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Arman Khalatyan AIP 2006 GROUP meeting at AIP

Arman Khalatyan AIP 2006

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AGN formation by Merging Galaxies. Arman Khalatyan AIP 2006. GROUP meeting at AIP. Outline. What is AGN? Scales The model Multiphase ISM in SPH SFR BH model Self regulated accretion ?! Galaxy mergers Setup, resolution, numeric's … Results Prospects. The Scales. - PowerPoint PPT Presentation

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Page 1: Arman Khalatyan AIP 2006

Arman KhalatyanAIP 2006GROUP meeting at AIP

Page 2: Arman Khalatyan AIP 2006

Outline• What is AGN?

– Scales• The model

– Multiphase ISM in SPH• SFR

– BH model• Self regulated accretion ?!

• Galaxy mergers– Setup, resolution, numeric's …

• Results• Prospects

Page 3: Arman Khalatyan AIP 2006

The Scales.

A false color composite image of the central parsec of the GC taken by the Very LargeTelescope.Old, intermediate mass cool red giants and young massive hot blue stars.

Genzel et al. 2003

Page 4: Arman Khalatyan AIP 2006

Scales

Page 5: Arman Khalatyan AIP 2006

Galaxy Model• DM Halo-NFW profile• Disk – exponential

– stellar– gaseous

• Bulge – Hernquist profile

Springel et al. 2005

Page 6: Arman Khalatyan AIP 2006

Model-MULTIPHASE ISM, SFR

McKee & Ostriker (1977)McKee & Ostriker (1977)

Page 7: Arman Khalatyan AIP 2006

Model-MULTIPHASE ISM, SFR• First implementation of two phase ISM was by

G.Yepes et al (1997) for Eulerian code.• Modified and extended ISM model were

implemented using SPH formalism by Springel et al 2003.– radiative heating and cooling– cold clouds embedded in an ambient hot medium– star formation – feedback from SN( thermal feedback and cloud

evaporation)– Galactic winds and outflows– Metal enrichment

Page 8: Arman Khalatyan AIP 2006

SFR in MULTIPHASE ISM• Rates at which the masses of

the hot and cold phases evolve can be written:

• Effective EOS:

• Density dependence of the SN evaporation

• SFR:

Springel et al 2005

Note:we use q=0.05

Page 9: Arman Khalatyan AIP 2006

“GOLDEN RULE FOR SFR ?”• Kennicut law for sfr:

• SFR parameters:– t0

* 2.1 Gyr

– A0 1.0e4 K

– TSN 1.0e8 K

Springel et al 2005

Page 10: Arman Khalatyan AIP 2006

Cooling functionKatz et al. 1996

Page 11: Arman Khalatyan AIP 2006

Cooling function including metals

Dopita & Sutherland 2003

x95

Page 12: Arman Khalatyan AIP 2006

Modeling AGN• by Bondi(1952)

• A fraction of the power generated by the accretion of matter onto the black hole heats the surrounding gas at a rate:

• The Cooling rate per unit mass of heated gas is:

Cattaneo 2006

SPH implementation by Springel et al 2005

Energetic efficiency of black hole accretion 0.1

Hydrogen baryon fraction

Page 13: Arman Khalatyan AIP 2006

The BH model• The heating rate per unit mass of the gas

depends on three parameters: – the accretion efficiency with respect to the

Bondi rate : – the fraction of the accretion power converted

into heat: – the mass Mgas on which the heat is distributed

Cattaneo 2006, Springel et al. 2005

Page 14: Arman Khalatyan AIP 2006

Local M – T equilibrium • Black hole – IGM coupling factor:

Cattaneo 2006

Page 15: Arman Khalatyan AIP 2006

Parameter tests• Simulations was done by GAGDET-2 TreeSPH code.• Set of simulations was performed ( ~70 different mergers)

Page 16: Arman Khalatyan AIP 2006

Magorrian relation: MBH - Mbulge

Page 17: Arman Khalatyan AIP 2006

Parameter space study • Model parameters:

– physical: , , gas– numerical: MBH0, , NGB, qToomre

Page 18: Arman Khalatyan AIP 2006

Final BH mass vs and

Page 19: Arman Khalatyan AIP 2006

Mbh vs Mgas

Page 20: Arman Khalatyan AIP 2006

Suppression of SFR

Page 21: Arman Khalatyan AIP 2006

COOLING and BH-growth

Page 22: Arman Khalatyan AIP 2006

Gas temperature surrounding BH

Page 23: Arman Khalatyan AIP 2006

MOVIE

Page 24: Arman Khalatyan AIP 2006

Thank You for Your Attention.

To be continued…

Page 25: Arman Khalatyan AIP 2006
Page 26: Arman Khalatyan AIP 2006
Page 27: Arman Khalatyan AIP 2006

Next Step: CosmologyElliptical galaxy N198, Zoomed simulation in box 50Mpc/h with special resolution 1024^3 particlesMgas=5.9 1e5 M⊙

200 kpc/h

Z = 3.7