160 research outputs found
Host galaxies of bright high redshift quasars: Luminosities and colours
We present the results of a near-infrared imaging study of high redshift
(z~3) quasars using the ESO-VLT. Our targets were selected to have luminosities
among the highest known (absolute magnitude M_B <~ -28. We searched for
resolved structures underlying the bright point-source nuclei by comparing the
QSO images with stars located in the same fields. Two QSOs (HE2348-1444 at
z=2.904 and HE2355-5457 at z=2.933) are clearly resolved in K_S, and with
somewhat lower significance also in H; one object is resolved only in K_S. At
these redshifts, H and K_S correspond almost exactlly to rest-frame B and V,
respectively, with virtually no K-correction. We also report briefly the
non-detection of some additional QSOs. The detected host galaxies are extremely
luminous with M_V ~ -25. Their rest-frame B-V colours, however, are close to
zero in the Vega system, indicating substantial contributions from young stars
and a stellar mass-to-light ratio below 1 (in solar units). Tentatively
converting M_V and B-V into rough estimates of stellar masses, we obtain values
of M_star in the range of several 10^11 M_sun, placing them within the
high-mass range of recent high-redshift galaxy surveys. We present optical
spectra and use CIV line width measurements to predict virial black hole
masses, obtaining typical values of M_bh ~ 5x10^9 M_sun. With respect to the
known correlation between host galaxy luminosity L_V(host) and M_bh, our
measurements reach to higher luminosities and redshifts than previous studies,
but are completely consistent with them. Comparing our objects with the local
(z~0) M_bh - M_bulge relation and taking also the low stellar mass-to-light
ratios into account, we find tentative evidence for an excess in the
M_bh/M_bulge mass ratio at z~3.Comment: 9 pages, 7 figures, accepted for publication in A&
Decomposition of AGN host galaxy images
We describe an algorithm to decompose deep images of Active Galactic Nuclei
into host galaxy and nuclear components. Currently supported are three galaxy
models: A de-Vaucouleurs spheroidal, an exponential disc, and a two-component
disc+bulge model. Key features of the method are: (semi-)analytic
representation of a possibly spatially variable point-spread function; full
two-dimensional convolution of the model galaxy using gradient-controlled
adaptive subpixelling; multiple iteration scheme. The code is computationally
efficient and versatile for a wide range of applications. The quantitative
performance is measured by analysing simulated imaging data. We also present
examples of the application of the method to small test samples of nearby
Seyfert 1 galaxies and quasars at redshifts z < 0.35.Comment: 12 pages, 15 figures, accepted for publication in MNRA
On-axis spatially resolved spectroscopy of low redshift quasar host galaxies: HE 1503+0228 at z=0.135
We present the first result of a comprehensive spectroscopic study of quasar
host galaxies. On-axis, spatially resolved spectra of low redshift quasars have
been obtained with FORS1, mounted on the 8.2m ESO Very Large Telescope, Antu.
The spectra are spatially deconvolved using a spectroscopic version of the
``MCS deconvolution algorithm''. The algorithm decomposes two dimensional
spectra into the individual spectra of the central point-like nucleus and of
its host galaxy. Applied to HE1503+0228, at z=0.135 (M_B=-23.0), it provides us
with the spectrum of the host galaxy between 3600A, and 8500A, (rest-frame), at
a mean resolving power of 700. The data allow us to measure several of the
important Lick indices. The stellar populations and gas ionization state of the
host galaxy of HE1503+0228, are very similar to the ones measured for normal
non-AGN galaxies. Dynamical information is also available for the gas and
stellar components of the galaxy. Using deconvolution and a deprojection
algorithm, velocity curves are derived for emission lines, from the center up
to 4arcsec, away from the nucleus of the galaxy. Fitting a simple
three-components mass model (point mass, spherical halo of dark matter, disk)
to the position-velocity diagram, we infer a mass of M(r<1kpc) = (2.0 +- 0.3)
10^{10} solar mass within the central kiloparsec of the galaxy, and a mass
integrated over 10 kpc of M(r<10kpc) = (1.9 +- 0.3) 10^{11} solar mass, with an
additional 10% error due to the uncertainty on the inclination of the galaxy.
This, in combination with the analysis of the stellar populations indicates
that the host galaxy of HE1503+0228, is a normal spiral galaxy.Comment: accepted by AA, 11 page
Decreasing intensity of open-ocean convection in the Greenland and Iceland seas
The air–sea transfer of heat and fresh water plays a critical role in the global climate system. This is particularly true for the Greenland and Iceland seas, where these fluxes drive ocean convection that contributes to Denmark Strait overflow water, the densest component of the lower limb of the Atlantic Meridional Overturning Circulation (AMOC). Here we show that the wintertime retreat of sea ice in the region, combined with different rates of warming for the atmosphere and sea surface of the Greenland and Iceland seas, has resulted in statistically significant reductions of approximately 20% in the magnitude of the winter air–sea heat fluxes since 1979. We also show that modes of climate variability other than the North Atlantic Oscillation (NAO) are required to fully characterize the regional air–sea interaction. Mixed-layer model simulations imply that further decreases in atmospheric forcing will exceed a threshold for the Greenland Sea whereby convection will become depth limited, reducing the ventilation of mid-depth waters in the Nordic seas. In the Iceland Sea, further reductions have the potential to decrease the supply of the densest overflow waters to the AMOC
Changes in global ocean bottom properties and volume transports in CMIP5 models under climate change scenarios
Changes in bottom temperature, salinity and density in the global ocean by 2100 for CMIP5 climate models are investigated for the climate change scenarios RCP4.5 and RCP8.5. The mean of 24 models shows a decrease in density in all deep basins except the North Atlantic which becomes denser. The individual model responses to climate change forcing are more complex: regarding temperature, the 24 models predict a warming of the bottom layer of the global ocean; in salinity, there is less agreement regarding the sign of the change, especially in the Southern Ocean. The magnitude and equatorward extent of these changes also vary strongly among models. The changes in properties can be linked with changes in the mean transport of key water masses. The Atlantic Meridional Overturning Circulation weakens in most models and is directly linked to changes in bottom density in the North Atlantic. These changes are due to the intrusion of modified Antarctic Bottom Water, made possible by the decrease in North Atlantic Deep Water formation. In the Indian, Pacific and South Atlantic, changes in bottom density are congruent with the weakening in Antarctic Bottom Water transport through these basins. We argue that the greater the 1986-2005 meridional transports, the more changes have propagated equatorwards by 2100. However, strong decreases in density over 100 years of climate change cause a weakening of the transports. The speed at which these property changes reach the deep basins is critical for a correct assessment of the heat storage capacity of the oceans as well as for predictions of future sea level rise
Mapping the ionised gas around the luminous QSO HE 1029-1401: Evidence for minor merger events?
We present VIMOS integral field spectroscopy of the brightest radio-quiet QSO
on the southern sky HE 1029-1401 at a redshift of z=0.086. Standard
decomposition techniques for broad-band imaging are extended to integral field
data in order to deblend the QSO and host emission. We perform a tentative
analysis of the stellar continuum finding a young stellar population (<100Myr)
or a featureless continuum embedded in an old stellar population (10Gyr)
typical for a massive elliptical galaxy. The stellar velocity dispersion of
sigma_*=320\pm90 km/s and the estimated black hole mass
log(M_BH/M_sun)=8.7\pm0.3 are consistent with the local M_BH-sigma_* relation
within the errors. For the first time we map the two-dimensional ionised gas
distribution and the gas velocity field around HE 1029-1401. While the stellar
host morphology is purely elliptical we find a highly structured distribution
of ionised gas out to 16 kpc from the QSO. The gas is highly ionised solely by
the QSO radiation and has a significantly lower metallicity than would be
expected for the stellar mass of the host, indicating an external origin of the
gas most likely due to minor mergers. We find a rotating gas disc around the
QSO and a dispersion-dominated non-rotating gas component within the central 3
kpc. At larger distances the velocity field is heavily disturbed, which could
be interpreted as another signature of past minor merger events. Alternatively,
the arc-like structure seen in the ionised gas might also be indicative of a
large-scale expanding bubble, centred on and possibly driven by the active
nucleus.Comment: 13 pages, 13 figures, 1 table, accepted for publication in A&
Quasar Host Galaxies in the FORS Deep Field
(abriged)In this paper we study different properties of quasars and their
host galaxies at high redshifts up to z~3.4. We compare our results to those of
other authors and discuss the correlation between galaxy evolution and quasar
activity. We analysed broad-band images in eight filters (from U to K) of eight
quasars in the FORS Deep Field with redshifts between z=0.87 and z=3.37. A
fully 2-dimensional decomposition was carried out to detect and resolve the
host galaxies. We were able to resolve the host galaxies of two out of eight
quasars between z=0.87 and z=2.75. Additionally, two host galaxies were
possibly resolved. The resolved low-redshift quasar (z=0.9) was identified as a
late type galaxy with a moderate star formation rate of 1.8 M_{sun}/yr hosting
a supermassive black hole with a mass of <10^{8}M_{sun}. The resolved high
redshift host galaxy (z=2.8) shows moderate star formation of 4.4-6.9
M_{sun}/yr, for the black hole mass we found a lower limit of >10^{7}M_{sun}.
All quasars host supermassive black hole with masses in the range
~10^{7}-10^{9}M_{sun}. Our findings are well consistent with those of other
authors.Comment: 16 pages, 5 figures, 11 tables, accepted for publication in A&
Host galaxy morphologies of X-ray selected AGN: assessing the significance of different black hole fueling mechanisms to the accretion density of the Universe at z~1
We use morphological information of X-ray selected AGN hosts to set limits on
the fraction of the accretion density of the Universe at z~1 that is not likely
to be associated with major mergers. Deep X-ray observations are combined with
high resolution optical data from the Hubble Space Telescope in the AEGIS,
GOODS North and GOODS South fields to explore the morphological breakdown of
X-ray sources in the redshift interval 0.5<z<1.3. The sample is split into
disks, early-type bulge dominated galaxies, peculiar systems and point-sources
in which the nuclear source outshines the host galaxy. The X-ray luminosity
function and luminosity density of AGN at z~1 are then calculated as a function
of morphological type. We find that disk-dominated hosts contribute 30\pm9 per
cent to the total AGN space density and 23\pm6 per cent to the luminosity
density at z~1. We argue that AGN in disk galaxies are most likely fueled not
by major merger events but by minor interactions or internal instabilities. We
find evidence that these mechanisms may be more efficient in producing luminous
AGN (L_X>1e44 erg/s) compared to predictions for the stochastic fueling of
massive black holes in disk galaxies.Comment: Accepted for publication in MNRA
High-redshift quasar host galaxies with adaptive optics
We present K band adaptive optics observations of three high-redshift (z ~
2.2) high-luminosity quasars, all of which were studied for the first time. We
also bserved several point spread function (PSF) calibrators,
non-simultaneously because of the small field of view. The significant temporal
PSF variations on timescales of minutes inhibited a straightforward scaled PSF
removal from the quasar images. Characterising the degree of PSF concentration
by the radii encircling 20% and 80% of the total flux, respectively, we found
that even under very different observing conditions the r_20 vs. r_80 relation
varied coherently between individual short exposure images, delineating a
well-defined relation for point sources. Placing the quasar images on this
relation, we see indications that all three objects were resolved. We designed
a procedure to estimate the significance of this result, and to estimate host
galaxy parameters, by reproducing the statistical distribution of the
individual short exposure images. We find in all three cases evidence for a
luminous host galaxy, with a mean absolute magnitude of M_R = -27.0 and scale
lengths around ~ 4-12 kpc. Together with a rough estimate of the central black
hole masses obtained from C_iv line widths, the location of the objects on the
bulge luminosity vs. black hole mass relation is not significantly dfferent
from the low-redshift regime, assuming only passive evolution of the host
galaxy. Corresponding Eddington luminosities are L_nuc/L_Edd ~ 0.1-0.6.Comment: 17 pages, 16 figures; submitted to Astronomy&Astrophysics. v2:
Absolute magnitudes corrected and as a consequence updated two figures, black
hole masses and stellar population age estimates in Discussion, but main
conclusions remain the same; accepted by A&
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Historical simulations with HadGEM3-GC3.1 for CMIP6
We describe and evaluate historical simulations which use the third Hadley Centre Global Environment Model in the Global Coupled configuration 3.1 (HadGEM3-GC3.1) model and which form part of the UK's contribution to the sixth Coupled Model Intercomparison Project, CMIP6. These simulations, run at two resolutions, respond to historically evolving forcings such as greenhouse gases, aerosols, solar irradiance, volcanic aerosols, land use, and ozone concentrations. We assess the response of the simulations to these historical forcings and compare against the observational record. This includes the evolution of global mean surface temperature, ocean heat content, sea ice extent, ice sheet mass balance, permafrost extent, snow cover, North Atlantic sea surface temperature and circulation, and decadal precipitation. We find that the simulated time evolution of global mean surface temperature broadly follows the observed record but with important quantitative differences which we find are most likely attributable to strong effective radiative forcing from anthropogenic aerosols and a weak pattern of sea surface temperature response in the low to middle latitudes to volcanic eruptions. We also find evidence that anthropogenic aerosol forcings play a role in driving the Atlantic Multidecadal Variability and the Atlantic Meridional Overturning Circulation, which are key features of the North Atlantic ocean. Overall, the model historical simulations show many features in common with the observed record over the period 1850–2014 and so provide a basis for future in-depth study of recent climate change
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