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Active Galactic Nuclei Ay 16, April 8, 2008. AGN DEFINITION PROPERTIES GRAVITATIONAL LENSES BLACK HOLES MODELS.

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Presentation on theme: "Active Galactic Nuclei Ay 16, April 8, 2008. AGN DEFINITION PROPERTIES GRAVITATIONAL LENSES BLACK HOLES MODELS."— Presentation transcript:

1 Active Galactic Nuclei Ay 16, April 8, 2008

2 AGN DEFINITION PROPERTIES GRAVITATIONAL LENSES BLACK HOLES MODELS

3 WHAT IS AN AGN? Objects that emit significant amounts of radiation from non-thermal sources (i.e. not stars or dust or thermal gas). In order of discovery: Seyfert Galaxies Radio Galaxies Quasars BL Lac Objects LINERS (Low Ionization Emission Regions)

4 Early History Carl Seyfert & strange emission line galaxies (1943) Birth of Radio Astronomy & discovery of strong sources = radio galaxies (40-50’s) Greenstein & Schmidt & QSO’s (1963) Surveys of Extremely Blue Objects (60-70’s) Surveys at other Wavelengths (70’s > )

5 SY1 AGN Spectra SY2 QSO

6 Mean UV QSO Spectrum

7 LBQSO Spectrum

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9 NGC 4151 Typical SY1

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11 Seyfert 1 galaxy and quasar spectra are dominated by broad line regions, lines often showing doppler velocities of 0.1c Seyfert 2 galaxies spectra are dominated by narrower lines, ~ 1-2000 km/s wide LINER spectra are dominated by stars plus emission lines from multiple ionization states indicative of non-thermal excitation BL Lac spectra show almost no features but strong continua

12 M87 Core In X-rays

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14 Markarian 231

15 Markarian 421 BL Lac in an E Galaxy TeV  Source

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17 BL LAC SED’s

18 Radio Galaxies M87 = Virgo A

19 M87 in the Radio (VLA)

20 M87 Central Jet

21 M87 Jet In 3 bands

22 Centaurus A Radio on Optical Image

23 Cygnus A (VLA Conway & Blanco)

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25 Synchrotron Power  = related to kinetic enegy of electron = (1 - (v/c) 2 ) -1/2 = (1 -  2 ) -1/2 where  = v/c

26 Synchrotron Spectra

27 Baldwin, Phillips & Terlevich AGN LINERS NORMAL

28 Ly Alpha Forest

29 Eddington Luminosity Largest Luminosity that can pass through a gas in hydrostatic equilibrium : Outward Force of Radiation Pressure > Inward Force of Gravity Gravity dP/dr = -  g = -GM  /r 2 Luminosity dP/dr = -(  T  /m p c) (L/4  r 2 )  T = Thomson Cross section L Edd = 4  GMm p c/  T = 3.3 x 10 4 L  (M/M  )

30 Gravitational Lensing Deflection of Light passing at a distance b by an object of mass M:  = 4GM/bc 2 Bending of light by the Sun: r = 6.96 x 10 10 cm M = 1.989 x 10 33 g  = 8.47 x 10 -6 radians = 1.74”

31 Gravitational lensing :

32 2237+0305 = Einstein’s Cross

33 Gravitational Redshift Photons lose E as the move out of a gravity well. For a photon E = hc/, “m” = E/c 2 = h/c Gravitational Potential E = -GMm/r  E = -GMh/c r  / = GM/rc 2 which generally is pretty small except for NS and BH

34 Black Holes Curvature around a point mass has a critical radius = Schwarzchild Radius Inside this is a singularity R S = 2GM/c 2 In units we know R S = 3.0 km (M/M  ) Gravitational redshift from R S = 

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36 NGC 4261 X-ray vs Optical

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38 V = 1100 km/s

39 M87’s central mass: Given the HST observations, what’s the enclosed mass?  v = 1100 km/s  ~ 1” D = 16.1 Mpc R = 0.078 kpc (78 pc) GMm/R = 1/2 mV 2 for circular orbits M = 0.5 V 2 R/G G = 4.309 x 10 -6 kpc (km/s) 2 / M  M core ~ 10 10 M 

40 Reverberation Mapping NGC5548

41 Lag ~ 20 days Size ~ 20 light days ~ 0.02 pc

42 Maggorian Relation (Nuker team) Almost every large galaxy has a central BH, and the BH mass is directly correlated with the galaxy’s total bulge mass!

43 A Unified Model of AGN’s We have come to believe that all AGN are essentially driven by the same phenomena --- a central black hole surrounded by an accretion disk, hot clouds of gas and dust. The disk is hot, 10 5 K plus. The AGN is powered by accretion onto the BH. And what you actually see is driven by the viewing angle.

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45 Unified AGN Model BH + Disk + Torus SY2 SY1 BL Lac edge on tilted down the pipe


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