782 research outputs found
Short timescale variations of the H{\alpha} double-peaked profile of the nucleus of NGC 1097
The broad (FWHM ~ 10,000 km/s) double-peaked H{\alpha} profile from the
LINER/Seyfert 1 nucleus of NGC 1097 was discovered in 1991, and monitored for
the following 11 years. The profile showed variations attributed to the
rotation of gas in a non-axisymmetric Keplerian accretion disk, ionized by a
varying radiatively inefficient accretion flow (RIAF) located in the inner
parts of the disk. We present and model 11 new spectroscopic observations of
the double-peaked profile taken between 2010 March and 2011 March. This series
of observations was motivated by the finding that in 2010 March the flux in the
double-peaked line was again strong, becoming, in 2010 December, even stronger
than in the observations of a decade ago. We also discovered shorter timescale
variations than in the previous observations: (1) the first, of ~7 days, is
interpreted as due to "reverberation" of the variation of the ionizing source
luminosity, and the timescale of 7 days as the light crossing time between the
source and the accretion disk; this new timescale and its interpretation
provides a distance between the emitting gas and the supermassive black hole
and as such introduces a new constraint on its mass; (2) the second, of
approximately 5 months, was attributed to the rotation of a spiral arm in the
disk, which was found to occur on the dynamical timescale. We use two accretion
disk models to fit theoretical profiles to the new data, both having
non-axisymmetric emissivities produced by the presence of an one-armed spiral.
Our modeling constrains the rotation period for the spiral to be approximately
18 months. This work supports our previous conclusion that the broad
double-peaked Balmer emission lines in NGC 1097, and probably also in other
low-luminosity active nuclei, originate from an accretion disk ionized by a
central RIAF.Comment: Published in ApJ (2012 March). 13 pages, 11 figure
Extended Gas in Seyfert Galaxies: Near Infrared Observations of NGC 2110 and Circinus
We present results of near--IR long-slit spectroscopy in the J and K bands of
the Seyfert 2 galaxies NGC 2110 and Circinus, investigating the gaseous
distribution, excitation, reddening and kinematics. In NGC 2110, the emission
line ratio [FeII]/Pa beta increases towards the nucleus (to ~ 7). The nuclear
[Fe II]1.257 (microns) and Pa beta lines are broader (FWHM ~ 500 km/s) than the
H2 (2.121) line (FWHM ~ 300 km/s). Both these results suggest that shocks,
driven by the radio jet, are an important source of excitation of [Fe II]. The
H2 excitation appears to be dominated by X-rays from the nucleus. In Circinus,
both [FeII]/Pa beta and H2/Br gamma decrease from ~ 2 at 4 arcsec from the
nucleus to nuclear values of ~ 0.6 and ~ 1, respectively, suggesting that the
starburst dominates the nuclear excitation, while the AGN dominates the
excitation further out (r > 2 arcsec). For both galaxies, the gaseous
kinematics are consistent with circular rotation in the plane of the disk. Our
rotation curves suggest that the nucleus (identified with the peak of the IR
continuum) is displaced from the kinematic centre of the galaxies. This effect
has been observed previously in NGC 2110 based on the kinematics of optical
emission lines, but the displacement is smaller in the infrared, suggesting the
effect is related to obscuration. The continuum J-K colours of the nuclear
region indicate a red stellar population in NGC 2110 and a reddened young
stellar population in Circinus. Right at the nucleus of both galaxies, the
colours are redder, apparently a result of hot dust emission from the inner
edge of a circumnuclear torus.Comment: 11 pages, 14 figures, accepted for publication in MNRA
Extended Gas in Seyfert Galaxies: Near-Infrared Observations of 15 Active Nuclei
Results from an analysis of low resolution (R~250) near-IR long-slit spectra
covering simultaneously the I, J, H, and K bands, for a sample of 15 Seyfert
galaxies and the N5253 starburst nucleus, are presented. The Seyfert galaxies
were selected as presenting `linear' or cone-like high excitation emission line
in the optical, most probably due to the collimation of the central source's
radiation by a dusty molecular torus. Our goal was to look for signatures of
this torus, and to investigate the gaseous distribution, excitation and
reddening. The IR emission lines are spatially extended in most cases, and we
have used the [FeII]/Pa(beta) ratio as a measure of the gaseous excitation in
Mrk573, N1386, and N7582. Values for this ratio between 1.5 and 6 are found,
suggesting excitation of [FeII] by X-rays or shock waves in some regions.
Nuclear Pa(beta) in N1365, and possibly nuclear Br(gama) in Mrk573, are broad.
From analysis of the spatial distribution of the continuum (J-H) and (H-K)
colours derived from our spectra, we find redder colours for the nucleus than
the nearby bulge in most of the Seyfert 2s observed. Comparison with models
including emission from dust and stars shows that hot (T~1000 K) dust emission
dominates the nuclear continuum in N1365, N2110, N3281, N7582, and ESO362-G18.
In N1386, N5643, and N5728 the main contributor is the underlying stellar
population, combined with some foreground reddening and/or cool dust emission.
In a few cases, the (J-H) colours on opposite sides of the nucleus differ by
0.3-0.8 mag, an effect that we interpret as partly due to differences in the
local stellar population, and possibly extinction gradients.Comment: 19 pages (LaTeX, mn.sty), 27 Postscript figures embedded. Accepted
for publication in the Monthly Notices of the R.A.
Short-Timescale monitoring of the X-ray, UV and broad double-peak emission line of the nucleus of NGC 1097
Recent studies have suggested that the short-timescale ( days)
variability of the broad (10,000 km s) double-peaked H
profile of the LINER nucleus of NGC1097 could be driven by a variable X-ray
emission from a central radiatively inefficient accretion flow (RIAF). To test
this scenario, we have monitored the NGC1097 nucleus in X-ray and UV continuum
with Swift and the H flux and profile in the optical spectrum using
SOAR and Gemini-South from 2012 August to 2013 February. During the monitoring
campaign, the H flux remained at a very low level --- 3 times lower
than the maximum flux observed in previous campaigns and showing only limited
() variability. The X-ray variations were small, only
throughout the campaign, while the UV did not show significant variations. We
concluded that the timescale of the H profile variation is close to the
sampling interval of the optical observations, which results in only marginal
correlation between the X-ray and H fluxes. We have caught the AGN in
NGC1097 in a very low activity state, in which the ionizing source was very
weak and capable of ionizing just the innermost part of the gas in the disk.
Nonetheless, the data presented here still support the picture in which the gas
that emits the broad double-peaked Balmer lines is illuminated/ionized by a
source of high-energy photons which is located interior to the inner radius of
the line-emitting part of the disk.Comment: The paper contains 14 pages, 7 figures and is accepted for
publication at the Astrophysical Journa
The circadian clock in the diatom <i>Phaeodactylum tricornutum</i>
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The Earliest Near-infrared Time-series Spectroscopy of a Type Ia Supernova
We present ten medium-resolution, high signal-to-noise ratio near-infrared
(NIR) spectra of SN 2011fe from SpeX on the NASA Infrared Telescope Facility
(IRTF) and Gemini Near-Infrared Spectrograph (GNIRS) on Gemini North, obtained
as part of the Carnegie Supernova Project. This data set constitutes the
earliest time-series NIR spectroscopy of a Type Ia supernova (SN Ia), with the
first spectrum obtained at 2.58 days past the explosion and covering -14.6 to
+17.3 days relative to B-band maximum. C I {\lambda}1.0693 {\mu}m is detected
in SN 2011fe with increasing strength up to maximum light. The delay in the
onset of the NIR C I line demonstrates its potential to be an effective tracer
of unprocessed material. For the first time in a SN Ia, the early rapid decline
of the Mg II {\lambda}1.0927 {\mu}m velocity was observed, and the subsequent
velocity is remarkably constant. The Mg II velocity during this constant phase
locates the inner edge of carbon burning and probes the conditions under which
the transition from deflagration to detonation occurs. We show that the Mg II
velocity does not correlate with the optical light-curve decline rate
{\Delta}m15. The prominent break at ~1.5 {\mu}m is the main source of concern
for NIR k-correction calculations. We demonstrate here that the feature has a
uniform time evolution among SNe Ia, with the flux ratio across the break
strongly correlated with {\Delta}m15. The predictability of the strength and
the onset of this feature suggests that the associated k-correction
uncertainties can be minimized with improved spectral templates.Comment: 14 pages, 13 figures, accepted for publication in Ap
The origin of the Narrow Line Region of Mrk 3: an overpressured jet cocoon
We have obtained HST FOC long-slit optical spectroscopy of the Narrow Line
Region of the Seyfert 2 galaxy Mrk 3. In the region cospatial with the
radio-jet the velocity field is highly perturbed and shows two velocity systems
separated by as much as 1700 km/s. We interpret this to be the consequence of
the rapid expansion of a cocoon of hot gas, shocked and heated by the
radio-emitting outflow, which compresses and accelerates the ambient gas. The
NLR itself is essentially a cylindrical shell expanding supersonically. From
the size and velocity of the expanding region, we derive an upper limit to the
radio-source age, ~ 2
E42 erg/s required to inflate the cocoon and estimate that the jet minimum
advance speed is 3 E-3 pc per year. The total kinetic energy of the high
velocity NLR gas can be estimated as ~6 E54 erg, comparable to the total energy
carried by the jet over its lifetime and this quantitatively supports the idea
that the NLR gas is accelerated by the jet. If the advance speed of Mrk 3 is
representative of the Seyfert population then these sources must also be short
lived and probably recurrent. The jet kinetic luminosity of Mrk 3 is between 2
and 3 orders of magnitude smaller than that derived for radio-loud AGNs with
similar emission-line luminosity. On the other hand, the fraction of jet power
dissipated in radio-emission is similar. We speculate that the main distinction
between radio-quiet and radio-loud AGN is ascribed to a difference in jet power
rather than to a different efficiency in synchrotron emission production.Comment: 13 pages, 8 figures, Astrophysical Journal in pres
Mass of the Southern Black Hole in NGC 6240 from Laser Guide Star Adaptive Optics
NGC 6240 is a pair of colliding disk galaxies, each with a black hole in its
core. We have used laser guide star adaptive optics on the Keck II telescope to
obtain high-resolution (") near-infrared integral-field spectra of
the region surrounding the supermassive black hole in the south nucleus of this
galaxy merger. We use the K-band CO absorption bandheads to trace stellar
kinematics. We obtain a spatial resolution of about 20 pc and thus directly
resolve the sphere of gravitational influence of the massive black hole. We
explore two different methods to measure the black hole mass. Using a Jeans
Axisymmetric Multi-Gaussian mass model, we investigate the limit that a relaxed
mass distribution produces all of the measured velocity dispersion, and find an
upper limit on the black hole mass at 2.0 \pm 0.2 \times 10^9 M_{\sun}. When
assuming the young stars whose spectra we observe remain in a thin disk, we
compare Keplerian velocity fields to the measured two-dimensional velocity
field measured and fit for a mass profile containing a black hole point mass
plus a radially-varying spherical component, which suggests a lower limit for
the black hole mass of 8.7 \pm 0.3 \times 10^8 M_{\sun}. Our measurements of
the stellar velocity dispersion place this AGN within the scatter of the
- relation. As NGC 6240 is a merging system, this may
indicate that the relation is preserved during a merger at least until the
final coalescence of the two nuclei.Comment: 10 pages, 12 figures; accepted to Ap
Primary structure and spectroscopic studies of Neurospora copper metallothionein.
When Neurospora crassa is grown in the presence of Cu(II) ions, it accumulates the metal with the concomitant synthesis of a low molecular weight copper-binding protein. The molecule binds 6 g-atom of copper per mole protein (Mr = 2200) and shows a striking sequence homology to the zinc- and cadmium-binding vertebrate metallothioneins. Absorption, circular dichroism, and electron paramagnetic resonance spectroscopy of Neurospora metallothionein indicate the copper to be bound to cysteinyl residues as a Cu(I)-thiolate complex of the polymeric mu-thiolate structure [Cu(I)6RS7]-. This metal-binding mode is also in agreement with the unusual luminescence of the protein. Spectral perturbation studies with HgCl2 and p-(chloromercuri)benzoate suggest that the 6 Cu(I)ions are coordinated to the seven cysteinyl residues in the form of a single metal cluster. Neurospora apometallothionein is also capable of binding in vivo group IIB metal ions [Zn(II), Cd(II), and Hg(II)] as well as paramagnetic Co(II) ions with an overall metal-to-protein stoichiometry of 3. The spectroscopic properties of the fully substituted forms are indicative of a distorted tetrahedral coordination. However, metal titration of the apoprotein shows the third metal ion to be differently coordinated than the other two metal ions. This difference can be explained by the presence of only seven cysteine residues in Neurospora metallothionein as opposed to nine cysteine residues in the three-metal cluster of the mammalian metallothioneins
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