926 research outputs found
Modeling the time-dependent polarization of blazars
Linear polarization is an extremely valuable observational tool for probing the dynamic physical conditions of blazar jets. Some patterns are seen in the data, suggestive of order that can be explained by shock waves and helical magnetic field components. However, much disorder is apparent, which implies that turbulence plays a major role as well, especially in the fluctuations of flux and polarization, and perhaps particle acceleration. Here, we present some actual flux and polarization versus time data, plus simulations of model jets. We analyze the output of the simulations in a manner that can be compared with observational data. The results suggest that the ratio of turbulent to ordered magnetic fields varies with time.AST-1615796 - National Science Foundation; NASA; NNX14AQ58G; NNX15AR45
Multiwavelength Variations of 3C 454.3 during the November 2010 to January 2011 Outburst
We present multiwavelength data of the blazar 3C 454.3 obtained during an
extremely bright outburst from November 2010 through January 2011. These
include flux density measurements with the Herschel Space Observatory at five
submillimeter-wave and far-infrared bands, the Fermi Large Area Telescope at
gamma-ray energies, Swift at X-ray, ultraviolet (UV), and optical frequencies,
and the Submillimeter Array at 1.3 mm. From this dataset, we form a series of
52 spectral energy distributions (SEDs) spanning nearly two months that are
unprecedented in time coverage and breadth of frequency. Discrete correlation
anlaysis of the millimeter, far-infrared, and gamma-ray light curves show that
the variations were essentially simultaneous, indicative of co-spatiality of
the emission, at these wavebands. In contrast, differences in short-term
fluctuations at various wavelengths imply the presence of inhomegeneities in
physical conditions across the source. We locate the site of the outburst in
the parsec-scale core, whose flux density as measured on 7 mm Very Long
Baseline Array images increased by 70 percent during the first five weeks of
the outburst. Based on these considerations and guided by the SEDs, we propose
a model in which turbulent plasma crosses a conical standing shock in the
parsec-scale region of the jet. Here, the high-energy emission in the model is
produced by inverse Compton scattering of seed photons supplied by either
nonthermal radiation from a Mach disk, thermal emission from hot dust, or (for
X-rays) synchrotron radiation from plasma that crosses the standing shock. For
the two dates on which we fitted the model SED to the data, the model
corresponds very well to the observations at all bands except at X-ray
energies, where the spectrum is flatter than observed.Comment: Accepted for publication in Astrophysical Journal. 82 pages, 13
figure
Time dependent spectral modeling of Markarian 421 during a violent outburst in 2010
We present the results of extensive modeling of the spectral energy
distributions (SEDs) of the closest blazar (z=0.031) Markarian 421 (Mrk 421)
during a giant outburst in February 2010. The source underwent rapid flux
variations in both X-rays and very high energy (VHE) gamma-rays as it evolved
from a low-flux state on 2010 February 13-15 to a high-flux state on 2010
February 17. During this period, the source exhibited significant spectral
hardening from X-rays to VHE gamma-rays while exhibiting a "harder when
brighter" behavior in these energy bands. We reproduce the broadband SED using
a time-dependent multi-zone leptonic jet model with radiation feedback. We find
that an injection of the leptonic particle population with a single power-law
energy distribution at shock fronts followed by energy losses in an
inhomogeneous emission region is suitable for explaining the evolution of Mrk
421 from low- to high-flux state in February 2010. The spectral states are
successfully reproduced by a combination of a few key physical parameters, such
as the maximum minimum cutoffs and power-law slope of the electron
injection energies, magnetic field strength, and bulk Lorentz factor of the
emission region. The simulated light curves and spectral evolution of Mrk 421
during this period imply an almost linear correlation between X-ray flux at
1-10 keV energies and VHE gamma-ray flux above 200 GeV, as has been previously
exhibited by this source. Through this study, a general trend that has emerged
for the role of physical parameters is that, as the flare evolves from a low-
to a high-flux state, higher bulk kinetic energy is injected into the system
with a harder particle population and a lower magnetic field strength.Comment: 13 pages, 5 figures, accepted for publication in MNRA
Blazar 3C 454.3 in Outburst and Quiescence During 2005-2007: Two Variable Synchrotron Emission Peaks
We monitored the flaring blazar 3C 454.3 during 2005 June-July with the
Spitzer Infrared Spectrograph (IRS: 15 epochs), Infrared Array Camera (IRAC: 12
epochs) and Multiband Imaging Photometer (MIPS: 2 epochs). We also made Spitzer
IRS, IRAC, and MIPS observations from 2006 December-2007 January when the
source was in a low state, the latter simultaneous with a single Chandra X-ray
observation. In addition, we present optical and sub-mm monitoring data. The
2005-2007 period saw 3 major outbursts. We present evidence that the
radio-optical SED actually consists of two variable synchrotron peaks, the
primary at IR and the secondary at sub-mm wavelengths. The lag between the
optical and sub-mm outbursts may indicate that these two peaks arise from two
distinct regions along the jet separated by a distance of 0.07-5 pc. The flux
at 5-35 microns varied by a factor of 40 and the IR peak varied in frequency
from <1E13 Hz to 4E13 Hz between the highest and lowest states in 2005 and
2006, respectively. Variability was well correlated across the mid-IR band,
with no measurable lag. Flares that doubled in flux occurred on a time scale of
3 days. The IR SED peak moved to higher frequency as a flare brightened, then
returned to lower frequency as it decayed. The fractional variability amplitude
increased with frequency, which we attribute to decreasing synchrotron-self
absorption optical depth. Mid-IR flares may signal the re-energization of a
shock that runs into inhomogeneities along the pre-existing jet or in the
external medium. The synchrotron peak frequencies during each major outburst
may depend upon both the distance from the jet apex and the physical conditions
in the shocks. Variation of the Doppler parameter along a curved or helical jet
is another possibility. Frequency variability of the IR synchrotron peak may
have important consequences for the interpretation of the blazar sequence, and
the presence of a secondary peak may give insight into jet structure.Comment: 38 pages, 15 figures, submitted to ApJS, comments welcom
LOFAR observations of 4C+19.44. On the discovery of low frequency spectral curvature in relativistic jet knots
We present the first LOFAR observations of the radio jet in the quasar
4C+19.44 (a.k.a. PKS 1354+19) obtained with the long baselines. The achieved
resolution is very well matched to that of archival Jansky Very Large Array
(JVLA) observations at higher radio frequencies as well as the archival X-ray
images obtained with {\it Chandra}. We found that, for several knots along the
jet, the radio flux densities measured at hundreds of MHz lie well below the
values estimated by extrapolating the GHz spectra. This clearly indicates the
presence of spectral curvature. Radio spectral curvature has been already
observed in different source classes and/or extended radio structures and it
has been often interpreted as due to intrinsic processes, as a curved particle
energy distribution, rather than absorption mechanisms ({ Razin-Tsytovich}
effect, free-free or synchrotron self absorption to name a few). Here we
discuss our results according to the scenario where particles undergo
stochastic acceleration mechanisms also in quasar jet knots.Comment: 13 pages, 4 tables, 4 figures, pre-proof version, published on the
Astrophysical Journal (Harris, et al. 2019 ApJ, 873, 21
Behaviour of the Blazar CTA 102 during two giant outbursts
Blazar CTA 102 underwent exceptional optical and high-energy outbursts in 2012 and 2016-2017. We analyze its behaviour during these events, focusing on polarimetry as a tool that allows us to trace changes in the physical conditions and geometric configuration of the emission source close to the central black hole. We also use Fermi gamma-ray data in conjunction with optical photometry in an effort to localize the origin of the outbursts.AST-1615796 - Boston Universit
MOJAVE: Monitoring of Jets in AGN with VLBA Experiments. VII. Blazar Jet Acceleration
We discuss acceleration measurements for a large sample of extragalactic
radio jets from the MOJAVE program which studies the parsec-scale jet structure
and kinematics of a complete, flux-density-limited sample of Active Galactic
Nuclei (AGN). Accelerations are measured from the apparent motion of individual
jet features or "components" which may represent patterns in the jet flow. We
find that significant accelerations are common both parallel and perpendicular
to the observed component velocities. Parallel accelerations, representing
changes in apparent speed, are generally larger than perpendicular acceleration
that represent changes in apparent direction. The trend for larger parallel
accelerations indicates that a significant fraction of these changes in
apparent speed are due to changes in intrinsic speed of the component rather
than changes in direction to the line of sight. We find an overall tendency for
components with increasing apparent speed to be closer to the base of their
jets than components with decreasing apparent speed. This suggests a link
between the observed pattern motions and the underlying flow which, in some
cases, may increase in speed close to the base and decrease in speed further
out; however, common hydro-dynamical processes for propagating shocks may also
play a role. About half of the components show "non-radial" motion, or a
misalignment between the component's structural position angle and its velocity
direction, and these misalignments generally better align the component motion
with the downstream emission. Perpendicular accelerations are closely linked
with non-radial motion. When observed together, perpendicular accelerations are
usually in the correct direction to have caused the observed misalignment.Comment: 17 pages, 11 figures, 1 table, accepted by the Astrophysical Journa
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