142,537 research outputs found
Jet emission in NGC1052 at radio, optical, and X-ray frequencies
We present a combined radio, optical, and X-ray study of the nearby LINER
galaxy NGC 1052. Data from a short (2.3 ksec) {\it CHANDRA} observation of NGC
1052 reveal the presence of various jet-related X-ray emitting regions, a
bright compact core and unresolved knots in the jet structure as well as an
extended emitting region inside the galaxy well aligned with the radio
synchrotron jet-emission. The spectrum of the extended X-ray emission can best
be fitted with a thermal model with keV, while the compact
core exhibits a very flat spectrum, best approximated by an absorbed power-law
with . We compare the radio
structure to an optical ``structure map'' from a {\it Hubble Space Telescope}
({\it HST}) observation and find a good positional correlation between the
radio jet and the optical emission cone. Bright, compact knots in the jet
structure are visible in all three frequency bands whose spectrum is
inconsistent with synchrotron emission.Comment: 8 pages, 5 figures (figure 2 in color), image resolution degraded wrt
journal version, needs aa.cls. Accepted for publication in A&
The compact radio structure of radio-loud narrow line Seyfert 1 galaxies
We present the compact radio structure of three radio-loud narrow line
Seyfert 1 galaxies from VLBA archive data at 2.3, 5 and 8.4 GHz. In RXS
J16290+4007, the radio structure is mostly unresolved. The combination of
compact radio structure, high brightness temperature and inverted spectrum
between simultaneous 2.3 and 8.4 GHz, strongly favors jet relativistic beaming.
Combining with the VLBI data at 1.6 and 8.4 GHz from literatures, we argued
that RXS J16333+4718 may also harbor a relativistic jet, with resolved core-jet
structure in 5 GHz. B3 1702+457 is clearly resolved with well defined jet
component. The overall radio steep spectrum indicates that B3 1702+457 is
likely a source optically defined as NLS1 with radio definition of compact
steep spectrum sources. From these three sources, we found that radio loud
NLS1s can be either intrinsically radio loud (e.g. B3 1702+457), or apparently
radio loud due to jet beaming effect (e.g. RXS J16290+4007 and RXS
J16333+4718).Comment: 20 pages, 3 figures, accepted for publication in The Astronomical
Journa
The Radio Properties of Radio-Loud Narrow-Line Seyfert 1 Galaxies on Parsec Scales
We present the detection of compact radio structures of fourteen radio-loud
narrow line Seyfert 1 (NLS1) galaxies from Very Long Baseline Array
observations at 5 GHz, which were performed in 2013. While 50\% of the sources
of our sample show a compact core only, the remaining 50\% exhibit a core-jet
structure. The measured brightness temperatures of the cores range from
to K with a median value of K, indicating
that the radio emission is from non-thermal jets, and that, likely, most
sources are not strongly beamed, then implying a lower jet speed in these
radio-loud NLS1 galaxies. In combination with archival data taken at multiple
frequencies, we find that seven sources show flat or even inverted radio
spectra, while steep spectra are revealed in the remaining seven objects.
Although all these sources are very radio-loud with , their jet
properties are diverse, in terms of their milli-arcsecond (mas) scale (pc
scale) morphology and their overall radio spectral shape. The evidence for slow
jet speeds (i.e., less relativistic jets), in combination with the low
kinetic/radio power, may offer an explanation for the compact VLBA radio
structure in most sources. The mildly relativistic jets in these high accretion
rate systems are consistent with a scenario, where jets are accelerated from
the hot corona above the disk by the magnetic field and the radiation force of
the accretion disk. Alternatively, a low jet bulk velocity can be explained by
low spin in the Blandford-Znajek mechanism.Comment: 39 pages, 17 figures, ApJS accepte
Bi-Directional Relativistic Jets of the Radio Galaxy 1946+708: Constraints on the Hubble Constant
We present measurements of bi-directional motions in the jets of the radio
galaxy 1946+708 at z=0.101. This is a Compact Symmetric Object with striking
S-symmetry. Sensitive 15 GHz observations reveal a compact component at the
center of symmetry with a strongly inverted spectrum, that we identify as the
core. From five 4.9 GHz observations spread over 4 years we have determined the
velocities of four compact jet components. If simple kinematic models can be
applied then the inclination of the source and the bulk jet velocity can be
directly determined for any assumed value of the Hubble constant. Conversely,
the measurements already place constraints on the Hubble constant, and we show
how further observations of 1946+708 can yield an increasingly accurate
determination of H_0.Comment: in press at ApJ Letters, 12 page LaTex document includes 5 postscript
figure
Fast TeV variability in blazars: jets in a jet
The fast TeV variability of the blazars Mrk 501 and PKS 2155--304 implies a
compact emitting region that moves with a bulk Lorentz factor of Gamma_{em}~100
toward the observer. The Lorentz factor is clearly in excess of the jet Lorentz
factors Gamma_j\simless 10 measured on sub-pc scales in these sources. We
propose that the TeV emission originates from compact emitting regions that
move relativistically {\it within} a jet of bulk Gamma_j~10. This can be
physically realized in a Poynting flux-dominated jet. We show that if a large
fraction of the luminosity of the jet is prone to magnetic dissipation through
reconnection, then material outflowing from the reconnection regions can
efficiently power the observed TeV flares through synchrotron-self-Compton
emission. The model predicts simultaneous far UV/soft X-ray flares.Comment: Moderate changes to match the published version, MNRAS, 395, L29
(2009
3D simulations of microquasar jets in clumpy stellar winds
High-mass microquasars consist of a massive star and a compact object, the
latter producing jets that will interact with the stellar wind. The evolution
of the jets, and ultimately their radiative outcome, could depend strongly on
the inhomogeneity of the wind, which calls for a detailed study. The
hydrodynamics of the interaction between a jet and a clumpy wind is studied,
focusing on the global wind and single clump-jet interplay. We have performed,
using the code \textit{Ratpenat}, three-dimensional numerical simulations of a
clumpy wind interacting with a mildly relativistic jet, and of individual
clumps penetrating into a jet. For typical wind and jet velocities, filling
factors of about > 0.1 are already enough for the wind to be considered as
clumpy. An inhomogeneous wind makes the jet more unstable when crossing the
system. Kinetic luminosities of the order 1.e37 erg/s allow the jet to reach
the borders of a compact binary with an O star, as in the smooth wind case,
although with a substantially higher degree of disruption. When able to enter
into the jet, clumps are compressed and heated during a time of about their
size divided by the sound speed in the shocked clump. Then, clumps quickly
disrupt, mass-loading and slowing down the jet. We conclude that moderate wind
clumpiness makes already a strong difference with the homogeneous wind case,
enhancing jet disruption, mass-loading, bending, and likely energy dissipation
in the form of emission. All this can have observational consequences at
high-energies and also in the large scale radio jets.Comment: Accepted for publication in Astronomy & Astrophysics. The quality of
the images has been reduced to fit into arXiv requirement
Jet-driven and jet-less fireballs from compact binary mergers
During a compact binary merger involving at least one neutron star, a small
fraction of the gravitational energy could be liberated in such a way to
accelerate a small fraction (~ 10^-6) of the neutron star mass in an isotropic
or quasi-isotropic way. In presence of certain conditions, a pair-loaded
fireball can form, which undergoes accelerated expansion reaching relativistic
velocities. As in the standard fireball scenario, internal energy is partly
transformed into kinetic energy. At the photospheric radius, the internal
radiation can escape, giving rise to a pulse that lasts for a time equal to the
delay time since the merger. The subsequent interaction with the interstellar
medium can then convert part of the remaining kinetic energy back into
radiation in a weak isotropic afterglow at all wavelengths. This scenario does
not require the presence of a jet: the associated isotropic prompt and
afterglow emission should be visible for all NS-NS and BH-NS mergers within 90
Mpc, independent of their inclination. The prompt emission is similar to that
expected from an off-axis jet, either structured or much slower than usually
assumed (Gamma ~ 10), or from the jet cocoon. The predicted afterglow emission
properties can discriminate among these scenarios.Comment: 5 pages, 1 figure, revised version submitted to MNRAS Letter
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