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(1) High overall luminosities<br />

Milky Way<br />

Radio galaxies<br />

Seyfert galaxies<br />

Quasars (3C 273)<br />

X-ray<br />

luminosity<br />

1<br />

100-5,000<br />

300-7×10 4<br />

2.5×10 6<br />

Optical<br />

luminosity<br />

1<br />

2<br />

2<br />

250<br />

Radio<br />

luminosity<br />

1<br />

2,000-2×10 6<br />

20-2×10 6<br />

6×10 6


Bright extragalactic radio sources


Normal galaxies<br />

Optical X-ray<br />

Quasar PKS 1127-145


(2) Non-thermal radiation<br />

Normal galaxies<br />

Blackbody radiation with peak<br />

energy at optical wavelength<br />

Radiation mainly comes from<br />

stars inside galaxies<br />

Active galaxies<br />

Non-stellar radiation<br />

Thermal (infrared) radiation +<br />

non-thermal radiation, with<br />

peak energy at far-infrared<br />

wavelength


(3) Unusual structure<br />

Bright nucleus, jets and irregular appearance


(5) Strong emission lines and polarized<br />

emission


Statistics of Active Galaxies<br />

Only 2% of all galaxies are active galaxies,<br />

bright active galaxies are more common at<br />

greater distances.<br />

Most active galaxies are ellipticals.<br />

The high luminosities of active galaxies<br />

implies a short lifetime, so active galaxies<br />

must represent a passing stage in the<br />

evolution of normal galaxies, rather than form<br />

a separate class of galaxies.


2. Radio Galaxies<br />

Active galaxies that emit most of their energy in the<br />

radio portion of the electromagnetic spectrum.<br />

Historical perspective<br />

In 1960s, British radio astronomers finished<br />

compiling the 3rd Cambridge (3C) catalog of radio<br />

sources.<br />

Many bright radio sources in the catalog were found<br />

to have optical counterparts (galaxies).<br />

They are both point-like and extended, and are<br />

called radio galaxies.


Cygnus A with two-lobe structure


(1) Characteristics<br />

Most active galaxies are radio galaxies.<br />

Radio luminosities ( ~10 42 -10 45 ergs -1 ) much<br />

higher than those of normal galaxies ( ~10 37 -<br />

10 39 ergs -1 ).<br />

Non-thermal synchrotron radiation.<br />

Most of them are elliptical galaxies, usually<br />

the brightest, largest ones in galaxy clusters.


Appearance<br />

Core-halo type: the radio<br />

images are comparable or<br />

slightly smaller than their<br />

optical images; most of the<br />

radio emission comes form<br />

the nucleus.<br />

Double-lobe type: extended<br />

structure (as long as 1 Mpc);<br />

the radio energy is released<br />

from the radio lobes.<br />

M86<br />

Centaurus A


M87<br />

The giant elliptical galaxy in Virgo cluster.<br />

The first galaxy found to have jets.<br />

The jet is about 2 kpc long and is made up of a series<br />

of distinct “blobs”.


NGC 1265: Head-Tail Radio galaxy


0313-192: The Wrong Spiral Galaxy


(2) Theoretical Model<br />

Energy is fired out from<br />

the nucleus in the form<br />

of narrow, high-speed<br />

jets that travel into the<br />

intergalactic medium<br />

and become extended<br />

lobes.<br />

Radio emission is<br />

produced by highspeed<br />

electrons in<br />

magnetic fields through<br />

synchrotron radiation.


Movement of radio galaxies causes different<br />

appearance.


The system may appear to us as either a lobe or a<br />

core–halo radio galaxy, depending on our location<br />

with respect to the jets and lobes.


Comparison: Seyfert Galaxies and Star Burst<br />

Galaxies<br />

Seyfert galaxy<br />

NGC 7742<br />

Starburst Galaxy M94


In type II, all allowed and forbidden lines are similar<br />

and narrower (≤10 3 kms -1 ) .<br />

Seyfert I<br />

Seyfert II


The reason for this difference is thought to be that the<br />

allowed lines are formed in denser gas near the<br />

nucleus (broad line region), and the forbidden lines in<br />

more diffuse gas further out (narrow line region).<br />

In type II Seyfert galaxies the denser gas is missing<br />

or obscured.


The activity of some Seyfert galaxies may result from<br />

galaxy interactions.<br />

Visible-light (left) and radio (right) image of galaxy pair:<br />

Radio image shows gas streaming between galaxies.


Non-thermal continuum with very weak or no<br />

emission lines.


Most energy emitted in γ-ray, with strong radio<br />

and infrared radiation.<br />

Usually elliptical galaxies.<br />

3C 279


Rapid and violent variability within days to<br />

months.


5. Quasars, QSOs<br />

Optically appear almost<br />

as point sources.<br />

Quasars – quasi-stellar<br />

radio sources<br />

QSOs – quasi-stellar<br />

objects.


The first quasar 3C273 with very strong,<br />

wide, unknown emission lines<br />

In 1963 Maarten Schmidt interpreted<br />

the optical emission lines of 3C273 as<br />

hydrogen Balmer lines redshifted by<br />

16%.<br />

Maarten Schmidt<br />

HST+VLA


High-z Quasars Discovered in Sloan Digital Sky Survey


The Most Distant X-Ray Jet from Quasar<br />

GB1508+5714


Quasar Absorption Lines<br />

In addition to their own strongly redshifted spectra, many<br />

quasars also show additional “forest” of absorption lines<br />

starting at the wavelength of the quasar’s own Lyman-alpha<br />

emission line and extending to shorter wavelengths.<br />

These lines are interpreted as Lyman-alpha absorption features<br />

produced by gas clouds in foreground structures (galaxies,<br />

clusters, and so on) along the line of sight.<br />

Lyman-Alpha Forest in the spectrum of quasar QSO 1422 + 2309


Observational Features of Gravitational Lensing<br />

The lensing tends to amplify the light of the quasar,<br />

making it easier to observe.<br />

There is a time delay, ranging from several days to<br />

several years, between different images.<br />

Microlensing — lensing by individual stars in the<br />

foreground galaxy — can cause large fluctuations in<br />

a quasar’s brightness.


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4GM<br />

2<br />

bc<br />

! ( " $ # )<br />

=<br />

D D<br />

S LS<br />

% = $<br />

D<br />

LS # " ! DL"<br />

DS<br />

For = 0,<br />

! =<br />

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4GM DLS<br />

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Time Delay in Lensing Images of Quasar RX<br />

J0911.4+0511<br />

Differences in the variation<br />

in each separate image<br />

can be used to tell<br />

information about the<br />

gravity and the expansion<br />

of the universe.


Abell 1835 IR1916, The Farthest Known<br />

Galaxy with a Redshift of 10


Dark Matter in Distant Galaxy Groups Mapped<br />

for the First Time


Implications from X-ray binaries<br />

Black hole accretion jets


RX J1242-11


Evidence of the Dust Torus<br />

Hydroxyl (OH) line emissions trace the obscuring material within<br />

the circumnuclear environment of the galaxy Markarian 231.


Super Massive Black Holes in Galactic Nuclei

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