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AGILE detection of intense gamma-ray emission from the blazar PKS 1510-089

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We report the detection by the AGILE (Astro-rivelatore Gamma a Immagini LEggero) satellite of an intense gamma-ray flare from the source AGL J1511-0909, associated with the powerful quasar PKS 1510-089, during ten days of observations from 23 August to 1 September 2007. During the observation period, the source was in optical decrease following a flaring event monitored by the GLAST-AGILE Support Program (GASP) of the Whole Earth Blazar Telescope (WEBT). The simultaneous gamma-ray, optical, and radio coverage allows us to study the spectral energy distribution and the theoretical models based on the synchrotron and inverse Compton (IC) emission mechanisms. AGILE observed the source with its two co-aligned imagers, the Gamma-Ray Imaging Detector and the hard X-ray imager Super-AGILE sensitive in the 30 MeV - 50 GeV and 18 - 60 keV bands, respectively. Between 23 and 27 August 2007, AGILE detected gamma-ray emission from PKS 1510-089 when this source was located about 50 degrees off-axis, with an average flux of (270 +/- 65) x 10^{-8} photons cm^{-2} s^{-1} for photon energy above 100 MeV. In the following period, 28 August - 1 September, after a satellite re-pointing, AGILE detected the source at about 35 degrees off-axis, with an average flux (E > 100 MeV) of (195 +/- 30) x 10^{-8} photons cm^{-2} s^{-1}. No emission was detected by Super-AGILE, with a 3-sigma upper limit of 45 mCrab in 200 ksec. The spectral energy distribution is modelled with a homogeneous one-zone synchrotron self Compton (SSC) emission plus contributions by external photons: the SSC emission contributes primarily to the X-ray band, whereas the contribution of the IC from the external disc and the broad line region match the hard gamma-ray spectrum observed. Comment: 5 pages, 5 figures, accepted for publication in A&A
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arXiv:0810.1676v1 [astro-ph] 9 Oct 2008
1
Astronomy & Astrophysics
manuscript no. 1510˙v10 c
ESO 2008
October 9, 2008
Letter to the Editor
AGILE detection of intense gamma-ray emission from the blazar
PKS 1510-089
G. Pucella1, V. Vittorini1,2, F. D’Ammando1,3, M. Tavani1,3, C. M. Raiteri4, M. Villata4, A. Argan1, G. Barbiellini5,
F. Boelli6,7, A. Bulgarelli8, P. Caraveo9, P. W. Cattaneo6, A. W. Chen2,9, V. Cocco1, E. Costa1, E. Del Monte1, G. De
Paris1, G. Di Cocco8, I. Donnarumma1, Y. Evangelista1, M. Feroci1, M. Fiorini8, T. Froysland2,3, F. Fuschino8,
M. Galli10, F. Gianotti8, A. Giuliani9, C. Labanti8, I. Lapshov1, F. Lazzarotto1, P. Lipari11, F. Longo5, M. Marisaldi8,
S. Mereghetti9, A. Morselli12, L. Pacciani1, A. Pellizzoni9, F. Perotti9, P. Picozza12, M. Prest13, M. Rapisarda14,
A. Rappoldi6, P. Sotta1, M. Trifoglio8, A. Trois1, E. Vallazza5, S. Vercellone9, A. Zambra1, D. Zanello11,
L. A. Antonelli15, S. Colafrancesco15, S. Cutini15, D. Gasparrini15, P. Giommi15, C. Pittori15, F. Verrecchia15,
L. Salotti16, M. F. Aller17, H. D. Aller17, D. Carosati18, V. M. Larionov19, R. Ligustri20
1INAF/IASF–Roma, Via del Fosso del Cavaliere 100, I-00133 Roma, Italy
2CIFS–Torino, Viale Settimio Severo 3, I-10133 Torino, Italy
3Dip. di Fisica, Univ. di Roma “Tor Vergata”, Via della Ricerca Scientifica 1, I-00133 Roma, Italy
4INAF, OATo, Via Osservatorio 20, I-10025 Pino Torinese (Torino), Italy
5Dip. di Fisica and INFN Trieste, Via Valerio 2, I-34127 Trieste, Italy
6INFN–Pavia, Via Bassi 6, I-27100 Pavia, Italy
7Dip. di Fisica Nucleare e Teorica, Univ. di Pavia, Via Bassi 6, I-27100 Pavia, Italy
8INAF/IASF–Bologna, Via Gobetti 101, I-40129 Bologna, Italy
9INAF/IASF–Milano, Via E. Bassini 15, I-20133 Milano, Italy
10 ENEA–Bologna, Via dei Martiri di Monte Sole 4, I-40129 Bologna, Italy
11 INFN–Roma “La Sapienza”, Piazzale A. Moro 2, I-00185 Roma, Italy
12 INFN–Roma “Tor Vergata”, Via della Ricerca Scientifica 1, I-00133 Roma, Italy
13 Dip. di Fisica, Univ. dell’Insubria, Via Valleggio 11, I-22100 Como, Italy
14 ENEA–Roma, Via E. Fermi 45, I-00044 Frascati (Roma), Italy
15 ASI–ASDC, Via G. Galilei, I-00044 Frascati (Roma), Italy
16 ASI, Viale Liegi 26, I-00198 Roma, Italy
17 Department of Astronomy, University of Michigan, U. S.
18 Armenzano, Astronomical Observatory, I-06083 Assisi (Perugia), Italy
19 Astron. Inst., St-Petersburg State University, Russia
20 Circolo AStrofili Talmassons, Via Cadorna 57, I-33030 Talmassons (Udine), Italy
received; accepted
ABSTRACT
Context.
We report the detection by the AGILE (Astro-rivelatore Gamma a Immagini LEggero) satellite of an intense gamma-ray
flare from the source AGL J1511-0909, associated with the powerful quasar PKS 1510-089, during ten days of observations from 23
August to 1 September 2007.
Aims.
During the observation period, the source was in optical decrease following a flaring event monitored by the GLAST-AGILE
Support Program (GASP) of the Whole Earth Blazar Telescope (WEBT). The simultaneous gamma-ray, optical, and radio coverage
allows us to study the spectral energy distribution and the theoretical models based on the synchrotron and inverse Compton (IC)
emission mechanisms.
Methods.
AGILE observed the source with its two co-aligned imagers, the Gamma-Ray Imaging Detectorand the hard X-ray imager
Super-AGILE sensitive in the 30 MeV ÷50 GeV and 18 ÷60 keV bands, respectively.
Results.
Between 23 and 27 August 2007, AGILE detected gamma-ray emission from PKS 1510-089 when this source was located
50o-axis, with an average flux of (270 ±65)×108photons cm2s1for photon energy above 100 MeV. In the following period,
28 August - 1 September, after a satellite re-pointing, AGILE detected the source at 35o-axis, with an average flux (E >100
MeV) of (195 ±30) ×108photons cm2s1. No emission was detected by Super-AGILE, with a 3-σupper limit of 45 mCrab in 200
ksec.
Conclusions.
The spectral energy distribution is modelled with a homogeneous one-zone synchrotron self Compton (SSC) emission
plus contributions by external photons: the SSC emission contributes primarily to the X-ray band, whereas the contribution of the IC
from the external disc and the broad line region match the hard gamma-ray spectrum observed.
Key words. gamma-rays: observations mechanism: non-thermal quasars: individual (PKS 1510-089)
1. Introduction
The radio source PKS 1510-089 was first identified optically as
a quasar with an ultraviolet excess, a visual magnitude of 16.5
(Bolton & Ekers 1966), and a redshift of z =0.361 measured
from its emission-line spectrum (Burbidge & Kinnan 1966).
PKS 1510-089 is a radio-loud highly polarized quasar (HPQ)
belonging to the class of the flat spectrum radio quasar (FSRQ)
in terms of its spectral energy distribution. Its radiative output is
dominated by the gamma-ray component, while its synchrotron
emission peaks around IR frequencies below a pronunced UV
bump, presumably due to the thermal emission from the accre-
tion disc (Malkan & Moore 1986, Pian & Treves 1993).
PKS 1510-089 has been extensively observed in X-rays by
EXOS AT (Singh, Rao & Vahia 1990, Sambruna et al. 1994),
GINGA (Lawson & Turner 1997), ROS AT (Siebert et al. 1998),
ASCA (Singh, Shrader & George 1997) and Chandra (Gambill
et al. 2003). The observed X-ray spectrum was very flat in the
2÷10 keV band (photon index Γ1.3), but steepened in
the ROS AT bandpass below 2 keV (Γ1.9). Observations by
BeppoS AX (Tavecchio et al. 2000) confirm the presence of a
soft X-ray excess below 1 keV. A similar soft excess has been
detected in other blazarssuch as 3C273, 3C279, and 3C454.3,
and the origin of the soft X-ray excess is still an open issue.
PKS 1510 was recently observed by S uzaku in August 2006
over approximately three days, and the campaign continued with
Swift monitoring over 18 days (Kataoka et al. 2007). Swift-XRT
observations reveal significant spectral evolution of the X-ray
emission on timescales of one week: the X-ray spectrum be-
comes harder as the source gets brighter.
Gamma-ray emission from PKS 1510-089 was detected by
the EGRET instrument on board CGRO with a integrated flux
above 100 MeV between (13 ±5) and (49 ±18) ×108photons
cm2s1and an energy spectrum modelled with a power law
with a photon index Γ = 2.47 ±0.21. In this Letter we present
the analysis of the AGILE data obtained during the PKS 1510-
089 observations from 23 August 2007 to 1 September 2007.
2. AGILE observation of PKS 1510-089
The AGILE scientific Instrument (Tavani et al. 2008) is very
compact and combines four active detectors yielding broad-band
coverage from hard X-rays to gamma rays.
The Gamma-Ray Imaging Detector (GRID) consists of a
combination of a silicon tracker (Prest et al. 2003, Barbiellini
et al. 2001), a non-imaging Cesium Iodide Mini-Calorimeter
(MCAL; Labanti et al. 2006) positioned under the silicon tracker
and sensitive in the 0.3 ÷100 MeV energy band, and a seg-
mented anticoincidence system (ACS) made of a plastic shield
which surrounds all active detectors (Perotti et al. 2006). A co-
aligned coded-mask hard X-ray imager (SuperAGILE; Costa et
al. 2001, Feroci et al. 2007) ensures coverage in the 18 ÷60 keV
energy band.
The GRID has a field of view of 2.5 sr, an angular resolu-
tion of 1.2at 400 MeV (68% cont. radius), an eective area of
500 cm2above 100 MeV, and an energy resolution E/E1
at 400 MeV. The silicon tracker and the on-board trigger logic
are optimized for gamma-ray imaging in the 30 MeV ÷50 GeV
energy band (Argan et al. 2004).
The AGILE observations of the PKS 1510-089 were per-
formed from 23 August 2007 12:00 UT to 1 September 2007
Send oprint requests to: G. Pucella, e-mail:
gianluca.pucella@iasf-roma.inaf.it
Fig.1. Gaussian-smoothed count map (140×140) in
Galactic coordinates integrated over the observing period 2007
August 23 - August 27. The circles are located at the PKS
1510-089 and Vela Pulsar coordinates. Only photons with en-
ergy greater than 100 MeV have been included.
Fig.2. Gaussian-smoothed count map (140×140) in
Galactic coordinates integrated over the observing period 2007
August 28 - September 1. The circle is located at the PKS 1510-
089 coordinates. Only photons with energy greater than 100
MeV have been included.
12:00 UT, for a total of 84 hours of eective exposure time.
In the first period, between 23 and 27 August, the source was
located 50othe AGILE pointing direction. In the second
period, between 28 August and 1 September, after a satellite re-
pointing, the source was located at 35o-axis.
3. Data reduction and analysis
Level–1 AGILE-GRID data were analysed using the AGILE
Standard Analysis Pipeline. The first step is to align all data
times to terrestrial time (TT), and it performs preliminary
calculations. In the second step, an ad-hoc implementation
of the Kalman Filter technique is used for track identifica-
tion and event-direction reconstruction in detector coordinates.
Subsequently, a quality flag is assigned to each GRID event:
(G), (P), (S), and (L), depending on whether it is recognised as a
confirmed gamma-ray event, a charged particle event, a single-
track event, or its nature is uncertain, respectively. The (L) event
class includes events typically aected by an order of magni-
tude higher particle contamination than (G). The single-track
G. Pucella et al.: AGILE detection of PKS 1510-089 3
Fig.3. a) AGILE-GRID gamma-ray light curve, with a 1-
day resolution, for the observation period 2007 August 28 -
September 1, for photons with E >100 MeV in units of 108
photons cm2s1. b) R-band optical light curve as observed by
the GASP of the WEBT for the observation period 2007 July 26
- September 11. c) GASP radio light curve (from UMRAO) at
14.5 GHz for the observation period 2007 July 24 - September
15.
(S) event class includes events for which only one track is re-
constructed in the two orthogonal views of the tracker. Then, an
AGILE log-file is created, containing all the information rele-
vant to computating the exposure and live time. The third step
is to create the AGILE event files, excluding events flagged as
particles. This step also reconstructs the event direction in sky
coordinates.
Once the above steps are completed, the AGILE Scientific
Analysis Package can be run. Counts, exposure, and Galactic
background gamma-ray maps are created with a bin-size of
0.5×0.5for photons with energy over 100 MeV. To reduce
the particle background contamination, we selected only events
flagged as confirmed gamma-ray events, and all events collected
during the South Atlantic Anomaly were rejected.
We also rejected all the gamma-ray events whose recon-
structed directions form angles with the satellite-Earth vector
smaller than 80, reducing the gamma-ray Earth albedo contam-
ination by excluding regions within 10from the Earth limb.
We ran the AGILE maximum likelihood procedure (ALIKE) on
the whole observing period, in order to obtain the average flux
in the gamma-ray band.
Fig.4. AGILE average gamma-ray spectrum of PKS 1510-089
for the observation period 28 August - 1 September 2007.
4. Results
Figure 1 shows a Gaussian-smoothed count map in Galactic co-
ordinates integrated over the observing period 2007 August 23 -
27 for photon energies over 100 MeV. In this period, AGILE de-
tected gamma-ray emission from a position consistent with the
quasar PKS 1510-089 at a significance level of 5.6-σas derived
from a maximum likelihood analysis using the PKS 1510-089
radio position (l=351.29,b=40.14). During this period
the source was located 50othe AGILE pointing direc-
tion. Thanks to the large field of view of AGILE, during this
period, the satellite simultaneously also detected the gamma ac-
tivity of the source Vela Pulsar (l=263.55,b=2.79), about
90 degrees from PKS 1510-089. In addition, the two sources
were characterised by an almost equal angular distance from the
AGILE pointing direction. This allowed us to obtain an estimate
of average flux of PKS 1510-089 through a direct calibration
with the flux of the Vela Pulsar. In this way, the average flux (E
>100 MeV) estimated for this first period was (270 ±65)×108
photons cm2s1. The reduced eective area and the conse-
quently reduced count statistics for these large o-axis angles
makes it dicult to create a light curve and an average energy
spectrum.
Figure 2 shows a Gaussian-smoothed count map in Galactic
coordinates integrated over the observing period 2007 August
27 September 1 for photon energies higher than 100 MeV.
In this period the satellite detected the source at a significance
level of 10.6-σ. With the likelihood method, the best position
for the gamma-ray emission above 100 MeV is (l=350.89,b=
40.34), with an average flux (E >100 MeV) over the period of
(195±30)×108photons cm2s1. The AGILE 95% maximum-
likelihood contour level has a semi-major axis a=0.43and
semi-minor axis b=0.09. The overall AGILE error circle, tak-
ing both statistical and systematic eects into account, has a ra-
dius r=0.53. During this period the source was observed at 35
o-axis. In Fig. 3 the gamma-ray light curve for this period with
a 1-day resolution, the R-band optical light curve as observed by
the GASP of the WEBT for the observation period between 26
July and 11 September 2007, and the GASP radio light curve
(from UMRAO) at 14.5 GHz for the observation period between
24 July and 15 September 2007 1are reported. Figure 4 reports
the average energy spectrum for this second period, when only
three energy bins were taken into account for the fit: 100 ÷200
1The optical and radio data presented in this paper are stored in the
GASP-WEBT archive (http://www.oato.inaf.it/blazars/webt). For ques-
tions regarding their availability, please contact the WEBT President
Massimo Villata.
4 G. Pucella et al.: AGILE detection of PKS 1510-089
Fig.5. Spectral Energy Distribution of PKS 1510-089 for the GRID observation period 28 August - 1 September 2007 (blue dots),
including simultaneous GASP optical (red square) and radio (orange triangle) data and the 3-σSuper-AGILE upper limit. Non-
simultaneous historical data (from 1969 to 2007) taken from NASA Extragalactic Database (NED) and Kataoka et al. (2007) over
the entire electromagnetic spectrum are represented in dark grey and light grey,respectively.
MeV, 200 ÷400 MeV, 400 ÷1000 MeV. The energy bins 50 ÷
100 MeV and 1000 ÷3000 MeV have not be used in the spec-
tral analysis waiting for on-flight calibration finalization that will
include these two energy channels.
A simple power-law model can fit the data. We obtain a
photon index Γ = 1.98 ±0.27 with the weighted least squares
method.
Super-AGILE observed PKS 1510-089 for a total on-source
eective exposure time of 200 ks. The source was not detected
above 5-σby the Super-AGILE Iterative Removal Of Sources
(IROS) applied to the image, in the 20–60 keV energy range. A
3-σupper limit of 45 mCrab was obtained from the observed
count rate by a study of the background fluctuations at the posi-
tion of the source and a simulation of the source and background
contributions with IROS.
Finally, in Fig. 5 the spectral energy distribution is shown
for the GRID observation period 2007 August 28 - September
1, including simultaneous GASP optical and radio data and the
3-σSuper-AGILE upper limit. Also non-simultaneous historical
data over the entire electromagnetic spectrum are represented.
5. Discussion
During the AGILE observation period, the PKS 1510-089 opti-
cal flux appears to be decreasing in the range R15.5 ÷15.8,
following a bright state that reached at least R=15.0 (see Fig.
3). The contemporaneous gamma-ray flux decrease of about a
factor 3 suggests that the two flux variations may be correlated.
In agreement with Kataoka et al. (2007), in order to model the
spectral energy distribution we used a homogeneous one-zone
synchrotron self-Compton (SSC) model, plus the contribution
of external seed photons originating both from the accretion disc
and the broad line region (BLR). We obtained a representative fit
for the spectral energy distribution with input parameters similar
to those chosen by Kataoka et al. (2007). We consider a rela-
tivistic moving spherical blob of radius R =2.5 ×1016 cm and
an electron energy distribution described by a double power law:
ne(γ)=Kγ1
b
(γ/γb)p1+(γ/γb)p2(1)
for electron Lorentz factor 40 < γ < 4×103with spectral indices
pre- and post-break p1=2.0 and p2=4.5, a normalization
factor K =80 cm3and the break energy Lorentz factor γb=
400. We assumed a magnetic field B =3 Gauss and a Doppler
factor δ=9 for the blob.
In order to interpret our gamma-ray data, an accretion disc
characterised by a blackbody spectrum with a luminosity of
1046erg s1at 0.1 pc from the blob is assumed as the source
of external target photons. The inverse Compton (IC) contribu-
tion from the disc is calculated up to the second order, but it is
not enough to account for the high gamma-ray state observed
by AGILE. The addition of the IC emission from a BLR, repre-
sented by a spherical layer extending between 0.1 pc and 0.4 pc
from the central black hole, reprocessing a 10% of the irradiating
continuum can explain the high state observed by AGILE com-
pared to the historical EGRET observations (see Fig. 5), and it
reflects on the dierent photon index obtained in the AGILE and
EGRET observations. In this model, the SSC emission primarily
contributes to the X-ray band, whereas the IC contribution from
the BLR can explain the observed hard gamma-ray spectrum.
Acknowledgements. The AGILE Mission is funded by the Italian Space Agency
(ASI) with scientific and programmatic participation by the Italian Institute of
Astrophysics (INAF) and the Italian Institute of Nuclear Physics (INFN). This
research has made use of the NASA/IPAC Extragalactic Database (NED) which
is operated by the Jet Propulsion Laboratory, California Institute of Technology,
under contract with the National Aereonautics and Space Administration.
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The non-thermal spectra of jetted active galactic nuclei show a variety of shapes in their low- and high energy components. In some of the brightest Fermi-LAT blazars, prominent spectral breaks at a few GeV have been regularly detected, which is inconsistent with conventional cooling effects. We study the effects of continuous time-dependent injection of electrons into the jet with differing rates, durations, locations, and power-law spectral indices, and evaluate its impact on the ambient emitting particle spectrum at a given snapshot time in the framework of a leptonic blazar emission model. The emitting electron spectrum is calculated by Compton cooling the continuously injected electrons, where target photons are assumed to be provided by the accretion disk and broad line region. We calculate the non-thermal photon spectra produced by inverse Compton scattering of these external target radiation fields using the full Compton cross-section in the head-on approximation. By means of a comprehensive parameter study we present the resulting ambient electron and photon spectra, and discuss the influence of each injection parameter. Varying the injection parameters has a notable influence on the spectral shapes, which can be used to set constraints on the injection scenarios. We apply our model to the flare state spectral energy distribution of 3C454.3, and to the FSRQ PKS1510-089. For both sources we show two different model fits, corresponding to different injection scenarios. In all four injection scenarios impulsive particle injection is disfavored. Our model aims towards bridging jet emission with acceleration models using a phenomenological approach. Blazar spectral data can be analyzed with this model to constrain injection parameters, in addition to the conventional parameter values of steady-state emission models, if sufficient broad multifrequency coverage is provided.
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We present the X-ray light curve (1.5-12 keV) for quasar PKS 1510-089 with the observation of the all-sky monitor on the Rossi X-ray Timing Explorer from January 1996 to December 2009. Using the discrete correlation function method, the wavelet analysis method and the power spectrum method to analyze the data, we find that the light curve variability period of quasar PKS 1510-089 is (0.94±0.08)a. The super massive binary black hole model in used to analyze this source, and the results show that the orbit period of the super massive binary black hole system is (1.85±0.10) a and the super massive binary black hole model is the better model for describing the light curve periodic behaviour of quasar PKS 1510-089 at present.
Conference Paper
We summarize here the main highlights of the AGILE astrophysics mission. The satellite, launched in April 2007, is devoted to γ‐ray observations in the 30 MeV–30 GeV energy range, with simultaneous hard X‐ray imaging in the 18–60 keV band, and optimal timing capabilities for the study of transient phenomena. The very large field of view (2.5 sr) of the gamma‐ray imager coupled with the hard X‐ray monitoring capability makes AGILE well suited to study Galactic and extragalactic sources, as well as GRBs and other fast transients. AGILE reaches its optimal performance near 100 MeV with good imaging and sensitivity. Gamma‐ray and hard X‐ray sources can be monitored 14 times a day, and an extensive database has been obtained for a variety of sources. We summarize here the breakthroughs and most important results obtained for several sources including microquasars and other Galactic compact objects (most notably, the discovery of gamma‐ray emission above 100 MeV from Cygnus X‐3), Supernova Remnants and pulsar wind nebulae, gamma‐ray pulsars, a bright class of blazars (3C 454.3, TXS 0716+714, HB 1510−089, Mrk 421), short and long GRBs (including the remarkable short burst GRB 090510), and terrestrial gamma‐ray flashes (TGFs).
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Aims. Amongst more than fifty blazars detected in very high energy (VHE, E > 100 GeV) gamma rays, only three belong to the subclass of flat spectrum radio quasars (FSRQs). The detection of FSRQs in the VHE range is challenging, mainly because of their soft spectra in the GeV-TeV regime. MAGIC observed PKS 1510-089 (z = 0.36) starting 2012 February 3 until April 3 during a high activity state in the high energy (HE, E > 100 MeV) gamma-ray band observed by AGILE and Fermi. MAGIC observations result in the detection of a source with significance of 6.0 standard deviations (sigma). We study the multi-frequency behaviour of the source at the epoch of MAGIC observation, collecting quasi-simultaneous data at radio and optical (GASP-WEBT and F-Gamma collaborations, REM, Steward, Perkins, Liverpool, OVRO, and VLBA telescopes), X-ray (Swift satellite), and HE gamma-ray frequencies. Methods. We study the VHE gamma-ray emission, together with the multi-frequency light curves, 43 GHz radio maps, and spectral energy distribution (SED) of the source. The quasi-simultaneous multi-frequency SED from the millimetre radio band to VHE gamma rays is modelled with a one-zone inverse Compton model. We study two different origins of the seed photons for the inverse Compton scattering, namely the infrared torus and a slow sheath surrounding the jet around the Very Long Baseline Array (VLBA) core. Results. We find that the VHE gamma-ray emission detected from PKS 1510-089 in 2012 February-April agrees with the previous VHE observations of the source from 2009 March-April. We find no statistically significant variability during the MAGIC observations on daily, weekly, or monthly time scales, while the other two known VHE FSRQs (3C 279 and PKS 1222+216) have shown daily scale to sub-hour variability. The gamma-ray SED combining AGILE, Fermi and MAGIC data joins smoothly and shows no hint of a break. The multi-frequency light curves suggest a common origin for the millimetre radio and HE gamma-ray emission, and the HE gamma-ray flaring starts when the new component is ejected from the 43GHz VLBA core and the studied SED models fit the data well. However, the fast HE gamma-ray variability requires that within the modelled large emitting region, more compact regions must exist. We suggest that these observed signatures would be most naturally explained by a turbulent plasma flowing at a relativistic speed down the jet and crossing a standing conical shock.
Article
We present results of modelling the broad-band spectral energy distribution (SED) and multiwavelength variability of the bright flat spectrum radio quasars PKS 1510-089 with our time-dependent multizone Monte Carlo/Fokker-Planck code. As the primary source of seed photons for inverse Compton scattering, we consider radiation from the broad-line region (BLR), from the hot dust of the molecular torus and the local synchrotron radiation [synchrotron self-Compton (SSC)]. We evaluate the viability of different Compton models by comparing simulated multiwavelength light curves and SEDs with one of the best observed flares by PKS 1510-089, in 2009 March. The time dependence of our code and its correct handling of light travel time effects allow us to fully take into account the effect of the finite size of the active region, and in turn to fully exploit the information carried by time-resolved observed SEDs that are becoming increasingly available since the launch of Fermi. We confirm that the spectrum adopted for the external radiation field has an important impact on the modelling of the SED, in particular for the lower energy end of the Compton component which is observed in the X-ray band, which in turn is one of the most critical bands to assess the differences between external Compton and SSC emission. In the context of the scenario presented in this paper, where the flaring is caused by the increase of the number of relativistic electrons ascribed to the effect of the interaction of a portion of the jet (blob) with a shock, we cannot firmly discriminate the three main scenarios for γ-ray emission. However, results show clearly the differences produced by a more realistic treatment of the emitting source in the shape of SEDs and their time variability over relevant, observable time-scales, and demonstrate the crucial importance of time-dependent multizone models to advance our understanding of the physics of these sources, by taking full advantage of the wealth of information offered by the high-quality data of current multiwavelength campaigns.
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A detailed study of X-ray emission from the high-polarization quasar PKS 1510 - 089, also known as a blazar, is presented, based on the Exosat observations in 1984 and 1985. There is no evidence for any variations in the X-ray intensity on hourly time scales during either of the two observations. The 2-10 keV X-ray flux shows no significant change over a year. The observed X-ray spectral data is best fitted by a power law with a photon index, of about 1.40. There is no detection of any significant low-energy absorption within the blazar, nor is there any evidence for a soft X-ray excess. A line feature modeled as a Gaussian is detected with a high significance near 5 keV. The emission line could be the redshifted 6.4 keV line due to the fluorescence of cold iron present around the nucleus of PKS 1510 - 089 or the redshifted 6.7 keV line due to ionized iron in a hot plasma.
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We present BeppoSAX observations of three γ-ray-emitting quasars, namely, 0836+710, 1510-089, and 2230+114. The three objects have been detected up to ~100 keV showing extremely flat power-law spectra above 2 keV (energy index α2-10 = 0.3-0.5). The soft X-ray spectrum of 0836+710 implies either an absorption column density higher than the Galactic one or an intrinsically very hard slope (α0.1-1 = -0.2) below 1 keV. 1510-089 shows a soft excess, with the low-energy spectrum steeper (α0.1-1 = 1.6) than the high-energy power law. The results are discussed in the framework of current inverse Compton models for the high-energy emission of flat-spectrum radio quasars and are used to estimate the physical quantities in the jet-emitting region and to shed light on the energy transport mechanisms in jets. Finally we discuss the estimates of the jet luminosity in the context of the Blandford & Znajek mechanism for jet production.
Conference Paper
AGILE is a small space mission of the Italian Space Agency (ASI) devoted to astrophysics in the gamma-ray energy range 30 MeV - 50 GeV, and in the X-ray band 15 keV - 45 keV. The AGILE Payload is composed of three instruments: a gamma-ray imager based on a Tungsten-Silicon Tracker (ST), for observations in the gamma ray energy range 30 MeV - 50 GeV, a Silicon based X-ray detector, Super-Agile (SA), for imaging in the range 15 keV - 40 keV and a CsI(Tl) Mini-Calorimeter (MCAL) that detects gamma rays or particle energy deposits between 300 keV and 200 MeV. The payload is currently fully integrated and the satellite is expected to be launched in the second half of 2006. MCAL, is composed of 30 CsI(Tl) scintillator detectors with the shape of a bar with photodiode readout at both ends, arranged in two orthogonal layers. MCAL can work both as a slave of the ST and as an independent gamma-ray detector for the detection of transients and Gamma Ray Bursts. In this paper a detailed description of MCAL is presented together with the first on ground calibration results.
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The gamma-ray observatory AGILE, the first ASI Small Mission, is planned to operate in 2002-2005. We present here Super-AGILE, an X-ray detector added on top of the gamma-ray tracker. Super-AGILE will have a large field of view, providing hard X-ray imaging and moderate spectroscopy together with the gamma-ray detector. Super-AGILE is composed by Si-microstrip detectors, equipped with a low-noise electronics allowing a sensitive range of 10-40 keV, and coupled with a set of mutually orthogonal one-dimensional coded masks. A bi-dimensional source location capability is obtained by dividing the total 1444 cm2 geometric area of the detectors in two orthogonal directions. .
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The IUE archive data on blazars are reconsidered. They refer to 47 objects, 24 radio-strong BL Lac objects, 15 radio-weak BL Lac objects, and eight optically violently variable quasars, increasing substantially the sample examined by Ghisellini et al. (1986). For each object a dereddened spectral slope is evaluated starting from the extraction of Kinney et al. (1991) and Edelson et al. (1992), and deriving the extinction from the hydrogen column density obtained through radio data. The 1200-3000 Å average spectral index is found to be α ≃ 1, with radio-strong BL Lac objects being steeper (αν ≃ 1.2) than radio-weak ones (αν ≃ 0.7). The behavior of blazars in the UV does not depart much from that of PG quasars for which the average spectral index is αν ≃ ≃ 0.8. Comparing with recent results of Falomo et al. (1993a) on the infrared-optical continuum of blazars we find no indication of a steepening in the 8 × 1013 -2 × 1015 Hz band, while the extrapolation to soft X-rays indicates at most a modest steepening.
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An analysis of observations of 50 radio-loud and radio-quiet quasars made by the X-ray satellite Ginga is presented. The spectra are the most accurate and sensitive yet obtained in the 2-20 keV band, and provide a unique opportunity to study the X-ray emission from these faint, although highly luminous, objects. The properties of the hard X-ray continuum are compatible with those of previous quasar surveys, with a highly significant variation of observed spectral indices which is unlikely to be due either to the radio heterogeneity of the sample or to spectral variability. The spectral variability shows no direct link to changes in luminosity. The spectra of the radio-quiet quasars are generally consistent with those of Seyfert galaxies, in support of current unification schemes, and there is also some evidence for the presence of Compton reflection and ionized absorption. However, a comparatively high percentage of quasars with soft spectra indicates that these features are unlikely to be present in all radio-quiet quasars. A comparison with recent ASCA observations of distant radio-quiet sources suggests that we may be seeing the start of a spectral transition between the low-luminosity Seyfert galaxies and these more powerful distant objects. It is shown for the first time that there is a definite range in the spectral index of radio-loud objects. Whether or not this is a direct indication of differing physical parameters in the nuclei of these objects is not known. It is possible that it is indirectly due to the observed relationship between radio core dominance and spectral index which has also been seen using the Einstein observatory. This relationship can be explained using a two-component beaming model, which also provides an explanation for the measured iron line strengths of the radio-loud objects.
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We investigate the X-ray properties of the Parkes sample of flat-spectrum radio sources using data from the ROSAT All-Sky Survey and archival pointed PSPC observations. In total, 163 of the 323 sources are detected. For the remaining 160 sources, 2σ upper limits to the X-ray flux are derived. We present power-law photon indices in the 0.1–2.4 keV energy band for 115 sources, which were determined either with a hardness ratio technique or from direct fits to pointed PSPC data if a sufficient number of photons were available. The average photon index is 〈Γ〉 = 1.95−0.12+0.13 for flat-spectrum radio-loud quasars, 〈Γ〉 = 1.70−0.24+0.23 for galaxies, and 〈Γ〉 = 2.40−0.31+0.12 for BL Lac objects. The soft X-ray photon index is correlated with redshift and with radio spectral index in the sense that sources at high redshift and/or with flat (or inverted) radio spectra have flatter X-ray spectra on average. The results are in accord with orientation-dependent unification schemes for radio-loud active galactic nuclei. Webster et al. discovered many sources with unusually red optical continua among the quasars of this sample, and interpreted this result in terms of extinction by dust. Although the X-ray spectra in general do not show excess absorption, we find that low-redshift optically red quasars have significantly lower soft X-ray luminosities on average than objects with blue optical continua. The difference disappears for higher redshifts, as is expected for intrinsic absorption by cold gas associated with the dust. In addition, the scatter in log (fx/fo) is consistent with the observed optical extinction, contrary to previous claims based on optically or X-ray selected samples. Although alternative explanations for the red optical continua cannot be excluded with the present X-ray data, we note that the observed X-ray properties are consistent with the idea that dust plays an important role in some of the radio-loud quasars with red optical continua.
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AGILE is a γ-ray astrophysics space mission which will operate, starting from 2006, in the 30 MeV–50 GeV energy range with imaging capability also in the 15–45 keV energy band. In order to achieve the required detection sensitivity, all AGILE detectors are surrounded by an anticoincidence detector aimed at charged particle background rejection with an inefficiency as low as 10−4. In this work, the design and the structure of this anticoincidence detector are presented, as well as its performances in terms of charged particles detection inefficiency as derived from extensive calibrations performed at CERN PS.