multiwavelength observations of the gamma-ray blazars detected by agile filippo d’ammando inaf -...
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Multiwavelength observations of the gamma-ray blazars detected by AGILE
Filippo D’Ammando
INAF - Istituto di Astrofisica Spaziale e Fisica Cosmica RomaINAF - Istituto di Astrofisica Spaziale e Fisica Cosmica Roma
Università degli Studi di Roma “Tor Vergata”Università degli Studi di Roma “Tor Vergata”
Ph.D in Astronomy - Cycle XXII Ph.D in Astronomy - Cycle XXII
Roman Young Researchers Meeting 2009
Active Galactic Nuclei - Unification ModelActive Galactic Nuclei - Unification Model
• central Black Hole (106 -109 Mʘ)
• accretion disk rotating around the SMBH
• clouds of gas gravitational attracted by the black hole and illuminated by the disk radiation
• optically thick torus of molecular gas and dust
• two collimated relativistic jets
Urry and Padovani 1995
RYRM 2009 Filippo D’Ammando 21 July 2009
Almost all galaxies contains a massive black hole but 99% of them are silent and 1% is active (mostly radio-quiet AGNs)... and only 0.1% is radio-loud AGNs
Blazar characteristics:
- compact radio core, flat or inverted spectrum
- apparent superluminal motion
- irregular, rapid and often very large variability at all frequencies
- high and variable polarization at optical and radio frequencies
RYRM 2009 Filippo D’Ammando 21 July 2009
Emission mechanisms in blazars
Leptonic processes:
- synchrotron emission
- inverse Compton where seed photons came from the internal synchrotron radiation
- inverse Compton where seed photons came from external radiation (accretion disk, BLR and/or torus)
Hadronic processes:
- synchrotron emission
- proton-initiated cascades
- proton-synchrotron emission
RYRM 2009 Filippo D’Ammando 21 July 2009
Synchrotron SSC
Synchrotron Self-Compton (SSC)Synchrotron Self-Compton (SSC)Electrons in a magnetic field can work twice: first producing
synchrotron radiation, and then Comptonizing it (SSC)
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Sikora, BegelmanSikora, Begelman and Rees 1994 and Rees 1994
In External Compton model the seed photons come from outside to the jet
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The blazar (spectral) sequenceThe blazar (spectral) sequence
Fossati et al. 1998 Donato et al. 2001
FSRQ
BL Lac
Epk of synchrotron and Compton components inversely correlated with L
L
peakRYRM 2009 Filippo D’Ammando 21 July 2009
Low power slow cooling large ɣpeak
Big power fast cooling small cooling small ɣpeakpeak
Ghisellini et al. 1998, 2002
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Giuliani, D’Ammando, Vercellone, et al. 2009, A&A, 494, 509
First extragalactic source detected in gamma-ray by AGILE-GRID, monitored simultaneously in optical band by REM telescope and in X-rays by Swift
<Fɣ> = (210 38) 10-8 ph cm-2 s-1 E > 100 MeV
Gamma-ray flux similar to the EGRET high state but soft spectrum
The soft spectrum during a flaring episode could be an indication of a dominant contribution of EDC emission compared to ECC emission model
9 - 13 July 2007
First AGILE multi-λ campaign: 3C 279
ECDECD
ECCECC
RYRM 2009 Filippo D’Ammando 21 July 2009
R-band light curve between December 2006 and December 2007: a strong minimum occurred about 2 months before the AGILE observation
This optical minimum might be correlated with a low accretion state of the disk and then with a ECC component deficit, delayed of about two months
Hartman et al. 2001
RYRM 2009 Filippo D’Ammando 21 July 2009
Pucella, Vittorini, D’Ammando, et al. 2008, A&A, 491, L21
<Fɣ> = (195 30) 10-8 ph cm-2 s-1 E >100 MeV
Possible correlation between optical and gamma-ray bands: contemporaneous decrease in fluxes
The IC contribution from the BLR can explain the observed hard gamma-ray spectrum
23 August - 1 September 2007
PKS 1510-089
RYRM 2009 Filippo D’Ammando 21 July 2009
D’Ammando, Pucella, Raiteri, et al., submitted to A&A
Serendipitous detection during an AGILE pointing towards the Galactic Center
3 ToO by Swift/XRT: the spectrum becomes harder when the source is brighter
GASP-WEBT observed intense optical activity between January and April 2008
17 - 21 March 2008
PKS 1510-089: a rapid gamma-ray flare in March 2008
RYRM 2009 Filippo D’Ammando 21 July 2009
Between January and April 2008, the blazar PKS 1510-089 showed intense optical activity with several episodes of fast variability detected by GASP - WEBT
Peaks was detected in the optical band on 15 February, 29 March and 11 April 2008
After two episodes of medium intensity the
source was not detected for some days in
gamma-ray band and suddenly a rapid flare
was observed by AGILE on 18-19 March 2008
RYRM 2009 Filippo D’Ammando 21 July 2009
Radio-to-optical behaviour
The light curve at 230-345 GHz suggests that the mechanism producing the flaring event observed in optical in the second half of February and in late March-April 2008 also interested the millimetric emitting zone, with some delay
At 22-43 GHz a hint of flux increase is visible in the second part of the light curve, while the radio flux at 5-15 GHz shows no trend
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Spectral Energy Distribution - March 2008
Likely signatures of the little and big blue bumps
hard X-ray spectrum: soft X-ray excess?
RYRM 2009 Filippo D’Ammando 21 July 2009
PKS 1510-089 showed an extraordinary gamma-ray activity
during March 2009, with several flaring episodes
D’Ammando et al., in preparation
PKS 1510-089 March 2009
RYRM 2009 Filippo D’Ammando 21 July 2009
GASP observations of PKS 1510-089
During March 2009 the optical activity of PKS 1510-089 is greatly increased with a peak on 26 March 2009
D’Ammando et al., in preparation
RYRM 2009 Filippo D’Ammando 21 July 2009
Chen, D’Ammando, Villata, et al. 2008, A&A, 489, L37
<Fɣ> = (97 15) 10-8 ph cm-2 s-1 E >100 MeV
with a peak level of (193 42) 10-8 ph cm-2 s-1
z = 0.31 0.08 (Nilsson et al., 2008)
Total power transported in the jet is extremely
high ( Ltot > 3 x 1045 erg s-1) , at the limit of the
maximum power generated by a spinning black
hole of 109 Mʘ
4 - 23 September 2007
S5 0716+714 in September - October 2007
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The Discrete Correlation Function (DCF) displays a significant peak for a time-lag of -1 day
Possible delay in the gamma-ray flux variations with respect to optical variations of the order of 1 day
To fit the SED we use 2 different SSC components:
- the first component reproduces the ground state
- the second components dominates the optical and gamma-ray bands
RYRM 2009 Filippo D’Ammando 21 July 2009
Giommi, Colafrancesco, Cutini, et al., 2008, A&A, 487, L49
<Fɣ> = (47 ± 11) 10-8 ph cm-2 s-1 E >100 MeV
The gamma-ray flux is about a factor of 2 lower than in September
Strong variability in soft X-ray, moderate variability at optical/UV and approximately constant behavior in hard X-rays
The SED is consistent with a two-components SSC model
23 October - 13 November 2007
Swift and AGILE simultaneous obs. in October - November 2007
RYRM 2009 Filippo D’Ammando 21 July 2009
Pacciani, Donnarumma, Vittorini, et al. 2009, A&A, 494, 49
<Fɣ> = (22 6) 10-8 ph cm-2 s-1 E >100 MeV
Fɣ [peak] = (33 11) 10-8 ph cm-2s-1 E >100 MeV
Multi-wavelength campaign: REM, Swift, RXTE, INTEGRAL and AGILE
No optical variability during the entire campaign. Hint of a possible anti-correlated variability
between X-rays and gamma-rays
SSC + EC: spectral variability consistent with an acceleration episode of the electron population
16 December 2007 – 8 January 2008
3C 273: simultaneous detection by GRID & SA
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Vercellone, Chen, Giuliani, et al. 2008, ApJL, 676, 13
AGILE repointing the source during a period of strongly enhanced optical emission
<Fɣ> = (280 ± 40) 10-8 ph cm-2 s-1 E >100 MeV
Highest gamma-ray flux from this source in the last 15 years but see Fermi obs.
3C 454.3: July 2007
24 - 30 July 2007
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MW Observations of 3C 454.3 in November 2007
10 November - 1 December 2007
Vercellone, Chen, Vittorini, Giuliani, D’Ammando et al. 2009, ApJ, 690, 1018
<Fɣ> = (170 13) 10-8 ph cm-2 s-1, with a peak of ~400 x 10-8 ph cm-2 s-1 E >100 MeV
Rapid variability in the optical band
Emission in the optical range appears to be correlated with that at gamma-ray energies
The DCF indicate a moderate correlation with no lag between gamma-ray and
optical flux variations
RYRM 2009 Filippo D’Ammando 21 July 2009
The contribution of ECD radiation alone cannot account for the hardness of the spectrum. The gamma-ray emission seems to be dominated by IC scattering of the external photons from the broad line region clouds
ECD
ECD
ECC
ECC
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RYRM 2009 Filippo D’Ammando 21 July 2009
MW Observations of 3C 454.3 in December 2007
Donnarumma et al., 2009, submitted to ApJ
Simultaneous multi-wavelength campaign with the contribution of Spitzer, REM, GASP-WEBT, MITSuME, Swift, Suzaku and AGILE
<Fɣ> = ~ 250 x 10-8 ph cm-2 s-1 E >100 MeV
A leptonic EC model is considered, with also a contribution of EC on a hot corona (T=106 K),
to account for the hard ɣ-ray spectrum
RYRM 2009 Filippo D’Ammando 21 July 2009
DCF analysis shows a (possible) delay of the gamma-ray flux variations with respect to the optical ones of about 10 hours
The longest monitor so far of a blazar in the gamma-ray band
A factor of about 10 in dynamic range in about 2 years with a
possible spectral trend (harder when brighter)
Vercellone et al., in preparation
Mrk 421: WEBT + AGILE + VERITAS + MAGIC = …
RYRM 2009 Filippo D’Ammando 21 July 2009
Donnarumma, Vittorini, Vercellone et al., 2009, ApJ 691, L13
<Fɣ> = (42 ± 13) 10-8 ph cm-2 s-1 E >100 MeV
Swift/XRT: Flux (2 - 10 keV) = 2.6 x 10-9 ph cm-2 s-1
Possible correlated variability between optical, X-rays and high-energy parts of the spectrum
SSC model: hardening/softening of electron energy distribution caused by particle acceleration process
Mrk 421 from optical to TeV energies
Summary and remarks• Gamma-ray astronomy is still a largely unexplored territory,
in particular for the class of blazars• AGILE (and EGRET) detected only few objects with flux
greater than 100 x 10-8 ph cm-2 s-1? Why? Selection effects or there is a subclass of blazar with peculiar characteristics?
• SSC vs EC vs more complex models? How to distinguish?• AGILE observations has brought to light a more complex
behaviour of blazars with respect to the standard models: - the presence of two emission components in any BL Lacs
- the possible contributions of an hot corona as source of seed photons for the EC in FSRQs
• The study of multi-wavelength correlations is the key to understanding the structure of the inner jet and the origin of the seed photons for the IC process
• The study of sources in different activity states, not only during flaring states, could provide new informations
Thanks for your attention!!!