Radio Galaxies - PowerPoint PPT Presentation

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Radio Galaxies

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models for different. ionization parameters. Broad line regions (BLR) ... No thick tori? Well known dichotomy: low vs high power radio galaxies ... – PowerPoint PPT presentation

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Title: Radio Galaxies


1
Radio Galaxies part 4
2
Apart from the radio the thin accretion disk
around the AGN produces optical, UV, X-ray
radiation
  • The optical spectrum emitted by the gas depends
    upon the abundances of different elements, local
    ionization, density and temperature.
  • Photons with energy gt 13.6 eV are absorbed by
    hydrogen atoms.
  • In the process of recombining, line photons are
    emitted and this is
  • the origin e.g. of Balmer-line spectra.
  • Collision between thermal electrons and ions
    excites the low-energy level
  • of the ions, downward transition leads to the
    emission of so-called
  • forbidden-line spectrum (possible in low
    density conditions).

3
Example of broad line radio galaxy (3C390.3)
4
  • Optical spectrum, what can we derive
  • which lines
  • flux/luminosity
  • width (kinematics)
  • ionization mechanism (line ratios)
  • density/temperature of the emitting gas
  • morphology of the ionized gas
  • (any relation with the radio?)
  • continuum and stellar population

using spectra and narrow band images
5
  • Ionization parameter
  • ratio between ionizing photon flux/gas density
  • Temperature of the emitting gas
  • Mass of the emitting gas

6
photoionization models for different ionization
parameters
Examples of diagnostic diagrams
7
  • Broad line regions (BLR)
  • typical size (from variability)
  • of 10-100 light-days (Seyferts) up to
  • few light-years (few x 0.3 pc, quasars).
  • electron density is at least 108 cm-3
  • (from the absence of broad forbidden lines)
  • typical velocities 3000-10000 km/s
  • Narrow line regions (NLR)
  • typical density 103 to 106 cm-3
  • gas velocity 300 1000 km/s
  • large range in size from 100-300 pc to tens of
    kpc

8
Powerful radio galaxies energetics
  • Radiation
  • Jets
  • Winds

Quasar luminosity1044 1047 erg s-1 Luminosity
integrated over lifetime10571062 erg
Jet power1043 1047 erg s-1 Jet power integrated
over lifetime 1057 1062 erg
Total wind power1043 1046 erg s-1 Wind power
integrated over lifetime1056 1061 erg
Starburst-induced superwinds.
9
Emission line nebulae what can we learn?
10
Emission line haloes lt1kpc scale
  • Kinematics. The emission line kinematics comprise
    a combination of gravitational motions,
    AGN-induced outflows, and AGN-induced turbulence
  • Black hole masses. Now possible to determine
    direct dynamical masses for nearby PRG using
    near-nuclear emission line kinematics
  • Feedback. The outflow component provides direct
    evidence for the AGN-induced feedback in the
    near-nuclear regions

the presence of the nuclear activity could
influence the evolution of the galaxy (e.g.
clear gas away from the nuclear regions)
11
Cygnus A viewed by HST
NICMOS 2.0mm
Optical images
12
2.0 micron image HST/NICMOS
Evidence for a super-massive black hole in Cygnus
A
13
Correlation between black hole mass and galaxy
bulge mass/luminosity
14
  • broad permitted line seen in polarized line
    only the scattered component can be seen

Broad- and narrow line radio galaxies become
undistinguishable
15
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16
Emission line nebulae 1-5kpc scale
  • Kinematics. Emission line kinematics a
    combination of AGN-induced and gravitational
    motions
  • Ionization. Gas predominantly photoionized by the
    AGN
  • Outflows. Clear evidence for emission line
    outflows in Cygnus A and some compact radio
    sources, but outflow driving mechanism uncertain

17
Example of complex kinematics
(IC5063)
700 km/s
Complex kinematics of the ionized gas in
coincidence with the radio emission this
suggests interaction between radio plasma and ISM
18
Emission lines in (powerful) radio galaxies
Wavelength (Å)
19
Diagnostic diagrams including ionization from
shocks
20
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21
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22
Emission line nebulae 5-100kpc scale
  • Kinematics.Activity-induced gas motions are
    important along the full spatial extent of the
    radio structures, regardless of the ionization
    mechanism
  • Jet-induced shocks. The shocks that boost the
    surface brightness of the structures along the
    radio axes also induce extreme kinematics
    disturbance
  • Gravitational motions. Require full spatial
    mapping of the emission line kinematics in order
    to disentangle gravitational from AGN-induced gas
    motions
  • Starbursts. Starburst-induced superwinds may also
    affect the gas kinematics out to 10s of kpc

23
Gas with very high ionization at 8 kpc from the
nucleus
Even if the nucleus is obscured by the torus, the
extended emission line regions can tell us about
the UV radiation from the nucleus.
24
Emission line clouds in the halo of CenA
CenA D3Mpc
25
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26
1000 km/s
27
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28
Contours radio Colors ionized gas
In some cases the radio galaxy seems to have a
strong effect on the medium around.
Diagnostic diagrams important to understand which
mechanism is dominant
29
Radio galaxies at high redshift
  • Morphology of the extended emission line regions
  • depends on the size of the radio source
  • Alignment between the emission lines and the
    radio axis
  • Interaction between radio and medium does this
    also trigger star formation?

30
Any difference (in the optical lines) between
low and high power radio galaxies?
31
What makes the difference?
Well known dichotomy low vs high power radio
galaxies Differences not only in the radio
WHY?
Intrinsic differences in the nuclear regions?
Accretion occurring at low rate and/or
radiative efficiency? No thick tori?
32
The central regions of low-power radio galaxies
No strong obscuration optical core very often
detected
33
From HST and X-ray
The HST observations
  • High rate of optical cores detected
  • Correlation between fluxes of
  • optical and radio cores

But so far we havent seen broad permitted lines
34
More on the host galaxy
35
The optical continuum of Radio Galaxies

Usually the old stellar population is the
dominant - as usual in elliptical galaxies - but
in some cases a young stellar population
component is observed (typical ages between 0.5
and 2 Gyr).
3C321
  • consistent with the merger
  • hypothesis for the triggering
  • of the radio activity.
  • but not a single type of merger
  • AGN appears late after the
  • merger

old stellar pop.
young stellar pop.
power law
36
3C305
3C293
3C321
Results from UV imaging
Allen et al. 2002
37
  • The young stellar component may come from
  • a recent merger
  • We can use the age of the stars to date when
    this merger
  • occurred
  • To be compared with the age of the radio source

38
Cavities created by the radio emission in the
hot (X-ray) gas
39
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40
Emission line nebulae what they can tell us
  • AGN Physics. Tests of the unified schemes, jet
    physics, black hole masses
  • Host galaxy properties. Mass distributions,
    abundances, gas masses
  • Galaxy Evolution. Clues to the assembly of
    massive galaxies at both high and low redshifts
  • Feedback. The importance of AGN-induced feedback
    effects in the evolution of the host galaxies
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