Title: Imaging the Event Horizon: Past, Present
1Imaging the Event Horizon Past, Present
Future VLBI of Sgr A
- Geoffrey C. Bower
- UC Berkeley
2Principal Collaborators
- Backer, D.C. (UCB)
- Doeleman, S. (MIT)
- Falcke, H. (MPIfR)
- Goss, W.M. (NRAO)
- Herrnstein, R. (CfA/Columbia)
- Quataert, E. (UCB)
- Wright, M.C.H. (UCB)
- Zhao, J.-H. (CfA)
3Why Study Sgr A?
- Unique Laboratory for Astrophysics
- 1 mas 0.1 milli-parsec 150 R_g
- Unprecedented multi-wavelength information
- Degeneracy in Measurements and Models
- Role of inflow, outflow, jets not settled
- i.e., 105 range for M_dot
4Sgr A Basic Properties
- Supermassive Black Hole
- 3 x 106 M_sun
- Extremely underluminous
- L L_sun 10-10 L_edd
- Inverted Spectrum
- a gt 0.1 0.7
- Compact, nonthermal
- Size lt 1 AU _at_ 3mm
- Tb gt 109 K
5Models of Sgr AWhy is L ltlt L_edd?
- Under-fed systems
- Jet
- CDAF
- Bondi-Hoyle
- Under-luminous systems
- ADAF
6Models of Sgr AWhy is L ltlt L_edd?
- Under-fed systems
- Jet
- CDAF
- Bondi-Hoyle
- Under-luminous systems
- ADAF
1mm Polarization Indicates dM/dt lt 10-7 M_sun y-1
7What We Want to See
- Structure
- Ejection of components
- Correlated changes with X-ray variability
- Astrometric measurements (Reid talk)
- ?
8What We See
- Elliptical Gaussian
- 2 x 1 ratio
- East-West major axis
- No detection of
- Extended structure
- Separate components
9Scattering Inhibits Imaging Points to Higher
Frequencies
Lo et al. 1998
10Is there Structure?
Lo et al. 1998
11Difficulty of mm Imaging SgrA
- Axisymmetric Structure
- Purely an amplitude measurement
- Low Declination High Frequency
- Poor and variable antenna gain
- High Tsys
- Variable opacity
- Short and variable coherence time
- Lack of North-South resolution
12Closure Amplitude
VmnVpq
Cmnpq -----------------
VmqVnp
Independent of station-based gain errors!
13Closure Amplitude Properties
- Independent of station-based gain errors
- Still dependent of baseline-based errors
- Decorrelation, for example
- Reduced sensitivity
- 2/3 for N7
- Non-Gaussian errors
- Doeleman et al. 2000 --- 3mm imaging
14Sample Closure Amplitudes
15Error Surfaces
16Slices through the Error Surface
17Herrnstein et al. 2003, Zhao et al. 2003
18Results 22 GHz
Equal scales
19Results 43 GHz
Equal Scales
20New ResultsConsistent with Scattering
9 Q, 4 K, 1 U experiments
3 7 13 20 mm
3 7 13 20 mm
21Past and Present Conclusions
- Mean properties consistent with scattering
- Axisymmetric structure only
- Based on closure phases
- Max variability between high and low flux states
no N-S extension - Delta Major axis 30 mas ? 60 /- 30 R_g
- Delta Minor axis 40 mas ? 90 /- 90 R_g
- No outflow? Slow outflow? Along line of sight?
22Whats Next for the VLBA?
- Add GBT at 7mm
- Links SC/HN to rest of array
- Increased SNR for closure amplitude
- 3mm
- Doeleman et al (2000)
- VLBA ad hoc
- Resolution over the scattering
23The Future
Falcke, Melia Agol 2000
Bardeen 1973
24Event Horizon Shadow
- Shadow with radius 5 R_g must exist
- Optically thin emission required
- Polarization suggests tau lt 1 at 1.3 mm
- Sgr A is the only realistic candidate
25Whats Necessary for the Future?
263- or 4-station Image
1.5 Jy
Shadow
Best-fit Gaussian
27Technical Requirements
- High frequency receivers antenna performance
- 230/350 GHz
- Phase stability
- Water vapor radiometers
- Time standards
- Array Phasing
- Correlator options
- gt Gigabit recording
28How Will We Do It?
- NSF-STC Gravity proposal
- UC Berkeley, Stanford, U Washington
- CMB, Quantum Gravity, Small-scale r-2 tests
- 3 station, full-polarization image by 2010
- Provide support for technical development,
instrumentation and observations - Collaboration!
29Summary
- Gold standard of imaging
- Closure amplitude
- Closure phase
- VLBA Future Observations
- Deviations in size of 10s of micro-arcseconds
- Detecting the event horizon
- Technical innovation
- Collaboration
- Proof of existence of black holes!