28. active galaxies goals goals: 1. describe and characterize the various types of galaxies that...

28. Active Galaxies28. Active GalaxiesGoalsGoals:1. Describe and characterize the various

types of galaxies that display high activity relative to “normal” (non-active) galaxies.

2. Examine the unified model used to explain the origin of activity in active galaxies and describe its features.

3. Discuss the nature of radio lobes and jets and how they are used to probe the universe.

Observations of Active Galaxies:The first indication that not all galaxies were quiescent conglomerations of stars with gas and dust mixed in was made by Fath in 1908 when he was examining spectra of spiral nebulae visually with a spectroscope. The galaxy NGC 1068 displayed a few bright emission lines rather than the expected stellar absorption-line spectrum.

Seyfert GalaxiesHubble later recorded emission line spectra for two other galaxies in 1926, but it was Carl Seyfert who was able to characterize the phenomenon when he noticed that a small percentage of galaxies have very bright nuclei that are sources of broad emission lines. Today they are designated as Seyfert galaxies, with further spectroscopic subdivision into Seyfert 1 and Seyfert 2, with Seyfert 1s displaying broad emission lines (permitted) and narrower forbidden lines, and Seyfert 2s displaying only narrow lines (permitted and forbidden).

The spectrum of Markarian 509, aSeyfert 1 galaxy.

Spectra of Seyfert 1 and Seyfert 2 galaxies (left) are compared with the spectra of a normal galaxy (top right) and that for BL Lacertae (bottom right).

Intermediate types (Seyfert 1.5) are also recognized, and the spectroscopic characteristics can be temporally variable. Seyfert 1 galaxies are frequently X-ray sources, Seyfert 2 galaxies less so, with huge column densities of hydrogen accounting for the difference for the latter.

About 90% of Seyfert galaxies are spirals.

Flux Distributions in Active Galactic NucleiThe spectral energydistribution (SED)of the Seyfert 1galaxy NGC 3783(Alloin et al. 1995)from radio togamma-rays. Alsoshown is the SEDfor a normal (typeSbc) galaxy from Elvis et al. (1994).The flux scale of thenormal galaxy spectrum has been adjusted to give the correct relative contribution of the AGN component and starlight for NGC 3783 (in mid-1992) at 5125 Å through a 5" 10" spectrograph aperture.

The spectra of ActiveGalactic Nuclei (AGNe)tend to be fairly flat,so they were initiallydescribed by fluxdistributions of thetype:

where α 1. TypicalSEDs contain a BigBlue Bump as wellas a smaller Infrared (IR)bump.

See typical SEDs atright.

F

Big Blue BumpIR Bump

A pure power-lawspectrum with αconstant is thesignature ofsynchrotronradiation:

where α 1.

An inverse Compton spectrum issimilar, but with differentbreaks.

F

Radio GalaxiesRadio astronomy is a relatively new area of astronomy that began following World War 2 with the availability of radio dishes, originally used for radar, in countries like The Netherlands (Holland), the United Kingdom, Australia, Canada, and the U.S.A. Radio sources had been detected prior to and during the war, but it was not until after that it was possible to begin the science in earnest. Radio surveys of the sky at various frequencies were done at places like Cambridge University (the various Cambridge catalogues), and the detection of the postulated 21-cm radiation from neutral hydrogen gas in the Galaxy was used by astronomers in Australia and Britain to map the spiral structure of the Milky Way. Early radio maps were of low resolution, so it was rarely possible to identify prominent radio sources with objects in the optical sky. The exceptions were sources in the ecliptic band that were regularly occulted by the Moon. Such events enabled precise positions to be established.

One of the first radio galaxies identified with an optical object was Cygnus A, a peculiar cD galaxy crossed by a ring of dust with two mammoth ejected radio lobes.

F

Radio galaxies can also be classified into subgroups: broad-line radio galaxies (BLRGs), like Seyfert 1s, and narrow-line radio galaxies (NLRGs), like Seyfert 2s. Optically, BLRGs have bright starlike nuclei surrounded by hazy envelopes, while NLRGs are giant or supergiant ellipticals (cd, D, and E) like Cygnus A. But Seyfert galaxies are relatively quiet at radio wavelengths, compared with radio galaxies.

Radio Lobes and JetsDouble-lobed structures and jets are fairly common among radio galaxies. Some have rather enormous dimensions. Where double jets are observed with one stronger and the other weaker, the stronger jet is probably directed more towards us than is the weaker. Solitary jets are believed to be double with the weaker counterjet too weak to be detected.

Examples.

The unusual radio galaxy NGC 1265.

The twin radio galaxies 3C 75 with their radio lobes (blue) and optical appearance (red).

M87 (NGC 4486) at optical wavelengths, deep and shallow exposures.

Jet

Wu & Tremaine (2006) estimate a mass of 2.4 1012 M (2 trillion solar masses ~ 10 Milky Way galaxies) within 32 kpc of M87 according to its globular cluster system.

Note the jet of high-speed particles emanating from the nucleus of M87.

Hubble Space Telescope view of the jet in M87.

The M87 jet at radio wavelengths.

Centaurus A radio source

3C 236 is one of the largest radio galaxies in terms of size. It has a redshift of z = 0.0988 and radio lobes extending to 40 arcmin (larger than the Moon’s apparent size), corresponding to 2 Mpc or more.

Many radio galaxies have jets of high-speed gas

ejected symmetrically

about the centre of the galaxy, well away from the optical galaxy.

Many such galaxies are referred to as

having active galactic nuclei, and

are termed AGN galaxies.

Quasars and QSOsTwo radio sources with precise locations derived in the late 1950s via lunar occultations were 3C 48 and 3C 273, where “3C” denotes the Third Cambridge Catalogue.

The spectrum of 3C 273 obtained by Maarten Schmidt revealed an emission-line spectrum that corresponded partly with the hydrogen Balmer lines redshifted by z = 0.158.

3C 48 proved to be even more unusual, appearing starlike on deep images, yet also displaying an emission-line spectrum with a large redshift, in this case of z = 0.367.

Such radio sources were classified as quasi-stellar radio sources, or QSRs, and became known as quasars. Studies later revealed that quasars had significant ultraviolet excesses (U−B < −0.4), undoubtedly because of emission lines in their spectra redshifted from the ultraviolet into the optical region of the spectrum. Following that discovery, searches for additional QSRs were made optically by searching for high-latitude stars with ultraviolet excesses. Many such objects were found, and also proved spectroscopically to be quasars, but without strong radio emission: radio-quiet quasars. They were referred to as quasi-stellar objects, or QSOs. Today both types, QSRs and QSOs, are referred to collectively as quasars. Spectroscopically, quasars are similar to broad-line radio galaxies and Seyfert 1 galaxies, but with large redshifts implying large distances.Chip Arp has published papers claiming connections of some quasars with nearby galaxies, but the evidence is open to interpretation.

Examples of (left) quasars = quasi-stellar radio sources (i.e., lots of radio noise) and (right) QSOs = quasi-stellar

objects (very little radio noise, if any).

Double QSO 0957+561

The Sloan Digital Sky Survey (SDSS) has catalogued some 46,420 quasars, some at extremely large implied distances. For example, SDSS 023137.65−07286 54.4 has a redshift of z = 5.4135, implying a recessional velocity of 0.95c. Note that the dimensions of the universe depend critically upon look-back time given the constant expansion occurring, i.e.:

Therefore:

So the universe is presently 6.4135 times larger than it was when the light from SDSS 023137.65−07286 54.4 was emitted.

emitted

emittedobs

emitted

emittedobs

R

RRz

zR

R1

emitted

obs

Evidence for Quasar Evolution... can be found when one compares the luminosities derived for quasars at different redshifts, which represent different epochs of the past. For example, intrinsically bright quasars were more common at earlier epochs than in the present era.

Statistical studies indicate that there are more than 1000 times as many quasars per Mpc3 (for a comoving space density) brighter than MB = −25.9 at z = 2 than today at z = 0. Yet the total number of quasars does not appear to have changed significantly between the present and the past epoch at z = 2. But changes are apparent in more distant epochs, z > 3, and it appears possible to study the birth and evolution of quasars in the early stages of the universe. That is the field of observational cosmology.

Like AGNe, quasars are believed to be powered by a supermassive black hole lying at the centre of a galaxy.

Quasar and AGN VariabilityA surprise from the initial studies of both quasars and AGNe was that both types of objects are light variable on fairly short time scales. The light curves below are from the Magellanic Quasars Survey, a study of QSOs near the LMC and SMC. X-ray fluctuations are the most rapid.

Spectroscopiccharacterization ofquasars in the MQS.

Properties of quasars in the MQS according to their measured magnitudes and redshifts.

BL Lacertae ObjectsBL Lacertae, as the name implies, is a starlike object originally included in the General Catalogue of Variable Stars because it displayed light variability. The spectrum of the star was difficult to classify, since it displayed few features on an almost featureless continuum.

It was Oke and Gunn (1974, ApJ, 189, L5) who were first able to record the faint spectrum from the object with the bright central regions obscured by an occlusion disk. The annulus spectrum for BL Lac displayed a few absorption lines redshifted by z = 0.07, implying quasarlike properties. Thereafter the object was considered to be a quasar with the main optical jet directly pointing towards the observer, producing the featureless continuum of synchrotron radiation with a power law spectrum of α = −1.55. Many other such objects have since been detected, and are sometimes referred to as Blazers.

Oke and Gunn’s resultsfor BL Lac. The annulus spectrumoriginates from thosegalaxy portions notobscured by the jet.It appears to be thespectrum of a quasaralthough without much emission.

LINERsA final class of objects consists of galaxies with low luminosity nuclei displaying low ionization (i.e., forbidden lines) nuclear emission-line regions (LINERs). LINERs are similar to Seyfert 2 galaxies, but it is not clear that they represent the low luminosity tail of Seyferts. Forbidden-line radiation is also seen in starburst galaxies and H II regions, for example.

A summary of theAGN menagerieis given in Table28.1 of the text.

Unified Model of AGNe

So a rough sketch of the unified model for AGNe consists of a central engine comprising an accretion disk orbiting a rotating, supermassive black hole. The AGN is powered by the conversion of gravitational potential energy into synchrotron radiation, although the rotational kinetic energy of the black hole may also serve as an important energy source. The structure of the accretion disk depends upon on the ratio of the accretion luminosity to the Eddington limit (the most rapid rate that energy can escape into space without leading to mass loss). To supply the observed luminosities, the most energetic AGNe must accrete between ~1 and 10 M yr−1. The perspective of the observer, together with the mass accretion rate and mass of the black hole, largely determines whether the AGN is called a Seyfert 1, a Seyfert 2, a BLRG, a NLRG, or a radio-loud or radio-quiet quasar.

Perspectives of Radio Lobes and JetsJets are generated by chargedparticles ejected from thecentral nucleus of an AGN.How they are seen from Earthdepends upon a variety offactors, including perspective.The calculations in Fig. 28.36are intended to explain ourview of the Einstein ringMG1131+0456 seen inFig. 28.37. A simplifiedpicture was first generatedby Dyer and Roeder in 1981.

A plexiglass simulation of a gravitational lens created by Charles Dyer and Robert Roeder (1981).

Double quasar, QSO 0957+561. The image of a single background quasar split into two halves by an

intervening galaxy.

An image of the galaxy ZW 2237+030, Huchra’s Lens, showing the multiple imaging of a background quasar

QSO 2237+0305.

Gravitational lensing in the galaxy cluster Abell 370.

A close-up view.

Superluminal VelocitiesThe most compelling argument for relativistic speeds in jets and radio lobes for galaxies involves radio observations of material ejected from the cores of several AGNe with so-called superluminal velocities. The effect is observed within ~100 pc of the AGN’s centre and probably continues further out. The perspective of the knot motion and observer is important for rseolving such situations.

Apparent motion of some galactic jets at speeds exceeding the

speed of light are projection effects only. The jets also have motion in the line of sight that produces such an

anomaly.

A photon is emitted in the line of sight at t = 0 when the source distance is d. A photon is later emitted at time te when the distance to Earth is d – vte cos .

The first photon reaches Earth at time t1, where:

The second photon arrives at Earth at time t2, where:

The time on Earth between reception of the photons is:

which is shorter than te. The apparent transverse velocity measured on Earth is:

c

dt 1

c

vtdtt ee

cos2

cos112 c

vtttt e

cos1

sinsinapp

cvv

t

vtv e

The solution for v/c is:

It can be shown that v/c < 1 for angles such that:

The smallest possible value of v/c is:

for:

cos/sin

/

app

app

cv

cv

c

v

1cos1/

1/22

app

22app

cv

cv

22app

22appmin

/1

/

cv

cv

c

v

c

vappmincot

Relativistic Beaming

The geometry for a gravitational lens. Light from the source, S, passes within a distance of approximately r0 of a lensing point mass at L on its way to an observer at O. The angles involved are actually just a fraction of a degree, and so r0 is very nearly the distance of closest approach.

Outside a spherical object of mass M the coordinate speed of light in the radial direction is (Eq. 17.28:

The effective “index of refraction” is:

The angular deviation of a photon passing a distance r0 from mass M is given by (Problem 17.6):

See section 28.4 of textbook.

2

21

rc

GMc

dt

dr

2

1

2

21

21

/ rc

GM

rc

GM

dtdr

cn

radian4

20cr

GM

Gravitational Lenses and Time DelaysHow different components of a lensed background object can appear to change in brightness with time, given that the path lengths in the two cases are different.

By 1996 the time delay had been measured in 4 quasars, giving values for the Hubble constant of H0 = 63 ±12 km/s/Mpc, H0 = 42 km/s/Mpc, although another analysis of the same data gave H0 = 60 ±17 km/s/Mpc, H0 = 52 ±11 km/s/Mpc, H0 = 63 ±15 km/s/Mpc, and H0 = 71 ±20 km/s/Mpc. All values are similar to what is implied from galaxy redshifts.

The double quasar, QSO 0957+561, shown again.

Spectra for the two components of the double quasar, QSO 0957+561, showing that the two images are from the same source. Note the Lyman-α forest in the spectra.

Lyman-alpha Forest

The more usual form of gravitational lensing by a rich cluster of galaxies.

Sample QuestionsSample Questions1. The radio galaxy Centaurus A has redshift z = 0.00157. The monochromatic flux of Cen A is Fν = 912 Jy at a frequency of 1400 MHz. Use its observed spectral index of α = 0.6 to estimate the radio luminosity of Cen A (see Example 28.1.1).

Answer: The distance to Cen A can be evaluated using:

The monochromatic flux of Cen A at 1400 MHz is:

So:

The radio luminosity can be found by integrating the monochromatic flux over the range of radio frequencies indicated by Table 3.1 of the textbook, namely from ν1 = 107 Hz to ν2 = 3 109 Hz. The power law behaviour does not continue to ν = 0, and a power law function is simple to integrate. Thus:

The Solution Book gets 2 1034 W using a Hubble constant of H0 = 71 km/s/Mpc.

Note that the solution is about 63 million times larger than the Sun’s luminosity.

2. A rough idea of how the population of quasars might have differed in the past can be learned by mathematical modeling of the dimming of quasars as they age. Consider the case where the total number of quasars has been constant from z = 2.2, and suppose that the average luminosity L of a quasar of redshift z has the form:

where L0 is the luminosity for z = 0 (today). Use Fig. 28.16 to estimate the value of the constant α. According to your answer, how much more luminous is an average quasar at z = 2 than at z = 0?Answer. Choose two points in Fig. 28.16 representing the least luminous quasars at z = 2.2 and z = 0.3. The values L1 2 1039 W at z1 = 2.2 and L2 1038 W at z2 = 0.3. So:

and

Solving for α we obtain:

Or:

Solving for α gives:

So:

The average quasar at z = 2 is about 38 times more luminous than a quasar at z = 0.

3. Estimate the effective index of refraction for light passing within 104 pc of a spherical cluster of galaxies having a total mass of 1014 M.Answer. Recall the equation for the effective “index of refraction” given in The Geometry of Gravitational Lensing section of Chapter 28:

Here M = 1014 M and r = 104 pc. Inserting the values and normalizing the units gives:

2

1

2

21

21

/ rc

GM

rc

GM

dtdr

cn

000958.1105713.91107732.2

106544.21

109979.2100857.310

10989.110106726.621

21

14

1

37

34

1

28164

3014111

2

rc

GMn