Top Banner
Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley- Bockelmann Steinn Sigurdsson Tom Abel Want more info? See astro-ph/0703540
13

Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

Jan 05, 2016

Download

Documents

Sheena Pope
Welcome message from author
This document is posted to help you gain knowledge. Please leave a comment to let me know what you think about it! Share it to your friends and learn new things together.
Transcript
Page 1: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

Supermassive Black Hole Growth from Cosmological N-body Simulations

Miroslav MicicKelly Holley-Bockelmann

Steinn SigurdssonTom Abel

Want more info? See astro-ph/0703540

Page 2: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

Original goal: approach SMBH merger rates ‘from the opposite direction’ of EPS

• •

••

EPS-derived BH merger rates (per year)

• 0.1 – 100 Haehnelt 94

• 1 - 100 Menou et al 01

• 10 Sesana et al 04

• 15 - 350 Wyithe + Loeb 03

• 15 Rhook + Wyithe 05

Page 3: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

How binary black holes meet and merge

O(10-5) pc

Galaxy merger BHs bound

O(106) pc

Dynamical friction

O(10) pc

3-body scattering Gravitational radiation

O(108) yr > O(1010) yr!** > O(1010) yr!*

*not anymore…thanks to excision and AMR

**in a static spherical galaxy with permanent ejections and no resonances

Page 4: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

10 Mpc3 from z=40-0 with 2 Mpc refined sphere

Mlow = 5.6 x 107 M rlow=4 kpc N=2 x 106

Mhigh = 8.9 x 105 M rhigh=2 kpc N=5 x 106

The nuts and bolts:

Page 5: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

Zooming into a group-sized volume of the universe

matter = 0.3 baryon= 0.045 dark energy = 0.7 n=1 8 = 0.9 h=0.7

Micic, HB, and Sigurdsson

Page 6: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

Strategy: Pop III seeds and fast, efficient mergers

• identify all the halos at z=20, and seed those with M > few 107 M with

200 M BHs

• continue seeding new halos until z~12 (Pop III star formation squelched by UV background…)

• Trace the evolution of halos and their embedded BHs from z = 20-0.

• Assume that BHs merge once the halos merge.

• Explore three accretion schemes:

– Dry mergers only– Salpeter accretion excited by at least 4:1 mergers.– Salpeter accretion excited by M1:M2 < 10:1 mergers.

Page 7: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

Sgr A*

M 31

Page 8: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

Max black hole merger rate is ~ 55 per year

Low mass ratio, ~ 1000 M BH mergers most abundant overall

High mass ratio ~ 1000 M mergers dominate 2<z<6 ULXs?

Page 9: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

Intermediate and Supermassive BH Growth

• BH merger rates ~55 per year

• Forming a 106 M SMBH requires major merger gas accretion

• To form a 107 M SMBH must also enlist gas accretion during minor mergers

• Largest SMBH is in place by z= 6, thereafter growth by mergers only (AGN era LISA era?)

• Lots of rogue IMBHs in a Milky Way-sized halo!

Page 10: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

A gravitational wave implication

• ‘new’ IMBH-SMBH merger source with rates > O(10) per year

Next paper: Can LISA be used as a tool to constrain BH growth mechanisms?

Page 11: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

…and a surprise: BH mass a product of environment

• a few isolated halos have extremely underweight bhs

Page 12: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

Following the leads with better dynamics

• gravitational wave kicks!

• proper treatment of dynamical friction

How robust is this merger rate?

Explore rogue black hole dynamics within Milky Way halo

Smaller volume, better resolved simulation – 1 pc resolution with on the fly BH mergers

Smooth accretion – tidal disruption + capture and inspiral

Do those BHs in the isolated halos stay vastly underweight?

How does this relate to downsizing?

Cosmic variance -- several realizations of same volume (~105 CPU hrs)

Suppression mechanisms

Page 13: Supermassive Black Hole Growth from Cosmological N-body Simulations Miroslav Micic Kelly Holley-Bockelmann Steinn Sigurdsson Tom Abel Want more info? See.

Ho et al 2003

Spitballing: Is there a variable spread in M-sigma?

Largest SMBHs require ‘all’ accretion mechanisms + kicks inefficient (early growth)

IMBHs have many formation/growth channels+ kicks efficient