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High Angular Resolution Imaging of the Galactic Center

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Title: High Angular Resolution Imaging of the Galactic Center


1
High Angular Resolution Imaging of the Galactic
Center
  • Andrea Ghez
  • University of California Los Angeles
  • Collaborators
  • E. E. Becklin, G. Duchene, S. Hornstein, J. Lu,
    M. Morris, A.Tanner, S. Wright

Image courtesy of 2MASS
2
Key Questions
  • Astrometry (Source Position) Questions
  • Is there a supermassive black hole at the center
    of our Galaxy?
  • Is it associated with the unusual radio source
    Sgr A?
  • What is the distance to the Galactic center (Ro)
  • Origin of young stars near black hole?
  • Is there a halo of dark matter surrounding the
    black hole?
  • Photometry Questions
  • Why is the black hole so dim (10-9 LEd)?
  • Does the black hole influence the appearance /
    evolution of the stars?

3
Dynamical Proof of Black Hole
  • Need to show mass confined to a small volume
  • Rsh 3 x MBH km (MBH in units of Msun)
  • Use stars as test particles
  • F -G Mencl m/ R
  • Impatient -gt velocity dispersions (ensemble)
  • Patient -gt full 3-d orbits (individual)
  • I. Black Hole II. Stellar Cluster (r a r -2)

BH
a r-1/2
(Velocity Dispersion)1/2
(Velocity Dispersion)1/2
r
r
stars
Enclosed Mass
Enclosed Mass
stars
BH
r
r
4
Inferred Dark Matter Density From Low Angular
Resolution Studies was too Small to Definitively
Claim a Black Hole
  • 3x106 Mo within 105 Rsh
  • Black Hole Alternatives
  • Clusters of dark objects permitted with the
    inferred density of 109 Mo/pc3
  • Fermion Ball

6
5
Inward Bound
  • Star closest to the center are the keys!
  • BUT
  • at center confusion due to high density of
    stars
  • Need high spatial resolution

Crowding Source separation 0.1 in central
1x1 Direct imaging resolution 0.4 Dynamic
Range 10001 (bright sources are at 1-3
and can be near the edge)
6
Two Independent High Resolution Imaging Studies
NTT La Silla
Keck (10-meter) NTT
(3.6-meter) 1995 - present 1992 - 2001
0.045 0.15 Ghez et al. 1998, 2000
Eckart Genzel 1996, 2002 Gezari et al.
2002 Genzel et al 1997, 2000 Tanner et al.
2002 Hornstein et al 2002 VLT (8-meter) Ghez
et al. 2003a,b,c 2002 - present
0.056 Schodel et al. 2002,
2003 Eisenhauer et al. 2003 Genzel et
al. 2003a,b
VLT Atacama, Chile
Keck Telescopes on Mauna Kea Hawaii
7
Diffraction-Limited Images Have Been Obtained
with 2 Methods Speckle Adaptive Optics (AO)
Beam Splitter
Deformable Mirror
Science Camera
AO allows deeper images spectra!
Wavefront Sensor.
Computer
8
Speckle Imaging
16NE
16NW
16C
16SW
  • Basic Building Block
  • A Single Short Exposure
  • 150 milliseconds
  • Shift reference source IRS 16C

Final Shift-and-Add Map 5,000 - 10,000 frames
9
Speckle vs. Adaptive Optics
Core Size Speckle 0.05 AO 0.11
Energy in Core Speckle 5 AO 35
  • AO images better for detection (finding) plus
    multi-l and spectra!
  • Speckle images better for astronomy (tracking)

10
Speckle PSF
  • Challenge for speckle is to minimize the effects
    of halo

11
Two passes ID sources - high correlation
threshhold to avoid false ID Find missing sources
- after sources have been tracked through
multiple images, look for them in maps where
they were missing at predicted locations with
lower threshhold
12
Tracking Issues
  • Alignment of the images
  • Using all possible sources, we minimized the net
    displacement of the stars
  • Initially all sources (200 sources)
  • Now eliminating sources with large velocities
    (gt600 km/sec)
  • Who is who?
  • Initially only taking data once a year
  • Now 2-3 times a year and have benefit of more
    info about how stars are moving (tricky at
    closest approach)

13
Positional Uncertainties
Centroiding depends on brightness Alignment
depends on location (grows towards the
edge) Central 1x1 (not shown!) brightest
stars (K14 mag) equal contribution
RA
DEC
1 milli-arcsec astrometric accuracy
14
Proper Motion Measurements Increased Dark Matter
Density (x103), Which Ruled Out Clusters of Dark
Objects
RA
DEC
Eckart Genzel 1997 Ghez et al. 1998 (shown)
15
Black Hole Case Strengthenedby Acceleration
Measurements
  • Accelerations provided first measurement of dark
    mass density that is independent of projection
    effects
  • r 3 a2-d / (4 G R2-d3)
  • Dark mass density increased by 10x ( 1013
    Mo/pc3) leaving only fermion balls as BH
    alternative.
  • Center of attraction coincident with Sgr A (30
    mas)
  • Minimum orbital period of 15 yrs for S0-2
    inferred

Ghez et al. 2000 (shown), Eckart et al. 2002
16
Proper Motions Now Permit Complete Astrometric
Orbital Solutions
1"
17
Orbits Increase Dark Mass Density By x104, Making
Black Hole Hypothesis Hard to Escape
Dark Mass Density Velocities 1012
Mo/pc3 Accelerations 1013 Mo/pc3
Orbits 1017 Mo/pc3 Fermion ball
hypothesis no longer works as an alternative
for all supermassive black holes m 50kev
c-2 Mass fermion ball lt 2x108 Mo Milky Way
is now the best example of a normal galaxy
containing a supermassive black hole
S0-16 has smallest periapse passage Rmin 90 AU
1,000 Rs
Ghez et al. 2002, 2003 (shown) Schoedel
et al. 2002, 2003
Independent solutions for 3 stars (those that
have gone through periapse)
18
Simultaneous Orbital Solution is More Powerful
than Independent Orbital Solutions
  • Improves Estimate of Black Holes Properties
  • Mass 3.70.4 x 106 (Ro/8kpc)3 Mo
  • Position 1.5 mas
  • Adds Estimate Black Holes Velocity on the Plane
    of the Sky
  • Velocity 30 30 km/s

19
Orbits Improve Localization of Black Hole in IR
Reference by an Order of Magnitude, Assisting
Searches for IR Emission Associated with Black
Hole
SiO masers used to locate Sgr A position in IR
frame (10 milli-arcsec) Reid et al. 2003
IRS 7
IRS 10ee
Sgr A
0.1
1
Dynamical Center pinpointed to 1.5 milli-arcsec
(12 AU)
20
At 3.8 mm, Stellar and Dust Emission are
Suppressed, Facilitating the Detection of Sgr A
Keck AO L(3.8 mm) images (Ghez et al. 2003,
ApJLett, in press, astro-ph/0309076) NIR results
fromVLT (Genzel et al. 2003, Nature)
21
Factor of 4 Intensity Change Over 1 week and
Factor of 2 Change in 40 minutes
22
Similarity of Flaring Time-scales Suggests IR and
X-ray Originate From Same Mechanism
Chandra / Baganoff et al. 2001
23
Flaring from non-thermal tail of high energy
electrons
  • Models
  • Markoff et al 2001
  • Yuan et al. 2003
  • Physical Process
  • Shocks
  • Magnetic reconnection
  • Emission Mechanism
  • IR Synchrotron
  • X-Ray Self-Synchrotron Compton or synchrotron
  • IR variability suggests electrons are accelerated
    much more frequently than previously thought

24
Simultaneous Orbital Solution Allows a Larger
Number of Orbits to be Determined
  • Black holes properties fixed by S0-2, S0-16,
    S0-19
  • M, Xo, Yo, Vx, Vy
  • Less curvature needed for full orbital solution
    for other stars
  • P, To, e, i, w, W
  • Need only 6 kinematic variables measured (Rx, Ry,
    Vx, Vy, Ax , Ay)

25
Eccentricities Are Consistent with an Isotropic
Distribution
While there are many highly eccentric systems
measured, there is a selection effect We only
measure orbits for stars with detectable
acceleration (gt 2 mas/yr2)
26
Lower Limit onSemi-Major Axis gt 1000 AUApoapse
Distance gt 2000 AU
No selection effect against detecting Klt16 mag
with Alt1000 AU
27
Possible Bias in Distribution of Apoapse
Directions
Other angle - inclination - appears random
28
With Only Imaging Data, Stellar-Type (age/mass)
is Degenerate
  • Based on 2 mm brightness (K 13.9 to 17 Mk
    -3.8 to -0.9) two expected possibilities
  • Late-Type (G/K) Giant (cool large old low
    mass)
  • Early-Type (O/B) Dwarf / Main-Sequence Star (hot
    small young high mass)

29
Stellar-Type Degeneracy Easily Broken with
Spectroscopy
30
Local Gas Makes it Difficult to Detect Weak Brg,
Unless Star has Large Doppler Shift
Local Gas
S0-1
1
  • Local Gas has strong Brg emission lines
  • Effects ability to detect stellar Brg absorption
    lines if Vz lt 300 km/s
  • For OB stars these are the strongest lines, which
    are already quite weak a few Angstroms
  • For low Vz sources, lack of CO is evidence that
    they are young

31
Brg in OB Stars in Sgr A Cluster Detected as
They Go Through Closest Approach
  • Example of S0-2
  • Vz 1100 to -1500 km/sec
  • EW(Br g) 3 Ang
  • EW (HeI) 1 Ang
  • Vrot 170 km/sec

32
Digression Addition of Spectra Also Provide a
Direct Measure of Galactic Center Distance (Ro)
NTT/VLT
Keck
33
Digression Ro is now largest source of mass
(spin) uncertainty
Ghez et al 2003 (Keck) Eisenhauer et al. 2003
(NTT/VLT)
1, 2, 3s contours
34
The Majority of Stars in the Sgr A Cluster are
Identified as OB Stars Through Their Lack of CO
Lack
Individual spectra Gezari et al. 2002 (shown,
R2,000), Lu et al (2004) Genzel et al. 1997
(R35) Integrated spectra Eckart et al 1999
Figer et al. 2000
35
Presence of OB Stars Raises Paradox of Youth
  • OB stars
  • Have hot photospheres (30,000 K)
  • Are young (lt10 Myr) massive (15 Mo), assuming
    that they are unaltered by environment
  • The Problem
  • Existing gas in region occupied by Sgr A cluster
    is far from being sufficiently dense for
    self-gravity to overcome the strong tidal forces
    from the central black hole.

36
Are These Old Stars Masquerading as Youths?
  • Possible Forms of Astronomical Botox
  • Need to make stellar photosphere hot
  • Heated (tidally?) by black hole (e.g., Alexander
    Morris 2003)
  • No significant intensity variations as stars go
    through periapse
  • Stripped giants (e.g., Davies et al. 1998)
  • Accreting compact objects (e.g., Morris 1993)
  • Merger products (e.g., Lee 1994, Genzel et al.
    2003)

37
Are Stars Young Formed In-Situ?
  • Past Gas Densities Would Have to Have Been Much
    Higher
  • What densities are needed?
  • 1014 cm-3 at R 0.01 pc (apoapse distance of
    S0-2)
  • Mechanism for enhancing past gas densities
  • Accretion disk (e.g., Levin Beloborodov 2003)
  • Colliding cloud clumps (e.g., Morris 1993, Genzel
    et al. 2003)

38
Are Stars Young, Formed at Larger Radii,
Efficiently Migrated Inwards?
HST/Figer
  • At larger radii, tidal forces compared to gas
    densities are no longer a problem
  • At 30 pc, young stellar clusters observed
  • Arches and Quintuplet (e.g., Figer et al. 2000,
    Cotera et al. 1999)
  • Massive (104 Mo) Compact (0.2 pc)

39
Migration Inwards is Difficult, Due to Short
Time-scales Large Distances
  • Ideas
  • Massive binaries on radial orbits experience
    three body exchange with central black hole
    (Gould Quillen 2003)
  • Cluster migration (Gerhard et al. 2000, Kim
    Morris 2003, Portegies-Zwart et al 2003, McMillan
    et al. 2003)
  • Need very central condensed cluster core
  • Variation on cluster migration - clusters with
    intermediate mass black holes, which scatter
    young stars inward (Hansen Milosavljevic 2003)

From New Scientist
40
Only Cluster Shuttled Inward with Intermediate
Black Hole Reproduces Orbital Properties, but
Where are They?
Directions of Apoapse Vectors
Distribution of Semi-major Axes
Orbital limit on reflex motion (lt 30 km/s) limits
IMBH to 2x105 (R / 16,000 AU)1/2 Mo
41
Conclusions
  • Dramatically improved case for black hole
  • Dark matter density increased to 1017 Mo/pc3
    with orbits, making the Milky Way the best
    example of a normal galaxy containing a
    supermassive black hole
  • First detection of IR emission from accreting
    material
  • More variable than X-ray
  • If from non-thermal tail of e-,
    shocks/reconnections happening more frequently
    than previously thought
  • Direct measure of distance to GC (Ro)
  • Raised paradox of youth
  • Majority of stars in Sgr A cluster appear to be
    young
  • Low present-day gas densities large tidal
    forces present a significant challenge for star
    formation (none of present theories entirely
    satifactory)
  • Dynamical insight from orbits

Central 1x 1
  • The Future
  • More orbits ( t3)
  • Ro to 1 (may allow a recalibration cosmic scale
    distance ladder)
  • Deviations for Keleperian orbits!

42
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43
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44
Original Case of Central Black HolesActive
Galactic Nuclei (AGN)
  • Emit energy at an enormous rate
  • Radiation unlike that normally produced by stars
    or gas
  • Variable on short time scales
  • Contain gas moving at extremely high speeds

Cyg A Jets 105 pc (galaxy 1/10 this size)
CENTRAL ACCRETING BLACK HOLES
45
Do normal (non-active) galaxies have quiet
black holes?
46
Milky Way is Best Place to Answer this Question
  • Pro - Closer (8 kpc)
  • Con - Obstructed View (dust)
  • Optical light 1 out of every 10 billion photons
    emitted makes it to us (invisible!)
  • Near Infrared light 1 out of every 10 photons
    emitted makes it to us (visible!)

47
Contribution from Luminous Matter
Gas Radial Velocity Measurements Gave 1st Hint
of Dark Matter
Evidence for Dark Matter
  • HI rotation along Galactic Plane
    (eg. Rougoor Oort 1960 Ooort 1977 Sinha 1978)
  • Circumnuclear disk/ring rotation (e.g.,
    Gatley et al. 1986 Guesten et al. 1987)
  • Ionized streamers in mini-spiral (e.g.,
    Serabyn Lacy 1985 Serabyn et al. 1987)

Plot from Genzel 1994 VLA 6 cm image of
mini-spiral
48
Dark Matter Confirmed with Stellar Radial
Velocity Measurements
  • Integrated stellar light
    (e.g., McGinn et al. 1989 Sellgren et al. 1990)
  • Individual Stars (OH/IR, giants, He I) (e.g.,
    Linquist et al. 1992 Haller et al. 1995 Genzel
    et al. 1996)

49
Sgr A Cluster Stars Amplifying a Problem
Originally Raised by the He I Emission Line Stars
  • He I Emission-Line Stars
  • Massive (20-100 Mo) post-main-sequence stars
    formed within the last 8 Myrs
  • Located at distances from the black hole of 0.1 -
    0.5 pc, which is 10x further than the Sgr A
    cluster stars
  • Formation problem
  • Required gas densities are not as severe, but
    still not found at 0.1 pc

OB stars in Sgr A cluster
Bright He I emission-line stars
50
Speckle vs. Adaptive Optics
Adaptive Optics Imaging 75 sec Klim16mag 170
stars
Speckle Image 1570 sec Klim16 mag 84 stars
AO detected twice as many sources! (extend l
spectra) Speckle better at astrometry in central
1x1
51
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