibata Observatoire de Strasbourg.
The Life Cycles of Stars and our Sun. Your Questions 1.Have you ever heard of the sun song by the group They Might be Giants?
Particle Astrophysics & Cosmology SS Chapter 7 Dark Matter.
Breaking tidal stream degeneracies with LAMOST Jorge Peñarrubia (IoA) Cambridge 2nd December 08.
Science Team Management Claire Max Sept 14, 2006 NGAO Team Meeting.
Basic Astrometric Methods William van Altena Yale University Basic Astrometric Methods Yale University July 18-22, 2005.
Mass to light ratio of the Milky Way disc Chris Flynn, Johan Holmberg, Laura Portinari Tuorla Observatory Burkhard Fuchs, Hartmut Jahrei ß Burkhard Fuchs,
The Galaxy as seen by RAVE L. Veltz, O. Bienaymé & A. Just.
The Milky Way Galaxy James Binney Oxford University.
DM in the Galaxy James Binney Oxford University TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AA A.
Distances. Parallax Near objects appear to move more than far objects against a distant horizon. Trigonometric parallax is used to measure distance to.
A Galactic halo road map The halo stars : where, whither, whence? Chris Thom, Jyrki Hänninen, Johan Holmberg, Chris Flynn Tuorla Observatory Swinburne.
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.
The Milky Way Center, Shape Globular cluster system
Levels of organization: Stellar Systems Stellar Clusters Galaxies Galaxy Clusters Galaxy Superclusters The Universe Everyone should know where they live:
In this talk we'll see that : We can only see about 1% of the Universe The dark side And ask: What is the Universe made of?
Galaxy-Galaxy Lensing What did we learn? What can we learn? Henk Hoekstra.
The Dark Universe Dark Matter Matters! Exploring the Dark Universe June 28-29, 2007 Indiana University.
1 Galactic Science and MOS on the WHT Amina Helmi.
The impact of Gaia on the future of astrophysics Coryn A.L. Bailer-Jones Max-Planck-Institut für Astronomie, Heidelberg.
Galaxy Rotation: How we know AS413 10/28/2014 D. Clemens.
The Nature of Galaxies Chapter 17. Other Galaxies External to Milky Way –established by Edwin Hubble –used Cepheid variables to measure distance M31 (Andromeda.
The Dark Side of the Universe Sukanya Chakrabarti (FAU)
Diaspora in Cercetarea Stiintifica Bucuresti, Sept The Milky Way and its Satellite System in 3D Velocity Space: Its Place in the Current Cosmological.
Numerical Simulations of Galaxy Formation in a LCDM Universe Mario G. Abadi Observatorio Astronómico De La Universidad Nacional De Córdoba CONICET, Argentina.
Parallax Luminosity and mass functions - a few basic facts Kinematics of the solar neighborhood Asymmetric drift Thin disk, thick disk Open and globular.
次世代位置天文衛星による 銀河系ポテンシャル測定 T. Sumi (Nagoya STE) T. Sumi (Nagoya STE) K.V. Johnston (Columbia) K.V. Johnston (Columbia) S. Tremaine (IAS) S. Tremaine (IAS)
Spiral Triggering of Star Formation Ian Bonnell, Clare Dobbs Tom Robitaille, University of St Andrews Jim Pringle IoA, Cambridge.
Today in Astronomy 328: the Milky Way Image: wide-angle photo and overlay key of the Sagittarius region of the Milky Way, showing vividly the effect of.
Lecture 39: Dark Matter review from last time: quasars first discovered in radio, but not all quasars are detected in the radio first discovered in radio,
Astronomy 404/CSI 769 Extragalactic Astronomy
The Milky Way Galaxy. Sky Maps in Different Bands.
Copyright © 2010 Pearson Education, Inc. Clicker Questions Chapter 14 The Milky Way Galaxy.
Stellar population Studies with LAMOST - Chen Bing - Contents Contents Galactic structure & Evolution Galactic structure & Evolution Related Projects Related.
On the other hand.... CDM simulations consistently produce halos that are cusped at the center. This has been known since the 1980’s, and has been popularized.
Title Galaxy Structure and Dark Matter Michael Merrifield University of Nottingham.
Dark Matter and Rotational Motion e.t. revised feb 09.
Galaxies: Our Galaxy: the Milky Way. . The Structure of the Milky Way Galactic Plane Galactic Center The actual structure of our Milky Way is very hard.
ASTR112 The Galaxy Lecture 4 Prof. John Hearnshaw 7. Globular clusters 8. Galactic rotation 8.1 From halo stars 8.2 From disk stars – Oort’s constant,
A Long Time Ago in a Galaxy Far, Far Away…. The Milky Way Galaxy: Home Sweet Home!! Our home Galaxy is called the MILKY WAY (like the candy bar ) Our.
Dark Matter in the Milky Way - how to find it using Gaia and other surveys Paul McMillan Surveys For All, 1st February 2016.
The Gaia Challenge Coryn A.L. Bailer-Jones Max-Planck-Institut für Astronomie, Heidelberg acknowledgements: ESA, the Gaia scientific community and industrial.
Pisa, 4 May 2009 Alessandro Spagna A new kinematic survey (from GSC-II and SDSS-DR7) to study the stellar populations of the Milky Way Alessandro Spagna.
From dark matter to MOND
Limits on the stellar mass content of galaxies from bar and spiral structure dynamics K.C. Freeman Research School of Astronomy & Astrophysics The Australian.
DM in the Galaxy James Binney Oxford University TexPoint fonts used in EMF. Read the TexPoint manual before you delete this box.: AAA.
Making action-angle disc models for Gaia Paul McMillan Lund Observatory Collaborators: J. Binney, T. Piffl, J. Sanders.
The Milky Way Galaxy. What are each of these?
ASTR112 The Galaxy Lecture 5 Prof. John Hearnshaw 8. Galactic rotation 8.3 Rotation from HI and CO clouds 8.4 Best rotation curve from combined data 9.
The prolate shape of the Galactic halo Amina Helmi Kapteyn Astronomical Institute.
Milky Way Galaxy 1 Dr. Bill Pezzaglia Updated: Nov 25, 2012.
THE CASE FOR MODIFIED GRAVITY James Binney Oxford University.
Beyond MOND: TeVeS and its Tests (Depeche MOND) Scott Noble CCRG RIT July 2, 2010.
(Collaborators: James Binney, Tilmann Piffl, Jason Sanders)
© 2017 Pearson Education, Inc.
An ACS High-latitude Survey
The Milky Way Galaxy 1/30/03.
Learning about first galaxies using large surveys
Disk, Bulge, Halo Rotation Curve Galactic Center
The Milky Way Our Galactic Home.
Constraining the Local Gravitational Potential in the MW by the Motion of Stars Student Workshop.
Dark Matter on Galactic Scales (and the Lack Thereof)
Presentation transcript:

Gaia – Revue des Exigences préliminaires 1 Testing dark matter with Gaia O. Bienaymé O. Bienaymé Strasbourg Observatory

Gaia / DM 2 Dark matter within our Galaxy Flat rotation curve => missing luminous mass =>dark matter halo

Gaia / DM 3 Dark matter within our Galaxy Vertical motion of stars (Kaptein, Oort 1920’) =>total mass density in the solar neigbourhood

Gaia / DM 4 Dark matter within our Galaxy Vertical motion of stars (Kaptein, Oort 1920’) =>total mass density in the solar neigbourhood (Hipparcos sat.) versus : seen mass (stars+gas) =>dark halo cannot be extremely flattened (Crézé et al 1998 ). =>dark disk is not massive, if any ….

Gaia / DM 5 Dark matter within our Galaxy Halo shape Local stellar 3D kinematics with Hipparcos satellite (about ten thousand stars) => vertical force perpendicular to the disk => (u,v,w) 3D velocity coupling => (u,w) tilt with RAVE and SDSS they give local constrain on the shape of the potential that is nearly spherical

Gaia / DM 6 Dark matter within our Galaxy Halo shape Local stellar kinematics with Hipparcos satellite => vertical force perpendicular to the disk => (u,v,w) 3D velocity coupling => (u,w) tilt with RAVE and SDSS they give local constrain on the shape of the potential that is nearly spherical

Siebert et al 2008; RAVE Tilt=6deg at z=1kpc Potential nearly spherical 500 red clump stars velocity ellpsoid tilt

Gaia / DM 8 Dark matter within our Galaxy Halo stars velocity distribution (radial velocities) (but no proper motions i.e. tangential motion) => flat rotation curve at large R High velocity star D.F. in the solar neigbourhood  Galactic escape velocity  total galaxy mass & flat rotation curve (model dependent) Globular clusters, dwarf galaxy satellites

Gaia / DM 9 Galactic escape velocity 33 stars

Gaia / DM 10 Halo stars: velocity distribution 552 Vrad

Gaia / DM 11 Dark matter within our Galaxy Halo shape Sagittarius tails precession of the orbit measures the shape of the potential Other streams

Gaia / DM 12 Dark matter within our Galaxy Halo shape Sagittarius tails precession of the orbit measures the shape of the potential Other streams Correnti 2010

Gaia / DM 13 Dark matter within our Galaxy

Gaia / DM 14 Dark matter within our Galaxy Need for distances (parallaxes), proper motions tangential velocities, radial velocities and very large samples, to constrain accurately the 3D shape of the galactic potential

Gaia / DM 15 Gaia: a unique experiment The next cornerstone of the ESA Science Programme Unique characteristics  Unprecedented astrometric accuracy (7-200  as)  Simultaneous astrophysical characterisation + radial velocity of observed objects  Survey down to V = 20  10 9 objects observed all over the sky  Launch 2012, Soyouz from Kourou

Gaia / DM 16 The third dimension: further and further Solar neighbourhood Up to ~ 30 pc Solar neighbourhood Up to ~ 200 pc All over the Galaxy Up to ~ pc In the bulge of the Galaxy Up to ~ pc In the Galaxy and the Local Group Up to ~ pc Ground-based, Hubble Precision: 3-5 mas Hipparcos (-2007) Accuracy: (0.1) mas Gaia ( ) Accuracy: 8-20  as Jasmine (?) Precision: 10  as SIM (?) Precision: 3  as

Gaia / DM 17 Performances for a G2 V star Astrometry: Photometry: accuracy on G magnitude Spectroscopy Magnitude< Accuracy [  as] V=15V=20 Per observation [mag] End of mission [mag] MagnitudeV=12.5V=16.5 RV accuracy [km/s]< 115

Gaia / DMAPC, 9 June

Gaia / DM Gavitational Potential with GAIA APC, 9 June Measure the total mass distribution from the gravitational potential Measure the baryonic mass (mainly stars, mainly the disk) Deduce the ‘exact’ shape of the D.M. distribution Hayashi, Navarro … 2007

Gaia / DM disk structure Disk warp and flare, relation with Monoceros stream? At 15 kpc: disk rotation ~ 6 mas/yr For a 1 kpc high warp: ~90  as/yr in latitude ~600  as/yr in longitude  easily measurable by Gaia 20

Gaia / DMAPC, 9 June Streams Intégrale du mouvement Amina’s figures Streams in the Galactic Halo

Gaia / DM 22 Streams in the Galactic Halo Again here, 3D kinematics at the faint end of the Gaia survey (V>16-17) would be a plus…or would even be crucial to identify sub-structures of the phase space Simulation of the accretion of 100 satellites galaxies (A. Helmi) Position spaceVelocity space

Gaia / DM Streams in the Galactic Halo APC, 9 June Integrals of motion space

Gaia / DMAPC, 9 June Constrains on the Clumpiness of the dark matter halo

Gaia / DM Gaia: long-term objective Choose potential, write Hamiltonian, write closest integrable Hamiltonian, find distribution function F(J), adjust potential… On shorter term: can we answer the crucial question of the existence of galactic dark matter by confirming/excluding (or at least constraining) a modified gravity approach?

Gaia / DM MOND within our Galaxy Stellar Disk within MOND  a newtonian astronomer observes  a spherical dark halo  and a dark disk (Milgrom, 86)

Gaia / DM Testing Newtonian gravity on galactic scales Modified gravity is only one version of MOND Only the relation between the potential and the matter source is altered, so one can constrain the potential in the usual way Crucially depends on our knowledge of the baryonic distribution Depends on the exact choice for  Then, the theory makes a unique and falsifiable prediction for the galactic potential => as an example let us use  (x)=x/(1+x) and the Besançon model based on the synthesis approach

Gaia / DM The « dark disk » from the Besançon Galactic model in MOND  eff = 78 M  pc -2 With  (x)=x/(1+x), at the solar position one has  eff = 78 M  pc -2 within z=1.1 kpc  dyn = M  pc -2 (TEST 1) to compare with present constraints  dyn = M  pc -2 (TEST 1) scale-length enhanced by 25% The effective radial density distribution in the disk has a scale-length enhanced by 25% [deep MOND => 50%]  even exclude MOND as modified gravity (TEST 2) => measuring dynamically the disk surface density as a function of R with GAIA (but problem of extinction, maybe JASMINE too) should allow to constrain  or even exclude MOND as modified gravity (TEST 2) => quick way to exploit GAIA data Bienaymé, Famaey et al. 2009, A&A 2.5kpc  3.1kpc Counts  Kz force

Gaia / DM The vertical tilt of the velocity ellipsoid (Bienaymé 2009) Angle  = arctg[2  2 UW /(  2 U -  2 W ) ]/2 is linked to the disk scale-legnth and dark halo flattening (Bienaymé 2009) => compute orbits in axisymmetric Besançon model to measure the tilt as a function of z at solar position Newton+DM MOND 6° 10°<14° RAVE data Siebert et al  (z=1kpc)= 7.3°+-1.8° TEST 3

Gaia / DM Conclusion We presented 3 quick tests to test MOND as modified gravity in the Milky Way with GAIA-like quality data constrain  even exclude MOND as modified gravity This should allow to constrain  or even exclude MOND as modified gravity knowledge of the baryonic distribution Testing gravity crucially depends on our knowledge of the baryonic distribution (even more than when determining the DM distribution) => importance of : - star counts, stellar population synthesis - gaseous content (including molecular gas) - inhomogeneities (clusters, gas clouds) Test other alternative theory