1,371 research outputs found
Deep LOFAR 150 MHz imaging of the Bo\"otes field: Unveiling the faint low-frequency sky
We have conducted a deep survey (with a central rms of )
with the LOw Frequency ARray (LOFAR) at 120-168 MHz of the Bo\"otes field, with
an angular resolution of , and obtained a sample of
10091 radio sources ( limit) over an area of .
The astrometry and flux scale accuracy of our source catalog is investigated.
The resolution bias, incompleteness and other systematic effects that could
affect our source counts are discussed and accounted for. The derived 150 MHz
source counts present a flattening below sub-mJy flux densities, that is in
agreement with previous results from high- and low- frequency surveys. This
flattening has been argued to be due to an increasing contribution of
star-forming galaxies and faint active galactic nuclei. Additionally, we use
our observations to evaluate the contribution of cosmic variance to the scatter
in source counts measurements. The latter is achieved by dividing our Bo\"otes
mosaic into 10 non-overlapping circular sectors, each one with an approximate
area of The counts in each sector are computed in the
same way as done for the entire mosaic. By comparing the induced scatter with
that of counts obtained from depth observations scaled to 150MHz, we find that
the scatter due to cosmic variance is larger than the Poissonian
errors of the source counts, and it may explain the dispersion from previously
reported depth source counts at flux densities . This work
demonstrates the feasibility of achieving deep radio imaging at low-frequencies
with LOFAR.Comment: A\&A in press. 15 pages, 16 figure
DTIC xenogenized lines obtained from an L1210 clone: clonal analysis of cytotoxic T lymphocyte reactivity.
Antineoplastic compounds can induce on tumour cells new antigens that undetectable on parental cells and which are transmissible as a genetic character. In this study mouse leukaemia L1210 was cloned in vitro by limiting dilution and one cloned line was recloned in vivo. Four subcloned tumour cell lines (A,D,R,S) were xenogenized in vivo by DTIC treatment (A/DTIC, D/DTIC, R/DTIC, S/DTIC) following a schedule previously described. Up to 10(7) cells of these xenogenized subclones, injected i.p., were rejected by syngeneic hosts, although they grew in immunosuppressed hosts. The DTIC treated subclones were lysed by in vivo-primed, in vitro-restimulated (with the relevant subclone) lymphocytes. The cytotoxic lymphocyte activity was not strictly specific since parental, DTIC-untreated cells were also lysed, although less efficiently. CTL directed against the D/DTIC subclone were cloned by limiting dilution. Ninety-four CTL clones were assayed against L1210 subcloned cells, DTIC-treated and untreated, and against different murine tumours (syngeneic or allogenic). Three specific antigens could be identified in the 51Cr release assay. The DTIC subclones expressed one antigen that was specifically recognized by a set of CTL clones. A number of CTL clones were able to lyse the L1210 subcloned cell exclusively, targetting a tumour-associated antigen that did not appear to be modified in the DTIC-treated subclones. A third antigen was demonstrated in the parental and DTIC treated D subclone. On the basis of these results it was postulated that there was at least one common DTIC-inducible antigen specific and reproducible within an identical cell population. Moreover, DTIC treatment did not modify histocompatibility antigens or TAA pre-existing in L1210 cells. The findings discussed here provide new information about permanent xenogenization of tumour cells, which might be exploited for experimental chemo-immunotherapy of cancer
A Quantitative Evaluation of the Galaxy Component of COSMOS and APM Catalogs
We have carried out an independent quantitative evaluation of the galaxy
component of the "COSMOS/UKST Southern Sky Object Catalogue" (SSC) and the
"APM/UKST J Catalogue" (APM). Using CCD observations our results corroborate
the accuracy of the photometry of both catalogs, which have an overall
dispersion of about 0.2 mag in the range 17 <= b_J <= 21.5. The SSC presents
externally calibrated galaxy magnitudes that follow a linear relation, while
the APM instrumental magnitudes of galaxies, only internally calibrated by the
use of stellar profiles, require second-order corrections. The completeness of
both catalogs in a general field falls rapidly fainter than b_J = 20.0, being
slightly better for APM. The 90% completeness level of the SSC is reached
between b_J = 19.5 and 20.0, while for APM this happens between b_J = 20.5 and
21.0. Both SSC and APM are found to be less complete in a galaxy cluster field.
Galaxies misclassified as stars in the SSC receive an incorrect magnitude
because the stellar ones take saturation into account besides using a different
calibration curve. In both cases, the misclassified galaxies show a large
diversity of colors that range from typical colors of early-types to those of
blue star-forming galaxies. A possible explanation for this effect is that it
results from the combination of low sampling resolutions with properties of the
image classifier for objects with characteristic sizes close to the
instrumental resolution. We find that the overall contamination by stars
misclassified as galaxies is < 5% to b_J = 20.5, as originally estimated for
both catalogs. Although our results come from small areas of the sky, they are
extracted from two different plates and are based on the comparison with two
independent datasets.Comment: 14 pages of text and tables, 8 figures; to be published in the
Astronomical Journal; for a single postscript version file see
ftp://danw.on.br/outgoing/caretta/caretta.p
Faint polarised sources in the Lockman Hole field at 1.4 GHz
We aim to study the nature of the faint, polarised radio source population
whose source composition and redshift dependence contain information about the
strength, morphology, and evolution of magnetic fields over cosmic timescales.
We use a 15 pointing radio continuum L-band mosaic of the Lockman Hole,
observed in full polarisation, generated from archival data of the WSRT. The
data were analysed using the RM-Synthesis technique. We achieved a noise of 7
{\mu}Jy/beam in polarised intensity, with a resolution of 15''. Using infrared
and optical images and source catalogues, we were able to cross-identify and
determine redshifts for one third of our detected polarised sources. We
detected 150 polarised sources, most of which are weakly polarised with a mean
fractional polarisation of 5.4 %. With a total area of 6.5 deg^2 and a
detection threshold of 6.25 {\sigma} we find 23 polarised sources per deg^2.
Based on our multi wavelength analysis, we find that our sample consists of AGN
only. We find a discrepancy between archival number counts and those present in
our data, which we attribute to sample variance. Considering the absolute radio
luminosty, to distinguish weak and strong sources, we find a general trend of
increased probability to detect weak sources at low redshift and strong sources
at high redshift. Further, we find an anti-correlation between fractional
polarisation and redshift for our strong sources sample at z{\geq}0.6. A
decrease in the fractional polarisation of strong sources with increasing
redshift cannot be explained by a constant magnetic field and electron density
over cosmic scales, however the changing properties of cluster environments
over the cosmic timemay play an important role. Disentangling these two effects
requires deeper and wider polarisation observations, and better models of the
morphology and strength of cosmic magnetic fields.Comment: 17 pages, 16 figures, to be published in A&
ROSAT Blank Field Sources I: Sample Selection and Archival Data
We have identified a population of blank field sources (or `blanks') among
the ROSAT bright unidentified X-ray sources with faint optical counterparts.
The extreme X-ray over optical flux ratio of blanks is not compatible with the
main classes of X-ray emitters except for extreme BL Lacertae objects. From the
analysis of ROSAT archival data we found no indication of variability and
evidence for only three sources, out of 16, needing absorption in excess of the
Galactic value. We also found evidence for an extended nature for only one of
the 5 blanks with a serendipitous HRI detection; this source (1WGAJ1226.9+3332)
was confirmed as a z=0.89 cluster of galaxies. Palomar images reveal the
presence of a red (O-E~2) counterpart in the X-ray error circle for 6 blanks.
The identification process brought to the discovery of another high z cluster
of galaxies, one (possibly extreme) BL Lac, two ultraluminous X-ray sources in
nearby galaxies and two apparently normal type1 AGNs. These AGNs, together with
4 more AGN-like objects seem to form a well defined group: they present
unabsorbed X-ray spectra but red Palomar counterparts. We discuss the possible
explanations for the discrepancy between the X-ray and optical data, among
which: a suppressed big blue bump emission, an extreme dust to gas (~40-60 the
Galactic ratio), a high redshift (z>3.5) QSO nature, an atypical dust grain
size distribution and a dusty warm absorber. These AGN-like blanks seem to be
the bright (and easier to study) analogs of the sources which are found in deep
Chandra observations. Three more blanks have a still unknown nature.Comment: 23 pages, 8 figures, accepted by ApJ main journa
The 500 ks Chandra observation of the z = 6.31 QSO SDSS J1030+0524
We present the results from a ks Chandra observation of the
QSO SDSS J1030+0524. This is the deepest X-ray observation to date of
a QSO. The QSO is detected with a total of 125 net counts in the full
( keV) band and its spectrum can be modeled by a single power-law model
with photon index of and full band flux of
erg s cm. When compared with the data
obtained by XMM-Newton in 2003, our Chandra observation in 2017 shows a harder
() spectrum and a 2.5 times fainter flux. Such a
variation, in a timespan of yrs rest-frame, is unexpected for such a
luminous QSO powered by a black hole. The observed source
hardening and weakening could be related to an intrinsic variation in the
accretion rate. However, the limited photon statistics does not allow us to
discriminate between an intrinsic luminosity and spectral change, and an
absorption event produced by an intervening gas cloud along the line of sight.
We also report the discovery of diffuse X-ray emission that extends for 30"x20"
southward the QSO with a signal-to-noise ratio of 6, hardness ratio of
, and soft band flux of erg s cm, that is not
associated to a group or cluster of galaxies. We discuss two possible
explanations for the extended emission, which may be either associated with the
radio lobe of a nearby, foreground radio galaxy (at ), or
ascribed to the feedback from the QSO itself acting on its surrounding
environment, as proposed by simulations of early black hole formation.Comment: 13 pages, 9 figures, A&A accepte
The Aquarius Superclusters - I. Identification of Clusters and Superclusters
We study the distribution of galaxies and galaxy clusters in a 10^deg x 6^deg
field in the Aquarius region. In addition to 63 clusters in the literature, we
have found 39 new candidate clusters using a matched-filter technique and a
counts-in-cells analysis. From redshift measurements of galaxies in the
direction of these cluster candidates, we present new mean redshifts for 31
previously unobserved clusters, while improved mean redshifts are presented for
35 other systems. About 45% of the projected density enhancements are due to
the superposition of clusters and/or groups of galaxies along the line of
sight, but we could confirm for 72% of the cases that the candidates are real
physical associations similar to the ones classified as rich galaxy clusters.
On the other hand, the contamination due to galaxies not belonging to any
concentration or located only in small groups along the line of sight is ~ 10%.
Using a percolation radius of 10 h^{-1} Mpc (spatial density contrast of about
10), we detect two superclusters of galaxies in Aquarius, at z = 0.086 and at z
= 0.112, respectively with 5 and 14 clusters. The latter supercluster may
represent a space overdensity of about 160 times the average cluster density as
measured from the Abell et al. (1989) cluster catalog, and is possibly
connected to a 40 h^{-1} Mpc filament from z ~ 0.11 to 0.14.Comment: LateX text (21 pages) and 12 (ps/eps/gif) figures; figures 5a, 5b and
6 are not included in the main LateX text; to be published in the
Astronomical Journal, March issu
The CoNFIG Catalogue - II. Comparison of Space Densities in the FR Dichotomy
This paper focuses on a comparison of the space densities of FRI and FRII
sources at different epochs, with a particular focus on FRI sources. First, we
present the concluding steps in constructing the Combined NVSS-FIRST Galaxy
catalogue (CoNFIG), including new VLA observations, optical identifications and
redshift estimates. The final catalogue consists of 859 sources over 4 samples
(CoNFIG-1, 2, 3 and 4 with flux density limits of S_1.4GHz = 1.3, 0.8, 0.2 and
0.05 Jy respectively). It is 95.7% complete in radio morphology classification
and 74.3% of the sources have redshift data. Combining CoNFIG with
complementary samples, the distribution and evolution of FRI and FRII sources
are investigated. We find that FRI sources undergo mild evolution and that, at
the same radio luminosity, FRI and FRII sources show similar space density
enhancements in various redshift ranges, possibly implying a common evolution.Comment: 15 pages, 15 figures, 6 tables + appendix (80 pages). accepted in
M.N.R.A.
Epidemiology and pathophysiology of cancer-associated thrombosis
Venous thromboembolism (VTE) is a common complication in patients with malignant disease. First recognised by Bouillard in 1823 and later described by Trousseau in 1844, multiple studies have since provided considerable evidence for a clinical association between VTE and cancer. Across all cancers, the risk for VTE is elevated 7-fold; in certain malignancies, the risk for VTE may be increased up to 28-fold. Venous thromboembolism is the second leading cause of death in patients with cancer; among survivors, complications commonly include recurrent VTE and post-thrombotic syndrome, and (more rarely) chronic thromboembolic pulmonary hypertension, which are costly, and have a profound impact on the patient's quality of life. Tumour cells can activate blood coagulation through multiple mechanisms, including production of procoagulant, fibrinolytic, and proaggregating activities, release of proinflammatory and proangiogenic cytokines, and interacting directly with host vascular and blood cells (e.g., endothelial cells, leukocytes, and platelets) through adhesion molecules. Increasing evidence suggests that elements of the haemostatic system also have a direct role in eliciting or enhancing angiogenesis, cell survival, and metastasis. Despite the problem posed by VTE in the setting of cancer, it is evident that a significant number of oncologists do not recognise the link between cancer, its treatment, and thrombogenesis. On 22 May 2009, a group of UK-based physicians met in London, UK, to evaluate recent data on cancer thrombosis. This article (1 of 4) briefly reviews key data on the epidemiology and pathophysiology of VTE as a context for a discussion and consensus statement developed by meeting attendees, on the implications of this information for UK clinical practice
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