Central supermassive black holes from SINFONI observations

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Central supermassive black holes from SINFONI observations R.P Saglia, MPE with R.Bender, N.Nowak, P. Erwin, J. Thomas Gas and stars in Galaxies A Multi-Wavelength 3D Perspective Garching, 10th June 2008

Outline Introduction: status of present direct (dynamical) SMBH mass measurements Near-IR integral-field observations of galactic nuclei with SINFONI What can we measure at the diffraction limit Dynamical Modeling The MBH-σ relation Conclusions

Supermassive black holes All galaxies with a massive (classical) bulge component host a SMBH. The mass of the SMBH correlates with the velocity dispersion and the luminosity/mass of the bulge strong link between bulge formation and black hole growth M77 M87 N7457 M32 MW Tremaine et al. 2002

Classical- and pseudo-bulges Two different bulge-types: - classical bulges: mini-ellipticals, formed by mergers - pseudobulges: disk-like characteristics (e.g. rapid rotation), formed by secular evolution M81: classical bulge mini-elliptical inner disk + starforming ring NGC1512: pseudobulge

Status few dynamical SMBH mass measurements (~40), mostly normal, massive E low-σ (<120km/s) and high-σ (>300km/s) regime not very well constrained very few non-e s (pure disks, pseudobulges) few core ellipticals very few merger remnants and AGN Goals: constrain MBH-σ slope by measuring low- and highσ range measure MBH for special galaxies

Problems direct (dynamical) MBH measurements require a very high spatial resolution to resolve the sphere of influence (usually <<1 ) high S/N (>30 per pixel) required (high surface brightness) strong dust obscuration in most disks, pseudobulges, AGN and merger galaxies in AGN: non-stellar emission dilutes spectral signatures dynamical modelling difficult if non-axisymmetries (bars) are present

SINFONI NIR-AO: high spatial resolution <0.1 less affected by dust non-stellar contribution less strong (in AGN) SINFONI@VLT: integral-field spectrograph SPIFFI+adaptive optics module MACAO near-ir (1-2.5μm): J, H, K and H+K FOV: 0.8 (25mas), 3.0 (100mas) and 8.0 (250mas) 32x64 spatial resolution elements Spectral resolution in K: ~50 km/s PARSEC: Na line laser, bright reference star for AO observations SINFONI PARSEC

Observed galaxies GTO time for SINFONI detectors and OmegaCam R. Bender Galaxy D 0.1 (Mpc) pc σ (km/s) dsoi ( ) resolution ( ) Type nucleus NGC1398 18 9 200 SBab 0.34 0.19..0.32 pseudo Sy NGC3368+ 10 5 128 SBb 0.22 0.15..0.25 pseudo LINER NGC3627+ 10 5 115 SABb 0.19 0.15/0.088 pseudo Sy2 NGC4501 13 6 161 SBa 0.33 0.13 pseudo Sy2 NGC4569 16 8 117 SABab 0.11 0.15 pseudo Lin/HII NGC4579 16 9 154 SABb 0.23 0.15 pseudo Sy1.9 NGC4699 19 9 215 SABb 0.37 0.13 pseudo Sy NGC3412 11 5 101 SB0 0.11 0.13 low-σ - NGC3489 12 6 105 SAB0 0.12 0.08 low-σ Sy2 NGC4486a* 16 8 110 de 0.13 0.10 low-σ - NGC5102 4 2 65 SA0 0.10 0.12/0.07 low-σ Stbrst/HII Fornax A 18 9 228 E pec 0.44 0.12/0.08 core? FRI *Nowak et al. 2007, MNRAS, 379, 909 + Laser Guide Star used

The 3D datacube PSF NGC 4486a Data Reduction: spred/gasgano

Stellar continuum 3.2 0.8

Stellar Kinematics Maximum penalized likelihood method (Gebhardt et al. 2000): non-parametric fit of template spectra convolved with line-of-sight velocity distribution (LOSVD) strongest spectral features in K band: CO bandheads LOSVD V, σ, h, In the following: Gauss-Hermite Parametrization 3 4 h

Stellar velocity fields NGC 3368 V σ h3 h4 NGC 3489 NGC4486a

Kinematics of NGC1316 Nowak et al. almost submitted v σ h3 h4 25mas 100mas 250mas

NGC 5102: σ~65 km/s

Line indices NGC1316 Na I Ca I Fe I CO(2-0) near-ir (K band) indices: Na I (2.21μm), Ca I (2.26μm), Fe I (2.23μm), CO (2.29μm) spectral synthesis models not yet available, but soon? Credit: Silva, Kuntschner, Lyubenova

NGC 3627 Gas emission H H 2 1-0 S(1) 2 Brγ 1-0 S(1) λ (μm) No flux calibration done yet, do not ask for gas masses! Brγ

Gas maps No emission detected in NGC 1398, NGC3412, NGC3489 NGC4486a, NGC4501, NGC4699, NGC 5102 H 2 1-0 S(1) NGC 4569 NGC 4579 NGC1316

-150 Gas Kinematics: NGC 3627 Gas might not trace the gravitational potential 150 Stellar Velocity Field H2 Velocity Field 0

Counterrotating gas in NGC 3368

Stellar dynamical modelling Schwarzschild (1979) orbit superposition technique (Gebhardt et al. 2003, Thomas et al. 2004/5): gravitational potential (from light distribution of stars) + assumed mass-to-light ratio M/L + assumed MBH generate orbit library (~2x7000 orbits) find weighted superposition of orbits that reproduce light distribution and best fits the LOSVDs repeat with systematically varied M/L and MBH best-fitting M/L and MBH follow from χ 2 analysis

Photometry and longslit data dust-corrected SOFI and NICMOS images NGC 1316 Siding Spring 2.3m, CaT region

Best-fit model NGC4486a

NGC 4486a Black hole masses NGC 1316 NGC 1316 NGC 3368 NGC 3489 1.5 10 M +0.25 8-0.80 6 6.3 10 M 6 6.8 10 M 8 more to come in the next months! +0.75 7 NGC 4486a 1.5 10 M -0.79

The M σ relation NGC3368 NGC3489 NGC4486a Cen A Fornax A M87

Conclusions SINFONI delivers diffraction-limit 2D spectra that probe well the central regions of local galaxies 12 galaxies with low σ and/or pseudo/classical bulges and/or merger remnant/agn observed with SINFONI Stellar (and gas) kinematics measured to constrain the mass of the central supermassive black hole Gas emission detected in 5 galaxies Modeling of 4 galaxies confirms predictions of the relation M σ From Period 82 on: observations of local giant Es with σ>300 km/s and/or cores.