Blazars and cosmic bkgs. Fabrizio Tavecchio INAF-Oss. Astron. di - - PowerPoint PPT Presentation

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Blazars and cosmic bkgs. Fabrizio Tavecchio INAF-Oss. Astron. di - - PowerPoint PPT Presentation

Blazars and cosmic bkgs. Fabrizio Tavecchio INAF-Oss. Astron. di Brera, Italy Introduction: AGNs, blazars Blazars: phenomenology Blazars: emission models Absorption of gamma-rays: backgrounds and the intergalactic B-field INTRODUCTION


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Fabrizio Tavecchio

INAF-Oss. Astron. di Brera, Italy

Blazars and cosmic bkgs.

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Introduction: AGNs, blazars Blazars: phenomenology Blazars: emission models Absorption of gamma-rays: backgrounds and the intergalactic B-field

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INTRODUCTION

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Almost all galaxies contain a massive black hole

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Almost all galaxies contain a massive black hole

e.g. Ferrarese & Ford 2004

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Almost all galaxies contain a massive black hole 99% of them is (almost) silent (e.g. our Galaxy)

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Almost all galaxies contain a massive black hole 99% of them is (almost) silent (e.g. our Galaxy) 1% per cent is active (mostly radio-quiet AGNs):

BH+accretion flow (disk): most of the emission in the UV-X-ray band

0.1% is radio loud: jets mostly visible in radio

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Powerful (FRII) Radiogalaxy: Cygnus A

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Weak (FRI) radiogalaxy: 3C31

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The radio-loud zoo is large and complex

Messy classification! FRI, FRII, NLRG, BLRG, FSRQ, OVV, HPQ, BL Lac objects … Idea: Jet emission is anisotropic (beaming): viewing angle + intrinsic jet (and AGN) power

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BH Broad Line Region Narrow Line Region

Urry & Padovani 1995

“Unification scheme”

Accretion flow/disk (T~1e4 K)

Obscuring torus (hot dust)

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Radiogalaxy (FRI, FRII), SSRQ

BH Broad Line Region Narrow Line Region

Urry & Padovani 1995

“Unification scheme”

Accretion flow/disk (T~1e4 K)

Obscuring torus (hot dust)

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Radiogalaxy (FRI, FRII), SSRQ

Blazar (BL Lac [no BL], FSRQ [BL] )

BH Broad Line Region Narrow Line Region

Urry & Padovani 1995

“Unification scheme”

Accretion flow/disk (T~1e4 K)

Obscuring torus (hot dust)

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Blazar characteristics:

  • Compact radio core, flat or inverted spectrum
  • Extreme variability (amplitude and t) at all frequencies
  • High optical and radio polarization

FSRQs: bright broad (1000-10000 km/s) emission lines

  • ften evidences for the “blue bump” (acc. disc)

BL Lacertae: weak (EW<5 Å) emission lines no signatures of accretion

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Evidences for relativistic beaming

Superluminal motions Level of Compton emission High brightness temperatures Gamma-ray emission/absorption

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Radio VLBI Optical HST

Superluminal motion

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Superluminal motion

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Jorstad et al. 2001

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Blazars: phenomenology

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The Fermi/LAT (0.1-100 GeV) sky

2LAC: (2 years) 395 BL Lac 310 FSRQ 5 radiogalaxy 2 SSRQ

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The VHE extragalactic gamma-ray sky

38 BL Lacertae 5 radiogalaxies 3 FSRQ (3C279, z=0.536)

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The bumpy spectral energy distribution

Bonnoli et al. 2010

The brightest source in GeV!

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LAT lightcurve

FT et al. 2010 See also Foschini et al. 2010 Abdo et al. 2010, arXiv:1007

.0483 for 3C454.3

The erratic light-curve

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Rapid variability implies compact regions!

Conical geometry

IF

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Fossati et al. 1998; Donato et al. 2001

FSRQs

BL Lacs

The “blazar sequence”

Blazars

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Fossati et al. 1998; Donato et al. 2001

FSRQs CT

AGILE Fermi

The “blazar sequence”

BL Lacs

Swift

Blazars

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Blazars: emission models

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BL Lacs: “clean” jets

Inefficient accretion flow (ADAF-ADIOS)*

*but see Raiteri et al. 2009 Capetti et al. 2010 for BL Lac itself

Blazars

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Emission Models

Simplest scenario: SSC model (HBL) Other : external radiation (LBL, FSRQs, HBL?)

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The relativistic Doppler factor

  • =

1

(1 cos )

Special relat. Photon “compression”

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The relativistic Doppler factor

  • L=L’4

=’ t=t’/

=

1

(1 cos )

Special relat. Photon “compression”

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The relativistic Doppler factor

  • L=L’4

=’ t=t’/

=

1

(1 cos )

Special relat. Photon “compression”

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Coordinated variability at different

Mkn 421

X-rays TeV

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One-zone Synch. Self-Compton models

Tagliaferri et al. + MAGIC Coll. 2008

  • B
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One-zone Synch. Self-Compton models

Tagliaferri et al. + MAGIC Coll. 2008

  • B
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The simplest model - 1

  • R

Log Log N() n1 n2 b Log Log L() 1 2 s B e

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The simplest model – 2a

Log Log N() n1 n2 b Log Usyn()

+

Log 1 2 ’s Log Log L() 1 2 s 1 2 C

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The simplest model – 2b

Log Log N() n1 n2 b

+

“Klein-Nishina regime” h ’s b >mec2 Log L() Log 1 2 s 1 KN C Log Log Usyn() 1 2 ’s

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Mkn 421: a BL Lac

"Pure" SSC

The simplest model - 4

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In principle, in the simplest version of the SSC model, all the parameters can be constrained by quantities available from

  • bservations:

Model parameters: R B No b n1 n2 Observational parameters: s Ls C LC tvar 1 2

7 free parameters 7 observational quantities

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FSRQs: the general scenario

Accretion disk

Blazars

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FSRQs: the general scenario

X-ray corona

Blazars

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FSRQs: the general scenario

BLR

Blazars

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DUSTY TORUS

FSRQs: the general scenario

Blazars

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e-

  • e-

e-

  • B

FSRQs: the “canonical” scenario

Dermer et al. 2009 Ghisellini, FT 2009 Sikora et al. 2009 Accretion disk X-ray corona BLR

DUSTY TORUS Blazars

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The simplest model - 5

Log Log N() n1 n2 b

+

Log Log Uext()

Broad line region,

Disk

  • ’o
  • 2

Log Log F() 1 2 s 1 2 C

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B = 0.6 - 0.5 = 17.8 - 12.3 b = 550 - 600

Ballo et al. 2002

3C 279 EC + SSC

The simplest model - 6