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The spectral sequence of blazars : present status and expectations from GLAST. L. Maraschi , G. Ghisellini and F.Tavecchio INAF - Osservatorio Astronomico di Brera. The Blazar Spectral Sequence. Fossati et al. 1998; Donato et al. 2001. RED. FSRQ. Average s pectral energy distributions - PowerPoint PPT Presentation
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The spectral sequence The spectral sequence of blazars : present of blazars : present
statusstatusand expectations from and expectations from
GLASTGLASTL. MaraschiL. Maraschi, G. Ghisellini and , G. Ghisellini and
F.TavecchioF.Tavecchio
INAF - Osservatorio Astronomico di INAF - Osservatorio Astronomico di BreraBrera
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
The Blazar Spectral Sequence
FSRQ
BL Lacs
Fossati et al. 1998; Donato et al. 2001
RED
BLUE
Th
th
Average spectral energy distributions of blazars:
a systematic dependence on jet luminosity ?
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
Construction Method Construction Method
• Three different complete samples:Three different complete samples: 2Jy FSRQs, 1Jy BLLacs, EINSTEIN Slew 2Jy FSRQs, 1Jy BLLacs, EINSTEIN Slew
Survey BL LacsSurvey BL Lacs• Sources binned in radio luminosity Sources binned in radio luminosity
irrespective of original sampleirrespective of original sample• Averages of monochromatic Averages of monochromatic luminosities within each binluminosities within each bin
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
Theoreticalmodeling of individual sources shows thatthe sequence corresponds to a systematicchange of the the model parameters
Ghisellini et al.1998……….
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
Jet - accretion flow Jet - accretion flow connectionconnection
From observations we can estimate the luminosityFrom observations we can estimate the luminosity
(or u.l.) of the accretion disk.(or u.l.) of the accretion disk.
Modelling SEDs with good data coverage (gammaModelling SEDs with good data coverage (gamma
important) the jet power can be estimated.important) the jet power can be estimated.
Comparing the two involves the radiative efficiencyComparing the two involves the radiative efficiency
of the accretion flow ~ 10%, for a standard diskof the accretion flow ~ 10%, for a standard disk
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
Jet power vs. accretion Jet power vs. accretion powerpower
Maraschi 2001Maraschi 2001Maraschi & Tavecchio, 2003Maraschi & Tavecchio, 2003Sambruna et al.2006,Sambruna et al.2006,
At high P At high P (FSRQ)(FSRQ)PPjet jet = Pacc= Paccdiskdisk
At low P (BL At low P (BL
Lac)Lac)
PPjet jet > L> LdisKdisK
If PIf Pjetjet ~ P ~ Pdiskdisk < 0.01< 0.01
From SEDs of objects with sufficient data
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
The blazar sequence can The blazar sequence can be understood as a be understood as a
sequence insequence in
- High accretion rates produce bright disks - High accretion rates produce bright disks and powerful jetsand powerful jets - Low accretion rates explain the absence of optical - Low accretion rates explain the absence of optical
signatures of disks by radiatively inefficient accretion signatures of disks by radiatively inefficient accretion (ADAF) in less powerful jets(ADAF) in less powerful jets
- The sequence can be related to cosmological evolution - The sequence can be related to cosmological evolution of black hole masses (increasing with time)of black hole masses (increasing with time) and accretion rates (decreasing with time) leading to and accretion rates (decreasing with time) leading to
an overall decrease of man overall decrease of m
Maraschi 2001; Boettcher & Dermer 2002; Cavaliere & D’ Elia 2002;Maraschi 2001; Boettcher & Dermer 2002; Cavaliere & D’ Elia 2002;Maraschi & Tavecchio 2003; Maraschi & Tavecchio 2003;
••m••
••
(Accretion rate in Eddington units )
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
For these possible profound implicationsFor these possible profound implications
it is important to test and extend withit is important to test and extend with
GLAST GLAST
the original blazar spectral sequencethe original blazar spectral sequence
-- complete the gamma-ray coverage of-- complete the gamma-ray coverage of
the old samples … remove flaring biasthe old samples … remove flaring bias
at least for bright objectsat least for bright objects
-- search for gamma–ray emission for-- search for gamma–ray emission for
other samples ( a gamma-ray selectedother samples ( a gamma-ray selected
sample? )sample? )
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
MKN 421
A collectionof X-ray andgamma-raystates:An obedientsource
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
PKS 2155
An HBL ofextreme luminosity;
Jul 06 flareFoschini et al.(see Poster)
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
A high redshift extremely luminous FSRQdiscoveredwith BAT(SWIFT)
GLAST detection expected
Sambruna et al.2006
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
J0746+25
A perfectfit to the sequence
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
3C 454.3A less extremeGamma-ray Blazar fromEGRET
An extended X-ray jet discoveredwith CHANDRA
Tavecchio et al 2007
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
Changing theangle of view
Observable with GLASTalso at largeranglesNote the changein the gamma-rayto blue bumpratio
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
Effect of theviewing anglewithin the sequence
The positionof the peaksdoes not changedramatically.The blue bumpretains its highluminosity
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
Accretion disk:
Blue Bump and X-ray p.l.Jet :Synchrotronand InverseComptoncomponents
Disentanglingdisk and jetin “mixed”Blazar cores
Sambruna et al.2006
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
1136-135FSRQ withextended X-ray jetEGRET u.l.
Expect GLASTdetection asfor 0723+679
Sambruna et al2006
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
The effectof a change in gamma peakis illustrated:
The gamma-rayluminositydecreases a lotbut the kineticpower carried by the jet is the same
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
1629+4008An unusualobject:
An HBL with aSeyfert likeaccretion disk
The jet SED Conforms to thesequence
Padovani et al.2002
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
The optical spectrum suggests a Seyfert-like accretion disk with L = 4 x 10 (44) erg/s
The accreion rate must be above 0.01 Eddington
This object should have relativly low mass10 (7-8) solar masses
Need gamma-ray data to estimatethe jet power
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
Synch.+ICSynch.+ICmodel for model for 1629 +40081629 +4008
Gamma-rayGamma-raycomponentcomponentuncertain:uncertain:here EC,here EC,but SSC couldbut SSC couldfill the hole…fill the hole…GLAST GLAST observationobservationneeded !needed !
First GLAST Symposium - Stanford U - Feb 20First GLAST Symposium - Stanford U - Feb 200707
Laura Maraschi INAF-OABrLaura Maraschi INAF-OABr
ConclusionsConclusions
• The unprecedented sensitivity of GLAST The unprecedented sensitivity of GLAST will allow to probewill allow to probe
• Jets at intermediate angles and Jets at intermediate angles and “intrinsically” less powerful jets in “intrinsically” less powerful jets in intermediate mass objectsintermediate mass objects
• Progress in understanding the jet Progress in understanding the jet spectral properties and the jet-disk spectral properties and the jet-disk connectionconnection
is expected but requires multifrequencyis expected but requires multifrequency coverage coverage