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The environment of high-redshift AGN OLIMPIA JUDIT FOGASY
The environment of high-redshift AGN OLIMPIA JUDIT FOGASY

Discovery of a Dwarf Poststarburst Galaxy near a High Column
Discovery of a Dwarf Poststarburst Galaxy near a High Column

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... −1.4 %, suggesting the rising tendency of AGN fraction in clusters with redshift from 0.05 to 1.5. With the Chandra Multiwavelength Project (ChaMP) and SDSS data, using L0.5−8keV > 1042 erg s−1 to select AGNs, Haggard et al. (2010) found that the AGN fraction in groups is 0.16% for z ≤ 0.125, and 3. ...
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... The analysis of the underlying host galaxy in AGN images is a challanging task, particularly in cases of low flux contrasts between the host and nucleus. The key issue for an accurate removal of the central point source and a determination of the host properties is a good knowledge of the Point Spre ...
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Probing nuclear activity versus star formation at z ∼ 0.8 using near

... formation properties of 58 X-ray-selected AGN at 0.5 < z < 1.4 by modelling their multifrequency SEDs and did not find strong evidence for either highly suppressed or enhanced star formation when compared to a mass-matched sample of galaxies at the same redshift. However, these AGN were selected to ...
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... for cD, E and S0 galaxies, compared to < S > = 1.1 for all spirals. The specific frequency < S > = 9.3 in nine cD/E galaxies is higher than that in 34 E + S0 galaxies for which < S > = 5.1. Furthermore, the specific frequency < S > = 0.8 in eight late-type spirals (Sb - Scd) is significantly lower t ...
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... ratio (attenuation) for UV galaxies. For IR (24m) selected galaxies at z~0.6, no evidence is found for evolution of either the stellar mass or the IR/UV ratio for given LIR. 8. Both IR and UV evolve significantly from z=0 to z=1, and the ratio IR/UV increases by ~ 4. This is consistent with the ...
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... generated by the first generation of collapsed objects. These highredshift objects are highly biased, leading to large variations in their number density. This, combined with the 1/r 2 dependence of the flux, causes large fluctuations in the Lyα background, which can be probed through their effect o ...
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Groups of galaxies in the SDSS Data Release 7*

... effects can be observed here. In the majority of recent papers dedicated to group searches, the group finders are tuned with mock N-body catalogues (Eke et al. 2004; Yang et al. 2005). The mock group catalogues are homogeneous and all parameters of the mock groups can be easily found and applied to s ...
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Markov Chain Monte Carlo Modeling of High-Redshift Quasar

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... as source 1, in Table A1. It has a linear size of ∼40 arcsec, which is just beyond the limit of extended structure detectable by the VLA in A configuration. It is the brightest source near the field by almost an order of magnitude and its residual sidelobes, after cleaning, were the major noise cont ...
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... clouds of the Magellanic Stream which may well have formed in situ. Models for the dynamics of the satellites and the Milky Way suggest that the tiny galaxies may be completely disrupted and disintegrate within a few hundred million years. 5.2 The Sagittarius Dwarf Elliptical Galaxy Another satellit ...
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Redshift



In physics, redshift happens when light or other electromagnetic radiation from an object is increased in wavelength, or shifted to the red end of the spectrum. In general, whether or not the radiation is within the visible spectrum, ""redder"" means an increase in wavelength – equivalent to a lower frequency and a lower photon energy, in accordance with, respectively, the wave and quantum theories of light.Some redshifts are an example of the Doppler effect, familiar in the change of apparent pitches of sirens and frequency of the sound waves emitted by speeding vehicles. A redshift occurs whenever a light source moves away from an observer. Another kind of redshift is cosmological redshift, which is due to the expansion of the universe, and sufficiently distant light sources (generally more than a few million light years away) show redshift corresponding to the rate of increase in their distance from Earth. Finally, gravitational redshift is a relativistic effect observed in electromagnetic radiation moving out of gravitational fields. Conversely, a decrease in wavelength is called blueshift and is generally seen when a light-emitting object moves toward an observer or when electromagnetic radiation moves into a gravitational field. However, redshift is a more common term and sometimes blueshift is referred to as negative redshift.Knowledge of redshifts and blueshifts has been applied to develop several terrestrial technologies such as Doppler radar and radar guns. Redshifts are also seen in the spectroscopic observations of astronomical objects. Its value is represented by the letter z.A special relativistic redshift formula (and its classical approximation) can be used to calculate the redshift of a nearby object when spacetime is flat. However, in many contexts, such as black holes and Big Bang cosmology, redshifts must be calculated using general relativity. Special relativistic, gravitational, and cosmological redshifts can be understood under the umbrella of frame transformation laws. There exist other physical processes that can lead to a shift in the frequency of electromagnetic radiation, including scattering and optical effects; however, the resulting changes are distinguishable from true redshift and are not generally referred to as such (see section on physical optics and radiative transfer).
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