acceleration in active galactic nuclei i

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Acceleration in Active Galactic Nuclei I Overview of AGN Roger Blandford KIPAC Stanford

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Page 1: Acceleration in Active Galactic Nuclei I

Acceleration in Active Galactic Nuclei I

Overview of AGN

Roger BlandfordKIPAC

Stanford

Page 2: Acceleration in Active Galactic Nuclei I

Brief History

Fath 1918- M87 JetReber 1939 - Cygnus ASeyfert 1943 – Active Galactic NucleiJennison, Das Gupta 1953 – Double Radio SourcesBaade, Minkowski 1954 - Elliptical GalaxiesSchmidt 1963 – QuasarsKerr 1963 – Black Hole MetricVLBI 1969 – Superluminal ExpansionRees 1971 – JetsEGRET 1991 – Gamma rays

Aug 11 08 SSI08 Cosmic Accelerators I 2

Page 3: Acceleration in Active Galactic Nuclei I

For Particle PhysicistsAGN (and galaxies) are more like people than particles• Properties historical not quantum numbersAGN astrophysics is mostly inductive not deductive• Hard to calculate implications of fundamental modelAGN studies have been led/limited by observations• GLAST should make and stimulate many discoveries

Aug 11 08 SSI08 Cosmic Accelerators I 3

Page 4: Acceleration in Active Galactic Nuclei I

Anatomy

DiskWindHoleJet

Aug 11 08 SSI08 Cosmic Accelerators I 4

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08 vii 25 IOA 5

AGN

10-8 < L/L* < 104

AGN

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Aug 11 08 SSI08 Cosmic Accelerators I 6

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Physiology

Black HolesAccretion ModesOutflows MechanismsJet formationSuperluminal MotionJet CollimationEnvironmental Impact

Aug 11 08 SSI08 Cosmic Accelerators I 7

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08 vi 29 KIAA 8

(T “Standard Model of AGN”Million to Billion solar mass spinning black holes• In most normal galaxies

Mass supplied through accretion disk• Angular momentum ~ r1/2

Unification Models• Orientation very important

- Beaming – radio and γ-ray jets- Obscuration – Seyferts and keV X-rays

Grand Unification/Central Dogma• Major physical (not orientation) properties of AGN depend upon:

- M’S/M’E; (M’E =4πGMmp/σTc); “Passive” black hole- α = Ωm; (0 < α < 0.5); “Active” black hole

• Mass M provides a scale for size for length, time, power (temperature)- Stellar black holes

Page 9: Acceleration in Active Galactic Nuclei I

08 vi 29 KIAA 9

Intermediate Mass Supply

Thin, cold, steady, slow, radiative diskSpecific energy e = -Ωl/2

G − ′ M l = const ≈ 0dLdr

=d(ΩG − ′ M e)

dr≈ 3 ′ M de

drG

Energy radiated is 3 x the local energy loss

Page 10: Acceleration in Active Galactic Nuclei I

08 vi 29 KIAA 10

Low, High Mass Supply

M’<<M’E, tenuous flow cannot heat electrons and cannot coolM’>>M’E, dense flow traps photons and cannot cool Thick, hot, steady, slow, adiabatic diskBernoulli function: b =e+h

G − ′ M l ≈ 0ΩG − ′ M b ≈ 0⇒ b ≈ −2e > 0

G

Energy transported by torque unbinds gas => outflow

Galaxy black hole (Sgr A*), BALQ

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08 vi 29 KIAA 11

“Active” Black HolesSpin acts passively to increase efficiency of thin disk accretion• 6-42 percent efficiency

- Very sensitive to pressure, radiation, magnetic stress

Rotational energy associated with spinning Kerr spacetimeSpin energy can be extractedelectromagnetically from spacetime and relativistic disk B

EMF ~ ΩΦ ~ ZVPower ~ EMF2/Z0 ~1039W

UHECR!

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24 iv 07 STScI 12

Angular MomentumFluid torques• Hole spun up by accretion• Spinning holes spun up less• Retrograde holes spun up moreMagnetic torques• Magnetorotational instability• Disks can support MHD wind• Gas flung out if q > 60o• Remove energy, ang. mom., mass• Decelerate hole

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Superluminal Motion

Aug 11 08 SSI08 Cosmic Accelerators I 13

βob =β sinθ

1− β cosθ

D =1

γ(1− β cosθ)Sν ∝ IνΩ ∝ nν '3 ∝ D3+α

•Typically, γ ~ βob~θ-1 ~ 10•Doppler Beaming

•Powerful amplifier

•Observe oncoming sources•Approaching/Receding~(2γ)7 ~109!

Page 14: Acceleration in Active Galactic Nuclei I

Radio Jets

Aug 11 08 SSI08 Cosmic Accelerators I 14

•Relativistically beamed•Dominated by approaching jets

•Core – shock structure•Core is stationary, self-absorbedsynchrotron emission

•Radio photosphere•ν ∼ γ2B MHz

•r ~ λ ∼ 1018−20 cm, B ∼ 0.1G,T~1012K•Moving features is shock or wave

•Moving superluminally•Jets may be magnetic pinches

•Relativistic cores

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24 iv 07 STScI 15

Pinched JetsToroidal magnetic field B in jet frameCurrent I in rest frame• I=2πrΓB/μ0

Static equilibriumMech. ~ 3-10 EM power

dPdr

+μ0

8π 2r2ddr

⎛ ⎝ ⎜

⎞ ⎠ ⎟

2

= 0

LEM =Z0

2πdr'r'0

r∫ (1− Γ−2)1/ 2 I2

LMech = 8πc dr'r'Γ(Γ2

0

r∫ −1)1/ 2 P

X Bφ

I[r]

r

Page 16: Acceleration in Active Galactic Nuclei I

Biochemistry

Disk emissionJet emission Radiative TransferParticle Acceleration

Aug 11 08 SSI08 Cosmic Accelerators I 16

Page 17: Acceleration in Active Galactic Nuclei I

Disk emissionOptical/UV emission• Black body T ~ r-3/4

• Scattering=>GreyX-ray emission• Comptonisation by hot electrons in active corona• Second order Fermi acceleration of photons• <Δν/ν> = 4kTe/mec2

- Limited by Compton recoil around MeV

• Spectral index α(α+3)= (kTeτ(1+τ)/mec2)-1

• Slope controlled by energetics- spectrum flattens with heating

Aug 11 08 SSI08 Cosmic Accelerators I 17

Corona – X-rays

Disk - OUV

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γ-ray JetsInverse Compton scattering• r ~ 1015-17cm? ν ∼ γ2νs

Soft photons• X-rays can be S or C-1; ν ∼ γ2B MHz• Internal synchrotron (lo L?)• External disk (hi L?)

Particle acceleration• >10 TeV electrons!• One zone

- standing shock?

• TeV emission inside GeV- Particle acceleration faster at small radius

• TeV emission outside GeV- Opacity domintes: TeV + eV -> e+ + e-

Aug 11 08 SSI08 Cosmic Accelerators I 18S C-1

TeV

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Aug 11 08 SSI08 Cosmic Accelerators I 19

Some Big Questions on JetsLocation

• TeV, GeV, Radio, X-ray…

Emission Mechanisms• Leptonic vs Hadronic, Synchrotron vs Coherent

Composition• EM, pairs, ionic plasma

Velocity Field• Monolithic, vs laminar vs turbulent

Collimation• Pinch vs inertial vs pressure

Particle acceleration• Shocks vs reconnection vs stochastic…

Transport• Power, thrust, discharge, current

Origin• Black hole, relativistic accretion disk

Page 20: Acceleration in Active Galactic Nuclei I

Some References

Krolik – Active Galactic NucleiFrank, King, Raine – Accretion Power in AstrophysicsBlandford, Netzer, Woltjer – Active Galactic NucleiRector, De Young (ed) – Extragalactic Jets

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