Title: Extragalactic Astronomy
1Extragalactic Astronomy
- First part Quasars and Active Galactic Nuclei
- Some supplemental reading GREAT compilation of
review articles at http//nedwww.ipac.caltech.edu/
level5/active_galaxies.html
2Introductions
- Who am I???
- See http//www.mikebrotherton.com and
http//physics.uwyo.edu/mbrother for information
about me and course materials. - Who are you???
- Tell me what you want to learn!
3Homework
- Read Introductory material from Peterson at
http//nedwww.ipac.caltech.edu/level5/Cambridge/fr
ames.html - Make your own redshift vs. magnitude diagram of
quasars from the Sloan Digital Sky Survey (hint
google sdss quasar catalog) and be able to
discuss it - Email me at mbrother_at_uwyo.edu if you have
questions or need help - Deadline Tuesday, October 14, 2008
4Quasars and Active Galactic Nuclei (AGNs)
- What are they?
- Observational Properties
- Standard Model
- Continuum, Lines, etc.
- How are they found?
- A variety of survey types, a zoo of AGNs
- Orientation and Unified Models
- How do they evolve?
- Strongly!
- Quasar Black Hole Masses
- Broad Absorption Line Quasars
- Relationship with their host galaxies
- Host galaxies
- Mutual Evolution?
5The (slightly) active nucleus of our galaxy
- Probable Black hole
- High velocities
- Large energy generation
- At a275 AU P2.8 yr ? 2.7 million solar masses
- Radio image of Sgr Aabout 3 pc across, with
model of surrounding disk
From Horizons, by Seeds
6The (slightly) active nucleus of our galaxy
- The Genzel et al. movie based on NIR speckle
interferometry of the Galactic core. - Basic orbital mechanics confirm, to high
precision, a mass of 2.6 million solar masses
that the stars are orbiting. - X-ray flaring also seen.
Other items from Genzels group
http//www.mpe.mpg.de/www_ir/GC/
7The (slightly) active nucleus of our galaxy
- FYI, here is one of the the Genzel groups
individual K-band images taken at high spatial
resolution using the technique of speckle
interferometry..
Other items from Genzels group
http//www.mpe.mpg.de/www_ir/GC/
8Active Galactic Nuclei AGNs
- A small fraction of galaxies have extremely
bright unresolved star-like cores (active
nuclei) - Shown here is an HST image of NGC 7742, a
so-called Seyfert galaxy after Carl Seyfert who
did pioneering work in the 1940s (you might look
up his original papers).
9NGC4151 with a range of exposures
10Spectra of Stars, Spectra of AGNs
Average quasar, from Brotherton et al. (2001)
Stars from Horizons by Seeds
11Active Galactic Nuclei AGNs
- Small fraction of galaxies have extremely bright
unresolved star-like nuclei - Very large energy generation
- Brightness often varies quickly
- Implies small size (changes not smeared out by
light-travel time) - High velocities often seen (gt 10,000 km/s in
lines) - Emission all over the electro-magnetic spectrum
- Jets seen emerging from galaxies
- Think about the implications of jets.
Timescales, angular momentum. What do they imply?
123C31
Red radio Blue visible
13Many Views of Radio Galaxy Centaurus A
14Many Views of Active Galaxy Centaurus A
15Quasar Images 1
16Theoretical Paradigm
- Supermassive black hole (millions to billions of
solar masses) - Powered by an accretion disk.
- Jet mechanisms proposed, but very uncertain.
Most quasars dont have strong jets. Some
quasars clearly have outflowing winds not well
collimated. - Also, an obscuring torus seems to be present.
(Unified models apply here.)
17AGN Accretion
- Old (1978!) basic accretion review paper
- http//nedwww.ipac.caltech.edu/level5/Rees3/Rees_c
ontents.html
18Accretion Disks
- Black hole is active only if gas is present to
spiral into it - Isolated stars just orbit black hole same as they
would any other mass - Gas collides, tries to slow due to friction, and
so spirals in (and heats up) - Conservation of angular momentum causes gas to
form a disk as it spirals in
From our text Horizons, by Seeds
19AGN Accretion Disks
- Modern disk paper with AGN application, Koratkar
and Blaes (1999), review in PASP - http//adsabs.harvard.edu/cgi-bin/nph-bib_query?bi
bcode1999PASP..111....1Kdb_keyASThigh3d657105
1d23256 - Basic ideas follow from Shakura and Sunyaev
(1973) standard alpha thin disks, plus
relativity, vertical disk structure, non-LTE,
Comptonization, etc. The models of Hubeny et al.
(2000) are the most advanced and available
on-line - http//www.physics.ucsb.edu/blaes/habk/
- alpha-disk solutions illustrate some basic
physics and arent too complicated. Check out
SS73 - My post-doc Shang and I fit these models to real
AGN SEDs. See these at the Wyoming AGN group
webpage at http//physics.uwyo.edu/agn
20Malkan (1983) Fitting the Big Blue Bump with a
power-law plus an accretion disk model using
three temperature zones
21Quasar Spectral Energy Distributions (SEDs)
- Very nice and relatively brief review article
from Quasars and Cosmology conference by
Belinda Wilkes (CfA), a world expert on the
subject - http//nedwww.ipac.caltech.edu/level5/Sept01/Wilke
s/Wilkes_contents.html - Must account for physical processes producing
prodigious luminosity from radio wavelengths
through the X-ray and even gamma ray regimes. - Particular features of interest include
radio-jets and the radio-quiet vs. radio-loud
dichotomy, the big blue bump that produces the
optical/UV energy peak and is thought to arise
from an accretion disk, and the far infrared that
represents re-radiation by hot dust.
22Quasar Spectral Energy Distributions (SEDs)
3C 273
23Orientation and Unified Models
As we have discussed, inner AGN structure
believed to feature a black hole fed by an
accretion disk. Jets may emerge along the spin
axis, and the disk illuminates BLR and NLR
clouds. A dense molecular torus exists on larger
scales and can obscure the central engine from
certain lines of sight.
From Horizons by Seeds
- Unified Models explain some of the different
classes of AGN, particularly type 1 and type 2
Seyferts, via orientation. - For specifics, see the Annual Reviews article by
Antonucci, 1993, a bishop in the Church of
Unification. - Another nice website http//www.mssl.ucl.ac.uk/ww
w_astro/agn/agn_unified.html
24Unified Models Different Views of the
Accretion Disk
- The torus of gas and dust can block part of our
view - Seyfert 2 galaxies Edge on view Only gas well
above and below disk is visible See only
slow gas ? narrow emission lines - Seyfert 1 galaxies Slightly tilted view Hot
high velocity gas close to black hole is
visible High velocities ? broad emission
lines - BL Lac objects Pole on view Looking right
down the jet at central region Extremely
bright vary on time scales of hours - Quasars Very active AGN at large
distances Can barely make out the galaxy
surrounding them Were apparently more common
in distant past
From our text Horizons, by Seeds
25Spectral differences in Seyferts
26Different Views of the Accretion Disk
- The torus of gas and dust can block part of our
view - Seyfert 2 galaxies Edge on view Only gas well
above and below disk is visible See only
slow gas ? narrow emission lines - Seyfert 1 galaxies Slightly tilted view Hot
high velocity gas close to black hole is
visible High velocities ? broad emission
lines - BL Lac objects Pole on view Looking right
down the jet at central region Extremely
bright vary on time scales of hours - Quasars Very active AGN at large
distances Can barely make out the galaxy
surrounding them Were more common in distant
past
27Radio Source Unification
- Core-dominant sources are seen jet-on, have flat
radio spectra, and are variable, optically
polarized and beamed. - Lobe-dominant sources are not very variable, have
steep radio spectra dominated by optically thin
synchrotron emission, and are not beamed
strongly. - Can measure orientation by various methods, e.g.,
LogR core/lobe radio flux at 5 GHz rest-frame
(Orr Browne 1982), also Rv which normalizes
core flux with an optical magnitude (Wills and
Brotherton 1995).
28Radio Source Unification
Core dominant
Lobe dominant
- From Wills and Brotherton (1995), plotting Log R
(which is rest-frame 5 GHz) core to lobe flux
ratio), vs. the jet angle to the line of sight
where the jet angle is estimated from VLBI
superluminal motion.
29What makes an AGN active?
- Need a supply of gas to feed to the black hole
- (Black holes from 1 million to gt1 billion solar
masses! - Scales as a few percent of galaxy bulge mass.)
-
- Collisions disturb regular orbits of stars and
gas clouds - Could feed more gas to the central region
- Galactic orbits were less organized as galaxies
were forming, also recall the hierarchical
galaxy formation - Expect more gas to flow to central region when
galaxies are young gt Quasars (quasar epoch
around z2 to z3) - Most galaxies may have massive black holes in
them - They are just less active now because gas supply
is less
30The AGN Zoo
- Quasars (M lt -23)
- Radio-Loud
- FR II Radio Galaxies (type 2 quasars)
- Radio-loud Quasars or just Quasars (type 1
quasars) - Optically violent variables (OVVs)
- Radio-Quiet
- QSOs type 1 (broad lines) and type 2 (only
narrow lines) - Infrared-Loud IRAS quasars, Far-IR Galaxies,
ULIRGs - Low Luminosity AGNs (M gt -23)
- Radio-Loud
- FR I Radio Galaxies
- Bl Lac objects, AKA Blazars
- Radio-Quiet
- Seyfert Galaxies type 1 through type 2 (see
QSOs) - LINERs (Low ionization nuclear emission-line
regions) - Shields A Brief History of AGN astro-ph/9903401
31Surveys/Catalogs
- SEDs immediately show AGNs dont look like stars
- Selection by optical colors works (e.g., Sloan is
best, http//www.sdss.org, also 2dF
http//www.2dfquasar.org ) - Mutliwavelength works (e.g., radio, X-ray, IR,
plus optical) - E.g., FIRST Bright Quasar Survey
- Also possible to find via
- Variability (e.g., MACHO)
- Proper Motion (lack thereof)
- Grism Surveys (e.g., Large Bright Quasar Survey)
- Older compilation catalogs like that of
Veron-Cetty and Veron (2000) are being surpassed
by SDSS and 2dF. http//www.obs-hp.fr/www/catalogu
es/veron2_9/veron2_9.html - Hewett Foltz (1994) on Quasar Surveys
http//nedwww.ipac.caltech.edu/level5/Hewett/frame
s.html - My NSF proposal focuses on physical samples.
32AGN Emission Lines
- Hagai Netzers section in Saas-Fee Advanced
Courses 20, 1990, available online - http//nedwww.ipac.caltech.edu/level5/March02/Netz
er/Netzer_contents.html - Classic textbook on photoionization is AGN2 by
Don Osterbrock, popular public tool is CLOUDY by
Gary Ferland (http//thunder.pa.uky.edu/cloudy/
). Section 9.1.2 in Combes et al.
Basically, treat ionization state,
heating/cooling balance, and relate emission line
ratios to metallicity, density, ionizing
continuum, etc. Note LOC models (Baldwin et
al. 1996).
33AGN Emission Lines
From Netzer et al. 1994 (I did the figures), on
the SED and unusual emission line profiles of the
OVV 3C 279. Note the steep power-law spectrum.
Optically polarization is high. There is optical
beamed synchrotron radiation in this source. In
many quasars, the emission line profiles are
similar from line to line (consistent with
optically thick BLR clouds). Not so for all
objects, and especially important for figuring
out BLR kinematics and dynamics (which is still
not so clear).
34Quasar Host Galaxies
- Hard to see. Why?
- How can you do it?
- HST (Bahcall, others)
- Near Infrared (eg., McLeod et al. 1996)
- AOsort of. Issues here.
- What are their properties? Are they related in
any way to the activity? - Very little known before advent of HST, AO, and
large near-IR detectors. Still a challenging
type of observation. - Initially thought (based on Seyfert galaxies and
radio galaxies) that radio properties were
related to host type. Seems to have been a
selection effect.
35Quasar Images II
36Quasar Images III Starburst-Quasar
From Brotherton et al. (1999).
37Ties to Host Galaxy Evolution
- Quasar, star-formation evolution (from Boyle and
Terlevich 1998)
38Ties to Host Galaxy Evolution
- Central black hole masses seem to correlate with
host galaxy magnitude (from McLure and Dunlop
2001)
39Ties to Host Galaxy Evolution
- Central black hole masses best correlate with
host galaxy stellar velocity distribution (from
Ferrarese 2000)
Reverberation mapping yields AGN black hole
masses. A good recent review is by Peterson.
More slides on this ahead! http//nedwww.ipac.cal
tech.edu/level5/Sept01/Peterson2/Peter_contents.ht
ml
40Taking a step back to fundamentalsArguments for
Black Holes in AGNs
- Energy Considerations
- Nuclear luminosities in excess of 1013 suns
- Gravitational release capable of converting on
order 10 rest mass to energy - Rapid Variability
- Timescales lt 1 day imply very small source
- Radio Jet Stability implies large, stable mass
with large angular momentum
41Measuring Black Hole Masses in Nearby Galaxies
- SgrA in the Milky Way
- Water Masers in NGC 4258, a few others
- Spatially Resolved Gas or Stellar Dynamics Using
the Hubble Space Telescope (HST)
42Max Planck Institutes Galactic Core Group
This plot shows the quantitative limits.
43Water Masers in NGC 4258
- Based on Greenhill et al. (1995)
- Warped Disk Model
- Radial Velocities and Proper Motions Measure a
Mass of 4x107 solar masses (20 times more massive
than SgrA)
44Spatially Resolved Spectroscopy from Space Shows
BH Signatures
- HST STIS shows evidence for a super massive black
hole in M84 based on spatially resolved gas
dynamics (Bower et al 1997). Can also be done by
examining spatially resolved stellar absorption
line profiles, plus complex 3D orbital modeling.
45The M-sigma Relation
- Black Hole Masses are about 0.1 of the central
galactic bulge mass (a big surprise to theorists)
and tightest correlation is with the stellar
velocity dispersion (after Gebhardt et al. 2000).
46Virial Mass Estimates
- M f (r ?V2 / G)
- r scale length of region
- ?V is the velocity dispersion
- f is a factor of order unity dependent upon
geometry and kinematics - Estimates therefore require size scales and
velocities, and verification to avoid pitfalls
(eg. radiative acceleration).
47Potential Virial AGN Mass Estimators
- Source Radius
- X-ray Fe Ka 3-10 Rs
- Broad-Line Region 600 Rs
- Megamasers 4x104 Rs
- Gas Dynamics 8x105 Rs
- Stellar Dynamics 106 Rs
- Where Schwarzschild radius Rs 2GM/c2 3x1013
M8 cm
48Reverberation Mapping (RM)
Kaspi et al. (2000) studied bright PG quasars,
particularly Hß, finding that R32.9(?L?5100/1044
erg s-1)0.7 lt-days For the Hß emitting gas.
- Broad lines are photoionized by the central
continuum, which varies. The line flux follows
the continuum with a time lag t which is set by
the size of the broad-line emitting region and
the speed of light. Recombination timescales are
very short, BLR stable, and continuum source
small and central.
49Does the BLR obey the Virial Theorem?
- Four well studied AGNs, RM of multiple emission
lines shows the expected relationship (slope
-2) between time lags and velocities (note each
of the three will have different central black
hole masses). - NGC7469 8.4x106 M
- NGC3783 8.7x106 M
- NGC5548 5.9x107 M
- 3C 390.3 3.2x108 M
Onken Peterson (2002)
50Does the BLR obey the Virial Theorem?
- RM-derived masses follow the same M-sigma
relationship as seen for normal galaxies that
have black hole masses measured from HST
spatially resolved gas or stellar dynamics. - Not more points since obtaining sigma for AGN is
difficult (the AGN dilutes the stellar absorption
line EWs). - Good to 0.5 dex
Ferrarese et al. (2001)
51Expect that BLR Scales With Luminosity
- Photoionization and LOC Models (Baldwin et al.
1996) suggests that strong selection effects make
line emission come from same physical conditions
(same U, n) - U Q(H)/4pR2nHc L/nHR2
- So, for same U, nH, then expect that
- R L0.5
- How about in reality?
52Empirically BLR Scales With Luminosity
- Mentioned previously the Kaspi et al. (2000)
result how R L0.7 (above). In China, Misty
Bentz of OSU showed that proper correction for
host galaxy leads to a slope of 0.5! Nice work.
This permits the possibility of using
single-epoch measurements to estimate black hole
masses much easier!
53Vestergaard (2002)
- Single epoch FWHM vs. rms FWHM for Hß
- Single epoch L vs. mean L
54Vestergaard (2002)
- Single epoch BH Mass vs. RM BH mass
55Vestergaard (2002)
- Extend Calibration to UV Line CIV ?1549
- This is a calibrated C IV Black Hole Mass not
wholly independent should be tested at high-z,
high-L
56Brotherton Scoggins (2004)
- Hß and C IV Black Hole Mass Comparison
- All high-z sources very luminous, massive, high
L/Ledd. Please excuse the color code.
57Brotherton Scoggins (2004)
- Hß and C IV Black Hole Mass Comparison
- All high-z sources very luminous, massive, high
L/Ledd. Please excuse the color code.
58Using O III FWHM as a Proxy for s
59From Peterson (2002)
60Current/future Work Real Astrophysics
- Black Hole Demographics (growth with z)
- Is all growth as AGN? Does that produce the mass
seen in relic black holes at low z? - How does the M-sigma correlation arise?
- That is, how is black hole growth linked to the
growth of galaxy bulges and star formation? - How do AGN behave as a function of mass, L/Ledd,
viewing angle, etc.?
61Quasar Absorption Lines
- Intrinsic
- Broad (BALs)
- Narrow (NALs)
- Intervening
- Galactic
- Lyman alpha
- Metal line systems
62BALQSOs What are they?
- Are they normal quasars with equatorial winds,
seen edge-on? - Or are they an evolutionary phase?
The AGN H-R Diagram, after Miller 1998
63Radio-Loud BALQSOs
- Originally exclusively radio-quiet, but the first
radio-loud BALQSOs found by Becker et al. 1997
and Brotherton et al. 1998. From Becker et al.
(2000), 90 of the radio-selected BALQSOs are
compact in FIRST maps (vs. 60 in the non-BAL
sample), and BOTH steep and flat radio spectra
are present. - Seems to rule out simple orientation schemes,
right?
64Radio-Loud BALQSOs
- BALQSO Spectra from Brotherton et al. 1998.
65Another look at the AGN model
- Not to scale!
- Probably updated from clouds to flows
- Ill look for more recent pictures