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Supermassive Black Holes

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Title: Supermassive Black Holes


1
Supermassive Black Holes their Host Galaxies
  • Ilana Klamer
  • CSIRO ATNF

2
Todays discussion
  • Some concepts
  • Supermassive black holes
  • The host galaxies
  • Active galaxies
  • Formation of SMBHs
  • Formation of massive galaxies
  • The current paradigm
  • and its problems
  • Where to from here?

3
Cosmological Distances
4
Sydney to Antofagasta 24 hours to
Antofagasta 0.04 seconds to Venus
4.3 minutes to Sun
8.3 minutes to V465 Cen 4.2
years to Canis Major 25 000 years to
UDF00452 12.8 billion years
X
5
REDSHIFT(i) Doppler (relative motion)(ii)
Cosmological (expansion of space-time)(iii)
Gravitational (bending of space-time)
a shift in the frequency of a photon toward lower
energy, longer wavelength, lower frequency.
6
(i) Doppler Redshift
7
(No Transcript)
8
  • Spectral lines from receding side of galaxy
    will be REDSHIFTED wrt local velocity of the
    galaxy whilst approaching spectral lines will be
    BLUESHIFTED

9
(ii) Cosmological Redshift
H?
H?
H?
z0.25 (D986 Mpc)
H?
H?
H?
H?
z0.06 (D247 Mpc)
H?
H?
H?
H?
z0.02 (D83 Mpc)
H?
H?
H?
H?
z0
10
(iii) Gravitational Redshift
Space-time bends in the presence of mass (a
strong gravitational field). Light, in order to
escape gravity, must expend energy to climb out
of the gravitational field.
11
Supermassive Black Holes
  • A black hole is a region of space-time from which
    nothing can escape from, not even light

12
Black Holes
  • Reverend John Michell (1783) - concept first
    proposed
  • That gravity could effect light as well as matter
  • Schwarzschild (1913) - derived formalism for the
    singularity
  • Using Einstein field equations
  • Chandrasekhar (1931) paper rejected by ApJ
  • A star of large mass cannot pass into the white
    dwarf stage, one is left speculating on other
    possibilities
  • Eddington the authority
  • a star would have to go on radiating and
    radiating, and contracting and contracting.I
    think there should be a law of nature to stop
    matter behaving in this absurd way
  • Oppenheimer (1939) exercise in abstraction
  • the star closes itself off from any
    communicationonly its gravitational field
    persists

13
Discovery of Quasars (1963)
  • The Lunar Occultation of 3C273
  • Parkes Observatory identifies a strong radio
    source with a bright (13th magnitude) star
  • A few of these weird stars already known
  • variable light so couldnt be extragalactic

14
  • Schmidt interprets spectrum as cosmological
    redshift z0.158
  • Only a black hole could provide this energy

Observational cosmology is born
15
The black hole at the centre of the Milky Way
(Sgr A)
NGC 1232- resembles our Milky Way
2x105 light-years across (2xMW) 70x106
light-years away
1 light year 1,000,000,000,000 km
16
Our black hole (Sgr A)
17
Our black hole (Sgr A)
Simultaneous fits to all the stellar orbits
yields a dark object which is 3.6 million solar
masses and confined to 8.5 light-hours in radius
18
Orbital motion under gravity
19
Black holes in other galaxies NGC 4258
  • Observed bright maser lines from rapidly rotating
    disk
  • Rotation purely Newtonian- 40 million solar mass
    central object
  • Extreme energies from the rotation can only come
    from a BH

20
And another one 1.2 billion solar masses
21
Very high redshift Quasars
Ly-? 121.6 nm Observed 885nm z 6.3 12.7
billion light years
22
Weighing a black hole
  • Binary systems (only good for small black holes
    orbiting around another star)
  • Proper motion of stars around black hole (only
    done for Sag A)
  • Rotation curves based on Maser emission lines
    from central accretion disk (NGC 4258 only)

23
other measurements
  • Rotation curves for gas
  • Velocity dispersion for stars

Velocity (km/sec)
M3 billion solar masses
24
Reverberation mapping
  • Based on a time delay between the continuum and
    emission line variations

Velocity (km/sec)
25
The host galaxies of supermassive black holes
26
The Hubble sequence
27
Spiral galaxies
  • NGC1232
  • young blue stars, and dark dust
  • Spectra dominated by light from stars.

28
Elliptical Galaxies
  • They are the most massive galaxies known at
    present (5000 billion solar masses)
  • Optical spectra dominated by old M and K stars
  • Their stars formed billions of years ago

29
The host galaxies
  • Massive black holes are at the centre of most
    galaxies (we already discussed this)
  • The black hole mass is intimately related to the
    host galaxy mass
  • i.e. the most massive black holes reside in the
    most massive galaxies

Black Hole Mass
Host Galaxy Mass
30
What have we discussed so far?
  • Space-time is curved by the matter (energy). In
    the vicinity of an extremely massive object, the
    curvature is so great that even light cannot
    escape and will be dragged back by its
    gravitational field. This is a black hole.
  • Since the discovery of quasars, we have had
    observational evidence exists for supermassive
    black holes at the centre of galaxies (I showed
    examples of Milky Way, NGC 4258, NGC4261)
  • It is now believed that supermassive black holes
    reside at the centre of most (all?) galaxies.
  • The masses of nearby host galaxies are
    proportional to the central black hole mass.
  • It is not clear that high-redshift (young)
    galaxies also display the same proportionality.

31
Questions?
32
Active galaxies
33
Seyfert galaxies
  • NGC 4151- a spiral
  • Spectrum is underlying spiral type (stars) plus
    emission lines from central AGN

Black hole masses 107-8 Msun
34
Radio Galaxies
35
Centaurus A
36
(No Transcript)
37
The CALOSIS project
  • CentaurusA Long Overdue Synthesis Imaging Survey

38
Formation and evolution of supermassive black
holes their host galaxies
39
The cosmic microwave background
  • Big Bang
  • (a tongue-in-cheek name given to the birth of the
    universe by Fred Hoyle)
  • Universe was born a hot plasma filled with e, s,
    photons.
  • too hot to combine and photons Thomson scattered
    off the plasma.
  • As universe expands and cools to about 3000K, e
    and p recombine to form H and photons can escape.
    This is at z1088 surface of last scattering
  • The photons have been redshifted down to 2.7K
  • 1948 Gamow, Alpher Hermann even predicted the
    CMB at 5K (28K later)
  • 1965 Penzias Wilson build a radiometer but
    cant account for 3.5K excess
  • Robert Dicke, Princeton Boys, weve been
    scooped!
  • Won Nobel Prize in 1978

Penzias Wilsons horn antenna
40
  • COBE Satellite confirms the BB nature of CMB
    the anisotropies associated with the surface of
    last scattering.
  • CMB isotropic to 1 part in 100,000.
  • Nobel Prize in Physics 2006 to Mather Smoot
  • "for their discovery of the blackbody form and
    anisotropy of the cosmic microwave background
    radiation
  • WMAP satellite is doing precision cosmology
    with finer detail studies of the anisotropies

41
The initial conditions of the Universe can be
summarized on a single sheet of paper, yet they
developed into the complex structures we see
today
42
The origin of structure
Time since Big Bang
43
The Universe
44
The first objects Pop III stars
  • Overdensities collapse and form first stars made
    of primordial gas
  • These are very massive and will collapse into
    black holes
  • These black holes grow by factors of a million in
    less than a billion years how?
  • Supermassive black holes detected 800 million
    years after the Big Bang.

BEWARE! these are simulations, predictions and
theory. Pop III stars have not yet been detected
45
setting the scene
46
  • Star Formation today
  • Gravitational collapse of cold dense clouds of
    gas
  • Complex highly inhomogeneous structures
  • Gravity v turbulence and magnetic fields
  • We still lack a comprehensive theoretical
    framework that predicts the IMF from first
    principles.
  • )

47
Star Formation in the Early Universe
  • Early Universe is much simpler?
  • Primordial gas left from big bang nucleosynthesis
  • H (75), He (25)
  • Absence of heavy elements and dust
  • No previous star formation
  • Magnetic fields weak/not dynamically important
  • 10-30 G compared with 10-6 G for spiral galaxies
  • May be easier to model, but why/how does it
    happen at all?

48
Star Formation in the Early Universe
  • Need cooling timescales ltdynamical timescales (or
    form a BH directly)
  • Most simulations, regardless of the initial
    conditions, produce lt1000K 106 Msun primordial
    clouds
  • These are gt10x lower than the atomic H cooling
    threshold
  • In the absence of all else, primordial gas must
    cool via H2
  • But since there is no dust, this must be in gas
    phase only
  • Free electrons or protons are required as
    catalyst, or some other direct process to ionise
    the atomic H

49
Star Formation in the Early Universe
  • LW (11.2-13.6eV) radiation from Pop III stars
    will photo-dissociate the H2 suppressing further
    star formation.
  • Need enhanced abundances of e- or e to enhance
    the H2 fraction reduce the negative UV
    feedback
  • X-ray photons from supernova remnants
  • Accretion onto black holes
  • free electrons in HII region
  • collisional ionisation in shock waves
  • relativistic plasma from AGN jets

50
Formation of supermassive black holes
  • The existence of 109 Msun SMBHs within 109 years
    of the Big Bang provides strong constraints on
    any galaxy/BH formation models.
  • Growth/mergers/accretion of 100-1000Msun Pop III
    black holes
  • Direct collapse of 108 Msun gas clouds below
    critical enrichment levels of order Z-3.5 Zsun
    with suppressed H2 cooling -gt BHs with average
    masses 5x104 Msun at zgt10.
  • Growth/mergers/accretion of above BH mass halos

51
Galaxy formation
  • Hierarchical formation (e.g lCDM)
  • Small things merge or coalesce to form larger
    things
  • This includes galaxies and black holes
  • Model explains large scale structure and is
    consistent with primordial fluctuations in the
    CMB radiation.
  • Consequence/Implication/Prediction
  • massive objects form last and do not exist in the
    early universe

52
We are clearly on the right track
53
We are clearly on the right track
But it cant explain everything yet?
Latest results from WMAP showing the structure in
the CMB radiation
54
Luminosity Functions
  • The most challenging outstanding problem in
    galaxy formation is to explain the shape of the
    luminosity function
  • the number of galaxies in L, L?L per unit
    volume.

faint end
faint end
bright end
bright end
data with original model prediction too many
high L and low L galaxies
55
Reproducing the mass function
What are these massive galaxies?
56
There are quasars,
radio galaxies,
and old ellipticals
SCUBA galaxies,
57
The problem with hierarchical formation
  • Reproducing the luminosity functions
  • Too many massive galaxies too early on
  • Too much star formation too early on
  • Too many supermassive black holes too early on
  • Too much chemical enrichment too early on
  • Too many satellite galaxies by a factor of 100

58
The end for ?CDM?
Slide adapted from Richard Ellis (Caltech)
59
Fixing ?CDM
  • The models dont agree with the observations.
  • Do you
  • 1. Add extra parameters to the models to fit the
    observations?
  • 2. Find new models through scientific process?

60
data with original model prediction too many
high L and low L galaxies
thermal conduction
energy injection
superwinds
61
Negative feedback
  • Radio jets (from AGN) heat the IGM and blowing
    gas out from the centre of the galaxy.

Perseus A in X-rays radio
62
Fixing the luminosity functionwith negative
feedback
Tah Dah!
63
Or, should we start to consider another paradigm?
  • Remember that
  • Mergers are clearly important
  • Large Scale structure well explained
  • Physics strongly prefers hierachical formation
  • So what have we left out?
  • Plenty! e.g. magnetic fields, masses of Pop III
    stars, chemical enrichment
  • Effects of the black hole energetics

64
Positive AGN feedback
  • Massive galaxies form faster than we think
  • Massive black holes exist earlier than we think
  • Black holes form first (suppressed H2 formation)
    and then hasten the formation of their galaxies
    (provide enhanced production of H2)
  • This is called positive FEEDBACK
  • (negative feedback is when the energy from the
    quasar halts the formation of the host galaxy)

65
Breakdown of M-? at high redshift?
  • Observations of high redshift radio galaxies
    suggest a SMBH is in place before the host
    galaxies form.
  • Recent measurements of the gas content in
    SDSSJ11485251 at z6.41 leave little room for a
    host galaxy which agrees with the M-s relation.

Mtot40-50 billion

Mgal3 trillion ???


Mbh3 billion
66
Examples of positive feedback e.g. Minkowskis
Object NGC 541
67
Positive Feedback in the early universe
  • UV (rest frame)
  • UV (rest frame)
  • Ly-a

Unpolarised shows absorption lines P-Cygni
type profiles similar to SF galaxies
68
Todays discussion (I hope!)
  • Some concepts
  • Supermassive black holes
  • The host galaxies
  • Active galaxies
  • Formation of SMBHs
  • Formation of massive galaxies
  • The current paradigm
  • and its problems
  • Where to from here?

69
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