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Multi-wavelength emission models in blazars Gabriele Ghisellini INAF-Osservatorio di Brera with A. Celotti, R. Della Ceca, L. Foschini, G. Ghirlanda, F.

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Presentation on theme: "Multi-wavelength emission models in blazars Gabriele Ghisellini INAF-Osservatorio di Brera with A. Celotti, R. Della Ceca, L. Foschini, G. Ghirlanda, F."— Presentation transcript:

1 Multi-wavelength emission models in blazars Gabriele Ghisellini INAF-Osservatorio di Brera with A. Celotti, R. Della Ceca, L. Foschini, G. Ghirlanda, F. Haardt, L. Maraschi, G. Pareschi, T. Sbarrato, G. Tagliaferri, F. Tavecchio, M. Volonteri

2 BL Lacs vs FSRQs: the blazar sequence

3 Fossati et al. 1998; Donato et al. 2001 The “blazar sequence” FSRQs BL Lacs BATIntegral

4 FSRQs Line strength Fossati et al. 1998; Donato et al. 2001

5 FSRQs BL Lacs M/M Edd Fossati et al. 1998; Donato et al. 2001 Next talk by Meyer

6 3 months, 10 

7 Blazars: the redder the more powerful  cooling GRBs: the bluer the more powerful  heating??  ? “Amati” “Ghirlanda” E peak [keV] E [erg]

8 Jet-accretion connection & location

9 Sbarrato+ 2011 SDSS+1LAC Do we really need to divide blazars? 5x10 -4 EW<5A EW>5A Narayan & Yi 1995: L BLR /L Edd ~ 10 -3 Sharma+ 2007: L BLR /L Edd ~ 10 -5 M-  Plotkin+ 2011

10 Torus ~1-10 pc Broad Line Region ~0.2 pc Within R BLR U BLR = const Within R Torus U IR = const  R BLR R Torus disk Big blazars Poutanen L>0.01L Edd Sikora Leptonic view. For adronic: next talk by Boettcher  T ~   HeII

11 Torus ~1-10 pc Broad Line Region ~0.2 pc ~VLBI region ~20 pc away (Marscher+)  R BLR R Torus disk Lyutikov Also Joshi, next talk L>0.01L Edd

12 TeV X TeV BLR <<0.2 pc weak cooling SSC only “ADAF disk”  L<0.01L Edd

13 Black hole masses (for FSRQs)

14 UVOT XRT Fermi GG, Tavecchio & Ghirlanda 2009 Low energy synchro peak: leave the disk naked! torus disk X-ray corona synchro SSC EC  M BH =2x10 9

15 GG, Tavecchio & Ghirlanda 2009 torus disk X-ray corona synchro SSC EC Small B M BH =2x10 9

16 BAT M BH =10 10

17 Jet power

18 The jet cannot have less power than what required to produce the observed luminosity: P jet L obs 2222 > If P jet is twice as much,  halves. We can take that as the minimum P jet. This limit is model-independent.

19   

20 1 proton per electron  no pairs Having pairs would reduce P jet. But where are they created?

21 Pairs and radio-galaxies

22  We cannot produce pairs here!!

23  Efficient pairs production if primary spectrum peaks at ~MeV

24 If z=0.3 Two goals: 1) reduce power 2) more energy to leptons, less to protons

25 Two epochs of heavy BH formation?

26 Recently, two complete surveys of blazars: BAT and LAT (Ajello+2009, 2012). BAT has fewer blazars, but more at high redshifts. All BAT blazars at z>2 have M BH >10 9 M 0. These all have L x > 10 47 erg/s and L disk > 0.1 L Edd

27 GG+2010, Volonteri+ 2012; GG+ 2013 Heavy & Active: M > 10 9 ; L disk > 0.1 L Edd

28

29 Hopkins+ 2007 Two epochs of formation of massive BH? Radio-loud: z~4 Radio-quiet: z~2

30 Jets  spin  high accretion efficiencies  slow growth

31 It takes too long! Eddington accretion starting at z=20

32 Jets for all M/M Edd Location is an issue Look if radio-galaxies peak at ~1 MeV with L~10 45 erg/s Heavy BH in jetted AGNs form earlier Jets & Spin? Something must be changed Conclusions


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