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Probing the close environment of the supermassive black hole at the center of the galaxy with GRAVITY Probing Strong Gravity Prague, February 18, 2010 Perrin
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Probing the close environment of the supermassive black hole at the center of the galaxy with GRAVITY Probing Strong Gravity Prague, February 18, 2010 Amorim, Araujo-Hauck, Bartko, Baumeister, Berger, Brandner, Carvas, Cassaing, Chapron, Choquet, Clénet, Collin, Dodds-Eden, Eckart, Eisenhauer, Fédou, Fischer, Gendron, Genzel, Gillessen, Gräter, Hamaus, Haubois, Haug, Hippler, Hofmann, Hormuth, Houairi, Ihle, Jocou, Kellner, Kervella, Klein, Kolmeder, Lacour, Lapeyrère, Laun, Lenzen, Lima, Moratschke, Moulin, Naranjo, Neumann, Patru, Paumard, Perraut, Perrin, Pfuhl, Rabien, Ramos, Reess, Rohloff, Rousset, Sevin, Straubmeier, Thiel, Vincent, Wiest, Zanker-Smith, Ziegleder, Ziegler
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Mini spiral (50’’) S star cluster (12-400 mas) Circumnuclear disk (120’’) 2-disk central cluster (0.5 pc-12.5’’) The environment of Sgr A* Sgr A* 10 µas
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Orbits of stars around Sgr A* Schödel et al. (2002) Sgr A*
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Orbits of stars around Sgr A* Schödel et al. (2002) S2S2
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Two ways of measuring strong GRAVITY effects around Sgr A* 1. Studying the closest star orbits inside the central 60 mas Need to resolve star cluster. Scale ~ 100 R g = 1 mas resolution. (mas) Relativistic precession in Schwarzschild metric
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Sgr A* blinking Genzel et al. (2003)
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Two ways of measuring strong GRAVITY effects around Sgr A* 2. Using flaring regions as test particles. Measure flare motion. Scale ~ 1 R g = 10 µ as accuracy Time scale = 10 min Genzel et al. (2003) Hot spot orbiting the ISCO or a more distant orbit. Eckart et al. A&A 500, 935 (2009)
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Sgr A* is quite dark Long wavelengths are well suited. Stars are bright in the near-infrared (orbits) and instruments sensitive enough to allow for short exposures (flares).
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How to get to the 1 mas resolution and 10 µas accuracy in the near-infrared ? One of Prague famous astronomers, Tycho Brahe, found the solution: use a large instrument Measurement accuracy scales as the reciprocal of the size of the instrument.
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Use the 4 VLT in interferometric mode ~ 140 m Resolution: 3 mas @ 2.2 µ m (K band) Build GRAVITY ! (General Relativity viA Vlt InterferomeTrY)
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Interferometric imaging in the near-infrared works Altair Monnier et al. 2007 Cep Zhao et al. 2008 Betelgeuse Haubois et al. 2009 Mira Perrin et al. in prep Cyg Lacour et al. 2009
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Imaging the closest stars with GRAVITY One-night observation image: Paumard et al. (2005) mas Point Spread Function Dirty 6-star imageAfter deconvolution mas
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Imaging the closest stars with GRAVITY Orbits after 15 months of observation: Paumard et al. (2005) mas 1 mas = 100 R g Schwarzschild advance of pericenter is detected
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Lens-Thirring and Quadrupole Precession Testing the no-hair theorem Orbital plane precession (precession of the angular momentum vector around the spin of the black hole) Will (2008) Wheeler’s “black holes have no hair” theorem: a BH is fully characterized by only three parameters: Mass M, Spin J, Electric charge In particular Quadrupole Q 2 = -J 2 / M 1 year orbit, e=0.9 Measurement of frame dragging precession may be feasible after a few years for orbits in the radial range between 0.2 mpc and 1 mpc (5 and 25 mas) Merritt et al. (2009)
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Reference star Sgr A* The measured distance between the two interferograms is: opd = B. S Hence: S = opd / B A 5 nm accuracy on opd with a 100 m baseline yields a 10 µas accuracy on S. SS opd 0 opd = B. S Narrow angle interferometric astrometry Performance analysis: errors from atmosphere, baseline, noise, pupil position, etc … 23 µas per baseline 13 µas with 6 baselines
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Muterspaugh et al. (2006): “… the 20μas level has been demonstrated …” 110 m and 87 m baselines 40 cm telescopes The Palomar Testbed Interferometer did it !
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See Frédéric Vincent’s talk Measuring the last stable orbit Newton primary GR image total image secondary GR image Paumard et al. (2005)
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Reference sources for GRAVITY near Sgr A* Reference source for adaptive optics Reference sources - IRS 16 - for interferometry (imaging and astrometry)
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GRAVITY is in the design … Adaptive Optics Wavefront Sensor
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… and prototyping phase Fibered delay line 4-telescope integrated optics beam combiner Laser metrology system Metrology test on VLT secondary mirror at Paranal
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Where we are standing and where we are going Preliminary Design Review took place in december 2009 Final Design Review is scheduled for June 2011 First tests at Paranal : 2014 Hopefully first results on Sgr A* in 5 years from now.
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